Korea-China Optical Technology Research Centre - OSTI.GOV

KAERi/RR-2737/2006

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SUMMARY

L Title: Korea-China Optical Technology Research Center

II. Objective of the Project

The main objectives of this project are to develop cooperative channel by personnel exchanges between industrial, educational and research partners of Korea and China on the fields of optical technologies which are the basis of optical industry and being spotlighted as new industry of 21th century, and to raise the class of Korean optical technology up to world class by utilization of Chinese large facilities through the cooperative research between the optical technology institutions of both sides.

Particularly the technique which can produce the high energy density state on the ground using high power laser is applicable to both the fast ignition as a core technology of laser fusion and the basic science of extreme material state. Therefore, the mutual research cooperation is strongly needed to utilize Chinese facilities and to acquire technique to establish the foundation of high energy density sciences in Korea

III. Scope and Contents of

To attain the goals mentioned above, we carried out the cooperative researches between the Korean and Chinese optical technology institutions in the following 5 fields in the 1st and the 2nd years,

o research cooperation between KAERI-SITP for the quantum structured far-IR sensor technology;

o research cooperation for the generation of femtosecond nuclear fusion induced neutrons;

o research cooperation between KAERI-AIOFM for laser environment analysis and remote sensing technology;

the Project

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o research cooperation between KAERI-SIOM for advanced diode-pumped laser technology "> and

o cooperative research related on linear and nonlinear magneto-optical properties of advanced magnetic quantum structures.

We also carried out the researches for laser system and its application related on high energy density sciences in the 3rd year;

o design of pico-second PW high power laser system and its simulation and

o cooperative research related on the femto-second laser-plasma interaction physics.

IV. Results of the Project

o research cooperation between KAERI-SITP for the quantum structured far-lR sensor technology.

- the development of technology for high quality quantum dot growth, design and band gap modulation.

o research cooperation for the generation of femtosecond nuclear fusion induced neutrons.

- the acquisition of measurement technology for high density plasma characteristics and the success of generation of nuclear fusion induced neutrons at Chinese nuclear fusion research facility.

o research cooperation between KAERI-AIOFM for laser environment analysis and remote sensing technology.

~ the technology development for realtime analysis of floating particles and detection quality enhancement of yellow sand storm LIDAR.

o research cooperation between KAERI-SIOM for advanced diode-pumped laser technology.

- the technology development for TEMoo. 15 W optical fiber laser and 500 W grade ceramic laser.

- (V -

o cooperative research related on linear and nonlinear magneto-optical properties of advanced magnetic quantum structures.

- research related on fabrication of MPC based multi-layered thin film structure and physical characteristics, and publication of SCI papers

o design of psec PW high power laser system and its simulation. - achievement of design technique for front-end fiber laser in psec PW

high power laser.

o cooperative research related on the femto-second laser-plasma interaction physics.

- realization of filamented high energy electron beam penetrating through high density plasma,

- the acquisition of numerical analysis technique for proton generation in laser heated cluster.

V- Future Plans

Korea and China agreed to continue mutual cooperation for the fields of high energy density sciences (laser nuclear fusion) at the ministry of Science and technology Ministers' meeting in June 2006. And even China is promoting the trilateral cooperation on the fields of high energy density sciences among China, Korea and Japan. So, afterwards Korea-China joint research center will focus on the cooperation on the high energy density sciences, and try to accumulate the fast ignition related laser technology developed by SIOM which is the key technology in demonstrating laser fusion energy.

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1*11 ^73144 4^31 £ 4 '06 4 ^ 4 *J4 ^ ^ f - 3 7 4 4 ^ 7 ^ 4 b 3144 -S-% 4 7 4 42: ^4A34 5x4 H444 4^. a .M^]4 434, '06.6. ^T-47144514^14 t f - 4 4 3-444i^£44(^0 l *1^4^)£4°11 314 ^% %4 4 i l 3 3144 ^ 4 4 4 ^&2H 4 ^ 4 ^ 4 4 2 7fl 4 4 4 4 4 4 b #5= 4^-44

- 5 -

31 2 4 trf1 4*)#^47-(20044~20051d)

*ll 2 S t*§ ^7|#§t^^(2004t3-2005y)

*ll 1 1 ^ H ^ -tl^^xd 4M 7l#oj| 3J8F KAERI-SITP?!^ 7llHH

1.1 gJ*rS £&7le

3l3.£ 7^47]# g *l|£& 711S.4 i o j ^ _g.gj} 4 3 ^ 7 j#o 47J-51144 a«)( e 104

f-4 ^ 47^1 45-^j 4 4 ^ (quantum dots; QDs) A344^4 In(Ga)As ^ GaAsf 4

£ 4 45=^ T|JJL§ -§-444 ^ 5 S 04€ i'-2:# 4£*l) 4 ^ i S2j4^ 7W4 t 4 ^

4 £ 4 3 &4. 4 b 44^3) 314 # 4 4 4 « bH. fH44, 4 £ 4 bulk ^ 4441-•?5S 4^*1 £ 4 b 4 4 b 2IA}1- - GaAs7l44 4f-^l2:7} ^ lOum 314 47437} W - 431 314 7)- 31 ^1^x14 ^ 4 4 ^ ^ In(Ga)As/GaAs 4 4 ^ 7J4ofli=. Stranski-Krastanov (S-K) model- 4 4 4 4^Â3 7144 -§"44 4 $3_4, 4 4 4 4 ^ 4 In ^ As^- a ^ A3444fe- 4 4 ^ 4 4 7 1 ^(atomic layer epitaxy: ALE) ^-& migration enhanced epitaxy $Vi (MEE)# 4 4 4 4 ^ 4 , S-K ^34^ °fl 4*H #2! 4 44°fl 4 1 4 4 4 4 4 photo)uminescencc (PL) spectrum4 Ji

4 3 , 59J4 44^Â32] -iH-g. ^ ^-g-4 7f^7A0| ^ . 4 4 a 44 . 4 ^3.4

<44b 4 4 4 4 4 441- t4*14 MBE 7344^351 480- 31*1 MEE 4 ^ #

Af-e-44 AJ44 InAs/GaAs442l2) 72^4 4 4 3 Â3-§- atomic force

microscopy ^ transmission electron 3.3. 4 4 4 4 , 4*14" 1 ML InAs 4 4 4 4

74A4O] <#*}% .ÂÎ 3 4 oj-^4 4^3^. jijL44.

3 4 2-1^- S-KA34^4 ALEA34^4 4 ^ 1 - ^ 4 ^ 4 , £ U33114 71144^ InAs 44^^ r (100) GaAs 4444} 480 °C4 7J4^-H.O)1A^ 3 monolayer (ML)4 InAs44 #4°il 2)44 A^4- 5 ]^4 4 4 4 ^ 4 ^ G a A s ^ I n A s ^ AJAJ-^.Q.

- 7 -

SK m o d e do t ALE m o d e do ts

W e t t i n g layer is i nev i t ab le Rela t ive ly s m a l l d o t s ize

( < - 2 0 x - 1 0 n m ) W a v e l e n g t h (1000 - 1300 nm + a)

• W e t t i n g layer is not n e c e s s a r y • Re la t i ve ly la rge do t s ize (> - 4 0 x - 1 0 n m )

• W a v e l e n g t h ( more t han 1400 n m is possible)

Dots N per iod of layers

/ | GaAs Wet ing layer i M L - G a A s 1 M L - l n A s

3%) 2-1. S-K*34^4 ALE ^ 3 4 ^ 4 «}3i

4 4 &% 1ML £ 0.07ML ^ - 4 4 A34°l] *H44b ^ 3 4 ^ 4 4 , As44 ^ 4 4 3 ^ &®%e] ^ 4 4 ^ 4 3~5 4 4 4 4- 3 4 2-2b ^*}°\\ *}-§-€ 4 4 4 sample4 4 AJ- sequence-! H 4 # 4 . #MEE $ #CONfer 4 4 4 .1-44 ALE/MEE, S-K 4 ^ 3 . ^ 4 4 4 sampled 4 ° 1 4 4 , #MEE-CON ^ #CON-MEEb 2ML1-4 4 MEE 9? C O N 4 ^ 3 ^ ^ 4 4 3 4*14 1ML1- CON ^ MEE4^3.5. 4 4 4 sampled 2 ) 4 4 4 .

Growth interruption

ij^rj Sample #MEE

[iMl-Uilcki

L3i5 i

1min

EZI Sample #CON

Anneal ing time for QD format ion

1ML-thK*l In

I iML-lbiok! i__i!L-J

1 min jSample #MEE-CON i J IML-lhlck

1 min Sample #CON-MEE flML-thlskl ( ln_

S a m p l e # M E E ; 3 M L - t h i c k InAs QDs g r o w n by m i g r a t i o n e n h a n c e e p i t a x y (MEE) .

S a m p l e # C O N - 2 .4ML- th ick I n A s QDs g r o w n by c o n v e n t i o n a l M B E (CON).

Sample #MEE-CON: 1 ML-thick C O N - g r o w n fnAs layer on MEE-g r o w n 2 M L - l n A s layer.

S a m p l e # C O N - M E E : 1 ML- th i ck M E E - g r o w n I n A s layer on CON-g r o w n 2 M L - l n A s layer .

[AS (2S>I

Time

3 ^ 2-2. 4^Ml 4-8-4 4 4 4 sample4 A34 sequence

- 8 -

Sample #MEE

4"^** -vv4v *.;:,

Dot density, width and height of the sample #MEE are ~4.1x1010/cm2, -40.8 nm, and -7.2 nm, respectively.

#CON

-134x1010/cm2, -31.0 nm, -2.6 nm.

#MEE-CON

~8.1x10,0/cm2,~30.1 nm, and -Z7 nm.

#C0N-MEE

~3 6x1010/cmz, - 45 0 nm, and - 6 8 nm

Structural properties of MEE and CON-MEE are very similar and those of CON and MEE-CON are simitar.

—> Final 1 ML-thick InAs play a critical role to define the shape and density of InAs quantum dots

3 ^ 2-3. 7fl4€ 4 4 ^ A 3 4 4 ^ 3 . S 4SMg 4 4 3 4 AFM 4 4 . (lum x lum)

3 ^ 2 - 3 ^ 4 4 2 l -^A^^^-S. jgsffi o o v ^ r ^ o | A F M 4 ^ l o . s > 4 - 4 4 o o t z | .^

4 ^ ^ ^ 4 A 3 4 4-8-4 4 4 . #MEE4 <#43 *2SL, ^ 3 4 3 ^ - 4 ^ 4-4-~4.1xl010/cnr, "40.8 nm, 3 4 3 ~7.2 nm44. #CON4 *3-f AA "13.4x10'/cm2, "310 nm, "2.6 nm43 , MEE-CON

^ #CON-MEEb 4 4 "8.1xl0l0/cm2, "30.1 ran, "2.7 nm 3 4 3 "3.6xl010/cm2, "45.0 nm, "6.8 nm44 . °i7l4 + 4 b #MEE S #C0N4VIEE4 42--^ 4A34 4 4 4 4 , #CON ^ #MEE~CON4 ^ 4 # A 34 -fr*W-§- 4 4s- 514.

§ The thicknesses of the wetting layer Is 2.1, 4, 3.6, 2.5 nm, respectively.

MEE SCON-MEE « MEE-CON SCON

Thicknesses of wetting layer of MEE and CON-MEE are very similar and those of CON and MEE-CON a«e- similar.

-►This irnplica that carrier dynamics as a function of femperato'e will be similar in &SEE and CON-MEE. And also in CON and MEE-CON.

3 ^ 2-4. 4 4 4 4 4 ^ *3 44^3.5. 4A$. #4^21 4 ^ TEM 4s.

- 9 -

3 fj 2-344 S .44 AFM ^ 4 - ^ 3 . 4 4.44- inAs 1ML4 431 4 ^ 4 4 H Ol

2ML4 InAs 4 4 ^ 7-fls 4^-^-4 °344 # # 4 ^ 01 fe^ o i^ ^ 2-44 4 $ TEM 4 3 \ 3 . £ 4 ? 1 4 4 . 4 4 4 ^ 4 4 4 4 / 4 ^ 4 44-1- 4 - f 4 b Wetting layer4 n ^ l b #MEE 4 #C0N-MEE4 T - 4 4 4 4 2.1, 2.5nm£ &4°H 441 #CON Ik #MEE-C0N4 *4f 4, 3.6 nmS 4^4 4 3 S . ^ 4 . Wetting layer4 ^ ?flb 4 4 2 ] 3 ^ 2-5, 2-6^14 iL°l^°l 4*14 421 earner dynamics# 4 4 4 b ^,9. SL^.3. 4 4 ^ 2 1 144*3*32] -f<i-§- 1*344 . t%*4±£. ^ 3 wetting

Iayer-t i M r t r 4 4 ^ 4 3 4 ° 1 1 4 4 * 3 € - § - 4 ^ : 4 ^ 1 € 4 -

3 ^ 2-5b 4 4 2 ] 44^3 sample4 70K 4 ^ PL ^ 4 1 - i £ 4 ^ 4 . <^14 #MEE S #CON~MEEb 4 £ 4 ground PL peak 4 4 - i £-°14 *fll44 peaki s f l44b peak.£ Ji2i4. 4°fl #^fl #CON ^ #MEE~CON-£- PL447} 47) #MEE 4 #CON-'MEE<>fl 4 4 4 4 4 4 4 214 %(34, 3.4 ground PL peak4 s i ! 4 4 b

In the case of MEE and CON-MEE, the spectra have 2 peaks which are attributed to ground and 1 s t exited level of the QDs. The PL peak wavelengh for MEE is longher than that of CON-MEE due to size effect. This is attr ibuted to size reduction of InAs caused by generation of coalescent QDs

For CON and MEE-CON, only 1 peak due to ground level is identif ied The shape of PL spectrum for CON and MEE-CON is very simi lar due to similar structural p roperttes

900 1000 1100 1200 Wavelength (nm)

i 2-5. 71144 4 4 ^ ^A»^SL£. 4 4 € 4 4 ^ 4 70 K-PL 3 ^ m ^

peak4 U 4 4 . ° l b 3 ^ 2-2°JM J£4^-°l f ^ ' ^ S #C0N % #MEE-CON4 4 4 H M ajajj 4€- 4 4 4 3 . ^ 4 ^ 4 4 3H14 ? 1 4 4 4 ° . s . H 4 4 4 4 4 1ML4 InAs*34 4^°1 34]*3?J 4*}4 A34°ll key-role-§- 4 3 &-§--§- 4 ^ 4 4-

- 10 -

MEE CON f 08

s >. i.oe

» <a 104

£l.02 1 6.

1.00

% TJn

D vo \ '

s_ □

•*%.#•»#_#^ 0 50 100 150 200 250 300

Tempefahi(e(K)

MEECON 122

0 50 100 160 200 299 300 Timperaturs(K)

CONMEE

The PL line width of MEE and CONMEE is relatively insensitive to cryostat temperature. This is attributed to reduced wetting ■layer as shown in crosssectional TEM images.

On the contrary, CON and MEECON has fluctuation or PL line width as a function of cryostat temperature.

These tendency are also shown in PL peak energy as a function of cryo

stat temperature.

0 50 103 150 200 250 303

T e m p e u t u i e (K)

0 50 100 *5D 200 25

T e m p ? u i t i j i e ( K )

3 ^ 26. 7i]4si < £ 4 ^ 7J UJU1 O.

peak*] 4 4 3l 4 # 71144 4 4 ^ 4 ^ - S - i c i 4€- PL

4 4 b 2 H rflti ^ 3 ms. 3 ^ 2-51- • 4 fl4. 3 * ! 2 6 4 4°A'$. 4*14 *3 444-?-^- 7il4€ 4 4 ^ 2 ] ^--^3i=4 n$g PL pCak4 4 4 ^ ^ 4 i i 4 f c 4 . 47Hl*iie ^ 4 ^ - 4 #MEE ^ #CON-MEEb 4*34:1241 4-B 4 ^ 4 £ 4 4 Dl 4 4 4 , #CON " #MEE-C0N4 #*3£-£o11 u}^. J ^ *3Sj_7i. cH i?-oji 441 ^ 4-1: 4 4 %XA. 4 b 3 f 2-44*1 H 4 wetting laycr4 - r^ l4 4 4 4 4 4 %\ 4- ^ &4r wetting layer# -M-ff4 4 * H i £ 7 M 4 ^r4 4 4 ^ 4 4 carrier 4 4 4b- ,36l 43JB.3. 4-44 carrierb 0 4 4 4 4 4A3 - carricr4 4 4 T 1 - ^ 4 4 -££<=fl 4€- P L - ^ 4 ^ - 4 4 & 4 -3t ^ - 4 4 . 4°fl 4*11 - r 4 £ wetting layer# -£-fr?r 4 4 ^ £ wetting laycr-^ -f^ carricr7} ^ 4 4*143-3- &7\ 4V]°ll 4 4 4 4 t r carrier dynamics!- UL44. 4°fl 4 4 PL 44-£- -&3\4 4 4 4 4 4 44-1- l i 0 J4 .

1 4 4 A S lnAs44^*l 4 4 4 4*14 1ML4 4&14^°fl 4 4 - 3 4 m%% <y- ^ £14.

: T ^ : * 3/44 s v ^

- 11 -

Schematic illustration of samples 300 K PL spectra

7.5 rimthick InAs QDs /

l n ?G a

osA s

L= 0, 1.2 and 2.5 rimthick

300 K PL spectra at tb = 1.2 nm 64meV

Thin !b induces redshift due to lowered barrier effect.

Thick ft invokes blueshift due to intermixing

1200 )300 Wavelength (nm)

PL spectra at tb = 1.2 nm as a function of cryostat temperature

900 1000 1100 1200 1300 1400 Wavelength (nm)

Linewidth of DAS WELL (f = 1.2 nm) is insensitive to cryostat temperature due to strong carrier confinement.

AEg_, is 64 meV which is smaller than InAs QDs in GaAs matrix (78 meV)

50 100 150 200 250 300 Temperature (K)

3 g 2-7. InAs xMEE444-§- °144 4^3*3 4*r4°ll ^ 4 4D £ 4 4 4

3 1 274 InAs MEE4*14§ °1£# ultfl^S 4 * l 4 i H14 # 3 £ 4 p H 4 4 4 421 #*VM^ 3t 4 4 ^ ^2] zri£s) level44 4*1€ 44*j2l 3 4 # JW 71147} 7}^

4 4 4 * 44*34 Ji t fsU ^ 4 4* }^4 2 3 * 4421 4 4 ^ 4 37HI 44 «144 b 4 4 4 4 4 4 4 &4. 34H5L 4 4 ^Hi4 4 4 4 4 241 $£■$ MEE°<)*HH 31 si Ino2GaosAs 44411 4 ^ 4 3 ^ ^34435. 4*14 ^ 1 4

yj3^§ £S}*14 4 4

4 ifl^i z.}zv ievel4:4 43§ €SM?U4 4b 4HfS 4s345S 4D4$24. «*H 4 4

^ 4 4 / 4 ^ InGaAs#4 r ^ l r 7.5nm, 1.2nm447} 44S-I- 4 ^ $13 4 4 4 4 4 ^ A3£ 4 b InAs4*14

0l l «l^fl 1 4 * 1 4 £ 3 . 4 4 4 3 1 . 3 u m 4 4 3 ^ 4 4 4 1 £•§: ^ 31

41 4 4 4 ^ 4 4 4 4 5 i 4 . 1 i 4 4 M E E L n A s 4 4 ^ t 4 * 1 ^ 4 3 4 7 } 4 4 8um 4

4 4 4 4 f47} ^ r ^ r a s . 4 4 4 4 4 4 4 1 : 34 4 4 4 147} 7 } ^ 4*14 4 5:4 4^4 7^44. 4 ^ 1 ^ ^ ^ 4#4°J £ 4 £ 4 4 4 4

S3 4 4 .

1.2 ^ S - § 4 A|ZJS § § 4 4 3 * t e 4 i ! i inAsgMS^I 7 ^ 4

^ 4

Molecular beam epitaxy 4 4 # 4 4 4 4 *14£ InAs 44^-§- 43-b 4 ^ £ 4 4 7}T]7\ 014. *1^4 4^-2/ In cell -&£., As cell ^r-£, Ga cell £-£, *34 4

12

4 £5., In 4 4 , As 4 4 f-4 4 4 1 - ^ 4 4 ^ £ InAs/GaAs 44*3-1: 4 1 4 & 4 . £ ^ ^ ^ 3 ^ 2-84 *34 # 4 *144 £ 1 4 4 4 ^ 3 InAs 44*3-i- 414 4 b 7^4 ^ - 4 4 4 .

-H- *iî£ 4 4 4 4 4-§-4£ 44214 ^4-i : 4 H V 3 S 4 4 4 43-4 (quantum cryptography) 7]ô\) A}^-S]^- #<£%7}^(single photon light source) 4 4 1 - b^?H 4-1 4 4 4 . 4 * r 4 £ 42J 4 4 1 - Ml-b 7 ^s 4 4 4 %\ 4 . 44*1 InAs/GaAs 4*14-1: r2/um2 4 4 ^ 4 ^ £ ^ 4 - t 4 4 4 . 4 4 4 4 4 4 1 - 4 ^ 4 4 4 ^€sH44.

3^J 2-8-g- 4 ^ 4 44)<U A34 ^ 4 4 4 4 H t € ^42] -g-42j°ll 4 4 s. 4 £ 4 4 . 44*3 44*1 in 4 ^ 1 - 3*3*14 9i^ 2-€- 4 4 1 - 4 3 4*1 As 4 4 1 4*3*14 3 * 4*1 -S-b 4 4 # 4 b 4*34 4 4 # 4 4 4 4 44*34 *3 4 4 $ 4 . 4 4 4 £.b 4 4 # 4 b W W x j ^ ^ ^ 1 4 ^ » K £ 4 44*3-1: 2 * ^ $14.

3 ^ 2-94 4 ^ 44°fl 4-§-€ 4 4 b £ 4 4 Ajf # * | S < ^ ^ 4 4 VG semicon44 V80 4 4 4 4 . # # i 4 4 4 6l-£- w f t 4 4 4 3 ^ , 4 , 44*4 4-.1- # 4 4 3 W 4 4 4 4 4 ^ - ^ 2.5 x 10"11 ton-43, ^ f^4 4 ^ £ ~ 2 x 10 7 torr4&4. -£ 4 ^ 1 i b 27H4 Ga 4 ^ 4 144 in %&%% 17H4 As i~i € 4 4 4 4 4 $14. As/Ga4 # 4 4-§-£ 4 10:14$4. GaAs 4 4 # 600°C5. 7}144 4 4 M 4 444- i - 4 4 4 +, 7l4t4 %'•£# 580°C5. S ^ 4 4 100 nm ¥421 GaAsl- 44(buffer)S*1 ^ # 4 ^ 4 . *]Ff 46001 3 ^ 2-94 4*14 42:1- * 3 4 4 ^ 4 .

3 ^ 2-10-g- <g*l 4 4 ^ 4 4 * 4 4 44f t ^ # 4 automic force microscope (AFM)3.s. 4 £ 4 4 4 4 . 3 ^ 2-l0a.b * 3 4 ^ 4 4 4 4 5^4 4 * 4 4 1.76X 1010 7fl/cm24 4 4 ^ 4 £ 1 *}44. 3 ^ 2-10bb * 3 4 ^ 4 4 4 4 10^4 K # 4 4 1.60X1010 7H/cm2 4 4=44 i s § 7}?i4. 35J 2 lOcb - f^ f^ 4 4 4 20 ô] ^ # 4 4 1.12XIO10 7B/cm2 4 44*3 « s * 4*J4. 3 ^ 2-10db A 34^4 4 4 4 30:*4 ^1-44 2.ooxio9 ?il/cm2 4 4 4 4 4^1- 4 4 4 . 4 4 4 4 4 ^ 444 4 4 4 4 $ ^ 4 ^ 4 4 # * ^14 4 4 4 44 £ 4 £4.

3 ^ 2-ll-€r 3 ^ 2-10a, 3 ^ 2-10b, 3% 2-10c, 3 ^ 2-10di «H44b H4 4 4 ^ 4 4 4 4 4 4 4 € ^ 4 4^.17,4^0]4, ZL^ 2-1H4 J i ^ 4 £ 4 ^ 4 a3-^4 4 4 4 ^ 4 1 S InAs 4*144 « # * 4 4 - 61 f i t 4 # * 1 4 3 ^ 2-1H4 £ 4 b 314! ^34^4 *144 44*3 4 4 4 4-8-4-4 4 4 4 4

- 13 -

u4- O 471 4 crrf4 1.76X1010 7JH14 4 4 ^ cm

24 ^ltfl 2.00X10° 7M o ^ ^ u£

1S.-1- <£-§- 4 4 4 . 4 € 4 441-S.iE 4 4 3 \ InAs 4 4 * 3 4 4Hb^ l l 4*3 ^ 7\ 0_ 5)-_0_ 4 ; 43.4, 4 4 2 i f 4 4 - t *3444 3 ^ 2-11*114 4 4 4 4 ^A\ 4 4 b 4 4 S 4 4 4 4 4 43.4, ^14 -S4 4 £ 4 £ 4 inAs 4 * H 4 4 4 t 4 44.

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- 14 -

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- 15 -

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3 ^ 2-134 ^ 4 4 ^ 1 4 FTIR #*3 4 4 # °)Â^ 4*34 PL spectmm4 £ 4 ^ 4 . 3 ^ 2-l3(aH14 ^ . 4 4 ^ - 4 --g- i g £ <$4-*34 cfêi =3.4 %.&£. o]§}

^ f f l - °142] 4 4 * 3 4 Â3^1b 744 ^ 4 4 - , ri^ 2-13(bH*i ±£°}4*-°l O.lmm 41-21 open 43H-& ^ 4 * 1 4 ^ si f ^ 4 <$x^ pLo] ^ . 4 4 . 4^ - #

<£ 44*3 4 ^ 2 ] ^ W ^ 4 1 - yi°14, *344 1 4 - i £.4*1 ^*H4b 4 ^ 4 open 4 ^ 3 4 4 4 4 4 4 4 ^ 4 PL#*34 £ - 4 € 4 .

1.4 8um H r#0|ej IR S T § S | ^ * l ^ 9 J 4 S ^^ |S |* j ^ £ k ^ 4 41

4 a â

QDIP ^*34*3"4 ^5:471 2]*114^ ^ 4 QD 7-^4 bandgap engineering4 1 ^ , 4 4 . Bandgap engineering 4 35£4 QD 4 4 4 ^ QD4 3711- ZL^1S\7\

4 , QD 5£^ DWELL (dots in a well)43:4 4 4 QD# # 4 4 4 4 # ^ 4 ^*3 i- s > i ^ - 3 ^ 4 4 ^ 4 ^ 4 4 . £- 4 ^ H 1 4 b Wts, 4 3 & b 8 - 12 pm4 **r ^ 4 4 b ^ 4 ^ 4 1 - 4 4 4 DWELL ^ 4 InAs QD-1- 4 b QDIPff- t 4 4 5 1 4 . DWELL ^ # 4 4 t *34 QD4 3 4 s ^ , QD ^ 3 4 ^ - 4 4 4 € 1:^4 ^73 £ S } ^ 0}44- -f-f-4 1=443. ^ ^ ^ - 0 . 5 . 4 <£§}i- 44-35-4 ^ 4 4

4 4 ^ 7 } b 4 4 b 4*34 $14. 3 ^ 2-14b £ 44°fl4 4 4 4 4 5 - 4 7fl?*34 ^ . ^ 4.4-^4-, DWELL 4

3:4 InAs QD4 ALE (atomic layer epitaxy) 4 4 ^ . 5 . Â 4 ^ 3 , 3ôfl4 & b 4 4 4 4 15 MLCmono layer)4 2.5 ML b ^ l 4 In0,i5Ga&ssAs % *H°1] €-4^ : 4 . QDi 4 4 # ^H47l 4 4 4 modulation 5 . ^ 4 4 & 3 , i ^ b ^ b 3xi017

crrf344. °1 DWELL b ^ b 5 ^ 4 4 4 3 4 3 . 4 , 4314*11 Alo.3Gao.7AS/GaAs SL(superlattice)7} 10 ^ 4 4 ^ 4 . 4 ^ InGaAs 4 4 £ 4 & 4 InAs QD4 AFM (atomic force microscope) 4 4 4 4 4 1 4 QD4 ^-4 ^ 4 ^ 11-3 b 4 4 41 nm, 7 nm, 4 * 10i0 cm~244.

3 ^ 2-15b 4 A]af QDIPS 4 4 ^ 10 K, 30 K/44 4 4 ^ 4 4 4 4 ^*3 4 J i4€ -4 . 3 4 4 4 10 K414 #*34 QDIP4 4 4 4 * 3 4 7.6 um 4 5.5 pm1 A\ 4-4- 4 a # J i t l 4 . 7.6 pm 4 ^ 4 4 4 - ^ b 18 meV 4 4 5.5 um4 « } 4 4 4 30 meV 4 3 , 7.6 um4 4 # 4 4 5.5 pm4 ^ # 4 i l 4 7 A 3 4 - 7.6 pm4 4 3 b InAs QD4 4 4 4 ^ 5 - 4 ^ i Ino.15Gao.85As 445L4 B - B (bound to-bound) %

- 17 -

http://Alo.3Gao.7AS/GaAs

http://Ino.15Gao.85As

4*11 4144b 74.0^ 4 4 4 4 . s ^ } ^ -ft- Lii4 4 4 4*Hb 4 4 #EH 4 4 4 *^4 4 4 4 4 * U 4 3 , 4^%) .4-ofl 4-g- £ 4 44f r &4 44*11 B-B 4 4 b 114- 4 4 4 4 ^ 4 1 ^ 4 3 ^ b 4 4 4 1 - ^-4*1 "11444 4441 5.5 um b InAs QD4 4 4 4 ^ 4 ^ GaAs 7d^4 4 4 b 4 # C M B-C 44*11 *11 4 4 4 . DWELL ba^# QDIP°11 144*3 4 S 4 g-44A3 4 4 ^4^1*1 4 4 4 b 4433.}t- 4 4 4 5 1 4 .

1.5 S A-j B| Ojl SIS S 4 § £ | r H?JJ £ £ ^ 0 | § 0|g°_r QDIP ^ g

(1) 44*11 gjfl 44*3 4*244 44*11 4 4 44*321 fc73 >ga

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4 4 ^ 4 4 °!4slb 0.9 torr4 4 4 30 watts] RF 4 4 , 200 °C4 4 4 4 - £ 54*114 S1O2 capping 4 4 300 nm 4 4 ^ 4 4 4 ^ N2 7}3 # 3 p}6\]A] 1 £. 4 650 °C 4 850 °C 7}4 4 4-ojfl £ H 4 H 4^4934-

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$ 4 . 3 ^ ^ A - ] ^.^ 4-4 ^-4 ^ 4 s . 4 PL 4 3 ^ 1287.5 nm4A1 JEL*!4. 650, 700 ^ 750 °C4*i 21444 4^-1:4 4 4 7 nm 4^^1 PL 4 3 4 *J4 4 4 4 PL 4 4 4 4 4 4 44. ir 4 4 4 . 4 4 4 4 PL 4714 ^ 4 4 4 4 ^§A QD b ^ 4 4 ^ 4 1 4 4 4 14^*11 441 i f s . 1 4 4 4 . 800 °C 4 4 4 4 H 4 4 4 4 4 44*11*14 PL *ll44 # £ 1 4 4 800 °C 4 850 PC 4 ^^v PL 437} 4 4 39.4 nm 4 117.7 nmS. e *3 4 4 4 4 4*J t 4 $14. Interdiffusion 4 4 b 2J44 4£*ll 3711 4 4 4 7 | 4 4 4 4 4 b ib^ jo iH 91444 *lS-4 4 €■ *34 4 4 € 4 4 J i 4 b 534 ^ 4 4 ^ ^ 014 800 °C 4 4 4 2144 ^ ^ QD 4 GaAs *34 4 ^ 4 480 °C 4 580 °C 2:4*11 *14 4 4 4 4 4-E4 *3-§-

- 18 -

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n+GaAs350nm(3el8)

GaAs, 50 nm

GaAs, 40 nm

n" GaAs, 3 nm(3e!7)

GaAs (2 nm)

InAs Q D s ^ I%l5Gaog5As 15 ML

In0 ^Ga , 85As 2.5 ML

GaAs, 45 nm

Al0 3Ga0 3As, 2 nm

GaAs, 2 nm

GaAs, 50 nm

n+ GaAs, 650nm(3el8)

S.I (100)GaAs substrate

x5

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3 ^ 2-14. DWELL 4 2 : 4 InAs QD4 5*4 QDIP

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- 20 -

14000

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3 ^ 2-17. As-grown QDIP4 850 °C4*1 4 4 4 I T QDIP4 4 4 4 4*3

- 21 -

6x10*

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10 K 7 Sum 8.3um

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- 22 -

4i 2 *i ^ # ^ t f^*> ^ * i ^m <g

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- 23 -

http://fe-S.tr

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D2 cluster

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solenoid valve

reaction chamber

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- 25 -

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- 27 -

JrLti*

Rotation Stag

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- 28 -

4. ^ 4 4 ^^-8- 4 4 £ 4

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S-KR6

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- 29 -

Vacuum chamber

Probe beam3.5- NdTAG 4 4 4 4 24 ^ 4 4 * *}-§-44. probe beam€- 4 ^ %4 4 4 ^ 4 4 ^ f e # f - 4 4 # 4 3 4 4-^-4 3 ^ 4 4 4 4 4 4 1-43. fe- 4 4 4 4*34-§-# i 4 4 4 4 4 4 # 2 ] pin holeA ^ 4 4 4 4 4 4 4 . # 4 ^ 4 4 E - 1 4 4 * 4 ^ 4 3 . 5 . 4 4 4 %A 4 4 4 4 4 4 4 beam stop# € 4 4 4 . Rayleigh scattering4 4 4 4 7 4 3 . S . 4 4 4 ^-i- ^ 4 3 1 ^ 1 - *}-§-44 A ^4143-5. ^ 4 ^ 4 3 oil- 4714 4 ^ £ - 4 7 4 4*11! l A ^ 3 2 i £ 4 4 4 4 .

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2) Michelson interferometer 4 4 4 4 4 4 ^ # 4

# 4 3 4 4 4 4 4 ^ - £ # # 4 4 ^ 4 4 4 4 4 4 4 £-44 i t - 4 7 %U 4 4 4 4 ^ 5 L # # ^ 4 ^ S 4 # 4 ^ 4 4 ^ £-§-4 € 4 . # 4 ^ 4 1 - ^AA WAA 4 4 D J ^ 4 4 4 ^ 4 4 ^ ^ # 4 ^ 4 ^ _ ^ 4 4 4 4 4 4 4 7 } 4 4 3 , 4 4 4 ^ Michelson interferometer!- *}-g-44 2 4 4 -§-443.5. 4-S-4 7 } ^ 4 4 .

- 30 -

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Michelson interferometer Roof prism

3 ^ 2-28. Michelson interferometer! 7*3

- 31 -

4 4 4 4 A°A beam-§- AAA interferometer - beam 2:^4 4 4 4 3 , sg_g^ 4 ^ £ 44-oil£ -i-^-43 7 beam4 4 4 4 °^lf 4 ^ 4 4 4 4 4 .

4. ^ 7 ^ -1^4 44-i- 4-§-4 ^ 4 4 f ^

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- 32 -

To momtorf ITT to monitor

To oscilloscope

Detectors: He3

CR39 Faraday cup

To monitor

'CCb camera to monitor front surface of target

Top cover of chamber

U s e r beam « made of 800nm,400mJ,30fs , Q c rV' p l a t e

10 Hz, p-polarized

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- 33 -

0 0 -

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time [microsec]

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- 34 -

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^ *W*7M<&*± Ruxm Li D i t m ] r e ^ ^ ^ 4*}%'4 4 4 4 ^44:7H eil44 4-B-4 4 7 4 4 (Laser Fusion Research Center)4 Yuqm Gu ^ 7 ^ 4 11443. 4 4 - 3 ^ 2~35fe 20054 4^ ^ 7 4 4 AS. 44*14*1 71144 4 ^ 4 4 # 4 3 ^ 4 4 Ruxm Li 1277} ^ £ 4 Rayleigh 4 4 4 4 4 4 4 4 4 4 4*1 Li 44fe ^ 7 3 7}^t\\A] ^ 7}+%

- 36 -

4-8-4534. 4 ^ 4 * 1 ^ # 7 £ # 4 7 4 -£- *3^4 §3,34 A&7\± &4*1 7 i ^ - 4 1 - 4 4 3 . 5 4 4 -t-4^-4i* t 4 4 4 3 - Rayleigh 4 4 AÂ 7 ^ 4 $ 4. 4-1-4 4 4 4 AAA 532 nm54 Nd:YAG 4 4 4 4 42 2:444$14.

Rayleigh Scattering and the Cluster Size for H2 Backingpressure >90 bars, > 5 X104 molecules ^lTiim)

0 3 0 6 0 ° 10 20 70 <B SO «0 tO 80 SO TOO Sacking Pressure (bar) oûi,,, *,-«.»*.« p0cb3o

Clustering begins to occur at backing pressure pQ of 5 bars and liquid nitrogen temperature (- 80K).

3 ^ 2-35. Â 4 4 4 4 * 3 ^ 4 ^ ) ^ 7 4 1 Ruxin Li 4 4 ^ 4 AS.A 7 ^ € 4 ^ 4 4 Rayleigh 4 4 4-£

o 4 4 , 2Q05\i 84 4 4 4 4 LFRC1- 4^ -44 i-~rk # 4 ^ 4 4 4 ^ 4 4 3 . 5 #*3*V I ^ M i ^ -^-^-3.5 7*34534. 4 4 4 4 4 4 4 4-§-£ 5. 4 . 4 4 ^ ^ 4 ^ 4 . 4*14 *I4£- 4 4 4 ^ 4 4 ^ 4 4 4 4 4 4 24-1-4 4 t 4 4 #*} 4 t ? - 4 # 4 £ 1 2 *!-§-# #*34-^r -^44 77} &$4 . 4 ^ ^ 4 4 4 4 LFRC4 Zhi Jian .Zheng 5L74 Hongjie Liu 4 4 4 3- 4 7 ^ # 4 ^ 4 4 7 4 4 ^ 7 4 - i : 41-4 4 4533.4, 4*1 & 4 7 ^ 4 47*H34 4 4 4 4 4 4 4 4^- S-ÂiA. 4 ^ 3-1-4 300TW 44*1 447} 4 # 4 ^ 4 4 4 214 2006 1 314 2 i ^ ^ 4 ^ <274# 4 £ * M ^ 4 1 4 4 4 3 4 4 4 4 &34 , ^ 4 14*1fe 41- - £ 4 ^ 4 3€ #7*3 ^-f-43f •§• 7*34524. LFRCT? # 4 4 4 4 4 4-B-^-i- 4 4 4 3 - i 4 4 ^ # 4 4 4 3 5 4 4 4 4 4 4 Ti:Sapphire 4 4 41- 4-§-4fer # 4 4 4 i 4 < £ 7 4 4 4 s 3 4 4 4 4 Nd:Giass44 4 4 4 - 1 *H-4 ^ 44*1 *|-§-tf *27# 7 4 4 3 5134, 4 QAÂ 4 4 4 301)44 ei!4 4 4-§-"t £ 4 4 4 4 4 § 4 ^ - 4 4 44-i- 4 4 #<£ 214 4 ^ 4 ^ # 3 5 4 4 4 4 ^3 .4 , W 41-4 # 4 4 # 4 4 <S7-& -§--^35 4 7 AA 4 4 #

- 37 -

S . 4 4 3 %XA. o 20054 81*3 4 * 3 4 £ 9 J 7 ^ 4 10TW 30fs 300mJ tfAA 4 4 4 4 4 4 * 1

4 4 1 - 4-§ -44 # 7 . - 3 t 4 ^ 4 4 4 3 5 4 4 4 4 * 1 4-§-44 4 4 # 4 4 1 -

4 4 4 4 ^ - A^A 7 4 4 5 3 4 . 1 4 4 4 4 2c#, 4 4 * 1 * 3 ! # 4 4 , # 4 4 5

4-& # 4 4 4 f-i- 4 4 / 7 4 4 4 5 4 3 - 4 4 ^ 4 4 7 ^ ^ ) 4 ^ - i £ 4 ^ 4 # 7

£• # 4 * ^ 4 4 4 4 4 ^ - 1 : 7 ^ 4 ^ 4 . 3 ^ 2-36£ 632.8nm 4 4 4 HeNe^kl

*1# # 7 : 3 € 4 ^ 4 4 ^ 4 4 4 4 4 ^ W 4 4 ^ - i : %<§# 4 - 4 4 4 3 ^

2-37^ f ^ £ 7 ^ 4 4 4 4 4-& 4 4 4 x 4 3 . 4 - t 4 4 4 4 .

. .

3 ^ 2-36. 4-2V4 4 4 4 7 } # 4 ^ 4 4 3 3 4 4 4 Rayleigh 4 4 ^ ■%■ ItAAA JZ#. (Ditmire 4 A} 4 BH014 4 4 OJAVJT}

«l/|)

gasuackinfe pressure (.M pocal)

n%! 2-37. # 7 4 i # 4 - - 3 4 4 HeNe (632.8™^) 4 4 7 ^ 2 : 4 4 4 # 4 4 Rayleigh 4 4 4 3 1 . 4 4 P 4 2 .8^4 4 4 4 ^ 4 3 . 5 4 4 4

o oi Rayleigh 4 4 A J l r # 7 3 4 3 4 4 4 P 4 2 .874 4^14-c- 4 3 5 . 4

4 ^ 3 - 4 Rayleigh 444.517} 4-§-4£- 4 4 - 4 4 # 4 4 4 4 4 - 4-i- 3 4 4 4 532nm 4 4 4 4 4 * 1 5 . # 4 4 4 P 4 3.2#4 4 4 4 f e AA-7} 4 4 , 4-4*1 4 7 4 # 7 Ruxin Li 32-74 4 ^ - 4 4 7 4 * i 4 - t 5 4 ^ 4 . 4 4 * 1 -£- ^ 4 4 4 AAA # 7 3 € 4 3 4 ^ 6.5 MPascal 4*1 4 10,0004 * 3 ^ 4 f ^ £ - 4 5 7 * 3 4 4 4-83% <*)1#4 4, ^ 4

0 4 4 f ^ ^ ^ ^ ^ ^ o i ] 3 0 f s 1 4 r a j ^ £ o | ^ o . ^ 7 | o ] 4 4 4 ^ - 1 - a^*}44

7 4 ^ - 4 # 3 : 4 4 ^ 4 - 7 4 4 U 4 ° i l44 7} 4 i .7m j 4 ^ 4 5 - ^ - 4 4 4 4 4

4 4 4 4 « - § : € - 4 90%4 7\AA 4-1: 4 4 1 7 AxiA o # 7 3 7 } 3 # 4 4 - 1 ^ 5 L 5 4 4 3 4 4 # 6.5 MPascal 5 # 4 ^ ^ # 4 £ 4

4 4 - 1 - 2ms5 3 : 4 4 4 # 7 3 7 } 3 * £ * } 4 ^ 4 300 mj 4 £1144 4 4 4 5

38

44-i : ^ 4 4 $ 4 . 4 4 # 4 4 4 5 ^ ^ 4 4 4 CR-39 plastic track detector, Faraday cup detector, 3 4 3 ^44^-ofl <*]*)].*] 4 71 (Liquid Scintilator)!- -M4 4 ^ 4 . ZL 1 4 ^ ^ 5 - 3 ^ 7 3 1 4 4 4 4x-b 3 ^ 2-384 4 4 4 ^ 4 # 4 4 AAi 4J-.1- J2.47&4. 3 ^ 2-39-b 5.4-533.:% 4 x 1 - £ 4 4 - 145*1 4 4^4714*1 #*3^ #^34 4iL, photodiode4*1 #*34 44*11] A J1, Faraday cup #*344*1 #*34 ° l£* l£# £ 4 ^ 4 . 44*14 4 4 # ^ - u

sv 4

4 4 4 ^ 4 4-&4 IMS 4 3 ^ 4 4 4 4^1-4 7 ¥ 4 4 4 J ? £ 4 DD 4-8-tr 4-1-4 1 H 4 # 4 * k t Ihfltr 4 4 4 *d^44 &AA. £ •£«£. ^4°fl*ife 2 ^ 5 . *3^-t ej|44 ^-g-^- ^ 4 4 A^Mi4£ 4011 4 ^ 4 o.f-4 &4 &

3 ^ 2-38. S/tJ-S^aH^ 4 4 As. ( 4 4 ^ 4 4 4 4 t r #^44-21(4), photo detector 4} 4 4 4°14 4J : (#4), Faraday cup 1 4 4 4£-4i£(4sI)))

- 39 -

12-,

10-

8-

6 -

3 4-| (0

CT) (5 2H

o-

-2---0 5 0 0 0.5

Time [microsecond] 1 o 1.5

^ 2-39. 30fs 300ml Ti:5apphire 44*17} -$i f-S^3Elol| £ 4 4 * H 4 ^4-§ Faraday cup-i 4 4 4 4 4 4 4^12] 3.7

A } - § - 4 4 4 4 ^ 4 * 1 (Liquid scintilator), Photodiode, # 4 4 i ^ s . * 2 2 4^.. (A ]4^ s.41-

legendoll ^ 4 4 314*1 ^ ^ . g . )

- 40 -

2.2 a||o|*( 5i 4§^4" S*1 S§A|^g

7}. # 4 4 f-^-g- 3:^4 5)144 -M4

1) # 4 4 1H-S- 4 4 42:4 3-t-4 314*1 2 4 ^ 4 H# ^-234 3 # ^ 44*11- 4-8-4 #A34 M 474 t - 3 4 # 7 ^ 4 4 ^ 4 3 4

4 4 4 #74:7} 5 4 4 3 4 N « H M 4 4 4 4-^44, 7 4 4 4 4 #fr4 4 4 4 4 4 3zA s 4 4 3.4 ^ 4 4 4 . #74i 4*fl ff*)£ti| 4 4 ^ 4440.5-!:- 4^1 4 4 4 4 4 ^ 4 5Jv74?J ^ 7 } 4*fl Hs*\] ^AA $t% 4*143.5^ 7 4 - 7 4 7H4 # 7 ^ -£-4#4 4 5 # 4 5 ^ # 4 ^ 4 # ^ 4 4 4 3^] 4 4 4 * & * 7}4 4. 4 4 4 # 4 ^ 4 4 4 4 4 4 4 4 444-1- £443-5- ^%#4 44*1rr # 4 3 E-17} 44471 44 4 4 4 4 4447V ^ 4 4 4 4 3 5 44*14 C-^-4 7 ^ fs 5 # 4 4 44, 4 4 4 4 #-£-& 1016 W/cm2 4 ^ 5 4 3 4 ^}s 44. 4 4 4 , 30 fs, 10 TW 4^-4 42-4 3 # 4 444 4 3 ^ AFg-4 - 40] 4 4 4 4 , 4 4^-44*14 *3 - 11 3 4 1 ; 200 um 4S-5 §114 44. 4 4 4 3 5 10 TW4 7.^4 3 #4 44*1 # 4 4 4^^r 50 mm^i 435 , i ^ 7 i 4 12m *3^4 43:5 5flo] *1 « * ^ # # H ^ # £ 4 1 # # £ » 2L§- 7 &4.

44 , 3 4 4 f l W M # 443-5 A}-g-4 ^-f^fe ^ < h ^ 7 } ^0} 4 4 7j-£7} ioJ9 W/cm2 4 4 4 4 4 435 , 10 TW 44*1# AA% *J-r- # # 4 37)7} 10 um 44*} 4 4 4 4 4 . 44*1, 21^44 10 cm 4 4 4 4~A 4441 - *B-44 44, 4-3,4 3-f-^ 4447} g £ oJ44 t H 443.5 7 4 4 4 f 4 4 ^ 4 , 4 7 47} t - f # * l $fe uu}^ 444-1 *}-g-4-ci- 44 4 4 4 4 . 2E#» 44*14 i 44 4 50 mm 4-^5 ^ 4 nfl -oil, -44m 2 ^ 4 4 4 444ri- 2:^44 10 cm *3£-4 off-axis ai-7-i-g-i- *}-8-4TT ^ 4 4444- 4 4 4 72,4 m#^ 314*1 23} ^ # # 3£ 2-14 *344&4.

i t 2-1. # 4 4 # A M 4 4 44*1 ^ 4 ^-4

tit 4^ As 4^r ^ 3 4 ( 1 0 TW

$ # 44*11 (U 4 4 50, mm Zl#)

# 7 ^ 4*1) # 4 ^ 4 4 4 ~ 10lb W/cm2

200 um

2:^7-14 1-2 m 4 $ 2 . ^ £ - 7 4 7-1 #

# 7 4 i # 4 4 H 4 4 4 ~1019 W/cm"

10 um

3,^7}?) 10 cm4 M M *

- 41 -

2) #*34 ^MA 4 4 42:4 3 # ^ 44*1 1 4 H 4 4

# 4 4 44-1: 4 4 4 ^ 4 Jitn 3144^^ ^443 .5 44w 4-444 4^-4 4 4 CPA 4 # i - 4-§-4 4 ^ 4 J L M 44^- 4 4 4 4 4447} 4-8-44. 4 s 4 i - t ^ 4 4 ^ 4 4 4 4 eiH*-!^ 4 ^ 4 i ^ £ S TW4 fe-8- M- i - *S4"t 7 ^ 3 4 , 10 Hz *3534 ^ £ 44-1-5 # 4 7}#44 # 4 4 44 € f 4 3 9 * ^*3 # 7>44. 444 43« j3 3 4 3;2:4 7 # 4 4 , 12:444, 1 3 444 , 44 # #4, 7 # ^ 4 1 * : 4 # 4 # 3 5 7*3€4.

• 42:4 7 # 4 4

7 2 4 3 # 4 44*14 4-8-4-^ 7 # 4 4 ^ #^-44 seed 1 3 5 *}-§-% ^52:4 ei!4*1 12:1- 441^4. 7 # 4 4 4 4 A$A^ 1 ^ 7 4 ^ 4 4 #^-44 A 4 4 4 tcfl -ofl ^ 01144^ 114 fe^ ^^.7} & W 1 ^ 4 ^ # 3 234,52^ y^r 44*1 1 3 1 : «* f l ° r 44. 4 4 4 ^ 4 # AÂA 7 # 4 4 # 4 4 4 4 4 44 44i9- 4 4 4 4 1 4 4 4 4 3 SLH^-3 ? l t ^ 4-§-4 44*1 ^ 4 4 1 - 3 ^ 2-404 44 4445S4. ¥ 44 344-1:4 444 ^£4- t \ 4 44 #34-fc 7 71)4 s 4 # #-5-5 #441 - 7A34A13.4, 4 4 ^ 4 4 4 4 €*3£ 7 3.^4-1- 4 4 4 144$14. 45!1 4 4 4 ^ 7 r 532 nm cw 44*1 (Millennia V, Spectra-Physics) t 7}-§-4ô.4; ^ ^ 1 4 4 4 4 # 4 4 4-^4 Âs £ 4 ^ ^ 4*114 ^ 4 -1-4 o_44-i-^ 2-7 chirped mirror# AAAxiA. ÂS £-4-1- 4423§44 4 4 4 fused silica ^ 4 # A% 77}5 *k§-4$l3.4, 4 ^2: £ 3 ^ 4 4 4 4*34 4 5 ^ 131- AJJ4U- ^ 010 4 k^s) ^ 4 J&±M.% 4 4 4 ^ 4 ^ 4 14 fs$3 4, # 4 4 4 £ 800 nm, AÂ 150 nm 444114. 533#*3 41^4 $ T ^ * ^ # 4 4 # 4 7 4 4 100 MHz4 44-S-5 A M 4 & O J ^ ^ ^ 3 5 W o ^ ^ #

4 £ 350 mW^4. 4 4 4 , ^'52- € 3 4 4 4 4 ^ 3.5 nj 4 A ! 4 .

• 1 3 44714 1 3 447|

^£2,4 42:4 1 ^ 1 4 5 # # t 3-f, # ^ 44*)7} 4 4 ^ ^ 7 # 4 4 ^ 4 4 ^ 4 4 4 4 ^ 4 , fe£ 4 7 M 4 4 4 444 ^ 4 4 4 ^ 3*47} 1 4 4 4 4 #47§-4 4 £ 1 4 1 4 44. 4 4 4 , 4234 l ^ - i # ^ 4 m - # ^ 4 4 1 3

- 42 -

4441- A}-§-44 l2-#-i- ^ £ 4 ^ 4 ^ 7 -t-4-S- ^ 7 4 4 4 4 1 ^ 4 4 4 4 4TT grating^- *}-§-44 5 ^ 4 3 ^ 4 &^M.$ *3 r€- # 4 4 3 . 5 £ 4 4 3 , 4 3 <¥s«8 W 44TT 4 ^ 5 ^ 4 1 - 4 ^ 4 44, 3^JEEJ^4 AI^SLM 1 4 4 1 4 ^ 4 47 4<>14. 4 4 4 4 4 ^ 4 4 4 1 ^ 4441- 3 ^ 2 414 444x14 1 3 4 4 4 ^ 1200 1/mm grating, 2 :444 30 cm4 3^-4-§- 2 :444 15 cm4 # ^ 4 #3 .5 7442134, Ofmer-triplet 44-1: 4-8-44 7 4 € 4^44x14 . A 4 4 4 4 4 12.^-^ 250 ps 444x14.

^-2:4 7#47H14 | A | ^ } ^ ^ 4 l ^ fe s.H^-44 ^rAA # 4 4 4 4 7 4 4 100 MH24 4 4 ^ 5 A J X ^ 4 ^ 4 4 #s-4?lfe #^-4 *g*8 44*14 4 ^ - i - 4 10 Hz43 .5 , 3HV4-i :5 A | 4 4 ^ - ^ ^ $}O}T\ J g ^ ^6)}A) | | f o f ] ^o^

1341- 4 4 4 4 44. 4 4 4 l2 t 44-2r 4 4 4 .£712: 4 4 ^ 4 £-1bl# 4-8-4 ^ 4441 - 4 4 4 i l 4 . 2.4^ -i 4, * s . j@#3-*M# 4 5 7 4 4 4 1 4 4 4 i -43 44 ^ 4 4 4 ?^3.^ J2.€- 4 4 4 I21M-4 4 4 4 ^ 43, 4 4 7 4 4 4 12:7} f-44-^ $ 4 4 4 573*1-3 ^ofl 4 4 i - 4.7}44 4 4 4 133} #44:534 4534. # 4 4 4 4 4 1^4 £4-^ P 4 4 4 S|£* 4x134, 13- 7-S-i-^ 5000:1 444514.

- 43 -

Concave mirror

44 ##4^ 7#444*1 444 nj 444 444 1 -t 7 mj *3 5 #^ n 7 - 41-&- 44 ofl-g-4, 44*1 4 -4 44444 44444. 44 14 ^£ 4^1- ^4 444 44^ 4444 1 3 44-415 44 4##4 f ^ i t 14 4x14. 2 : ^ 4 4 50 cm 344- i : 242} ^ ^ 4 4 45 cm £.A~AA 2 4 1 # 2 : ^ 3 5 4 4 4 3 3 ^ 4 4 4 4^-4|L§- AAAA°-^, ^ 4 4 ^7,7} ^ g# 4^114^- f. AAs^r 4x14. 1 ^ 4 4 4 5 ^ Q 3 4 4 4 NdYAG 4 4 4 4 24544-1: 4-8-4 $1.3.4, # ^ 4 4 4 f e -50 mJ45l4. 1 ^ D a.4fe 4 ^ - 4 1 4 4 4 4 -1.5 mm *3£^ 4 4 l^ 1 fluence7} 4 3 J/cnM 4 ^ 4 x 1 4 . # ^ - 4 4 4 7 4 4 mj4 9134. AA 4^-4 4 4 gain narrowing 5l4 4^-4 # # -¥- -3*]5%) # 4 3%i 2-424 4 4 &4 # 4 4 7AA 444x14.

_ 44 -

=LJ& 2-42. 4 4 #^-44*1 # ^ 4 4 4 4 I 2 i 4 *M:MJ

O i \-L

7 #-^ti-a- 4 4 # 4 4 4 * 1 # # £ 7 mj4 4 4 4 13-1- 4 4 ^ 4TT # 4 4 fe 4 4 # t>4. 5 f - 44*1 1 ^ 4 4^-44-8: 44 4 4 5 4-44B 4 7 4 7 ^ 4 4, ^^7-¥i-4i : 4-8-44 7 4 * 4 . ^ 4 4 4 5 ^ 4 4 # 4 4 4 44*}*15 Q^ 4 4 4 Nd.TAG 4 4 4 4 2 4 ^ 4 4 1 4-8-44, # 1-D 4 4 4 ^ -1.4 J44. 4 4 # 4 4 4 4 # 4 4 7 mJ4 4 4 4 12 -1 s . 4 4 3 5 # 4 4 4 4'44 244 # # 4 -1 4-8-44 4 4 , 0.2 J, 1.2 J4 1 ^ 4 4 4 1 - £ 4 4 4 4-8-44. 4 # # 4 4 4 4 fe 500 mj 4 4 4 4 .

42. 4 4 4

12: 9j-^4fe- 1 3 4444*1 4 4 € 44*1 1 3 1 #-^ ^41 4 4 4 1 3 4 4 7>44 4 ^ 4 4 4 # 4 3 5 TW4 ^A ^ 7 #4-1- 4A34^f 4 4 4 4 . 1.3 4 4 4 4 4 4 4 4 4 4 tifl!4 3*)5^-§: 4 4 grating^ *}^-44 # 4 4 3 . 5 £ 4 4 3 ^ s t 1 4 4 7, 4 4 t 4 * 1 SL-& £ * £ . « ^.g-oi f - t j ^ . 44^ ] #4453%f 4 3 5 4 12:4-1: 4efl4 1^4<1 7 k M 4 # t 7 x l 4 3 ^ 2 434 1 4 7 4 4 1200 1/rnm grating-8: *}-§-44 7*344, 4 4 4 grating-8: linear stage4 1 4 4 4

- 45 -

grating*}44 441- 2:14 7 44 43.54, #4 1^4# 4444 7 $14. 1 3 4#7|1- f-44 44*1 I24r I-¥ #44 TW -35 ^4 4£4 444 ^1 44*§ H41- 4444 444 4##4*1 4-8-44 44 4£4 44 13 4#4i 4# ^444 1444.

1) 4-2,4 3#4 444 #4 2^2^ £4

o 42:4 3f-4 444^ 4# 1^44 -OT-i- 1*347 4144 -3337 44 4 f-4, #474E 12.41: 4£4€ 7 4fe ££ 2453 -g- 444-b 44 #3.4 4 £ 474 42:4 3i#4 444^ nj 444 AA 4444 ei)44 131 7 4 mj 443-5 #444 44, 108 44-4 ^£ #4## 3744 444 ^A # 4 §~8: 7444 44*1, 106 444 ¥zA #4#-fr *r47 44#444 244 7# 445 #44-1- 7*34x14.

- 46 -

o 3 ^ 2-44^ 4 4 4 #4*144 # 4 4 3^E^.g- 4 ^ 4 7^444. ZL^°\\ 4 4 4 4 4 £ 4 #-^-7Hl <^4-b 213)51-^ 150 nm *3£2] ^ 2 ^ ] E ^ IL.P- 7} 444:, 14 # 4 4 (44 # 4 4 ) 4 ^ 4 2 . 4 ^ 4 4 ^ 4 4 ^-4-txl4. 44-& £ £ # 4 ^ 7}4^ 4 4 # 4 4 4 4*33.5, gain narrowing 44°) *ov44 1 4 1 4 4^-44. 77}44 24, 34 # 4 4 4 * 1 ^ #4-1:4 fe*l 8 5 « 1 (10-20 4) i ^ E ^ j ^ 7j-^ 4 4 0 . i g s 4 4 4 4 2^0.4 4^- ^ 4 4AV01 4ri)4A5 4 4 4, #42.^1 E&!4 4 4 4 ^0.5. 4 # 4 ^ #■§■ 1 7 4 4 . Gain narrowing4 4 4 £ 4 SHHls. 1-743, 4 # # 4 4 2.4^^3.5^-4 <£-§- 7 517 41-4 4 3 4 4 4 4 1.344- 2} 20 fs§14. ° I44 # 4 ^AA 3 4 4 4 Frantz-Nodvic #^-£^-S- ^ 4 4 4 4^444^8- 1-44 3 ^ 2-454 1 4 -e-443-5 4 '€ f 7 51x14

700 800 900 Wavelength (nm)

3 ^ 244. ^2\4 3t4 44*14 4 #444*1 # 4 4 343sr3.

47

1 .o r l nPy t spectrum^ 1st amp (4 mJ) 2nd amp (55imJ)

0.8 r- 3 r d a mP (78^ m J )

% 0.6

04

02

0.0 700 800

Wavelength (nm) 900

T! 2-45. 4234 ^ - ^ 44*14 1:44*14 14-

3 ^ 5 1 ! 1 4 4 4

2) 72:4 3 t -4 44*1 4 # 1 ^ 4 € 4

o 42.4 3 . M 4444*1 1 3 4 # 4 4 ^ 4 4 # ^ s - | - ^ 4 4 4 4 4 4 4 fi 1 3 4^-4441- 4-8-4x14 4 1 1 3 4 4 4 4 4 4 * 1 ^ 3 ^ 2-464 1 4 1 3 l i t 4 # ^ 1 4 5 ^ 5 4 7 4 l-£ 1 4 4 ^ L l * 4 4 4 4 7, 4 4 24 2:44 14-8- 4 1 ^ 1 4 4 4 4 4 4 . 4 4, 7 l 2 3 t 4 5 4^1-44 ^ A } 4 4 a.^4 1 4 1 3 4 44-1- 7}545-& 4 4 4 7 1 3 4 4 4 4 4 4

7- •714 4 wJ 3.71 -S- ^

4 3 4 4x13, ^ 4 4 - i ; ^ 2-7 ^ -2^4 41 - 4-8-4x134, 4 4 ^ 1*3°.5-

4 4 4 H 4 44 . 44*1, 4 4 4 4 4 4 1 4 4 T T 1 £ 4 3T}| 4 3 ^ ^ 4 4 * }44 4 4 4 4 4 4 4 4 4 4 4 ^ 1 - A% 7 $14. 4 4 4 4 4 4 AA £ 1 4 ^ 7 4 I mm4 AA 1 4 4 5 4 7 4 4 ^As. £AA

7 4 0.1 mm4 BBOl 4-8-4x14. o .3^ 2-47^ 4 1 1 3 4 4 4 4 4 - 1 4-8-44 # 4 1 : 4 # 44*1 134° !4 .

12- 4#7l4 grating 4^.4 grating 4 4 4 4 4 #-|- 2:144 34 ^ 4 4 £ 44*1 ^-44x13.4, #*31 44*3-44s544 4 4 4 21144 ^ 3 4 ^ 27 fs 4$14. 1 3 4 # 4 4 A - I 533-4 7 &fe 44 4 4 4 3 4 7 4 1 ^-4 4^-4,

- 48 -

-Z^ 2-444 4 # # 4 2 ^ ^ 3 2 i ^ E l <£-g: ^ o j - g ^ ^ ^ ^ ^ ^ 4 20 fs 5.4 1 4 1 3 4 4 1 4 #*34xl4. 5E4, 7}^ i444s.4 7>444^-5 4s . 3 4 5 - 4 ^ ^ 4 4 An 4#*3f-4 444-1 : 1 7 $14. 4 4 4 3 4 S 4 4-S-4-I: 4 4 4 4 4 4 4 f e # # 4 4 4 4 2 : 1 4 1 - A}-g-si}4 4 4 .

Laser pulse

3 f 2-46. 4 # 1 ^ 4 ^-44 4-oL^l 4 1 12: 4*114 :44 AA

S.

1 0 -

0 8 -

0 6 -

0 4 -

0 2 -

0 0 -150 -100 -50 0 50

Delay (fs) 1 0 0 150

3 ^ 247. I 2 i i # 4 # f - 4 1 ; 51144 ^ 4 4 4 * 3 - 4 ! 3 L

- 49 -

U- .4 44*14 414*31: 4 4 4-S- 4 4 4

4^4-i-# Af-g-4 4-g.^44#^ 44*14 4141-1- 5445.54 4 4 !#£# 44*14 77 41-1- 14. 7 TW 4^4 42-4 44*1* 4-8-f ^7 44 44fe Ji# 10W W/cm2 4 E t t 7 44 t-434 441- 4-8-44 #*341 1441 4fe 4#444#^ 4#44 #*}£. 444, 34 444 4 ll- 4-8-1 47 10J8W/cm2 444 447} 444 435 4 <1747 4#44 4#1 4-8-44 14 !#£.§- 44 44fe 44 1-2-44. 444 12_4 345-44-1- 444 47H 4#44 43^4 4 -§- 1443, 444 #-& 444 4 4 444 44 134#1- 144$14

1) 4 4 44533 4 3 ^ 7fl 711

41 144 44*1 1 4154-8- 4#44 43^-8: 3 l 2-484 1° 7444. 44 423,*£ 41#4 444 415-41- 44 4^4-g-4 3.44 5 444 343 44# 1445_ 7444. 1- 1744fe 414*3 AA^Z Shack-Hartmann 441 4-8-43, 4151 441 1*341€- 4# PZT 44* 5 7#4fe 4^4^-1- 7} MiUn

-8-44. 4 1 £ 4 4 ^ 4 j — 431 4 4 1 - 4 4 1 4 4 -b l»l«te°™f* 3f}4^ iv-3-4 PCI- 4-8-4x14. H34 4 # 4 7}4 4 5 4 4 * AJA146.S. 41

4 1 7 $itr 4 4 5 1 3 4 # 3 5 4 4 4 s ^ 3 ^ 1- 4144 144 4 4 4 444 47}574 411-

larls Harfmann itoafitsisor

DMDriver

Lnser Bcvin Onf

4 4 4 3 533*1"^ AAA ^ 2_48 3 ^ ^ - a . 3*). ^ s aj -451-7114 -?^ 4 1 5 4 1 - 1 4 4 4 . 3 4 3 4^71-1-4 1 ^ 4 7 (influence function) 7 4 3 4 4 4 ^ - 4 4 # 4*144 4 4 4 4 4 4 Fizeau 4 1 4 1 - 11144 4 4 7 4 4 4 .

- 50 -

2) -4^4*3 4 4 7\ ui-

4 4 4 4 4 4 ^ ^ ^ 4 ^ - 4 ^-4 4 4 4 4 4 4 4 4 1 4 5 1 4 1 4 4 3 . 5 7 f 4 7 r 4 4 4 4 4 4 # J & 4 743 .^44 . 4 4 4 7*34 441-41-4 1 4 35 , 1 4 4 5 4 4 4 T T 4 4 4 4 7 1 4 4 4 4 4 3 4 3 £ = e * « H l 7 4 4 4 44-8- 1 4 4 #3.5 4 ^ 4 1 4 . 4 4 4 1 4 4 7 4 4 4 l 3 4 # 4 4 4 4 4 1 1 1 : 4 7 4 4 4 4 1 4 A^ 4 4 4 3 , 3 4 4 4 ^ s . 1 4 1 44011 4 4 4 4 ^ 4 .

M. 44O] ]A^ Shack-Hartmann 4 4 4 4 ^ ^ 4 4 # 7H144 44*1 4 4 ^ 4 4*34551-^4, 44^1 4 4 4 4 4 31=3#4 4 1 5 4^-41 4 1 4 3 4 2 4 1 4 ! # € 4 1 CCD 4 4 4 3 4 3 41-S-4 $3-3441- £ 4 4 4 4 4 ^-445 7 1 4 4 $14. 4 1 4 ^ 4 4 ^ 4 4 l l l i t - I r ^ 4 7 1 447} ^ 4 4 4 4 4 p445_ 4 4 4 4 4 1 4 l 3 4 # 3 . 5 4 1 4 3 a * ^ - i t 7 4 $1 $14. Shack-Hartmann 4 1 4 1 4 4 4 4 4 !-£ 4 4 4 ^-^^ÂA 4 4 4 14 .

4 1 4 4 1 7 4 4 4 4 4 4 4 4 1 4 1^:4 1 4 3 5 4-744 1 4 ~ 4 4 4 , 4 1 4 4 3 4 1 4 4 1 4 4 3-14 $ 4 7}44 4 4 4 7 H34 4 1 4 4*1 1 4 4 &4 *}44 4 4 . 1 1 1 4 44 4 1 4 Shack-Hartmann 4 1 4 1 445. $J*}44 4 4 te^5 7 1 4 4 1 4 2 , 1 # 4 4 1 4 4 7 ^ 4 ! 1 4 3 5 4 4 4 4 43 , 4 4 €2:4 ^ H ^ H 4^0} ^ o f l tfl4 45-I- 4 1 1 77 r $14.

44*1 14 1 4 4 4 4 1 4 a - l f - 44 ^ 4 1 7 4 4 4 4 Hartmann ^ 4 1 4 * ^ 4 4 4 4 4 4 7 2 i l l 1 4 1 4 4 4 4 4 fei afl-1 4 A§ 4*11 5.7}. z i f 2-497 4 4 &a# - f 4 4 «]oi 44^4-ofl 4-^ 3 ^ 4 4^-4 ^r 1 4 # s.444$14. 4 1 7 4 4 1 4 1 4 # 1 4 4 4 4 42,4 #435544 4 4 4 4 4*Js A -g- 4?-414 4 ^ 4 1 4 1 7 $14. 4 1 7 4 1 4 1 4 7} 44*1 4 *34444 4 4 1 73441, 7 4 4 4 4 4 4 4 4#4<3 4°k°l 1 5 4 4*3 s.4 #444*1 ^ 1 4 4 4 4 11- 444*1 4 4 4 4*3 3 4 3 4 4 =1^4 2:114*1 # 4 1 4 4 4 4 4 1 4 4 412] 74-1 7-ilH 77} $14. ^44) 4 ^ 4 ^ 4 4-t-44(Tilt) $143 7}441, ^ 4 443.54 2.14 4 4 15-4 ^= / (P f /4 )442 i 1 7 $14. 4 1 , 44*14 4 4 4 4 4 1 4 1 4 4 Â\ 411 -44 s£3 l ^ / f l ^ i ; ^ 4 4 4 4 ^.3ôflA^4 ^t f l^sfe Airy 44-4

- 51 -

#14 4 4 1 144

Wavefront

Single Subaperture

Focal length

-► z

-L$ 2-49. 1 4 *l!2o)i4 4 ^ 4 ^ . 4 4 4 4 1 4 ^

Spot deviation

44414 R= Wd(x2 + y2)[/2/f°}A. 1 4 4-1-44 4 1 4 4 4 4 4 4 sxA 14*14 1 4 1 4 4 4 1 4 Axfe 4 21 1 4 4 4 € 4 .

r — ^ ~ ^ r _ A* . W

/ / " rf (2)

444*1 xrA xa^ 4 ^ 4 4 4 4 # 4 1 4 °$AAA 4 4 4 4 4 SJ-3-&4 44-

14 . y 4 4 ^ 3 . 5 £ 1 4 4^3 .5 7 1 7 $14.

3) 4 4 5 415*3 1 3 4

- 52 -

7 4 4 4 4 4 4 4 1 4 4 4 4 44*1 ^ 4 4 4 4 4*343 5*344 1 ^ 4 A7i^\ 445(closed-loop) 443.5 1 4 4 5*344 44. 4&H 5*3 1 3 4 # ^ 4^-4 7^4.

Shack-Hartmann 4 1 4 ^ A*)^&\ 4 # 4 4--- 414*1 1 4 o jx j -^ 4 4 *3S.# 4 4 4 4 , 4 1 4 ^ 4 4 4 1 ^ 1 4 ^ 1 3 4 4 4 4 4 4 1 4 7 45L44 4 4 4 3 , 2344 4 4 4 4 1 4 1 4 1 4 4 4 4 cg*ov14 4 4 1 4 # 4 1 4 3 1 4 5 4 4 4 442344 4 4 4 4 4 4 4 1 H 4 .

415*34 4*34 4 1 4 4 4 4 *3554e1 4 4 4 4 1 4 4 4 1 4 4 7 *34s 4^-1 4 1 4 44 ^ f 4 4 4 ^ 4 4 7 1 - 4 4 4 4 5*3 *331 4 4 4 ^-, 4 1 4 5*3^-4 4s1 4^-1 4 1 4 4 4 f 43.5 # f 4-g-4 4 4 1 4 1 1 4 l 7 } 4 ^ 443-5 4 7 4 4 4 . 4 4 5 4 1 5.*34*1fe 4 4^-g- 4 4 4 4 4 4 4 ! * J 4 4 4 4 4 3 ^ 2-504 5 4 7AA 1 4 4 4 4 4 1 4 4 1 4 3 5*3 *3s-l 4 1 4 4 £ f 44-4 7 4 4 4 5*34 4 1 4 1 4 4 4 1 4 4 4 4 4 I 4 4 0 . 5 I f 4 *3^3# 4 4 4 4 .

4 4 4 4 1 4 5*344 4*114 Shack-Hartmann A^*2 AAA 4 1 5 *3 4 4 1 4 # PZT ^ f 4 4 4 4 4 4 4 - i S-H ^ I J ^ l 4 4 4 7 4 4 4 1 3 4 4 4 13.44. I f 4 4 4 7 1 4 4 4 4 4 414*3 4 4 4 ^ 4 1 4 4 4 4 1443.5 4 4 4 4 4 4 4 144*1 &44 . ^ f 4 4 4 $344 4 4 1 4 I f 4x14 4 7 1 4 4€- 44*14^ I f l<2_j£. <§ .£ ^4711 4 4 4 , 4 4 I f 4 4 4 $§^47 7 4 5 4 4 *351 1 ^ 4

414*3 441 Shack-Hartmann 14*34 44 4 -§-7) ^5544 ^f 4 44 4 41 444-t 744 7 $1^4 44 4444 414 44 13444 1-9.44. 1443.5 444441- 4444 4^4 H41 44444- s.r.445 44 7 $14. 44444 414 23415 474 41.5*3 444 7} 4#^x}

- 53 -

444 4 4 4 4 I J c l 1444 4 4 4 4 4 ^ 4 3 , 5371144 414 *35M-Zernike 42744 1 4 1*34 4*1471:21 I f 4 3 5 £ 4 4 4 4 JE-Hofl 4 4 4 4 4413-5- 1^44 14 4 1 4 4 4 4 4 4 ^ 4 4 . 4 174*14 44 44 ! 3 l # 4 4 4 4 3 , 41*351- 4 4 4 4 4 1 4 1 4 5*344 1-14 4 44$14

41*351- 4444 4 1 4 1 4 5*344 ^ 4 4 4 1 4 7 4 4 4*34 4 4*1 ms. 444 4 1 4 5*344 4144 . 4-§-44 I f 4 444<>11 17>44 114 4444 f *3°1 1 4 1 I f 4 4 4 I f 4^-3.544 4 4 1 7 $14. 4 (3)4 4444 ! * } 4 4 1 1 K2-4 4 4 I f 4 4 414 444*35 s(x,y)«H 4 4 444 44.

N s(x,y) = 2 VtB,{x,y) (3)

2 = 1

4 4 4 4 4 NA 4 4 4 4 71171- 4 4 4 4 . 4 4 4 4 4 1 4 4 7 £ 4 4 4 ^ 4 4 4 4 4 1 4 4 4 4 4 7}4 ^ 3 4 5144. 4 174*14 4 4 4 4 1*34 1 1 4 !7}4 4 4-1-44 I f 4 4 4 *351 Shack-Hartmann 414*3 4 4 5 4 *344 444*351- 4 4 4 4 44 PZT 4 4 4 4 4 4 444*35.574 I f 444 A^% 4 4 4 4 44-414471- f l 5 714$14. 7*34 4 4 4 1 4 47 ^ I S ^ - B ] 4 34 ^114443.5. 4 4 4 1 4 4 4 1°1 4£ ^ o l

=1 r A*. 4.

fs"A s\

b 120

v^W

/

V

BJ Bf Bf 4

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£ * £ » _ ^ 2 0

7>!M20 D^20

• ' B% ' \ \

r>s*!20 -°37

(4)

V^ 3 7 7

1 4 4 Shack-Hartmann $ * H 4 4 ojxov^o| ^ - 1207115 4xl3, 4 4 4 4 4 4 *354 x - 4 4 4 y - 4 4 4 4 4 4 120443.5 1 7 24047} 4 4 . S 4 PZT I f 4-S-4 4 4 4 4 7 4 37 4 1 5 4 ^ 4 . 44*1 B *J^4 27)^ 240x37 4 4 4 .

s^BV 4 4 1 4 1 4 4*344 14 444*35544 41.5*34 4 4 1 1 4 4444 4 4 4 4 4 44 4-§-414474 44 4 f l 4 1-2-44. 3 4 4 4-§-4<344 7 4 1 BA 4 4 1 4 4 4 3 4 4 # 4 4 4 4 4 I E . 5 4 4 4 ^ 1 B+ 4 4 1 4

- 54 -

4 444514. 4 4 £ 4 4 4 ^ ^ 4 7 ^ 1 4 4 4 4 * 1 1 ^

XI

4 <

1 5-o

4 4 4 44 4 4 4 1 4 4 # 7 14 .

V=B+s

V(Nx l)=B+(NxM)s(M* 1) (5) 5574 ^ f 4 4 4 4 447H1 l 7 r 4 4 4 44-§- 4 4 4 4 4 4 4 4 1 4

4 4 4 4 1 4 4 4 4 1*142.5 4 1 4 5*344 44 . 4 4 4 1 1 4 4 1 4 44*114 414*3 -> 4144— 415*34 4 4 4 I f 4 4 4 4 4 4 47} 1 1 4 1 -» >af 4 4 447m 4 4 47} — 4 ^ 5*3 — 414*3> 4 4 4 4 4 4 1 4 5*341*1 7*144 44 . 3 ^ 2-514 42:4 4 4 4 ^ 4 3 4 4 4 4 4 4J44 ^ 4 ^ 5 415*3 423*4 1 4 4 415*3 * H 1 3 4 4 4 4 ^ 4 4 .

C

3 1 2-51. 4 1 4 4 4 1 % 51^4 4 4 ^ 5 . 3 ^ 4 4 * 1 ^

- 55 -

4. 4 1 4 4 5*34 4 4 44*1 1 1 4 S 4 4 4

o 314414 4 4 ^ 4 4 ^ 1 3 1 4 ^ 1 4-f-*l 4 4 4 . 44*1 3 1 4 4 4 4 4 44*14 3144^4 4 1 4 4 4 ^ n AAA 4 4 4 , 4 1 7 4 4 4 44 4 1 4 44*^011 4 # 14^141 3 ^ 2-524 1 4 1 1 1 7*344 4^15-(open-!oop)5 5*343 1 4 5 . 1 4*344 144- 7%4$14. 1 4 1 1 44*11 He-Ne 44*114 415*3 4 4 1 4 # I f 444*1 1 4 4 1 4 I f 4 4 4 4 4 4 4-^ 4 4 4 1 4 14*3521 4*344 l f 4 4 4 1 1 4 4 4 ^ ^A$ S-A 4-^-4x14. 1 4 1 1 eil44«J4 1 4 3.4fe 7 - 7 1 um l £ 5 . 1 4 CCD 4 4 4 4 ^4 3.7]^ e i 4 P - 5 4 1 4 1 4 4 4 4 1 4 . 4 4 4 4 144*14 1 4 4 44*1a*4 4 4 745*34 1 4 4 4 1 €^(x!0 4 4 4 2 ) # A}-§-44

4 4 4 4 CCD 4 1 4 4 4 DH£4 4 4 414x14. 3 ^ 2-534 4 1 4 4 4 ^ 4 4 ( 4 1 4 4 &-: 2.2 44)4 4 4 4 1 4 1 4 *35i43, 3 ^ 2-544 4 1 4 4 4 4 4 $14 a|(4144 &: 0.25 4 4 ) 1 1 1 4 5 , 4 1 4 4 4 4 4 44*1*J4 14527} 3 4 1 4 1 4 1 7 $14.

- 56 -

4 . #*34 7fl4 4

l) # 1 4 4 4 4 4 1 4 7H4

44*1 4 4 4 4 *|*H 1 ^ 4 4 1*} 3=t- 44 l3-5 fe # ^ 4 , 47}, 4 4 4 , 4 4 1 , X - l , AAiA, # 1 4 4 4 $14- 4 4 4 423=4 $]*}44 4*34(yield), 44*1 4£ , 44?- 4 4 4*344 44*14 44 ±144 1 4 4 133)4*1 A5L 1- 4 4 ^ 5 444-1 7*3444 14 . #*3*>! 444-4 44*14 4 4 4 4 4 *J 1(T0F)4 4 4 4 4 4 - i 1 4 7 $14 42:44 7 1 4 4 4 44 , 4 5 4-& 4234 4 4 4 4 7 4 4 4 4*11*14 3 ^ 2-554 1 4 # 1 4 , 4 1 1 4 , 14 , X~ *d * J # 4 i 4 4 t r 4 . 4 4 4 4 1 4 $14 W?lfe 4 5 4 4 4 4 4 1 4 4

^AJ o.fri^ ci-g-4 4 4 . # 1 4 1 4 4 5 ^ - 4 4

Neutron TCF

Electron TOP

444(BC501), 4*34 ~% #0, 4 144 54 4434 1 44 (NE102A), 1 4 4 414 1 # 7]Jfe I - 4 3 4 4 4 4 (NE102A), X-*i 1 4 4 5 4 4 4 4 1 4 4 1 BaF,7} 4 4 4 4 .

4 4 4 4 4 4 1 4*3 4 5 7 1 4 4*34 4 4 4 ^ (TOF)l gstS^- 44*1 £ 1 1(E-AE)4 4 4 1 1232-47 41(PSD)14 4 4 4 4 4 4

3 ^ 2-55. 44*1444 1 A § 4 ^ 4 0 ^ oj7x 444^ -5 # 1 1 1 4 4 4 1 414 4 ^ 7^s. 14 , 41°d*l-4 1 4 1 7 4 4

7 f 1 4 . # 4 4 1 4 4 TOF4 PSD^4, 4*34, # 4 4 1 # 4 T0F2} E-AE14, 1 4 , 4 1 4 4 4 4 TOF4 E-AE^4,343 X-14 1 4 1 1 # 4 TOF, PSD H I o. ~q XL 3444 4*344

2) #14, 414, 14, 414, #44 4-41344 ^ 4445 4441

- 57 -

4444 44 144 34444 4414 HT|| 144 41144 #1 144 44 4^4 4*144*3135 741 7 14. 4f44414^14*14 1^4 7}43 $14 144 *>4 4-£5 4*34 7 giAH.5 444 14*} 74 14. 714 144*1 4444114 4441 44 344 414 ^44 44 4 414 543.5 4144 44*14 #4441 24143.5 444*344 7 *341 #44, 444 444, 14*1 7144.

#44, 4*34, 14, 114, #44 4413444 zi% 2-564 14.

31 2-56. #*3*l 44,1*1414, #44 441344

4144 144 414 1^4 441: 7M-H.5. 714 4*1 &34 44 44 17 lf-4 4W-4 4^ 444 fi-sL -11 4 4411 511 keV 4414 4#44. AfA'e 4*34 4414 4*1441- 4141 144 14*} 1414 4441*1 1 7 $14 44 441444 14 4144 #141 7144^ 4 ^4. 4*14 444 4114 44 4444 414 714414. 444 #41

- 58 -

4 1 # 1 4 4 X14 4S

M 4 4 4 4 4 1 4 441444*1 4 4 4 4 1 7114 4 5 444*1 54 44441 4 4 4 4 4 1 l 2 i 4 f 1 1 ^ 4 4444 #*34 4 X14 7444 .

1 4 4 3 . 5 TOF, E-AE, PSD 4^-§- 44471 4*1144 4 4 4 14431 7 4 4 1-&44. 3 ^ 2-574 4 4 4 7 1 1 4 4 s l 5 J £ 4 4 . 4-444 4*344 4 4 4 1 X 4 # 4 4 3 . 5 14l5.#44(PreAmplifer)4 7 1 X#44(Amplifier) -1 4 4 4 # 1 x 4 4 1 - 1 7 1 4 CAMAC 4 4 VME 4 ^ 4 ADC-& 4 4 * i 4 1 x s . 71^-44.

444 144*1 ^ 4 4 ^ 444 735^ 314*1^4 £44 1 4 4 4 1 S.^: 440.5.4JZ 7fl^44*1 £ 4 4 ^ 4J1I- CFD-E-1:4 4*fl*1 4€- 1 4 4 I x t - 1*^44 7 21.2.44 4 4 4 4 CAMAC 4 4 VME 423^4 TDC-t 4 4 I I I 2 1 5 71^.^4. 4 4 4 4 4 1 1 x 4 4 4 4 4 4 4 4 4 2 3 1 4 4 44*1 DELAY 51-4 4 4 4 4 4 4 4 #23144 . 314*1 1 x 4 GDG5^4 44*1 CAMAC 4 4 VME 4 * i ^ 4 Gate 1 x 1 Logic 1 x 1 - 1^*14 4 4 4 4 .

Laser B earn Trigg\

Neutron Scintillator *<—* W I I 1 H I 1 UdtAM* 1

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PreAmp Amp

PreAmp

Xrray Scintillator

\ PreAmp i

High Energy Charge Particle

" PreAmp "

Electron

Positron Scintillator

" PreAmp '

DLA

' CFD

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*,CFD

Amp

CFD

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CFD

Tin \J \D

PSD

Delay

Delay

Delay

Delay

Delay

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Delay

Delay

Time

Energy

Time

Time

Energy

Time

■j Energy

Time

■, Energy

1 Time 1

0

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171 <"" C

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- 59 -

3 ^ 2-584 42, 4 4 1 TOF4 PSD 4 4 4 # 4 4 1 1 Cf-2525 7*444 4 1 4 4 . I f 4 4 4 4 2142} 5 1 4 1 BC501 4 4 4 4 4 4 4 4 241 4 4 4$t4. 2144 4 4 1 x 1 - # 3 5144 *341x-i- # 4 , 514 l f - 4 4 4 4 #*34*f 1 4 4 4x14. 3%' 2-59444 44234 #147} 44<H] 4 4 4 y]-^ 4 4 4 443.5 7 4 4 4 4 4 4 4 4 x 4 f 1 1 1 4 4 4 4 4 #*341 1 1 4 4 4 ^ 4 4 4 4 4 4 4 4 5 4 1 4 4 1 4 1 141- 5.473 $14. 4 4 1 4 2

MeVl 3J-S3544 I f 4 1 Fission i ^ H ^ t 5 .4714.

4) #*34 4 # 4 ^ 4 1 *3^ x\q

# 1 4 4 44*1 4 ^ 4 4 *344 4 1 4 4 44*14 4 4 4 4 4 TOF 4 *3 *l*3f 4 ^ 7 4 3 5 J2-744, 4 4 4 ^ 4 1 4 41437} 4 *J444 He-3 4 4 4 7 4 4 4 4 4 1 4 4 4 7}#44. 4 ?3444 TOF, coincidence 4 5 4 4 4 4 14457} ^ 3 4 %v335 4^.4 4 4 4 4 ^^^ 7 $14. 4 4 4 ^ 4 4 * i #44 4 4 4 i8.3MeV5 7}44 4*34 1 4 Li i t4 4 $J444 # 1 4 1

- 60 -

4 4 ^ £ £ 4 %.%x\7} ^ iU' -S. , 4 f f ^ 4 4 4 4 4 4 4 Li foil4 4 4 4 *344 444*1 &4 3-f 3. 4 7 4 #(H4 4 4 € f 4 7 f 4x14. Li foi!4 A

3 ^ 2-60. He-3 4 4 7 1 4 4 4 &3 4*34 # 4 4 3-4-^48- ^ y 2-624 44 . En < 0 4 °344 yield4 X-4, 4 4 4 4 # 4 4 4 4 4 $J44 4 4 ^ 4 4 4 4 4 4 4*144 4 4 4 , 7 7 4 #*344 yield4 7 4 4 4 4 4 4 444*1 444$14. En > 0 4 2J44 *^45%l4 # 4 4 4 4 4 4°-5 4 # °J44 4 4 3 4 5 * 4 ^ 4 4 4 4 7 $144 444$1 4. Li foil4 4 4 4 3 ^-^^ ^ ^ t ^ 4 3 ^ 2-634 ^ 3 4 , 3 * 2-624 4 4 4 En > 0 4 °3 4 4 2i3«5^4 s 4 4 ^ 4 4 4 4 4 4 3 5 ^ ^A) 4 4 %v 7 $14. 442:4 4 441- S. 2-24 *344 xt4. 4 ^ 4 neutron yield 4 MCNP 2LH5 4 4 4 £ 4 4 4 $244x14.

3 ^ 2-61. <4*34 ^ 4 4 4 4 # *34 M £ 4

-:j50 - S » ; : : ; r i s * 3523 B»0«V3

^ 2-62., He-3 33 # 4 S Li-foil &4 4*3 ?1 #*34 3 « J E ^

- 61 -

-1 OOD -sea o En(k eV)

H) 2-63. He-3 ^ # 4 X Li -foil4 4 4 4 3 ^ 4 * 1 ^ x f i ^ H ^

3. 23. #*34 4 # 4 4 * 3 ^ *3# Parameter

23434- ^ 4144 1 44

Data Acquisition Time Neutron Moderator Thickness Absolute Detector Efficiency Beam Current Uncertainty

Neutron Yield

18.3 MeV 0.36 nA 600 sec 8 cm 0.0054 12.3 %

9.3 ± 1.1 x 105 Neutrons/nA/sec

- 62 -

2.3, ^ 4 4 ^ § tf^m 4E! oie <27

7}. 42i4 44*14 4 4 #A34 f $4 4 ^ 4 43

# 4 4 4 4 7}<*4 # 7 3 4 4 4 4 D + D -> He3 + n (2.45 MeV) 4 4 4 4 4 3 . 5 $1444 € 4 . # 4 4 4 4 ^ 45.4 4 4 4 444- 4 4 3 . 5 4 £ 4 7 $1x14 105 neutrons/j4 # 4 4 4*3x44 4 - ^ 4 4 D2 # 4 ^ 4 4 2if 3 4 4 4234 4 4 4 1 - 7>44 7 * 5 4 4 4 4 H 4 # A J 4 4 ^ x 4 4 ^*3%v 7$14 9J44 ^ 1 4 4 4#4xU[ i ] 3 4 4 4 4 4 4 3 ^ 2 64

4 3 ^ 4 [1]4 T Ditmire4 *T<|H1 4 4 4 4 4 4 €2-vr 820 nm 4 4 4 35 fs 1 3 4 4 4-2:4 44*15 ^ 3 4 120 mj4 44*12} 10 Hz4 4 4 1 : 4 4 4 44x13.4, 44*1 spoi4 4 4 100^m4 4 4 3 . 5 4 4 4$14.

1) Gas Jet444 € 4 ^ 4 #H

D2 gas jet4 4 -14241- f AA'A 4 4 4 4 -170.E 4 4 4 4*1435 '-3444. 4 f 4 4*34 442^44 sjtf 4^£- 4 50 Angstrom4$14. Gas

- 63 -

jet442l f 4 4 4 #42344 4 ^ 4^-4 empirical Hagena 4 7 5 4 4 *3t 7 $14[2].

i* = k (d/tan a

\0.8c. Po

7 P 9 (6)

4 441*1 dA gas jet4 $174 Am444 ~A^A 4 4 4 3 , a 4 jet4 4 447}4 ASA 4 4 4 4 4 4 , po 4 mbar444 backing pressure, To 4 2 4 4 gas4 Kelvin 4 ^ 4 3 k4 4 4 4 # 4 4 4 4 ^4*14 4 7 4 4 . 4^1 *}*1 4 4 "A 4*}4 4 4 4 7 k4 4 4 4 4 £ 2-34 4 4 4 $ 1 4

S. 2-3. Hagena ^ 4444 44 47 gas

k

H2

184

D2

181

N2

528

0 2

1400

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3660

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2360

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3.85

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185 1650

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5500

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4 4 4 ^ N4 4 4 4 IN=Af2ChltI0$) 4 4 5 91444 Rayleigh

scattering signal4 4*344 7 4 7 $14- Rayleigh scattering 4 3X4 5 # 10ns4 Nd:YAG 314*14 second hannonic4 532nm 4 4 4 0.1 mj442l 4 4 4 4 4 1 - 4 4 44*11- 4 4 3 5 4 4 gas jet4 4 4 4 4 4 44*14 4 4 4 4 4 7 4 4 4 ^ 4 CCD 4 4 4 4 ¥ 3 4 x # 4*34:4.

44*14 4 4 4 4 °^.AA # 4 ^ 4 4 -1-744 D-D fusion4 4 4 4 4 4 4*14 $.£■& D, gas jet4 As. 4 4 4 4 4 4 4 44*1^4 ^1441-

calorimeter5 4*344 7 4 7 $14. 4 4 4 44*14 ^ 7 4 4 gas jet4 backing pressure7} 4 4 7 4 #7}447} 4 3 4 4 444*14 $i*344 5^4 4 4 AA-%: 5 4 4 , D2 7}^} £5.7} ^ 4 -170£ 4 4 4 7 4 4 3 5 ^4-4

- 64 -

file:///0.8c

4 4 4 4 44*1 -f-7 £ 4 4 4 4 7 $14 4 4 4 4 €423444 £dUMh&a 4*3^ D* 4 4 4 4i£4- 4 4 ^ 4 4

Micjhelson interferometer-! 4 4 4 4 4 ^ 4 4 . D*4 "US^ <£44 interferogram 3 5 4 4 Gas jet4*1 f*34 4 4 ^ 4 4 ^ ( ^ 4 ^ 5 ) 4 cylindrical symetry44 *}*34 4 Abel conversion4 4 4 4^-4 7 $14.

D-D «|-8-1|\£.3. *8A& # 4 4 4 plastic scintillator# % 4 4 4 4 5 4 # 4 4 4 * 4 Time-of-Flight spectrum4 4 *344 7 1 : 7 4 4 . 4 4 4 3 .

1 0 4 -

444 -5- 44- c* 4 4 55 o

1t>3-

6 x 1 0 1 6

Peak Laser Intensity (W/cm2)

g 2-65. el!44 4 4 4 * H 4-B #A3 4 -M 4 4*3 &[3].

# 4 3 ^ 2-6544 5^-4 4 4*14 447} #744^ -S-44 4 4 4 *3f 4 5 4 4 .

42*4 4 4 4 4 4 4 # 4 4 A^A 3 4 target ^ gas target4*1i $14'^ 7 $13-4, gas target4 debris7} 4 3 4 44*1 * 7 £ 4 4 4 3 Jl ll target4 gas target4 4 4 4 4 4 -f-744 # 3 4 debris7} ^-4 4 4 4 ^ 4 4 . iF -feiN target4 Gas target4 3 4 target 4 4*34 5_4%v 7 $ 4 4 4 4 4 4 4 .

3) ^ 4 2 1 4 4 3 44*14 4-31.444 4 4 44[4].

# 4 3 E ; ) 4 J I # ? | 4 ^ 4 44*14 *3-3\444 4 4 *3%H4 4 4 4 4 4 4 4 314*1 1 3 4 4 4 37-11444 $ H 4 4 4 4 *}4 4 4 , 4 44*1 4 4 4 ¥ 7 , 4 4 4 , # 4 2 4 ^44-4 4 4 S-^f 4 t ^ - 4 4 . s . t # 42144 4 # 4 4 4 4 € 4 ^ 4 # 345£ 1-4^44 4 4 # 3 . ^ 474$14. WA^-4 2144 4 4 # 4 3 4 ^ 4 # 4 2 4 4 # 4 4 4 # 4 4 4*1 # 4 ^ 4 4 4 thermal gradient.4 $ A | ) 4 4 &O> ^-g-^7}. ^ 4 ^ E ] \#d\}A] 4*344^1 4 3 4 4 4 4 £ &£M # 4 4 4 4 Maxwellian35 7}*34$14. 4 4 4 *}*3 2j. sjiof4 ^ 4 44- A.7]iojoii 4*fl 4 4 4 ^ 4 A] 4 ^?-ii4<4 # # 4 4

- 65 -

4 4 4 , 4 4 4 34214 4 4 4 4 4 ^ 4 5 1 4 $3^4 ^ 4 ^ #42344 H

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# 4 2 i 4 4 4 4 4 4 44*144 43*444 4 4 4 4 4 4 4 4*}*1 #21 4 4 4 4 4 4 4 4 4 $14 4 4 4 44*14 # 4 3 4 4 4 42*444 2,4 4 4 4 4 # 4 2 t 4 # f *344 4 4 1 - f l * 1 4 4 4 4 4 5 4 4 4 4*344 4 4 4 4 4 4 . 4 4 4 4 4 4 4 4 44*14 4 7 4 4 4 4 4 ^ 4 4 tunnel ionization rate4 44*1 $344 ^ 4 4 4 4 4 4 4 4 4 £ 4 4 4 .

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Xexp(2{2Lf/2A^) 4 xioilxl 14 m £ 4 ^ ^ ^ oj:7j.^o]ji( a)a4 atomic frequency

(wo = 4.13X1016.s-1), n^r n=Z[2Ip(eV)}~1/2£. 74*14 4 s 7 4

4 7 , E4 atomic umt35 7 4 4 4 44*1 field4 441 : , 34/n ^,-b atomic

unites. 74*14 4 4 4 £ E M &44.

7 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 # 4 5 37} 4 4 4 4 4 4 4 f 4 4 4 4 4 4 4?144. $144*11: # 4 4 4 4 4 4 4 4 # 4 4 4 4 4 4 4 4 4 4 4 4 4:4 4^4*1 2144 parameter^ * i^ L o t z

formula544 7"f 7 $14 ( 4 4 4 thermal 4 4 4 4 Maxwellian 4 ^ 5 4 4 4 5 - 4 4 3144.).

WhT = ne 3 7 •oo - «

i(fcrj^J7 * d£ <PA r,

4 44*1 ne4 444 4^43, ,4 eV5 4444 444 £4*144 a%-4^455 7444 471, g,4 44-4 44 ^44 444 71- 44^4.

- 66 -

All 4 4 4 4 4 *fl?14#4 ^144^1 4 ^ 4 - ^ 4 ^ 4 4 4 4 # 4 3 4 4 47} $1444 4 3 . 5 3 4 4 4 4 4 4 4 4 4 4 4 £ 4 4 4 4 4

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(9)

4 444 at4 4^4 4^4^ 4^4 44444 cr-f- 433.4 444^ ^

4 Lotz 44 444 ai=alqtln{Ke/Ip)/KeIp Jl5 4443 44*14 4

744 444 SJ^4£ 44444 4444 444 44.

= „ OiQi ( 1 Y/2 f2a»MKA)

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(10)

$14 4 4 4 44*14 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 47} 4 4 4 a | 2-664 4 4 4 $14.

UpMp (dashed fine) U\/lv (solid li«e>

3?J 2-66. 1023 cm3 4 4 4 VH2« 7}4 ^ ^ . v ^ e ) Ar«" 4 4 4 4 4 4 4 7114 44. 4 4 4 $14 4 4 4 s)# 4 4 4 4 4 4 4 4 3 , ^AJO. oi^ofl 4-5H ^ 4 ^ -AJAHI s]# 4 4 4 4 4 4 4 4 4

- 67 -

423^ 7}2[ *H44

4444 4447} #43444 44 445 4444 4*34 #44 44 inverse bremsstrahlung 4 4 — 5 4 f e ~T~ M. o) o 4 ■ 4 2 4 4 7 f 4 dielectric 4 ^ 5 ^ 4 4 4 # 4 ^ 4 ifl<H]A1 4 4 f4^1 uflgsfe °1]441 4

4 4 4*3435 4 4 1 7 4 4 .

1*!L = J _ # \ 322_ ID

# 4 3 4 1 - uniform4 7 5 7144 4 £ = 3/|e72|#05 4 4 ^ 7 $134

If^eEA 4 4 5 4 4 4 4 * 1 4 4 7 4 4 4 4 4 ^ 5 4 4 7}2|§£r 4 4 4

4 4 4 4 1 7 $14

dU CO T r n ci2 9ceJ J^72 |€ I r •,> = -?-- Im e Lc'l = ~—:

L~A\&A dt 8TT 9 lHJI

^ |f + 2|2

I -42 .4 dielectric Aj- ofl cfl4 4 4 4 Drude 231.4

e = 1 - wl/u){w + iv), u)„ = / 47re 2 n e /m e 544 #423=3 4 4 A 4 4

7 4 A 7}%%A 4 4 4 4 4 4 4 4 4 4 .

dU _ 9OJ2(JL>II7 1

dt Sir 9 o j2

( w2

7 ^ ) 7 ^ ( w 2 _ 6 a ; 2 11? |2 (13)

44*1 z/4 4 4 4 4 # 4 4 4 7 4 4 . 4 4 4 4 ^ 4 4 4 4_x}4 7}$J42]

47} 4 4 4 3 ^ 2674 4 4 4 4 4

• # 4 3 4 ^ 4 4 4 4 4

44*1 1*3 } 4 4 4 4 4 4 4 4 4 7 4 4 # 4 2 3 4 4 s

3 4 4 4 4 7*}*1 force*} 5^4 7 4 4 4 4 4 4 2 : 4 4 4 447} 4 3 5 ^ 4 4 4 4 # 4 3 4

68

4 4 4 *}3 7714 4 4 4 4-H.5. 4*14 hydrodynamic pressure42t 4 € 4 4 4 4*}7} # 4 2 . 4 4 4 a ^ 4 4 S 4 4 # 4 4 4 4 1 - 7}4 4 4 4 conductor sphere!- f * 3 4 4 7 f # 4 ^ 4 4 4 4 4 4 4 4 Coulomb pressure°14. Hydrodynamic pressure-k- Pe = riekTc5Z. 4 4 4 7 $134 4 4 4 ™iS7} #4234 44ofl 4 4 3 1 4 R 5 . 4 3 r 4 4 4 : £ 4 4 4 4 4 4 & 4 *144. 4 ^ Coulomb pressure4 7 f conductor4 4 4 4 4 44*17>

D>

*V"crtt

3 ^ 2-67. *i44 ^5.7} ^§}f- 4 825-nm, peak intensity 10lf> W/cm" 51 Elicit ^ i of l o]-cV *?44 7}<M - £«}.

Ea=:Q2e2/ZrsL £ 4 4 3 5 4 4 ^ 4 4 f 4 P buf = Q2e2Aur435 4

4 4 4 4 4 r4 4 4 # 4 4 4 4 4 A A 4 4 4 4 . 4 4 4 347V 4 4 # 4 3 44*1 Coulomb pressure4 <^44 # 3 . 4 3 4 $2 7 $14. 47}*1 force4 3 4 4 #423-1 4 7 34 4 4 »^AA AAA %v4.

d2r_ _ n^eAPcod 1 dt n.;m, r

(14)

4 4 # 4 2 . 4 4 ^ 4 4 4€- 4J£4 4^ -44 4 4 4 43-5 4 4 4 4 .

- 69 -

dt lcxp r dt (15)

• # 4 3 4 4 4 4 4 - 4 4 4 7}4

4 4 * 1 4 4 4 7}$J4 energetic4 4 4 4 4 4 4 # # 5 # 4 ^ 4 4 4 ^ 4

4 4 4 AAA AAA 4 4 * 1 1 4 4 5 4 4 4 4 7 $14 4 3 4 ^ 1 4 ^AA

4 4 4 thermal equilibrium rate4 4 4 # x 3 4 3 . 5 A^A 7 $14.

4 4 * 1 ^ 3 ^|o]4 ^ s ^ 4 4-jr4-g-4 o ^ 7 }4 process 4 4 4 4

4 4 # 3 4 4 4 # 4 3 4 4 ^ 7 4 4 4 4 4 4 $14. 4 2. 3. 5 5 4 4 # 4

3E-1 4 4 4 4 4 4 4 4 # 4 4 4 4 4 4 4£(#4*34v.)Hx-i ^ 4 4 4 5 7 7}

*34$14.)f- 7 4 7 $134, 4 4 # 4 3 4 4 4 * 1 4 4 4 4 4 shielding s 4

fe £ = 3 / 1 e T 2 | £ 0 4 4 4 3 . 5 4 4 3 4 4 7 $14. # 4 2 3 4 4 4 * 3 4 4 9

5 7 4 , 4 4 * 1 4 4 * 1 4 # 4 3 4 5 . 4 4 ^ 4 4 8 5 4 4 7 4 7 $43, 4 4 4 4 4 4 4 ^ 4 4 10, 115 4 4 ^ 4 4 4 . 4 4 4 4 4 ° . 5 4 4 4 # 4 3 4 4 7 4 4 4 4 4 3 ^ 2-684 4 4 4 $ 1 4

References

[1] T. Ditmire et. alt Nature (London) 398, 489 (1999).

[2] 0. F. Hagena, Rev. Sci. Instrum. 63. 2374 (1992).

[3] T. Ditmire et al, Phys. Plasmas 7, 1993 (2000).

[4] T. Ditmire et al, Phys. Rev. A 5, 3379 (1996).

- 70 -

4 #44 ^*34 44

o io18 W/cm2 4 4 4 4 4 4 7 ^ fs *3£4 1 2 4 4 4 4 3 4 ^ 2 4 1 - 3 44*17} n 4 targets $ J 4 t 4, 3 4 target 4 4 $*H 7 4 ^ 4 $14 4 4 4 %m± 31444 4 4*3-4 45711 4 4 4 431 1-4241- f A344 44-. 4 4 4 4 4 314*14 5 34f (rjansverse)/25. 4 4 4 ^ 4 4 4 4 s ] 4*3 4f4ongitudinal)4 4 4 4 ^ 4 4 4 3 . 5 drift 4 4 4 4 , 4 5 4 4 space-charge separation4 $1444 4 4 4 ¥ 4 f A34 electrostatic field force4 4 4 4 4 4 7}^4^) 4 4 7}^4 4 4 4 4 3*fl target44 ^ 4 4 # 4 4 4 € 4 . 3 4 targeti #72 - (D)7} £ 4 4 4 $14^ 7}4€ 3414*1 D+ 4 4 4 D7} # -^4 4 D"' + D -> He3' + n (2.45 MeV)4 4 4 4 4 4 4 4 #A3*k} ^ 3 € 4 . 4 4 7 4 4 - ^ 0)44 ^4-§-4 4 4 f.xj4 ^ i h g - 4 4 4 1 - ^ 1 4 ^ . 5 444x14.

-, -, , , . , -200 -10© 6 10ft iQO 300 *00

n ^ 2-68. 130-fs, 825-nm 3] 4 4 1 2 . 4 # £ . 44*}fe #4.^4^-1 ^7¥-^l ^S}; 4 7114 4 € 3)°14 peak intensity0)] uflsflAi TflAlsl^jz, A ^ ^ O . 5 X 1 0 1 6 W/cm2, ?J ^ x j ^ 1.0 xio1 6 W/cm2, 4 4 4 2.0 x 10 6 W/cm2 4 peak intensity°fl tfl*} 31441a) Pulse intensity profile, (b) Cluster 4 4 (c) # 4 2 4 4 * i 4 4 135.. (d) * i44 ^ ^ 4 .

- 71 -

o 3 4 target^ 4 4 f*34 34.5L(overdense) 4 4 ^ 4 4 4°l7l2}4 AJ- - 4^.^- ^ 4 4 4 4 4 4 4 47144 1 4 4 4 PlC(particle-m-cell) code*! LPIC++ [l]4 4 4 4 4 4 4 4 4 ^ 4 $ t 4 # 4 2 4 4 4 ^ 4 cnticai density n c4 414

n = 10nc{nc = to2m(,e0/e2 = 1.1 X 1021 / \[y.mf {cm'*))

5 7$l3.4, 4 4 vis n 4 4 3 3 4 4 4 4 4 4 4 4 4 A4 4 4 4 d=2A°J AASA 4 # 4 2 4 DJ5 profile4 4*34$14. 5114*14 4 4 800 nm, t*vf 30 fs FWHM, focal length4 4 4 15 pmo]3.t # 4 4 400 mj/pulse44 10 Hz4 4 4 4 4 4 4 4 f %A 4

&H4443 ^ $ 4 , 4 4 4 4 4 a(=eE/meix)c)$:£: 4 4 2 4 4 Spatial grid As (cell

size)4 A/1005 4x^3.4, cell4 macro particle7 1035 7$l3, Ar- = Az/c7} 4 4 .

4 4 4 '4.AA # 7 2 : D4 4 4 7 4 ^ = 3672me5 7$14.

o ZL& 2-69# a=243 t=60T (T, 4 4 4 44)$i 4, *d44 4 4 4 vds 4 ^ 4 $*A% (Ey)^ # 4 4 4 44*3- (Ex), 7}-44 D+ 4 4 4 4 4 4 3 4 5 * 3 4 4 4 4 4 11444 4 4 4 4 4 4 4 4 4 # t i3-f3.5 4 4 4 4 3 ( n ^ 2-69(a)), 4 4 4 4 4 4 £££- $14 space charge field ( 3 ^ 2-69(b), Ex)7\ f - 444 7 4 4 4 4 4 4 - 4 4 4 4 4 4 4 AA 4 4 4 a: 4 4 4 f 4 el)444 4 4 4 4 4 4 ^ 4 0)4. -1% 2-69(b)4 Bv pattem4*1 5 4 4 , 4 4 4 4 44*1 137} # 4 2 , 4 4 91444 4 4 4 3 $247} ^ 4 4 4 4 4 1 7 4 4 . 4 4 £114*1 I 2 4 4 4 4$14 4 4 4 R4, 4 4 4 4 *H4 H rfl*fl P=(I+R)T/'C

5 7 4 4 4 4 ^ 4 4 4 4 D+ 4 4 4 As 4 ^ 5 - 7 4 3 ^ 2-69(c)4 4 4 4 T(keV) ( T(keV)=miV2/2 )4 4 £ 4 $3$14. o a&A 1035 £ 4 4 4 4 4 4 4 2 4 "is. 4 £ ^ 44*1 field4 4 f 4 4 , D+ 4 4 4 AS 4 £ 4 3 ^ 2-704 4 4 4 4 4 . 4 £114*142) 4 4 4 4*11 a=2$l 4 £ 4 a=10 °4 4, 4 4 4 D+ 4 4 4 44*17} # 4 4 7 $14

- 72 -

3 ^ 2-69. a=2 o)ZL t=60 T $J 4 , 4 4 4 4 4 4 JE.-g-.SE. ^ % ^"$-$2] 4 4 4 , D+ 4 4 4 4 4 4 2 3 ^ 5 ^

W

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T (keV)

3 ^ 2-70. a=10 4 3 t=60 T $J 4 , 442} 4 4 4 4 £ 4 3 . ^ 3§ f-f # 4 ^ - 4 44*3-, D+ 4 4 4 4 4 4 2^:524

- 73 -

o 4 ^ 4 7 4 4 4 4 4 13.4 7}44 D+ 4 4 4 44*1 422544 # 4 4 4 *M^A 7 7 3t 7 $14. ^1444 reaction rate4

YD+D{cm sec" nD+n0\0vt DD

5 7 4 4 4 . 4 4 4 nD^ D 4 4 4 SJ&f, nD^ # 7 3 4 45*i 4 4 4 3 4 PIC

>1#4443544 74*14, 4 4 4 DT 4 4 4 44*1 T (keV)4 4 4 #4V144

M)DDA 4 # 4 D-D 4 4 4 4 *>5 [2]5f4 7 t 7 $14. ell4 4 1 ^ 4 # 4 4 *H

f 4 rn = r ^ • i 4 « T 2 ] 4 4 4 2 . 5 7 4 7444-. 44*1 A4 44*14 4 4 2 4

4 45- 4 4 4 AA^A, d4 4 4 ^ 4 4 7 4 4 , r # 314*14 1*:44 44-^4. 4 4 4 4 field44 a4 314 5 ,4 £ 4 4 4 4 S. 2-44 5 4 4 4 a4 3I444 intensity^

2x2 / = a2 x 1.37 X 1018 W- fim2/cm2A

4 4M14 4 4 4 . 3. 2-444 54 , a=6$i 4 7}44 4 4 4 44*]7} 7«fl KeV4 sq 4 4 #AJX} A|xj#^ 3144 ^ 4 10

5 4 4 4 4 4 7 $14 a=6$3 4, 14 AA 4 4

8xl019 W/cm2 4 4 4 4 7 4 4 4 4 4 2 4 4 4 a=2?14. 4 4 4 ^144 I 2 4 ^144 1 4 4 3 4 4 focal length!- #4°d 1019 W/cm2 4 4 4 44*1 # 4 4 4 4 7 $U #AJ 4 4 4 4 - t 105/Joule4 3 ^ 4 7 9)A 4 3.5 4 4 4 4

5 2-4. 44*14 44<Hl 4^- 1-42:4 4 4 4 4H, # 4 4 4 4 , 4 4 45£4 #*3*f 1 H 4 .

a

2

4

6

8

10

T, (KeV)

3.8

8.4

159

496

962

<JV (cm3s : )

6.5X10~20

6.0X10~19

4.3X10~17

1.3X10~16

1.8X10~16

n D+{l.7X1021/c7)

27.4

18.8

13.7

15.6

21.4

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1.54 X103

9.8 X103

5.1 X105

1.8 X106

3.3 X106

- 74 -

o 4U #42,444*14 4 4 4 ^AA^A 4 4 4 4 $144 # 4 ^ 4 4 3 4 4 \°1 4 4 4 4 4 4 2 4 347} 2A 4 42*H 4 4 4 4 4 4 4$14 ( 3 ^ 2-71)

2\ (1.6 gm)

. 1

' J 0.5 1.0 1.6 2.0

3 ^ 2-71. 4 1 : 4 4 ^ 4 4 4 4 : X=800nm, T=A/c=2.7fs, t 24=27fs. 1000 cellA. # 4 i r 4 4 ^ 4 4 = 200T

o 3 ^ 2-724 4 4 2 4 4 4 4 4 4 £4*1 1 S # 4 4 4 3 flonj 40T4 7 0 T 4 4 4 4 4 4 4 3 - 1 4 4 ^ 4 . 4 4 2 : 4 # 4 4 4 € 4 * 1 4 4 4 4 4 4 4 4 ^ 4 4 £ 4 4 4-531 A 7 $12.4 4 3 4 1 7 4 4 ^ 4 4 4 4 4 4 4 4 4 5 4 ^ 4 4 4 ^ . 5 « f 7 $1 4 . 4 4 *14 42-4- 4 5 X 105 m/s 4 4 3 . 5 4 4 4 4 , 4 4 4 # 7 2 : 4 4 4 AS7\ 4 5keV$l ^ 4 4 4 4 4 4 4 3 . 5 4 4 f 4 4 7 * 3 4 4 $ 1 4 4 4

3 ^ 2-72. # 4 ^ 4 4 ^ - 4 4 4 4 ^ 4 4 4 £ # , 4 4 4 4 4 s n a p s h o t 3 5 4 4 ^ 1 - 4 4 4 ^ 5 X 105 m/s 4 4 3 5 4 4 ^ .

References [1] R. Lichtcrs et al., computer code LPIC++ Report MPG225, MPI Quantenoptik, Garching, 1997.

[2] S. Glasstone and R. H. Lovberg, Qmlrolled Theimoniidear Reactions (D. van Nostrand, Princeton, NJ, 1960).

- 75 -

2.4. *r§a 4^ §3 4^ Z&

7}. 44 f 34 44 fla# 44

1) #4: 3 444 'gs. 4#4 44 4 • # • ° 4# $3 43.4 2) 4 4 : 2004 A 8 1 15 $i - 8 t 19$i 3) 2>k3 : 4 7 4 4 4 ^ 7 4 1 7 4 4 4 4 4 7 4 4) 4 4 4 :

Prof. Wei Yan Zhang: # 4 4 * 3 4 4 4 7 € A^A *l # 7 ICF ( 4 * 3 / 4 4 4 ^ 4 t ) 4214 4 ^ 4

Prof. Jian Qiang Zhm # 7 4 4 ^ 4 * 3 4 4 4 4 7 ^ 2 i4 7j # 7 ICF 4^14 4 4 4 4

Prof. Zun Qi Lin: # 7 4 " 4 4 4 ^ ^ 4 A\AA^ SG B 4°d*V 4 # 7 4 4 4 4 4 (Academician)

Prof. Yasukazu Izawa : $14 Institute of Laser Engineenng 4 4 IFE ( 4 4 / 4 4 4 4 4 4 ) 4 7 4 ^ 4$J/4

Prof. Masahiro Nakatsuka: a 4 Institute of Laser Engineering $J4 IFE 4 7 4 4 4 ° J 4

Prof. Konaki Miyanaga: 4 4 3*} 4 4 4 3 5IL^ < 3 s e 5 i7 : 4 7 4 7 ) 4 f 4 ^ 7 ffJ AA) # 4 4 H 7 : 4 7 4 4 4 ^ 4 4 4 4 4 ^ 7 4 4 7 4 4 : 4 7 € 4 4 4 7 ^ $344- 4*V 4 7 4 4 4 4 7 2 . 4 4 7 4*k 4 7 4 ^ 4 4 4 ^ 4 7 4

5) ^ 4 A } 4 :

4 4 2 L 4 4 4 4 A 4 7 4 4 # 7 4 4 4 * 1 4 4 4 4 4 4 44*3" 4 7 4 4 4 , 4 4 4 4 4 * 1 4 4 4 4 7 4 4 $ J 4 # 4 4 4 4 4 4 4 7 } 4 4 4 4457-1, 4 7 4 31 4 4 4 Us 7} it 4 7 4 4 4 $1-354 ^ 4 4 4 4 1 4 4x14.

¥ 4 3 4 4 7 4 4 4 4 3 5 7 * 3 4 4 4 4 4 , 4 4 4 44*1 4 4 4 4 4 4 7 4 ^344 4 4 4 # 7 4 ^ 4 4 $>*i 4 ^ 4 7 4 5 # 4 5.7] 4 4 7l£ f 4 ^ $1*3 4 5 4 4 4 x 1 3 . 21 4 4 4 # 7 4 4 4 4 4 4 4 4 4 4 7 } 4 4 4 3 & # 4444*3^47114-7-214 ^ 4 4 SG II AA4

- 76 -

4 4 4 ^ 4 4 7 4 4 300TW# 42:4 3 # 4 Ti:Sapphire 44*1 4A^4 # 4 3 5 4 4 4 4 #4$ i74 4 4 # 4 4 444x14.

6) 4 4 4 14 5 4HA>4 4 4 5 4 4 4 4 4 ^ 4 4 4 4 -(Minutes of

Minutes)4 4A34$x3-4, 3 ^infl-8-^- 4 4 4 A A.

$253 '^L

<44*1 4444 4 4 4 • # • $i 4 4 34> # 7 4 $i44 4 7 4 4 44*1 4 4 4 $t7*} 4 4 1 7 444 44 444*1 4444 . (3*) 2-73)

, i. n^s # 4 2 4 4 44*1 4444 4 4 4 ^ 4 4 ^ 4 4 4 4 4 2. 114*14 44 A$A$. f-4^-44 ^-^ 4^-444 # 4 4 f 4 $i7 3. 2 l £ #42:44 314*14£ #4-2,44 4 4 w 4. 44 4 4 4# 5. 4 4 4 4 4 4 4 4 4 44*1 7fl*l

<#74 44*144 t444 4 4 4 4 4 4444 4 4 1444> Wei Yan Zhang J S 7 # 44*3-35 4 4 # 7 44*1 4 4 4 4 4 4 (#7 4*3449174, # 7 4 4 4 4 4 ^ 7 ^ , *J-444*34 7)711473, 4 4 # 4 4 4 7 4 < £ 7 £ , # 4 ^ 4 44472^4 # ^ 4 T A $!744 4 1004 4 4 4 4 4 4 3 $14)544 4 4 4 £ 4 4 7 4 # 7 4 4*i4 4 4 4 4 # 4 3 5 7 ^ 4 4 ^ # 4 4 # 4 4 £$13.4, 41- 4 4 7 4 4 4 4 4 4 # 7 4 ^ *3445 4534. U i 2-74) 1. IAW (ion Acoustic Wave)I- 4*344 3 4 £ #42 :44 ^

A A #*344 Thomson 4 4 *lf o o $

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- 77 -

4. nAAA 44 344*1 444 3444 4^ 44

£ 4 4 ^ 4 4 4 4 4 $143.5 4 4 4 4 * 1 4 # 4 # 4 4 4 4 7 4 (CAEP; Chian Academy of Engineering Physics)44 4 4 7 4 4 300TW -§- 44*14 # # 4 4 4 4 4 4 #44^1*1 4 - M 4 xl34, 4 4 224 4 # 4 4 4 4 4 4 * 1 1547} 4*34x^34 4 $ 1 7 ^ 4 4 4 4 4 # 4 4 ^ 4 4 4 4 AAS 444x14 .

4 4 4 4 7 4 4 7 # 4 4 2 : 4 44*14 4 7 4 3 4 4 4 4 4 7 £ 4 25 TW7> 4 4 4 4 , 4 4 7 1 H 1 4 4 lOTW *3£4 4°1*11- 4 4 4 4 4 4 4 5 4 4 4 € *435 4 4 4 4 . 4 4 4 : 4^4*1 300TW^-4 4 1 4 4 4 1 : 4 4 4 7 $14 44-ir 4 4 # 3 . 4 4 4 5 4 4 4 4 4 H3 4 4 ^ 4 4 4 7^14-7} 4*^43.5 4 7 4 4 4 4 4 4 44*1 4 4 €■ 4 4 4 3 4 4 4 4 . ^ 4 4 4 4 7 # 4 4 $14 SG II 4 * i 4 4 ^ .44 4 4 / 7 3 s 4 3 %IA SG I I H 4 4 114*1 4 4 4 42j<45i 4 4 - 4 4 # 4 4 4 * } 7}^44 4 4 4 4 4 *344- % 7 $14. 4 4 4 44: 4*H*14 # 4 ^ 4 4 4 4 4 4 4 7 ^ 4 * 1 # 4 4 4 4 4 4 4 £ 4 4 4 4 4 4 / 4 4 4 -^4 % 4 7 4 4 4 4 4 4 7 7 gfrjfc */4°l ^3-oiq-.

- 78 -

MINUTES OF MEETING Of the Workshop

ForTri-lateral collaboration among Korea, China, and Japan

Date: 17th August, 2004 PJace : INTEC (international Nuclear Technology Education Center)

Korea Atomic Energy Research Institute Daejeon, Korea

Participants: From China : Prof. Wei Van ZHANG (CAEP)

Prof. Jian Qiang ZHU (SIOM) Prof. Zunqi LIN (SIOM)

From Japan: Prof. Yasukazu IZAWA (ILE) Prof. Masahiro Nakatsuka (ILE) Prof. Noriaki Miyanaga (ILE)

From Korea : Prof. Hyogun KIM (KJIST) Prof. Hong-Jin KONG (KAIST) Dr. Yong-Joo RHEE (KAERI) Dr. Chang-Hwan LIM (KAERI) Dr. Bong-Ju LEE (KBSI)

Subject: Tri-lateral collaboration on the high density plasma physics

The participants listed above get together and have a workshop on the Tri-laterai collaboration on the high energy density physics from 15 to 18 of August, 2004 at the I NTEC building in Daejeon Korea

The participants had meetings to review the past and present collaborative activities on LFE (Laser Fusion Energy), and to discuss about the future collaboration including experimental and theoretical studies which are related to HDPP (the high density plasma physics) and spin-offs of it.

The participants agreed that the collaboration regarding the LFE is beneficial to 3 countries and agreed to encourage the enhancement of the level of collaboration in such a way that Korea can take part in the LFE experiments and theoretical analysis which are planned and managed by Chinese and Japanese IFE experiments, to join the experiments using IFE/HEDP facilities such as SG II, III, IV, Gekko XII, and FIREX, to cooperate for data analysis and simulations, and to propose some experimental scheme for joint experiments.

Accordingly for the near future collaboration on the LFE research, Chinese and Japanese participants expressed their willingness to do the collaboration by allowing the participation of Korean scientists jointly in the research field of;

A. theoretical simulation on the high density plasma physics and laser-plasma interaction B. experimental work on the high density plasma physics and laser-plasma interaction C. diagnosis of the experimental work on the high density plasma physics and laser-plasma

interaction D. target fabrication E. development of the laser driver for LFE

In the witness whereof, 3 parties have signed this MoM.

On behalf of China : Prof. Wei Yan ZHANG (CAEP)

Chairman of Chinese National Hi-Tech ICF Committee Prof. Jian Qiang ZHU (SIOM)

Vice-chairman of Chinese National Hi-Tech Committee Prof. Zunqi LIN (SIOM)

Academician of Chinese Academy of Science On behalf of Japan:

Prof. Yasukazu IZAWA (ILE) In charge of Japanese IFE facilities

Prof. Masahiro Nakatsuka (ILE) In charge of Japanese IFE facilities

Prof. Noriaki Miyanaga (ILE) Osaka University

On behalf of Korea : Prof. Hyo-gun KIM (KJIST)

Professor Emeritus of Kwnag-Ju Institute of Science and Technology Prof. Hong-Jin KONG (KAIST)

Professor of Korea Advanced Institute of Science and Technology Dr. Yong-Joo RHEE (KAERI)

Principal Investigator of IFE research Dr. Chang Hwan LIM (KAERI)

Project Manager of high energy lasers Dr. Bong Ju LEE (KBSI)

Plasma diagnosis and Software manager

.% 2-73. 4 • # • 4 371R4 4 € 447k4 4 ^ 4 44-IL ( ^ i

- 79 -

MINUTES OF MEETING On the visit of scientists

From the China Academy of Engineering Physics (CAEP, PRC) and the Shanghai Institute of Optics and Fine Mechanics (St'OM, PRC)

To the Korea Atomic Energy Research Institute (KAERI, ROK)

Data: August 18,2004 Place : INTEC (International Nuclear Technology Education Center)

Korea Atomic Energy Research Institute Daejeon. Korea

Participants: From Korea : Dr. Yong-Joo RHEE(KAERI) From China : Prof. Wei Yan ZHANG (CAEP)

Prof. Jian Qiang ZHU (SIOM) Prof. Zunqi LIN (SIOM)

Subject: Collaboration on the high energy density physics

Prof. Wei Yan ZHANG (CAEP), the chairman of Chinese national hi-tech ICF committee, Prof. Jian Qiang ZHU (SIOM), the vice chairman of Chinese high-tech ICF committee, and Prof. Zunqi LIN (SIOM), academician of Chinese Academy of Science, visited KAERI to have discussion about the collaboration on the high EDP (Energy Density Physics) from August 15 to August 19,2004

The oarticipants had meetings to review the past and present collaborative activities between KAERI and Chinese institutes related to high EDP and IFE (Inertial Fusion Energy), such as CAEP, LFRC, SIOM. JAPCM, IOP, CIAE, etc. and to discuss about the future collaboration including experimental and theoretical studies which are related to high EDP and spin-offs of it.

The participants agreed that the collaboration regarding the high EDP is beneficial to both countries and agreed to encourage the enhancement of the level of collaboration in such a way that KAERI can take part in some of the high density plasma experiments and theoretical analysis which are planned and managed by Chinese national hi-tech ICF committee (HICFC). with the cooperative permission by HICFC to access the yearly schedules of IFE experiments, to join experiments using IFE facility such as SG II, to cooperate for data analysis and simulations, and to propose some experimental scheme for joint experiments.

Accordingly for the near future collaboration on the high EDP research, Chinese participants expressed their willingness to do the collaboration by allowing the participation of KAERI scientists jointly in the researches such as:

1. Thomson scattering experiments to analyze the plasma characteristics of the IAW (Ion Acoustic Waves)

2. High energy density physics simulation with the faculty of sciences of Zhejiang University 3. Small scale experiments to study the nuclear reaction (neutron generation by

femtosecond lasers) with CAEP (300TW) and SIOM (20TW) 4. Hot electrons and fast ignition study with CAEP

Details of the implementation of the collaboration mentioned above may be discussed further with the involved institutes. Regular joint meetings for the planning and evaluation of IFE experiments may be thought of as one form of higher level of collaboration.

The participants agreed that the collaboration between KAERI and IFE community of China including CAEP, LFRC. SIOM, IAPCM, IOP, CIAE, etc. is beneficial to each participating research group and it can enhance the ROK-PRC cooperation for the future clean energy production in Korea and China.

Both parties noted good and friendly spirit of the meetings.

In witness whereof, both parties have signed this MoM.

On Behalf of KAERI On Behalf of SIOM

Yong"-Joo RHEE Jian Qiang ZHU Principal Investigator Vice Chairman of Laboratory for Quantum Optics Chinese Hi-tech ICF Committee Korea Atomic Energy Research Director of Shanghai Institute of Optics Institute and Fine Mechanics

Aug. 18, 2004 Aug. 18, 2004 Date Date

3 ^ 2-74. #-7 44*1 4 4 4 4 4 4 44*3- $T3)4 ^ 4 4 44-1=- (4-g-)

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S. 2-5. i 4 3 a i ^ ^ K M 711 14 IFSA2005 4 ^ 4 * 1 4^52 4 4 4 7 } 4 4 4 7 A ^^ofl 4 4 4 S3] 4 3 4 4 4 4 4 ^ -

MtNUTES OF MEETING On the Tri-lateral CoJIaboration

Among Japan, China, and Korea

Date ; September 9. 2005 Place : The Bellevue Congress Center, Biarritz, France

During IFSA 2005 confererce Participants :

From Japan: Prof. Yasukazu .IZAWA (JLE, Japan) Prof. Kuntoki MIMA {ILE. Japan) Dr. Hiroshi AZECHI (ILE. Japan)

From China: Prof. Xian Tu HE (IAPCM, China)) From Korea: Dr. Yong Joo RHEE (KAERI. Korea)

Dr. Chang Hwan LIM (KAERI, Korea)

Subject ; Collaboration on the high energy density sciences

During September 5 and September 9, 2005 the fourth International Conference on Inertial Fusion Sciences and Applications (IFSA) 2005 was held at the Bellevue congress center at Biarritz, France.

And Prof. Yasukazu .IZAWA (ILE. Japan). Prof. Kunioki MIMA (ILE, Japan), Dr Hiroshi AZECHI (ILE, Japan). Prof. Xian Tu HE (JAPCM, China). Dr. Yong Joo RHEE (KAERJ, Korea), and Dr. Chang Hwan LIM (KAERi. Korea) gathered together and had meetings dunng the IFSA2005 conference to discuss about the collaboration among three counties (Korea, Japan, and China) regarding the High Energy Density Sciences (HEDS) for Laser Fusion Energy.

Dr. Yong Joo RHEE explained briefly about the background and the current status of trie bi-lateral collaborations between China and Japan under CUP (Core University Program), between Korea and China under ROK-PRC Optical Technology Research Center project, and between Japan and Korea under institute-level collaboration agreement. He also introduced In more detail the Korea-China collaborations including (1) laser fusion studies using Chinese SG II facilities In SIOM (Shanghai Institute of Optics and Fine Mechanics) to understand the fusion plasma characteristics by measuring Thomson scattering spectra, and (2) joint studies for neutron generation from deuterium clusters by Table-top Terawafl Trsapphire lasers with LFRC/CAEP (Laser Fusion Research Center of China Academy of Engineenng Physics) fusing 300TW laser system) and with SIOM (using 20TW laser system).

The participants discussed about the proposal to the agenda of Minister-Level Meeting for Science and Technology Cooperation among Korea, China, arid Japan. Since there has been established bi-lateral collaborations between Korea and China, between China and Japan, between Japan and Korea, it has been thought that upgrading the cooperative relation to tri-lateral collaboration would be more beneficial to the three countries in developing the HEDS-related technologies, where tri-lateral means three countries consisting of Korea, China, and Japan as north-eastern Asian countries. So the participants agreed to propose an agenda, under the title of "High Energy Density Sciences for Laser Fusion Energy", if this title is fine with each institute after internal discussions in each institute, to the working group meeting which is scheduled to be hed in Tokyo in late September of 2005 before the Minister-Level Meeting In this agenda the representatives of each country would be expressed as follows:

Korea Atomic Energy Research Institute (KAERI) for Korea (Key person: Cheat-Jung KIM)

Institute of Laser Engineering (ILE) for Japan (Key person: KLnioki MIMA)

Shanghai Institute of Optics and Fine Mechanics (SIOM) for China (Key person : Zunqi LIN. Xian Tu HE. or Wei Yan ZHANG)

where regarding the Chinese key person there might be some more discussions in Chinese side. For Chineseside. LFRC/CAEP would be a strong backbone of this collaboration under the National High Tech ICF Committee (NHTICFC) and SIOM will be the front end of this collaboration.

For Japanese side, there would be discussions internally before submitting the agenda to Japanese government, andKorean side will give appropriate information to Japanese side to help them preparing the Japanese agenda. Thatinformation may include the objectives, scopes, modes of collaboration and so on.

The participants agreed that the collaboration among KAERI and IFE (Inertial Fusion Energy) communities of Japan and Chinais beneficial to each participating research group and It can enhance the cooperation forthe future clean energy production in north-eastern Asian countries

Ail the participants noted good and friendly spirit of the meetings.

In witness whereof, representatives of each country have signed this MoM.

On behalf of KAERI On behalf of ILE

Yongjoo RHEE Kunioki MIMA Principal Investigator Director of Korea Atomic Energy Research Inst Institute of Laser Engineering

Sep. 9. 2005 Sep 9, 2005 Date Date

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2E. 2-6. 2005<d 81 f^ CAEP 4 4 4 4 KAERI 44*1 4 4 4 3 4 4

MINUTES OF MEETING On the visit of scientists

From the Laser Fusion Research Center (LFRC, PRC) To the Korea Atomic Energy Research Institute (KAERI, ROK)

Date : August 11, 2005 Place : The First Research Building

Korea Atomic Energy Research Institute Daejeon, Korea

Participants From Korea : Dr. Cheol Jung KIM (KAERI)

Dr. Yong Joo RHEE (KAERI) Dr. Hyung Ki CHA (KAERI) Dr. Chang Hwan LIM (KAERI)

From China : Prof. Zhi Jian ZHENG (LFRC/CAEP) Mr. Hong Jie LIU (LFRC/CAEP)

Subject : Collaboration on the high energy density sciences

Prof. Zhi Jian Zheng, the director of Science Commission of LFRC of CAEP (China Academy of Engineering Physics), and Mr. Hong Jie Liu visited KAERI from August 8 to August 12, 2005 to have technical discussions about the collaboration on the High Energy Density Sciences (HEDS) for Laser Fusion Energy and to carry out the joint experiments using KAERI equipments for micro-n eutron generation.

The participants had meetings to review the past andpresent collaborative activities between KAERI and LFRC/CAEP related to HEDS and to discuss about the future collaboration including experimental and theoretical studieswhich are related to HEDS. Prof. ZHENG and Mr LIU gave talks regarding Laser Fusion research in LFRC and Clusters interacting with UUL (Ultra-short Ultra-high-intensity Laser), respectively.

The participants discussed about the proposal to the agenda of Minister-Level Meeting for Science and Technology Cooperation among Korea, China, and Japan. Since there has been established bi-laterai collaborations between Korea and China under "Korea-China Optical Technology Research Center" programme, between China and Japan under "Core University Program", between Japan and Korea under institute level collaboration agreement, it has been thought that upgrading the relation to tri-lateral collaboration would be more beneficial to the three countries in developing the HEDS-reiated technologies, where tri-lateral means three countries consisting of Korea, China, and Japan, as north-eastern Asian countries. So the participants agreed to propose an agenda, under the title of "High Energy Density Sciences for Laser Fusion Energy", to the working group meeting which is scheduled to be held in Tokyo in September of 2005 before the Minister-Level Meeting. In this agenda the representatives of each country would be expressed as follows:

Korea Atomic Energy Research Institute (KAERI) for Korea Shanghai Institute of Optics and Fine Mechanics (SIOM) for China Institute of Laser Engineering (ILE) for Japan

For Chineseside, LFRC/CAEP would be a strong backbone of this collaboration under the National High Tech ICF Committee (NHTICFC) and SIOM will be the front end of this collaboration. Accordingly the Chinese participants would contact appropriate persons in SIOM and CAEP for more official progress in China. The Chinese participants would also contact the representative for the working group meeting in Chinese MOST and inform them of the progress done through their visit to KAERI. Furthermore, considering the interests of CAS (Chinese Academy of Science) on the Fusion Energy Science, the Chinese participants would let the Chinese representative for tri-lateral collaboration in SIOM to contact CAS to inform the progress on the agenda of Korea-China-Japan Minister-Level Meeting on the High Energy Density Sciences (HEDS) for Laser Fusion Energy.

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The participants discussed about the scientists exchanges. Since the Korean side needs some people to help them in assembling high energy laser components, two or three laser experts from China may join this project for about six months or longer. Also for a more efficient collaboration on the micro-neutron generation studies, Chinese side expressed their interests in joiningthe KAERI experiments using the newly built 10 TW laser system. KAERI accepted this suggestion and would plan the detailed schedule for joint experiments upon the request of Chinese side as situation allows.

Considering the due date of applications for the joint experiments using Chinese SI LEX (Super Intense Laser Experiment) system, which is usually February of the year. KAERI will submit the experimental proposal accordingly for the following year.

The campaign for Thomson scattering using SG II facilities this year will begin Nov. 20 for 2 weeks and Korean side is invited to participate in the experiment.

The participants agreed that the collaboration between KAERI and IFE (Inertial Fusion Energy) community of China including CAEP, LFRC, SIOM, IAPCM (Institute of Applied Physics and Computational Mathematics), IOP (Institute of Physics), etc. is beneficial to each participating research group and it can enhance the ROK-PRC cooperation for the future clean energy production in Korea and China.

Both parties noted good and friendly spirit of the meetings.

In witness whereof, both parties have signed this MoM.

On Behalf of KAERI On 8eha)f of LFRC/CAEP

Cheol Jung KIM Zhi Jian Zheng Vice President of Director of Science Commission, LFRC Korea Atomic Energy Research Inst. China Academy of Engineering Physics

Aug. 11, 2005 Aug. 11. 2005 Date Date

S. 2-7. f^-oj) *1]O>-&L " j io f lu ix i^s . AW 4 : ^ AA 4-B-

Project Description

1. Background

A. Worldwide active research area for future clean energy

- Reduction of the global warming gas has become an important issue and rapid industialization of China with increasing usage of energy has been noticed.

- All major countries are developing Inertial/Laser Fusion Energy (IFE) facilities such as NIF in the USA, LMJ in France, GEKKO XII and FIREX in Japan, ShengGuang III in China, Vulcan in UK, ISKRA 6 in Russia, in parallel with the Magnetic Fusion Energy (MFE) devices such as Tokamaks, for the future clean energy,

- 86 -

- As an economic and R&D block, the north-east asian countries such as China, Japan and Korea are supposed to take part in the enhancement of human life standards, as those in European Union or America.

- China, Japan, and Korea are lack of natural resources for energy generation, compared to the hugh demand for the energy for social development.

- Ultrashort pulse high bright fast neutrons generated in the fusion reaction are expected to have extensive application areas in industries, medical sciences, academies, and so on in a very near future.

B. Upgrade from bi-lateral collaboration to tri-lateral collaboration - Collaboration between China and Korea

Since 1999, SIOM and KAERI have been carrying out "Optical Technology Research Center" project, and under this "cooperation umbrella" collaborations on "neutron generation by laser fusion reaction" and "fusion plasma diagnostics by Thomson scattering" have been being successfully performed.

- Collaboration between China and Japan Under the Core University Program, SIOM and ILE have been in collaboration regarding "High energy Density Physics" for past 5 years.

- Collaboration between Korea and Japan KAERI has established the collaboration agreement with ILE since 1995 and under

this agreement high energy laser system so called GEKKO IV has been transferred to KAERI this year.

3. Objectives and Scopes

A. Research and Development Collaboration on the following areas shall be pursued:

- Fast/impact ignition and electron transport - Laser Driver and amplifier - High density plasma diagnostics - Target fabrication and reactor material - Computer simulation - Neutron generation and application technologies

B. Common Usage of Large Facilities 1) Chinese SG II for;

- Studies on fusion plasma characteristics - Studies on implosion dynamics

2) Japanese GEKKO XII and Mil for: - Studies on fast/Impact ignition - Hot electron transport

3) Korean p7flspective facilities for; - Neutron yield characteristics - Optimization for Laser amplifier parameter - Radiation technology development - Reactor material testing

C. Education and Tranining 1) Scientists exchanges

Joint seminar for information exchange Scientific visits for joint experiments visit for lecturing and tutoring

2) Student training and education Summer/winter school for 2 weeks each Long term visit for degree Joint degree/deploma program

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Joint experiment between CAEP and KAERI 1.Proposed Experiments-'

Enhancement of neutron yield generated by Coulomb explosion using UUL (Ultrashort and Ultra intense Laser)

2. Reference experimental setup-

Sctnllllnttng plastic neutron dotoetor*

probe pulse

3

35 fs laser in

RaylalgT) scatter detector

" backscatter monitor

A ' E=120mJ

0.5 mm nozzle. 100 "K avg cluster: a nm

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532 amNrfrYAG 10 ns, 0.1 mJ

estimate from avg gas lensity, scattering X section, sensitn ity,

located al 1.0m. 2.5m, 3.2m. 4.1m 6 mm lead shield

Fig. 1. Reference setup for neutron generation experiments

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3. Synopsis of the joint experiment-

The above setup was for the experiment done by T. Ditmire in 1999 at LLNL to prove the nuclear fusion by Coulomb explosion using table-top (small scale) femto--second laser. After this pioneering experiment many similar experiments have been carried out so far to enhance the neutron yield. (Related papers are attached.) It is generally understood that the neutron yield is about 10 neutrons/J for this kind of D-D reaction. 1 would like to dr the joint experiments to enhance the neutron yield by using several kinds of targets including D2 cluster. Da and CD4 gas mixture deuterated polyethylene, deuterated polystyiene. and so on. For r.his purpose, the following activities may be performed;

a. Evaluation of 105 neutrons/J yield with the 300TW CAEP laser system. b. Analysis of target characteristics c. Evaluation of experimental conditions such as pressure, density, temperature, size, etc.

4. Experimental diagram^

The figure below is rough schematic diagram of the proposed experiments.

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44 44S#4 AAA 4444 44^r €-4 4444 r«L4443 &£■ 471444. 444^ 44 <M4 ^41 15.44 4444 €^444^ 443. 4, 4 47 444 74 43-£ M £-4^4 ^44-37} 44. 44^4 44 4 4 3.4 44 4^44 ^44- 444 $13.35. 44 474iH 4747 444 4^4 44 444 4444, 474 34 47444 AAA A 2-34 4^4B. ^,444 44 44 ^4 4^4 44.

144^4^ < 44 44^-4 444 1^44 4^f>4 £44 -t^lil 4434, 244£4^r 44 114^ 441- 4444 44 ^44 44 t 7 $14 4. ^^44 1£ 444-t 1443 7}4 4^- 4^f4 4444 iL$l-°-4, 44 t^-44 44 43*>4 4V4444 4 £44 44 7 AAA. 44444 ^-44 7 4, f>7444 -Mf 444 4441 7 $1$34. 4444 £444 4?1 44-fe 4£ 44 444 -M44 a4 47^1 rfls} 44 ^ 44 7f 4 7 $1514. 4 ^444 -^4474 4A3- AAA 44 ^4 444 %4t 7 $1524.

4. 44^t 4444 £°J4 ^31 7l#

(1) 44^.^4 44 31 44 47

44^#4 £^47r 44 44-b 4^ 3 44^1 44£t- 44-7-4 ^44 534. 4 44 ^444^ 2-5 mbar 4 444 4443, 7 447- 5xl0~2 mbar, 3 444 5x105 mbar 43 4 44444 4-4. A %AA 4^4 344 d^AAA 44, 343 £#4 ^444 444 4^4 4^4 444 1444 44^1 5-4 £44 444 1:44 4 444 4fr £4 1-44 444 £4 4 &44 444

- 109 -

3^ 2-109. 4 ^ 4 AA]s £ 7i]44 A^4£4 4444 444 <44 44

34 23104 444 f 44 444 4 - 44^4 444 ^-444 44 44. ^444 4 44 ^44 44 £4^44 4 cm 144 44 445-4 44 44 €44-3 l 474 AA £4 4 4 ^ 4 £444 3 34-i- 4444 AA St 44. ^444 £474 4444 44-4 %v444 ^4 4344 %&#& 44 43 44 4-44 47}44 444- 4 44 £4 4444 4374 444 %*\ A 35. 447} -444 4444.

- 110 -

0.025 1 . [ . 1 . 1 . 1 . 1 . 1 1 ( . 1 . 0 10 20 30 40 50 60 70 80 90

pressure of nozzle (mbar)

3^ 2-110 . ^44 444 4# ^44 #44

(2) of lojst AAA 3 4 4 4 4^7H^

444 f 4 444 445.44 4£# 441 7 $17 44# 444$i4. <>1145# 4£ 4^4 4°l££ 4444 444 ^ ^ 4 44^41 50 mW # Nd:YAG 444^- 7^£4. 4-4 43.e 44 5.4 £44 444444 444 4 ^ 44 444 4444 4 4£^ £4£4 A%iA. 44 7}^ 4444 341 0.4 um 445 3 AAA 44 444 444 44 4^.4 #4 £4 7 $1 ^ 4€44 444 £4€ 44 <i£* PMT4 44 44£4 ^4/444534.

&%*& 444747 4 4444 444 444 4£^44 44 4^4 444 IkA 444 €3-44. 4 4444 444 444 $14 ^44 444 4 4-4 4^4^ ^44 4£# 4- 7 $14. 4 444 4£ 4444 4444 44 3} 44 44 4 445.44 ^£-4 44^£(10\V/cm2)# 3444 43 45_44 t-Q-tt 2:44 H.47} 34€4. 4#4744 443*1-7} 444-7 444 €7 4<i -an444 4£-4 700 MHz 4 4 41- 44"t ^4, 4 ±1.4 nsec4 £4€ 4 44 44. 4 44 447} 4£7} 300 m/sec 5 44 44447 0.84 um 4 444 44£4 £44 !:A3fr4. 4 444744 44 4^£4447 44 4 4sHl 44 <^4 44 &7-4. 444 4£ 447} 10 % 447 44 12 cm4 444~b 44, 44 444 300 m/sec44 40 usec4 4444 4^44 444

- 111 -

4£ 44-7} 4 4-2-U-4 4 7 $14. 4 47447 25 MHz 4444 *14-b 4 44741- ^4-444534.

44 432.-1 *14^ 4£ ^AA £44 444 3 4 * 44^4 444 441- *144 444 4444 44 444 444 444 444 444 444 314*14 444 £44 444 44444. AAA 44 444 34 444 44 4 444 34 44, 4444 47} 34 44£5 44 7 $174, 444 A^A 47}4 4 1 344 4444 44444 $14 &7 444 $J3, 444 444 1 um 444 44 4444 44(Di$persion) 4^4 4444. 34 2-1114 5xl0"3

mbar444 4 4AAA 4 44 44 1.5 cm4 3 cm4 73 47 ?1 444 4£ 4 444 444. 3444 4 7 $144 AA7\ 7 44 3444 4 4 4 ^ 4 A<& °t!44 4£ 44(0.4-3.2 um)4 4444, 4^4 3144(3 cm)4 44t} 4 44 1.5 um < 44 3 um 444 4£7} 44 <4AAA A 7 $14. 47 ^14 AA°\\ A A 4£5 4444.

444 37H1 4§ 45: 4444CI4, 44 4444 £4 4 J * s<Q 44 44 44 4-2-44. 4 47447 TSI 444 93024 444^4. £4 4 4514 Duke44 44-31- 444$374, 3 3.7] ^°4S7\ 5 % 44 4 44 444534. 44 ^4 445 4447 <M44 *44 4444 7441- 44 *> -4. x}4 ^44 $4*|-fe «4 £^ ^4 5J £44 44 4^4.

JO 15 2.0 2.5 particle size (nm)

15 2( panicle size (/on)

3 ^ 2-111. 444 344 4^ 47}4 4£ : (a) 7 444 4:44 1.5 cm °4 7iA, (b) 4 3144 444 3 cm 4 47 ~r

4444 £ 4.

4 4 4 4 4 AAA As 4 4 4 4 4 4 4 ^ 4 4 7 ^ 4 ^ 3I44 4 4 4 44-j- 5^-44x1 ^ $.£..§. & ^ 7J4 3Xio"3

mbar 4 4

- 112 -

44^ °«44 MFP(Mean Free Path) 7} g-44 4£4 J2.44 444 °4: 7 $1& 4. -24P_£ 4-44 ^7}'&o\) 44 <$7}<>) ^sA 44 444 4£7} 447} 3 4 444 ^ 4 $H4 4^-lr 444 AAA £44 ^ 444 34 440JI tfl 4 44£7} ^444.

4. 44 444 €44 44 4 4 ?m

^-4 44-4 4 -§- -4^fe 4^4 HTJI 4-M- 443 fl*r €^4 34 4 44 4# s444 44^4 445. 443, 4 4^44 ^444 14 44-

4 °J44 444 444^ 4 (LIBS)4 0d4# 3.4^ *M4 £444 4# 4 4 44 g 44S}# 444 ^44445 7^ V M 4 44 4447r 4^4 A 4. 444 ^ £ 4^ 4£7} 3 4 4 ^ - 1 7144 414-7 4^4 $l£4, 44 444 44 444 7>443 444 444444 44 44 444^44 444 7}444 444 4#44447r ^£5 &% 44 444 4-2-44.

_, fS_

, .ft.. .A,.,.

3^W

r^r^V ,— AAA; ■^A^JV^

x^SxIO'^sec

(a) €4^44 4#4 sf, (b) 4474(44)4 4€- LIBS 4^4 £5} 3 4 2-112. 4 4 4 ^

x (.7.44)44 ^ 4 4 7 4 4 ^ 4 4 ^ 4 4 4 ^4 44

113

4 47444 £444 £44 7}445. 444 445 4*3 4441: 4444 44^41 4£4£ 3 3 ^ 4 4 M.A^ 4444 43. «aM|444 4444 4-^444 AA 7}444 45.4$14. 34 2-ll2fc 4^4 4£# 44?} 341-4 ^44 7}445 44 444 445 44^ 47H1 44 44 i 444 4£ w

sv44&4 4 #4 ^41 44^ 44 4. 34*1)4 <£ 7 $144 -I-

4^47 ^4 4435s 44 4444. 34 (b)4 44^4 4x4 44 74 4 44A1444 44 3^5,^44. 44^4 ^AJ £4^^ 4^ 4A} ^.4 jg. 4 V34 4444 ^A 34^44 544, 444 4^4 44 44 4444?} ^44 4£ AAA A 7 $14.

3 3 2-113(a)4 34 2-112(b)44 4=4 74444 4^44444 (Monochrometer)5. 74(scanning) 444 44 444. 7444 4447 i}:£7 658 nm 444 344 £4 444- 43 AAA A 7 44. AAA Na4 t * 44 4444^441- 3i7$*\3i 4AA^ SA}4JL 4 X # 44 44 34 (b) 44. 44^44 4444 £4 4444 44 23}444£ 3 453} 0 4 34 7} 3M ^fl-44. g 44 ^4 44544 £44 44 444 344 ^44 4 444- 445.44 4444 44^4^ 4 44 4 3 45.7} 4444.

ta*B is igti ( m )

!a) 4^444441 744 44

- 114 -

X A ■ It T ite

(b) 444 34^ 7 £4 4£

3.4 2-113. 444 5:44 4?} 44^44 4444 ;

3£) 2-1147 4°144 445.^4 4£ 444 444 lNfo-}4 44^4 4 1H54^4 4^-£34£5. 44\£ 444. 3^44 44^44 ^-^o) 4-47II ^44^ 444 444 °4<pK:- 4 4435 744 47 44 t 7 $14. 4 TT 3 A*A ^444 4444-°-5 £- *Hr 44^#4 4444 -2-44 4^ 44 4444. 4 4.4 €f 44j4 44 444 $ AAA 4471- 44 44^44 4fe T74444 47-4 44^4 44544 4447} 44444 #$M «H44 €4 444# 4447 ^44£ 4 41} ^4-t 4443 44444 4-i- £47 4. 34 (b)£- 4£ 344 ^-44^4 44-444 £4 44.

1= 5

n i 1

01

> e 3

350

30D

Z 5 0

280

tSD

I D D

Histogram

so 10a 1 so zca

Mum v&rof phoion(Art>. Unit)

(a) 4 ^ S 3 ^

- 115 -

T 1 1 ' 1 ■ 1 1 1 ' 1 ' 1 ■ 0 I 00 200 300 400 SCO 600 700

Blackbody Radiation

(b) 4 ^ 4 3714 ^ 4 4 £ 4 4 4 4 4

3 4 2-114. 4 4 5 # <a*H4 1 H 4 4 <>144 ffl As. 4 4

44 4 4 4 4 4 4 4 4 4 4 4 5 4 4 4 7 4 4 4^ -4444 4 4 4 7 44 4 4 4 ?£A 4 4 4 $l£4, SMI 4 4 ^ 4 * ^ 4 4 445 .^4 AA # 4 ^ . 4 4 1k$ 4 4 4 4 4 4 4 , £ 4 4 4 4 4 4 4 5 # 4 ^ 4 4 ^ 1-9-7} 44. 3 4 2-1157 4 4 7}4 # t 4 ofl<>ls. o||4 AA 4 4 5 4 4 4 4 4 44-4 4 4 4 . ^443-5 £ # 4 4 4 4 4 4 4 £ ^ 4 4 5 # 4 £ ^ 4 £ 4 4 4 4 4 ^ 4 4 4 . 7}44 4 4 ^ 4 4 AA 4 4 4 ^ 4 4 4 4 4 4 4 444-1 134 4 4 4 3 , £ # 4 4 f - 4 4 4 4 4 7 4^* } # £ ^ 4 £ £ 4 4 4 4 4 4:4. £ 4 4 ^ 4 * 1 mm, 4 mm (4 4: 0.4 mm) 4 4 4 4 4 4 4 4 4 4 ^ 4 £ 4 4 . 0.7 4 4 3 4 H44 AA4A 3.2 4 4 3 ^ 4 4 £ 4 # £ 4 4 # 4 4 £ 4 £ $l£4, 4-b 3 £ 3 7 4 4 4 4 ^ 4 4 4 . €■ 4 4 4 4 4 # 4 ^ 4 4 ^ 4 <£4 4 4 4 £ # 4 43-8- ^ 4 4 4 , l 4 ^ 4 4 £ # 4 4 4 4 ^ 4 4 t !4 . najq 4 4 4 3 5 . ^ 4 4 4 4 4 447} 7}444, £ 4 4 4 ^ 4 447} l -7}444 4 4 4 fe4 £ # 4 4 4 4 4 4, 4-44 44444"44 .

£ 300

e 200

LU

Nozzle : 4mm Nozzle : 1 mm

(a) Particle size •' 0.672 um

34 2-115. £44 444 4-S 44£4 444 44

3^ 2-1164 £44 444 445.44 444 44 44 44 A-& LIBS 4x44. 3^ 2-11347 44 444 4£ 44^47} 4 ^344 54144 ^ 444 44« 444£ AS.A -3-44 444 &£4, £4 444 £44 43 44435 3 4.x 4s} 444 <244£ 3 44-7} £.4 &44 A 7 $14. # 444 41 4-M4 © 4444 M4-4 ^4§4 444 44444, £#44 444 4^££ 0114 4 *!£_§. -§-£4 4344 t ^ ^#4.

- 117 -

c o

0.

w3«slength(650-660 nm )

444 445444 44 LIBS As.

moon -

35DQD -

3QPDD -

-^ 25000 -c

I if) 3Dana -|

15DD0 -

10000 -

saoo _

tH i A / / I

r so

i 10

Numberof

" I — ED

shot

80

(b) 4 444 445444 444 £44-3 44 LIBS As.

34 2-116. £^44 444-7 LIBS 4^4 44

3 4 23174 4 4 4 °44441: 4-4 4 ^ £ 5 £ 4 4 7}445 445^ 5 4 4 4 44 4 4 #£4-£ 4 - i ^1435 ^ 4 4 4 4 . £^-#4 4 4

- 118 -

4£4 47.7} ofl i AVEflg. E -SMI 6flojs.#4| 44 $14 444£, 147444 4-oofl 6flo]s o)i 444 ^-f-44 0 7}7} $4t!4. £^44 344 444 £ 4£4 444 £*i7£ $14- 4 44 ^£4 444^4 47 44, 3 %±7\ i 4^44 4444 #444 344£ LIBS 4^££ 3 vfl oi %±& £ 4 t 7 $144 5*144. 4£444 AA AA 44£#°14, ^44 444 4444 ofl4£#4 4 •44 •714 4 4 4 ^ 4 445.44 3-AT\ 44-£ £?} o l

7}4 347} 4444£ 4 4^£5 3 ^44 4^1 7 $144 £4 44.

sth<392 3 9 ^

(a) 4444 444 LIBS As. 4^(££££44)

20CIUQ -

>s 200 00 -

■- 15000 -j

§> 1O000 -GO

50 DO

1 1—T 1—T 1—T 1 1 1 1 1 1 1—r~-> 1 ■ 1 384 386 388 390 392 394 390 398 400 "02 404

VVavelenglri (nm)

(b) 44°14 444 LIBS AS. 4^(£^££44)

3f 2-117. 4444 4454^ 4444 As. 4^

- 119 -

3.2 Bj|0|X-l &?\ Q\?\ SLjElii (LIDAR) 7,

7}. 4 4 4 44 4 4 4 4 £ 4 4 SAV 4^-

444 ofl4^ 4444 4£444 SAV4 44 47444 £4 44 -0-34 34 49- 40)44. a. <£7ofl4fe a ^oj. c ^ ^ S / W 1 - ^ 4 ^ 4 4

4, 4 4 44 AAA AAA * $ 3144 444 %A~£ 7 $1£4 4 4 4 4 4 £ f 4 4-44 7 f 4 ^ 4 .

444 4447 444: £44£1- 7}47 4454 444 44 LIDAR 44 44474 4-447 4 4 4 7 4^4 43444 444 ^4 444 £44 £4 AsA 444 44444 444£ 4£# 4444 AA 7l£4_g.5. *}•%■% 7 44. 4^3} 4^4 4 4 4 7 4 ^ 444 744 44£5 444^4 44 3£4 444 44 &4£ £44£4 4£> 4£4 4 4 t 7 AAA ^44, 3: 44 4*J4 44 4£^4 74£5»£ 4444. AAA °s

v£44^ £4 4^ 4344-4 w # , ^ -v4£ 7444. I£ 2-9 7 44 °4£444 7444 Matlab file 4 444 4 444 £444.

5. 2-9. 4-3444 7447 Matlab A°4 ^ 4 ^

4°J4

pn.m

pnp.m

ks m

ksp m

an.m

bn.m

71 *r

Ricatti-Bessel function

Ricatti-Bessel

function4 £ f - 7 Ricatti-

Bessel function Ricatti-Bessel

function 4 £ 4 4

Scattering coefficient

Scattering coefficient

4^4

apb.m

amb.m

efbac.rn

efext.m

kerbacl.m

kerextl.m

71 4

4 4 3 1 7 4

4 4 4 7 4

4 4 4 4 : ^

4 « 4

4 4 4 4 4 7

4317117*31

* } ° j ^

kercof.m

tikhsol.m

gcvpara.m

sol.m

distr.m

get j .m

71 4

4744^1 4£^

Tikhonov Solution

GCV

Parameter

Solution

Log- Normal distribution

Discrete derivative Operator

- > 4 4 , 4 - > 4 445 . , pn.m 4 4 kercof.m 4 4 7 4 4 4 - 3 ^ 4 7 3

- 120 -

4 7 4-741 3 4 3 gcvpara.m 4 4 sol.m 4 4 7 : 4if2}4 4:44 4 ^ 4 4 , 4 4 kercof.m 4 sol.m 4 4 Matlab M-filc D 4 4 £ 4 4 4 4 £ 4 4*2 4 4 4 4 £ 4 4 4 £ 4 1 - 4 4 ■ 4 4 t 7 $ l£4 Matlab function ^ 4 4 44$14. 4 4 4 4 4 Function file4 3 4 4 4 4 4 £ 4 4 4 4 ♦ 4 4 £77} 4 ^ 4 4 $14. 4 4 4 distr.m 4 € £ 4 4 4 4 £ 4 4 4s}4€ 7 $17, 4 4 H 4 4 £ ^ 7 S 4 4 4 £ 4 " 7 # 4 4 4 4 getj.m 4 4 T W 4 ^ £ T & Smoothing Operator 5 4 314-4 4 7 4 Discrete derivative operator!- #-$ 4 4 £ 4 £ 4 4 $14.

44J 4 £ f ■ * '■ 4 4 4 4 4 P 4 ^ 4 4 4 44 4 7 «ov44££44 4 £

^74 £ 4 4 7 4 4 A4^t 4 4 4*3444 4 £ ^ 4 7 4 4 3 , 4 5 4 4 4 4 £ 4 4 £ ^ 4 4 &4 4714 44*r4 . 4 4 ^ 4 4 4

wo

v44 % 4 4 s 4 4 4

4 4 4 14 4£^it75 a^ .4££ £ 4 # 4££}44e 4 4 4 4 1 £ 4 4 4 3 tll ZL ^47fe Size parameter, x A 4 7 x 7 4x

lA + 2 4 7}4 7}T4£ 475.

3 ^ 2-118. QM3.7]o\] 4 = 444 .4 . n.4 2-119. ^A3.7)o\] # # 4 4 S 4

3 ^ 2-1184 3 ^ 2-119^ 4 4 efbacm 4 efext.m 4 4 4 4 4.41- £ 4 4 4 . 4 ^ 4 4 4 4 £ E ^ 4 4 7 1 : 4 Gauss£44 Trapezoidal rule4 4 4 4 4 kercof.m44 4 4 4 ^ 4 4 4 4 4 4 * ^ l r , ^ 4 3 4 , 4 4 4 7 4 4 4 4 4 4 4 4 ^ 7 £ t>4. 4 4 4 ^ £ 7 ^ 5 1 4 7 4 4 ^ 4 4 4 1-44 7 $k°-4 4 4 1 4 - 7 kercofm.mat files. 4 ^ € 4 . 4 4:7414 £ ^ file-44 4 4 4 4 4 4 4 4 £ 5 4 4 1 7 $174, 4 4 - 4 4 4 4-44 4 4 4 4 4 3:4, 4 7 , Kernel matrix

121

4 4 7 4 4 4 4 . 4TT4- : 4A-4- 4 4 4 kercof.m44 4 4 4 4 7 4 4 4 4 4 4 4 ^ 4 ^v

^A 7 $17 £ 4 # 714 4 4 ^ 4 4 4 4 4 4 4 3 £47} 7 4 4 4 2145.44 4 4 4 4 4 4 4 4 4 4 a 4 4 £ 4 7 4 4 4 4 4 4 4 £ 4 4 4 7 4 7 4 4 4 4 4 4 4 4 4 . 4 4 4 ^ 4if4- 714^ £ 4 4 4 Tikonov Method44 AAA 4 7 1- <£A 4 4 4 GCV Method 4 4 .

x 10

- 2 0 2 4 6 Logarithmic Scaled Regularization Parameter. Log10(A)

-3 2 -1 Particle Radius. (, (nm)

3 4 2-120. GCV 4-4 zi-4 2321. Direct Inversion Solution

3 4 2-120^ GCV 4 7 4 4 # 4 3 4 4 4 4 4 £ 4 4 4 4 4 4 4 4 A A 4 4 £ 5 4^-4-^ £ 4 4 £ 1 - 4 4 . 3 4 2-1214 4 T T S } # 4 4 4 & 4 7 l 4 £ 4 4 z$QA Direct Inversion- 4 7^1 ; M 4 0 l £ 5 ell 4 £ £ ^ 4 4 4

^ i ^ L t : ] <>) _0__0_ O o 4 4 AA a °4 7 $14.

^ 5 0

Continious. Onginal Discrete. Exact Discrete. Tikhonov

A 1 e

3 2 CO

0 1 5

£

* 0 LO

5

4 \

■—■ Exact Tikhonov

— Error Contaminated

- -—., -3 2 -1

Particle Radius, r. (nm)

3 4 2-122. 4 ^ 5 . 44x1 sfl

1 2 ^ 4 6 6 7 lndlces(1-2 ior Extinction 3-8 for Backscatlering)

£ 4 2-123. 4 4 4 4 ^ 4-47417

- 122 -

3^ 2-12244- 4fl-s}- 44 <££- £££!- 44^ 4£ 441-4 4£ *r 444. 4fl-s}4 444 &4 444 *M AAA 4£5 44-4- 4£4 -B4 f44 4444 £44 $1447 444 44^14 $14. 444££ 4T?^4^4

4*} 4£4 A^ 444 &4 44, £4£ 4^1r 441- 34 2-1234 A^-A%i 4. £^€ 474 £4 4£f 4 Poisson 4£44. 4T?4-4: 14 fluctuation4 4444 44ti- 474£ ¥4 7}44^£4 444£5. 44: 47}?} £-44 4 7 $14.

4. £«4 44 4 H4 4#

£#4 444^ 44 4-^4 4444 4441- 44^- 44££ 444£ 4444. 4444 £3 3 4-5 4444 4£4 £74^ 4£ 444444 4 ^ 44 4 4#o]i tff*j| 4454 74 &4 ^>^tl 474W-4 444 4444 AAyr 44 ££44 4454 ^-47# 44 4441-4 £4434 AA.

4 4744^ f4 44147£44 TJ#^ 4444 #4* 4444 44 4 -M443 4-1- 444^ 471- 7*S4$4. 4 43 47£444 £7}4 74 A 41*4 444£ $l£4| 447 444 44"^£5. 44 444 444*114 4 7 $l r 44-t A4A]A%iA. 444 ^4# 444£ 4*1 444 444 44 H 7 $14 4-S-4 7}44 ^#43 444 4 -$444 -444££ $447:- 44 4(444) £4(fluctuation)4 $144-£ 7444 4^££ ^44 444 7 $1 4 4^ £44 44 44£ 441* 7 AA 44 44 ^144 ¥4 7 $14. -i 314 4^£^ £^ 2-1244- -4. 3^H4 44313- 444 44 444(1), 44 44 °J4(2)4 4444 4£4 924 ££^ 444(3), 34£ £44 ^4 #4 4445 S44-4 #4£V 4 44 44 444££ 47^ 44-4(4), 44 44 4444 44 44 44 sgf^AS 44fe 3!£(5), 44 4££ ^447 ^4 4444-7 4€€- ^4(6), f*|€ 44*1 ^^144 44 44-££5 477 4£ (7), 4^-44 44 4-B ^145 £M17 4-44 44(8), 343 444 s}44£ 444 ^4 444 4AS. 444 44(9)4 4# 441 4£5. 474 4444 4 444(10)5 7 ^ 4 .

- 123 -

3 4 2-124. 4 4 4 £ 4 4 £ 4 4 4 4 4 4 7 4 4 4 4 4 4 4

^ 4 £ £ ^ 4 4 4 ( 2 ) ^ 4 4 4 4 $1 4 4 4 4 1 : 4 4 4 -4 4-4 4 4 7 4 4 4 4 , ? 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 . 4 4 4 ^ 4 4 S°] 4*344 4 4 4 4 4 £ £ 4 4 4 4 £ 4 4 3 , 4 4 4 4 4 eJl£4 £ 4 4 4 4 4 >}3X}5 -?<•§- - r 4 4 4 ^ £ # ^-44} 4 4 ^*344 €4- 4 4 4 AAAA 4 4 4 °444££ 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4445-44 4 4 4 r ^ 4 4 4 4S34£5 4 £ 7 4 £ 4 4 4 4 4 4 4 f 4 4 4 4 N 44 4*«§4££ ^ f i t 4 4 4 4 4 1/N4 4 4 t 4 £ , 4 4 4 4 1AN-D4 444-4, 4 4 4 4 l/(N-2)4 4 4 t 4 , 34^1 £]#4£5->r 4 4 4 4 1/24 4 4 t 4 , 4 4 4 4 1 4 4 4 t 4 5 . 7 4 ^ 4 . 4 4 4 ^ 4 4 4 € £ 4 4 4 4 4 4 4 4 4 4 7 4-444 4 4 4 4 *J5344 4 £ £ 4 £ 4 £ 4 4 4 1 4 4 4 £ £ 4 1 3 4 .

^l£4 £444 ^44435 414 4£7 3 44 4 44- 4# 4£4 M 4 4 44. 44 4£5 41^4 444£ 444 ^4 ^4 AAA 44£ $14 £ 41- -4 444 44(Optical Path Length)7} 44 4 4§-4 44£7} ^ 4 4 4 4 4 4 4 4 4 4 4 4 4 € £ 4 4 4 4 « 4 4 4 ^ 4 41:^4 ^A-^ 4 4 4 4 4 4 4 1 ^ 4 4 4 3 4 4 4 747} 4 £ 7p>445_ SJ4€ til o o

7*; 1 - a 4 4£7} 4 4 4 4 4 4 4 447]- ^ 4 4 4 . 3 4 £ 5 4 ^ 4 4 4 4 £ 4 4 4 ^ °4 4 4 4 ^4ofl 44-4 rx f -4^7} ^ 4 4 4 . 4 4^- 4£5. 444 -^ 4-44-^

- 124 -

4€ 444 4447r 44 #4 4-S-4 44^£4 £444 $1£ 4-44 #4£ S-T: 45. 4€ 444 3M 44^4.

34 2-1254 444 444 4444 4,£7} 47 444 4443 $14. 44 7H4 ^H444 4444 £4 444, 444 4444 444^ S£ 44 444 4?1 44^4^44 44 444 444 4447- 44\£44 71 t 7 $l£4, 44 4444 44^ 4£44 ^4444 £4444 4-4^44 444 ^ 4 4 4444 ¥44 -&££ ^-44 441 7 $14.

— _ 8-1- 8-2 8-3 8-48- 8- 8-N-1 8-N '

34 2-125. 444 4445 444^- 44^ 74 444 144 £4

4. 4 4 4 4 4 4 As. 744 7f%

A4 444 £^-§-^4 -$14 444-7: 4# f Aj DIAU Differential Absorption Lidar ) 4^4 4 0444 $14. DOAS 4444 ^744^4 ^7-)e] 44 44435. £^44 4^4-3, £ -?-I4 444 477} ^447 444 4 4*14. 44?} 4444 4.4444 44 44 £443 44444 4444 4 4£4 S3 £4£44 £44^ 44 3 4^4 £4447} $14. 444 444 ^4 444 7444 £444££ 4444 44 44 4£44

£44 4444 7^ 44 4££ 44 $344 4447} 41-444 44

- 125 -

^ 4 4 4 4 4 4 4 ^ 4 4 4 £ 3^-44 44-4 ^ 4 4 4 4 4 4 4 SLAA 44 £ 5 4 4 £ 4 4 4 4 4 4 4 4 4 4 £ 4 4 4 4 £ 5 4 4 4 4 £ 4 4 4 4 4 4 SM 4 4 4 3 $14. 4 4 4 4 4 4 4 4 4 4 4 4 4 4 ^ £ -S-44-7 4 4 4 4 4 4 4 4 . 3 4 2-1264 4 4 4 4 4 4 4 4 4 4 4435 . 4 4 4 4 £ t4? r 4 4 £ 4 # 4 4 4 4 4 4 4 4 4 4 4 4 4 44°Hr 4 4 4 4^514 4. 4 4 4 3 5 7 4 4 7 4 4 4 £4*114 4 ^ 4 £5-144 4 4 4 4 4 4 4 4 1 4 2 4 4 4 3 5 . 4*144

0 5 10 15 20 25

CCD (X-axis) mm

(b). 4 ^ 4 £ 5 444r r 4 4 4 4^- CCD 4 4 3 4 2-126. 4^v4 4 4 4 4 7fl^£ % 4 ^ 4 314<H1 44: 4 4 4 £

- 126 -

34 2-1274 4«>4 444# 4 4 7}*] 4-g- #44 £444 4- £4 £444. £ 4 J 5 * ^ CCD4 444 44"t 7 £4 44 CCD1- 444$4 44 ol] £44 44 £4£^(44 444 444 3H8* 4)4 Wl 44 £44 ^v

444 £44.

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- 128 -

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- 129 -

Distanoe(x37.5m)

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34 2-132. 445.#4 444 44^7

- 131 -

3.3 ^ ^ * | 3 g 4*1 4 £ § 4 6 4 n r

7}. CKOTW (China-Korea Optical Technique Workshop) 2004 4 4

4 - 4 4 4 4 4 £ 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 £ 4 M 4 4 4 4 £ f - 4 # 4 $ ! 4 . 7 4 7 " 4 4 4 4 4 4 4 4 4 4 ( Remote sensing & Laser analysis) " 4 4 5 . 4 4 4 5 ^ 4 . 4 £ 4 4 £ 7 4 4 4 AA.

• 4 3 ^ 4 : CKOTW (China-Korea Optical Technique Workshop) 2004 7 4 : Remote Sensing & Laser Analysis Detection

A A 2-1. 7 £ 4 4 4 4 4 4 € 4 4 4 2-2. CKOTW2004 t £ 4 4 (Hefei, China)

- 132 -

o 44-44 4344% 44 €S4 47-^r4 444 ;£4.

%A

^ 7

^ 4 £ 4 4"l7l

(?}74*H473) 4A®

(?}744^147£)

(474.43 473) pi # 4

( 4 4 u 1 4 3 )

4 7 1 4 ( 7 ^ 4 : £ )

Dongsong Sun (AIOFM)

Hongmei Wang (AIOFM)

Li Fang (AIOFM)

Xiaoming Gao (AIOFM)

Ting Yu (SIOM)

M * $

Ultra sensitive laser spectroscopic technologies in KAERI

KAERI Raman Lidar System for Meteorological parameter

An adaptive optics system with hierarchical wave front

Recent development of laser-induced breakdown spectrometry (LIBS) for direct elemental analysis

Study on the vertical aerosol distribution by aerosol LIDAR at Korea Global atmosphere watch observatory

Analysis of the duaJ Fabry-Perot etalon for a direct detection wind lidar

Detection of sulfur dioxide by metastable N2 energy transfer

Design and performance of single particle laser mass spectrometer

Diode laser spectroscopy and its application

All solid state laser system for DIAL measurement of N02

4. KCOTW (Korea China Optical Technique Workshop) 2005 4 4

o °4A : 20054 11^. 44 - 111 5$J o 4 £ : 4 4 4 ^ 4 4 3 4 7 £ o ^-4 4 4 4 4 : 4 4 4 : 4 7 4 4 4 4 7 £

f -3 4 : 4 4 # t } 4 ^ 4 4 A 7 £ o 4 4 : 4 4 £ - 4 4 4 4 4 4 4 4 4 4m 4 3 - 4 4 4 ^ * } 4 o\6\t % 4

- 133 -

4 445. 4 4 4 4 7U44 As^s, 44 43144434 4. o ^ £ 7 4 : 444 4 4 44 g 44 4 4 4 4

4 4 2-3. 44- 4 4 4 4 7 £ 4 4 14 4 4 4 4 4 4 £ 4 AS. 4 4 £

4 4 2-4. 4 4 4 4 4 4 £ 4 4 4 4 4 £4 4 ^ 4

- 134 -

o £ ^ ^ i £ 4 4 11i£44

Veijun Zhang (AIOFM, China) Dong Geun Lee

(Pusan Nat' 1 Univ., Korea)

Huanling Hu (AIOFM, China)

Duck Hyun Kim (KAERI, Korea)

Jun Zhou (AIOFM, China) Sung-Joo Cho

(Lidartech Co. Ltd. Korea)

Dongsong Sun (AIOFM, China) Sung Cheol Choi (GIST, Korea)

Li Fang (AIOFM, China) Young M. Noh (GIST, Korea)

Liu Bo (AIOFM, China) Sang-Woo Kim

(Seoul Nat' 1 Univ., Korea)

Gao Xiaoming (AIOFM, China) Tae-Young Goo, (METRI, Korea)

Aerodynamic Diameter Measurement of Aerosol Particles by Using Diode Laser Developing Single Particle Mass Spectrometer as a Probing Tool of Nanoscale Phenomena

Lidar Monitoring Aerosol Pollutant Layer

Study on the Cloud Characteristics (Solid and Liquid) Depending on the Temperature, Humidity Using Hulti-Wavelength Lidar

Lidar Observations of Cirras over liefef. China

A Review on Commercial Lidars in Korea

Development of a Direct Detection Doppler Lidar

A Development of Remote Monitoring System by using Differential Absorption LIDAR (DIAL) Technologies Rapid Detection of Trace 1,4-DichJorobenzene Using Laser Mass Spectrometry Study on Lidar Ratio at Anmyeon Island, Korea Using a Multi-Wavelength Raman Lidar System Detection of the Atmosphere over Wuhan with a Fe Fluorescence Lidar Ver t i ca1 Prof i1es of As i an Dus t and Thei r R ad i at i ve Effects

Mid-Infrared DFG Laser and its Application

A Case Study for the Vertical Aerosol Distribution and Ion Components on Asian Dust at Anmyeon in 2004

- 135 -

4. 4 4 4 4 4 £ ^ 444 -

o Prof. Yinchao Zhang - £ 4 ■ 4 4 4 4 4 ^ 4 4 4 7 £ (AIOFM) - 44 : 44474 - £ ^ 4 4 : 2005. 3. 16-19 - £^44 : 444 44 44 44 - 7 £ 7*3 4 4 :

£ q44 4oil7-| 7 ^ 4 ^ Pollution Lidar, Aerosol Lidar, Raman 7] XL

4 4 4 4 4 4 4 4 4 314 4 4 4 4 4 4 4 4 4 ^ 4 4 4 4 4 4 4 4 4 4 4 4 4 4 7*34 4 4 4 4 4 4 4 4 4 SAV 4

4 4 4 4 % 4 4 ■ 1447£ 474444£ (44£) 4444 3 44 444 £# 444, 44 4 4 4 445# 444 44 44*1 444 14

■ 4 7 4 4 4 4 4 4 4 4 4 4 4 cfl4 71144 w*v£ o Dr. Wei Huang

- £ 4 ■ A$\ 4 4 4 ^ 4 74147£ (AIOFM) - 44 : 44474 - £ ^ 4 4 : 2005. 3. 16-19 - £^44 ■ 444 44££l- 444 4 44 4 44 7 - 7 £ 7*J 4 4 ■

' r

444444 7*344 4°1*1 44££# 444 444 ZA *444 4 44 4 £44 H4 £ ^AA 4 4 44 4447£ 474444£ (°44£) 4-444 3 44 AAA 444 44 44 444 444 444 4 44££ 444 44 44 #444 f 4 f^sj ei)44 44 44 444 44 444 ^£

- 136 -

9-4 2-5. Zhang44-4 Huang447} 4 4 4 4 7 £ 4 7 4 4 4 H 4 4 4 &%■ 474fe

4 4 2-6. 4 4 £ 4747l4:4£ 444°1 € 4 4 4 4 4 444°i 4 4 4 4 4 4 4 4 4

- 137 -

41 4 4 4°l-£-—-^71 ^ ^ A0)*] ^1^41 4t^-KAERI -SIOM # £ | 71 3 i

4.1. 4|a}°iE||o|x-l 7Hg

7}. 4

44" 4 4 4 £ 4 4 4 4 4 4 4 4 7 £ ( S I 0 M , Shanghai Institute of Optics and Fine Mechanics)4 £ 4 ^ 4 4 4 1 H 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 £ 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 y

sv 4 4 4 4 4 4 4 ^ 4

4 7 4 7*344 A9XA. £ 4 4 4 4 4 ^ 4 4 4 4 4 4 4 £ 5 4 ^ 4 4 4 t 4 4 444^47£(KAERI)44 4 4 4 4 4 ^ 4 ^ 4 7 £ 4 £ SI0M447 4 4 4 £1144 4 4 4 7 £ 4 4 4 4 ^ 4 4 4 4 £ 4 4 7£%v7 4 4 £ 5 ^ 4 4 4 ^

4 AA. xll5}-4 ell 4 4 4 4 4 4 4 4 r SI0M4 Dr. Jun Zhou £77} KAERHl

4 4 4 4 4 1 4 1 4 ^ - ^ 4 7 # 7 5 34Si£4 ) 7*34 4£4#-8r 4 4 4 4:4.

o JL^ 44-4 4-^-4 7 14 $ 4 4 - 500 w ^-4 £-44 ^1444 711144 4 4 4 4 4 £ 4 4 7 £ 4 4 444

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o 444 4444 4 4 4 4 - 500 W -4 1144 444 £ ^ 4 4 4 4 4 534-^*3 4 4 4 # 7 4 4 £ 4

444 t 4 4 ^ 4 £44214.

- 138 -

4. £44 444 4^4 44 3? *14

500 W #4 £#^ 4444 4^-44 444 444 34 2-1334 47i 7£44 444£ 4 4 t 44££ 4°14 44 4444 95% 444 4444 4-b 4444 4444 4441: A4 444514. 34 2 1343 -3-444 44 44£ 444 4444 £44 £47£ ?U4. 4444 44 444 16 mm 4 4, 444 4444 444 444 ^4444 44 4 1.5 mm4 44.4 34 4 #44 4£4, 444-(ftow tube)4 44 11 mm 444 744 44 444 %l^ 7£44

4 4 7 £

3^ 2-1357 444 4*35 444 444 44 £44 £47£ SXA. 4 44 4^4 444 44 6 mm x 44 173 mm 44, Nd-3 at. 4£7 0.6% 44-47144 °d44fe 444 44 44(barrcl)4 4444 44 34 2-136 44 4 444 4444 444 444 444 4444 £4€ 500 W #4 *H4 £€4 £44 £473 44.

- 139 -

4 2-134.. 7 4 4 4 4 4 4 4144 4 4 4 4 sA

3 4 2-136. 500 W-? 4 4 4 4°1*14 £ ^ 4 £ 4

- 140 -

4. £ 4 3 4 4 4 4 4 4 4 4 4 4 4 4 £ 4 4 4 £ 4 4 4 4 4 £ 4 4 4 , ?141Nt 4 4

4D t r 4 4 4 4 4 4 4 dm = 5 cm, 4 4 3 4 4 4 4 70%44 4 4 4 4 ^ 4 4 ^ 4 6 mm 4 4 4 173 rnm4 4 4 4 4 7 4 4 4 4 4 " l £ 4 4 4 ^ 4 $ 4 . 4 7 l # ^ 4 ^7\°\] rx} - o3<g^j|. /1]ALC-}O1 z±4 2 137 1 4 4 4 & £ 4 , 4 4 4^£4( l / f )4 4444(Pin)4 4 4 £ l/f - 5.34 p£n - 1.74 £ 7 4 4 4 . 4 4 & 3 i a ^ £ 4 4 4 4 4 4 4 4 4 ' ^ 4 4 4 4 4 £ 4 4 4447r 4 4 4 4 2 1 4 .

4 4 4 4 # 4 1251 W 4 4 4 4 4 4 ?-47l4 4 4 £ 4 4 4 ^ 4 4 4 4 4 4 4 4 4 « # 4 4 4 4 4 ^ 4 i£°-544 17 cm 4 4 4 4 4 4 4 4 4 4 4 4 # 4 4 7 } ^ 4 4

6 -

Ceramic Rod, 6 mrruf> x 173 mmL - Linear Fit of 1/f Output Coupler, R = 70%

V - V

Input Pump Power ( W )

3 4 2-137. 4 4 4 4 4 4 4 4 4 70%-g- A- AAA AAA ■A$ NiYAG 4 4 4 4 4f£"4 4-^ 1 4

4 4 4 4 4 £ £ 4 °}4444 W 4 4 4 4 4 4 i 4 ^ 4 4 ^ ^ 4 ^ %.AA 4 4 4 $ £ 4 3 7444 3i% 2-1384 4 4 4 ^ 4 . 3144 4 4 £ £ 4 47} 447} 25 A4 4 30 A, 35 A, 3 4 £ 40 A5 47}t4 4 4 ^4-^4 4 4 4 4 4 4 4 °4 7 4 4

- 141 -

(a) 25 A (b) 30 A

(c) 35 A (d) 40 A

34 2-138. 44M4 £444 4^4 44 444444 <14 4 4414

4. 444 444 4 4444

34 2-1394 S°l 500 W i-4 444 444 £44 4444 #4-^^ •4714 7443 4444 ^4444 £44?34.

3^ 2-139. 34-4*3 ^44* 444 500 W 444 444 ^44 4 £4

34 2-1404 44 44 444 60%4 4 444 444 444 4474 4 444 4-€ 44 4 44 4 44 44141: £47£ TU4.

- 142 -

Laser Oulpul ( dm = 11 cm. T = 19 'C. R ■ 60% ) Laser Culpul ( dm = 5 cm, T = 19 °C R - 60% ) Laser Output ( dm = 5 cm, T * 15 °C R = 60% )

3C0 600 900 1200 Input Pump Power ( W )

3 ^ 2-140. 4 4 4 4 4 4 44, ^ 4 7 4 4 £ 4

o 3 4 2-1404 44MI 4 4 4 4 4 4 £ 4 5 . 4 4 4 4 4 4 4 7-147} 5 cm, # 4 ^ 4 4 4 4 70%, ^ 4 7 4 -&£ 15 £, 4 4 4 4 4 4 44.4 Ndt3 4 £ 0.6%, 3 4 £ 4 4 4 4 ^ 4 4 ^ 4 6 mm4 £ 4 4 4 4 4 4 4 4 4 4 4 4 4 542.3W4 45134, 4 £ 4 4 500 W t £ 4 ^ A r j 4 ^ 4 . o o]un ^144 44,2 .^4 4 4 ^ 4 £ 1392.9 W4£5. 4 4 4 2 - 4 4 4 4 4 542.3 W7 4 - 4 4 4 ^ : 4 39.5%4 £ £ 4 4 4 4 4 4 .

300 6DC 900 1200

Input Pump Power ( W )

o.% 2-141. 4 4 4 4 3 4 4 4 4 4 70%, 4 4 4 £ 4 5 4 4 el]44 4 4 4 4 4 44 5 cm, ^ 4 7 4 4 £ 15 °C44 4 4 € 4 4 4 4 4 47}*f 41- 4 4 4 21144 4 4 4 4 4 4 4 ^ 4

- 143 -

4.2. g^45)|0|4 41J

7\. 4

4 4 4 4 4 4 411 4 4 4 4 7 SIOM4 Dr. Jun Zhou £-74 KAERI4 4 4 4 4 4 1414 4 4 4 7 4 7*34^4. 10 w^- 4 4 4 4 4 4 4 4 4 £.-§- 4 4 4 7 4 7 4 ^ 4 S H 7flM> £-^-0114^ D-f (350/400 /jm dia.)4 4 •44

A A 4 4 4 $7} 4 4 #sfl4 4-445. 7 4 4 15 w-g-4 44 ££-4 4 4 4 4 ?iA 4 4 4 4 4 4 4 4 4 4 4 1 4 fe4 £ 4 4 4 4 4 4 4 4 4 4 4 € 4 74 A 414 3.43 4434 4 4 44447} 4 4 4 4 4 4 £ 4 £ ^ 4 4 4 ^ ^ 4 4 £ 4 4 t 4 . loo w^ 4 ^ 4 4 4 4 4 4 4 4 4 ^ 4 t 4 4 4 J 4 4 4 4 4 f e 100 V\4r 4 4 4 4 4 4 4 4 4 4 4 £ 4 ^ 4 4 7*34$£4, 20 W 4 4 4 4 4 4 4 4 4 4 ASXA-

4. 10 W-3- 4 4 4 4 4 4 4 4 4 £ 4 4 4 4 7 4 7 4 4 4 £ £ H*&

10 W-S- 4 4 4 4 4 4 4 7 £ ^ 3 ^ 2-1424 AA. 4 4 35 W(@46 A)4 4 4 4 975 nm4 4 4 4 4 4 7}4£ eil44 44££(Apollo, C35-975-0)# 4 4 4 ^ £ 4 , D-*S (350/400 //m dia.)4 4 4 4 4 4 4 4 £ 4 4 4 ^7} 4 4 # 4 4 4 4 4 7 } 4 4 4 4 ^ 5 4 4 4 S 2 4 . 4 4 4 4 4 £ £ - 4 4 4 4 4 ^7} 4 4 4 4 4 4 4 4 4 4 4 1 t fe4 £ 4 4 4 4 4 4 4 4 4 4 4 ^ 4 ^ 4 4 4 , 3 4 £ 4 4 4 1-4 444s}7V 4 4 4 4 4 4 £ 4 £ 4 4 4 4 ^ 4 4 4 £ 4 4 ^ 4 .

HT@975 nm HR@1 um

Laser Diode Coupling @975nm Lens

Yb~doped DCF

3 ^ 2-142. 15 W-g- 4 4 4 4 4 4 4 4 4 4 7 4

- 144 -

4 3_44£4 £ ^ 4 4 4 4 f = 25 mm, 30 mm, 3 4 3 35 mm £ 4 4 4 4 4 4 4 4 4 OT(launched)47 4 4 4 4 4 4 4 4 $ £ 4 , 3 4 4 - t 3 4 2-1434 4 4 4 $ 4 f = 35 mm44 4 l t S . 4 4 55.3%, f = 30 mm44 62 %, 3 4 3 1 = 25 mm44 57.7 %£ 4 4 4 & £ 4 , ^ £ 4 AR £ 4 4 4 4 1 - ^ 4 ^ £ 4 4 ^$\7\ <>\)A&A.

25

2 0

• f = 35 mm, Coupling Eff. = 55.3% * f = 30 mm, Coupling Eff. = 62% ■ f = 25 mm, Coupling Eff. = 57.7%

■:♦

10 "i r

15 25 20

LD Power (W ) 30 35

3 4 2-143. AA. ^ t 4 £ 4 pt14 447} f = 25, 30, 35 mm 4 7i 4 4 44(launchcd)€ 4 4 4 ^ 4 £ 4

40

4- $-*) ) o n

4444 74A7\ 30 m 4 21 m 4 4 4 4 4 4 4 °J44 4 4 4 ^ 4 444 4-S-

4 4 4 444 444 4 4 4 4 4 £ 3 441- 3 ^ 2-1444 444&4 74 w 34 4 # 4 444444-1 4 4 4 7 4 4 44 aJ4 4 ^ 4 4 4 4 4 47-444 4 4 4 30 m 4 £7} l £ t 4 £ 4 4 4

- 145 -

18

16

| 12-

g 10 u_

I 8 i - 6 -<D (/> - I 4 ^

Laser Output, I = 30 m Laser Output, I = 21 m Coupling Lens, f = 30 mm

25

Launched Pump Power ( W )

4 2-144. 4 ^ 4 fAA 30 m 4 21 m °4 34 4 4 4 4 4 4 4 44 34 444 4 ^ 4 4 4 444 4 3 4 4 4 44 1 4

:±4 2-1454 AA 4 4 4 #4 4 4 § 4 4 4 4 4144 4 4 4 £ ^ £ ^ 4 4 4 £ 4 4 4 £44514. 7 44 4 4 4 44 4 4 4 $ £ 4 , 4 4 4 4 4 £ f 4 4 4 4 4 4 18.92 Wi 44A q% Di = 133 mm 4 4 44 1-4 441: 4 4 t 4 4 4 4 4 3 4 4 4 4 4 4 4 4 4 4 2.44 67.8%, Di = 133 mm £ 4 £ IVf 153 mm4 7 -7114 4 4 4 4 1 4 4 4 7 68.2%, 34 £ Di = 133 mm4 LV} 88 mm 4 4 4 4 7 68.4%£ 4 3 4 &

3 ^ 2-1464 4 4 4 44 4 4 4 4 4 7 4 444 4 ^ 444 434 4 4 4 4 4 4 l!4# 444514. 4 3 4 4 4 1 4 4 44-M4 4 4 ^ 4 4 4 A 7 $J£4, 4 3 88 mm4 4 4 4 4 4 44 447}4t4 £ 4 4 4

- 146 -

Oichroic Mirror

LD

D,

Yb-doped Double Clad Fiber

Lens BS

Coupling Lens

Fiber Length : 30 m Fiber Roll Dfameter: D, = 31 cm

D 2=31, 15, 9 cm

QD Power Meter

Spectrum Analyzer

34 2-145. 444 1-4 43 444 4B 4144 44 ^ £4£4 £4 €$ 44£

I o a.

i a "3 O i_ a> W <0

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12

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■ D = 88 mm, 9 turns

* D2 = 153 mm, 5 turns

D =310 mm

6 8 10 12 14 1 Launched Pump Power(W)

18 20

3 4 2-146. 444 44 43444 4^- 4144 #4 4 4 4^14 . 44444444 4-4 445-4

- 147 -

4AA 4 4 4 4 4 4 4 250-1300 nm4 4444-1^ 4 7 600 1/mmS] $\A 4 4 4 CCD(Andor, DB401-UV)7} 4 4 4 l/8m 4 4 4 (Oriel, MS125M 4 4 4 4 tLA^i c

" I 4 $ £ 4 , 3 4 2-1474 £ 4 4 4 4 3 4 4 £ £ 4 4 4 7 £ 4 4 7 4 4 4 4 4 ££7} 4 4 4 yev444 A 7 AA. 4 3 4 310 mm44 88 mm£ 4 £ 4 4 4 4 4 4 4 4 4 44£fe 34^1 4 t 4 £ 4 .

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D2=38rnm, Stums

D2=153mm, Stums D~=3l 0mm

Launched Pump Power18 92W

1080 1090 1100 1110 Wavelength(nm)

1120

3 4 2-147. 444 44 43444 4 ^ 444 £4§JJ 4 4 4

4 100 w-3- 4 4 4 4 4 4 4 4 4 4 4 ^ 4 ^ 4 4 4 4 4

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- 148 -

3 4 2-149. 4 44 * 4 4 5 4 4 4 4 3144 wd 4H

- 149 -

3 ^ 2-1504 4 4 4 4 4 £ £ 4 7 4 4 4 4 4 4 4 41- 4 4 4 4 4 £ £ 4 4 4 4 4 # 4 4 4 ^ 4 4 444524.

LD Laser Output @ T = 19 °C

i—■—i—■—i—'—i—■ r~ 10 15 20 25 30

LD Injection Current (A) 35 40

£ 4 2-150. £1144 44£-£4 7 4 4 # 4 £44 4 # 3 4 4 4 4 1 4

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- 150 -

3 ^ 2-151. A<4 474 3!£f- 4 4 4 100 W -a- 4 ^ 4 444

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10 12 14 16 LD Injection Current (A)

3 4 2-152. £444 60 mm4 44 474 4£ 41f"4 # 4 4 4 344 3144 44££74444 4 4 4 4-2- 4 4 4 444 44 £ 4 44 1 4

A°4 4 7 4 €£- t 4 4 4 4 4 4-14 £ 4 4 ^ 4 4 4 4 4 7fl444 4 4 4 3 ^ 2-1534 4 4 ^ 4-44 4* f t44-& -M44^4. 4 4 BJ£ ^ 4 € 4 4

- 151 -

4*114 4 4 4 4 4 NAO.354 4 7 4 4 £ 4 4 4 4 4 4 4 4 ^ 4 44344 4 4 7 7 £ 4 4 .

I Diode stack @975nm

HT@975nm Y b . d o p e d D C F HR®lum

*

: ^ spatial filter Aspherical lens

Laser out

4 2-153. 100 W $ 4 4 4 4 4 4 7 4

- 152 -

4 4 4 4 4 4 4 4 4 £ £ 4 4 4 spin-photonics 4 4 44 .4 ^ 4 f - £ 4 4 4 4 144 MPC (magnetic photonic crystal) 7 £ 4 4 ^ " 4 4 6 3 4443 4 4 4 4 - 4 4 As £ 4 4 £ £ i N 4 4 , 4 7 4 4 7 £ 4 4 4 4 4 4 4 4 4 7 £ 4 A 4 4 4 4tr 4 4 4 4 ^ 4 4 3 4 4 i t £ 4 4

1 4 4 £ 4 4 spin-photonics 4 4 4 4 4 4 %^4A 4 7 ^ 4 4 4 4 4 £ 4 4 4 7 1 - 7*344. 4 4 4 4 # 4 4 £ 7 Heusler ff-g^l ^ ferromagnetic, ferroelectric, ferroclastic 4Ai 4 4 4 4 4 27}4 4 4 A A multi-ferro material -g-4 $134, 4§ 444 44 444 £74 M^lf 4444, 444 4441-44££ 4s.# 444 4 44447£, 41 ^ 44^ 444 4AJ, 44 44 474534

244£4fe 144£4 47141- 4 4 £ £ 2 - 37)14 4441- 4 4 4 4 4 1- 4 4 4 4 4 4 4 7 £ 7 4444 , ^.4 ^ 444 4 4 4 4&J £ 4 4 ^ 4 4 4 4 4 4 4144 474534. 44, 44 44 4^244 4 4 444 MPC 7 £ # f ^ t 7 $X^ 44A^ 4 4 4 4 47 ^ 41- 4 4 £ £ 4 4 4 4 4 4 4 4 4 4 4 f l ^ 47£ 4534$4. 44 4 4 4 4 4*J-44f 444 A^A 4 4 4 4 p-s ^ 4 ^ ^^i^-2-c^ ^ ^ ^ o i 433£, £ 4 4 4 4 4 44M- 4 4 4

4 4 1 4 4 4444 7 £ 44 4 4 4 4 4-^4 4 4 1 4 4 As 4144 44 4534.

Ni2MnGe Heusler ^ 4 4 4 ^ 4 AA%^§ ^ 4 4 4 , La-Ca-Mn-0/BaTi03 ^ La-Sr-Mn-0/BaTi034 CMR/443 multi ferro 4 4 4 4 £ 4 7 £ % 4 4 3 4 £ Er-doped H ErA'b-codoped 4 4 4 ^ 4 4 4 7 4 4 4 4 4 - 4 ^ 4 4 71- 4 4 7 « 5 3 £ 4 4 7 2 4 4 £ 4 MPC 4 4 4 4 4 4 7 £ 4 7 1 - 4 4 4 4 4 4524. 444 4^ 4-47£4 4^ 4 44*1 444 44 AAA 44 44 444

471- M 7^4^4.

7}. Ni2MnGe Heusler ^ 4 4 4 4 7 4- CMR/444 multi-ferro 4 4 4 4 7 4. Er-doped % Er/Yb-codoped 4 4 4 ^ 4 7 4. MPC 44 44447£ 4£ 47 4. MPC 44 44447£ H-$ 47 4. £4M. 4. 44£44 24 4$

- 153 -

5.1 Ni2MnGe Heusler ff^^SfTll ^ 4

4. 477^4HJ A 4 4 477444] 7 4 4 4 n i4

* Flash evaporation * 4 4 *H2: A 4 4 4 £ 4 4 A

4 ^ 4 4 * SQUID ^ ferromagnetic

resonance (FMR) jll- J=L J^-^-A^

* 4 4 4 4 4 4 4

* Ni2MnGe Heusler 4 n " 4 4 4 £ * 4 4 4 7 £ 7 4 4 £ 4 7 4 4 4 4 4 4 4 £ 1

150-730 K £ 4 4 4 4 3 , 4 £ 4 650 K 4 4 4-7 <M44£ 7 f

* 4 4 4 0-100 Oe4 4 4 4 4 4 4 £ 4 £ 4.2-300 KA 4 £ 4 4 4 4 4 4 4 4 . 4 4 4 AsA^*§ ^ 4 4 4 £ £ 4 7 1 - AA. F M R 4 4 4 4 4 # 4 4 4 4 4 H £ 4 4 4 4 4 4 £ 4 4 . 4 4 4 4 4 0.5-5.3 eV4 4 4 4 4 4 4 73°4

4 4 4 4 4 polanmetric Beattie^££ 4 4 4 4 ^7£ -I o

* 4 4 4 € - 1.1-5.0 eV4 ^ 4 4 4 4 4 4 4 0-950 :° ul 77° £ Oe4 4 4 4 4 4 4 p - 4 4 &AAA

4 4 4 4 dynamic tiov^££ 4 4 4 4 4 equatorial Kerr Jl 4 1 - 4 4

4. Ni2MnGe Heusler 4 ^ 4 4 4 4 £ 4 4 4 # 4 4 4 4 4 4 7 1 4 o Ni2MnGe Heusler 4 ^ 4 4 4 4 4 £ o 4 - 4 4 7 £ 4 1 4 £ 1 - 4 7 4 4 4 £ ( 3 4 2-154) o £ s 4 £ £ 4 4 4 4 4 4 4 4 7 4 4 4 4 ^ 4 4 ^ 4 £ , 4 4 4 4 £

^ j £ 4 UV 4 4 4 4 4 4 y J £ 4 4 7 7 } 3.4 4 4 ( £ 4 2-155) o 7 £ 4 ^ 4 £ 7 f 4 4 Ni2MnGe 4 4 4 4 4 4 £ 4 £ £ 4 4 4 4 £ 4

4 Ni2MnGa ^ Ni2MnIn4 1 4 4 £ 4 4 4 4 4 4 4 4 3 , 3 4 4 4 4 4

- 154 -

d

(220) (a)

(3U)

" t t f t

(422) (400)(420)J\m3) ((40)

(331)

w4 YVA

v,

(b)

t~*1*'V»~»rvv*w.

60 90 26 (degrees)

3 4 2-154.. NbMnGe (a) ^ 4 4 4t? 5! (b) 441-4 x 4 4ll 44 44

V * > /

S M , V ^ A ^ " V ^ ^ V A - ' ^ V ^ v

''^Ww 3

60 26 (degrees)

90

£ 4 2-155. (a) NizMnGe fl-g- ^ (b) Ni2MnGa, NWnlri, NizMnAl 4 4 1 4 4 4 £ £ 4 4 : €4

- 155 -

5.2. CMR/2J^E! multi-ferro ^ 4 1 ^ r

7}. 477-3)44 A 4 4

^44 7 4 4 4 44

* Soft-target 4 4 rf magnetron sputtering * X-4 s\A £4*fl 4 4

4 4 444

* 44 probe, SQUID

magnetometer

* AAA?}AA

* La-Ca-Mn-0/BaTi03 31 La-Sr-Mn-07BaTi034 CMR/444 2 4 4 4 4 £

* Cu KQ X 4 4 4 4 4 4 4 £ 4 ^ - 4 4 4 low- 4 high-angle X-4 4*4 4 4 4 4 4 € 4 7 £ 4 4 . 300 kV4 4 4 4 4 4 4 4 4 4 4 4 4 ^ 4 4 4 0.12 nm£ T> 7 £ 44

^A * 4 4 4 ^ 4 44-probe 4 ^ £ £ 4.2-300 K4 ^ 4 4 £ ° J 4 4 4 3 4 £ 0-5 T 4 4 4 4 4 4 4 7 * M £ . 4 4 7 r 0-100 0e4 4 4 4 4 4 4 3 4 £ 4.2-300 K4 4 £ 4 4 4 4 4 4 4 4 , 4 4 3 4 4 4 4 £ 4 4 4 £ 4 £ 4 4 4 4 4 ASA^ %% 4 4 4 £ , £ 4 7

* £ 4 4 4 4 7 } 4 7 l 4 4 % v 444 PES, MCD, XAFS, SPEM

4 4

f 44 4 4 4 4 ^ 4444 44-7£, 74 4 £ orbital ^ spin 44£*QJ=, 7 £ 4 4 % 447£ f 54 4 £ 4 £ 44 4 4 4 £ * §?443 4444 , 4 1 44 •37^444 4 t l

- - r £ 4 4 LaAlOa 4 4 4 £ ^T

4. CMR/7j-^-4 multi-ferro 4 4 4 4 £ 4 7 £ ^ # 4 4 7 ^ 4 o 4^1 7l]t4- soft-target 4 4

La-Ca-Mn-O/BaTiOs ^ La-Sr-iMn-0/BaTi034 CMR/444 2 4 4 4 4 ^ 4 £

o 4 4 4 BaTi03 4 4 4 4 4 4 CMR44£ 4 3 4 4 7 A A 4 4 4 £ £ ^ 4 4 4 4 ^ 1 , 74 44£ 4 4 4 ^ 4 4 ( 3 ^ 2-156)

o CMR/444 4 4 4 CMR/4£4 4 4 £ 4 £ 4 4 4 4 4 4 4 4 4 ( 3 ^ 2-157)

o Mn-O-Mn ^ - ^ 4 4 4 4 4 4 4 4 4 4 4 4 4 , CMR44 £ 4 4 * 1 4 Mn-0 1 ^ 4 £ 4 4 4 4 4 4 4

o 4 4 ^ 4 4 4 4 4 4 4 4 4 4 4 4 4 4 £ 4 ^ ^ 4 4 7 } 4 ^ 4 ^ 1 4

- 156 -

4, 47 4£4 444 4714££ 4^-444 4444 3 444 44 44444 £44 ^444 4^ ^ 447£ If- 444£ 4

o La-Sr-Mn-0/BaTiOs 24444 4£ 47144 44 44 ^44 4 4/444 ^4 multi-ferro 44 4iH 4^£4 14 44

0 50 100 150 200 250 300 T(K)

3 4 2-157. LCMO/BTO (1) $ LCMO/LAO (2) 4444 4^44 44 £4

- 157 -

5.3 Er-doped ^ Er/Yb-codoped I f S M i ! "34

7}. 477*34-4 ^ 4 4

4 . Er-doped % Er/Yb-codoped 4 4 M 1"4 4 7 4 4 4 ^ 7 ^ 4 o 4 7 4 4 AAA £ 4 4 £ # 4 4 ffi^Ap 4 4 ^ 7 4 4 7 4 4 4

4 4 4 4 4 4 £ 4 4 4 4 4 7 7 } 7 4 4 o 4 4 4 Er 4 Yb £ - ^ 4 4 £ Er-doped4" Er/Yb-codoped soda-silicate

laser glass 41 £ o Er-doped glassfe 0.5 at.% E r £ 4 4 4 4 1536 n m 4 4 4 PL4l7l7} 4

rl]7} 4 4 , 3 £ . 4 4 0.144 0.8 a t%£ 4 4 4 P L 4 3 4 FWHM£ 18 4 4 26 nm£ ^ 7 } ( 3 4 2-158)

o Er/Yb-codoped 4 4 4 ^ - 4 PL41714 E r £ 4 4 0.5 at.%0^ 4 Yb doping££ 4 4 4 4 ^ 4 4 £ , 1536 nm°1144 PL^7l7} 21^7} 4 ^ Y b £ 4 4 30 at .%44 if 4 ( 3 ^ 2-159)

o Yb4 ^ 7 H 4 4 P L 4 £ 4 4 $ 4 4 , Yb£4 4 6.0 at.%7} 4 4 80 nm4 FWHM7} 4 4 4 4

o 4474 PL 44 4444 343 PL 4444 47 ^-A 44

- 158 -

Wavelength (nm)

3 ^ 2-158. Er-doped glass4 PL 4 4

10CO rOcO

Wavefeojjtti {rim

3 4 2-159. ErAb codoped slass4 PL 4X3

5.4 MPC 7IS!- c f g s j - ^ a *fl£ 2 7

4. 477*14^ £ 44

4 . MPC 4 4 4 4 4 4 7 £ 4 £ ^ 7 4 7 1 4

o ^ 4 44-0] 600 nm^ 4 , Ti024 Al20344 # * H 4 4 4 2.30, 1.674 4 44

- 159 -

4 4 4 * 3 A^ (4€-4 - ^ 4 A^rA'U) -4144J 4 4

Face-to-face double-pair target sputtering ^ £ 3 4 4 rf-magnetron sputtering 4 444 44441 44

* aVT3V r x ^ i . « A - 1 - i - i 7~>- U7 —i

S.A %<$ AA

AI2O3/T1O2 4 4 4 - 4 : £ 3 4 4 rf magnetron sputtering 4 ^ 4 4 , 4 4 2] 4 4 4 4 4 4 4 4 £ , 4 £ 4 ° 4 , 4 4 4 £ £ ^ AL03/Ti02 4 4 44517 4 4 : 1, 2, 5, 6, 10 Fe/Au 4 ^ 4 4 •' face-to-face double-pair

target sputtering 4"^ 4 4 , Fe44 7^111- 3 nm£ 31A, Au#4 44f - 1-3 nm£ 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 £ 4 4*11-1- 4 4 FexAui.x (x=0~l) t^-444 4^4 44£444 44 High-angle ^ low-angle x-ray diffraction

Atomic force microscope 4 4 o 44-0II 4-i- 4 4 4 4 ^ 4 4*11 600 nmoll bandgap4 ? 5 f i } 5 4"^4

4 4 4 4 4 o 44711^4 £ £ £ 4 4 4 4 4 4 4 4 £ 4 ~4AA 4sz 4 4 ( 3 4 2-160)

n(TiO2)=2.30@600nni n(AI2O3)=1.67@600nm \

—•— Experimental data

—o— Simulation data (Al,O/80 rm imOj lWnm I] 6-/0a ss

300 400 500 600 700 800 900 1000 1100

Wavelength (nm)

3 4 2-160. 1 4 4 4 ^ 4 4 4 4 4 4 ^ 4 ^ 4 4 £ 4 4 4

- 160 -

5.5 MPC 7|£! c l § 4 ^ 7 5 § ^ 3 7

7}. 477*nVl3 $ 4 4

(4^4 -M^^^e W<J43)

* #!4§

* 4 4

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4 4 4 4 4 **■!■, 4 4 4 , 4 4 4 41- 4 4 4 4 4 4 4 44

* Spectroscopic ellipsometer-i- 4 4 4 4 Fe/Au 4-444 ^ FexAut., ^ 4 4 4 # 4 £ £ 4 ^ , 44H4 ^ *147£ 741-41.44 4 £ 4 4 4 4 4 4

71) 7 £ 4§u * Vibrating-sample magnetometer 4 4 4 4 4

hysteresis 4<3 4 ^ * 4 ^ # 4 4 : 248-1130 nm (5.0-1.1 eV) ^ 4 4 4 44 * til^ %*}<>§ : fg-laser ^ 4 4 4 800 nm44 4 4 * 4 4 4 ^ 2 4 4 4 4 ^ 4 4 4 4JI £ 4 4 4 £ 4 £

S 4l£ 4 4 £ ^ £ 4 4

4. MPC 714 Fe/Au 4 4 4 4 ^ FexAui.x fj-#44 4 4 4 7 ^ 4

o 4 ^ 4-44 %-A ^ 4 ^ 4 4 4 4 4 4 44-2 ^ 4 £«)££ 47)7} Fe£4 4 4 4 4

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4 4 4 £ 4 ^ 4s x}4 £i$£7} 4 4 2.21 % 0.224 yB££ Feofl 4 n 4-44££ €■ &4 7>44 S 3 (£42-163)

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- 161 -

A*o. OOAfalOAAol J AAr-fJOAFo'MA.Au).)

paA«..(3(IAFe-55*Au)] PMA».-(»AF*30A/S4i)j

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700 710 720 730 740 Photon energy (e V )

3 4 2-163. Fe-Au t r ^ 4 4 4 4 4 4 4 2 4 4

5.7 4 4 4 £ 4 4 24 TI^I o 4 ^ 4 0 3 ^ 3 4 5 3-s., 4 4 4 4 £ 4 £ 4 4 4 4 4 4 4 4 4 4 £

4 4 4 7 ^ §■■§• 4 4 o 4 £ 4 4-1 4 £

O O □ £ "5?xl 15- 4 4

- 162 -

- 4 £4 4 *i : The 2nd International Symposium Science and Technology - 4 4 - 0J4 - 4 £ - 5£ j - 4 - ^

: 4 4 4 4 # : 2004. 8. 21 -24 ; ^\37- 4-§- £ £«i}g 20$, £££"! 364

4 4 ^ 4 ^ 1 % f 4 £ ( 4 ^ 4 7p-l

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on Advanced Photonic

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- 163 -

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4 4 4 4 4 £ 4 4 4 4 4 4 4 4 4 inhomogeneous 4 ^ 4 4 4 4 4 3 4 ^ 3 . jr.44 ^ 4 4 4 ^14 sfl- -a- 4 4 4 4 4 4 £f_4 4 4 4 5 1 3 , 4 £fl 4 4 4 £ £ 4 program££ SG II, KFL (KAERI Laser Facility)0) 4 4 4 ^ 4 . £ 4 4 4 4 4 4 4 4 4 4 4 44,11, B-factor# -§-44 41444 4 4 ^ 4 4 •£■

- 165 -

http://5jt6.nl

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- 166 -

CPA is THE big development

bispei*sivfe daisy iiiw

S Mourou and coworkers 1985

omprcssiM

We can stretch the pulse by a factor of 10,000, amplify it, and then recompress it'

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34 3-64 44-4444^344 4^ 44 Nd:Glass 444 ^444 4 4 44 44 4 444 4^ 444 4444 444 4£4 444 444. 44 4 4444 444 44 44 44 4 i ^ 4 4444 4444 4444 44 4f 4 4^4 afl-cH] Gaussian 4^4 .444^3 44 ^4 4^4 4444 4 447144 444 4444 444534. 44 4444444 5 J/cm2 44444 44444 4444 44 4°-£- 444 %IA. AA^-S.^ Gaussian*.3. f4 4 4 80 mm 444 444444 4447} 5 J/cm24 3.41 44 10 J/cm24 4^-3 44 ^444 444 44 444-b ^4 444 4444 ^4 4^1- plat-top 3S. 4^44 44 4-S34 44 £ 4 $14.

44-44444:344 4443 slfe 1 kj-g- 444 -^44 43^4 ^4 1- __i 74 444514. ^43.5.44 sA& 4444 444 80 mm 4447} 2 4 5. 4444 3X4 A* 444 #44^ 44=3. 444# ^44^3.4 44 ^4 80 mm 444 ^f-AA 444 4444 5 J/cm24 44 444 4444. 4 % 3144 W c 47}4 80 mm 444 Mf- 4^ 444 fluence7} 3 J/cm2 44^ ft 4 4.4 4-M4 ^-4 444A5. A°3A A 44 43.3. 444 4.

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n^ 3-6. t^4434^i 3144 AA4A rod #4 4444 44 4 4 44 44.

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Dangeioux point

FR a.u ; - IK: 40mm - j ^ C I - ' 6 0 m m •"" K 3X3 / 80mm t - a 5 -) X J — 100mm

14 mJ 6.42 J 5.8 J 38 J 3 5 J 177 J

Out 250 J

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70 J 63 J

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14 mJ 6.42 J 5.8 J 38 J

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Out 250 J

Out 1 250 J

70 J 63 J

.3 3-7. H^-4143 4 ^ #3-4 131. 31 } ^ M l 4 4 80 mm # 4 4 4 4 4 £ 4 4 4 4 4 4 4 4 4 AA ^ 4 £ £ ^Efls. 3M4 ufl^# 71)3^4514.

444 4 444 AA 4444 44s4 £ 444 4444 444 broadband model4 4144514. 4 ^ 4 SL"i4 4 4 4 4 chirped 4 3 4 ^^ 4A3

4 3 : 4 4 ^ 3 , 4 4 - 4 4 4 4 ^ 3 : 4 4 4 4 4 4 4 ^ 4 4 S i 4 . Broadband model 4 4 4 4 4 4 4 -£444 € 3 1 - 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 A.7) 4 4 4 4 4 4 ^ 4 4 4 4 4 1 4 .

4 4 4 ^ 4 4 3 . 4 ^ 4 - b f } ^ 4 4 4 4 ^ ^ 4 4 4 4 4 ^ 4 -M44 4 4 4 4 4 3^.7} A } ^ - 4 ^ O . 4 4 4 4 4 4 4 $ 4 4 4 ^ 4 4 # 4 4 4 4 4 4 4 41 4 4 4 4 4 1 £ t 4 4 4 ^ 4 . 4 4 ^ 4 °^4 ILE44 4 4 4 4 4 4 4 4 ^4 7} Sttfe 4 4 ^ 4 4 ^ 3 4 # 4 4 4 4 4 4 4^-4 44711- ^ 4 4 4 4524.

7flt€ 3 H 4 4 4 4 4 4 4 4M.# 4-3 $14 *fl44 n-sec -^44 A4 * 4 4 4 a^.5. 4 4 € 4 4 4 4 4 4 4 ^ 4 p-sec 4144 4 ^ A444£ 4 4 4 4 4 4 € 4 $i4 444 .

xF-7 = s4 en - L I - H T I_!

[1] L. M. Frantz and J. Nodvik, J. Appl. Phys. 34, 2346 (1963).

[2] Y. H. Chung, L. Zheng, and D. D. Meyerhofer, IEEE J. Q-E 29, 270 (1993).

- 171 -

41 2 dt SG-II PW A}o}A\ ## #^-{f ^Ai\

24. SG-II, PW SE+¥ ^ H

7}. 4 4 4 4 4 4 4 £ 4 4 4 4 4 4 ^ ^ 4 £ (SIOM) 4 444KSG-II) 4 4 4

4-€4 4 4 4 ^ 4 4 4 444(Front End) 4 4 4 4 i | , 4 4 4 4 4 , 4^3.4 ^ 4 4 , 3.43 34 S 4 4 4 4 4 4 4 4 ^ - -7444 9XA. 4 4 4 4144 AkEJ 4 3 4 3-84 £ 4 DFB, AO £ 4 4 4 4 , AAA 4 4 4 , EO £ # 4 4 4 , 4 4 4 4 4 4 , 4 ^ 4 4 4 , € ^ 4 4 4 3 ^ i 1 4 4 4 $13.4, SG-II4 444^(PW) 4144 4 3 ^ 4 4 4 4 4 4 4 5. 4 4 4 3 $14.

Solid-state Amp.

3 4 3-8. SG 114 PW 4 4 4 4-33^4 4 4 4 4 4 %

4. ^-44 4 4 4 414 4 ^-44 \ /4 4 4 4 4 (phase shift)# A^ 4 4 4 4 4

&4 Yb-DFB 4447} 444S24. 4 4 4 4 4 Yb-£44 AAAA 4 4 4 4 4 4 4 4:44 4 4 4 4 4 4 4 4 4 4 4445 .4 ^.4 4 4 4 ,5.1 ^ m ^ ^ 4 A°43.S 4 4 4 4 4 . 4 4 4 4 cutoff 4 4 4 907 nm44, 975 nm44 68 dB/m4 441- £44.

4 10 cm4 ^ 4 4 A A Bragg 44(grating)fe 193 nm4 4 4 4 A A ArF 4 4 4 4 41444 4 4 4 4 SIOM 4 4 4 A44 4445S4. DFB- *H 4 4 4 4 3 3 ^ 44(period)7} 3.7 ^ m44. Yb-£4€ 4 4 4 4 4 4 AS7}

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s^44 ^444 444 3444 $l°-4, 444^4 20515 3444 $13, A 444 44 444 ttstp] $44 44 31^^ 44 ^444 $14.

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34 3-9. F--P 4^44 444 44£ 44 4

34 3-10. F-P 4444 444 444 4°

- 173 -

4 3 5 . 44" 543442-44-444£(LLNL)4 NIF(National Igmtion Faality)4 4 4 4 - £ 3 4 114 AA 4 ^ 4 DFB 4 4 4 4 4 4 1 - 4 4 4 s 4 4 4 4 . 4 4 4 4 4 4 SL*} 4 4 4 2.8 ix m, 4 4 4 4 4 4 4 4 20 mW 4 3 , 4 4 4 4 4 4 4 0.01 nm4 4 £ # 4 3 1052.91 nm4 5>444 AA. 4 4 4 4 £ 4 4 Kaifa4 Isolator4 4 4 4 3 $14-

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3 4 3-11. LLNL4 NIF4 4 4 4 A 4 4 4 4431 -?£

4 1144 444 1^4

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AAA 4 4 4 4 - 4 4 4471 (Acousto-Optic chopper)! 4 4 4 4 €32}

- 174 -

4 4 4 , 4 4 4 4 ^ AO-s .4444^ 44- Gooch-Houscgo AA 41444-. 4 4 4 €&*= 2.5 GHz4 4A^4 7 J t 4 PIN 5 S 443.n l - 4 4 4 4 4 4 4 3 $1 $134, € 3 4 4 3 4 3-124 AA 4 200 ns44, 4 3 4 44^^:- 1%445. 4 4 4 4 . € 3 4 AA3- # 4 441H4 4 5.5%44, 4 4 4 4 4 24 4 4 4 4 4 4 4 A°4 4S.H4 4 4 4 3 $14.

NIF4 444-3 A-0 £.44441- 4 4 4 4 4 4 4 4 4 4 3 &4 ^ 4 4 4 4 4 4 4 .^444 , 4 4 € 3 4 4 4 100 ns, € ^ 4 4 4 4 960 Hz44. AO H.1-4444 4 ^ 4 TeCfe £ . # 4 4 4 4 4 4 4 4 4 4 4 42:44. AO fi.444 4 4 14 4 € 4 4 4 4 4 4 4 , 4 85%4 4 € £ 4 4 4 ^ 4 . AO S 4 4 4 4 4 4 4 4 4 14 ^ 4 4 4447-1 4 50 dB4 44(isolation) H 4 t A^A.

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AO 4 4 4 ^ 4 4 4 4 4 4 4 14 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 f-444 4 4 4 4 4 4 4 4 4 4 4 ^ 975 nm4 4 4 4 4 4 250 mW4 4 4 4 4 4 #fe AAA 44-2334 4 4 4 4 4 4 4 . ^443.5 . 4 4 4 4 4 4 4 4 4 ^4?Hi 444 %s}^ ^ 4 4 #43 .5 # 4 4 7}444, 4 4 4 4 4 4 4 4 t e ASE4 4 4 4 4 4 4 4 4 4 4 ^?144-t ^ 4 4 4 4 4 443- 4 4 4 4 4 4 4 4 4 4 4 4 ASEt- 4 4 4 ^ 2:4^ $14. £ 4 4 4 4 4 4 4 4 4 ^ 4 3 4 ^ 4 4 4 €41- 4 4 4 4 4 4 4 4 4 4 4 4 4*3.5. 4-H.5. 4*84^- ASE4 4 4 t 43.7} $14.

NIF4 4 4 28 |x m4 s 4 4 4 4 fe 4°^£ \H 4 ^ 4 4 4 4 1 - 4 4 4^3.4, &A 4 4 4 4 4 4:£.g- 4 4 4 4 4 4 4 4 4 2-44(polarization controller) 4 4 4 4 # 4 4 4 4 4 3 $14. 4 4 4 4 4 4 4 4 4 4 4 4 ^ 4 4 (small signal gain)4 500 4 4 4 4 , 30 ns4 4 . ^444 30 ^ j 4 4 4 f.3^44 4-1- ^ 1 4 4 -

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- 175 -

http://443.nl

4 4 € ^ 4 4 3 GHz4 -S.421144 4 4 4 4 4 0.1 nm.4 4 4 4 4-£4 A^444 4 4 4 4 4 4 4 4 %v^44 SBS1- 4 4 4 ^ 4 4 4 AAA. ^ 4 , 4 4 4 4 4 4 4 4 4 -^444 4 £ 4 H 4 17 GHz4 £ # 4 4 4 4 4 4 4 4 0.3-0.5 nm4 4 ^ 4 H 4 ^ 4 4 4 $14. 3 GHz4 444:23} &4 4 4 4447} 4 4 € 4 4 7} $14 3 GHz4 1 H 4 AAAxr failsafe 4 ^ 4 A^3l $14. 4 100 ns4 € 3 4 4 4 4 4 4 4 As.^ optical gate4 4 4 4 4 30 ns4 € 3 4 4 AS^ ^ 14-4.

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4. 4 4 4

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EO £-44144-1- 4 4 4 ^ €3^-^71 (pulse generator)^ NIF4 AWG4 4 4 4 f £ t ^"3 4 3 4 , 200-300 ps4 € 3 4 4 A3. $13, 4 ^ 4 4 4€- 4 44i44 4€-4$S4. 4 4 4 4 4 3 4 ^ 44441i-47l(AWG) Arbitrary Waveform Generator)^ 300-500 ps4 l ^ f t A33. $134, 3.-^4^ 100-200 ps4 € 3 4 4 AA AWG4 &4 447} $143 $«34, 3 .44A 100-200 ps4 € 3 4 4 ^ 4 AWG 4 4 4 4 4 4 ^ 4^- 4 ^ 4 4 4 4 4 4 4-S-443 4.^-4

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&4. 3 4 3-14TT SI0M44 4 ^ t r # 4 4 4 ^ 4 4 4 ^ 4 ^ 4 4 4 4 4 4

43} 4 ^ # j ^ .443 $134, 3 4 3-15TT 4 4 434%^i-Aij7l (electrical-pulse-shaping generator)4 4 2 : 4 .1.1443. $J4.

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- 177 -

1 2 Time/ns

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3 4144 4 f^7](solid-state amp)r NdTLF 44 4 SL&& 4-§-44 4 44$14. € 3 4^(QCW) 4144 4 4 ^ H # 4 4 4 3 ^ AAAA 5 4 ^ 4 4 444-fe ^ ^ i 4 3 $134, 4 4 4 4 # 4 ^ 4-5 kW 4 ^ 4 . 4 4 4 4 4 3 . 3 fe f - ifl Tsi ^)44$134. 44€: <800 nm 4 ^ 4 . 3 4 4 4 4 4 44-S- 1053 nm4 4, 1 Hz44 ^ 4 4 4 . 4 4 # 4*114 TE-coolerf- 4-8-4^ $1$14.

3 4 4 4 4 1 ^ 4 4 4 4 4 4 4 4 4 4 4 4 444A nj 4-5-44, #^f 7l# f-44 ^ 4 ^ # 4 41444 4 4 4 r r 10 ^ J 7§£44. 4 4 3 . 3 - 4 4 3 4 4 4 4 1 - 4-B-4 45.-S- 4 4 ^ 4 1 - 4 ^ 4 $1$134, 20-pass # 4 4 7}^ 4331- ^ 4 4 ^ 4 .

- 178 -

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4*4^44 e7l 741 -74i(Shanghai Research Institute of Optics and Fine Mechanics, SIOM)44 Aiktf-SL $XA 4 4 4 ^ - 4 4 4 " : chirped pulse amplification (CPA)4#4 4 4 4 4 4 ^ 4 4 4 4 4144^-4 2 4 4 4 AA 4 4 4 3 $14. Q4, CPA4 4 4 4 4 4 4 4 4 H 4 4 ^ 4 4 4 4 ^ 4 4 4 4 A 4 4 , 4 3 SM4, 4 4 AÂ, 344 ^ A^-A, 1 3 4 4 4 AA 4 4 AÂli 3.4, 1 3 4 ^ 4 1 - 4 ^ S i r 4 3 $14. 4 4 4 4 4 4 ^ t- 74 433} 4 4 4 3 $13.4, 4 ^ 44-££- 4 4 4 4 4 ^ : 4 £ 4 ,

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4 4 4 ^ - 4 4 ^ 4 4 4 4 4 4 4 4-344 4-8-43- 43-.4 4 4 4 -2-44 ^ Kerr-lcns ^.H-^-4^1 4 4 4 4 . ^ 4 AAA 4 4 4 4 4 4 4 ^-14314, A%-

4 4 4 (Femtosecond Laser COMPACT scries, 3 3 ¥ . 4 4 ) # 4 # 4 3 $1$14 ( 3 ^ 3-I8). 43-4 4 4 4 ^ - 4 4 4 4 4 4 4 4 - ^ T T 4 4 3 3 AAA 4 4 Nd:YV04 4 4 4 (Verdi 10, Coherent)!- 4 ^ 4 3 $1$134, 4 4 #4-& 6 W$ 4. A33A 4 4 4 4 4 ^ # 4 £ 4 650 mW$34, 4-3~i-8: 80 MHz. -4, 1=3 4 44AA 4 9 nj4$14. ^4^-^^-ar 4 100 nm$!34, 700 - 900 nm4 4 4 3ÊBÔI ^7H4$14. s iOM44i 4 2 : 4 44-B- 4 4 4 4 4 4 4 1 - 4 4 4 ^ 4 4 H 4 $134, 4^- a 4 4 4 4 1 4 4 4 , AA N 4 4 # ^ 4 4 5 3 4 3 tk4. 3 4 4 , ^ 4 4 AA AAAs AA A4A AAA 4 4 4 , 4 ^ 4 4 3 4 # 4 £ 4 4 ^ 4 4 4 4 4 4 1 1 - 4 4 4 3 , 7}^*l <mA £ 4 4 ss^Â < g ^ §. 47} $143 4 4 4 4 4 4 4 4 : i 1 ^ 4 4 s 4 4 4 4 -oL447} 4 4 4 $■ 144 4 4 4 ^ - 4 4 1 4 # 4 4 1 §14 4 4 4 3 S . A } * § - ^ 4 ^ ^ 4 4 ^ , As±A- A 4 4 ^ 4 4 7)^s 4 4 4 4 ^ - 3 7 } 4 AAA 43.iL 4 4 4 4 .

1 3 4 4 4 ^ ^ 7 k i f 4-3-43 $i$i-b4, f}7Hfe i 4 4 3 S 4-g-4-b Offner-triplet ^ 4 4 1-3 4 4 4 4JLJ 4 ^ 3}7|-fe- cylindrical mirror # 4-g-s}^-

4 ^ ^^^^® ^ 4 4 1 ^ 444$14 . cylindrical mirror 1- 4-§-4^ 1-^ 4 4 4 T T

3 4 4 g-^s £■#■§- 2 L « T $14 SL4 # £ 4 4 4 1 3 ^ 4 4 TT-444 4 ,

^23} 4 4 4 3 4 1 4 44-7-4, -f-4 3t-£r4 ^ 4 , 44fe- Offner-triplet 4 4 4 1 3 4 4 4 1 - 4 4 4 3 $),£4 Offner-triplet %44 1^- 4 4 4 ^ 4 4 300 mm, ^ 4 4 4 500 mm4 3^4-g;4 ^ 4 4 4 250 mm4 A-Â-g-, 3 4 3 , 1200

- 179 -

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l/mm4 grating f-3.5-1 ^ 4 4 4 $ 1 $ 1 4 ( 3 ^ 339). Grating4 %?}A ô] 200 mm, ^ 4 100 m m ^ 3 4 , 4 4 4 U 4 * 84 grating4 4 4 4 ^ 4 4 -§- AAA $14. 4 4 4 4 4 4 l ^ f r 4 1.5 ns^4, M | 3 S . ^ 4 ps Ass. 444fe 44 44 1 3 ^ i : &4 4440*4. s t f ^ H M £ | o ] ^ f ^1444^4 ^ # 4 4 4 4 4 4 4 £ 3 %-A £ 4 € 4 4 # 4 ^ 4 4 4 4 4 4 7}Â l i ^ l &4 4 4 4 43.5. ^4^14. 3 4 4 , 13^ i #°1 4 4 4 ^ <£# 1 3 4 4 4 4 3 4 7} 4 4 3 , ^ 4 4 4 4 # 4 4 ^ §444 5ft£4. A4s., 4§43 $XA 4s4 ^ 4 4 4 3^}K4^r 700900 nm 4 4 Â 4 4 4 ^ 4 4443 . $134, 1 3 4471i ^ 4 4 3*?U=4^ 750850 nm.4 ^ 4 4 4 3^1^4 ^4 €■# #4^

44 . 4 4 4 4 ^ ^ 4 4 4 4 4 1 3 444fe 4 4 4 13^4 250 ps£. 4 ^ 4 AA 44, f44 ^ 4 ^ 4 730890 nm ^ 4 4

y44 160 nm 4^4 4^§ 7}

4 3 $14. £ 4 , 1 3 4447} 4 ^ 4 4 4 4 4 4 AAs 44^b AAs $14. 3 « ] E ^ mo] ^ 3 4 ^ # 4 4 3^1H4£ ^ 4 4 4 iL4 &A l i ^ t ^ 4 ! ' <r $14. 4 4 4 , ^ 4 4 4 4 4 44^ #4 £444 4 4 4 5:47} ^ 4 t ^ f e

- 180 -

3%> 3-19. Offner-triplet *§A4 1 3 ^ 4 4

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CPA 4 4 1 - 4-§-4^ 3 # 4 4 4 4 43*H4-k: 4 4 4 1^1 - ^ # 4 4 4, ^ 4 1 ^ # 4 4 , 4 4 4 4 4 4 , 4 4 4 4 4 3a.7.}2] ^ - H £-44 o ^ 1 3 ^ 4 Ad^s. $Hr44 %%IA #47} 1^3t A $14. 4 4 4 ^-44-i- 4 4 4 7l 4 4 4 SI0M44fe Acousto-Optic Programable Dispersive Filter (AOPDF) 1-4-o-4&4. AOPDF-b -§--^443:4!- 4-1-44 ^As. £ 4 4 ^ 4 ^ . 4 2-4-1-3^44^ AA3-4, AAA 4 ^ 4 4 4 4 3 , ^43 .5 . 414 7}- - } 4 4 4 $14. SIOM44-& 3 4 ^ 4 4 ^ 4 - 4 ^ 4 4 AA AOPDF (Dazzler)l 4 - ^ 4 3 $1&

- 181 -

Cylindrical mirror M MSo\^ £±mA\J

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3 ^ 3-20. Cylindrical mirrorl- AAAA 1 3 44714 AOPDF.

4. 3 4 4 , AOPDF r 5\A&-§rA 50% 4 ^ . 4 4 4^-4. ^ 4 ^ . 4 4 4 ^ 4 4 4 1-^ 4 4 4 7 } 4 ^ 4 3 , s\A& AAA 4 4 $ 4 4 4 4 4 4 46l^l 4^-7} 4^-4 4^-4, 4 4 4 4 1 4 # 4 4 4 4 4 - ^ 4 4 4 $14. 4 4 4 , 3L7}O\ ^ £ €-44 ^4-i- # 4 ^ ^ 33 |EBJOI y ^ 4 4 - 4 ^ 4 4 ^ 4 ^ ^ 4 4 5 £. $ 1 4 4 t 4 # 4 4 3 4 4 4 4 .

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- 182 -

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4-g-^ 14-1- A}-§-44 #£ 4W 6 m J ; 4 ^ ^ r J ^ A j .^ig. ^-9-oflfe 4 mjoi &4. 4 4, 44 i^-444 444 1^4 %AAA 31AA 204534- 44 ^ 44 ^4# £-44 ^4 44^ 45l 1344. 44 ^ - 4 4 4 444 137} f^4^r #4 4 4 ^ 444 444 1^1 ^#44 44£ 44£t7H14 4 444 447] ^^7} 4A}44 434, 444 4144 13^4 4*J13S. 4-§-44. 4*S13^ 3#44 444 137} 444 43-4-g- 44 44 444 4 4 A 44 44444 4£-4 4^131- 4^4 43,43.^ 4444. 4XS AA7) A ^-44 4SJ1^7} 434 444 4-$-4 nfl -o]i( siONMH^ 44 ^#4 ^ 4 ^44 Pockels cell-i- ^4 f ^ ^4 4*1131 444$14. SI0M£- 444 44 ^44£ 4# ^-443 $15334, 44 ^ ^4 1=3 444, 3*4H4 4 -.o_ 4440^^14 J^4-4JI 01^ 4^f-4 ^444 4-f4 4^4$^4. 34 4, 4^f-4 f^4fe 47jj ^ 4 a.4 ^ 7 } 4^43, ^^440114 ^ £ g. 44 44 ^^44 4 « 3 7 } 4^AA QA f-4 444 $13.3 ., £3sL 47}

- 184 -

4 < 3 ^ 4 4 ^ 4 * 4 4 * 4 SIOM4 4 4 * 4 4 * * H#4fe 44 * * s. -S-4 € 4 4 4 .

4 ^ ^ 4 4 4 4 4 *&te 14 * ^ # 4 4 4 4 800 mj ^ £ ^ * 4 4 $ 4. 14 * *44fe 4 ^ 25 mm, AA 15 mm4 rod 4 4 4 4 4 * 4 4 4 4 4 3 * # 4 4 * £ 4-^-4^3.4, SIOM44 4 4 4 4 4 * * 4 * 4 3 $1$14. 4 4 4 £ 3 * 4-8:4 * W * ^44$l3.4, 4 4 4 4 a 4 ^ 4 ll mm&4. 4 ^ 4°14Sfe Q-switching4 Nd'-YAG 4 4 4 (Quanta-ray, Spectra-Physics) 2 4 # 4-§-4^3.4, * 4 4 444*5 4 4 2.4 J 4^.$i4. 4 4 ^ 4 4 4 4 < * 4 4 4 4 4 4 4 4 4 *3t# 4 4 4 ° ^ 4 4 4 4 4144, NdYAG 4 4 4 4 4 4 4 44- tt4 £ 4 4 4 4 4 ^ 4 & 3 4 , 4 # 4 4 4 9 4 4 4 4 4 ^M * 4 4 # # * * 4 4 » 4 . 14 ^ *44*1 **JM*fe 54 $13.4, * 4 £ * £ 35% 4 ^ 8 4 . SIOM4 14 -r fr*4fe 4 4 4 4 ^ ^ . 4 ft# £ 4 4 4 4 4 4 4 £ 4 8 4 . €444-7^-4 4 # M^lfc ^ 4 4 4 4 4 1.2 J 4 ^ 4 4 , * 4 4 4 4fe 600 mj 4^-5-, # 4 JL-S-4 4 50% 4 ^ 4 4 . 4 4 4 , 4 4 4 4 4 3 4 4 ^ 4 4 4 4 4 fk* * 9 * 4 4 QAs, f 4 4 4 4 4 4 4 * 4 ^ 1 4 4 4 * 4 , ^ 4 4 4-2:71 1*) 4 - ^ 4 4 AAA AA ¥ 4, AA 4 4 4 4 4 1 - 4 * 4 4 As, 4 4 4 4 4 s 44 , 2.1 i-4 4 4 4 * 4 4-^-4, 4 £ 4 ^ - 4 4 3 ^ 4 4 $l-b 4 4 A4s 4 ?i* 1:4 f-4 44 ^ 4 4 4 t A &3s ^ 4 4 4 4 * * ^ 4 37}1 4 4 4rr 4 # °4 4- $14. 4 4 4 , 4 4 4 , AA 4 4 4 4 4 4 4 ^ 1 34HH8 4&, 4 4 4 4 * 43511434 4Afc 4 4 4 4 4 4 4 9 4 * . * # 4 ^ at* 444.

3.3.2xi s m § 4 ? I ° I ? # * ^

SI0M4 4 4 4 s . ell44 4 & 4 4 4 24 r # # 4 4 4 * # 4 4 4 4 4 444*fc SIOM44 4*1 4 ^ 4 4 4 4 4 4 * 4 * 4 ^ $14. 4 ^ 4 4 4 4 H ^ 511444 4 ^ ^444U= 4443.i?_ 100 J4 4 4 4 4 4 4 4 1-2-44, 5d 4, 4-§- Nd:YAG 4 4 4 4 * # * £ * 2 J 4 4 4 4 4 4 4 4 4 1 # 4 4 4 4 £41, 5J144J= -3-4 sj# * 4 4 4 4 ^ 4 * 4 4 4 £ 4 4 ^ 4 #4 . 4 4 4 , 4 # ^ 4 4 * 4 4 A AAA. AA ^ * 4 4 4 4 4 , SIOM4 4 4 4 4 4 4 4 3 - 4 4-7} ?>4. SlOM-a «(*4* 4 4 4 4 4 4 4 4 4 * * # 4 £-443 $J4 *$$■ 4, 4 4 4 ^ 4- * 4 4 * 4 4 4 4 4 1 4 4 7fl44 -t- $1$*4 4 3 ^ 4-444. 4 4 4 , 444473V3 4 4 4 4 4 4 # 4 4-f44 4-S-4, 4 4 4 ^ ^ 4 4 4

- 185 -

* 4 4 4 4 4 4 4 ^ 4 4 4 4 4 1 - f*- 4 4 4 4 t 4 4 4 . SI0M44 4 4 4 4 4 4 4 4 * * S.AAA A As 5a* <r $134, 4 4 4 4 4 ^ 4 4 4 4 4 * 4-0] 0 ^ 4 -0.4. -g-o|( ^ j j . o^jT. ;££ oj^ol go] ^ ^ 4 4 4Z4, **$ t 4 4 , 4 4 4 4 4 &A 4, tf* 4 4 4 # # £ 4 4 4 ^ 4 4 44f- $£.£ 4 4 4 4 . SIOM4 4 4 4 4 4 444-c Nd:glass 4144 4 4 4 4 4 3 s , single-frequency 1054 nm 1 3 4 4 4 4 44^4 Nd:glass # 4 4 , 24 ^ 4 4 4 4A 4 4 1 1 4 *^2-S. 4 4 4 4 4 4 (34 3-23). Nd:glass # 4 4 4 4*11 # 4 4 4 # 4 4 4 1 ^ 4AAA 4 4 300 J 4 ^ ^ 3 . 4 , 1 3 4 £ 20-30 ns4$14. # 4 4 4144 f i f e 24 2:44 1 4 4 4 4 1 4 4 4 4 4 4 150 J4 527 nm l i s ^ 4 4 & 4 . SI0M44 *1144 1 4 4 4 4 4 4 4 4 4 * 4 4 7)14 4

3 ^ 3-23. 3 * # 4 4 4 M 4-§-4^ 4 4 4 4 4 44 3144.

443.5.^-4 150 J4 4 4 4 # 4444-^r 4 4 4 . ^4435_, # £ 4 4 4 ^ 100 J9- ^ 4 4447} 6-8 4 4 4 4435L £1144# 4 ¥ 4 4 4 4 4 4 444-1-20 J 4 4 3 445- AA^- 4 4 ^ 4 ^ 4 4 . 4 4 4 dJ-i- AAA 4 ^ 4 4 4 4 41- ^ 4 A4AA f-4 &4*-§r fe°U(~0.1 Hz), 4 =i* fe44 4 4 4 4

- 186 -

4. 4 4 4 , SI0M44tr 4 4 4 4 444-1- 4-8-SI4 4 ^ 4 , 4 4 4 4 4 4 4 4 4 £ 4 i 15* 4 £ 5 3 4

S10M44 3- 4 4 4 4 4 9 4 4 4 41- 4-8-4^ 24 # # 4 4 4 4 # # 4 4 * 9945S4. 24 # #47H1 A}-§-4 4 4 4 4 4 ^ 4 4 20 J4533-4, iL4 15 J4 4 4 4 4 4 1 - 4*45314. 24 # # 4 4 4 AA$. 44-^- 44014 744 £■ A } 4 4 SASLS., 7} 5. 60 mm, 4 5 . 40 mm$3.4, parastic lasing *LAA 4 4 4 4 4 £ 4 3 S ^ i 4 4 4 44-1- **r4fe coating-t 45914. 4 4 4 ^ - 4 4 4 4 4 4 4 4 SI0M44 4 4 4 4 4 AAAA. 24 ^ # 4 4 4 4 %AA 44 5334, # 4 4 4 4 ^ 5 J4&4.

4 * # 4 4 4 4 ^ 4 4 4 ^ 4 4 130 J 4 4 , i lf-4 75 J ^sA 4 4 4

3 ^ 3-24. 4 # # 4 4 4 4 4 AAAxr 4 4 4 4 4 4 4 4 4 4 .

# * 4 * 4 4 . 4 4 ^ A } 4 4 4 T ^ £ 473 go mm4 4 ^ 4 * 4 4 , 44"4 Crystal systemA}£Jf 4 ^ 4 4 ^ 4 . 4 4 4 4 $ 4 4 f e parastic lasing* 4 4 4 4 4 4 4 1 4 S44kr index matching * 4 * #&3-4, * 4 4 f e 4 4 4 4 4 * ^A^ A $!-£- 43-Ff-i- lk44584. # 4 4 M S - ? - b 3 4 ^ 3 4 , # 4 4 4

- 187 -

44 75 J 4444 35 J 4^534. #444 4444 51144 44 4441 4, 4 444 444 yJ4 A 4*44 4 14 444£ AA 444$143 44. 4 44, 4 4*4 444 44 41-4 1444 &$14. 444 A2iA 44 444 443.4, 144333.4 HL44 4#44 #444 4444^ £H44 44 444 # 4 44. 514, 4 4*4 44, 444 4*44 ^4 44 ^4 4 4^ 4 £4 444534. 4 444 4-4 444 144533.4, 4 44 444 444 44533, 444 144 As $144 4444 4534. 4# #4444 #44 4144 44 444 £$13.4 # 4 4444 44*4 444 1 4 $15 ,3-4, 44 444 4 444444 447} 44 #4- 4# #444 4441 447} H5S4

3.4. g± ^47|2J 4^

4# #4444 #44 4144 134 13 44444 1344 4444. 13 4444 13 4444 14 grating 43.5. 4444, SI0M444 # 44 4 1480 1/mm grating4 13 4444 4*4^4. 13 4471444 1200 1/iran grating4 4*4$144, 44 4 13 4444 1^ 4-4444 4*44 grating 4 44 44 #44444 1444 344 ^As 444 ^4 3:443.5. ii4 44 44444. 13 4444 4# #44 444 44 -£44 44 444 yd 4 4^ 150 mmS. 3144-533-4, 44 4# #44 4144 444 2-44 13 4 444 444444 &$14. f- -S, #44 444 ^14 44 ^'44 4# 13 4 3=44 4S.4 4, 1^ 4444 # 4444 4441 4444. 44, 44 1344 2:41-44 444 #444 24 4 #444 44444 &3, 10 HzS 4444 14 4 #44444 44443 $14- 10 Hz4 4445. 1344 4^ 44 4444 44 #4444 44443, 4# #44 4 4 44 14 4444 4 13 4444 4444 1344 4443 $14. ^A$. 4^4 1344 29 IS5S34, 4 44 4 13 SH satellite 137} 444$143 44. 444 satellite 1^4 &°V) A4 AOPDF4 3:4 4 444^ 1344 32 fsS. 444 4. 13 4444 44 l t ^ 4 70%5334, 4^44 444 4# 444 13 4444 4 25 J4 143.5. 4443 $14. 444, 4# 444 4^4 4 0.8 PW7} 1 444.

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35i 3-25. 4 4 4 ^ - ^1144 * 1 ^ 4 4 4 .

- 189 -

41 4 ^ fs 4 M * ! * °1-§-?!: e f l o j ^ - f ^ ^ } ^-Jr-v-g- ^

43 ^ 1 ^ 4 4 ^

4 # 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 SIOM 4 4 s ! 353?JMl 4 4 TW 414 4 4 4 * 4 4 4 ^ 4 4 £ ÂAA^ 41)4534. # 4 4 4 4 4 4 Prof. Jiansheng Liu 4 4 SIOM4 State Key Laboratory of High Field Laser Physics 4 £ 4 4 4 5*4.

27}4 4 4 4 4 A^-GAA% 4*345344 3 l £ 4 4 ^ 4 4 4 4 4 3 * 4 4 4 * 1 4 , #43.4 3.7] 4 4 4 4 4 1 4 4 4 4 4 4 4 45,4 4 4 4 4 4 4 ^ 4 3 1 4 4 4 4 4 4 4 As £47} 53534.

4.2 Zl^S. MBfâl LHCH[Aio.| u e £ 4 2 £

3 l £ 4 4 ^ 4 4 4 4 4 3 4 4 4 4 * 4 4 4 4 4 4 ^ 4 4 4 4 4 4 4 1 J L # 4 4 4 4 5 . 4 4 4 4 4 4 4 4 4 4 2:44 4 4 4 1 - 4 1 4 4 4 4 ' t 4 4 4 4 4 fast ignition 4 7}^7§A ^ 4 4 4 4 $14. 4 41444 4 4 7}^$. AA 4 4 4 4 € 44^ -444 3 1 ^ ^ 4 4 4 4 4 4 4 4 4 3 4 4 3 5 4 4 4 4 4 1 4 4 4-443.5L 7}144 4 4 ^ - 4 ^ 4 £ 1 4 4 44 4AÂ 4 4 4 - 4 ^ 4 4 4 4 . 4 4 4 4 ^ 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 ! " 4 $144 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 1 4 533 4 4 4 4 1-2-4 4 4 4 4 4 4 4 ^ 4 1 4 $14. 4011 ^£,4 ^ 4 4 4 4 441J-45. 4 4 4 4-4 As 4 4 4 4 AÂ 4 3, 4 4 4 1 3 4 4 4 4 4 4 4 3L44.&3. 4 4 4 4 3 . 3 l £ 4 4 4 4 ^ #4 4 4 YiA 4 4 4 4 4 4 4 4 4 4 4 4 4 1 ^ 4 4 4 4^5 . £ 4 4 4 . 4 4 4 4 4 4 4 4 4 4 f - 4 s 4 4443 .5 4 ^ 4 4 3 4 4 4 4 4 4 4 44 4 4 4 4 ^ - 4 4 3 ^ 4 4 t * 3 4 £.14 4 4 4 4 4 . 4 4 4 7}4 #3.4 4 4 3 l £ 4 4 3 4 4 4 4 4 4 3 4 4 4 4 4 4 * 4 4 4 4 4 4 1 4 ^ - 4 4 4 4 4 4 . 4 4 2 , 4 4 4 4 4 4 4 4 4 4 4 4 1 4 4 4 4 4 341 4 7}45. 4 4 4 4 . 4 4 4 4 vxB 4 4 4 ponderomotive 7}4oicd 4 4 4 ^ 41}4 4 4 4 4 4=5 4 4 4 1 4 4 4 . 4 £ 4 4 4 4 4 4 1 s 4 4 4 4 4 4 4 &4 7}444. 4 4 4 4 4 1 , 4 4 4 4 , 444^-4 4 4 4 4 43.5. 1 4 4 4 . 4 4 4 44f- 4 4 4 4 1 4 1 4 4234444 4 4 4 4 4 4 4 1 4 4 ° i ° s

- 190 -

4 444 44444 4-4* 2-44444 5344 44 #3.4 444 4"44. 4 ^4 44444 444 14444 #4€ 44 £444 444 4'44 144 4444144 44435. 444444 441 4 $1534. A}*4 ^£^4444 800nm #444^.5. lOHz5. 44^4. 1- 4 41444 4 2543=3i 1^144 75mJ 44 444^4 4 5TW4-£44. 4443-5 44 4 3:4444 ^ 37)rz 4 lOumS. 44^44^4 4xio17W/cm244. 4414 44 4 ^ ium ^v\)^ 14444 #4-o-}&4. s4 4144 lum 44414. 4 44 4*4 444 #4 44^-4 4444, 4444 ^4f 444 S444 4 44 44 444S4 444 44444 7}#44 4534. ^ ^ 4*14 44^ n^ 3-264 14. ^14444 &A 444 4^414 IO£4^ 314441 4444. x4 444444 44 ^4 3.4* 4444444 X44 4 ^44 144534. 44444 144 1444 BBO 144 4444 400nm 4 43.^ 24444 4444 s l 4 7}#44 44 S4 ^4 4^35, 44^14. !44wS444 A 4 ^ 4 4 4 44°J44 444 444 44. 44^444 4 444 * .M\44 400nm 44 147} 444 ccd 4444 Shadowgram4 °l -#4 BM1 €4. 444 4^ll£c|i ^44 ^4444 4-3*1 T!144 445. 1 444 444444 44 44 44444-°-5\ 44 44. 444 44 444 4 44 441-^7} 400nm444 441-^4 6.9xio21cm3 ii4 44 444 44. £ si*^4 44 444 3:144 44 14444444 44 444 4444 44 4 7}#*}4.

- 191 -

Probe beam

Beamsplitter

am beam

CCD<\

Pin-hole imaging \ \

Micro-step translation stage

CCD

Fused glass with ljxm Al overcoat

34 3-26. diAs 443,4 4444 3.444 44 14 44 s

34 3-27. 31 s 4434 444 4 3444 4* 14 4

- 192 -

3 4 3-284 4 ^ 4 4 4 4 4 4 Shadowgram4 5 . 4 4 4 . 4 4 4 4 3^5.x4 4 $14 4 4 4 4 4 4 & 4 4 4 ^ - # 4 ^ 4 3 . 5 . 4 4 4 4 4 4 ^ 4 4524. 4 4 4 4 W J 4 £ 4 ^ 4 4 4 4 4 4 4 4 4 4 4 $ t 4 4 4 4 4 4 4 4 4 # 4 ^ 4 4 1 ^ 4 4 3 4 4 - 1 4 4 4 4 -5.54 4 4 4 4 4 1 ^ 4 4 4 4 4 4 4 7 } 4 4 ' t 4 5 . 4 4 4 € 4 . 4 4 4 4 4 4 4 4 1 ^ 4 6.9xio2!cm3 4 4 4 4 4 4 4 4 4 . 4 4 4 4 ponderomotive 4 4 43.5 . 4 * 4 4 # 4 ^ 4 4 4 ^ 4 4 4 . 4 3 4 O I ] A ^ 4 ^ 4 4 4 - 4 ^ ^ 4 4 4 4 4 4 2xio18cm/s 4 4 4 4 1 4 4 # 4 4 4 ^ 4 ° J 4 1 4 4 4 . 4 4 4 4 53E-44 e 4 4 4 4 4 4 4 4 4 4 4 4 4 4 3 i s 4 4 5 . ^ 4 1 ^ 4 4 S 4 4 4 ^ 4

u.$ 3-28. lps 4 4 l-f-4-H- 3LA ^ 4 4 Shadowgram.

4 4 4 4 4 £ 4 4 4 4 4 1 4 4 4 4 1 ^ 4 444$ !44 5.4- 4 4 4 1 4 4 ^47} 4 4 ^ 4 . #^- 4 4 4 4 4 4 33E 1 4 4 4 4 4 4 4 4 4 4 4 4 tfl*v 1 ^ 4 4 4 4 1 4 4 ^ 4 4 4 1- 1-2-44 $14-4 1 4 4 4 4 4 AAA.

4 4 sfl44 4 4 4 4 4 1 4 4 M 3rd order autocorrelator 1- 4 * 4 $ 4 - 4 4 4 4 SIOM44 7}*H43:5 4 4 4 4 247} 4 * # 4 4 . 3 4 3-294 A}.g-4 autocorreLator4 AA% .£ -444. 4 4 4 4 harmonic generation crystal 4 4 4

- 193 -

4 S 4 4 4 7 } 4 4 4 4 4 4 3 1 4 4 ^ 4 4 4 4 ^ 3 4 $ 1 4 . 3rd order harmonic beam4 447117} 4 1 4 1 4 4 5 - 4 4 3 - 5 . 4 4 4 1 4 7 r # 4 4 .

spectrometer spectrometer controller

ND filters OD1-5

frequency doubler

3 4 3-29. 3rd order autocorrelator 4 4 4 S

dielectric mirror 800 nm 0°

dichroic mirror

4 3-30. # ^ " 4 4 4 4 7H11- 3rd order autocorrelatorl 4 4

3rd order autocorrelatorl- 4 * 4 4 4 4 4 W J 4 4 4 4 4 4 1 3 4 4 4 ZiA'A : 4 3 4 3-314 1 4 4 £ 4 ^ 4 1 3 7 } 4 4 4 514. 4 3 4 1 3 4 ell 4 4 7 } 1 -

- 194 -

44 544 44 S44 44^44 ^7H f-^44 ^d\] £444 4444 4 34 4*34 4443 2:4 444 444 3.4 4444 £44 44 4443) 4 4444 44.

1.0xlOc

l.OxlO"1

l.OxlO"2

l.OxlO'3

c

£

1.0x10"*

l.OxlO'5

1.0x10"*

l.OxlO'7

1.0x10*

1.0x10*

l.OxlO'10

-6.00 -5.00 -4.00 -3.0Q -2.00 -1.00 O.QO 1.00

time [ns] 4 3 31. 3rd order autocorrelatorl- A } 4 4 4 4 4 4

4 4 4 4 4 4 4 4 4 4 1 3 4 4

5.4 444 444 444 4444 447} 34444 44 444 4 4 ^ 4 £«* 445. f 44 4^4. 4 444 44 44 44444 44^44 444 4443 44 444444 444 4445. 4»4.

~ 195 -

41 5 4 OPCPA 7}^ o]£$. A)o}A\ contrast # # 'A"k 7fl*

Optical parametric chirped-pulse amplification (OPCPA)4 71^4 CPA 7} 4 4 4 4 4 4 5-4H 4 4 4 4 5 4 4 4 4 4 ^ 4 1 3 ^ 4 4 4 4 4 . OPCPA 4 4 4 optical parametric amplification (OPA) 4 4-^ 4 4 4 £ 4 4 4 * 4 ° ^ 4 A A 34 #444 444 444 444144 444 144 #4415. 4 * 44. 444 144A14 ^4 444 104 #44 444 444 45. #£4*4 4 44 44 444 1H44 »4 444, 444 44414 4*44 444 CPA 44<>ll 44 1 447} 4, 4444 444 4- -4, 4^4 $4 AAA 44 44 -3 ^3L£r^ 444H;5 i*j35. #444 44t 4 44. £4. 444 44^ 144 444t S44 4*44 444 444 44 445.4 4 V34 4 4444 l#^}4 ttrl-g-oll gain narrowing 3-44 44 4443. 4 4 ^ 44"t 4 4 4 344, OPA £44 4^ 444 1^4 #4444 44 4 1^7} 44 4, 44435- 4444 4444 #4s47} 4443S. 444 ^3^-4 444 ^44 4443, 44 4444 444 #4^44 444 444 AA. 4444, OPA 47} *14 444 €34 #4 444 1^7} °44t 4444 #44 4 4 £41- 44*44 #^f€p4 #444 &3 4 1344 43 M1 #444 4 13.4 4D1^ 444 contrastl- 444 14-7} 5.343 43.4, 444 CPA 444 OPCPA 444 444 hybnd CPA 4^s 444524.

51OPCPA2} stefss" ?na

34 3-324 0PCPA4 4*44 44 4444 signal, idler 444 arH 44 444 44NH 444. 344 44 0PA444 4 44 444 44 4-5 4 £4*43, 4#44 44 444 IM 4 * 44 4444 7>44> 444 444 tid #, 44 4444 4144 4 44 444 44444 314444 signal 4144, 4444 idler43 44- 44, signal, idler4 4444 44. 4* wv 0^43 44 444 5.4 444 44, wp = wstwi A 4444 4444 44. 3=% A 44 4 44 wave vector 44 444 5.4 ^44 4444 4334 k^k^h^ 4 4444 4%144 44. 44, ^4, signal, idler 1144 444 4 443.5. 453 t 4444 %^ 4 4 4 t 4 4 3 44, a44 #* 4444 4^^ 444 4443 44.

- 196 -

Nonlinear Medium

Amplified

3 f 3-32. 0PCPA4 4 4 .

5.2 ^ B S ^ 0||U| ^2\ contrast |}^tf *|*h 0PA2.| 0 |^ ?||A1-

OPA* 4 * 4 4 4 4 4 contrast-!- #7}44 4 &TT 4 4 4 4 4 1 - 4 4 4 4 4 4 4 4 0PA4 4 4 4 4 4 4 4 ^ 1 4 4 4 4 4 3 4 4 4-S- # 4 4 4 4 4 4 4 4 4 - BBO 1 4 4 4414-2-5. 4 * 4 4 4 4 3 , 4 4 4 4 4 a 4 4 4 4 , -43i4 4 4 4 4 4 4 4 31444 Nd:glass 4 4 4 4 4 4 1 4 4 4 4 4 4 ^ 4 4^1 3 1444. 4^4 BBO 144 4444 4444 444t4s, 14, 444°^ 44 4 444 4 444 As 44 44 0PA4 44 444 4f 4 1:4444 1- 44 2:444 44. 444 OPA 44 444 4444 4444 ^4 444 4 4 4 4 4 * i , 4 4 4 4 S.% 4 4 4447} signal44 idlers. 4 4 4 4 4-£ 4 4 3 4 4 4 4 4 4 coupled wave equation4 4 4 4443.-S. 4 4 * M 4 4 4 , ^ 4 4447} AAA, 4 4 4 3 5 . 3f°4% A±M: / k l i , ^ 4 &H4 4°Q4 signal4 4 idlerS £ 4 4 4 4 4 4 4 4 4 3 7}44-4 (no pump depletion), signal 4 4 4 4 gain4 4 4 4 ?M 4 ^ 4 4 4 4 4 4 3 ^ S 4 € 4 .

4 d / 4 = l + (ff ): sinh2( V{gW-AAkL/2f) (9LfAAkL/2f

(d)

- 197 -

<^*W& _A 2)

4 4 4 4 , / w i 4 4 4 °rJ4, 4 4 4 signal 4 4 4 4 intensity0H, £ 4 4 4 4 1

4 4 1 4 , Iv 4 4 4 4 4 4 4 intensity, d t / / 4 4 5 - 4 4 4 4 4 , c 4 4 4 , np,

%, TI84 4 4 4 4 4 , signal, idler4 1 1 4 , \ , \ : 4 signal4 idler4 4 4 4 4

4 4 . 4 4 4 A A 4 4 4 , 4%T 4 4 4 4 intensity. 4 4 4 4 4 , 4 1 4 4 3 5 4

4 , 4 4 4 4 g% 4 4 4 4 , 0PA4 4 4 4 4 4 4 4 t i £ 4 Ak4 4 4 4*1144.

4 4 4 , 4 4 4 4 4 ^ 4 4 4 4 3 5 . 4 0PA4 4 4 AA^ 4 4 1 : 4 S14.

4 4 4 4 4 $ : ^ 4 4 4 4 4 4 & « € 4 .

zi/c = | ^ ^ , - / c ,

4 4 4 , / > fcSJ ^ 4 4 4 4 4 4 - signal, idler4 wave vector44- B B 0 4 1 4

4 4 1 4 4 A | 4 4 3 type 14 4 4 4 4 4 4 * 4 4 4 (e -> o+o)44 4 4 4 t

$ 4 4 4 4 1 4 4 4 4 4 4 4 1 4 4 4 AAA idler wave vector, 1%, 5. 4 4

4 4 4 4 4 4 4 4 .

Ak — \k7— kq— kip-r ky— k,t\ = \kip — kj

4, 44 4444 singai 4444 4444 4444 444 44444 44 idler4 wave vector4 4}4 A 4 4 3 , !*ll idler wave vector4 3 7 ) ^ «^144

5 4 ^ 4 4 4 4 4 1 - 4 AA 4 4 4 , 4 wave vectors] 4 5 - 4 4 4 4 4 4 f #

4 4 ol- Si 4 . 4 4 4 4 4 4 signal 4 4 4 4 wave v e c t o r ^ 4 4 4 4 4 4 4 4 " t 4 4 4

idler4 wave vector 4 3.7} 4 4 4 4 1 4 A A 4 $14.

ki = kl-dk*~2cosahk "tp "p p i 5)

= (2 7T. 3> /«. \2 n

\ A i —2cosa npns

\A,

- 198 -

® Ordinary wave

^^Extra-ordinary wave

3 ^ 3-33. BBO 1 4 44Ai 4 4 4 4 4 , signal, idler sj 4 4 4 ^ - .

1 _ cos'fl sin^ 2 ~~ 2 + "

n„ n, (6)

p op • "ep

4 4 4 , 04 BBO 1 4 4 4 4 4 ^ 4 4 4 4 4°k l 4 - £ 4 3 , $& 1 4 4 4 A 1 4 4 41444 signal 4447} oW^ zj-£| ^ 4 ^ . - 4 ^ 4 4 (a.4 3-33 t 2 4 BBO 1 4 4 type-I 4 4 4 4 4 A ^ 4 ^ 414 4 4 4 4 4 extraordinary42-5- 4 4 4 4 4 4 ^ 1 4 4 BBO 1 4 4 4 4 4*3 4 ^ 4 4 4 ^ 4 4 4 4 4 4 , 4 4 4 1 4 4 4 4 4 4 4444(532 nm) BBO 1 4 4 ordinary 4 # 4 4 , nopA extraordinary 4 -^44 nep5.44 4 4 4144-4 3*444 4 4 4 4 4 - ^ 4

idler 4144 4 4 wave vector4 3 4 ( ^ = 2 ^ / 4 ) 4 4 4 4 5_4 U4

(cop = uAs + u)j4 4 4 4 4 4 1 4 4*1144.

\ K A l \ \ K) -1

k = 2TT-n. (A;)

A,.

(7)

(8)

- 199 -

Signal 4 4 4 4 idler 41444 ordinary wave 4 H. 5. BBO 1 4 4 4 4 4 4 4 4 Â AS4 4 4 1-144 4 4 4 $ 4 tl4 4 4 4 4 4 . 4 4 4 43 .544 , 4 4 4444 44(A7))4 AÂs(S)7} 4 4 4 3 , 4 4 4 4 4 4 signal ell4 4 4 4 4£(a)7} 4 4 4 4 , 4 (5)4 (6)4 signal 414 4 4 44(AJ4 4 4 Â7} 4 a 5. 4 4 -r-4t& Am signal 4 4 4 4 4 4 4 4 4 4 4 ^ 4 %XA. 4 4 4 , 4 (1)^.^-4 signal 4 4 4 4 4 4 4 4 4 OPA 4 4 4 4 4 A 4 4 4 .

0PA4 4 4 4 4 4 4 4 4 4 4 4 4 4 ^ 1 4 4 ÂAA 4 * 4 4 4 4 , 4 4 4 4 4 4 4 1 4 4 ^ 4 4 4 4 4 4 Sellmeier 4 4 4 4 4 A } 4 4 4 -B44 35. 4 4 4 4 . 44 , AA Sellmeier 4 4 4 * * V H L H 4 4 4 4 4 4 ^ 4 4 4 A 4 4 447} 4- 4 %XA. 4 4 4 4 4 4 4 4 4 1 4 BBO 1 4 4 Sellmeier 4 4 4 4 4 * 4 i t 4.

0 01 P>7 nA\) = 2.7359 + ^ — 0.01471 A2 + 0-00060 81 A4 - 0-O0OO6740A6 (9)

A2-0-01822

(A) = 2.3753 + r: 0.01627A2 + 0.0005716A4-0.00006305Ab (10)

A2-0.01667

3 4 3-344 S H 4 4 4 4 4 ^ 4 4 4 Nd:glass # 4 4 4 4-g-t 4 4 4 42V4 4 4 4 1 3 4 4 4 4 4 4 4 4 4 0PA4 ^ÂrA 4 4 4 4 4 4 . 4 4 1 1 4 3 . 5 . 4 1 4 15 mm4 BBO 1 4 4 A>4o-}$$34, type I 0PA4 4 4 4 ^ - 4 4 4 43Mt -22.893.5 4 T 1 4 . 4 4 4 4 4 4 4 4 4 532 nm, 4 4 l £ 4 400 MW/cm2443 7 } 4 4 $ i 3 4 , BBO 1 4 4 4 4 4 2 \ 4 4 4 4 4 0.5£4 4 - £ « 4 4 3 4 4 ^ 4 . n 4 4 4 4 4: 7H4 BBO 1 4 4 3 5 . s 30004 4 4 4 # 4 4 4 4 4 4 4 , Nd:glass* ^^.A AAA 3 ^ ^ . 4 4 -2-4 4 * 1 " 4 4 4 4 4 4 4 4 4 4 4 4 t 4 5A4. 4 4 4 , O 1 4 4 BBO 1 4 2 4 4 4 4 ° . 5 . 4 * * 1 - ^ IO6

4 4 4 4 4 4 4 4 4 4.4, nJ4 4 ^ 4 4 4 4 1 ^ 4 m]^43 -5 . # 4 1 : 4 4 4 44 , # 4 t 4 ^ 4 4 4 4 1^4 1443.5 . 4 4 4 4 5-^44 4 4 4 4 4 -10 ns4 44°-5. 444H.5, 1 3 4 4 10 ns 4 4 4 4 4 4 4 4 4 4 * 4 4 , 4 4 1 3 4 # 4 4 4 &3 4 1 3 4 4 # 4 4 B . S . 41444 conirast4 4 4 4 3 5 #7}41 4 AA. 44 , contrast ÂAA 4 1 3 4 # 4 4 4 1 4 4 4 . OPA 4 4 * 4 4 4 4 4 4 4 4 4 4 4 4 3.4S14 4AA 1 3 5.44 4 4 4 4 ° 5 . injection seeding 4 4 4 4 * 4 4 1 # 5 . ^ 1:4 4 4 4 4 4 * 4 4 4 4 . 4 4 4 4 4 4 4 4S^r injection seeding^ 24 ^ 4 4 A4 Q-switching Nd:YAG 4 4

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47} 4 4 4 4 , 5.4 10 ns 4 4 4 1 3 4 4 4 4 4 4 4 4 , S H 4 1 4 4 4 4 1 4 4 4 4 contrast 4 4 4 £ 4 4 3 . 5 . *°4 4 AA. t 4 , 41.5 4 1 4-^4 4 4 4 4 * 4 4 4 4 4 4 £ ^ t °'rJ-

"CD

o

960 980 1000 1020 1040 1060 1080 1100 1120 1140 Wavelength (nm)

3 4 3 34. BBO 1 4 4 4 * 4 OPA4 # 4 4 . Nd:glass 4*34 4 4 4 1 3 # 4 4 4 ^ASMr OPA db44 4 4 4 4 5 3 4

5.3 3||0|4 contrast S ^ S 4 ^ front-end 7H£ ^ 4

SM4 1 4 4 OPA 4 4 4 4 * 4 4 4144 44^ contrast-i- $ # 4 1 4 &4 Nd:glass # 4 4 * front-end4 4 4 4 4 4 4 ^ 4 3 4 3-354 4 4 4 & 4 . Nd:glass ^ 4 4 4 4 4 4 4 4 4 4 ^-7) 4 4 4 4 4 4 Q-switched Nd-.YAG 4 4 4 4 4 * 4^Efl4H5. 4^-4 4 4 4 4 front endt- 4 4 t 4 4. Nd:glass # 4 4 * 4 ^ 4 4 4 4 4 4 4 4 4 4 4 4 <200 fs4 4 4 4 13-

o l /■A

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CPA 7 ) 4 71144 4 4 1 3 4 4 4 4 4*1 ~ l n s ^ 1 3 4 4 4 4 4 4 , 4 1 3

4 4 4 * 4 4 # 4 1 : 4 4 4 4 4 4 1 3 4 4 4 4 4 4 . 4 4 4 4 4 4 1 ^ 4

4 4 4 1 4 4 4 4 4 * 4 4 4 # 4 4 4 1 4 4 4 m j 4 4 4 4 ^ # 4 £ 4 . 4 4

4 , front-ends] 4 # 4 4 4 1 ^ 4 - 1 ns, 1 3 4 4 4 4 mj, # 4 4 4 ~1060

n m

Injection seeded Q-switched Nd;YAG laser

Pulse stretcher

Nd:glass laser oscillator

4~S BBO crystals

Pulse selection Front-end

output

3 4 3-35. OPCPA 4 4 * 4 4 ° 1 4 1 ^ contrast 4 4 " 7 l 4 4 4 * 4 front-end

44 14 .

35*^4 4 5-8 nm7} 1 4 4 4 , 4 1 ^ 4 4 AM 1 3 AAA 1010 4 4 4 4 4 4 4 4 4 contrast7} 4 4 4 4 . 4 4 front-end4 1.2x2.4 m 4 4 4 4 4 4 7fl 4 1 4 1 4 A-^r AAA, 4 4 4 * 4 4 4 4 1 4 4 5 . ^1444. Front-end A^ 4 4 4 4 4 4 &3-4, Nd:glass # 4 4 ^ « * 4 * 4 4 4 4 4 4 # 4 4 3 4 # 4 3 5 . 4 4 ^ 4 4 4 4 47} 4 4 4 4 1 3 44717} 1^-44. 1 3 4 # 7 H 1 ^ 1 3 4 4 4 4 4 * 4 - 4 3 . grating4 4 * 4 4 , 4 4 , 4 4 J4 4 4 4 4 4 4 4 * 1 4 $14 4 4 4 grating* 4 4 Lawrend Livermore National Lab.444 447} 444. 444 1^ 4444 44 AAs 4444 44 435. 4444

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41 6 € €^333i 3.7} £5H 4€- *HH£^1 *N*1 3ri4l rfl *& °1IM ^ ^

4*8 f - 4 ^ 4 4 102-10744 4 4 4 4 van der Waals forced 4 4 I t l 4 4 A 4 ^ 4 7}44. 4 4 4 4 4 A } 1 H 4 45.4 4 4 4 4^1 4 4 4 4 , # 4 ^ 4 4 4 4 4 4 4 4 4 3 4 4 4 1 4 4 4 4 4 4 4 3147} 41444 3 1 5 . 4 4 ^ 4 s_4 41444 3^7} s 4 4 ^ - s 1 4 4 4 4 1 4 ^ 4 ^ 4 4 4 Â7} 4 4 5 * 4 4 4 . 3 443 .5 1 4 4 4 4^1 € 4 ^ 4 4 x4 31444 ' ^ ' k ^ l 4 4 4 4 4 4 1 3 5 . 1 4 4 4 4 3 4 4 . # 4 4 413.5. A^^.4 444fe #44.4 4 4 4 4 t # 4 4 4 4 4 4 4 # 4 4 1 ^ 4 4 4 4 4 4 4 4 4 4 4 4 4 4 # 4 £ 4 4 4 #°1 ^71 4 4 4 4 4 45-4 * M 4 3 44 . 4 4 4 4 ÂA^t 4 4 # 4 ^ 4 4 4 1 4 4 4 4 44437]- ^ 4 .

4 4 3 4 4 147}4 1 4 4 44 4444 4 4 4 4 % 7}44 1 144 A°-4 W:4d^4A 3.7)7} 4 1 4 4 4 4 4 4 4 4 4 4 4 4 4 4 . 4 4 4 4 4 4 4 4 4 4 4€-4 4 5 4 4 %t3-4 3 # molecular dynamic model4 particle in cell (PIC) code modeH 4^ .444 . 3 4 4 4 4 7}4 4 ^ 4 # 4 4 4 4 4 4 4 4 4 4 £3.44.

4 4 4 3 4 4 l e 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 * 4 4 4 4 Coulomb explosion model* 4 4 4 3 4£7l*ni- 4 4 ° . 5 t - 4 ^ 4 4 3.7)t 4 4 4 4 AS, 4 4 4 4 1 ^ 1 4 4 4 4 ^ 4 4 4 4 4 4 &3f--^ 444S34.

4 4 Rol # 4 3 4 4 £ 4 4 4 4 4 4 4 A^ 4 4 4 4 4 * 4 1 4 . d2R(t) Ne(t)e2 Nrq(t)e2

dt2 A^Rit) 47re0/?2(t)

(nv4444 4 4 1 4 , e:44 4-44, R(t):444 1 4 4 -14^44 44 , Ne(t):44:3444 4 4 4 4 4 4 44)

p7} 4 ^ 4 4 ^ 4 4 lA}liE.oljl # 4 ^ 4 1 4 4^4401 7fl^:u Nc-4irRo3p/3 4H5- q(t)7} # 4 3 4 4 4 4 ^ 4 4 4 4 4 Ne(t)=q(t)Nc4 4 4 .

4 4 ^4 4°147} 7ÂS 14 7}JL 440H pondcromodve energy Up4 4 1 4 4 Ne(t)4 447} 4 4 4 4 4 4 4 4 4 4 4 1 4 4 4 4 'ASA s £ * 7}44 4 4 .

4 A r — = 933A2km)XO(l016 IV/cmAe V\ > ZTjh / " ^ W = l - « W ^ l $7rcJ€0mc 47re0.ft(t) R{t){nm,)

(0.^4 4 £ , e0:4#4 4 4 4 4 , nvl7}4 4 4 1 4 )

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4 14 24 4444 ASA 444 44 44 43.5. 44 #434 £444 4

444 4445.4 44 4 4.4.

33444 Ro4 4^44344 I A H ^ - ^ I Q=4irR03pe/3 4 H 5 #434 44

£4 I*}!- 44444 4 444 4^4 4 444 444 14.

/ -A 8Ac2m.,pPd ,r pl{nm) lnti(w/cm2)= * ~ 1.94 X101 ' 4

3A A K/J,m) ( 4 £ 1 - 4 3 4 4 4 4 1 5 1 4 3xio22/cm3 4) 4 4 4 4 Coulomb ^4:$-A 4 4 4 - 4 4 7}^j- $o\%\ 7 ^ 4 ° J 4 4 4

# 4 3 E 1 4 4 4 4 41^-4 4 4 4 4 . 4 4 A 1 4 4 A } 4 4 4 4 4 4 4 4 4 4 3 ^ 1 -4 4 4 4 4 4 4 ^o-}4 4 4 4 4V4 4 4

t = e V ^ y PQ { Ro ~ l\-3ln Pit) Rit) - l

4 4 4 € 4 3 ^ 4-7J4 - a)] 7 ^ ^ 3H44 4 4 4 4 4 4 14. ^ = 2^o = [ s/2- ln( 32"+ 1)] y/$m~^/e >/2p

4 3*4 # 4 3 4 4 34 4 4 444 4 4. 4 £ 4 4 4 # 4 414 3 3 4 4 4 12.3fe 44.

44A1 #434 44 47}7} oi A14- 014011 H.4 44°1 4 4 A A44 4 44 444444 7}4TH 43 444 4444451 447} 44. 344 4444 A 4 47} 45.4^ 14 44 4-4 4-44 4-4 444.

4-444 4 4 4 4 4 4 4 4 4 14 4 4 4 4 4 4 . B, = ^-~eAr> 4ire0 3

3 4 3 4 4 4 4 4 4 4 4 4 4 4 4 4 4 ^ 4 4 4 # 4 3 4 4 JEJW4 4441 4 35. 4 4 4 14.

1 4?r e2pf$ = Q.181 RAnm)ke V ^ " » = 1 , r ^ o 47re0 3

44*} 4 44444 ^4 4 4 143 444 #4344 444 4 3-4 4 44 5.5 #4344 344 444 4444 44444 %,% 444.

#43El7} 4^43 Slt l ^£1- 7}444 44 r4 rHlrA}44 ^x} ^ dNc=4Tip2dr 4 43 4AJA}4 o(|u|4 4^4 444 14-

r//Vc 3 / 3 e 0 ^ "

4 44 4 4 4 4 44-2-4 4 444. 444 4-S4444 4 4 4 4 4 4 14.

i f 3 Bui = ~^rj BtdNc = y£",.„ax

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1.4-4 Barrier-Suppression ModeHl 4 5 - 4 tunneling &o] ^ H V ^ X } 7 } 4 4 4 4 4 1-2-4 4 4 4 4 si 4 4 4 4 4 4 4 4 1"4.

Iih{ W/cm2)= 4.00 x 109 ~2 y

A^A 4 4 4 ^ € - 1 4 13.6V4 4 4 4 $ 27} 143 .5 4 4 4 5 1 4 4 1.37xio14W/cm244. 4 4 # 4 ^ 4 4 4 4 4 4 1 4 4 4 4 4 4 7 } 1 4 4 3 3 4 # 4 3 , 4 4 4 4 4 4 4 7 } A%€4. 4 4 4 4 £ - 4 4 4 4 4 4 4 7 } # 4 ^ 4 4 4 4 & 4 4 4 7 } 4 4 4 4 # 4 4 4 Q(t)4 eNe(t)7} 4 * 5 . 4 2 4 4 4 4 4 4 4 . 4 4 4 # 4 ^ 4 5 .44 4 4 A 44s 4 1 4 4 4 4 4 4 4 4 4 4 .

3 4 3-364 1 4 4 4 4 4 4 # 4 4 4 4 - 3 4 4 4 4 4 4 4 # 4 ^ 4 4 4 4 4 4 1 4 4 z\o\47^7\ #8 f l o )$ * 5 . 4 4 4 .

3 4 3-374 1 4 4 1 4 4^ -4514 7>44 4 4 4 1 4 4 5 1 1 ^ 1 4 7 } # 4

£ 4 1 4 4 4 ^ - 4 5 . 4 4 4 .

3 4 3-384 1 4 4 4 4 4 4 4 4 7 } AA 4 4 4 4 4 4 4 1 4 7 } 1 4 4 4 H

4 5 . 4 4 4 .

3 4 3-394 1 4 4 # 4 3 . 4 4 3.7)7} 4 4 4 4 3,7)4 4 4 4 7 } AS-^A 5.

4 4 4 3 4 3-404 1 4 4 4 4 4 4514 4 4 4 4 4 4 4 * } 4 4 4 4 4 4 4 4 4 4 4

4 4 4 4 M 4 4 4 4 5 a 4 4 4 4 4 4 4 4 4 7 } # 7 } 4 4 4 4 4 4 4 1 4 4 4 5 . 4 4 4 .

3 4 3-414 1 4 4 4 4 4 4 4 4 5 1 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 7 } 4 4 47} 4S.4 4 4 4 4 4 1 4 4 4 #7}o-}44iri 3. £ 4 4 S 4 4 4 4 4 4 4 4 5. 4 4 4 .

3 4 3-424 1 4 4 4 4 4 4 4 # 4 ^ 4 4 - 3 : 4 * 4 3 4 4 4 ^ 4 : 4 4 4 4 4 7} 1 ^ 4 5 4 4 4 4 4 4 4 5 . 4 4 4 .

3 4 3-434 1 4 4 4 4 4 2 ^ 4 4 4 4 45142M- 3 4 m 4 4 4144 4 # 4 4 4 4 4 4 4 4 4517} #7}^}T11 4 3 3 31-44 4 4 4 4 4 4 4 4 4 ^7}s3 4 4 4 4 .

4 4 4 4 4 4 * 4 4 4 4 4 4 4 ^ 4 4 4 4 4 4 4 4 3 1 4 4 1 1 4 4 4 4 4 4 4 4 4 4 4 # 4 4 3 7 4 4 4 4 4 4 4 4 1 4 4 4 4 4 4 4 4 . 4 4 4 4 4 # 4 4 1 4 4 4 4 145 .451 4 a t 4 4 4 ^ : 2 . 4 4 4 40 )4 4 4 4 7fl4U 4 $144 4 4 443 . i L 4 4 4 4 t k 4 4 4 4 4 4 4 4 - i 4 4 4 4 . # 4 ^ 4 4 3 4 4 4 4 4 451 # - 8 . 4 4 4 4 4 4 4 1 ^ B I | 7 } 4 ^ 44-g- 4 1 4 3 ^ 4

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http://443.iL

25 FWHM330fs

pure Coulomb Explosion = 2x 10

16 W/cm2

R2 (nrn

2)

meanx '

3^ 3-36. 444 A44A 44 451 444 444 #4^4 *g 44444 44 444-4 4^ 44444

3.0

0.0

FWHM=10fs -FWHM=60fs FWHM=1 OOfs FWHM=200fs

1 I ■ 1 ■ I ' ! ' 1 ' 1 ' 1 ' I — 0 0 02 0.4 0.6 0 8 1.0 1.2 1.4 1.6

I M017 W/cm

2)

peak % '

3 4 3-37. 5J144 1 ^ 1 4 4 4 4 4 4 A } 4 47? 4 4 4 4 4

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3.0 R =5.0nm

mean

=1 x1016

W/cm2

2x1016

W/cm2

=5x1016

W/cm2

=5x1017

W/cm2

100 150 200

FWHM(fs) 34 3-38. 44 4 44 451 i 44 4444 ^tf 4444*

4.0 I =5x10

16W/cm

2

peak

LU 1.5-

1.0-

0.5

0.0 + 0

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R =3nm "-"N

mean

50 100 150

FWHM(fs) 200

3% 3 39. 1-4^4 37\4 4 4 4-^A}4 sg# 4 4 4 4 4

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Proton energy(eV) 3 4 3-40. 4 4 4 AS.A 4 4 4 4 4 4 4 A } 4

^ 4 4 4 4 4 4

• Measured Fit line

~i ' r

LU 1.2-

0.8

Measured Fit line

—1 [ 1 1 . j 1 1

0.0 0.2 0.4 0.6 0. 1.0 1.2 1.4

I MO18 W/cm2) peak x '

3 4 3-41. 4 4 4 4 ^ - 5 : 4 ^ o f l cfl4 4 ^ A } 4 4 4 4 4 4

- 208 -

ro O CD

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4 4 7 4 4 A } 4 4 Shack-Hartmann 4 4 4 4 4 4 4 4 4 3-24 ^ 3 , 4 4 £ 4 4 4 4 4 4 4 A S\4A Bimorph 4 ^ 4 4 4 A}4 3-34- 4"4.

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A } 4 3-2. Shack-Hartmann Wavefront 4 4 4 4

Shack-Hartmann 4 4 4 ^ $ 4 4 414 4 ^ 4 S. 14 AA.

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3-1. 4 ^ - 4 4 4 4 4 4 4 4

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4 4 4 4 4 % 4 4 4 4 - 4

°d4 ^ 4 ^ CCD 4 4 4 4 £ 3

working sub-apertures4 4

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400nm " lOOOnm

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30... 65mm

Matrox Meteor- II 2/4 400711 4 4

S. 3-14 £ 4 4 4 4 ^ 4 4 4 4.44 A 4 4 4 4 10um44 4 4 t 4 43. 4 ^ 4 4004 4 4 4 4 4 4 4 4 4 t 4 4 4 . 4 4 4W514 4 0.1ym43 4 4 7}4t} 44" 4 4 4 400nm44 lOOOnm 4 4 44-

4-EL4 ^14 4 4 4 4 4 4 4 4 4 4 4 4 4%v44, X44 Y4 4 ^ 4 4 4 4 4 4 4 Ca£* VIM 4443.5 . ^ 4 4 3 , 4 4 4 4 3 £ 4 4 4 4 3 £ 4 4 4 4 4

4 4 4 4 € X44 Y4 AA-A 4 4 4 (<„ Vij>^$-4 4.4 5t4 4 4 4 4 4 St 4 4 4 H%flA 4 4 4£4(local gradient) ^ 4 3 4 4 4 4 4 4 4 (1), 4(2) 4 4 4 .

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444 Sx4 Sy-& Sx=zc-xr ^ S,=y-y*} £4. 44 € 4 4 4 4 4 (3), (4)4 AA Zemike 4 4 4 3 5 a ^ € T A 4.4

d(p u dFk(x>y) dx & dz (3)

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$A & dFk{x,y)

dy h=--l dy (4)

AAA Fk{x,y)\f 2 4 4 A& Zemike 4%>4 4 3 M# 4 4 ?M* ak4 7 4 4 .

^ f S ^ / i ^ 4 5 i5^i4a 4 3 47}4 A3 2NxMy^4 M°i 3 4 4 gradient rectangular matrix0! 4 .

4 5 4 4 3 *)oj4o))4 4 *<>J44 # $ f # 4 4 ^} (5)4 (6)4 4 £ * H 7 4 4 4 , 4-4 4 4 4 £ ^ 4 b Zernike 4-%v4 4 ^ ^ ^ 4 ^ i£ 3-24 # 4 .

X Nx / Ay \ Me

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i - l t f - l / ?-l\./ = l , (5)

ASc / Ay \ Afr / Aty

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S 3-2. Zernike 4 % v 4 4 4-S- 4

4 4

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0(90)5.444 astigmctism

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X 4 4 4 3 4 coma

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—i

x

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2xy

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4 4 4 4 4 AA^r 31444 4 ^ 4 4 4 7 4 4 4 4 4 3 4 3-444- 44. 4 4 3-44 4 4 4 4 4 4 4 3 4 4 A2--A AAA 4 4 4 4 4 4 S-M 4 4 4 4 4 ^§}4 4 4 4 7 4 tr A } 4 4 4 4 4 7 } 4 4 € 4 4 4 4 A } 4 4 4 .

- 213 -

'^:~,K 9 ' 9 / 4 3 1

10 4 - - . 4 Q \ ' ' Vl8\30

Di = 23 mm = 40 nun

Dj = 50 mm

1' / 3 \

zAAAdAAA/^ ' 44 4 i 1 5 V43

ZiU 3-44. 'S^ - f r -?*^s) T1^

- 214 -

A}4 3-4. 4 4 4 4 4 3idt4 4 ^ 4 4 4 4 4 4 4 4 4 3 s L 4 4 4 4 4 4 4 7 4 A A } 4 4 4 4 4 4

3 4 3-444 4 4 3 344 £ 4 4 4 4 4 4 4 4 7 4 A ^ 4 4 4 4 4 4 Bimorph 4 5 J 4 4 3 4 ^ 4 55mm43 3144 7 4 4 3 - i l 7 4 4 4 9X4. 4 4 £ 4 4 4 4 4 4 4 4 4 4 4 4 4 4 10um44 44 4 4 4 4 4 4 4 4 £ 4 4 4 4 t} 4^314 O.lym 42-44 . 4 4 € 44344 3 4 4 4 3 4 4 4 3 4 4 4 4 ^ 4 4 4 4 800nm4 4 4 99.8%44-4 4 A } 4 4 4:44. 4 ^ 4 4 4 4 4 4 A7}4 4 4 0 44 -300V ~ 300V44 4 4 4 4 4 4 4 ^ 4 4 3KHz44 4 4 . AA% substrate4 4^-fe Glass LK-10544 PZT*fl£.4 PKR-7m44. 4 4 4 4 4 4 3.2mm43 4*1444 4^444^(Hysteresis)4 15% 4 ^ . 4 4 . 4 4 4 J 4 4 4 ^ 4 4 4 USBSS4 4 4 4 4 4 4 4 4 4 4 4 7 } 4 4 4 £ .2-444 1 4 4 4 4 4 4 lms4 4 4 4 l-S-4-4 314U44 a.4 7 4 4 4 4 4 4 4 4 £ £ - 4 4 4A-Sr 4 2ms 4 4.

- 215 -

7.2 4§£R A|4gM o|g i nfSsR ^3 a MS 44 44 44 ^ ^-44 444 4 4 £.( closed -loop) 5. 4444 4 4 ^ 4

44 J£3 4£4 0.5Hz44. 4444 4£"^4 4444 £33=3144 ^ ^ 744 3 4 3-454 v4.

3 4 3-45. 4 4 4 4 43*34 4 44 £ * ^ 4 4 4 7 4 4 4 4

444-4 43*34 2:4 4 4 4 4 4 4 4 4 4 £ 4 44*} 4 4 4 4 4 4 4 4 *J3£.44 4 4 4 4 ^ 4 4 4 4 4 ^ 4 . 4 4 AA-^ 4 4 4 4 4 4 4 f 4 4 4 4 44 4 44 A44 4 4 4 4 4 44 ^ 4 4 AAA 4 4 4 3 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 X4 4 ^ 4 4 4 4 4 4 4 Y4 4 ^ 4 4 4 4 4A4 t & 4 4 ^ 4 4 4-4 A^A 4 1 4 ^ 4 . s&4 4 4 4 4 4 4 4 4 4 44 4 4 4 4 4 4 ^ 4 4 4 4 4 £.£4 4 4 4 4 4 4 4 4 4 4 4 7}4 4 4 4 4 4 4 4 4 44 i . 4 ^ 4 444-514. 441} 4 4 4 4 4 3 3 .4^4 4 4 4 ^ 4 4 4 4 4 4 4 AA 4 435.4 4 4 4 4 4 3?1\ # 4 4 4 .

- 216 -

4 474A-1 44*} 714 4 4 ^ 4 4 3 ^ 3-464 ^ 4 . 3 4 3-464 4 4 4 Shack-Hartmann44^ ^4^1 4 4 4 4 ^4"4 4 ^ 4 4 4 J±44 ^ 4 4 4 - 3 4 3-464 4 4 4 4 ^ 4 4 4 4 4 $444 4 4 4 4 4 &4 °§AA 4 4 4 4 4 4 4 4 4 4 4 4 ^44-3 X 4 4 4 Y4 4 ^ 3 . ^ 4 4 4 4 4 4 Si 4 °J444.

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Channels Configuration

Use i Channels

o 0 0

0 0 0 i n

Channel # 1 Channel # 2 Channel # 3 Channel # 4 Channel # 5 Channel # 6 Channel # 7 Channel # 8 Channel # 9

Channel # 10 '"rv-innfil * 11

OK

31

34 3-47. 4 4 4 4 4 £ 4 4 4 1 4 4 4 4t} ^ 4 4 4

- 217 -

Control Unt

System Delay j5 0 0

Numbei Electrodes ■

Polarization Voltages

1-stElecbod I * "

Wave Length um '-''u

b Lenslet Focus mm

u

Pwel Size, urn j8

-3

Channels Config

Another J300 Electrodes

Dark Spots Checking -Intensity I ' iS j f '

Threshold '•

f Full Aperture

tv Exclude Dark Frame

Reference Grid -

Spot's See j5

Ond Factoi

Focal Spot Filter

Filter Power

30

OK Cancel

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Pei-Nan Wan Lei Xu

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(AIOFM) Hongmei Wang

(AIOFM) Li Fang (AIOFM)

Xiaoming Gao (AIOFM) Ting Yu (SIOM)

^AiA^r Ultra sensitive laser spectroscopic technologies in

KAERI KAERI Raman Lidar System for Meteorological

parameter An adaptive optics system with hierarchical wave

front Recent development of laser-induced breakdown spectrometry (LIBS) for direct elemental analysis

Study on the vertical aerosol distribution by aerosol LIDAR at Korea Global atmosphere watch observatory

Analysis of the dual Fabry-Perot etalon for a direct detection wind lidar

Detection of sulfur dioxide by metastable N2 energy transfer

Design and performance of single particle laser mass spectrometer

Diode laser spectroscopy and its application

All solid state laser system for DIAL measurement of N02

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Zun Zhou (SIOM, CAS)

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Chinese Academy of Sciences Dr. Zhang Yinchao . Professor . Anhui Institute of Optics and Fine Mechanics (AIOFM),

- 238 -

- Mrs. Ting Yu . Engineer . Advanced Laser Technique & Applied System Laboratory . Shanghai Institute of Optics and Fine Mechanics

- Dr. Weijun Zhang , Professor . Lab. of Environmental Spectroscopy . Anhui Institute of Optics and Fine Mechanics (AIOFM),

~ Dr. Songlina Wu . Professor . Ocean Remote Sensing Institute . Ocean University of China

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(Atmospheric Optics Laboratory)

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compensation

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aerosol

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. Chemical mechanism of environmental pollution

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depletion processes

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methods

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satellite remote sensing of environment

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space-borne sensors

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infared hyper-spectroscopy, polarized spectroscopy and laser

fluorescence techniques

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waterbodies and solids

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C. ^ ^ " ^ r Homepage •§:*%-

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Prof. YoungPak Lee ( Hanyang University ) Title "Progress in Spin-photonics and Spin-photonic

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Baoli Yao (CIOPM)

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III-V Semicon. Photonic Devices in Korea

Crystal Growth and Properties of Optical LiNb03

Progress in spin-photonics and spin-photonic structures

Coihdal Photonic Crystal: Fabrication and optical characterization

Optical characterization of the narrow-band filter with in-situ spectrum monitoring by the high resolution infrared spectrometer

Current Injection Pulse-lasing of GaN-based Laser Diode in Peking University Xu Ke

Microstructural ferroelectric domain engineering

Organic and biological photochromic materials used in optical storage and processing

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(SIOM) Ruxin Li (SIOM)

Chen Jing (B1APCM)

Peixiang Lu (HUST)

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Qihong Lou (SIOM) Bo Pei

(GKLaser) Peng Zhou

(Fudan Univ.) Wei Zhao (XIOM)

Zhiyi Wei (IPHY)

Heping Zeng (ECN Univ.)

Ruxin Li (SIOM)

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Huanling Hu (AIOFM, China)

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Jun 2 (AIOFM, China)

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Bibliographic Information Sheet

Performinf Org. Report No.

Sponsoring Org Report No.

Standard Report No.

IN IS Subject Code

KAREI/RR-2737/2006

Title/Subtitle Korea-China Optical Technology Research Centre

Project Manager and Dpt. Kim, Cheol-Jung (Advanced Nuclear Technology Development)

Researcher and Dept.

H. K. Cha, Y. J. Rhee, S. M. Lee, B. D. Yoo, C. H. Um, S. M. Nam, J. M. Han, D. H. Kim, K. H. Yang, S. 0. Kwon, S. K. Park. Y. H. Cha( KAERI, Quantum Optics Center), Y. P. Lee( Han Yang Univ. Physics Department)

Pub, piace Taeion Pub Org KAERI Pub. Date 2004 6 Page p.274 Fig. & Tab Y ( 0 ), N ( ) Size 30cm Note

Classified Open( 0 ), Outside( ), Class Report Type Reserach Report Sponsoring Org Contract No.

Abstract ( 300 words

The main objectives of this project are to develop cooperative channel by personnel exchanges between industrial, educational and research partners of Korea and China on the fields of optica) technologies which are the basis of optical industry and being spot-lighted as new industry of 21th century, and to raise the class of Korean optical technology up to world class by utilization of Chinese large facilities through the cooperative research between the optical technology institutions of both sides.

To attain the goals mentioned above, we carried out the cooperative researches between the Korean and Chinese optical technology institutions in the following 7 fields,

o research cooperation between KAERI-SITP for the quantum structured far-TR sensor technology;

o research cooperation for the ge/ieration of femtosecond nuclear fusion induced neutrons; o research cooperation between KAERI-AIOFM for laser environment analysis and

remote sensing technology, o research cooperation between KAERI-SIOM for advanced diode-pumped laser

technology; o cooperative research related on linear and nonlinear magneto-optic a I properties of

advanced magnetic quantum structures; o design of pico-second PW high power laser system and its simulation and o cooperative research related on the fern to-second laser-plasma interaction physics.

Subject Keywords (about 10 words)

optical technologies, cooperative channel, personnel exchanges, research cooperation, nuclear fusion induced neutrons

Korea-China Optical Technology Research Centre - OSTI.GOV

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Transcript of Korea-China Optical Technology Research Centre - OSTI.GOV