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ASE Suppression in a Diode-Pumped Nd:YLF Regenerative Amplifier Using a Volume Bragg Grating
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Transcript of ASE Suppression in a Diode-Pumped Nd:YLF Regenerative Amplifier Using a Volume Bragg Grating
ASE Suppression in a Diode-Pumped Nd:YLF Regenerative Amplifier Using a Volume Bragg Grating
A. V. OkishevUniversity of RochesterLaboratory for Laser Energetics
Frontiers in Optics 2007/Laser Science XXIIIOSA 91st Annual Meeting
San Jose, CA16–20 September 2007
Sp
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B)
–40
–30
–20
–10
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Wavelength (nm)
1053.0 1053.3 1053.6
MirrorVBG
Collaborators
A. V. Okishev, C. Dorrer, and J. D. Zuegel
Laboratory for Laser Energetics, University of Rochester
V. I. Smirnov
OptiGrate, Orlando
L. B. Glebov
CREOL, University of Central Florida, Orlando
Regenerative amplifier with volume Bragg grating (VBG) decreases out-of-band ASE to the more than –40-dB level
E16051
• VBGintroducedinthediode-pumpedregenerativeamplifier(DPRA) as a spectrally selective element does not alter the performance of DPRA.
• UnseededDPRAproduces150-pmFWHMwithamirrorand a43-pm-FWHMoutputspectrumwithVBG.
• Out-of-bandASEfilteringhasbeendemonstratedevenataverylow(comparable to ASE) level of DPRA seeding.
• DPRAwithVBGasasubsystemfortheopticalparametricchirped-pulse amplifier (OPCPA) pump provides significant temporal contrast improvement for recompressed pulse.
Summary
OMEGA EP is designed to achieve high radiation intensity on a target
E16052
Achieving high intensity on target requires high temporal contrast of the pulse to avoid target modifications before interaction with the main pulse.
OMEGA
Laser Bay Mainamplifiers
OMEGA EP Laser Bay OMEGA EP Laser Bay
Compressionchamber
OMEGA EPtargetchamber
Boosteramplifiers
Beam 1 2 3 4
OMEGA targetchamber
Performance capabilities
Short-pulseBeam 1
Pulse width 1 to 100 psEnergy on target (kJ)
2.6 kJ, 10- to 100-psgrating limited <10 ps
Intensity (W/cm2) ~2 × 1020
Focusing (diam) >80% in 20 nm
OPCPA is the heart of a laser system for generating high-intensity ultrashort pulses
E16053
The regenerative amplifier is an optimal subsystem of the OPCPA pump for ASE spectral filtering because of its high gain and multiple number of roundtrips, which allows using spectral filters in a multipass configuration.
ASE-induced temporal variations of the OPCPA pump lead to spectral-density variations of an amplified pulse that, in turn, deteriorate the temporal contrast of the recompressed pulse.
OPCPA pump
Masteroscillator
Regenerativeamplifier
Poweramplifier SHG
Mode-lockedlaser
Stretcher OPCPAamplifier
Nd:glass mainamplifier
CompressorTarget
chamber
Filtering the OPCPA pump to reduce the ASE bandwidth greatly improves the temporal contrast of the OPCPA signal
E16054
OPCPA parameters• High-gainpreamplifier(2 × 29.75 mm of LBO) operated at saturation• ASEwithGaussianspectraldensityandFWHMequalto140pmor30pm• EnergyofASEinthedurationofthepumpis0.1%ofthetotalenergyofthepump• 1053-nmsignalwith8-nmbandwidth
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No
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Time (ps)
Simulated signal amplified inconventional OPCPA system
Simulated signal amplified with filtered pump pulse
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–80
–100–100 –50 0 50 100
Time (ps)
ASE FWHM = 140 pm ASE FWHM = 30 pm
–100 –50 0 50 100
Angularly tuned VBG is used in DPRA* as a spectrally selective element for ASE suppression
E16055
Using an angularly tuned VBG doubles the number of passes for better spectral selectivity.
* The DPRA design is identical to the one described in A. V. Okishev and J. D. Zuegel, “Highly stable, all-solid-state Nd:YLF regenerative amplifier,” Appl. Opt. 43, 6180–6186 (2004).
VBGNd:YLF
Pump
Seed
Opticalspectrumanalyzer
(OSA)
Beamdiagnostics
(CCD)
Energymeter
DPRA
VBGwitha230-pm-FWHMfilterfunctionproducesa 23-pm-FWHMfilterfunctionafter50two-passround-tripswithout distorting the temporal pulse shapes
E15623
200 0 200
0.5
1.0
Wavelength offset (pm)
Experimental data
Simulations
Inte
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0.5
1.0
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One passTwo passes, 50 round-trips
–1 0 1Time (ns)
–2 –1 0 1 2Time (ns)
MirrorVBG
Input pulseFiltered pulse
The DPRA output-beam profile is not affected by using VBG as a resonator element
E15624
DPRA output energy is reduced by ~25% due to lower VBG reflectivity. This decrease has been compensated for by the pump-diode-current increase.
0.0
0.2
0.4
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0.8
1.0
DPRA with mirror(R = 99.8%)
DPRA with VBG(R = 99.4%)
VBG narrows the unseeded DPRA output spectrum from150pmto43pmFWHM
E15625
In the DPRA with VBG, the spectral width and shape are defined by the common action of the VBG reflection curve and Nd:YLF gain profile.
MirrorVBG
0.0
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0.8
1.0
Sp
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Linear scale
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–20
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1053.0 1053.3 1053.6
Sp
ectr
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B)
Wavelength (nm)
1053.0 1053.3 1053.6Wavelength (nm)
log scale
VBG in seeded DPRA provides out-of-band ASE suppression to the –40-dB OSA dynamic-range limit
E15626
Simulations show that for a reliable OSA recording of an ASE filtering effect the injected energy must be about equal to the DPRA ASE. In this case EASE = 0.7 Ein; seed-pulse energy is 0.0025 pJ; DPRA gross gain is >1012.
0.00.20.40.60.81.0
Sp
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Sp
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–30
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1053.0 1053.3 1053.6Wavelength (nm) Wavelength (nm)
Simulation Experimental Data
1053.0 1053.3 1053.6
MirrorVBG
Linearscale
logscale
Using a DPRA with VBG provides OPCPA output-contrast improvement even when the DPRA seed is 100× reduced
E16056
Third-order scanning cross correlation of the OPCPA output pulses
Nominal seed-pulse energy is 100 pJ
–100
–80
–60
–40
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1000Time (ps)
Inte
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dB
)
–100 1000Time (ps)
Prepulse contrast enhancement
Seed-pulse energy is reduced to 1 pJ
MirrorVBG
Regenerative amplifier with volume Bragg grating (VBG) decreases out-of-band ASE to the more than –40-dB level
E16051
Summary/Conclusions
• VBGintroducedinthediode-pumpedregenerativeamplifier(DPRA) as a spectrally selective element does not alter the performance of DPRA.
• UnseededDPRAproduces150-pmFWHMwithamirrorand a43-pm-FWHMoutputspectrumwithVBG.
• Out-of-bandASEfilteringhasbeendemonstratedevenataverylow(comparable to ASE) level of DPRA seeding.
• DPRAwithVBGasasubsystemfortheopticalparametricchirped-pulse amplifier (OPCPA) pump provides significant temporal contrast improvement for recompressed pulse.