Pulse (photon) counting: determination of optimum measurement system parameters
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Transcript of Pulse (photon) counting: determination of optimum measurement system parameters
Hyphenated Techniques
Hyphenated Techniques combine chromatographic and spectral methods to exploit the advantages of both.
Chromatography - Produces pure or nearly pure fractions of chemical components in a mixture.
Spectroscopy – Produces selective information for identification using standards or library spectra.
LC-Absorbance Data
James K. Hardy and The University of Akron http://ull.chemistry.uakron.edu/chemsep/hyphen/
Spectra to Identify and Test Purity
Sample spectra overlaid with standard spectra
Sign
al
Wavelength (nm)190 230 270 310 360 390
Sign
al
Wavelength (nm)190 230 270 310 360 390
Overlaid spectra from beginning, middle and end of
eluting peak
LC with UV Absorbance Detection
D. Wickam in A Practical Guide to HPLC Detection, D. Parriott, ed., Academic Press, San Diego, CA, 1993, p67
Fully Integrated Positive-PressureDriven Microfabricated Liquid Analyzer
The basic idea is to incorporate on-chip near real-timesampling, capillary separation, and multivariatedetection in a single integrated microfabricated device. Soft lithography is used for rapid prototyping for proof of principle design and testing.
References:
(1) Initial analyzer development - P. G. Vahey, S.H. Park, B. J. Marquardt, Y. Xia, L. W. Burgess and R.E. Synovec, Talanta, 2000, 51, 1205 - 1212.
(2) Incorporation of GLRS detection - P.G.Vahey, S. A. Smith, C. D. Costin,Y. Xia, A. Brodsky, L.W. Burgess and R. E. Synovec, Analytical Chemistry,2002, 74, 177 - 184.
Separation Channel
SampleBy-pass
SampleInlet
Mobile Phase
Inlet
Outlet
Detection Region
100µm10µm
Channels in PDMS
Micro-fabricated Liquid Analyzer
BlockBy-passMobile
Phase Inlet
SampleBy-pass
Sub-Nanoliter Sample Injection by Flow ProgrammingPositive pressure driven with a pump.
An alternative to electrophoretic and electro-osmotic flow
Inject Sample
SampleInlet
To Separation
Channel
Micro-fabricating a Channel
1. Spin Coatphotoresist
2. UV Exposure 3. Develop Channel Master
4. Cast PDMS 5. Remove PDMS(stationary phase)
6. Affix PDMSto glass substrateusing thin PDMS coat
3 injections, 2 nL each
4 6 8 10
0
40
80
Time, min
Abso
rban
ce, m
AUAutomation Provides Reproducible Injection
8 mM Bromocresol Green
5 mM phosphate mobile phase, pH 7, 40 nL/min
PDMS channel 100 µm x 10 µm x 23 cm
Valcor Solenoid
Absorbance Detection Ocean Optics SD2000
Micro-fabricated LC with Absorbance Detection
Water m.p., 6 nL/min
Injected Volume 1 nL
Separation Channel in PDMS 100 µm x 10 µm x 6.6 cm
Absorbance Detection using Equitech Spectrophotometer
400500
600700
600650
700750
800
Time, secWavelength, nm
FD&C Red #3
FD&C Blue #1
Micro-fabricated LC Separation of Two DyesTemporal and Spectral Selectivity are Both Provided
Water m.p., 6 nL/min
Injected Volume 1 nL
Separation Channel in PDMS 100 µm x 10 µm x 6.6 cm
Absorbance detection using Equitech spectrophotometer
FD&C Red #3
FD&C Blue #1
400 500 600 700600
650
700
750
800
Wavelength, nm
Tim
e, s
ec
LC vs. Micro-fabricated LCLab Scale Microfabricated
Column Diameter 4.6 mm 10 µm x 100 µm
Flow Rate 1 mL/min 10 nL/min
Waste Generated 500 L/year 5 mL/year
Sample Used 10 µL 1 nL or less
Pump Pressure 1000 psi 5 psi
Cost per column $400 and up $10
“A disposable, plug and play LC device.”
The basic idea is to utilize optical waveguide principles to produce a low volume (~ 2 µL) detection cell that simultaneously provides over a 1000-fold enhancement in the limit of detection relative to a typical Raman measurement. A Teflon AF 2400 tube provides a lower refractive index than just about any liquid of interest, so the tube functions as a long optical path Raman detection cell. The flow cell is suitable for HPLC, FIA or direct process monitoring.
Reference:
B. J. Marquardt, P. G. Vahey, R. E. Synovec and L. W. BurgessAnalytical Chemistry, 1999, 71, 4808 - 4814.
Raman Spectroscopy:
Application to Process Analysis and HPLC Detection
Light Scattering• Two types of Electromagnetic Radiation scatter occur
•Elastic (Rayleigh scatter)
•Inelastic (Raman scatter)
Incident Beam
• Raman spectroscopy provides information about vibrational energies of molecules
• The Raman mechanism is emission from a momentarily induced dipole versus a change in dipole vibrational mode for molecular IR
• Raman is complementary to IR, producing relatively stronger peaks for symmetrical stretching versus anti-symmetrical stretching modes
Raman versus IR Spectroscopy
Benefits of Raman Spectroscopy
• Multicomponent Analysis
• Useful for measuring aqueous phase chemistries
• Identification of analytes by molecular signature
• Spectra obtained in seconds
• Applicable to in situ analysis
• Ease of sampling ! no sample pretreatment needed! only require optical access to sample
Raman-Waveguide Detector: Using a Liquid Core Waveguide (LCW) Flow Cell
10x
785 nmLaser
RamanDetector
Sampling Window
Teflon AF Waveguide Flow Cell
Sample Outlet
HPLC Fitting
Sample Inlet
• Basics of light transmission in an optical fiber/waveguide
• Fibers/waveguides consist of a core, RI = n1, and a cladding, RI = n2
• Numerical aperture (NA) describes the acceptance cone
• NA = sin θa = (n12 - n2
2)1/2
• Critical angle for transmission of light, sin θc = n2/n1 ( n1 > n2 required)
θθθθa
cladding (tube) critical anglecore
eventually lost
θθθθc
Total Internal Reflection: Basics for LCW construction
acceptance cone
n1
n2
Index of Refraction for LCW Materials
Values from: Applied Spectroscopy, 1990, 40, 163-5 and Applied Optics, 1997, 36, 8992-8
Solvents and Cell Materials Index of Refraction (RI)
Teflon AF 2400 (capillary tube) 1.29 (good choice)Teflon AF 1600 1.31Methanol 1.326Water (solvent) 1.333
FEP 1.338Acetonitrile 1.342Acetone 1.357
PTFE 1.35-1.381-Butanol 1.397Chloroform 1.444
Quartz 1.458Benzene 1.498Bromoform 1.587
Excitation and Raman Scatterin an Optical Waveguide
Benefits of the liquid core optical waveguide(1) Enables the excitation of more molecules since total internal reflection
in sampling tube (flow cell) increases pathlength within a small volume (2) Since Raman scatter is isotropic it allows very efficient collection of the
Raman scattered light