Physical Chemistry 3: — Chemical Kinetics — - Christian-Albrechts ...

Physical Chemistry 3: — Chemical Kinetics — - Christian-Albrechts ... Physical Chemistry 3: — Chemical Kinetics — - Christian-Albrechts ...

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Appendix B 265 I Figure B.1: Exponential decay curve of a particular vibration-rotation state of the CH 3 O radical resulting from the unimolecular dissociation reaction of the radical according to CH 3 O → H+H 2 CO (Dertinger 1995). The small box is the output box from a fit usingtheORIGINprogram. I Example 2: Multiexponential decay. In femtosecond spectroscopy, we often observe ultrafast multiexponential decays of laser-excited molecules. The laser prepares an excited wavepacket, which usually does not decay single-exponentially. Further, we need to take into account the final duration of the pump laser pulse (by deconvolution, or by forward convolution). • Model function to be fitted to measured data: () = X exp (− ) (B.11) with adjustable parameters and . • Instrument response function (IRF): Often represented by a Gaussian centered at time 0 Ã ! 1 () = √ exp − ( − 0) 2 (B.12) IRF 2 2 2 IRF with width parameter IRF related to the full width at half maximum (FWHM) of the IRF by FWHM = √ 8ln2≈ 2355 IRF (B.13)

Appendix C 266 • Convolution of the molecular intensity () and () gives the signal function () = Z +∞ −∞ ( 0 ) ( − 0 ) 0 = where ⊗ denotes the convolution. Z +∞ −∞ ( − 0 ) ( 0 ) 0 = () ⊗ () (B.14) • Resulting model function to be fitted to the data: () = 1 X ∙ 1 2 IRF exp − ( − ¸ ∙ µ ¸ 0) ( − 0 ) − 2 IRF 1+erf √ + 2 2 2 2IRF (B.15) where erf () is the error function and is a simple constant background term (can be replaced by background + drift + ). I Figure B.2: Excited-state relaxation dynamics of the adenine dinucleotide after UV photoexcitation. I References: Bevington 1992 P. R. Bevington, D. K. Robinson, Data Reduction and Error Analysis for the Physical Sciences, McGraw-Hill, Boston, 1992. Dertinger 1995 S. Dertinger, A. Geers, J. Kappert, F. Temps, J. W. Wiebrecht, Rotation-Vibration State Resolved Unimolecular Dynamics of Highly Vibrationally Excited CH 3 O( 2 ): III. State Specific Dissociation Rates from Spectroscopic Line Profiles and Time Resolved Measurements, Faraday Discuss. Roy. Soc. 102, 31 (1995). Press 1992 W. H. Press, S. A. Teukolsky, W. T. Vetterling, B. P. Flannery, Numerical Recipes in Fortran, Cambridge University Press, Cambridge, 1992. Versions are also available for C and Pascal.

Appendix B 265<br />

I<br />

Figure B.1: Exponential decay curve of a particular vibration-rotation state of the<br />

CH 3 O radical resulting from the unimolecular dissociation reaction of the radical according<br />

to CH 3 O → H+H 2 CO (Dertinger 1995). The small box is the output box<br />

from a fit usingtheORIGINprogram.<br />

I Example 2: Multiexponential decay. In femtosecond spectroscopy, we often observe<br />

ultrafast multiexponential decays of laser-excited molecules. The laser prepares<br />

an excited wavepacket, which usually does not decay single-exponentially. Further, we<br />

need to take into account the final duration of the pump laser pulse (by deconvolution,<br />

or by forward convolution).<br />

• Model function to be fitted to measured data:<br />

() = X exp (− )<br />

(B.11)<br />

with adjustable parameters and .<br />

• Instrument response function (IRF): Often represented by a Gaussian centered at<br />

time 0 Ã !<br />

1<br />

() = √ exp − ( − 0) 2<br />

(B.12)<br />

IRF 2 2 2 IRF<br />

with width parameter IRF related to the full width at half maximum (FWHM)<br />

of the IRF by<br />

FWHM = √ 8ln2≈ 2355 IRF<br />

(B.13)

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