Physical Chemistry 3: — Chemical Kinetics — - Christian-Albrechts ...
Physical Chemistry 3: — Chemical Kinetics — - Christian-Albrechts ... Physical Chemistry 3: — Chemical Kinetics — - Christian-Albrechts ...
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.
- Page 229 and 230: 9.2 Heat explosions 214 10. Catalys
- Page 231 and 232: 10.1 Kinetics of enzyme catalyzed r
- Page 233 and 234: 10.2 Kinetics of heterogeneous reac
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- Page 243 and 244: 11.1 Qualitative model of liquid ph
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- Page 247 and 248: 11.2 Diffusion-controlled reactions
- Page 249 and 250: 11.3 Activation controlled reaction
- Page 251 and 252: 11.4 Electron transfer reactions (M
- Page 253 and 254: 11.5 Reactions of ions in solutions
- Page 255 and 256: 11.5 Reactions of ions in solutions
- Page 257 and 258: 12.2 Fluorescence quenching (Stern-
- Page 259 and 260: 12.4 Radiationless processes in pho
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- Page 273 and 274: 14 Combustion chemistry* 258 15. As
- Page 275 and 276: 16 Energy transfer processes* 260 1
- Page 277 and 278: Appendix B 262 Appendix A: Useful p
- Page 279: Appendix B 264 The Marquardt-Levenb
- Page 283 and 284: Appendix C 268 C.2 Application to t
- Page 285 and 286: Appendix C 270 C.3 Application to p
- Page 287 and 288: Appendix D 272 Final solutions for
- Page 289 and 290: Appendix D 274 D.2 Special matrices
- Page 291 and 292: Appendix D 276 I Multiplication by
- Page 293 and 294: Appendix D 278 D.4 Coordinate trans
- Page 295 and 296: Appendix D 280 D.5 Systems of linea
- Page 297 and 298: Appendix D 282 D.6 Eigenvalue equat
- Page 299 and 300: Appendix E 284 Secular equation: de
- Page 301 and 302: Appendix E 286 Appendix E: Laplace
- Page 303 and 304: Appendix F 288 Appendix F: The Gamm
- Page 305 and 306: Appendix G 290 Appendix G: Ergebnis
- Page 307 and 308: Appendix G 292 I Anschauliche Bedeu
- Page 309 and 310: Appendix G 294 Ergebnis: = 1 X
- Page 311 and 312: Appendix G 296 (2) Grenzfall für
- Page 313 and 314: Appendix G 298 G.4 Mikrokanonische
- Page 315 and 316: Appendix G 300 G.5 Statistische Int
- Page 317 and 318: Appendix G 302 y = (G.7
- Page 319 and 320: Appendix G 304 G.8 Zustandssumme f
- Page 321 and 322: Appendix G 306 G.9 Zustandssumme f
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)