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

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Appendix D 272<br />

Final solutions for [B ()]:<br />

i.e.<br />

[B ()] = − 1 [A] 0<br />

2 − 1<br />

× − 2 + 1 [A] 0<br />

2 − 1<br />

− 1 <br />

= 1 [A] 0<br />

2 − 1<br />

− 1 − 1 [A] 0<br />

2 − 1<br />

× − 2 <br />

[B ()] = 1 [A] 0<br />

1 − 2<br />

× ¡ − 2 − − 1 ¢<br />

(C.63)<br />

(C.64)<br />

(C.65)<br />

• In the time-resolved fluorescence measurements, we observe<br />

() ∝ [A ()] + [B ()]<br />

(C.66)<br />

with some unknown factor accounting for the (lower) transition probability of<br />

state B, i.e., the fluorescence-time profile () is<br />

() =[A] 0<br />

− 1 + 1 [A] 0<br />

1 − 2<br />

× ¡ − 2 − − 1 ¢<br />

=[A] 0<br />

− 1 + 1 [A] 0<br />

1 − 2<br />

× − 2 − 1 [A] 0<br />

1 − 2<br />

× − 1 <br />

= µ<br />

1 [A] 0<br />

× − 2 + [A]<br />

1 − 0<br />

− <br />

1 [A] 0<br />

× − 1 <br />

2 1 − 2<br />

= 2 × − 2 + 1 × − 1 <br />

(C.67)<br />

(C.68)<br />

(C.69)<br />

(C.70)<br />

This is the same result as would be obtained by a fit toasumoftwoexponentials<br />

with the rate constants 1 = 1 + 1 and 2 , i.e., time constants<br />

1 =( 1 + 1 ) −1 and 2 = 2 .

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