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

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12.4 Radiationless processes in photoexcited molecules 252<br />

With some rewriting 53 ,weobtain<br />

± = 1 ³ ´<br />

(0)<br />

1 + (0)<br />

2 ± 1 r ³<br />

(0)<br />

1 + (0)<br />

´2<br />

(0)<br />

2 − 4 1 (0)<br />

2 +4| 12 | 2 (12.58)<br />

2<br />

2<br />

y<br />

± = 1 2<br />

³ ´<br />

(0)<br />

1 + (0)<br />

2 ± 1 r ³<br />

(0)<br />

1 − (0)<br />

´2<br />

2 +4|12 | 2 (12.59)<br />

2<br />

I Shorthand form: Using the abbreviations<br />

± (R) = ± (12.60)<br />

1 (R) = (0)<br />

1 (12.61)<br />

2 (R) = (0)<br />

2 (12.62)<br />

2 (R) =| 12 | 2 (12.63)<br />

Σ (R) = 1 2 ( 1 (R)+ 2 (R)) (12.64)<br />

∆ (R) = 1 2 ( 1 (R) − 2 (R)) (12.65)<br />

we can rewrite the solution for the eigenvalues + and − in a compact form as<br />

± (R) =Σ (R) ±<br />

q<br />

(∆ (R)) 2 +( (R)) 2 (12.66)<br />

12.4.4 Radiationless processes in polyatomic molecules: Conical intersections<br />

I “Traditional” view on the cis-trans isomerization of C 2 H 4 :<br />

• Reaction coordinate can be approximated by torsion angle (0 ≤ ≤ 180 ◦ ).<br />

• Reaction proceeds via a perpendicular transition state ( =90 ◦ ), in which the C<br />

atoms are connected by a single bond.<br />

• Correlation diagram shows that the orbital of the trans-isomer transforms into<br />

the ∗ orbital of the cis-isomer and vice versa.<br />

• Crossing of the two diabatic states corresponds to an avoided crossing of the<br />

adiabatic states.<br />

53<br />

³<br />

(0)<br />

1 + (0)<br />

´2 ³<br />

(0)<br />

2 − 4 1 (0) 2 =<br />

(0)<br />

1<br />

´2<br />

+<br />

³<br />

³<br />

=<br />

(0)<br />

2<br />

(0)<br />

1<br />

´2<br />

+2<br />

(0)<br />

´2<br />

+<br />

³<br />

1 (0) 2 − 4 (0)<br />

1 (0) 2<br />

(0)<br />

2<br />

´2<br />

− 2<br />

(0)<br />

1 (0) 2 =<br />

³<br />

(0)<br />

1 − (0)<br />

´2<br />

2

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