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

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12.4 Radiationless processes in photoexcited molecules 250<br />

I<br />

Figure 12.6: Conical intersection of potential energy surfaces of a polyatomic molecule.<br />

Conical Intersections of Potential Surfaces in Polyatomic Molecules<br />

V E W V V V V<br />

1 2 1 2 1 2<br />

0 E<br />

W<br />

with: ; <br />

W V2<br />

E<br />

2 2<br />

V<br />

S 2<br />

Conical Intersections<br />

Diatomic Molecules: s = 1<br />

<br />

2<br />

V ( R) ( R) ( R) W( R)<br />

S 1<br />

S 0<br />

Q 1<br />

Q 2<br />

Polyatomic Molecules: s = 3N-6<br />

V ( Q , Q ) ( Q , Q )<br />

<br />

1 2 1 2<br />

<br />

( Q , Q ) W( Q , Q ) <br />

<br />

1 2 1 2<br />

2<br />

<strong>Physical</strong> <strong>Chemistry</strong> III: <strong>Chemical</strong> <strong>Kinetics</strong> • © F. Temps, IPC Kiel 257<br />

12.4.3 Quantum mechanical treatment of a coupled 2×2 system<br />

We can easily verify the “avoided crossing” of two coupled potential energy curves as<br />

follows:<br />

I<br />

Schrödinger equation:<br />

( − ) |i =0 (12.36)<br />

I<br />

Hamilton-Operator:<br />

= (0) + (1) (12.37)<br />

I<br />

Ansatz:<br />

|i = 1 | 1 i + 2 | 2 i (12.38)<br />

with orthonormal basis vectors that are eigenvectors of (0) , i.e.,<br />

½<br />

­ ® 1<br />

| = =<br />

0<br />

for = <br />

for 6= <br />

(12.39)<br />

and the zero-order energies<br />

(0) | 1 i = (0)<br />

1 | 1 i (12.40)<br />

(0) | 2 i = (0)<br />

2 | 2 i (12.41)

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