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

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12.4 Radiationless processes in photoexcited molecules 244<br />

12.4 Radiationless processes in photoexcited molecules<br />

I<br />

Figure 12.2: Jablonski Diagram.<br />

Elementary Photochemical Processes: Jablonski Diagram<br />

Energy<br />

RXN<br />

(10 -14 .. 10 -6 s)<br />

S 2<br />

T 2<br />

IC<br />

S 2 -S 1 Abs.<br />

T 1<br />

T 2 -T 1 Abs.<br />

IVR<br />

IC<br />

VET* S 1<br />

ISC<br />

(10 -9 ..10 -3 s)<br />

S 0 VET* (10 -11 s)<br />

IVR (10 -13 ..10 -9 s)<br />

Absorption<br />

(10 -18 s)<br />

Fluorescence<br />

(10 -9 ..10 -8 s)<br />

Phosphorescence<br />

(10 -3 ..10 -6 s)<br />

*also known as VR<br />

<strong>Physical</strong> <strong>Chemistry</strong> III: <strong>Chemical</strong> <strong>Kinetics</strong> • © F. Temps, IPC Kiel 253<br />

12.4.1 The Born-Oppenheimer approximation and its breakdown<br />

a) The full Hamiltonian<br />

We consider a non-moving, non-rotating molecule in the laboratory framework. The<br />

molecule is described by the Schrödinger equation (SE)<br />

ˆ(r R) = (r R) (12.12)<br />

or ³<br />

ˆ − ´<br />

(r R) =0 (12.13)<br />

with being the energy eigenvalue associated with the wavefunction (r R) as function<br />

of the electronic (e) coordinates r and the nuclear (N) coordinates R.<br />

The Hamilton operator ˆ appearingintheSEcanbewrittenas<br />

ˆ = ˆ + ˆ = ˆ (r)+ ˆ (R)+ (r R) (12.14)<br />

where<br />

ˆ = − ~2<br />

2 <br />

X <br />

=1<br />

∇ 2 (12.15)<br />

ˆ = − ~2 X <br />

∇ 2 (12.16)<br />

2 <br />

=1

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