28.02.2013 Views

Handbook of Solvents - George Wypych - ChemTech - Ventech!

Handbook of Solvents - George Wypych - ChemTech - Ventech!

Handbook of Solvents - George Wypych - ChemTech - Ventech!

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

664 Mati Karelson<br />

vector, containing the unknown surface charges. Ein is also a column vector collecting the<br />

effective components <strong>of</strong> the solute electric field multiplied by the surface elements<br />

�<br />

0<br />

E =−ΔS ∇Φ<br />

s n [11.1.81]<br />

( )<br />

in, k k M, in k k<br />

The D matrix depends only on the shape <strong>of</strong> the cavity and the dielectric constant <strong>of</strong> the<br />

medium. Therefore, when the system <strong>of</strong> linear equations [11.1.80] has to be solved several<br />

times with different E in, as in the case <strong>of</strong> the polarizable solute, it may be convenient to work<br />

with the single inversion matrix D -1 .<br />

The PCM model has been implemented for the calculation <strong>of</strong> the electronic excitation<br />

energies <strong>of</strong> solvated molecules within the quantum-mechanical configuration interaction<br />

method. 47,48 The respective final expression for the excitation energy from the ground state<br />

(0) to the I-th state has the following form<br />

1<br />

ΔW = ΔE<br />

− − + − +<br />

( 0I) ( 0I)<br />

CI [ J20( PI 2<br />

P0) PT 0 0( PI P0)<br />

]<br />

[ J2∞( PI P0) P IT∞( PI − P0)<br />

]<br />

1<br />

+ − +<br />

2<br />

[11.1.82]<br />

where P I and P 0 are the electronic density matrices <strong>of</strong> the solute in the excited state and in<br />

the ground state, respectively,<br />

[ ( ) ( ) ( ) ]<br />

( 0I)<br />

1<br />

ΔECI EI E0<br />

I 0 0 0 I 0 10 20 I 0<br />

2 2<br />

= − + P − P T P + P − P J + J P −P<br />

[11.1.83]<br />

are the diagonal elements <strong>of</strong> CI matrix, and<br />

−<br />

T = C W C<br />

t 1 ∂ � [11.1.84]<br />

−1<br />

J = CW ∂MZ � [11.1.85]<br />

1<br />

t t<br />

J = Z M W<br />

2<br />

−1<br />

−<br />

B= Z M W MZ<br />

∂C� [11.1.86]<br />

t t 1 ∂ � [11.1.87]<br />

In the last equations, C and ∂ � Care the matrices representing the electrostatic potential<br />

and the electric field generated from the electron distribution in the solute molecule, respectively.<br />

The matrices M and ∂ � Mare the matrices representing the electrostatic potential and<br />

the electric field generated from the nuclear charges in the solute molecule, respectively.<br />

The diagonal elements <strong>of</strong> the matrix W are defined as the following function <strong>of</strong> the dielectric<br />

constant <strong>of</strong> the solvent<br />

Wii = + ε 1<br />

ε − 1<br />

[11.1.88]<br />

The subscripts 0 and ∞ in the J 1, J 2, and T matrices in equation [11.1.82] correspond to<br />

the static and optical dielectric constant <strong>of</strong> the solvent. Equation [11.1.82] can be considered

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!