19.01.2015 Views

MOLPRO

MOLPRO

MOLPRO

SHOW MORE
SHOW LESS

Create successful ePaper yourself

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

47 POTENTIAL ENERGY SURFACES (SURF) 351<br />

47 POTENTIAL ENERGY SURFACES (SURF)<br />

SURF,Start1D=label1,options<br />

The SURF program allows for the calculation of the potential energy surface around the equilibrium<br />

structure as required for the calculation of anharmonic frequencies (see the VSCF and<br />

VCI programs). Currently the program is limited to the case of one minimum. The potential<br />

is represented by energy grid points rather than a Taylor expansion. Within the SURF program<br />

the potential energy surface is expanded in terms of normal coordinates, linear combination of<br />

normal coordinates or localized normal coordinates. Consequently, a harmonic frequency calculation<br />

needs to be performed first. The potential will then be represented by a hierarchical<br />

scheme given by<br />

with<br />

V (q 1 ,...,q 3N−6 ) = ∑<br />

i<br />

V i (q i ) +∑V i j (q i ,q j ) + ∑ V i jk (q i ,q j ,q k ) + ... (64)<br />

i< j<br />

i< js<br />

V rs (q r ,q s ) −<br />

∑<br />

r ∈{i, j,k}<br />

V r (q r ) − V (0) (67)<br />

V i jkl (q i ,q j ,q k ,q l ) = ... (68)<br />

where q i denotes the coordinates. This expansion needs to be terminated after an n-body contribution<br />

as controlled by the keyword NDIM. The SURF program is fully parallelized in a sense<br />

that the calculation of different grid points is send to different processors (MPPX scheme). The<br />

START1D keyword is mandatory and defines the label where to jump in the input in order to<br />

do an electronic structure calculation which is terminated by the SURF command. This way the<br />

quality of the potential energy surface is defined.<br />

label1<br />

hf<br />

ccsd<br />

surf,start1D=label1<br />

The SURF program is based on a iterative algorithm, i.e. grid points will be added automatically<br />

to the grid representation of the potential until a convergence threshold will be met. This<br />

guarantees a well-balanced description of the different terms in the expansion of the potential<br />

and simultaneously minimizes the number of ab initio calculations for a representation of the<br />

potential. For further details see:<br />

G. Rauhut, Efficient Calculation of Potential Energy Surfaces for the Generation of Vibrational<br />

Wave Functions, J. Chem. Phys. 121, 9313 (2004).<br />

T. Hrenar, H.-J. Werner, G. Rauhut Accurate Calculation of Anharmonic Vibrational Frequencies<br />

of Medium Sized Molecules Using Local Coupled Cluster Methods, J. Chem. Phys. 126,<br />

134108 (2007).

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

Saved successfully!

Ooh no, something went wrong!