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Section Freq

This section contains information about (progress) of the Frequencies calculation and results.

kountf

An integer counter that keeps track of how many geometric displacements have been carried out to scan the potential energy surface around the equilibrium

nraman

Integer to flag whether or not Raman intensities are computed

numdif

Integer to determine the type of numerical differentiation (of gradients, to get the second derivative): 1=one-sided, 2=two-sided displacements.

disrad

Size of displacements of Cartesian coordinates or bond lengths (in case of displacements in internal coordinates)

disang

Size of displacements of angular coordinates

geocrd

Type (string) of coordinates to displace: CART or ZMAT

atmcrd

ZMAT if a z-matrix structure is available. This determines printed output but does not affect the computation. Compare the variable geocrd

nfree

The number of degrees of freedom

idfree

An array (3,natoms) that stores for each atomic coordinates (Cartesian or internal, depending on geocrd) the number of the (1..nfree) variational freedom it corresponds to. If zero, the coordinate is frozen by constraint.

xyz

Cartesian coordinates of the equilibrium geometry

kmatrix

Connection matrix that defines a Z-matrix

zmatrix

The Z-matrix variable values of the equilibrium geometry

all freedoms

Logical: true if all atomic coordinates are allowed to be displaced, not restricted by constraints.

nr of atoms

The total number of atoms, including dummy's

rigids

Vectors of rigid motion directions, expressed in the atomic coordinates (3,natoms,6)

Dipole previous

The dipole moment of the previous geometry. This is used to compute dipole derivatives by numerical differentiation. The 'previous' geometry is the equilibrium geometry in case of one-sided displacements.

Dipole

The dipole moment corresponding to the current geometry

Dipole derivatives

The matrix of dipole derivatives with respect to atomic displacements

Polbty previous

The polarizability tensor (6 elements, triangular representation) of the 'previous' geometry. See the remarks about the dipole moment

Polbty

The polarizability tensor corresponding to the current geometry

Polbty derivatives

The matrix of derivatives (w.r.t. the atomic coordinates) of the polarizability tensor

Gradients

The energy gradients corresponding to the current geometry

Gradients previous

The energy gradients of the 'previous' geometry. See the remarks about 'previous' dipole moment

Force constants

The matrix of force constants (second derivatives), built up during the frequencies calculation.

xyz displaced

The Cartesian coordinates of the current (displaced) geometry

zmatrix displaced

Internal coordinates of the current (displaced) geometry

Dipole derivatives_CART

Dipole derivatives with respect to Cartesian coordinate changes

Hessian_CART

The Hessian matrix in Cartesian coordinates, computed at the end, when the construction of the 'Force constants' has been completed.

Frequencies

An array with harmonic frequencies.

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