Difference between revisions of "Fdkup.m"
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==See also== | ==See also== | ||
[[fdvec.m]], [[fdlap.m]], [[fdhess.m]], [[fdmat.m]], [[fdweights.m]], [[fftdiff.m]], [[fourdif.m]], [[fourlap.m]] | [[fdvec.m]], [[fdlap.m]], [[fdhess.m]], [[fdmat.m]], [[fdweights.m]], [[fftdiff.m]], [[fourdif.m]], [[fourlap.m]] | ||
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''Version 2.2, authors: [[Gareth Charnock]], [[Ilya Kuprov]]'' | ''Version 2.2, authors: [[Gareth Charnock]], [[Ilya Kuprov]]'' | ||
Revision as of 12:25, 25 April 2026
Returns a finite difference representation of the Kuprov operator:
K[rho]=-(1/3)*Trace(Hessian[rho]*chi)
with the number of stencil points in the finite difference approximation specified by user. The resulting operator is a sparse matrix designed to act on the vectorisation of rho. The dimensions of rho are assumed to be ordered as [X Y Z]. For further information, see http://dx.doi.org/10.1039/C4CP03106G.
Contents
Syntax
K=fdkup(npoints,extents,chi,nstenc)
Arguments
npoints - a three-element vector specifying the dimensions
of the 3D cube of data that the operator will be
acting on, in Angstroms. The dimensions are assu-
med to be ordered as [X Y Z].
chi - the electron magnetic susceptibility tensor in
cubic Angstroms, a symmetric 3x3 matrix.
extents - a three-element vector specifying axis extents
in Angstroms. The dimensions are assumed to be
ordered as [X Y Z].
nstenc - number of finite-difference stencil points for
the finite-difference approximation. Periodic
boundary conditions are used.
Outputs
K - a sparse matrix designed to act on the vectori-
zation of the array. The dimensions are assumed
to be ordered as [X Y Z].
See also
fdvec.m, fdlap.m, fdhess.m, fdmat.m, fdweights.m, fftdiff.m, fourdif.m, fourlap.m
Version 2.2, authors: Gareth Charnock, Ilya Kuprov