Correlation.m

Correlation order selection function - keeps only the specified orders of spin correlation in the state vector. This is useful as a replacement for gradients and phase cycles because correlation order filtering can be accomplished analytically, by just picking out the required correlation orders and zeroing everything else.

Syntax

    rho=correlation(spin_system,rho,correlation_orders,spins)

Parameters

  rho     -  a state vector or a horizontal stack thereof

  orders  -  a row vector of correlation orders to keep

  spins   -  which spins to consider (e.g. '1H', '13C', 'all')

Outputs

  rho     - the state vector with the undesired orders of
            spin correlations zeroed out

Notes

Because quantum number information is required for this function to work, it is restricted to sphten-liouv formalism. It supports Fokker-Planck direct products.

See also

adelim.m, coherence.m, dfpt.m, homospoil.m, human2opspec.m, lin2lm.m, lin2lmn.m, lm2lin.m, lmn2lin.m, path_trace.m, scomponents.m, sinkhole.m, sparse2csr.m, sphten2zeeman.m, stitch.m, zte.m, Kernel_functions, Kernel_utilities

Version 2.8, authors: Ilya Kuprov, Luke Edwards