Difference between revisions of "Coherence.m"
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| − | Coherence selection function - keeps only the specified coherence | + | {{DISPLAYTITLE:function.m}} |
| + | Coherence order selection function - keeps only the specified orders of coherence in the state vector. This function is useful as a replacement for gradients and phase cycles because coherence order filtering can be accomplished analytically, by just picking out the required coherence orders and zeroing everything else. | ||
| + | |||
| + | ==Syntax== | ||
rho=coherence(spin_system,rho,spec) | rho=coherence(spin_system,rho,spec) | ||
| − | Arguments | + | ==Arguments== |
| + | |||
| + | rho - a state vector or a horizontal stack thereof | ||
| + | |||
| + | spec - a cell array containing the specification of | ||
| + | which coherences to keep on which spins. For | ||
| + | example | ||
| + | {{'13C',[1 -1]},{'1H',-1}} | ||
| + | |||
| + | keeps the states that have coherence order | ||
| + | |||
| + | ((1 OR -1 on 13C) AND (-1 on 1H)) | ||
| − | + | ==Outputs== | |
| − | + | rho - the state vector with the undesired orders of | |
| − | + | spin correlations zeroed out | |
| − | Examples | + | ==Examples== |
rho=coherence(spin_system,rho,{{'13C',[1 -1]},{'1H',-1}}) | rho=coherence(spin_system,rho,{{'13C',[1 -1]},{'1H',-1}}) | ||
| − | + | keeps all states that simultaneously have coherence order 1 or -1 in the 13C subspace, and coherence order -1 in the 1H subspace. | |
rho=coherence(spin_system,rho,{{3,0},{5,-1}}) | rho=coherence(spin_system,rho,{{3,0},{5,-1}}) | ||
| − | + | keeps all states that simultaneously have coherence order 0 on spin number 3, and coherence order -1 on spin number 5. | |
| + | |||
| + | ==Notes== | ||
| + | Because projection quantum number information is required, this function only works with ''sphten-liouv'' [[Basis set specification|formalism]]. It supports Fokker-Planck direct products. | ||
| + | |||
| + | ==See also== | ||
| + | Links to related functions. | ||
| − | |||
| − | '' | + | ''Version 2.2, authors: [[Ilya Kuprov]], [[Luke Edwards]]'' |
Revision as of 14:18, 28 August 2018
Coherence order selection function - keeps only the specified orders of coherence in the state vector. This function is useful as a replacement for gradients and phase cycles because coherence order filtering can be accomplished analytically, by just picking out the required coherence orders and zeroing everything else.
Contents
Syntax
rho=coherence(spin_system,rho,spec)
Arguments
rho - a state vector or a horizontal stack thereof
spec - a cell array containing the specification of
which coherences to keep on which spins. For
example
{{'13C',[1 -1]},{'1H',-1}}
keeps the states that have coherence order
((1 OR -1 on 13C) AND (-1 on 1H))
Outputs
rho - the state vector with the undesired orders of
spin correlations zeroed out
Examples
rho=coherence(spin_system,rho,{{'13C',[1 -1]},{'1H',-1}})
keeps all states that simultaneously have coherence order 1 or -1 in the 13C subspace, and coherence order -1 in the 1H subspace.
rho=coherence(spin_system,rho,{{3,0},{5,-1}})
keeps all states that simultaneously have coherence order 0 on spin number 3, and coherence order -1 on spin number 5.
Notes
Because projection quantum number information is required, this function only works with sphten-liouv formalism. It supports Fokker-Planck direct products.
See also
Links to related functions.
Version 2.2, authors: Ilya Kuprov, Luke Edwards