Difference between revisions of "Sec2kite.m"
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==See also== | ==See also== | ||
| − | [[Kernel_utilities | + | [[adelim.m]], [[blinv.m]], [[blprod.m]], [[corrfun.m]], [[magpump.m]], [[ngce.m]], [[rlx_scalar.m]], [[rlx_split.m]], [[rlx_t1_t2.m]], [[spden.m]], [[Kernel_utilities]], [[Relaxation theory parameters]] |
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| − | [[Relaxation theory parameters]] | ||
''Version 2.11, authors: [[Ilya Kuprov]]'' | ''Version 2.11, authors: [[Ilya Kuprov]]'' | ||
Latest revision as of 19:41, 6 June 2026
Converts the secular relaxation superoperator into the Redfield kite form by dropping all non-longitudinal cross-relaxation processes. Useful when the relaxation superoperator is huge, but TROSY-like effects are negligible.
Syntax
R=sec2kite(spin_system,R)
Parameters
spin_system - Spinach spin system object R - relaxation superoperator
Outputs
R - relaxation superoperator
See also
adelim.m, blinv.m, blprod.m, corrfun.m, magpump.m, ngce.m, rlx_scalar.m, rlx_split.m, rlx_t1_t2.m, spden.m, Kernel_utilities, Relaxation theory parameters
Version 2.11, authors: Ilya Kuprov