Difference between revisions of "S2m.m"
(→Arguments) |
(Normalise sequential blank lines) |
||
| Line 29: | Line 29: | ||
==See also== | ==See also== | ||
[[singlet.m]], [[m2s.m]] | [[singlet.m]], [[m2s.m]] | ||
| − | |||
''Version 2.1, authors: [[Ilya Kuprov]], [[Ahmed Allami]]'' | ''Version 2.1, authors: [[Ilya Kuprov]], [[Ahmed Allami]]'' | ||
Revision as of 12:29, 25 April 2026
S2M sequence of Pileio and Levitt.
Contents
Syntax
rho=s2m(spin_system,L,Hx,Hy,rho,J,delta_v)
Description
Moves singlet state into observable magnetisation.
Arguments
L - background Liouvillian
Hx - X spin operator
Hy - Y spin operator
rho - initial state vector
J - J-coupling (Hz)
delta_v - Zeeman frequency difference (Hz)
Outputs
rho - final state vector
See also
Version 2.1, authors: Ilya Kuprov, Ahmed Allami
