Difference between revisions of "S2m.m"
(Created page with "{{DISPLAYTITLE:s2m.m}} S2M sequence of Pileio and Levitt. ==Syntax== rho=s2m(spin_system,L,Hx,Hy,rho,J,delta_v) ==Description== Moves singlet state into observable mag...") |
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L - background Liouvillian | L - background Liouvillian | ||
| − | + | ||
Hx - X spin operator | Hx - X spin operator | ||
| − | + | ||
Hy - Y spin operator | Hy - Y spin operator | ||
| − | + | ||
rho - initial state vector | rho - initial state vector | ||
| − | + | ||
J - J-coupling (Hz) | J - J-coupling (Hz) | ||
| − | + | ||
delta_v - Zeeman frequency difference (Hz) | delta_v - Zeeman frequency difference (Hz) | ||
Revision as of 20:21, 2 January 2018
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
