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...") |
(Update function See also links and function index membership) |
||
| (7 intermediate revisions by the same user not shown) | |||
| Line 1: | Line 1: | ||
| − | {{DISPLAYTITLE:s2m.m}} | + | {{DISPLAYTITLE:s2m.m}} __NOTOC__ |
| − | S2M sequence of Pileio and Levitt. | + | S2M sequence of Pileio and Levitt that moves singlet state into observable magnetisation. |
==Syntax== | ==Syntax== | ||
| Line 6: | Line 6: | ||
rho=s2m(spin_system,L,Hx,Hy,rho,J,delta_v) | rho=s2m(spin_system,L,Hx,Hy,rho,J,delta_v) | ||
| − | == | + | ==Parameters== |
| − | |||
| − | |||
| − | |||
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) | ||
| Line 28: | Line 25: | ||
==See also== | ==See also== | ||
| − | [[singlet.m]], [[m2s.m]] | + | [[singlet.m]], [[m2s.m]], [[Built-in_experiments]] |
| − | |||
''Version 2.1, authors: [[Ilya Kuprov]], [[Ahmed Allami]]'' | ''Version 2.1, authors: [[Ilya Kuprov]], [[Ahmed Allami]]'' | ||
Latest revision as of 19:41, 6 June 2026
S2M sequence of Pileio and Levitt that moves singlet state into observable magnetisation.
Syntax
rho=s2m(spin_system,L,Hx,Hy,rho,J,delta_v)
Parameters
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
singlet.m, m2s.m, Built-in_experiments
Version 2.1, authors: Ilya Kuprov, Ahmed Allami
