Difference between revisions of "M2s.m"
(Created page with "{{DISPLAYTITLE:m2s.m}} M2S sequence of Pileio and Levitt. ==Syntax== rho=m2s(spin_system,L,Hx,Hy,rho,J,delta_v) ==Description== Moves observable magnetisation into sin...") |
(Update function See also links and function index membership) |
||
| (6 intermediate revisions by the same user not shown) | |||
| Line 1: | Line 1: | ||
| − | {{DISPLAYTITLE:m2s.m}} | + | {{DISPLAYTITLE:m2s.m}} __NOTOC__ |
| − | M2S sequence of Pileio and Levitt. | + | M2S sequence of Pileio and Levitt that moves observable magnetisation into the singlet state. |
==Syntax== | ==Syntax== | ||
| Line 6: | Line 6: | ||
rho=m2s(spin_system,L,Hx,Hy,rho,J,delta_v) | rho=m2s(spin_system,L,Hx,Hy,rho,J,delta_v) | ||
| − | == | + | ==Parameters== |
| − | |||
| − | |||
| − | |||
L - background Liouvillian | L - background Liouvillian | ||
| Line 18: | Line 15: | ||
rho - initial state vector | rho - initial state vector | ||
| − | + | ||
J - J-coupling (Hz) | J - J-coupling (Hz) | ||
| Line 28: | Line 25: | ||
==See also== | ==See also== | ||
| − | [[singlet.m]], [[s2m.m]] | + | [[singlet.m]], [[s2m.m]], [[Built-in_experiments]] |
| − | |||
''Version 2.1, authors: [[Ilya Kuprov]], [[Ahmed Allami]]'' | ''Version 2.1, authors: [[Ilya Kuprov]], [[Ahmed Allami]]'' | ||
Latest revision as of 19:38, 6 June 2026
M2S sequence of Pileio and Levitt that moves observable magnetisation into the singlet state.
Syntax
rho=m2s(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, s2m.m, Built-in_experiments
Version 2.1, authors: Ilya Kuprov, Ahmed Allami
