Difference between revisions of "Zftrip.m"
(Created page with "{{DISPLAYTITLE:zftrip.m}} __NOTOC__ Projection of the zero-field triplet state with user-specified populations of Cartesian ZFS eigenstates onto the higher-field ZFS + Zeeman...") |
(Normalise sequential blank lines) |
||
| Line 26: | Line 26: | ||
==See also== | ==See also== | ||
[[Kernel_functions#Elementary_states|Elementary states]] | [[Kernel_functions#Elementary_states|Elementary states]] | ||
| − | |||
''Version 2.11, authors: [[Guinevere Mathies]], [[Ilya Kuprov]]'' | ''Version 2.11, authors: [[Guinevere Mathies]], [[Ilya Kuprov]]'' | ||
Revision as of 12:32, 25 April 2026
Projection of the zero-field triplet state with user-specified populations of Cartesian ZFS eigenstates onto the higher-field ZFS + Zeeman eigenstates. This is commonly seen in triplet DNP with photo-generated two-electron triplets.
Syntax
rho=zftrip(spin_system,ZFS,pops,Z,B,idx)
Arguments
spin_system - Spinach spin system object ZFS - 3x3 ZFS tensor (Hz) in the laboratory frame of reference pops - populations of X, Y, and Z eigenstates of the ZFS tensor at zero field [pX pY pZ] Z - 3x3 Zeeman interaction tensor (Hz/Tesla) in the laboratory frame of reference B - magnetic field along the laboratory Z axis, Tesla idx - index of the electron triplet in the sys.isotopes list
Outputs
rho - spin density matrix (Hilbert space) or state vector (Liouville space)
See also
Version 2.11, authors: Guinevere Mathies, Ilya Kuprov