Difference between revisions of "Zftrip.m"
m (Rename Arguments section heading to Parameters) |
(Update function See also links and function index membership) |
||
| Line 28: | Line 28: | ||
==See also== | ==See also== | ||
| − | [[Kernel_functions | + | [[deut_pair.m]], [[equilibrium.m]], [[four_spin_states.m]], [[partner_state.m]], [[singlet.m]], [[state.m]], [[triplet.m]], [[Kernel_functions]] |
''Version 2.11, authors: [[Guinevere Mathies]], [[Ilya Kuprov]]'' | ''Version 2.11, authors: [[Guinevere Mathies]], [[Ilya Kuprov]]'' | ||
Latest revision as of 19:43, 6 June 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)
Parameters
spin_system - Spinach spin system object
ZFS - 3x3 ZFS tensor (Hz) in the laboratory frame of reference;
use zfs2mat() to get it from D, E, and molecular Euler angles
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; use functions like axrh2mat() to get it
from eigenvalues and molecular Euler angles
B - magnetic field along the laboratory Z axis, Tesla
idx - index of the electron triplet, using 'E3', in the sys.isotopes list
Outputs
rho - spin density matrix (Hilbert space) or state vector (Liouville space)
See also
deut_pair.m, equilibrium.m, four_spin_states.m, partner_state.m, singlet.m, state.m, triplet.m, Kernel_functions
Version 2.11, authors: Guinevere Mathies, Ilya Kuprov