Difference between revisions of "Topdnp.m"
m (Rename Arguments section heading to Parameters) |
(Update function See also links and function index membership) |
||
| Line 32: | Line 32: | ||
==See also== | ==See also== | ||
| − | [[Built-in_experiments | + | [[beamdnp.m]], [[dnp_field_scan.m]], [[dnp_freq_scan.m]], [[dnp_time_dep.m]], [[masdnp.m]], [[noveldnp.m]], [[noveldnp_steady.m]], [[solid_effect.m]], [[xixdnp.m]], [[xixdnp_steady.m]], [[Built-in_experiments]] |
''Version 2.7, authors: [[Guinevere Mathies]], [[Venkata Subbarao Redrouthu]]'' | ''Version 2.7, authors: [[Guinevere Mathies]], [[Venkata Subbarao Redrouthu]]'' | ||
Latest revision as of 19:42, 6 June 2026
Time-optimised pulsed DNP experiment from (https://doi.org/10.1126/sciadv.aav6909).
Syntax
contact_curve=topdnp(spin_system,parameters,H,R,K)
Parameters
H - Hamiltonian matrix, received from context function
R - relaxation superoperator, received from context function
K - kinetics superoperator, received from context function
parameters.irr_powers - microwave amplitude (aka electron
nutation frequency), Hz
parameters.rho0 - initial state
parameters.coil - detection state
parameters.pulse_dur - pulse duration, seconds
parameters.delay_dur - delay_duration, seconds
parameters.nloops - number of TOP DNP loops
Outputs
contact_curve - time dependence of the coil state
See also
beamdnp.m, dnp_field_scan.m, dnp_freq_scan.m, dnp_time_dep.m, masdnp.m, noveldnp.m, noveldnp_steady.m, solid_effect.m, xixdnp.m, xixdnp_steady.m, Built-in_experiments
Version 2.7, authors: Guinevere Mathies, Venkata Subbarao Redrouthu
