Difference between revisions of "Dnp time dep.m"
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| − | [[Built-in_experiments | + | [[beamdnp.m]], [[dnp_field_scan.m]], [[dnp_freq_scan.m]], [[masdnp.m]], [[noveldnp.m]], [[noveldnp_steady.m]], [[solid_effect.m]], [[topdnp.m]], [[xixdnp.m]], [[xixdnp_steady.m]], [[Built-in_experiments]] |
''Version 2.5, authors: [[Ilya Kuprov]], [[Maria Grazia Concilio]]'' | ''Version 2.5, authors: [[Ilya Kuprov]], [[Maria Grazia Concilio]]'' | ||
Latest revision as of 19:36, 6 June 2026
Time-domain spin dynamics under microwave irradiation.
Syntax
answer=dnp_time_dep(spin_system,parameters,H,R,K)
Parameters
parameters.mw_pwr - microwave power, rad/s
parameters.mw_off - microwave frequency offset
from free electron,rad/s
parameters.rho0 - thermal equilibrium state
parameters.coil - coil state vector or a hori-
zontal stack thereof
parameters.mw_oper - microwave irradiation operator
parameters.ez_oper - Lz operator on the electrons
parameters.dt - time step, seconds
parameters.nsteps - number of time steps
H - Hamiltonian commutation superoperator
R - thermalised relaxation superoperator
K - chemical kinetics superoperator
Outputs
answer - a matrix of projections of the trajectory on
each of the coils provided at each time step
Examples
Below is the output of examples/dnp_liquids/dnp_liquid_2.m example file.
Notes
The relaxation superoperator must be thermalised for this type of calculation.
See also
beamdnp.m, dnp_field_scan.m, dnp_freq_scan.m, masdnp.m, noveldnp.m, noveldnp_steady.m, solid_effect.m, topdnp.m, xixdnp.m, xixdnp_steady.m, Built-in_experiments
Version 2.5, authors: Ilya Kuprov, Maria Grazia Concilio
