Difference between revisions of "Dnp field scan.m"
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''Version 2.5, authors: [[Ilya Kuprov]], [[Walter Kockenberger]], [[Alexander Karabanov]]'' | ''Version 2.5, authors: [[Ilya Kuprov]], [[Walter Kockenberger]], [[Alexander Karabanov]]'' | ||
Revision as of 14:53, 20 September 2020
Magnetic field scan steady-state DNP experiment. Returns the steady-state population of the user-specified state as a function of magnetic field.
Syntax
dnp=dnp_field_scan(spin_system,parameters,H,R,K)
Arguments
parameters.mw_pwr - microwave power, Hz
parameters.mw_frq - microwave frequency, Hz
parameters.fields - a vector of B0 field values, T
parameters.rho_eq - thermal equilibrium state
parameters.coil - detection state vector or a horizon-
tal stack thereof
parameters.mw_oper - microwave irradiation operator
parameters.ez_oper - Lz operator on the electrons
parameters.method - 'backslash' to use Matlab's
linear equation solver, 'gmres'
to use ILU preconditioned GMRES
H - Hamiltonian matrix, received from context function
R - relaxation superoperator, received from context function
K - kinetics superoperator, received from context function
Returns
dnp - an array of the steady state amplitudes of the
states specified in parameters.coil as at each
of the magnetic fields supplied
Examples
Cross effect in a system with two spin-1/2 electrons (cross_effect_field_scan_1.m example file in examples/dnp_solids directory):
Solid effect in a system with a spin-7/2 gadolinium ion (solid_effect_field_scan_1.m example file in examples/dnp_solids directory):
Notes
- The relaxation superoperator supplied to this function should NOT be thermalized.
- Thermal equilibrium state is assumed to be the same at all fields in the sweep. Do not use this function for broad magnetic field sweep experiments.
- Backslash method is recommended for small spin systems and GMRES method for large ones.
See also
Version 2.5, authors: Ilya Kuprov, Walter Kockenberger, Alexander Karabanov

