endor_davies.m
Davies ENDOR sequence with explicit soft pulses and all of the attendant effects, such as orientation selection. Soft pulses are simulated using the Fokker-Planck formalism.
Syntax
answer=endor_davies(spin_system,parameters,H,R,K)
Parameters
The following parameters refer to the electron pi pulse. The duration of the electron pi/2 pulse is obtained by halving parameters.e_dur:
parameters.e_frq - frequency of the electron pulse, Hz
parameters.e_phi - phase of the electron pulse, rad
parameters.e_pwr - power of the electron pulse, rad/s
parameters.e_dur - duration of the electron pulse, s
parameters.e_rnk - Fokker-Planck cut-off rank for
the electron pulse
The following parameters refer to the nuclei pulse:
parameters.n_frq - vector of frequencies for the nuclei
pulse, in Hz. The answer is returned
as a vector of the same dimension.
parameters.n_phi - phase of the nuclei pulse, rad
parameters.n_pwr - power of the nuclei pulse, rad/s
parameters.n_dur - duration of the nuclei pulse, s
parameters.n_rnk - Fokker-Planck cut-off rank for
the nuclei pulse
parameters.method - method to use during the call
to shaped_pulse_af()
H - Hamiltonian matrix, received from context function
R - relaxation superoperator, received from context function
K - kinetics superoperator, received from context function
Outputs
answer - amplitude detected on the coil state for each
frequency of the nuclear pulse
Notes
Fokker-Planck ranks should be increased until convergence is achieved in the output. The same applies to the size of the spherical grid.
See also
endor_cw.m, endor_mims.m, hyscore.m, fieldsweep.m, deer_3p_hard_deer.m, deer_3p_hard_echo.m, deer_3p_soft_deer.m, deer_3p_soft_diag.m, deer_3p_soft_hole.m, deer_4p_soft_deer.m, deer_4p_soft_diag.m, deer_4p_soft_hole.m, deer_analyt.m, endor_mims_echo.m, endor_mims_ideal.m, eseem.m, oopeseem.m, rapidscan.m, ridme.m, rydmr_exp.m, sifter.m, Built-in_experiments
Version 2.3, authors: Luke Edwards