Difference between revisions of "Deer 4p soft deer.m"
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parameters.coil - detection state | parameters.coil - detection state | ||
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| + | parameters.spins - irradiated spins, normally {'E'} | ||
parameters.method - soft puse propagation method, | parameters.method - soft puse propagation method, | ||
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# For the method, start with 'expm', change to 'expv' if the calculation runs out of memory, and use 'evolution' as the last resort. | # For the method, start with 'expm', change to 'expv' if the calculation runs out of memory, and use 'evolution' as the last resort. | ||
# Simulated echoes tend to be sharp and hard to catch because simulation does not have distributions in experimental parameters. Fourier transforming the echo prior to integration is recommended. | # Simulated echoes tend to be sharp and hard to catch because simulation does not have distributions in experimental parameters. Fourier transforming the echo prior to integration is recommended. | ||
| − | # The time in the DEER trace refers to the | + | # The time in the DEER trace refers to the third pulse insertion point, after end of the second pulse. |
==See also== | ==See also== | ||
Latest revision as of 06:43, 30 August 2026
Four-pulse DEER/PELDOR pulse sequence. The sequence uses soft pulses computed with the Fokker-Planck formalism.
Syntax
echo_stack=deer_4p_soft_deer(spin_system,parameters,H,R,K)
Parameters
parameters.pulse_frq - frequencies for the four
pulses, Hz
parameters.pulse_pwr - power levels for the four
pulses, rad/s
parameters.pulse_dur - durations for the four
pulses, seconds
parameters.pulse_phi - initial phases for the four
pulses, radians
parameters.pulse_rnk - Fokker-Planck ranks for the
four pulses
parameters.p1_p2_gap - time between the end of the
first and the start of the
second pulse, seconds
parameters.p2_p4_gap - time between the end of the
second the start of the third
pulse, seconds
parameters.p3_nsteps - number of third pulse posi-
tions in the interval between
the first echo and the fourth
pulse
parameters.echo_time - time to sample around the ex-
pected second echo position
parameters.echo_npts - number of points in the second
echo discretization
parameters.rho0 - initial state
parameters.coil - detection state
parameters.spins - irradiated spins, normally {'E'}
parameters.method - soft puse propagation method,
'expv' for Krylov propagation,
'expm' for exponential propa-
gation, 'evolution' for Spin-
ach evolution function
H - Hamiltonian matrix, received from context function
R - relaxation superoperator, received from context function
K - kinetics superoperator, received from context function
Outputs
echo_stack - DEER echo stack, a matrix with p3_nsteps echoes
with echo_npts points each
Examples
A number of complete examples for two- and three-electron systems are given in examples/esr_solids folder. A good way to proceed (soft_4_pulse_deer_2e.m example file) is to look at how the pulses affect the system:
then to inspect the echo stack as a function of the pump pulse position:
and finally to inspect the principal components of the echo stack. The most prominent component is the DEER trace, the other components come from the finite size of the spherical integration grid.
Notes
- For the method, start with 'expm', change to 'expv' if the calculation runs out of memory, and use 'evolution' as the last resort.
- Simulated echoes tend to be sharp and hard to catch because simulation does not have distributions in experimental parameters. Fourier transforming the echo prior to integration is recommended.
- The time in the DEER trace refers to the third pulse insertion point, after end of the second pulse.
See also
deer_3p_hard_echo.m, deer_3p_hard_deer.m, deer_analyt.m, eseem.m, oopeseem.m, deer_4p_soft_hole.m, deer_4p_soft_diag.m, deer_3p_soft_deer.m, deer_3p_soft_hole.m, deer_3p_soft_diag.m, endor_cw.m, endor_davies.m, endor_mims.m, endor_mims_echo.m, endor_mims_ideal.m, fieldsweep.m, hyscore.m, rapidscan.m, ridme.m, rydmr_exp.m, sifter.m, Built-in_experiments
Version 2.4, authors: Ilya Kuprov



