Difference between revisions of "Masdnp.m"
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dnp=masdnp(spin_system,parameters) | dnp=masdnp(spin_system,parameters) | ||
| − | == | + | ==Parameters== |
parameters.spins - the spins to microwave | parameters.spins - the spins to microwave | ||
parameters.rate - spinning rate, Hz | parameters.rate - spinning rate, Hz | ||
| − | + | ||
parameters.axis - spinning axis direction vector. | parameters.axis - spinning axis direction vector. | ||
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==See also== | ==See also== | ||
| − | [[dnp_field_scan.m]], [[dnp_freq_scan.m]], [[solid_effect.m]] | + | [[beamdnp.m]], [[dnp_field_scan.m]], [[dnp_freq_scan.m]], [[dnp_time_dep.m]], [[noveldnp.m]], [[noveldnp_steady.m]], [[solid_effect.m]], [[topdnp.m]], [[xixdnp.m]], [[xixdnp_steady.m]], [[Built-in_experiments]] |
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''Version 2.5, authors: [[Frederic Mentink-Vigier]], [[Ilya Kuprov]]'' | ''Version 2.5, authors: [[Frederic Mentink-Vigier]], [[Ilya Kuprov]]'' | ||
Latest revision as of 19:38, 6 June 2026
Magic angle spinning DNP simulation, returning the rotor period averaged steady state magnetization. This function takes a lot of inspiration from the code donated by Fred Mentink, please cite Fred's papers if you are using it.
Syntax
dnp=masdnp(spin_system,parameters)
Parameters
parameters.spins - the spins to microwave
parameters.rate - spinning rate, Hz
parameters.axis - spinning axis direction vector.
parameters.max_rank - rotor discretization grid rank
parameters.mw_pwr - microwave power, rad/s
parameters.mw_frq - microwave frequency, Hz
parameters.mw_time - microwave irradiation duration
before the average magnetistion
is computed, seconds
parameters.grid - the name of the spherical avera-
ging grid
parameters.coil - detection state
parameters.verbose - set this to 1 to enable diag-
nostic output
Outputs
dnp - enhancement of the user-specified state relative to
the thermal equilibrium
Examples
A detailed walkthough for solid effect and cross effect MAS DNP is given in the example set. For a simple three-spin system discussed in Fred's paper, cross_effect_mas_enlev.m returns the rotor phase dependence of the energy levels in the system:
The energy level population dynamics during the first rotor cycle is returned by cross_effect_mas_dynam.m example:
The energy level population dynamics during the steady state rotor cycle is returned by cross_effect_mas_steady.m example:
and finally the steady state rotor-averaged, powder-averaged DNP amplitude is returned by a call to this function in cross_effect_mas_powder.m example file.
Notes
- Increase the rotor rank and the spherical grid size until the answer stops changing. You will likely need huge values for both parameters.
- This function must be called directly, without a context wrapper.
See also
beamdnp.m, dnp_field_scan.m, dnp_freq_scan.m, dnp_time_dep.m, noveldnp.m, noveldnp_steady.m, solid_effect.m, topdnp.m, xixdnp.m, xixdnp_steady.m, Built-in_experiments
Version 2.5, authors: Frederic Mentink-Vigier, Ilya Kuprov


