Difference between revisions of "Shaped pulse xy.m"
(Changed to current revision - control operators in a cell array, and control amplitudes in a call array of amplitude vectors.) |
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Shaped pulse function using Cartesian coordinates. Applies a user-specified pulse shape on user-specified operators while the rest of the drift Liouvillian continues to affect the spin system. Syntax: | Shaped pulse function using Cartesian coordinates. Applies a user-specified pulse shape on user-specified operators while the rest of the drift Liouvillian continues to affect the spin system. Syntax: | ||
| − | [rho,P]=shaped_pulse_xy(spin_system,drift,controls,amplitudes,time_grid) | + | [rho,P]=shaped_pulse_xy(spin_system,drift,controls,amplitudes,time_grid,rho) |
Parameters: | Parameters: | ||
Revision as of 11:53, 27 January 2017
Shaped pulse function using Cartesian coordinates. Applies a user-specified pulse shape on user-specified operators while the rest of the drift Liouvillian continues to affect the spin system. Syntax:
[rho,P]=shaped_pulse_xy(spin_system,drift,controls,amplitudes,time_grid,rho)
Parameters:
drift - the drift Liouvillian, the part of the Liouvillian that
should continue running in the background. This should
include the pulse frequency offset, if any.
controls - cell array of control operators corresponding to each
channel, this may include operators for spatial degrees
of freedom.
amplitudes - a cell array of control amplitude vectors {ncontrols}
(nsteps), in angular frequency units. Order of cell array
corresponds to the same order of the control operator
cell array.
time_grid - a vector containing the duration (not time position!)
of each pulse slice, seconds.
rho - state vector of the initial state, or a stack thereof.
The pulse is assumed to be piecewise-constant and should be supplied with sufficiently fine time discretization to properly reproduce the waveform.
Outputs:
rho - the final state vector or a stack thereof
P - total pulse propagator
Note: pulse propagators are expensive, do not request unless you really need that propagator.
Revision 3141, authors: Ilya Kuprov