Difference between revisions of "Phan2fpl.m"
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==See also== | ==See also== | ||
| − | [[fpl2phan.m]], [[fpl2rho.m]], [[v2fplanck.m]], [[hydrodynamics.m]], [[imaging.m]] | + | [[fpl2phan.m]], [[fpl2rho.m]], [[v2fplanck.m]], [[hydrodynamics.m]], [[imaging.m]], [[corrfun.m]], [[fdhess.m]], [[fdkup.m]], [[fdlap.m]], [[fdmat.m]], [[fdvec.m]], [[fdweights.m]], [[interpmat.m]], [[oscillator.m]], [[overwound.m]], [[qxspen_kernel.m]], [[spden.m]], [[Kernel_utilities]] |
''Version 2.3, authors: [[Ilya Kuprov]]'' | ''Version 2.3, authors: [[Ilya Kuprov]]'' | ||
Latest revision as of 19:39, 6 June 2026
Projects a spatial intensity distribution into the Fokker-Planck space, using it as the image painted by the the spin state supplied.
Syntax
rho=phan2fpl(phan,rho)
Parameters
phan - phantom (the spatial distribution of the
amplitude of the specified spin state)
rho - Liouville space state vector
Outputs
rho - Fokker-Planck state vector
See also
fpl2phan.m, fpl2rho.m, v2fplanck.m, hydrodynamics.m, imaging.m, corrfun.m, fdhess.m, fdkup.m, fdlap.m, fdmat.m, fdvec.m, fdweights.m, interpmat.m, oscillator.m, overwound.m, qxspen_kernel.m, spden.m, Kernel_utilities
Version 2.3, authors: Ilya Kuprov
