Difference between revisions of "Phan2fpl.m"

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.

    rho=phan2fpl(phan,rho)

    phan  - phantom (the spatial distribution of the
            amplitude of the specified spin state)

    rho   - Liouville space state vector

    rho   - Fokker-Planck state vector

@@ Line 1: / Line 1: @@
-Projects a spatial intensity distribution into the Fokker-Planck
+{{DISPLAYTITLE:phan2fpl.m}} __NOTOC__
-space, using the spin state supplied. Syntax:
+Projects a spatial intensity distribution into the Fokker-Planck space, using it as the image painted by the the spin state supplied.
-                      rho=phan2fpl(phan,rho)
+==Syntax==
-Parameters:
+     rho=phan2fpl(phan,rho)
-        phan  - phantom (the spatial distribution of the
+==Parameters==
-                amplitude of the specified spin state)
-        rho   - the spin state in question
+     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]]''