nickthequick
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Hi,
I am currently confused about something I've run across in the literature.
Given that
\nabla^2\phi = \phi_{xx}+\phi_{zz} = 0 for z\in (-\infty, 0]
and
\phi_z = \frac{\partial}{\partial x} |A|^2 at z=0.
for A= a(x)e^{i \theta(x)}.
The author claims that
\phi_x = A_xA^*-AA^*_x at z=0
and where A* represents the complex conjugate.
The author then claims a more general formula for \phi_x can be found in terms of the Hilbert Transform.
I do not understand how the author finds the expression for \left.\phi_x\right|_{z=0}. Also, although I'm vaguely aware that Hilbert Transforms can be used to find Harmonic conjugates, I don't see how that can be exploited in this case.
Any suggestions are appreciated!
Thanks,
Nick
I am currently confused about something I've run across in the literature.
Given that
\nabla^2\phi = \phi_{xx}+\phi_{zz} = 0 for z\in (-\infty, 0]
and
\phi_z = \frac{\partial}{\partial x} |A|^2 at z=0.
for A= a(x)e^{i \theta(x)}.
The author claims that
\phi_x = A_xA^*-AA^*_x at z=0
and where A* represents the complex conjugate.
The author then claims a more general formula for \phi_x can be found in terms of the Hilbert Transform.
I do not understand how the author finds the expression for \left.\phi_x\right|_{z=0}. Also, although I'm vaguely aware that Hilbert Transforms can be used to find Harmonic conjugates, I don't see how that can be exploited in this case.
Any suggestions are appreciated!
Thanks,
Nick