- #1
binbagsss
- 1,326
- 12
When one does the phase transformation ##\psi(\vec{x},t)=R(\vec{x},t)\exp^{iS(\vec{x},t)/\bar{h}}##
For this transformation to be valid doesn't it need to have the same asymptotic behaviour ##x \to \pm \infty##, and also at ##x=0 ## as the original wave-function ##\psi## does? How come this is the never mentioned?
Also on the Wikipedia page, it assumes ##R(\vec{x},t) \geq 0 ## and both ##R,S \in \Re ##, how is this possible without loss of generality? Also, obviously the w.f squared needs to be ##\geq 0## but, by assuming ##R(\vec{x},t) \geq 0 ## the amplitude of both the real and imaginary part of the w.f also now need to be positive. This surely restricts what the wave-function is able to describe, or is this true for a lot of problems?
(Although I have seen other derivations which transform the Lagrangian of the Schrodinger Lagrangian instead by ##\psi=\sqrt{rho}\exp{i\theta/\bar{h}}##, s.t. the relevant equations are given by the E-L equations,: variation w.r.t ##\theta## yields the cty, and variation wrt ##\rho## yields the quantum Hamilton-Jacobi. so taking the Real and Imaginary part is not required..)
Thanks.
For this transformation to be valid doesn't it need to have the same asymptotic behaviour ##x \to \pm \infty##, and also at ##x=0 ## as the original wave-function ##\psi## does? How come this is the never mentioned?
Also on the Wikipedia page, it assumes ##R(\vec{x},t) \geq 0 ## and both ##R,S \in \Re ##, how is this possible without loss of generality? Also, obviously the w.f squared needs to be ##\geq 0## but, by assuming ##R(\vec{x},t) \geq 0 ## the amplitude of both the real and imaginary part of the w.f also now need to be positive. This surely restricts what the wave-function is able to describe, or is this true for a lot of problems?
(Although I have seen other derivations which transform the Lagrangian of the Schrodinger Lagrangian instead by ##\psi=\sqrt{rho}\exp{i\theta/\bar{h}}##, s.t. the relevant equations are given by the E-L equations,: variation w.r.t ##\theta## yields the cty, and variation wrt ##\rho## yields the quantum Hamilton-Jacobi. so taking the Real and Imaginary part is not required..)
Thanks.