Non-Linear Schroedinguer equation

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SUMMARY

The discussion centers on solving the Non-Linear Schrödinger Equation (NLSE), represented as iħ ∂ψ/∂t = -ħ²(2m)⁻¹ ∇²ψ + |ψ|³. Key insights include the use of iterative procedures starting from linear solutions to approximate solutions for specific boundary conditions. The existence of soliton solutions, which behave like particles, is highlighted as a significant feature of non-linear equations. Additionally, the interpretation of the wave function ψ in the context of probability density is clarified, referencing A.O. Barut's work on combining relativity and quantum mechanics.

PREREQUISITES
  • Understanding of the Non-Linear Schrödinger Equation (NLSE)
  • Familiarity with quantum mechanics concepts, particularly wave functions
  • Knowledge of iterative methods for solving differential equations
  • Basic principles of soliton theory in non-linear dynamics
NEXT STEPS
  • Research iterative methods for solving differential equations, focusing on the NLSE
  • Explore soliton solutions in non-linear wave equations
  • Study the probability interpretation of wave functions in quantum mechanics
  • Investigate A.O. Barut's theories on the intersection of relativity and quantum mechanics
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Physicists, mathematicians, and researchers in quantum mechanics, particularly those interested in non-linear dynamics and the interpretation of wave functions.

eljose
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Let be the NOn-linear Schroedinguer equation:

[tex]i\hbar \frac{\partial \psi}{\partial t}=-\hbar^{2}(2m)^{-1} \nabla ^{2} \psi + |\psi|^{3}[/tex]

for example..the question is..how the hell do you solve it for certain boundary conditions that the Wavefunction must satisfy if you can,t apply superposition principle?...How do you express the probability of finding a particle in state a with energy E_a?..
 
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eljose said:
Let be the NOn-linear Schroedinguer equation:

[tex]i\hbar \frac{\partial \psi}{\partial t}=-\hbar^{2}(2m)^{-1} \nabla ^{2} \psi + |\psi|^{3}[/tex]

for example..the question is..how the hell do you solve it for certain boundary conditions that the Wavefunction must satisfy if you can,t apply superposition principle?...How do you express the probability of finding a particle in state a with energy E_a?..
A few comments :
(a) you usually find good approximations through an iteration procedure starting from a solution of the linear equation.
(b) the interesting part about non-linear equations is that soliton, ie. particle-like, solutions might exist.
(c) One should not interpret the [tex]\psi[/tex] wave associated to the NLSE as a probability density - there is however a ``clever'' way to get to the standard probability interpretation; see ``combining relativity and quantum mechanics : Schroedingers interpretation'' A.O. Barut 1987.
(d) energy eigenstates are never observed and neither does a full dynamical treatment of the radiation degrees of freedom allow for such thing *theoretically*.

Careful
 

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