[QM] Finding probability current from Hamiltonian and continuity equation

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SUMMARY

The discussion centers on deriving the probability current from the Hamiltonian \( H = \vec{\alpha} \cdot \vec{p} c + mc^2 \) and the continuity equation in quantum mechanics. The participants applied the Schrödinger equation \( H \psi = i \hbar \frac{\partial \psi}{\partial t} \) and the continuity equation \( \frac{\partial \rho}{\partial t} + \nabla \cdot \vec{j} = 0 \) to derive the expression for the current density \( \vec{j} \). They reached the equation \( \nabla \cdot \vec{j} = c \vec{\alpha} \cdot \nabla \rho - \frac{m c^2}{i \hbar} \rho \) but struggled to prove that the term \( \frac{m c^2}{i \hbar} \rho \) evaluates to zero, despite hints from their teacher. The problem was ultimately resolved, but the specific solution details were not shared.

PREREQUISITES
  • Understanding of quantum mechanics principles, specifically the Schrödinger equation.
  • Familiarity with Hamiltonian mechanics and the role of the Hamiltonian in quantum systems.
  • Knowledge of continuity equations in physics and their significance in quantum mechanics.
  • Basic proficiency in vector calculus, particularly divergence operations.
NEXT STEPS
  • Study the derivation of probability current in quantum mechanics using the continuity equation.
  • Explore the implications of the Hamiltonian \( H = \vec{\alpha} \cdot \vec{p} c + mc^2 \) in quantum field theory.
  • Learn about the role of the term \( \frac{m c^2}{i \hbar} \rho \) in quantum mechanics and its physical interpretation.
  • Investigate the methods for quantizing the electromagnetic field and its relationship to photon behavior.
USEFUL FOR

Students and professionals in quantum mechanics, particularly those studying Hamiltonian dynamics and continuity equations, as well as researchers interested in quantum field theory and photon quantization.

NanakiXIII
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Homework Statement



Given the Hamiltonian

[tex]H=\vec{\alpha} \cdot \vec{p} c + mc^2 = -i \hbar c \vec{\alpha} \cdot \nabla + mc^2[/tex]

in which [tex]\vec{\alpha}[/tex] is a constant vector. Derive from the Schrödinger equation and the continuity equation what the current is belonging to the density

[tex]\rho = \psi^{\ast} \psi[/tex].

Homework Equations



Schrödinger: [tex]H \psi = i \hbar \frac{\partial \psi}{\partial t}[/tex]

Continuity: [tex]\frac{\partial \rho}{\partial t} + \nabla \cdot \vec{j} = 0[/tex]


The Attempt at a Solution



Applying Schrödinger and the given Hamiltonian to the density gives

[tex]-i \hbar c \vec{\alpha} \cdot \nabla \rho + mc^2 \rho = i \hbar \frac{\partial \rho}{\partial t}[/tex].

The right hand side of the equation can be rewritten, by applying the continuity equation, and you end up with

[tex]\nabla \cdot \vec{j} = c \vec{\alpha} \cdot \nabla \rho - \frac{m c^2}{i \hbar} \rho[/tex].

After some tinkering I managed to turn this into

[tex]\nabla \cdot \vec{j} = \nabla \cdot c \vec{\alpha} \rho - \frac{m c^2}{i \hbar} \rho[/tex].

This is as far as I and my fellow students managed to get on this problem. Our teacher seemed to think that this was right, but that the second term,

[tex]\frac{m c^2}{i \hbar} \rho[/tex],

was supposed to be zero. We've had absolutely no luck, however, in proving any such thing and we don't see how that term should ever evaluate to zero. The hints our teacher gave us didn't get us any further, and I think we may have misinterpreted some of them because they led to very strange results. If anyone can give a hint or point in the right direction, or perhaps spot errors I made in the derivation so far (I hope it is clear enough without me providing the entire derivation), I would greatly appreciate it.
 
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The problem has been solved. If anyone is interested in what I did wrong, I'll post it. If not, I won't go through the trouble of LaTeXing it.
 
How to quantization photons
the electromagnetic field?:cry::confused:
 

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