External Fields and Negative Energy Transitions In Dirac Particle

javiergra24
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Homework Statement



Suppose a relativistic particle with spin 1/2 at rest. Show that if we apply an electrical field at t=0 there's a probability fot t>0 of finding the particle in a negative energy state if such negative energy states are assumed to be originally empty.

Homework Equations



Dirac equation at rest:
<br /> (\boldsymbol{\hat{\beta}} mc^2) \psi (\mathbf{x},t) = i \hbar \frac{\partial\psi(\mathbf{x},t) }{\partial t}<br />
Spinor solutions with positive energy for t<0
<br /> $\Psi_{+}=\begin{pmatrix}<br /> \psi^{(1)}\\ \psi^{(2)}<br /> \end{pmatrix}={1\over\sqrt{V}}\begin{pmatrix}<br /> 1\\ 1\\ 0\\ 0<br /> \end{pmatrix}e^{-imc^2t/\hbar}$\\<br /> <br />
Applied electrical field and consecuent magnetic potential
<br /> $\mathbf{E}=E_0 \cos(\omega t)\mathbf{u}_{x} \qquad \mathbf{A}=-\frac{E_0}{\omega} \sin(\omega t)\mathbf{u}_{x}$<br />

The Attempt at a Solution



I'm not sure how to solve this problem. Is it supposed that the particle at t>0 remains at rest? Or it has a negative energy E'?. First order perturbation theory must be used, but how about the final state of the particle?

Perturbed Hamiltonian should be
<br /> $\displaystyle H&#039;(t)=q c \boldsymbol{\hat{\alpha}} \mathbf{A}=q c\hat{\alpha}_{x}A_{x}$<br />
Is it correct?

Thank you
 
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The perturbed Hamiltonian acts on the spinor wavefunction. You'll need to use the Dirac matrices to write things in terms of the positive and negative energy components.
 
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But the final state would be an antiparticle at rest? Or with some energy?
 
javiergra24 said:
But the final state would be an antiparticle at rest? Or with some energy?

Oh I missed that the spinor is relativistic. A relativistic particle is not at rest, so neither the initial or final state are at rest.
 
Umm a relativistic particle can be at rest, with E=mc^2. The exact problem is:

"Consider a positive energy spin-1/2 particle at rest. Suppose that at t=0 we apply an external
(classical) vector potential (see mi first post)
which corresponds to an electric field of the form
Show that for there exists a finite probability of finding the particle in a negative energy state if
such negative energy states are assumed to be originally empty. In particular, work out quantitatively
the two cases: w>>mc^2 and w=mc^2 and and comment."
 
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