Exponential of momenta to entangle harmonic oscillators

Join the discussion
Registration is free. Start your own thread to ask a follow-up.
2 replies · 2K views
matteo137
Messages
42
Reaction score
9
TL;DR
What is the state evolution under a P*P entangling Hamiltonian
Consider two harmonic oscillators, described by annihilation operators [itex]a[/itex] and [itex]b[/itex], both initially in the vacuum state. Let us imagine that there is a coupling mechanism governed by the Hamiltonian [itex]H=P_A P_B[/itex], where [itex]P_i[/itex] is the momentum operator for the oscillator [itex]i[/itex]. For example [itex]P_A = (a-a^\dagger)/(i\sqrt{2})[/itex].

I would like to derive the time evolution
[tex] \vert \psi \rangle = e^{-i t P_A P_B} \vert 0,0 \rangle[/tex]
but it is not very clear to me how to proceed. I can decompose the exponential as [itex]e^{i \mu P_A P_B} = e^{i t P_A (b-b^\dagger)}[/itex], and using [itex][P_A b, - P_A b^\dagger]=-P_A^2[/itex] in the Baker-Campbell-Hausdorff (BCH) formula I obtain [itex]e^{i t P_A (b-b^\dagger)}=e^{i t P_A b} e^{-i t P_A b^\dagger} e^{- \frac{t^2}{2} P_A^2}[/itex]. If needed the BCH can be applied once more to [itex]P_A[/itex]. However, I'm not sure if this is useful, or how to continue from there.
 
Physics news on Phys.org
The hamiltonian you provide is only the interaction. To this one must add the free non-interacting HO hamiltonian ##\omega_a a^\dagger a + \omega_b b^\dagger b##. Once this is added use the BHC relation to

##e^{itH}|0,0\rangle##

where

##H = \omega_a a^\dagger a + \omega_b b^\dagger b + P_AP_B##

good luck!
 
You could probably diagnaolize that Hamiltonian with a linear combination of ##a##s and ##b##s.
 
  • Like
Likes   Reactions: vanhees71