Title: Squeezing generation and revivals in a cavityion system
1Squeezing generation and revivals in a
cavity-ion system
- Nicim Zagury
- Instituto de Física, Universidade Federal
- Rio de Janeiro, Brazil
colaboradores R. Rangel. L. Carvalho
2A ion inside a Paul trap in a cavity
3is being shined by two laser fields
The lasers and the cavity mode are quasi resonant
to a electronic transition of the ion.
4Level scheme
atomic transition frequency
cavity frequency
vibration frequency
laser frequencies
5A effective Hamiltonian
RWA adiabatic elimination of the upper state
( Lamb-Dicke parameter )
6Master Equation
Even though we have considered a bad cavity, we
were able to obtain an analytical solution for
the total density operator of the system
7The system reaches the steady state
A product of the vacuum of the cavity field and
an ideal squeezed state of the motion of the ion
Very large squeezing
8For finite times the two subsystems are, in
general, entangled, but periodically at times
and
they disentangle.
Remarkably, even though there is dissipation
there is a complete revival of the state of the
motion at t
and of the state of the field at t
9Periodically, the state of motion returns to
the same ideal squeezed state
The cavity field also returns periodically to the
initial vacuum state
10The solution for the reduced density operators at
any time are squeezed thermal states
11Behaviour of n with time
12Squeezing
revivals
13(No Transcript)
14Remarks and conclusions
, the two subsystems
disentangle periodically at given times ?n and ?n
2. Although there is dissipation the the state of
motion and the cavity field and revive
completely at ?n and ?n Respectively 3. At any
time the reduced density matrices correspond to
squeezed thermal states 4. These results can
be easily generalized for a initial coherent state
15References
- 1 H. Zeng and F. Lin, Phys. Rev. A 50, R3589
(1994). - 2 E. Massoni, M. Orszag, Opt. Comm. 190, 239
(2001) - 3 R. Rangel, E. Massoni, and N. Zagury, Phys.
Rev. A 69, 023805 (2004).