Title: The Theory of Effective Hamiltonians for Detuned Systems
1The Theory of Effective Hamiltonians for Detuned
Systems
Universität Ulm, 18 November 2005
Daniel F. V. JAMES
Department of Physics, University of
Toronto, 60, St. George St., Toronto, Ontario
M5S 1A7, CANADA Email dfvj_at_physics.utoronto.ca
2Detuned Systems
Example Two level system, detuned field
Is there a systematic way to get Heff from HI
(preferably without all that tedious mucking
about with adiabatic elimination)?
3Time Averaged Dynamics Definitions
- Unitary time evolution operator
4General Expression I
5General Expression II
(5)
etc...
6- Hamiltonians have to be Hermitian!
- This can be justified by deriving a master
equation - excluded part of the frequency domain takes role
of reservoir - Lindblat equation with unitary part given by (7)
- Neglect dephasing effects.
7General Expression III
- Result is independent of lower limit in integral
for V1(t).
- Also applies statistical averages over a
stationary ensemble.
- This is NOT a perturabtive theory.
-YES, we have used perturbation theory with
reckless abandon, BUT
-Solving Schrödingers equation with this
Hamiltonian gives a result that involves all
orders of the perturbation parameter
8(No Transcript)
9Harmonic Hamiltonians Low Pass Filter
important special case
- Suppose we have a Hamiltonian made up of a sum of
harmonic terms
10Ref D. F. V. James, Fortschritte der Physik 48,
823-837 (2000) Related
results Average Hamiltonians (NMR) C.
Cohen-Tannoudji J Dupont-Roc and G. Grynberg,
Atom-Photon Interactions (Wiley, 1992), pp. 38-48.
11Example 1 AC Stark Shifts
12Example 2 Raman Processes
13Waless Grand Slam, 2005 5th February 2005 Wales
11 - 9 England 12th February 2005 Italy 8 -
38 Wales 26th February 2005 France 18 - 24
Wales 13th March 2005 Scotland 22 - 46
Wales 19th March 2005 Wales 32 - 20 Ireland
14Example 3 Quantum A.C. Stark Shift
C. dHelon and G. Milburn, Phys. Rev. A 54, 5141
(1996) S. Schneider et al., J. Mod Opt. 47, 499
(2000) F. Schmidt-Kaler et al, Europhys. Lett.
65, 587 (2004).
15(No Transcript)
16What about two ions?
big-ass laser
17(No Transcript)
18Hence the effective Hamilton is
Add another laser (with negative detuning)
Quantum A.C. Stark shifts cancel, but coupling
term is doubled Mølmer-Sørensen gåtë
19Conclusions
Quantum Simulations are a lot easier than
Porras and Cirac said.