Title: The asymmetric atomoptics deltakicked rotor
1The asymmetric atom-optics delta-kicked rotor
- Philip Jones
- University College London
Messina, 22 September 2005
2Overview
- Intro Quantum Chaos
- The Atom-Optics d-kicked Rotor
- The weakly kicked rotor
- Finite temporal width kicks
- Unequal period kicked rotor
- The 2d-kicked rotor
- Conclusion
3Chaos
- it may happen that small differences in the
initial conditions produce very great ones in the
final phenomena. A small error in the former will
produce an enormous error in the latter.
Prediction becomes impossible, and we have the
fortuitous phenomenon. - Henri Poincaré (1903)
4Kicked Rotor
- Standard system for investigation of chaotic
dynamics - Hamiltonian H r2 Kcos(f)Sd(t n)
- Dynamics described by K, the stochasticity
parameter - Diffusive energy growth D K2 / 4
5The Standard Map
- rn1 rn Ksin(fn)
- fn1 fn rn1
- Energy
6Phase Space
- Stable trajectories break up as K increases
7Kicked Rotor
- Correlations between kicks lead to corrections to
D(K)
8Cold Atoms
- Compare to Hamiltonian of cold atoms in a pulsed
optical lattice
9Dimensionless Units
- r 2p ? 2Tp/Ml
- f 2p ? 2x/l
- f,r i8wrT
K (V0/h) ? tp ? ?
10Experimental Realisation
- Retro-reflected laser beam
- 1-D lin lin optical lattice
- Sinusoidal potential
11Experimental Realisation
- Divide kicking beam into two
- Control with separate AOMs
- Lattice moves at lDf
12Laser Cooling Lab
13Step 1 Magneto Optical Trap
14Step 2 Optical Molasses
15Step 3 Kicking
16Step 4 Imaging
17Dynamical Localisation
- Quantum interference phenomenon
- Energy diffusion for finite time
- Momentum freezes after break time, t
- Momentum distribution becomes exponential
18Dynamical Localisation
- Dynamical Localisation shows characteristic
exponential profile
e.g. Moore et al. Phys. Rev. Lett. 73 2974 (1994)
19The weakly kicked rotor
- Use regularly spaced kicks, but Kltlt4
- Large islands in phase space
- Use moving lattice to explore stable vs chaotic
regions
20Results Mixed Phase Space
- Resolve stable islands and chaotic regions
- Resolution depends on ?
21Mixed Phase Space
M. Goonasekera et al, in preparation (2005)
22Finite Temporal Width Kicks
- Finite width causes momentum boundary
- Atom travels l/2 in time tp
- sinc2 envelope to diffusion constant
- rb l ?
23Results cut-off distribution
24Results moving lattice
- Large asymmetry develops due to proximity of the
momentum boundary - Quantify by first moment of the momentum
distribution
25Results moving lattice
- Plot asymmetry as a function of momentum in the
lattice frame
P. H. Jones et al, Europhys. Lett. 67 (6) 928
(2004)
26Unequally spaced kicks
- Break time symmetry of kicks
- Use two period cycle
- T(1b) T(1-b)
- Two-kick correlations now give rise to
momentum-dependent diffusion constant
T. Jonckheere et al. Phys. Rev. Lett. 91 253003
(2004)
27Effect of C2(r)
- ltrgtnp/2b
- Symmetric
- diffusion
28Effect of C2(r)
ltrgt?np/2b Asymmetric diffusion
29Results momentum asymmetry
30Asymmetry Oscillates
- Current oscillates with expected period p / b
- Top panel, b 1/16
- Lower, b 1/8
- K 3.3, ? 1
P. H. Jones et al, arXivphysics/0504096 (2005)
31Break Spatial Symmetry
- Include a potential gradient of alternating sign
- Adds a phase shift to C2(r)
- Achieve by accelerating the lattice
T. Jonckheere et al. Phys. Rev. Lett. 91 253003
(2004)
32Accelerating Lattice
- Adds an inertial term to the Hamiltonian (in the
accelerating frame) - Change the frequency difference by df in the time
T - Scaled gradient, A 2ptpdf
- Can easily control magnitude of A
33Results asymmetry
- Asymmetry oscillates with period 2p
- K 2.6, ? 1, b 1/16
P. H. Jones et al, arXivphysics/0504096 (2005)
34Results distribution
- Example of the momentum distribution for A 0,
p/2, -p/2
35The 2d-kicked rotor
- Use closely-spaced pairs of kicks
- long period, t, short period e
- Again modifies kick-to-kick correlations
362d-kicked rotor results
- Atom travels half a period between kicks of the
pair - Effect of kicks cancels out
- e 0.045
372d-kicked rotor phase space
- Phase space shows momentum trapping regions
- At r (2m1)(p/e) atoms absorb little energy
- Maxima at r 2m(p/e)
382d-kicked rotor results
- Narrow dips appear for slightly larger e
- e 0.16
- Consequence of long-range global correlations
P. H. Jones et al. Phys. Rev. Lett. 93 223002
(2004)
392d-KR correlations
- C1 ltK2sin(fm)sin(fm1)gt ? cos(re)
- couples nearest-neighbour kicks, acts over short
timescales - CG1 ltK2sin(fm)sin(fj)gt ? - cos(re)
- couples kick j with all preceding kicks,
accumulates to dominate at long times
M. Stocklin et al, arXivphysics/0408088 (2004)
402d-KR correlations
- At intermediate times C1 and CG1 cancel
- Correlation CPn ? cos(nre), n 2,3,4 becomes
evident - From correlations between kick j and j n
- Sum to give sharp dips in energy growth
- Poisson sum rule
- S(-1)n cos(nre) S d(re (2m1)p)
M. Stocklin et al, arXivphysics/0408088 (2004)
41Compare theory experiment
- Compare experimental data with theory of Stocklin
et al - As e increases observe change from dominant C1 to
CG1, with narrow dips evidence of CPn
42Conclusions
- Have investigated variations on simple
delta-kicked rotor - Verified effect of finite temporal width kicks
- Demonstrated asymmetric diffusion due to chaotic
dynamics only (chaotic ratchet) - Observed new global correlations in 2d-kicked
rotor (momentum filter) - Prepare atoms in stable islands of chaotic sea
43Acknowledgements
- Experiment
- David Meacher (EPO, Munich)
- Malika Goonasekera
- Harry Saunders-Singer (Channel 4)
- Ferruccio Renzoni
- Theory
- Tania Monteiro
- Thibaut Jonckheere (Marseille)
- Charles Creffield
- Nic Hutchings (ABN Amro)
- Matt Isherwood (FRM)
- Gwangok Hur
- Mischa Stocklin
44Laser Cooling Group (experiments)
David Meacher
Phil Jones
Harry Singer
Malika Goonasekera
Quantum Chaos Group (theory)
Matt Isherwood
Tania Monteiro
Nic Hutchings
Thibaut Jonckheere
Gwangok Hur
45Further work
- Effects of decoherence destroys dynamical
localisation - Momentum filtering
46Results Time Evolution
- Current grows linearly with time and saturates
47Results Time Evolution
- Ratchet time, tRat ? 1/Db2
48Results Pulse Shape
49Results Mixed Phase Space
- Mixed phase space with 2p periodicity
- Start on islands no diffusion