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The asymmetric atomoptics deltakicked rotor

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The Atom-Optics d-kicked Rotor. The weakly' kicked rotor ... Prediction becomes impossible, and we have the fortuitous phenomenon.' Henri Poincar (1903) ... – PowerPoint PPT presentation

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Title: The asymmetric atomoptics deltakicked rotor


1
The asymmetric atom-optics delta-kicked rotor
  • Philip Jones
  • University College London

Messina, 22 September 2005
2
Overview
  • 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

3
Chaos
  • 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)

4
Kicked 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

5
The Standard Map
  • rn1 rn Ksin(fn)
  • fn1 fn rn1
  • Energy

6
Phase Space
  • Stable trajectories break up as K increases

7
Kicked Rotor
  • Correlations between kicks lead to corrections to
    D(K)

8
Cold Atoms
  • Compare to Hamiltonian of cold atoms in a pulsed
    optical lattice

9
Dimensionless Units
  • r 2p ? 2Tp/Ml
  • f 2p ? 2x/l
  • f,r i8wrT

K (V0/h) ? tp ? ?
10
Experimental Realisation
  • Retro-reflected laser beam
  • 1-D lin lin optical lattice
  • Sinusoidal potential

11
Experimental Realisation
  • Divide kicking beam into two
  • Control with separate AOMs
  • Lattice moves at lDf

12
Laser Cooling Lab
13
Step 1 Magneto Optical Trap
14
Step 2 Optical Molasses
15
Step 3 Kicking
16
Step 4 Imaging
17
Dynamical Localisation
  • Quantum interference phenomenon
  • Energy diffusion for finite time
  • Momentum freezes after break time, t
  • Momentum distribution becomes exponential

18
Dynamical Localisation
  • Dynamical Localisation shows characteristic
    exponential profile

e.g. Moore et al. Phys. Rev. Lett. 73 2974 (1994)
19
The weakly kicked rotor
  • Use regularly spaced kicks, but Kltlt4
  • Large islands in phase space
  • Use moving lattice to explore stable vs chaotic
    regions

20
Results Mixed Phase Space
  • Resolve stable islands and chaotic regions
  • Resolution depends on ?

21
Mixed Phase Space
M. Goonasekera et al, in preparation (2005)
22
Finite Temporal Width Kicks
  • Finite width causes momentum boundary
  • Atom travels l/2 in time tp
  • sinc2 envelope to diffusion constant
  • rb l ?

23
Results cut-off distribution
24
Results moving lattice
  • Large asymmetry develops due to proximity of the
    momentum boundary
  • Quantify by first moment of the momentum
    distribution

25
Results moving lattice
  • Plot asymmetry as a function of momentum in the
    lattice frame

P. H. Jones et al, Europhys. Lett. 67 (6) 928
(2004)
26
Unequally 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)
27
Effect of C2(r)
  • ltrgtnp/2b
  • Symmetric
  • diffusion

28
Effect of C2(r)
ltrgt?np/2b Asymmetric diffusion
29
Results momentum asymmetry
30
Asymmetry 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)
31
Break 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)
32
Accelerating 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

33
Results asymmetry
  • Asymmetry oscillates with period 2p
  • K 2.6, ? 1, b 1/16

P. H. Jones et al, arXivphysics/0504096 (2005)
34
Results distribution
  • Example of the momentum distribution for A 0,
    p/2, -p/2

35
The 2d-kicked rotor
  • Use closely-spaced pairs of kicks
  • long period, t, short period e
  • Again modifies kick-to-kick correlations

36
2d-kicked rotor results
  • Atom travels half a period between kicks of the
    pair
  • Effect of kicks cancels out
  • e 0.045

37
2d-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)

38
2d-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)
39
2d-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)
40
2d-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)
41
Compare 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

42
Conclusions
  • 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

43
Acknowledgements
  • 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
  • Funding
  • EPSRC (UK)

44
Laser 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
45
Further work
  • Effects of decoherence destroys dynamical
    localisation
  • Momentum filtering

46
Results Time Evolution
  • Current grows linearly with time and saturates

47
Results Time Evolution
  • Ratchet time, tRat ? 1/Db2

48
Results Pulse Shape
49
Results Mixed Phase Space
  • Mixed phase space with 2p periodicity
  • Start on islands no diffusion
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