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T. Kitagawa (Harvard), S. Pielawa (Harvard), D. Pekker (Harvard), R. Sensarma (Harvard/JQI), V. Gritsev (Fribourg), M.

Probing many-body systems of ultracold atoms. Harvard-MIT. $$ NSF, MURI, DARPA, AFOSR. Eugene Demler Harvard University. T. Kitagawa (Harvard), S. Pielawa (Harvard), D. Pekker (Harvard), R. Sensarma (Harvard/JQI), V. Gritsev (Fribourg), M. Lukin (Harvard), Lode Pollet (Harvard).

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T. Kitagawa (Harvard), S. Pielawa (Harvard), D. Pekker (Harvard), R. Sensarma (Harvard/JQI), V. Gritsev (Fribourg), M.

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  1. Probing many-body systems of ultracold atoms Harvard-MIT $$ NSF, MURI, DARPA, AFOSR Eugene Demler Harvard University T. Kitagawa (Harvard), S. Pielawa (Harvard), D. Pekker (Harvard), R. Sensarma (Harvard/JQI), V. Gritsev (Fribourg), M. Lukin (Harvard), Lode Pollet (Harvard) Collaboration with experimental groups of T. Esslinger, I. Bloch, J. Schmiedmayer

  2. Outline • Lattice modulation • experiments with • fermions • Ramsey interference • experiments in 1d Also yesterday’s talks by Henning Moritz and Andreas Ruegg

  3. Lattice modulation experiments with fermions in optical lattice. Probing the Mott state of fermions Expts: Joerdens et al., Nature (2008) Greif, Tarruell, Strohmaier, Moritz, Esslinger et al. Theory: Kollath et al., PRA (2006) Huber, Ruegg, PRA (2009) Sensarma et al. PRL 2009 Pollet, Pekker, Demler, unpublished Yesterday’s talks by Henning Moritz and Andreas Ruegg

  4. Modulate lattice potential Lattice modulation experiments Probing dynamics of the Hubbard model Measure number of doubly occupied sites Main effect of shaking: modulation of tunneling Doubly occupied sites created when frequency w matches Hubbard U

  5. Lattice modulation experiments Probing dynamics of the Hubbard model R. Joerdens et al., Nature 455:204 (2008)

  6. Mott gap for the charge forms at Antiferromagnetic ordering at Mott state Regime of strong interactionsU>>t. “High” temperature regime All spin configurations are equally likely. Can neglect spin dynamics.

  7. Doublon production rate depends on propagation of doublons and holes Retraceable Path Approximation Brinkmann & Rice, 1970 preliminary data Experimental data courtesy of D. Greif Spectral Fn. of single hole Doublon Production Rate

  8. Lattice modulation experiments. Sum rule Ad(h) is the spectral function of a single doublon (holon) T-independent ? Sum Rule : Simple model to include temperature dependence and trap: multiply production rate by the average fraction of nearest neighbors with opposite spins preliminary data courtesy of D. Greif

  9. Ramsey Interference in one dimensional systems • Using quantum noise to study many-body dynamics

  10. One dimensional systems in condensed matter Non-perturbative effects of interactions: Absense of long range order Electron fractionalization GaAs/AlGaAs Heterostructures carbon nanotubes 1d organics Emphasis on equilibrium properties and linear response

  11. 1D Ramsey Interferometry (Widera, et.al PRL 2008) 1d systems of ultracold atoms: analysis of nonequilibrium dynamics Time evolution of coherence in split condensates S. Hofferberth et al., Nature (2007)

  12. Introduction:Ramsey Interference

  13. 1 Working with N atoms improves the precision by . t 0 Ramsey interference Atomic clocks and Ramsey interference:

  14. Ramsey Interference with BEC Single mode approximation Gaussian distribution of Sz Spin squeezing: possible application in quantum enhanced metrology Sorensen, Moller, Cirac, Zoller, Lewensstein, …

  15. Ramsey Interference with 1d BEC 1d systems in microchips 1d systems in optical lattices Two component BEC in microchip • Ramsey interference in 1d tubes: • Widera et al., • PRL 100:140401 (2008) Treutlein et.al, PRL 2004

  16. Ramsey Interference in 1d:a probe of many-body dynamics

  17. Ramsey interference in 1d condensates Spin echo experiments A. Widera, et al, PRL 2008 Only partial revival after spin echo! Expect full revival of fringes

  18. Spin echo experiments in 1d tubes Single mode approximation does not apply. Need to analyze the full model

  19. Low energy effective Hamiltonianfor spin dynamics Bosonization Tomonaga-Luttinger Hamiltonian 19

  20. Small uncertainty in Ramsey interference: Initial State After p/2 pulse, spins point in x direction Initial state: squeezed state infs Wk determined from Short distance cut-off at spin healing length related argument in Bistrizer, Altman, PNAS (2008)

  21. Ramsey interference in 1dTime evolution Luttinger liquid provides good agreement with experiments. A. Widera et al., PRL 2008. Theory: V. Gritsev Technical noise could also lead to the absence of echo Need “smoking gun” signatures of many-body decoherece

  22. Distribution functionsof Ramsey amplitude

  23. Distribution Probing spin dynamics through distribution functions Distribution function contains information about higher order correlations Joint distribution function can also be obtained

  24. Interference of independent 1d condensates S. Hofferberth, I. Lesanovsky, T. Schumm, J. Schmiedmayer, A. Imambekov, V. Gritsev, E. Demler, Nature Physics (2008) Higher order correlation functions probed by noise in interference

  25. Joint distribution functions Short segments |S|^2 does not changebut Sx decays Long segments both Sx and |S|^2 decay

  26. Two regimes of spin dynamics Modes with λ>l leads to the decay of Sx but not |S| Modes with λ<l leads to the decay of both Sx and |S|

  27. Analytic solution for the distribution function

  28. Summary • Suggested unique signatures of the multimode decoherence of Ramsey fringes in 1d • Ramsey interferometer combined with study of distribution function is a useful tool to probe many-body dynamics • Joint distribution functions provide simple visualization of complicated many-body dynamics

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