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Cold Atoms in rotating optical lattice Sankalpa Ghosh, IIT Delhi Ref: Rashi Sachdev, Sonika Johri, SG arXiv: 1005.4391 Acknowledgement: G.V Pi, K. Sheshadri, Y. Avron, E. Altman HRI Workshop on strong Correlation, Nov. 2010

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Bosons and Fermions

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Nobel Prizes 1997, 2001

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Bose Einstein Condensate of Cold Atoms Bose Einstein condensate of cold atoms Characterized by a macroscopic wave function Described by Gross-Pitaevski equation T=nK Gross Pitaevskii description works if

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Optical Lattices Optical lattices are formed by standing waves of counter propagating laser beams and act as a lattice for ultra cold atoms. These systems are highly tunable: lattice spacing and depth can be varied by tuning the frequency and intensity of lasers. These optical lattices thus are artificial perfect crystals for atoms and act as an ideal system for studying solid state physics phenomenon, with more tunability of parameters than in actual solids. Nature, Vol 388, 1997

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Bose Hubbard Model If the wavelength of the lattice potential is of the order of the coherence length then the Gross-Pitaevskii description breaks down. Tight binding approximation The many boson hamiltonian is

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Bose Hubbard Model Trapping potential confining frequency 10-200 Hz Optical Lattice potential confining frequency 10-40 KHz I Bloch, Nature (review article)

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Bose Hubbard Model Bose Hubbard Model : It describes an interacting boson gas in a lattice potential, with only onsite interactions. Fisher et al. PRB (1989) Sheshadri et al. EPL(1993) Jaksch et.al, PRL (1998) Superfluid phase : sharp interference pattern Mott Insulator phase : phase coherence lost t>> U U >> t

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Mean field treatment Sheshadri et al. EPL (1993) Decouple the hopping term and retain the terms only linear in fluctuation Gutzwiller variational Wave function

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Cold Atoms with long range Interaction Example 1 : dipolar cold gases ( 52 Cr Condensate, T. Pfau’s group Stutgart ( PRL, 2005) Example 2: Cold Polar Molecules Example 3: BEC coupled with excited Rydberg states: ( Nath et al., PRL 2010) Add Optical lattice Tight binding approximation Extended Bose Hubbard Model

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NNN NNNN NN K Goral et al. PRL,2002 Santos et al. PRL, 2003 Minimal EBH model-just add the nearest neighbor interaction New Quantum Phases – Density wave and supersolid T D Kuhner et al. (2000)

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Phase diagram of e-BHM with DW, SS, MI and SF phases Due to the competition between NN term and the onsite interaction, new phases such as Density wave and supersolids are formed Kovrizhin, G. V. Pai, Sinha, EPL 72(2005) G. G. Bartouni et al. PRL (2006) Pai and Pandit (PRB, 2005) At t=0, we have transitions between DW (n/2) to MI(n) at and then to DW(n/2+1) at d - being the dimension of system. DW (½)=|1,0,1,0,1,0,......> MI( 1) =|1,1,1,1,……>

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Density Wave Phase : Alternating number of particles at each site of the form Superfluid order parameter or the macroscopic wave function vanishes. There is no coherence between the atomic wave functions at sites, on the other hand site states are perfect Fock states Supersolid Phase : Why Superfluid?, there is macroscopic wave- function showing superfluid behaviour, flows effortlessly. Why Crystalline ? Order parameter shows an oscillatory behaviour as a function of site co- ordinate ( Superfluid +Density wave ) Soldiers marching along coherently Crystalline Superfluid Kim and Chan, Science (2004)

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Magnetic field for neutral atoms How to create artificial magnetic field for neutral atoms? JILA, Oxford G. Juzelineus et al. PRA (2006)

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Rotating Optical Lattice Y J Lin et al. Nature(2009)

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Bose Hubbard model in a magnetic field M. Niemeyer et al(1999), J Reijinders et al. (2004), C. Wu et al. (2004) M Oktel et al. (2007), D. GoldBaum et al. (2008) (2008), Sengupta and Sinha (2010), Das Sharma et al. (2010)

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Topological constraint

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Extended Bose Hubbard Model under magnetic field Ground state of the Hamiltonian is found by variational minimization with a Gutzwiller wave function For the Density wave phase we have two sublattices A & B * Set m=n Mott Phase ( R.Sachdeva, S.Johri, S.Ghosh arXiv 1005.4391v1 )

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Reduced Basis ansatz Goldbaum et al ( PRA, 2008) Umucalilar et al. (PRA, 2007) Close to the Mott or Density wave boundary only two neighboring Fock states are occupied MI-SF DW-SS

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Variational minimization of the energy gives DW BoundaryTime dependent variational mean field theory

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Include Rotation Substitute the variational parameters

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Minimize with respect to the variational parameters Two component superfluid order parameter

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Harper Equation Spinorial Harper Equation Where the spatial part of the wave function satisfies Eigenvalues of Hofstadter butterfly can be mapped to

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Hofstadter Butterfly Hofstadter Equation in Landau gauge Color HF Avron et al.

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Typically electron in a uniform magnetic field forms Landau Level each of is highly degenerate A plot of such energy levels as a function of Increasing strength of magnetic field will be a set Of straight line all starting from origin If a periodic potential is added as an weak perturbation then it lifts this degeneracy and splits each Landau level into n Φ sublevels where n Φ =Ba 2 /φ 0 namely the number of fluxes through each unit ce ll Hofstadter butterfly

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DW Phase Boundary Boundary of the DW & MI phase related to edge eigen value of Hofstadter Butterfly

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Modification of the phase boundary due to the rotation or artificial magnetic field

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Plot of Eigenfunction Vortex in a supersolid Vortex in a superfluid Checker board vortices Surrounding superfluid density Shows two sublattice modulation Highest band of the Hofstadter butterfly

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What about the other eigenvalues ? Density wave order parameter Good starting points for more general solutions within Gutzwiller approximation

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Experimental detection Time of flight imaging : interference pattern will bear signature of the sublattice modulated superfluid density around the core Bragg Scattering : Structure factor, Phase sensitivity etc. Real Space technique ? Momentum space

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