Bose-Bose mixtures in confined dimensions

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Bose-Bose mixtures in confined dimensions Francesco Minardi Istituto Nazionale di Ottica-CNR European Laboratory for Nonlinear Spectroscopy 22nd

1 Bose-Bose mixtures in confined dimensions Francesco Minardi Istituto Nazionale di Ottica-CNR European Laboratory for Nonlinear Spectroscopy 22nd International Conference on Atomic Physics Cairns, July 29, 2010 Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 1 / 34

2 Why Bose-Bose mixtures? (Our) motivation Bose-Bose mixtures in optical lattices map to spin hamiltonians J. Catani et al., Phys. Rev. A (2008) few-body physics in ultracold collisions: - Efimov resonances with heavy/light atoms [G. Barontini et al., Phys. Rev. Lett. (2009)] - scattering in confined dimensions [G. Lamporesi et al., Phys. Rev. Lett. (2010)] entropy control (and thermometry) of species A by means of a species B [J. Catani et al., Phys. Rev. Lett. (2009)] Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 2 / 34

3 Two-body scattering in low dimensions Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 3 / 34

4 Scattering in a waveguide [M. Olshanii, Phys. Rev. Lett. 81, 938 (1998)] Quick reminder: scattering of two atoms via a pseudo-potential U(r) = gδ( r)(r r ) in a tight waveguide Strong confinement along two directions: E ω, k l 1, l = /mω - Scattering amplitude - 1-dimensional scattering length 1 f = 1 + ika 1D a 1D = l2 a (1 C a l ), C = / 2 - Same as 1D potential U(z) = g 1D δ(z), g 1D = 2 µa 1D Confinement-induced resonance (CIR): a 1D 0, g 1D for l = Ca Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 4 / 34

5 Confinement-induced resonances, interpretation [T. Bergeman et al., Phys. Rev. Lett. 91, (2003)] - 1D, bound state for all values of scattering length, a (vs 3D: bound state for a > 0) - CIR as FR: closed channel = set of excited harmonic transverse levels - only 1 CIR for all excited states - decoupling of internal and center-of-mass motion Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 5 / 34

6 Confinement-induced molecules and resonances, exp Experiments - Confinement-induced molecules with 40 K atoms [H. Moritz et al., Phys. Rev. Lett. 94, (2005)] Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 6 / 34

7 Confinement-induced molecules and resonances, exp Experiments - Confinement-induced molecules with 40 K atoms [H. Moritz et al., Phys. Rev. Lett. 94, (2005)] - CIR on Cs atoms [E. Haller, Science 325, 1124 (2009)] Very recently, - CIR in elliptic waveguide [E. Haller et al., Phys. Rev. Lett. 104, (2010)] - CIR in quasi-2d with 6 Li atoms [P. Dyke et al., poster Mo77] Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 6 / 34

8 Mix-dimensional configuration Different kind of particles can live in different dimensions - In our experiment, two atomic species: 87 Rb free in 3D, 41 K confined in 2D Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 7 / 34

9 Scattering resonances in mixed dimensions [in collaboration with Y. Nishida, MIT] Translational symmetry in the (xy) plane, drop center-of-mass X, Y coordinates [ 2 2µ 2 r 2 2 z1 2 2 z2 + 1 ] 2m 1 2m 2 2 m1ω2 z1 2 + gv ψ(r, z 1, z 2) = Eψ(r, z 1, z 2), where r = (x 1 x 2, y 1 y 2) Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 8 / 34

10 Scattering resonances in mixed dimensions (II) General solution ψ(r, z 1, z 2) = ψ 0(r, z 1, z 2) + g dx G E (r, z 1, z 2; 0, z, z )ψ reg (z ) V ψ(r 1, r 2) ψ reg (r) r=r1 =r 2 = ψ reg (z) At large distance r, z 1 z 2 : ψ(r, z 1, z 2) = φ 0(z 1) 1 a eff which defines the effective scattering length a eff At short distance R = r 2 + (z 1 z 2) 2 0 [ 1 ψ(r, z 1, z 2) = a 1 ] ψ reg (z) z=z1 =z R 2, Secular equation ties a eff with a: 1 a b i M ij b j = [ 1 a eff 1, (1) m2 z 2 µ 2 + r 2 ] m2 µ δ 0iδ 0j + M ij b j Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 9 / 34

11 Scattering length in mixed dimensions (III) Result: a eff for multiple values of a/l depending only on the mass ratio m 1/m 2 ( ) [courtesy of Y. Nishida] Analysis very close to previous work of P.Massignan and Y.Castin, Phys. Rev. A 74, (2006) ( ) only approx with effective range corrections... Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 10 / 34

12 How-to? Species-selective dipole potential Suitable choice of laser wavelength optical dipole potential selective on atomic species [L. J. LeBlanc and J. H. Thywissen, Phys. Rev. A 75, (2007)] For our particular mixture, i.e. 87 Rb 41 K, λ = nm. For Rb, D1 and D2 light-shifts cancel out Tight confinement realized by 1D optical lattice V 0 = se r Array of 2D traps: l = λ/(2πs 1/4 ) (e.g. l = 1200a 0 for s = 15) Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 11 / 34

13 Entropy transfer Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 12 / 34

Interspecies entropy transfer Idea: compress only K - ω(k), T c(k) increase - T const (thanks to Rb) - T /Tc(K) decreases K entropy lower before Similar to reversible BEC with dimple

14 Interspecies entropy transfer Idea: compress only K - ω(k), T c(k) increase - T const (thanks to Rb) - T /Tc(K) decreases K entropy lower before Similar to reversible BEC with dimple potential [D. M. Stamper-Kurn et al., Phys. Rev. Lett. 81, 2194 (1998)] after compression Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 13 / 34

15 BEC transition Textbook thermodynamics, ideal gases in harmonic trap ω K BEC fraction Total entropy conservation - Above T c: S/(Nk B ) = 4g 4(z)/g 3(z) log(z) with N = g 3(z)(T /ω) 3, g n(z) = k>0 z k /k n - Below T c: S/(Nk B ) = 4[g 4(1)/g 3(1)](1 f c) BEC fraction f c = 1 t 3 η[g 2(1)/g 3(1)]t 2 (1 t 3 ) 2/5, t = T /T c, η = µ/k B T [J. Catani et al., Phys. Rev. Lett. 103, (2009)] Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 14 / 34

16 Reversibility of BEC phase transition Compression/decompression cycles: ω K /(2π) = Hz Up to 5 cycles of BEC In practice, reversibility limit is heating/atom loss of Rb Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 15 / 34

17 Interspecies Feshbach resonances Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 16 / 34

18 Interspecies 41 K- 87 Rb Feshbach resonances Inelastic atomic collisions, 2 interspecies FR: broad, B 0 39G narrow, B 0 79G G. Thalhammer et al., Phys. Rev. Lett. 100, (2008) Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 17 / 34

19 RF association of Feshbach molecules Precise method to locate FR molecular spectroscopy, i.e. drive free-to-bound transitions by oscillating magnetic field [S. T. Thompson et al. Phys. Rev. Lett (2005)] Measure loss of atoms converted in molecules [C. Weber et al. Phys. Rev. A (R) (2008)] Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 18 / 34

20 Control of interspecies interactions Feshbach spectroscopy + collisional model, A. Simoni, University of Rennes knowledge of 41 K- 87 Rb scattering length Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 19 / 34

21 Mix-dimensional scattering Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 20 / 34

22 Experiment - Mixture in (1,1)+(1,1) hf states, sympathetic cooling in optical trap to 300 nk - Set B below both FR, raise SSDP lattice to selectively confine K in 2D - Set B to final value, hold for fixed time, record remaining atom number Assumption: enhancement of inelastic collisions, i.e. atom number minima, for a eff Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 21 / 34

23 Experiment - Mixture in (1,1)+(1,1) hf states, sympathetic cooling in optical trap to 300 nk - Set B below both FR, raise SSDP lattice to selectively confine K in 2D - Set B to final value, hold for fixed time, record remaining atom number Assumption: enhancement of inelastic collisions, i.e. atom number minima, for a eff 3 2 M a g n e tic F ie ld (G a u s s ) N R b + N K s = 0 s = 2 0 1,0 1,2 1,4 1,6 1,8 2,0 2,2 2,4 2,6 2,8 3,0 F ie ld (V ) Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 21 / 34

24 Experiment - Mixture in (1,1)+(1,1) hf states, sympathetic cooling in optical trap to 300 nk - Set B below both FR, raise SSDP lattice to selectively confine K in 2D - Set B to final value, hold for fixed time, record remaining atom number Assumption: enhancement of inelastic collisions, i.e. atom number minima, for a eff Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 21 / 34

25 Simple physical picture Position of resonances obtained by a simple argument Degeneracy: E(threshold) = E of bound state Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 22 / 34

26 Simple physical picture Position of resonances obtained by a simple argument Degeneracy: E(threshold) = E of bound state Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 22 / 34

27 Simple physical picture Position of resonances obtained by a simple argument Degeneracy: E(threshold) = E of bound state from excited confined states (1/2)ω K =(n + 1/2)ω KRb E binding / where ω KRb =ω K mk /(m K + m Rb ) p 2 Rb/(2m Rb ) neglected - very good agreement with above results of scattering theory - multiple resonances because internal and center-of-mass motion are coupled - by parity conservation, only states with even-n couple to n = 0 (for p Rb = 0) Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 22 / 34

28 Predictions for our specific FR To change a KRb, change magnetic field To change ω K, ω KRb, change s, strength of SSDP lattice Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 23 / 34

29 Experimental data Predictions do not match the data - positions are offset - peaks at odd-n Harmonic oscillator levels are not correct lattice band structure - At T = 300 nk, k B T /m K 0.6 k thermal filling of 1st BZ - quasi-momenta q 0 not parityeigenstates odd-n peaks allowed Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 24 / 34

Experimental data Predictions do not match the data - positions are offset - peaks at odd-n Harmonic oscillator levels are not correct lattice band structure - At T = 300 nk, k B T /m K 0.

30 Experimental data Predictions do not match the data - positions are offset - peaks at odd-n Harmonic oscillator levels are not correct lattice band structure - At T = 300 nk, k B T /m K 0.6 k thermal filling of 1st BZ - quasi-momenta q 0 not parityeigenstates odd-n peaks allowed Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 24 / 34

Experiment/theory comparison Energy degeneracy re-calculated: p 2 /(2m Rb ) + ɛ K (0, q; V K lat) = ɛ KRb (n, q + p; V K lat) E b - ɛ i (n, q; V K lat), energy of the Bloch wave of particle i = K,

31 Experiment/theory comparison Energy degeneracy re-calculated: p 2 /(2m Rb ) + ɛ K (0, q; V K lat) = ɛ KRb (n, q + p; V K lat) E b - ɛ i (n, q; V K lat), energy of the Bloch wave of particle i = K, KRb - (n, q) quasimomentum/band index - V K lat lattice potential - p initial Rb momentum - E b, binding energy Neglect resonance shift due to channel coupling, for all n > 0 Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 25 / 34

32 Summary species-selective potential engineers a mix-dimensional configuration entropy transfer and reversible BEC mix-dimensional scattering resonances are observed, their position is accounted for by simple energy argument lattice band structure needed mix-dimensional configuration a route to Efimov physics? Identical particles: 2.3 < D < 3.8 D = 3 2 fermions: m 1/m 2 > 13.6 in 3D, m 1/m 2 > 6.35 in 2D-3D, m 1/m 2 > 2.06 in 1D-3D Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 26 / 34

Acknowledgements BEC3 Group at LENS, Firenze Staff: Postdocs: PhD students: Undergraduate students: M. Inguscio, FM J. Catani, G. Lamporesi, G. Thalhammer (now in Innsbruck) G.

33 Acknowledgements BEC3 Group at LENS, Firenze Staff: Postdocs: PhD students: Undergraduate students: M. Inguscio, FM J. Catani, G. Lamporesi, G. Thalhammer (now in Innsbruck) G. Barontini, C. Weber (now in Bonn) F. Rabatti Positions available for PhD students Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 27 / 34

The end Thank you http://quantumgases.lens.unifi.

34 The end Thank you Francesco Minardi (INO-CNR and LENS) Bose-Bose mixtures in confined dimensions 22nd ICAP, Cairns 28 / 34

arxiv: v2 [cond-mat.quant-gas] 17 Mar 2010

arxiv: v2 [cond-mat.quant-gas] 17 Mar 2010 Scattering in Mixed Dimensions with Ultracold Gases arxiv:1.114v [cond-mat.quant-gas] 17 Mar 1 G. Lamporesi 1, J. Catani 1,, G. Barontini 1, Y. Nishida 3, M. Inguscio 1,, and F. Minardi 1, 1 LENS - European