ROTONS AND STRIPES IN SPIN-ORBIT COUPLED BECs

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1 INT Seattle 5 March 5 ROTONS AND STRIPES IN SPIN-ORBIT COUPLED BECs Yun Li, Giovanni Martone, Lev Pitaevskii and Sandro Stringari University of Trento CNR-INO Now in Swinburne Now in Bari Stimulating discussions with: Jean Dalibard, Gabiele Ferrari, Giacomo Lamporesi

2 Simplest realization of (D) spin-orbit coupling in s=/ Bose-Einstein condensates (Spielman team at Nist, 9) Two detuned ( L ) and polarized laser beams + non linear Zeeman field ( Z ) provide Raman transitions between two spin states, giving rise to new single particle physics

3 New single particle Hamiltonian h [ px k z p] x z p x k is canonical momentum is laser wave vector difference is strength of Raman coupling L Z is effective Zeeman field physical velocity equal to vx ( px k z) / m Hamiltonian h - is translationally invariant despite the presence of the laser fields [ h, ] p x - Breaks parity, time reversal and Galilean invariance

4 Symmetry properties of the spin-orbit Hamiltonian h [ px k z p] x z - Translational invariance: uniform ground state configuration, unless crystalline order is formed spontaneously (stripes, supersolidity) - Violation of parity and time reversal symmetry breaking of symmetry ( q) ( q) in excitation spectrum (exp: Si-Cong Ji et al. PRL 5; theory: Martone et al. PRA ) - Violation of Galilean invariance: breakdown of Landau criterion for superfluid velocity and emergence of dynamical instabilities in uniform configurations (exp: Zhang et. al. PRL, theory: Ozawa et al. (PRA 3))

5 Different strategies to realize novel quantum phases - First strategy (Lin et al., Nature 9). Spatially dependent detuning ( (y)) in strong Raman coupling ( k ) regime yields position dependent vector potential h px Ax ( y) and effective Lorentz force m* in neutral atoms. This causes the appearence of quantized vortices. No y-dependence In detuning strong y-dependence In detuning

6 Second strategy (Lin et al. Nature ) - Small detuning ( ) and smaller Raman coupling ( k ) give rise to the appearence of two degenerate minima which can host a Bose-Einstein condensate.

7 Key question: Role of interactions in the presence of the novel spin-orbit single particle Hamiltonian. Rich scenario with new quantum phases

8 Theory of quantum phases in D SO coupled s=/ BECs (T=) Ho and Zhang (PRL ),., Yun Li, Pitaevskii, Stringari (PRL ) H ( drgn n h i) i, - With h [ px k z p] x z - We assume g g g phase mixing in the absence of Raman coupling - Interactions are treated within mean field approximation (s=/ coupled Gross-Pitaevskii equations)

9 For small values of two sp states can host BEC with canonical momentum k k /[k int] k Order parameter in the new phases cos sin V sin cos N ikx ik x I) Stripe phase e e + higher harmonics cos k k n( x) n( cos kx) k density fringes fixed by k I) Plane wave phase sin e V cos N ik x z k k II) Zero momentum phase N V

10 New quantum phases (T=) 87 F, m F, m a a Rb.4a a F F B.94a B (phase separated) (phase mixed)

11 Plane wave-single minimum phase transition Transition is second order. It has been observed at the predicted value 4E L k of the Raman coupling Lin et al., Nature Phase transition is driven by single-particle Hamiltonian. does not require two-body interactions. Spin polarizability diverges at the transition (G. Martone, Yun Li, S.S. EPL ) k ( z ) k (4k ) ( ) k z k Zhang et al. PRL

12 Striped-plane wave phase transitions Transition is first order. Critical frequency is (Ho and Zhang PRL ) cr k where g g g g g g A phase transition between a spin mixed and a spin separated phase has been observed at the predicted value of Lin et al., Nature Si-Cong Li et al. Nat. Phys.,4 Density modulations are not however visible in the spin mixed phase (too small contrast and too small fringe separation) Proof of coherence is provided by fringes, not by mixing.

13 Spin-orbit coupling has important consequences on the dynamic behavior of BECs Experiments already available Quenching of Center of mass frequency in harmonic trap (violation of Kohn s theorem) (exp: Zhang et al.; theory: Yun Li et al. EPL ) Emergence of Roton and softed Phonon Modes (exp: Si-Cong Ji et al.; PRL 5; theory Yun Li et al. Martone et al. PRA ) Two Goldstone modes in striped Phase Theory: Yun Li et al. PRL 3

14 Emergence of Rotons in Plane Wave phase Excitation spectrum exhibits two branches. Due to Raman coupling only one branch is gapless and exhibits a phonon behavior at small q phonons Exp: Si-Cong Ji et al., PRL 5 Theory: Martone et al., PRA

15 At small Raman coupling, a roton structure emerges in the lower branch Exp: Si-Cong Ji et al., PRL 4, 53 (5) Theory: Martone et al., PRA 86, 636 () ( q) ( q) consequence of violation of parity and time reversal symmetry cr Roton gap decreases as Raman coupling is lowered: onset of crystallization (striped phase)

16 Roton Gallery Liquid Helium (historical) Spin-orbit BEC s (4) Other theoretical proposals BEC s in shaken lattices (4) Pancake dipolar BEC s BEC s with soft core repulsive potentials

17 THE STRIPED PHASE Why is the striped phase of a Bose-Einstein condensate interesting? Can we make stripes visible and stable?

18 Striped phase is the result of interaction effects Competition between spin and density dependent interactions (for simplicity we assume g g g ) - Spin dependent term (proportional to ( g g ) dr ( n n ) ) favours spin mixing and hence, in the presence of SO term and Raman coupling, favours the emergence of density modulations (stripes) - Density dependent term (proportional to ( g g ) dr ( n n ) ) favours uniformity (plane wave phase). At small Raman coupling (for cr ) stripes are energetically favoured. Value of depends only on the ratio ( g g ) /( g g ) cr

19 Striped phase results from spontaneous breaking of two continuous symmetries. gauge and translational symmetries Two Goldstone modes: - Double band structure in the striped phase of a SO coupled Bose-Einstein condensate - Lower phonon branch better excited by spin operator (Yun Li et al. PRL 3)

20 Improving visibility and stability of superstripes (Martone, Yun Li and Stringari, Phys. Rev. A 9, 464(R) (4)

21 In Nist (Lin et al., Nature ) and Shanghai (Si-Cong Li Nat. Phys. 4) experiments stripes are not visible: - contrast is too small. Doubly integrated density from Gross-Pitaevskii simulation in the same condition of 87Rb Nist exp. exhibits small contrast...5k E L - Separation between fringes is too small (fraction of micron) - Stripes are fragile against magnetic fluctuations. Tiny magnetic field (corresponding to detuning of 3-5 Hertz) destabilizes the stripes.

22 How to increase the contrast of density modulations? n( x) n[ cos(k x )] k Maximum value of Raman coupling compatible with the striped phase is given by where g g g cr k ( ) g g g In 87Rb cr. k and hence achievable contrast is very small. cr In order to increase one should reduce. HOW? g - Feshbach tuning of interspecies scattering length preserving condition a a a - We propose D geometry based on two spin layers separated by distance d. Separation reduces g by factor exp( d / ) with respect to g and a z g V d ext ( z) z ( z z ) d

23 3D Gross-Pitaevskii simulation for Rb atoms in harmonic trap Parameters: (,, ) (5,, 5) Hz a E r x y z.4a B a a k /.8 KHz ; V ext ( r) x x y y z ( z z.94 a B cr d ) d. E r 7Hz

24 3D Gross-Pitaevskii simulation for Rb atoms in harmonic trap Parameters: (,, ) (5,, 5) Hz a E r x y z.4a B a a k /.8 KHz ; V ext ( r) x x y y z ( z z.94 a B cr d ) d. E r 7Hz Increasing contrast of fringes d a z.5 E r.6 KHz

25 Increasing wave length of fringes Apply / Bragg pulse transferring momentum p B k to the atomic cloud (with k ). Each component of the condensate function in the striped phase i( k k ) x i( k k ) x e e (a) (b) will be fragmented in 3 terms. Components (a) and (b), after / pulse, will be able to interfere with wave length /

26 Density fringes of striped phase after / Bragg pulse with momentum k and. k p B d a z Without Bragg

27 Density fringes of striped phase after / Bragg pulse with momentum k and. k p B d a z Without Bragg Increasing wave length of fringes d a z With Bragg

28 Stability of the striped phase Reducing interspecies coupling constant enhances robustness of the striped phase. Chemical potential difference between mixed and demixed phase at is given by n( g g ) / with g g g Choosing d ( g g ) critical detuning corresponds to tiny fraction of recoil energy (few Hertz) d

29 Stability of the striped phase Reducing interspecies coupling constant enhances robustness of the striped phase. Chemical potential difference between mixed and demixed phase at is given by n( g g ) / with g g g Choosing d ( g g ) critical detuning corresponds to tiny fraction of recoil energy (few Hertz) Choosing d a z ( g. 6g ) critical detuning corresponds to.6 E r (a few hundred Hertz) d d a z Increasing stability of fringes e ~ d / 4a

30 Rotonic structure, static structure factor and static response function in plane wave phase Rotons and stripes V cos e sin N ik x Apply static perturbation ikx Vext ser (k e ) Strong non linear effects caused by large value of static response: Emergence of stripes

31 - Stripes have small contrast in stripe phase - No polarization..5k E L - stripes have large contrast in PW phase with s=.5 - spin polarization is strongly reduced - No stripes in PW phase - Almost full spin polarization

32 Main conclusions : - Rotonic excitation in plane wave phase is onset of crystallization exhibited by striped phase - Two Goldstone modes in striped phase - Contrast and stability of stripes can be significantly enhanced creating two separated spin layers. - Wave length of density fringes can be increased by applying Bragg or rf pulse / - Stripes can be produced in plane wave phase by adding small static perturbation

33 arxiv:5.495 The Trento BEC team Visit our web site

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