Abstract:We explore the quantum phases emerging from the interplay between spin and motional degrees of freedom of a one-dimensional quantum fluid of spinful fermionic atoms, effectively interacting via a photon-mediating mechanism with tunable sign and strength g, as it can be realized in present-day experiments with optical cavities. We find the emergence, in the very same system, of spin-and atomic-density wave ordering, accompanied by the occurrence of superfluidity for g > 0, while cavity photons are seen to drive… Show more
“…Since the longrange (in fact, in our setup it is infinite-range) nature of the cavity-mediated interaction implies that any atom will always interact with a large number of other atoms, this approach is well justified. This was found to be the case even in one dimension in [36] using bosonisation methods. We decouple the electron interactions using the mean fields…”
mentioning
confidence: 88%
“…Artificial magnetic fields can be induced to create distinct topological phases [27][28][29]. Most importantly, various types of cavity-mediated interactions could give rise to a plethora of many-body phases [30][31][32][33][34][35][36][37][38], including superfluid and charge density states, and even more exotic phases with no direct analog in condensed matter systems. All these developments render ultracold fermionic atoms natural candidates to explore exotic physics, such as topological phases [39][40][41], which would be more difficult to observe in condensed matter.…”
mentioning
confidence: 99%
“…Previous theoretical works describing cavity-mediated interactions of fermionic atoms had focused on one-dimensional lattices [33][34][35][36]. In [36], the spin states were energetically separated, such that the cavity coupling was shown to induce either singlet superfluidity or spin-density order. Camacho-Guardian et al [35] investigate the same effective interaction mechanism as considered here.…”
We investigate long-range pairing interactions between ultracold fermionic atoms confined in an optical lattice which are mediated by the coupling to a cavity. In the absence of other perturbations, we find three degenerate pairing symmetries for a two-dimensional square lattice. By tuning a weak local atomic interaction via a Feshbach resonance or by tuning a weak magnetic field, the superfluid system can be driven from a topologically trivial s-wave to topologically ordered, chiral superfluids containing Majorana edge states. Our work points out a novel path towards the creation of exotic superfluid states by exploiting the competition between long-range and short-range interactions.Ultracold fermionic gases form an ideal platform for a new generation of quantum technologies [1,2], and for the quantum simulation of many-body phenomena [3,4] such as superfluidity [5,6]. Their key feature for these applications is that local (on-site) atomic interactions can be tuned very precisely using Feshbach resonances to explore, e.g, the crossover from BCS to BEC regimes [7], quantum simulation of the Fermi Hubbard model [8], and strongly correlated fermions in reduced dimensions [9][10][11][12]. Coupling ultracold atoms to optical cavities [13][14][15][16][17][18][19][20][21][22] promises to extend this control to longranged interactions.
“…Since the longrange (in fact, in our setup it is infinite-range) nature of the cavity-mediated interaction implies that any atom will always interact with a large number of other atoms, this approach is well justified. This was found to be the case even in one dimension in [36] using bosonisation methods. We decouple the electron interactions using the mean fields…”
mentioning
confidence: 88%
“…Artificial magnetic fields can be induced to create distinct topological phases [27][28][29]. Most importantly, various types of cavity-mediated interactions could give rise to a plethora of many-body phases [30][31][32][33][34][35][36][37][38], including superfluid and charge density states, and even more exotic phases with no direct analog in condensed matter systems. All these developments render ultracold fermionic atoms natural candidates to explore exotic physics, such as topological phases [39][40][41], which would be more difficult to observe in condensed matter.…”
mentioning
confidence: 99%
“…Previous theoretical works describing cavity-mediated interactions of fermionic atoms had focused on one-dimensional lattices [33][34][35][36]. In [36], the spin states were energetically separated, such that the cavity coupling was shown to induce either singlet superfluidity or spin-density order. Camacho-Guardian et al [35] investigate the same effective interaction mechanism as considered here.…”
We investigate long-range pairing interactions between ultracold fermionic atoms confined in an optical lattice which are mediated by the coupling to a cavity. In the absence of other perturbations, we find three degenerate pairing symmetries for a two-dimensional square lattice. By tuning a weak local atomic interaction via a Feshbach resonance or by tuning a weak magnetic field, the superfluid system can be driven from a topologically trivial s-wave to topologically ordered, chiral superfluids containing Majorana edge states. Our work points out a novel path towards the creation of exotic superfluid states by exploiting the competition between long-range and short-range interactions.Ultracold fermionic gases form an ideal platform for a new generation of quantum technologies [1,2], and for the quantum simulation of many-body phenomena [3,4] such as superfluidity [5,6]. Their key feature for these applications is that local (on-site) atomic interactions can be tuned very precisely using Feshbach resonances to explore, e.g, the crossover from BCS to BEC regimes [7], quantum simulation of the Fermi Hubbard model [8], and strongly correlated fermions in reduced dimensions [9][10][11][12]. Coupling ultracold atoms to optical cavities [13][14][15][16][17][18][19][20][21][22] promises to extend this control to longranged interactions.
“…These systems exhibit many more interesting phenomena, including the emergence of synthetic strong magnetic fields and spin-orbit coupling [46][47][48][49], disorder-driven density and spin self-ordering [50], topological states [51,52], and a variety of magnetic Any further distribution of this work must maintain attribution to the author(s) and the title of the work, journal citation and DOI. orders [53,54]. Very recently, first experimental implementations showing spin self-ordering in a spin-1 BEC in a standing wave cavity were realized [55,56].…”
The coupled nonlinear dynamics of ultracold quantum matter and electromagnetic field modes in an optical resonator exhibits a wealth of intriguing collective phenomena. Here we study a Λ-type, threecomponent Bose-Einstein condensate coupled to four dynamical running-wave modes of a ring cavity, where only two of the modes are externally pumped. However, the unpumped modes play a crucial role in the dynamics of the system due to coherent backscattering of photons. On a mean-field level we identify three fundamentally different steady-state phases with distinct characteristics in the density and spatial spin textures: a combined density and spin-wave, a continuous spin spiral with a homogeneous density, and a spin spiral with a modulated density. The spin-spiral states, which are topological, are intimately related to cavity-induced spin-orbit coupling emerging beyond a critical pump power. The topologically trivial density-wave-spin-wave state has the characteristics of a supersolid with two broken continuous symmetries. The transitions between different phases are either simultaneously topological and first-order, or second-order. The proposed setup allows the simulation of intriguing many-body quantum phenomena by solely tuning the pump amplitudes and frequencies, with the cavity output fields serving as a built-in nondestructive observation tool. New J. Phys. 21 (2019) 013029 S Ostermann et al *
“…With the prediction of new intriguing phenomena such as Umklapp superradiance [26,27], topologically protected edge states [28,29], superconducting pairing [30,31], artificial dynamic gauge fields [20], unconventional momentum correlations and quantum phases in multiple dimensions [32][33][34][35], implementations of fermionic systems coupled to cavity fields have gained more attention recently. In the present article, we propose the realization of density and spin self-ordering for a transversely driven multi-level Fermi gas coupled to a pair of counterpropagating degenerate modes of a ring cavity as depicted in figure 1 [36][37][38][39][40][41][42].…”
We explore the density and spin self-ordering of driven spin-1/2 collisionless fermionic atoms coupled to the electromagnetic fields of a ring resonator. The two spin states are two-photon Ramancoupled via a pair of degenerate counterpropagating cavity modes and two transverse pump fields. In this one-dimensional configuration the coupled atom-field system possesses a continuous U(1) translational symmetry and a discrete Z 2 spin inversion symmetry. At half filling for sufficiently strong pump strengths, the combined U(1)×Z 2 symmetry is spontaneously broken at the onset of a superradiant phase transition to a state with self-ordered density and spin structures. We predominately find an antiferromagnetic lattice order at the cavity wavelength. The self-ordered states exhibit unexpected positive momentum pair correlations between fermions with opposite spin. These strong cavity-mediated correlations vanish at higher pump strength.
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