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arXiv:cond-mat/0610317 · Physical Review A

Miscibility in a degenerate fermionic mixture induced by linear coupling

Sadhan K. Adhikari, Boris A. Malomed

Published Nov 22, 2006• 25 citations
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Abstract

We consider a one-dimensional mean-field-hydrodynamic model of a two-component degenerate Fermi gas in an external trap, each component representing a spin state of the same atom. We demonstrate that the interconversion between them (linear coupling), imposed by a resonant electromagnetic wave, transforms the immiscible binary gas into a miscible state, if the coupling constant, $\ensuremath{\kappa}$, exceeds a critical value, ${\ensuremath{\kappa}}_{\mathrm{cr}}$. The effect is predicted in a variational approximation, and confirmed by numerical solutions. Unlike the recently studied model of a binary Bose-Einsten condensate with the linear coupling, the components in the immiscible phase of the binary fermion mixture never fill two separated domains with a wall between them, but rather form antilocked ($\ensuremath{\pi}$-phase-shifted) density waves. Another difference from the bosonic mixture is spontaneous breaking of symmetry between the two components in terms of the numbers of atoms in them, ${N}_{1}$ and ${N}_{2}$. The latter effect is characterized by the parameter $\ensuremath{\nu}\ensuremath{\equiv}({N}_{1}\ensuremath{-}{N}_{2})∕({N}_{1}+{N}_{2})$ (only ${N}_{1}+{N}_{2}$ is a conserved quantity), the onset of miscibility at $\ensuremath{\kappa}\ensuremath{\geqslant}{\ensuremath{\kappa}}_{\mathrm{cr}}$ meaning a transition to $\ensuremath{\nu}\ensuremath{\equiv}0$. At $\ensuremath{\kappa}<{\ensuremath{\kappa}}_{\mathrm{cr}}$, $\ensuremath{\nu}$ features damped oscillations as a function of $\ensuremath{\kappa}$. We also briefly consider an asymmetric model, with a chemical-potential difference between the two components. The relation between the imbalance in the spin population, induced by the linear coupling, and the developing spatial structure resembles the known Larkin-Ovchinnikov-Fulde-Ferrell states in the Fermi mixture. Dynamical states, when $\ensuremath{\kappa}$ is suddenly switched from zero to a value exceeding ${\ensuremath{\kappa}}_{\mathrm{cr}}$, are considered too. In the latter case, the system features oscillatory relaxation to the mixed state.

DOI
10.1103/physreva.74.053620

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We consider a one-dimensional mean-field-hydrodynamic model of a two-component degenerate Fermi gas in an external trap, each component representing a spin state of the same atom. We demonstrate that the interconversion between them (linear coupling), imposed by a resonant electromagnetic wave, transforms the immiscible binary gas into a miscible state, if the coupling constant, \ensuremathκ\ensuremath{\kappa}\ensuremathκ, exceeds a critical value, \ensuremathκcr{\ensuremath{\kappa}}_{\mathrm{cr}}\ensuremathκcr​. The effect is predicted in a variational approximation, and confirmed by numerical solutions. Unlike the recently studied model of a binary Bose-Einsten condensate with the linear coupling, the components in the immiscible phase of the binary fermion mixture never fill two separated domains with a wall between them, but rather form antilocked (\ensuremathπ\ensuremath{\pi}\ensuremathπ-phase-shifted) density waves. Another difference from the bosonic mixture is spontaneous breaking of symmetry between the two components in terms of the numbers of atoms in them, N1{N}_{1}N1​ and N2{N}_{2}N2​. The latter effect is characterized by the parameter \ensuremathν\ensuremath≡(N1\ensuremath−N2)∕(N1+N2)\ensuremath{\nu}\ensuremath{\equiv}({N}_{1}\ensuremath{-}{N}_{2})∕({N}_{1}+{N}_{2})\ensuremathν\ensuremath≡(N1​\ensuremath−N2​)∕(N1​+N2​) (only N1+N2{N}_{1}+{N}_{2}N1​+N2​ is a conserved quantity), the onset of miscibility at \ensuremathκ\ensuremath⩾\ensuremathκcr\ensuremath{\kappa}\ensuremath{\geqslant}{\ensuremath{\kappa}}_{\mathrm{cr}}\ensuremathκ\ensuremath⩾\ensuremathκcr​ meaning a transition to \ensuremathν\ensuremath≡0\ensuremath{\nu}\ensuremath{\equiv}0\ensuremathν\ensuremath≡0. At \ensuremathκ<\ensuremathκcr\ensuremath{\kappa}<{\ensuremath{\kappa}}_{\mathrm{cr}}\ensuremathκ<\ensuremathκcr​, \ensuremathν\ensuremath{\nu}\ensuremathν features damped oscillations as a function of \ensuremathκ\ensuremath{\kappa}\ensuremathκ. We also briefly consider an asymmetric model, with a chemical-potential difference between the two components. The relation between the imbalance in the spin population, induced by the linear coupling, and the developing spatial structure resembles the known Larkin-Ovchinnikov-Fulde-Ferrell states in the Fermi mixture. Dynamical states, when \ensuremathκ\ensuremath{\kappa}\ensuremathκ is suddenly switched from zero to a value exceeding \ensuremathκcr{\ensuremath{\kappa}}_{\mathrm{cr}}\ensuremathκcr​, are considered too. In the latter case, the system features oscillatory relaxation to the mixed state.
A one-dimensional mean-field model of a two-component condensate in the parabolic trap is considered, with the components corresponding to different spin states of the same atom. We demonstrate that the linear coupling (interconversion) between them, induced by a resonant electromagnetic wave, can drive the immiscible binary condensate into a miscible state. This transition is predicted in an analytical form by means of a variational approximation (for an infinitely long system), and is confirmed by direct numerical solutions of the symmetric and asymmetric models (the asymmetry accounts for a possible difference in the chemical potential between the components). We define an order parameter of the system as an off-centre shift of the centre of mass of each component. A numerically found dependence of the order parameter on the linear-coupling strength reveals a second-kind phase transition (in an effectively finite system). The phase transition looks very similar in two different regimes, namely, with a fixed number of atoms, or a fixed chemical potential. An additional transition is possible between double- and single-humped density distributions in the weak component of a strongly asymmetric system. We also briefly consider dynamical states, with the two components oscillating relative to each other. In this case, the components periodically separate even if they should be mixed in the static configuration.
We consider a model of a two-component condensate in one dimension, where the components represent two different spin states of the same atom. We demonstrate that linear interconversion between them, induced by a resonant electromagnetic wave, can make the immiscible binary condensate miscible. This transition is predicted by means of a variational approximation, and is then confirmed by direct numerical solutions of the symmetric and asymmetric models (the asymmetry is accounted for by a chemical-potentil difference between the components). The dependence of the corresponding order parameters on the linear-coupling strengths reveals a typical phase transition of the second kind. However, in dynamic states the species may remain separated, even if they would get mixed in a static configuration.
We investigate the effects of dipole-dipole (DD) interactions on immiscibility-miscibility transitions (IMT's) in two-component Bose-Einstein condensates (BEC's) trapped in the harmonic-oscillator (HO) potential, with the components linearly coupled by a resonant electromagnetic field (accordingly, the components represent two different spin states of the same atom). The problem is studied by means of direct numerical simulations. Different mutual orientations of the dipolar moments in the two components are considered. It is shown that, in the binary BEC formed by dipoles with the same orientation and equal magnitudes, the IMT cannot be induced by the DD interaction alone, being possible only in the presence of the linear coupling between the components, while the miscibility threshold is affected by the DD interactions. However, in the binary condensate with the two dipolar components polarized in opposite directions, the IMT can be induced without any linear coupling. Further, we demonstrate that those miscible and immiscible localized states, formed in the presence of the DD interactions, which are unstable evolve into robust breathers, which tend to keep the original miscibility or immiscibility, respectively. An exception is the case of a very strong DD attraction, when narrow stationary modes are destroyed by the instability. The binary BEC composed of copolarized dipoles with different magnitudes are briefly considered as well.
We explore a few-body mixture of two bosonic species confined in quasi-one-dimensional parabolic traps of different length scales. The ground-state phase diagrams in the three-dimensional parameter space spanned by the harmonic length scale ratio, interspecies coupling strength, and particle-number ratio are investigated. As a first case study we use the mean-field ansatz (MF) to perform a detailed analysis of the separation mechanism. It allows us to derive a simple and intuitive rule predicting which of the immiscible phases is energetically more favorable at the miscible-immiscible phase boundary. We estimate the critical coupling strength for the miscible-immiscible transition and perform a comparison to correlated many-body results obtained by means of the multilayer multiconfiguration time-dependent Hartree method for bosonic mixtures (ML-X). At a critical ratio of the trap frequencies, determined solely by the particle-number ratio, the deviations between MF and ML-X are very pronounced and can be attributed to a high degree of entanglement between the components. As a result, we evidence the breakdown of the effective one-body picture. Additionally, when many-body correlations play a substantial role, the one-body density is in general not sufficient for deciding upon the phase at hand which we demonstrate exemplarily.
In this Thesis is presented a study on dynamical properties of mixtures of ultraold Bose gases. The behaviour of this system in different regimes is analysed: with and without coherent coupling between the two components, in homogeneous and harmonic shaped trapping potentials and in different dimensions and geometries. Most of the results presented here have been obtained by means of numerical solutions of coupled Gross-Pitaevskii equations and have been compared with theoretical predictions (and sometimes experiments), describing the same phenomena. In particualr the stability of persistent currents in a two-component Bose-Einstein condensate in a toroidal trap is studied in both the miscible and the immiscible regime. In the miscible regime we show that superflow decay is related to linear instabilities of the spin-density Bogoliubov mode. We find a region of partial stability, where the flow is stable in the majority component while it decays in the minority component. We also characterize the dynamical instability appearing for a large relative velocity between the two components. In the immiscible regime the stability criterion is modified and depends on the specific density distribution of the two components. The effect of a coherent coupling between the two components is also discussed. A study on the collective modes of the minority component of a highly unbalanced Bose-Bose mixture is also presented. In the immiscible case we find that the ground state can be a two-domain walls soliton. Although the mode frequencies are continuous at the transition, their behaviour is very different with respect to the miscible case. The dynamical behaviour of the solitonic structure and the frequency dependence on the inter- and intra-species interaction is numerically studied using coupled Gross-Pitaevskii equations. The results of the study on the static and the dynamic response of coherently coupled two component Bose-Einstein condensates due to a spin-dipole perturbation is also sown. The static dipole susceptibility is determined and is shown to be a key quantity to identify the second order ferromagnetic transition occurring at large inter-species interactions. The dynamics, which is obtained by quenching the spin-dipole perturbation, is very much affected by the system being paramagnetic or ferromagnetic and by the correlation between the motional and the internal degrees of freedom. In the paramagnetic phase the gas exhibits well defined out-of-phase dipole oscillations, whose frequency can be related to the susceptibility of the system using a sum rule approach. In particular in the interaction SU (2) symmetric case, when all the two-body interactions are the same, the external dipole oscillation coincides with the internal Rabi flipping frequency. In the ferromagnetic case, where linear response theory is not applicable, the system shows highly non-linear dynamics. In particular we observe phenomena related to ground state selection: the gas, initially trapped in a domain wall configuration, reaches a final state corresponding to the magnetic ground state plus small density ripples. Interestingly, the time during which the gas is unable to escape from its initial configuration is found to be proportional to the square root of the wall surface \ntension.
Attraction of the quantum particle to the center in three-dimensional space with potential $\ensuremath{-}{V}_{0}{r}^{\ensuremath{-}2}$ gives rise to the quantum collapse, i.e., nonexistence of the ground state (GS) when the attraction strength exceeds a critical value [(V0(cr))1=1/8{({V}_{0}^{(\mathrm{cr})})}_{1}=1/8(V0(cr)​)1​=1/8, in the present notation]. Recently, we have demonstrated that the quantum collapse is suppressed and the GS is restored if repulsive interactions between particles in the quantum gas are taken into account in the mean-field approximation. This setting can be realized in a gas of dipolar molecules attracted to the central charge, with dipole-dipole interactions taken into regard as well. Here we analyze this problem for a binary gas. GSs supported by the repulsive interactions are constructed in a numerical form, as well as by means of analytical approximations for both miscible and immiscible binary systems. In particular, the Thomas-Fermi approximation is relevant if V0{V}_{0}V0​ is large enough. It is found that the GS of the miscible binary gas, both balanced and imbalanced, features a weak phase transition at another critical value, ${({V}_{0}^{(\mathrm{cr})})}_{2}=1/2\ensuremath{\equiv}4{({V}_{0}^{(\mathrm{cr})})}_{1}$. The transition is characterized by an analyticity-breaking change in the structure of the wave functions at small rrr. To illustrate the generic character of the present phenomenology, we also consider the binary system with attraction between the species (rather than repulsion) in the case when the central potential pulls a single component only.