LPTMC Seminars

Salle 523, couloir 12-13, 5è étage

Collective dynamics in binary superfluids: From dissipationless flow to dispersive shock waves

Binary superfluids are typically characterized by two distinct internal states, giving rise to a spin mode in addition to the conventional density mode. These systems can be realized, for example, using Bose-Einstein condensation into two hyperfine atomic states, or the propagation of a two-polarization laser in a birefringent nonlinear medium. In this talk, I will mainly present two theoretical investigations into collective phenomena in these systems. First, inspired by a recent experiment at LKB [1], I will discuss the critical speed for dissipationless flow of a two-dimensional binary superfluid of light past an impurity [2]. For a weak impurity, the drag is determined within linear-response theory and aligns with Landau’s criterion. For an impurity of arbitrary strength, the critical speed is obtained from the conditions for strong ellipticity of the stationary flow equations. We identify the emission of linear waves and vortex structures in the density and spin sectors as primary mechanisms for dissipative flow. Second, I will examine a coherently driven binary Bose-Einstein condensate, inspired by an experiment at Institut d’optique [3]. In its ground state, this system can be effectively described by a single coherent field satisfying the cubic-quintic nonlinear Schrodinger equation. In a one-dimensional geometry, we investigate nonlinear periodic solutions arising from steplike initial conditions. Using modulation theory, we analyze contact dispersive shock waves [4], nonlinear structures that are fundamentally absent in the standard, cubic nonlinear Schrodinger framework. To conclude, I will briefly complement these results by looking toward simpler, single-component systems, to highlight a recent experimental result at LKB [5, 6]: the observation that a finite-mass impurity can self-propel against a two-dimensional superfluid flow via vortex-antivortex shedding. Reducing the impurity to its center of mass and using a point-vortex model, I will describe how quantized vortices can serve as momentum-transfer agents, effectively bridging the physics of quantum fluids with the field of active matter.

[1] C. Piekarski, N. Cherroret, T. Aladjidi, and Q. Glorieux, Spin and density modes in a binary fluid of light, Phys. Rev. Lett. 134, 223403 (2025).
[2] P.-E. Larré, C. Michel, and N. Cherroret, Critical speed of a binary superfluid of light (2026).
[3] A. Hammond, L. Lavoine, and T. Bourdel, Tunable three-body interactions in driven two-component Bose-Einstein condensates, Phys. Rev. Lett. 128, 083401 (2022).
[4] T. Congy, P.-E. Larré, and P. Sprenger, Modulation theory for cubic-quintic nonlinear Schrodinger equations (2026).
[5] M. Baker-Rasooli, T. Aladjidi, T. D. Ferreira, A. Bramati, M. Albert, P.-E. Larré, and Q. Glorieux, Swimming against a superfluid flow: Self-propulsion via vortex-antivortex shedding in a quantum fluid of light, arXiv:2512.09028 (2025).
[6] T. Aladjidi, M. Baker-Rasooli, T. D. Ferreira, A. Bramati, M. Albert, P.-E. Larré, and Q. Glorieux, Critical velocity of a flow of superfluid light past a finite-mass impurity of tunable width (2026).