Abstract:We use classical field simulations of the homogeneous Bose gas to study the breakdown of superflow due to vortex nucleation past a cylindrical obstacle at finite temperature. Thermal fluctuations modify the vortex nucleation from the obstacle, turning anti-parallel vortex lines (which would be nucleated at zero temperature) into wiggly lines, vortex rings and even vortex tangles. We find that the critical velocity for vortex nucleation decreases with increasing temperature, and scales with the speed of sound o… Show more
“…14 . Finally, the fundamental problem of vortex nucleation due to fast impurities has been thoroughly investigated at zero temperature [11][12][13] , but few results are known in the finite temperature regime 51,52 . In particular, the PGP model coupled with impurities (1) would be a suitable framework to address the impurity-vortex interaction at non-zero temperature.…”
The dynamics of an active, finite-size and immiscible impurity in a dilute quantum fluid at finite temperature is characterized by means of numerical simulations of the projected Gross-Pitaevskii equation. The impurity is modeled as a localized repulsive potential and described with classical degrees of freedom. It is shown that impurities of different sizes thermalize with the fluid and undergo a stochastic dynamics compatible with an Ornstein-Uhlenbeck process at sufficiently large time-lags. The velocity correlation function and the displacement of the impurity are measured and an increment of the friction with temperature is observed. Such behavior is phenomenologically explained in a scenario where the impurity exchanges momentum with a dilute gas of thermal excitations, experiencing an Epstein drag.
“…14 . Finally, the fundamental problem of vortex nucleation due to fast impurities has been thoroughly investigated at zero temperature [11][12][13] , but few results are known in the finite temperature regime 51,52 . In particular, the PGP model coupled with impurities (1) would be a suitable framework to address the impurity-vortex interaction at non-zero temperature.…”
The dynamics of an active, finite-size and immiscible impurity in a dilute quantum fluid at finite temperature is characterized by means of numerical simulations of the projected Gross-Pitaevskii equation. The impurity is modeled as a localized repulsive potential and described with classical degrees of freedom. It is shown that impurities of different sizes thermalize with the fluid and undergo a stochastic dynamics compatible with an Ornstein-Uhlenbeck process at sufficiently large time-lags. The velocity correlation function and the displacement of the impurity are measured and an increment of the friction with temperature is observed. Such behavior is phenomenologically explained in a scenario where the impurity exchanges momentum with a dilute gas of thermal excitations, experiencing an Epstein drag.
“…The GPE is conventionally used to model a zero temperature condensate, but it is now established that, provided the modes of the gas are highly occupied, the gas evolves as an ensemble of modes, each of which follows (to leading order) the classical trajectory described by the GPE [21][22][23]. Various phenomena have been studied within this classical field formalism, including equilibration dynamics [12,13,15,24], critical temperatures [25], correlation functions [26], vortex nucleation [27][28][29][30] and decay of vortex rings [31], as well as extensions to binary condensates [32][33][34].…”
Using the classical field method, we study numerically the characteristics and decay of the turbulent tangle of superfluid vortices which is created in the evolution of a Bose gas from highly nonequilibrium initial conditions. By analysing the vortex line density, the energy spectrum and the velocity correlation function, we determine that the turbulence resulting from this effective thermal quench lacks the coherent structures and the Kolmogorov scaling; these properties are typical of both ordinary classical fluids and of superfluid helium when driven by grids or propellers. Instead, thermal quench turbulence has properties akin to a random flow, more similar to another turbulent regime called ultra-quantum turbulence which has been observed in superfluid helium.
“…As the shedding of vortices causes the depletion of the condensate fraction, we would expect the presence of thermal effects to lower the critical velocity [15] which in turn would lead to the nucleation of more vortices, until the condensate is depleted. In fact, since the long term behaviour of the condensate fraction is to equilibriate, we deduce that the system stops shedding vortices.…”
Section: The Velocity Of the Condensate And Non-condensate Modesmentioning
confidence: 99%
“…As the velocity of the flow around the obstacle increases, there is a transition from the regular shedding of vortex dipole pairs to an irregular shedding of larger clusters of same-sign vortices, indicating that the system has become turbulent [3,12]. The transition to turbulence in superfluid flow past a potential obstacle has been the focus of recent theoretical [2,3,[13][14][15][16] and experimental [11,12,17,18] work. These works have investigated the effect of obstacle shape [14,19,20] and finite temperature effects [15,16] on the critical velocity for vortex nucleation past a single obstacle.…”
Section: Introductionmentioning
confidence: 99%
“…The transition to turbulence in superfluid flow past a potential obstacle has been the focus of recent theoretical [2,3,[13][14][15][16] and experimental [11,12,17,18] work. These works have investigated the effect of obstacle shape [14,19,20] and finite temperature effects [15,16] on the critical velocity for vortex nucleation past a single obstacle.…”
Superfluid flow past a potential barrier is a well studied problem in ultracold Bose gases, however, fewer studies have considered the case of flow through a disordered potential. Here we consider the case of a superfluid flowing through a channel containing multiple point-like barriers, randomly placed to form a disordered potential. We begin by identifying the relationship between the relative position of two point-like barriers and the critical velocity of such an arrangement. We then show that there is a mapping between the critical velocity of a system with two obstacles, and a system with a large number of obstacles. By establishing an initial superflow through a point-like disordered potential, moving faster than the critical velocity, we study how the superflow is arrested through the nucleation of vortices and the breakdown of superfluidity, a problem with interesting connections to quantum turbulence and coarsening. We calculate the vortex decay rate as the width of the barriers is increased, and show that vortex pinning becomes a more important effect for these larger barriers.
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