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2016
DOI: 10.1103/physreva.93.023640
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Critical velocity for vortex nucleation in a finite-temperature Bose gas

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

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Cited by 11 publications
(9 citation statements)
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“…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.…”
Section: Discussionmentioning
confidence: 99%
“…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.…”
Section: Discussionmentioning
confidence: 99%
“…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].…”
Section: Classical Field Methodsmentioning
confidence: 99%
“…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%
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