Abstract:The superfluid phase transition of the general vortex gas, in which the circulations may be any non-zero integer, is studied. When the net circulation of the system is not zero the absence of a superfluid phase is shown. When the net circulation of the vortices vanishes, the presence of off-diagonal long range order is demonstrated and the existence of an order parameter is proposed. The transition temperature for the general vortex gas is shown to be the Kosterlitz-Thouless temperature. An upper bound for the… Show more
“…The description of the two-dimensional quantum vortices used in [9,15,16,13] and [17] follows in direct analogy with the description of vortex lines used in three-dimensional superfluids. In this description vortices are characterized by {κ i , z i }, where κ i is the circulation associated with the i th vortex at the position z i (in complex coordinates) on a Riemann surface M. Vortices are formed due to a current flow j z in the fluid.…”
Section: Vortices In Two-dimensionsmentioning
confidence: 99%
“…In the phenomenological theory given in [17] the superfluid state is marked by the presence of vortices while the normal fluid state does not have vortices. Consequently, ξ = 1 when T > T c and when T < T c , ξ = 0.…”
Section: Application Of Sheaf Theorymentioning
confidence: 99%
“…There are effectively no free vortices in the superfluid state in this theory. In theory given in [17], on the other hand, vortices are only present in the superfluid state and the phase transition is due to the annihilation of oppositely charged vortices at the transition temperature. In this case, there are no quantum vortices in the normal fluid state.…”
Section: Introductionmentioning
confidence: 99%
“…We do so by using the results from analysing the classical equations of motion for the vortices given in [9,15,16,13] and [17] as a motivation for studying sheaf theory. Results from sheaf theory are then combined with an effective-field description of the system to construct the order parameter.…”
Using results from sheaf theory combined with the phenomenological theory of the two-dimensional superfluid, the precipitation of quantum vortices is shown to be the genesis of a macroscopic order parameter for a phase transition in two dimensions.
“…The description of the two-dimensional quantum vortices used in [9,15,16,13] and [17] follows in direct analogy with the description of vortex lines used in three-dimensional superfluids. In this description vortices are characterized by {κ i , z i }, where κ i is the circulation associated with the i th vortex at the position z i (in complex coordinates) on a Riemann surface M. Vortices are formed due to a current flow j z in the fluid.…”
Section: Vortices In Two-dimensionsmentioning
confidence: 99%
“…In the phenomenological theory given in [17] the superfluid state is marked by the presence of vortices while the normal fluid state does not have vortices. Consequently, ξ = 1 when T > T c and when T < T c , ξ = 0.…”
Section: Application Of Sheaf Theorymentioning
confidence: 99%
“…There are effectively no free vortices in the superfluid state in this theory. In theory given in [17], on the other hand, vortices are only present in the superfluid state and the phase transition is due to the annihilation of oppositely charged vortices at the transition temperature. In this case, there are no quantum vortices in the normal fluid state.…”
Section: Introductionmentioning
confidence: 99%
“…We do so by using the results from analysing the classical equations of motion for the vortices given in [9,15,16,13] and [17] as a motivation for studying sheaf theory. Results from sheaf theory are then combined with an effective-field description of the system to construct the order parameter.…”
Using results from sheaf theory combined with the phenomenological theory of the two-dimensional superfluid, the precipitation of quantum vortices is shown to be the genesis of a macroscopic order parameter for a phase transition in two dimensions.
“…The purpose of this paper, therefore, is to develope a quantum mechanical description of vortices in superfluid 4 He films. There are two approaches that one can take.…”
A quantum mechanical description of vortices in two-dimensional superfluid 4 He films is presented. Single vortex creation and annihilation operators are defined and wavefunctions for these states are explicitly constructed.
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