The Equation of State for Cool Relativistic Two-Constituent Superfluid Dynamics
| dc.creator | Carter, Brandon | |
| dc.creator | Langlois, David | |
| dc.date | 1995-07-10 | |
| dc.date.accessioned | 2026-07-07T12:03:49Z | |
| dc.date.available | 2026-07-07T12:03:49Z | |
| dc.description | The natural relativistic generalisation of Landau's two constituent superfluid theory can be formulated in terms of a Lagrangian $L$ that is given as a function of the entropy current 4-vector $s^ρ$ and the gradient $\nablaφ$ of the superfluid phase scalar. It is shown that in the ``cool" regime, for which the entropy is attributable just to phonons (not rotons), the Lagrangian function $L(\vec s, \nablaφ)$ is given by an expression of the form $L=P-3ψ$ where $P$ represents the pressure as a function just of $\nablaφ$ in the (isotropic) cold limit. The entropy current dependent contribution $ψ$ represents the generalised pressure of the (non-isotropic) phonon gas, which is obtained as the negative of the corresponding grand potential energy per unit volume, whose explicit form has a simple algebraic dependence on the sound or ``phonon" speed $c_P$ that is determined by the cold pressure function $P$. | |
| dc.description | 26 pages, RevTeX, no figures, published in Phys. Rev. D. 15 May 1995 | |
| dc.identifier | https://arxiv.org/abs/hep-th/9507058 | |
| dc.identifier | http://arxiv.org/abs/hep-th/9507058 | |
| dc.identifier | Phys.Rev.D51:5855-5864,1995 | |
| dc.identifier | doi:10.1103/PhysRevD.51.5855 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/207917 | |
| dc.subject | High Energy Physics - Theory | |
| dc.subject | General Relativity and Quantum Cosmology | |
| dc.title | The Equation of State for Cool Relativistic Two-Constituent Superfluid Dynamics | |
| dc.type | text |