Phase Transitions Driven by Vortices in 2D Superfluids and Superconductors: From Kosterlitz-Thouless to 1st Order

Abstract

The Landau-Ginzburg-Wilson hamiltonian is studied for different values of the parameter $\lambda$ which multiplies the quartic term (it turns out that this is equivalent to consider different values of the coherence length $\xi$ in units of the lattice spacing $a$). It is observed that amplitude fluctuations can change dramatically the nature of the phase transition: for small values of $\lambda$ ($\xi /a>0.7$), instead of the smooth Kosterlitz-Thouless transition there is a {\em first order} transition with a discontinuous jump in the vortex density $v$ and a larger non-universal drop in the helicity modulus. In particular, for $\lambda$ sufficiently small ($\xi /a\cong 1$), the density of bound pairs of vortex-antivortex below $T_c$ is so low that, $v$ drops to zero almost for all temperature $T<Tc$.

8 pages, 5 .eps figures

References in corpus (2)

• Vanishing of phase coherence in underdoped Bi_2Sr_2CaCu_2O_8+d
• First Order Transition in the Ginzburg-Landau Model

Cited by in corpus (4)

• Provable first-order transitions for liquid crystal and lattice gauge models with continuous symmetries
• Nature of Phase Transitions in a Generalized Complex |psi|^4 Model
• The Effect of Large Amplitude Fluctuations in the Ginzburg-Landau Phase Transition
• A vortex description of the first-order phase transition in type-I superconductors