Effects of magnetic order on the upper critical field

J. Sauls*

*Corresponding author for this work

Research output: Contribution to journalArticlepeer-review

18 Scopus citations

Abstract

I present a Ginzburg-Landau theory for hexagonal oscillations of the upper critical field of (Formula presented) near (Formula presented). The model is based on a two-dimensional representation for the superconducting order parameter, η→=((Formula presented),(Formula presented)), coupled to an in-plane antiferromagnetic (AFM) order parameter, m(Formula presented). Hexagonal anisotropy of (Formula presented) arises from the weak in-plane anisotropy energy of the AFM state and the coupling of the superconducting order parameter to the staggered field. The model explains the important features of the observed hexagonal anisotropy [N. Keller et al., Phys. Rev. Lett. 73, 2364 (1994)] including (i) the small magnitude, (ii) persistence of the oscillations for T→(Formula presented), and (iii) the change in sign of the oscillations for T≳(Formula presented) and T<(Formula presented) (the temperature at the tetracritical point). I also show that there is a low-field crossover (observable only very near (Formula presented)) below which the oscillations should vanish.

Original languageEnglish (US)
Pages (from-to)8543-8548
Number of pages6
JournalPhysical Review B - Condensed Matter and Materials Physics
Volume53
Issue number13
DOIs
StatePublished - 1996

ASJC Scopus subject areas

  • Electronic, Optical and Magnetic Materials
  • Condensed Matter Physics

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