A–B transition of superfluid in aerogel under magnetic field
Introduction
Since the discovery of the superfluidity of liquid in aerogel, there has been considerable interest in impurity scattering effects on p-wave superfluid. Clear evidence of the impurity scattering effect has been observed as the reduction of the superfluid transition temperature and the superfluid density. However, the identification of the order parameter structure and the modification of the phase diagram have not yet been established. In the p-wave spin-triplet pairing systems under magnetic field, A-phase with equal-spin pairs is more favorable than the B-phase that has ↑↓+↓↑ pairs as well. Such an A–B transition under magnetic field has been observed in the superfluid phase of in aerogel [1], [2]. Brussaard et al. measured the superfluid density ρs in aerogel under magnetic fields using a vibrating wire technique and found a clear signature of A–B transition as an abrupt change in ρs. Gervais et al. succeeded in detecting multiple phase transitions of the -aerogel system in magnetic fields using high-frequency sound.
In this paper we present a theoretical study of impurity scattering effect on the phase diagram under magnetic field on the basis of the homogeneous impurity model [3]. We calculate the A–B transition line over the whole temperature range using the self-consistent order parameter within the weak coupling theory.
Section snippets
Formulation
Here, we consider the second-order transition from the BW state with d-vector and to the planar state with and dz=0. As long as the energetics of the A–B transition is concerned, it suffices to consider the phase transition between the BW state and the planar state, because the ABM state and the planar state have the same free energy within the weak coupling theory even in the presence of impurities.
We start with the Gor'kov equation including the Zeeman
Numerical results
We calculate the phase diagram using the parameters for liquid in 98% aerogel with [5]. In Fig. 1, we show the second-order A–B transition line in the Born and unitarity limits and compare the result with that of the pure liquid at the same pressure. The transition temperature is substantially suppressed by the impurity scattering. In the unitarity limit, we find no hump behavior at intermediate temperatures. It may happen that in the unitarity limit there is no first
Acknowledgements
This work is supported in part by a Grant-in-Aid for COE Research (No. 13CE2002) from the Ministry of Education, Culture, Sports, Science and Technology of Japan.
References (5)
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