Volovik effect in the ±\pms-wave state for the iron-based superconductors

preprint2010arXivOpen access

Abstract

We studied the field dependencies of specific heat coefficient γ(H)=lim⁡T→0C(T,H)/Tγ(H) = \lim_{T \rightarrow 0} C(T,H)/T and thermal conductivity coefficient lim⁡T→0κ(T,H)/T\lim_{T \rightarrow 0} κ(T ,H)/T of the ±\pms-wave state in the mixed state. We found that it is a generic feature of the two band s-wave state with the unequal sizes of gaps, small ΔSΔ_S and large ΔLΔ_L, that Doppler shift of the quasiparticle excitations (Volovik effect) creates a finite density of states, on the extended states outside of vortex cores, proportional to HH in contrast to the H\sqrt{H} dependence of the d-wave state. Impurity scattering effect on the ±\pms-wave state, however, makes this generic HH-linear dependence sublinear approaching to the H\sqrt{H} behavior. Our calculations of lim⁡T→0κ(T,H)/T\lim_{T \rightarrow 0} κ(T ,H)/T successfully fit the experimental data of Ba(Fe1−x_{1-x}Cox)2_x )_2 As2_2 with different Co-doping xx by systematically varying the gap size ratio R=∣ΔS∣/∣ΔL∣R= |Δ_S | / |Δ_L |. We also resolve the dilemma of a substantial value of γ(H→0)γ(H \rightarrow 0) but almost zero value of lim⁡T→0κ(T,H→0)/T\lim_{T \rightarrow 0} κ(T ,H \rightarrow 0)/T, observed in experiments.

Explore this paper’s authors, topics and related work.

Building this map preview

BZPEER is loading the nearby papers, people, topics and institutions for this page.

Reviews 0

Write a reviewWrite

No reviews yet.

Discussion 0

Add a commentWrite

No comments yet.