TY - JOUR
T1 - Multiple intertwined pairing states and temperature-sensitive gap anisotropy for superconductivity at a nematic quantum-critical point
AU - Klein, Avraham
AU - Wu, Yi Ming
AU - Chubukov, Andrey V.
N1 - Publisher Copyright:
© 2019, The Author(s).
PY - 2019/12/1
Y1 - 2019/12/1
N2 - The proximity of many strongly correlated superconductors to density-wave or nematic order has led to an extensive search for fingerprints of pairing mediated by dynamical quantum-critical (QC) fluctuations of the corresponding order parameter. Here we study anisotropic s-wave superconductivity induced by anisotropic QC dynamical nematic fluctuations. We solve the non-linear gap equation for the pairing gap Δ (θ, ωm) and show that its angular dependence strongly varies below Tc. We show that this variation is a signature of QC pairing and comes about because there are multiple s-wave pairing instabilities with closely spaced transition temperatures Tc , n. Taken alone, each instability would produce a gap Δ (θ, ωm) that changes sign 8 n times along the Fermi surface. We show that the equilibrium gap Δ (θ, ωm) is a superposition of multiple components that are nonlinearly induced below the actual Tc= Tc , 0, and get resonantly enhanced at T=Tc,nm). This variation progressively disappears away from a QC point.
AB - The proximity of many strongly correlated superconductors to density-wave or nematic order has led to an extensive search for fingerprints of pairing mediated by dynamical quantum-critical (QC) fluctuations of the corresponding order parameter. Here we study anisotropic s-wave superconductivity induced by anisotropic QC dynamical nematic fluctuations. We solve the non-linear gap equation for the pairing gap Δ (θ, ωm) and show that its angular dependence strongly varies below Tc. We show that this variation is a signature of QC pairing and comes about because there are multiple s-wave pairing instabilities with closely spaced transition temperatures Tc , n. Taken alone, each instability would produce a gap Δ (θ, ωm) that changes sign 8 n times along the Fermi surface. We show that the equilibrium gap Δ (θ, ωm) is a superposition of multiple components that are nonlinearly induced below the actual Tc= Tc , 0, and get resonantly enhanced at T=Tc,nm). This variation progressively disappears away from a QC point.
UR - http://www.scopus.com/inward/record.url?scp=85074847407&partnerID=8YFLogxK
U2 - 10.1038/s41535-019-0192-x
DO - 10.1038/s41535-019-0192-x
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AN - SCOPUS:85074847407
SN - 2397-4648
VL - 4
JO - npj Quantum Materials
JF - npj Quantum Materials
IS - 1
M1 - 55
ER -