Sensitivity of the Superconducting Transition Temperature to Changes in the Spin-Fluctuation Spectral Weight

Abstract

In the simplest model of magnetic pairing, the transition temperature to the superconducting state depends on the dynamical susceptibility $\chi (\mathbf{q},\omega )$. We discuss how $T_c$ is affected by different momentum and frequency parts of $\chi (\mathbf{q},\omega )$ for nearly antiferromagnetic and nearly ferromagnetic metals in two dimensions. While in the case of phonon-mediated superconductivity any addition of spectral weight to ${\alpha }^{2}F(\omega )$ at $\omega >0$ leads to an increase in $T_c$, we find that adding magnetic spectral weight at any momentum $\mathbf{q}$ and low frequencies ($[0:3T_c]$ and $[0:(5-9)T_c]$ for nearly antiferromagnetic and ferromagnetic metals respectively) leads to a suppression of $T_c$. The most effective frequency and momentum range consists of large momenta $\mathbf{q}\sim (\pi ,\pi )$ and frequencies around $10T_c$ for nearly antiferromagnetic metals and small momenta $\mathbf{q}\sim 0$ and frequencies of approximately $(13-22)T_c$ for nearly ferromagnetic metals.

arXiv comment18 pages, 39 figures

References in corpus (3)

• p-wave and d-wave superconductivity in quasi-two-dimensional metals
• Spin-fluctuation exchange study of superconductivity in two- and three-dimensional single-band Hubbard models
• d- and p-wave superconductivity mediated by spin fluctuations in two- and three-dimensional single-band repulsive Hubbard model

Cited by in corpus (2)

• Strong correlation between ferromagnetic superconductivity and pressure-enhanced ferromagnetic fluctuations in UGe${}_2$
• Superconductivity in heavy fermion compounds