Nuclear spin relaxation rate near the disorder-driven quantum critical point in Weyl fermion systems
Nuclear spin relaxation rate near the disorder-driven quantum critical point in Weyl fermion systems
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DOI:
10.1103/physrevb.101.155103
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发表时间:
2019-12
影响因子:
3.7
通讯作者:
Tomoki Hirosawa;H. Maebashi;M. Ogata
中科院分区:
文献类型:
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作者:
Tomoki Hirosawa;H. Maebashi;M. Ogata
Disorder such as impurities and dislocations in Weyl semimetals drives a quantum critical point (QCP) where the density of states at the Weyl point gains a nonzero value. Near the QCP, the asymptotic low-energy singularities of physical quantities are controlled by the critical exponents $\ensuremath{\nu}$ and $z$. The nuclear spin-lattice relaxation rate, which originates from the hyperfine coupling between a nuclear spin and long-range orbital currents in Weyl fermion systems, shows intriguing critical behavior. Based on the self-consistent Born approximation for impurities, we study the nuclear spin-lattice relaxation rate $1/{T}_{1}$ due to the orbital currents in disordered Weyl SMs. We find that ${({T}_{1}T)}^{\ensuremath{-}1}\ensuremath{\sim}{E}^{2/z}$ at the QCP where $E$ is the maximum of temperature $T$ and chemical potential $\ensuremath{\mu}(T)$ relative to the Weyl point. This scaling behavior of ${({T}_{1}T)}^{\ensuremath{-}1}$ is also confirmed by the self-consistent $T$-matrix approximation, where a remarkable temperature dependence of $\ensuremath{\mu}(T)$ could play an important role. We hope these results of ${({T}_{1}T)}^{\ensuremath{-}1}$ will serve as an impetus for exploration of the disorder-driven quantum criticality in Weyl materials.