TY - JOUR
T1 - Nonreciprocal thermal and thermoelectric transport of electrons in noncentrosymmetric crystals
AU - Nakai, Ryota
AU - Nagaosa, Naoto
N1 - Funding Information:
R.N. was supported by JSPS KAKENHI Grant No. JP17K17604 and the RIKEN Special Postdoctoral Researcher Program. N.N. was supported by JST CREST Grants No. JPMJCR1874 and No. JPMJCR16F1, and JSPS KAKENHI Grants No. JP18H03676 and No. JP26103006.
Publisher Copyright:
© 2019 American Physical Society.
PY - 2019/3/4
Y1 - 2019/3/4
N2 - Nonreciprocal transport phenomena indicate that the forward and backward flows differ and are attributed to broken inversion symmetry. In this paper, we study the nonreciprocity of the thermal and thermoelectric transport of electronic systems resulting from inversion-symmetry-broken crystal structures. The nonlinear electric, thermoelectric, and thermal conductivities are derived up to the second order in an electric field and a temperature gradient by using the Boltzmann equation with the relaxation time approximation. All the second-order conductivities appearing in this paper are described by two functions and their derivatives, and they are related to each other in the same way that linear conductivities are, e.g., via the Wiedemann-Franz law. We found that nonvanishing thermal-transport coefficients in the zero-temperature limit appear in nonlinear conductivities, which dominate the thermal transport at a sufficiently low temperature. The nonlinear conductivities and possible observable quantities are estimated in a 1H monolayer of the transition-metal dichalcogenide MoS2 and a polar semiconductor BiTeX (X=I,Br).
AB - Nonreciprocal transport phenomena indicate that the forward and backward flows differ and are attributed to broken inversion symmetry. In this paper, we study the nonreciprocity of the thermal and thermoelectric transport of electronic systems resulting from inversion-symmetry-broken crystal structures. The nonlinear electric, thermoelectric, and thermal conductivities are derived up to the second order in an electric field and a temperature gradient by using the Boltzmann equation with the relaxation time approximation. All the second-order conductivities appearing in this paper are described by two functions and their derivatives, and they are related to each other in the same way that linear conductivities are, e.g., via the Wiedemann-Franz law. We found that nonvanishing thermal-transport coefficients in the zero-temperature limit appear in nonlinear conductivities, which dominate the thermal transport at a sufficiently low temperature. The nonlinear conductivities and possible observable quantities are estimated in a 1H monolayer of the transition-metal dichalcogenide MoS2 and a polar semiconductor BiTeX (X=I,Br).
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U2 - 10.1103/PhysRevB.99.115201
DO - 10.1103/PhysRevB.99.115201
M3 - Article
AN - SCOPUS:85062715522
SN - 2469-9950
VL - 99
JO - Physical Review B
JF - Physical Review B
IS - 11
M1 - 115201
ER -