Theoretical study on loop current phase and non-reciprocal transport in Kagome superconductors
- Datum: 20.02.2025
- Uhrzeit: 14:00 - 15:00
- Vortragende(r): Rina Tazai
- Yukawa Institute for Theoretical Physics, YITP, Kyoto, Japan
- Ort: Max Planck Institute for Solid State Research
- Raum: 4D2
- Gastgeber: Dep. Quantum Many-Body Theory

In the Kagome superconductor AV3Sb5, time-reversal
symmetry breaking has been observed through various experiments
such as μSR, STM, and NMR [1]. One of the possible origins for
this is the loop current (LC) order (often referred to as iCDW).
The order parameter of LC is described as a symmetry-breaking part
of the self-energy of the electronic system. In Hermitian systems,
it can be simply expressed as the pure imaginary hopping term. The
orbital magnetization induced by such LC is expected to be very
small , making direct experimental observation difficult.
One key experiment for indicating the LC is the nonlinear
response [2] in 2022. They measured the non-reciprocal voltage,
which is proportional to the square of the electric field E, it
was found that the resistivity is proportional to the magnetic
field Bx and Jz. Furthermore, it was
discovered that the resistivity is proportional to Bz,
which was traditionally considered a material-dependent constant,
jumps depending on the Bz. Such a jump
behavior cannot be accounted for in the conventional polar-type
nonlinear response theory (please refer to [3]). In this study
[5], we start from the Boltzmann equation under the LC order and
go beyond the conventional approximation by considering
higher-order terms in relaxation-time [4], developing a
theoretical formula for this jump-type nonlinear response. As a
result, we found that the jump term, which could not be explained
by the conventional Drude term, can be explained by the
higher-order term. Furthermore, by applying the obtained formula
to a two-orbital 12-site Kagome model and performing numerical
analysis, we found that the dominant component of the nonlinear
conductivity is large at band crossing points, and even larger at
points where the orbital character changes sharply. This behavior
can be understood using the concept of quantum geometry, where the
conductivity resonates with the LC gap size. (The present
nonlinear conductivity is considers as "quasi"-quantum geometry,
as its dimension differs by the 1/E.)
[1] C. Mielke et al., Nature 602, 245 (2022)
[2] C. Guo et al.,
Nature 611, 461 (2022)
[3] Y. Tokura, et al., Nat. Commun.9, 3740 (2018)
[4] X. Liu et
al., arXiv: 2303.10164 (2023)
[5] R. Tazai et al., arXiv:2408.04233