The 68th JSAP Spring Meeting 2021

Presentation information

Oral presentation

10 Spintronics and Magnetics » 10.1 Emerging materials in spintronics and magnetics (including fabrication and characterization methodologies)

[16p-Z19-1~23] 10.1 Emerging materials in spintronics and magnetics (including fabrication and characterization methodologies)

Tue. Mar 16, 2021 1:00 PM - 7:30 PM Z19 (Z19)

Takashi Komine(Ibaraki Univ.), Hiroaki Sukegawa(NIMS), Tetsuya Hajiri(名大), Ryo Iguchi(物材機構)

1:15 PM - 1:30 PM

[16p-Z19-2] Seebeck-driven Colossal Transverse Thermoelectric Generation

Weinan Zhou1, Kaoru Yamamoto1, Asuka Miura1, Ryo Iguchi1, Yoshio Miura1,2, Ken-ichi Uchida1,3,4, Yuya Sakuraba1,5 (1.NIMS, 2.CSRN, Osaka Univ., 3.IMR, Tohoku Univ., 4.CSRN, Tohoku Univ., 5.JST PRESTO)

Keywords:transverse thermoelectric generation, anomalous Nernst effect, Heusler alloy

The anomalous Nernst coefficient (SANE) can be separated into two components as SANE = ρxxαxyρAHEαxx, where ρxx is the longitudinal resistivity, ρAHE is the anomalous Hall resistivity, and αxx and αxy are the diagonal and off-diagonal components of the Peltier tensor, respectively. The second term on the right hand side can be rewritten as – SSE × ρAHE / ρxx, indicating it originates from the anomalous Hall effect (AHE) of the longitudinal carrier flow induced by SE, and SSE is the Seebeck coefficient. Here, inspired by the second term, we propose a different approach for transverse thermoelectric generation. We consider a system that consists of a thermoelectric material and a magnetic material electrically connected at both ends along the ∇T direction to form a closed circuit. The large electric field generated by SE of the thermoelectric material was converted to transverse thermoelectric generation by AHE of the magnetic material, which showed a similar symmetry to anomalous Nernst effect, but surprisingly, potential for a colossal enhancement in thermopower. This is referred to as the Seebeck-driven transverse thermoelectric generation (STTG).