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Observation of the Spin Seebeck Effect in Bi 2 Te 3 Topological Insulator without an External Magnetic Field
Author(s) -
Yoon ImTaek,
Kim JinSang,
Cho HakDong,
Cho Sangeun,
Yuldashev Shavkat U.
Publication year - 2020
Publication title -
physica status solidi (rrl) – rapid research letters
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.786
H-Index - 68
eISSN - 1862-6270
pISSN - 1862-6254
DOI - 10.1002/pssr.202000004
Subject(s) - topological insulator , condensed matter physics , seebeck coefficient , thermoelectric effect , physics , spin polarization , magnetic field , spin hall effect , electron , spin (aerodynamics) , semiconductor , topology (electrical circuits) , materials science , quantum mechanics , mathematics , combinatorics , thermodynamics
The 3D topological insulator Bi 2 Te 3 is a well‐known semiconductor material with a large Seebeck coefficient, and it is widely used in thermoelectric generators. The spin‐momentum‐locked surface states in topological insulator induce electronic spin polarization which may be used for spin generation and accumulation. Under a temperature gradient, the accumulation of surface electrons with opposite spin directions at the hot and cold sides of the sample will occur. Thus, the spin Seebeck effect (SSE) is detected through the inverse spin Hall effect in heavy metal Pt electrodes with a strong spin–orbit interaction. The SSE is observed in the topological insulator Bi 2 Te 3 without application of an external magnetic field. The spin Seebeck coefficient in the Bi 2 Te 3 topological insulator increases with increasing surface disorder, which is explained via the Dyakonov–Perel mechanism of the spin relaxation time.