2020
DOI: 10.1103/physrevb.101.100407
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Spin Seebeck effect in Cu2OSeO3 : Test of bulk magnon spin current theory

Abstract: We report measurements of the low-temperature (T ≤ 15 K) longitudinal spin-Seebeck coefficient (SLSSE) in bulk single-crystals of the helimagnetic insulator Cu2OSeO3 with Pt contacts. Simultaneous measurement of both SLSSE and the magnon thermal conductivity (κm) demonstrates their correlation and allows for quantitative and favorable comparison to bulk magnon spin-current theory.

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Cited by 9 publications
(6 citation statements)
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“…A quantitative disentanglement of these spurious signals is therefore necessary in order to extract the intrinsic LSSE contribution . Other effects such as an electronically/magnetically coupled structural phase transition, phase coexistence, , and surface magnetization ,, on the SSE have also been reported in various systems but have yet to be understood. It is therefore essential to find a magnetic system within which the effects can be investigated systematically.…”
Section: Introductionmentioning
confidence: 99%
“…A quantitative disentanglement of these spurious signals is therefore necessary in order to extract the intrinsic LSSE contribution . Other effects such as an electronically/magnetically coupled structural phase transition, phase coexistence, , and surface magnetization ,, on the SSE have also been reported in various systems but have yet to be understood. It is therefore essential to find a magnetic system within which the effects can be investigated systematically.…”
Section: Introductionmentioning
confidence: 99%
“…This could be due to the nature of the thermal spin signal observed from bulk magnetic materials, which have been found in other systems. [ 40,41 ]…”
Section: Resultsmentioning
confidence: 99%
“…This could be due to the nature of the thermal spin signal observed from bulk magnetic materials, which have been found in other systems. [40,41] It is most universally informative to present the transverse thermopower data in terms of transverse electric field per unit heat flux through the device cross-section. This helps avoid errors introduced by assumptions made about the actual temperature drop across the active device, [42,43] especially in a setup where the temperature of the Cu blocks is measured, as in this work.…”
Section: Resultsmentioning
confidence: 99%
“…in Figure 2 in the previous review article (2). Recent updates include ferromagnetic EuO (15), two-dimensional (2D) ferromagnetic Cr2Si2Te6, Cr2Ge2Te6 (16,17), ferrimagnetic garnet ferrites R3Fe5O12 (R = Eu, Tb, Dy, Tm) (18,19,20), Y3−xRxFe5O12 with R being 14 rare-earth elements from La to Lu (except for Pm) (21), Lu2Bi1Fe4Ga1O12 (22), spinel ferrites ZnFe2O4 (23), γ-Fe2O3 (24), LiFe5O8 (25), Ni0.65Zn0.35Al0.8Fe1.2O4 (26), Mg 0.5−δ Mn0.5Fe2O4 (27), Y-type hexagonal ferrites Ba2Co2Fe12O22, Ba2Zn2Fe12O22 (28), orthorhombic ferrimagnetic ε-Fe2O3 (29), molecular-based ferrimagnetic Cr II [Cr III (CN)6] (30), various antiferromagnetic (AF) insulators such as NiO (31,32,33,34), FeF2 (35), α-Fe2O3 (36,37), MnCO3 (38), α-Cu2V2O7 (39), SrFeO3 (40), SrMnO3 (41), DyFeO3 (42), and other intriguing materials including a chiral helimagnet Cu2OSeO3 with a skyrmion lattice phase (43,44) and quantum magnets Sr2CuO3 (45,46), CuGeO3 (47), Pb2V3O9 (48), LiCuVO4 (49). In particular, the ferrimagnetic insulator YIG has been essential (1,2), as it exhibits the lowest magnetic damping, high Curie temperature (TC ∼ 560 K), and high resistivity and also is a playground to reveal the role of magnon polarization in SSEs (see Section 6).…”
Section: Introductionmentioning
confidence: 99%