spin seebeck effect
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AIP Advances ◽  
2022 ◽  
Vol 12 (1) ◽  
pp. 015320
Author(s):  
Ruchipas Bavontaweepanya ◽  
Yingyot Infahsaeng ◽  
Ekkarat Pongophas ◽  
Wasan Maiaugree ◽  
Piyawat Piyasin ◽  
...  

2021 ◽  
Vol 127 (27) ◽  
Author(s):  
Zhong Shi ◽  
Qing Xi ◽  
Junxue Li ◽  
Yufei Li ◽  
Mohammed Aldosary ◽  
...  

2021 ◽  
Vol 130 (22) ◽  
pp. 223902
Author(s):  
Guang-Qing Li ◽  
Zhen-Gang Zhu ◽  
Gang Su

Author(s):  
fayuan zhang ◽  
Yuxi Qiao ◽  
Jiajia Wang ◽  
Wenjing Liu ◽  
Shan Qiao

Abstract Magnon-phonon thermal relaxation holds a fundamental role in condensed matter physics, and the difference between local phonon and magnon temperature ΔTmp as an important part of this subfield was theoretically considered responsible for the spin Seebeck effect. Experimental determination of ΔTmp is necessary to give more insight into magnon-phonon coupling. Here we report spatially resolved measurements of magnon temperature performed by magneto-optic Kerr effect in yttrium iron garnet. Our results indicate a strong interaction between magnon and phonon subsystems in YIG with an upper limit of the phonon-magnon thermal relaxation length of 1.4 mm, and means this method is valid.


2021 ◽  
Vol 13 (37) ◽  
pp. 45097-45104
Author(s):  
Won-Yong Lee ◽  
No-Won Park ◽  
Min-Sung Kang ◽  
Gil-Sung Kim ◽  
Young-Gui Yoon ◽  
...  

2021 ◽  
Vol 9 ◽  
Author(s):  
Lian-Liang Sun ◽  
Zhen-Guo Fu

Properties of spin Seebeck effect (SSE) in a quantum dot (QD) connected to a topological superconductor or semiconductor nanowire with strong spin-orbit interaction are theoretically studied by the noneqilibrium Green’s function method combined with Dyson equation technique. At low temperatures, Majorana zero modes (MZMs) are prepared at the ends of topological superconductor or semiconductor nanowire, and are hybridized to the QD with spin-dependent strength. We consider that the QD is coupled to two leads in the presence of spin heat accumulation (SHA), i.e., spin-dependent temperature in the leads. We find that the thermopower is spin-polarized when the hybridization strength between the QD and one mode of the MZMs depends on electron spin direction, and its spin-polarization can be effectively adjusted by changing the magnitude of SHA. By proper variation of the spin-polarization of the QD-MZM hybridization strength, magnitude of the SHA, dot level, or the direct coupling between the MZMs, 100% spin-polarized or pure thermopower can be generated. Our results may find real usage in high efficiency spintronic devices or detection of the MZMs, which are under current extensive study. The present model is within the reach of current nano-technologies and may by used in high efficiency spin caloritronics devices.


2021 ◽  
Vol 12 (1) ◽  
Author(s):  
Yao Chen ◽  
Masahiro Sato ◽  
Yifei Tang ◽  
Yuki Shiomi ◽  
Koichi Oyanagi ◽  
...  

AbstractA triplon refers to a fictitious particle that carries angular momentum S=1 corresponding to the elementary excitation in a broad class of quantum dimerized spin systems. Such systems without magnetic order have long been studied as a testing ground for quantum properties of spins. Although triplons have been found to play a central role in thermal and magnetic properties in dimerized magnets with singlet correlation, a spin angular momentum flow carried by triplons, a triplon current, has not been detected yet. Here we report spin Seebeck effects induced by a triplon current: triplon spin Seebeck effect, using a spin-Peierls system CuGeO3. The result shows that the heating-driven triplon transport induces spin current whose sign is positive, opposite to the spin-wave cases in magnets. The triplon spin Seebeck effect persists far below the spin-Peierls transition temperature, being consistent with a theoretical calculation for triplon spin Seebeck effects.


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