4.8 Article

Utilization of the Antiferromagnetic IrMn Electrode in Spin Thermoelectric Devices and Their Beneficial Hybrid for Thermopiles

Journal

ADVANCED FUNCTIONAL MATERIALS
Volume 26, Issue 30, Pages 5507-5514

Publisher

WILEY-V C H VERLAG GMBH
DOI: 10.1002/adfm.201505514

Keywords

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Funding

  1. National Research Foundation of Korea (NRF) - Ministry of Science, ICT & Future Planning [NRF-2015M3D1A1070465, 2014R1A2A1A11051344, 2013R1A4A1069528]
  2. Ministry of Education, Science, and Technology [NRF-2013R1A1A2011103, 2013R1A2A2A01067144]
  3. National Research Foundation of Korea [2015M3D1A1070465, 2014R1A2A1A11051344, 2013R1A4A1069528, 2013R1A2A2A01067144, 2013R1A1A2011103] Funding Source: Korea Institute of Science & Technology Information (KISTI), National Science & Technology Information Service (NTIS)

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The thermoelectric effect in various magnetic systems, in which electric voltage is generated by a spin current, has attracted much interest owing to its potential applications in energy harvesting, but its power generation capability has to be improved further for actual applications. In this study, the first instance of the formation of a spin thermopile via a simplified and straightforward method which utilizes two distinct characteristics of antiferromagnetic IrMn is reported: the inverse spin Hall effect and the exchange bias. The former allows the IrMn efficiently to convert the thermally induced spin current into a measurable voltage, and the latter can be used to control the spin direction of adjacent ferromagnetic materials. It is observed that a thermoelectric signal is successfully amplified in spin thermopiles with exchange-biased IrMn/CoFeB structures, where an alternating magnetic alignment is formed using the IrMn thickness dependence of the exchange bias. The scalable signal on a number of thermopiles allowing a large-area application paves the way toward the development of practical spin thermoelectric devices. A detailed model analysis is also provided for a quantitative understanding of the thermoelectric voltages, which consist of the spin Seebeck and anomalous Nernst contributions.

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