Seebeck coefficient S, high electrical conductivity σ, and low thermal conductivity κ, which are normally expressed by the thermoelectric figure of merit, ZT = σS 2 T/κ, where T is the absolute temperature. [1][2][3][4][5] To improve ZT, research on various materials has been performed, where κ is minimized by phonon engineering, [3] and the power factor (σS 2 ) is enhanced by modification of the band structure. [4] As an alternative and novel route to improve the thermoelectric efficiency, several interesting approaches, such as the spin Seebeck, anisotropic Seebeck, electrolyte Seebeck, and photo Seebeck effects, have been proposed recently. [6][7][8][9] Among these approaches, the spin Seebeck effect [9] has especially attracted attention with regard to thermoelectrics in various magnetic systems (or spin thermoelectrics) as a new strategy for thermoelectric energy conversion [10][11][12][13][14] and as a spin current source in spintronic devices. [15][16][17][18][19][20] Although the spin Seebeck effect is fascinating as the spin counterpart of the Seebeck effect, practical thermoelectric power generation using spin Seebeck effect is yet to be developed. Therefore, obviously, the most critical aspect of spin thermoelectrics for practical applications is to increase the efficiency of energy conversion, which has been engineered with regard to thermal conductivity, [21,22] band gap of the semiconductor, [16,23,24] and the spin Hall angle (θ SH ), [13] among others. In addition to these attempts, a spin thermopile consisting of wire elements of a ferromagnetic (FM)/electrode bilayer can increase the overall voltage by alternating the polarity of each element in a zigzag structure, [13,[25][26][27] as magnetic materials certainly can gain benefits from tunability of the magnetic direction and a nanoscale modulating structure. [28][29][30] Previously, spin thermopiles utilizing the anomalous Nernst effect (ANE) alone showed enhanced signals with alternating signs of ANE coefficients (C ANE ) or with an alternating magnetic direction. [27] However, its operating magnetic field is somewhat large, on the order of kOe, and the signal shows hysteretic behavior when subjected to coercive-field modulation to control the magnetic direction. It has also been reported that thermopiles with the inverse spin Hall effect (ISHE) can be fabricated 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 ...