With the advancement of spin science and spintronics research, study on spin current has become increasingly important. Spin current has been used to explain new phenomena and electronic states and to organize conventional spintronics phenomena. In this article, recent developments in spin physics, spin current, and related phenomena are discussed, with a focus on the interaction between spin angular momentum and other forms of angular momentum. The article covers topics such as spin pumping, topological Hall torque, emergent inductor, spin Seebeck and Peltier effects, and the interaction between mechanical motion and electron/nuclear spins.
Along with the progress of spin science and spintronics research, the flow of electron spins, i.e., spin current, has attracted interest. New phenomena and electronic states were explained in succession using the concept of spin current. Moreover, as many of the conventionally known spintronics phenomena became well organized based on spin current, it has rapidly been recognized as an essential concept in a wide range of condensed matter physics. In this article, we focus on recent developments in the physics of spin, spin current, and their related phenomena, where the conversion between spin angular momentum and different forms of angular momentum plays an essential role. Starting with an introduction to spin current, we first discuss the recent progress in spintronic phenomena driven by spin-exchange coupling: spin pumping, topological Hall torque, and emergent inductor. We, then, extend our discussion to the interaction/interconversion of spins with heat, lattice vibrations, and charge current and address recent progress and perspectives on the spin Seebeck and Peltier effects. Next, we review the interaction between mechanical motion and electron/nuclear spins and argue the difference between the Barnett field and rotational Doppler effect. We show that the Barnett effect reveals the angular momentum compensation temperature, at which the net angular momentum is quenched in ferrimagnets.
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