TY - JOUR
T1 - Chirality as generalized spin–orbit interaction in spintronics
AU - Yu, Tao
AU - Luo, Zhaochu
AU - Bauer, Gerrit E.W.
N1 - Funding Information:
This work is financially supported by the National Natural Science Foundation of China (Grant No. 0214012051 ), the startup grant of Huazhong University of Science and Technology (Grants No. 3004012185 and No. 3004012198 ), the startup grant of Peking University , as well as JSPS KAKENHI Grant No. 19H00645 . T.Y. started his research on chirality in spintronics with G.B. at the Kavli Institute of Nanoscience of the TU Delft six years ago, acknowledging many useful discussions with his colleagues Sanchar Sharma, Xiang Zhang, Yuguang Chen, Yaroslav M. Blanter, and Toeno van der Sar. He continued these studies at the Max Planck Institute for the Structure and Dynamics of Matter and Huazhong University of Science and Technology, thanking Michael A. Sentef, Dante M. Kennes, and Angel Rubio for their help. We thank Yu-Xiang Zhang, Weichao Yu, Kei Yamamoto, Bimu Yao, Jinwei Rao, Bowen Zeng, Jin Lan, Haiming Yu, Mehrdad Elyasi, Ji Zou, Xiangyang Wei, Akashdeep Kamra, Canming Hu, Ping Tang, Alejandro O. Leon, and Sergio Rezende for numerous inspiring discussions.
Funding Information:
This work is financially supported by the National Natural Science Foundation of China (Grant No. 0214012051), the startup grant of Huazhong University of Science and Technology (Grants No. 3004012185 and No. 3004012198), the startup grant of Peking University, as well as JSPS KAKENHI Grant No. 19H00645. T.Y. started his research on chirality in spintronics with G.B. at the Kavli Institute of Nanoscience of the TU Delft six years ago, acknowledging many useful discussions with his colleagues Sanchar Sharma, Xiang Zhang, Yuguang Chen, Yaroslav M. Blanter, and Toeno van der Sar. He continued these studies at the Max Planck Institute for the Structure and Dynamics of Matter and Huazhong University of Science and Technology, thanking Michael A. Sentef, Dante M. Kennes, and Angel Rubio for their help. We thank Yu-Xiang Zhang, Weichao Yu, Kei Yamamoto, Bimu Yao, Jinwei Rao, Bowen Zeng, Jin Lan, Haiming Yu, Mehrdad Elyasi, Ji Zou, Xiangyang Wei, Akashdeep Kamra, Canming Hu, Ping Tang, Alejandro O. Leon, and Sergio Rezende for numerous inspiring discussions.
Publisher Copyright:
© 2023 Elsevier B.V.
PY - 2023/4/10
Y1 - 2023/4/10
N2 - Chirality or handedness distinguishes an object from its mirror images, such as the spread thumb, index finger, and middle finger of the right and left hand. In mathematics, it is described by the outer product of three vectors that obey a right-hand vs. left-hand rule. The chirality of ground state magnetic textures defined by the vectors of magnetization, its gradient, and an electric field from broken inversion symmetry can be fixed by a strong relativistic spin–orbit interaction. This review focuses on the chirality observed in the excited states of the magnetic order, dielectrics, and conductors that hold transverse spins when they are evanescent. Even without any relativistic effect, the transverse spin of the evanescent waves is locked to the momentum and the surface normal of their propagation plane. This chirality thereby acts as a generalized spin–orbit interaction, which leads to the discovery of various chiral interactions between magnetic, phononic, electronic, photonic, and plasmonic excitations in spintronics that mediate the excitation of quasiparticles into a single direction, leading to phenomena such as chiral spin and phonon pumping, chiral spin Seebeck, spin skin, magnonic trap, magnon Doppler, chiral magnon damping, and spin diode effects. Intriguing analogies with electric counterparts in the nano-optics and plasmonics exist. After a brief review of the concepts of chirality that characterize the ground state chiral magnetic textures and chirally coupled magnets in spintronics, we turn to the chiral phenomena of excited states. We present a unified electrodynamic picture for dynamical chirality in spintronics in terms of generalized spin–orbit interaction and compare it with that in nano-optics and plasmonics. Based on the general theory, we subsequently review the theoretical progress and experimental evidence of chiral interaction, as well as the near-field transfer of the transverse spins, between various excitations in magnetic, photonic, electronic and phononic nanostructures at GHz time scales. We provide a perspective for future research before concluding this article.
AB - Chirality or handedness distinguishes an object from its mirror images, such as the spread thumb, index finger, and middle finger of the right and left hand. In mathematics, it is described by the outer product of three vectors that obey a right-hand vs. left-hand rule. The chirality of ground state magnetic textures defined by the vectors of magnetization, its gradient, and an electric field from broken inversion symmetry can be fixed by a strong relativistic spin–orbit interaction. This review focuses on the chirality observed in the excited states of the magnetic order, dielectrics, and conductors that hold transverse spins when they are evanescent. Even without any relativistic effect, the transverse spin of the evanescent waves is locked to the momentum and the surface normal of their propagation plane. This chirality thereby acts as a generalized spin–orbit interaction, which leads to the discovery of various chiral interactions between magnetic, phononic, electronic, photonic, and plasmonic excitations in spintronics that mediate the excitation of quasiparticles into a single direction, leading to phenomena such as chiral spin and phonon pumping, chiral spin Seebeck, spin skin, magnonic trap, magnon Doppler, chiral magnon damping, and spin diode effects. Intriguing analogies with electric counterparts in the nano-optics and plasmonics exist. After a brief review of the concepts of chirality that characterize the ground state chiral magnetic textures and chirally coupled magnets in spintronics, we turn to the chiral phenomena of excited states. We present a unified electrodynamic picture for dynamical chirality in spintronics in terms of generalized spin–orbit interaction and compare it with that in nano-optics and plasmonics. Based on the general theory, we subsequently review the theoretical progress and experimental evidence of chiral interaction, as well as the near-field transfer of the transverse spins, between various excitations in magnetic, photonic, electronic and phononic nanostructures at GHz time scales. We provide a perspective for future research before concluding this article.
KW - Chiral interaction
KW - Chiral spin pumping
KW - Chiral spin seebeck effect
KW - Chirality
KW - Evanescent electromagnetic fields
KW - Generalized spin–orbit interaction
KW - Magnon doppler effect
KW - Near-field spintronics
KW - Non-reciprocity
KW - Spin diode effect
KW - Spin isolator
KW - Spin skin effect
KW - Spin trap
KW - Spin waves
KW - Spin-momentum locking
KW - Surface acoustic waves
KW - Surface plasmon polaritons
KW - Transverse spin of evanescent waves
KW - Unidirectionality
KW - Waveguide microwaves
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U2 - 10.1016/j.physrep.2023.01.002
DO - 10.1016/j.physrep.2023.01.002
M3 - Review article
AN - SCOPUS:85147209578
SN - 0370-1573
VL - 1009
SP - 1
EP - 115
JO - Physics Reports
JF - Physics Reports
ER -