Abstract
The orbital angular momentum of electrons presents exciting opportunities for developing energy-efficient, low-power magnetic devices. Typically, the generation of orbital currents is driven by the transfer of orbital angular momentum from 3d transition metal magnets, either through the application of an electric field using the orbital Hall effect or through magnetization dynamics. Chiral phonons are quantized lattice vibrations that carry non-zero angular momentum due to the circular motion of atoms. An interplay of chiral phonon dynamics and electrons would enable the direct generation of orbital angular momentum, even without the need for magnetic elements. Here we experimentally demonstrate the generation of orbital currents from chiral phonons activated in the chiral insulator α-quartz under an applied magnetic field and a temperature gradient. We refer to this phenomenon as the orbital Seebeck effect. The generated orbital current is selectively detected in tungsten and titanium films deposited on quartz through the inverse orbital Hall effect. Our findings hold promise for orbitronics based on chiral phonons in non-magnetic insulators and shed light on the fundamental understanding of chiral phonons and their interaction with electron orbitals.
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The data that support the findings of this study are available from the corresponding authors upon request. Source data are provided with this paper.
References
Zhang, L. & Niu, Q. Chiral phonons at high-symmetry points in monolayer hexagonal lattices. Phys. Rev. Lett. 115, 115502 (2015).
Zhu, H. et al. Observation of chiral phonons. Science 359, 579–582 (2018).
Ishito, K. et al. Truly chiral phonons in α-HgS. Nat. Phys. 19, 35–39 (2022).
Ueda, H. et al. Chiral phonons in quartz probed by X-rays. Nature 618, 946–950 (2023).
Oishi, E., Fujii, Y. & Koreeda, A. Selective observation of enantiomeric chiral phonons in α-quartz. Phys. Rev. B 109, 104306 (2024).
Chen, H. et al. Chiral phonon diode effect in chiral crystals. Nano Lett. 22, 1688–1693 (2022).
Hamada, M., Minamitani, E., Hirayama, M. & Murakami, S. Phonon angular momentum induced by the temperature gradient. Phys. Rev. Lett. 121, 175301 (2018).
Kim, K. et al. Chiral-phonon-activated spin Seebeck effect. Nat. Mater. 22, 322–328 (2023).
Ohe, K. et al. Chirality-induced selectivity of phonon angular momenta in chiral quartz crystals. Phys. Rev. Lett. 132, 056302 (2024).
Schaack, G. Magnetic-field dependent phonon states in paramagnetic CeF3. Solid State Commun. 17, 505–509 (1975).
Schaack, G. Observation of circularly polarized phonon states in an external magnetic field. J. Phys. C: Solid State Phys. 9, L297 (1976).
Cheng, B. et al. A large effective phonon magnetic moment in a Dirac semimetal. Nano Lett. 20, 5991–5996 (2020).
Baydin, A. et al. Magnetic control of soft chiral phonons in PbTe. Phys. Rev. Lett. 128, 075901 (2022).
Juraschek, D. M. & Spaldin, N. A. Orbital magnetic moments of phonons. Phys. Rev. Mater. 3, 064405 (2019).
Ren, Y., Xiao, C., Saparov, D. & Niu, Q. Phonon magnetic moment from electronic topological magnetization. Phys. Rev. Lett. 127, 186403 (2021).
Hernandez, F. G. G. et al. Observation of interplay between phonon chirality and electronic band topology. Sci. Adv. 9, eadj4074 (2023).
Jo, D., Go, D., Choi, G.-M. & Lee, H.-W. Spintronics meets orbitronics: emergence of orbital angular momentum in solids. npj Spintronics 2, 19 (2024).
Seifert, T. S. et al. Time-domain observation of ballistic orbital-angular-momentum currents with giant relaxation length in tungsten. Nat. Nanotechnol. 18, 1132–1138 (2023).
Choi, Y.-G. et al. Observation of the orbital Hall effect in a light metal Ti. Nature 619, 52–56 (2023).
Lyalin, I., Alikhah, S., Berritta, M., Oppeneer, P. M. & Kawakami, R. K. Magneto-optical detection of the orbital Hall effect in chromium. Phys. Rev. Lett. 131, 156702 (2023).
Rothschild, A. et al. Generation of spin currents by the orbital Hall effect in Cu and Al and their measurement by a Ferris-wheel ferromagnetic resonance technique at the wafer level. Phys. Rev. B 106, 144415 (2022).
Xu, Y. et al. Orbitronics: light-induced orbital currents in Ni studied by terahertz emission experiments. Nat. Commun. 15, 2043 (2024).
Go, D. et al. Orbital pumping by magnetization dynamics in ferromagnets. Phys. Rev. B 111, L140409 (2025).
Komiyama, H. & Murakami, S. Universal features of canonical phonon angular momentum without time-reversal symmetry. Phys. Rev. B 103, 214302 (2021).
Hayashi, H., Go, D., Haku, S., Mokrousov, Y. & Ando, K. Observation of orbital pumping. Nat. Electron. 7, 646–652 (2024).
Go, D., Jo, D., Lee, H.-W., Kläui, M. & Mokrousov, Y. Orbitronics: orbital currents in solids. EPL 135, 37001 (2021).
Salemi, L. & Oppeneer, P. M. First-principles theory of intrinsic spin and orbital Hall and Nernst effects in metallic monoatomic crystals. Phys. Rev. Mater. 6, 095001 (2022).
Kikkawa, T. et al. Observation of nuclear-spin Seebeck effect. Nat. Commun. 12, 4356 (2021).
Zhong, J. et al. Abnormal phonon angular momentum due to off-diagonal elements in the density matrix induced by a temperature gradient. Phys. Rev. B 107, 125147 (2023).
Juraschek, D. M., Fechner, M., Balatsky, A. V. & Spaldin, N. A. Dynamical multiferroicity. Phys. Rev. Mater. 1, 014401 (2017).
Ideue, T. et al. Bulk rectification effect in a polar semiconductor. Nat. Phys. 13, 578–583 (2017).
Rikken, G. L. J. A., Fölling, J. & Wyder, P. Electrical magnetochiral anisotropy. Phys. Rev. Lett. 87, 236602 (2001).
Yokouchi, T., Ikeda, Y., Morimoto, T. & Shiomi, Y. Giant magnetochiral anisotropy in Weyl semimetal WTe2 induced by diverging Berry curvature. Phys. Rev. Lett. 130, 136301 (2023).
Uchida, K. et al. Observation of the spin Seebeck effect. Nature 455, 778–781 (2008).
Wu, S. M., Pearson, J. E. & Bhattacharya, A. Paramagnetic spin Seebeck effect. Phys. Rev. Lett. 114, 186602 (2015).
Niimi, Y. & Otani, Y. Reciprocal spin Hall effects in conductors with strong spin–orbit coupling: a review. Rep. Prog. Phys. 78, 124501 (2015).
Wang, H. L. et al. Scaling of spin Hall angle in 3d, 4d, and 5d metals from Y3Fe5O12/metal spin pumping. Phys. Rev. Lett. 112, 197201 (2014).
Uchida, K. et al. Longitudinal spin Seebeck effect: from fundamentals to applications. J. Phys. Condens. Matter 26, 343202 (2014).
Du, C., Wang, H., Yang, F. & Hammel, P. C. Systematic variation of spin-orbit coupling with d-orbital filling: large inverse spin Hall effect in 3d transition metals. Phys. Rev. B 90, 140407 (2014).
Saitoh, E., Ueda, M., Miyajima, H. & Tatara, G. Conversion of spin current into charge current at room temperature: inverse spin-Hall effect. Appl. Phys. Lett. 88, 182509 (2006).
Hayashi, H. et al. Observation of long-range orbital transport and giant orbital torque. Commun. Phys. 6, 32 (2023).
Pai, C.-F. et al. Spin transfer torque devices utilizing the giant spin Hall effect of tungsten. Appl. Phys. Lett. 101, 122404 (2012).
Wang, T.-C., Chen, T.-Y., Wu, C.-T., Yen, H.-W. & Pai, C.-F. Comparative study on spin-orbit torque efficiencies from W/ferromagnetic and W/ferrimagnetic heterostructures. Phys. Rev. Mater. 2, 014403 (2018).
Sui, X. et al. Giant enhancement of the intrinsic spin Hall conductivity in beta-tungsten via substitutional doping. Phys. Rev. B 96, 241105 (2017).
Anastassakis, E., Burstein, E., Maradudin, A. A. & Minnick, R. Morphic effects—III. Effects of an external magnetic field on the long wavelength optical phonons. J. Phys. Chem. Solids 33, 519–531 (1972).
Gonze, X., Charlier, J.-C., Allan, D. C. & Teter, M. P. Interatomic force constants from first principles: the case of α-quartz. Phys. Rev. B 50, 13035–13038 (1994).
Strauch, D. & Dorner, B. Lattice dynamics of alpha-quartz. I. Experiment. J. Phys. Condens. Matter 5, 6149 (1993).
Kresse, G. & Furthmüller, J. Efficiency of ab-initio total energy calculations for metals and semiconductors using a plane-wave basis set. Comput. Mater. Sci. 6, 15–50 (1996).
Togo, A. & Tanaka, I. First principles phonon calculations in materials science. Scr. Mater. 108, 1–5 (2015).
Acknowledgements
D. Sun acknowledges primary financial support from the Department of Energy under award number DE-SC0020992. D. Sun, J.L., X.L. and A.H. acknowledge the Air Force Office of Scientific Research, Multidisciplinary University Research Initiatives (MURI) Program, under award number FA9550-23-1-0311 for the phonon calculation, modelling work and interpretations. Device fabrication at NC State was partially supported by the National Science Foundation (NSF) under award number DMR-2143642. Y.X. and W.Z. acknowledges US NSF under grant number DMR-2509513 for sample preparation assistance. B.Y. acknowledges financial support from the Israel Science Foundation (ISF: 2974/23) and from the Penn State Materials Research Science and Engineering Center for Nanoscale Science from the NSF under award number DMR-2011839. M.H. acknowledges financial support from NSF under grant numbers OAC-2311202 and CNS-2320292. T.M. and R.R. acknowledge funding from Air Force Office of Scientific Research grant number LRIR 23RXCOR003. Z.V.V. acknowledges funding from Air Force Office of Scientific Research grant number 23RT0542 for Raman measurements. The magneto-Raman measurements supported by the US Department of Energy (DE-FG02-07ER46451) were performed at the National High Magnetic Field Laboratory, which is supported by the NSF Cooperative Agreement No. DMR-2128556 and the State of Florida. J.L. acknowledges financial support from the NSF under award number CBET-1943813 for the simulation work done by Z.W.
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Y.N., D. Sun, J.L. and J.Z. conceived the experiment and supervised this research. Y.N. was responsible for the magnetotransport measurements. Y.N., W.Z., Y.X., H.J., B.E., J.B. and R.S. fabricated the samples. T.M. and R.R. performed the polarization-dependent Raman measurements. H.S., J.Z., Y.N., X.L., A.H.C., A.H. and B.Y. provided theoretical interpretations. T.W. and X.L. conducted the vibrational circular dichroism calculation. C.Y., H.S. and M.H. conducted the density functional theory calculation and analysis. Z.W. conducted a transient heat conduction simulation under J.L.’s supervision. R.B. and B.P. performed circular-polarization-resolved magneto-Raman spectroscopy under D. Smirnov and Z.V.V’s supervision. Y.N. and D. Sun wrote the manuscript. All authors contributed to editing the manuscript.
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Nature Physics thanks Takashi Kikkawa for their contribution to the peer review of this work.
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Nabei, Y., Yang, C., Sun, H. et al. Orbital Seebeck effect induced by chiral phonons. Nat. Phys. 22, 245–251 (2026). https://doi.org/10.1038/s41567-025-03134-x
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DOI: https://doi.org/10.1038/s41567-025-03134-x
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