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Yang B, Ji Q, Huang FZ, Li J, Tian YZ, Xue B, Zhu R, Wu H, Yang H, Yang YB, Tang S, Zhao HB, Cao Y, Du J, Wang BG, Zhang C, Wu D. Picosecond Spin Current Generation from Vicinal Metal-Antiferromagnetic Insulator Interfaces. PHYSICAL REVIEW LETTERS 2024; 132:176703. [PMID: 38728713 DOI: 10.1103/physrevlett.132.176703] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 10/06/2023] [Accepted: 03/22/2024] [Indexed: 05/12/2024]
Abstract
We report the picosecond spin current generation from the interface between a heavy metal and a vicinal antiferromagnet insulator Cr_{2}O_{3} by laser pulses at room temperature and zero magnetic field. It is converted into a detectable terahertz emission in the heavy metal via the inverse spin Hall effect. The vicinal interfaces are apparently the source of the picosecond spin current, as evidenced by the proportional terahertz signals to the vicinal angle. We attribute the origin of the spin current to the transient magnetic moment generated by an interfacial nonlinear magnetic-dipole difference-frequency generation. We propose a model based on the in-plane inversion symmetry breaking to quantitatively explain the terahertz intensity with respect to the angles of the laser polarization and the film azimuth. Our work opens new opportunities in antiferromagnetic and ultrafast spintronics by considering symmetry breaking.
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Affiliation(s)
- B Yang
- National Laboratory of Solid State Microstructures, Jiangsu Provincial Key Laboratory for Nanotechnology, Collaborative Innovation Center of Advanced Microstructures and Department of Physics, Nanjing University, Nanjing 210093, People's Republic of China
| | - Qing Ji
- National Laboratory of Solid State Microstructures, Jiangsu Provincial Key Laboratory for Nanotechnology, Collaborative Innovation Center of Advanced Microstructures and Department of Physics, Nanjing University, Nanjing 210093, People's Republic of China
| | - F Z Huang
- National Laboratory of Solid State Microstructures, Jiangsu Provincial Key Laboratory for Nanotechnology, Collaborative Innovation Center of Advanced Microstructures and Department of Physics, Nanjing University, Nanjing 210093, People's Republic of China
| | - Jiacong Li
- National Laboratory of Solid State Microstructures, Jiangsu Provincial Key Laboratory for Nanotechnology, Collaborative Innovation Center of Advanced Microstructures and Department of Physics, Nanjing University, Nanjing 210093, People's Republic of China
| | - Y Z Tian
- National Laboratory of Solid State Microstructures, Jiangsu Provincial Key Laboratory for Nanotechnology, Collaborative Innovation Center of Advanced Microstructures and Department of Physics, Nanjing University, Nanjing 210093, People's Republic of China
| | - B Xue
- National Laboratory of Solid State Microstructures, Jiangsu Provincial Key Laboratory for Nanotechnology, Collaborative Innovation Center of Advanced Microstructures and Department of Physics, Nanjing University, Nanjing 210093, People's Republic of China
| | - Ruxian Zhu
- National Laboratory of Solid State Microstructures, Jiangsu Provincial Key Laboratory for Nanotechnology, Collaborative Innovation Center of Advanced Microstructures and Department of Physics, Nanjing University, Nanjing 210093, People's Republic of China
| | - Hui Wu
- National Laboratory of Solid State Microstructures, Jiangsu Provincial Key Laboratory for Nanotechnology, Collaborative Innovation Center of Advanced Microstructures and Department of Physics, Nanjing University, Nanjing 210093, People's Republic of China
| | - Hanyue Yang
- National Laboratory of Solid State Microstructures, Jiangsu Provincial Key Laboratory for Nanotechnology, Collaborative Innovation Center of Advanced Microstructures and Department of Physics, Nanjing University, Nanjing 210093, People's Republic of China
| | - Y B Yang
- National Laboratory of Solid State Microstructures, Jiangsu Provincial Key Laboratory for Nanotechnology, Collaborative Innovation Center of Advanced Microstructures and Department of Physics, Nanjing University, Nanjing 210093, People's Republic of China
| | - Shaolong Tang
- National Laboratory of Solid State Microstructures, Jiangsu Provincial Key Laboratory for Nanotechnology, Collaborative Innovation Center of Advanced Microstructures and Department of Physics, Nanjing University, Nanjing 210093, People's Republic of China
| | - H B Zhao
- Key Laboratory of Micro and Nano Photonic Structures (Ministry of Education), Department of Optical Science and Engineering, Fudan University, Shanghai 200433, People's Republic of China
| | - Y Cao
- National Laboratory of Solid State Microstructures, Jiangsu Provincial Key Laboratory for Nanotechnology, Collaborative Innovation Center of Advanced Microstructures and Department of Physics, Nanjing University, Nanjing 210093, People's Republic of China
| | - J Du
- National Laboratory of Solid State Microstructures, Jiangsu Provincial Key Laboratory for Nanotechnology, Collaborative Innovation Center of Advanced Microstructures and Department of Physics, Nanjing University, Nanjing 210093, People's Republic of China
| | - B G Wang
- National Laboratory of Solid State Microstructures, Jiangsu Provincial Key Laboratory for Nanotechnology, Collaborative Innovation Center of Advanced Microstructures and Department of Physics, Nanjing University, Nanjing 210093, People's Republic of China
| | - Chunfeng Zhang
- National Laboratory of Solid State Microstructures, Jiangsu Provincial Key Laboratory for Nanotechnology, Collaborative Innovation Center of Advanced Microstructures and Department of Physics, Nanjing University, Nanjing 210093, People's Republic of China
| | - D Wu
- National Laboratory of Solid State Microstructures, Jiangsu Provincial Key Laboratory for Nanotechnology, Collaborative Innovation Center of Advanced Microstructures and Department of Physics, Nanjing University, Nanjing 210093, People's Republic of China
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Qiu H, Seifert TS, Huang L, Zhou Y, Kašpar Z, Zhang C, Wu J, Fan K, Zhang Q, Wu D, Kampfrath T, Song C, Jin B, Chen J, Wu P. Terahertz Spin Current Dynamics in Antiferromagnetic Hematite. ADVANCED SCIENCE (WEINHEIM, BADEN-WURTTEMBERG, GERMANY) 2023; 10:e2300512. [PMID: 37083225 PMCID: PMC10288251 DOI: 10.1002/advs.202300512] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 01/23/2023] [Revised: 03/10/2023] [Indexed: 05/03/2023]
Abstract
An important vision of modern magnetic research is to use antiferromagnets (AFMs) as controllable and active ultrafast components in spintronic devices. Hematite (α-Fe2 O3 ) is a promising model material in this respect because its pronounced Dzyaloshinskii-Moriya interaction leads to the coexistence of antiferromagnetism and weak ferromagnetism. Here, femtosecond laser pulses are used to drive terahertz (THz) spin currents from α-Fe2 O3 into an adjacent Pt layer. Two contributions to the generation of the spin current with distinctly different dynamics are found: the impulsive stimulated Raman scatting that relies on the AFM order and the ultrafast spin Seebeck effect that relies on the net magnetization. The total THz spin current dynamics can be manipulated by a medium-strength magnetic field below 1 T. The control of the THz spin current achieved in α-Fe2 O3 opens the pathway toward tailoring the exact spin current dynamics from ultrafast AFM spin sources.
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Affiliation(s)
- Hongsong Qiu
- Research Institute of Superconductor Electronics (RISE)School of Electronic Science and EngineeringNanjing UniversityNanjing210023P. R. China
| | - Tom S. Seifert
- Department of PhysicsFreie Universität Berlin14195BerlinGermany
| | - Lin Huang
- Key Laboratory of Advanced Materials (MOE)School of Materials Science and EngineeringTsinghua UniversityBeijing100084P. R. China
| | - Yongjian Zhou
- Key Laboratory of Advanced Materials (MOE)School of Materials Science and EngineeringTsinghua UniversityBeijing100084P. R. China
| | - Zdeněk Kašpar
- Department of PhysicsFreie Universität Berlin14195BerlinGermany
| | - Caihong Zhang
- Research Institute of Superconductor Electronics (RISE)School of Electronic Science and EngineeringNanjing UniversityNanjing210023P. R. China
| | - Jingbo Wu
- Research Institute of Superconductor Electronics (RISE)School of Electronic Science and EngineeringNanjing UniversityNanjing210023P. R. China
| | - Kebin Fan
- Research Institute of Superconductor Electronics (RISE)School of Electronic Science and EngineeringNanjing UniversityNanjing210023P. R. China
| | - Qi Zhang
- Department of PhysicsNanjing UniversityNanjing210023P. R. China
| | - Di Wu
- National Laboratory of Solid State MicrostructuresJiangsu Provincial Key Laboratory for NanotechnologyCollaborative Innovation Center of Advanced Microstructures and Department of PhysicsNanjing UniversityNanjing210023P. R. China
| | | | - Cheng Song
- Key Laboratory of Advanced Materials (MOE)School of Materials Science and EngineeringTsinghua UniversityBeijing100084P. R. China
| | - Biaobing Jin
- Research Institute of Superconductor Electronics (RISE)School of Electronic Science and EngineeringNanjing UniversityNanjing210023P. R. China
| | - Jian Chen
- Research Institute of Superconductor Electronics (RISE)School of Electronic Science and EngineeringNanjing UniversityNanjing210023P. R. China
| | - Peiheng Wu
- Research Institute of Superconductor Electronics (RISE)School of Electronic Science and EngineeringNanjing UniversityNanjing210023P. R. China
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3
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Heeg KP, Kaldun A, Strohm C, Ott C, Subramanian R, Lentrodt D, Haber J, Wille HC, Goerttler S, Rüffer R, Keitel CH, Röhlsberger R, Pfeifer T, Evers J. Coherent X-ray-optical control of nuclear excitons. Nature 2021; 590:401-404. [PMID: 33597757 PMCID: PMC7889490 DOI: 10.1038/s41586-021-03276-x] [Citation(s) in RCA: 13] [Impact Index Per Article: 3.3] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 10/22/2018] [Accepted: 12/02/2020] [Indexed: 12/02/2022]
Abstract
Coherent control of quantum dynamics is key to a multitude of fundamental studies and applications1. In the visible or longer-wavelength domains, near-resonant light fields have become the primary tool with which to control electron dynamics2. Recently, coherent control in the extreme-ultraviolet range was demonstrated3, with a few-attosecond temporal resolution of the phase control. At hard-X-ray energies (above 5-10 kiloelectronvolts), Mössbauer nuclei feature narrow nuclear resonances due to their recoilless absorption and emission of light, and spectroscopy of these resonances is widely used to study the magnetic, structural and dynamical properties of matter4,5. It has been shown that the power and scope of Mössbauer spectroscopy can be greatly improved using various control techniques6-16. However, coherent control of atomic nuclei using suitably shaped near-resonant X-ray fields remains an open challenge. Here we demonstrate such control, and use the tunable phase between two X-ray pulses to switch the nuclear exciton dynamics between coherent enhanced excitation and coherent enhanced emission. We present a method of shaping single pulses delivered by state-of-the-art X-ray facilities into tunable double pulses, and demonstrate a temporal stability of the phase control on the few-zeptosecond timescale. Our results unlock coherent optical control for nuclei, and pave the way for nuclear Ramsey spectroscopy17 and spin-echo-like techniques, which should not only advance nuclear quantum optics18, but also help to realize X-ray clocks and frequency standards19. In the long term, we envision time-resolved studies of nuclear out-of-equilibrium dynamics, which is a long-standing challenge in Mössbauer science20.
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Affiliation(s)
- Kilian P Heeg
- Max-Planck-Institut für Kernphysik, Heidelberg, Germany
| | | | | | - Christian Ott
- Max-Planck-Institut für Kernphysik, Heidelberg, Germany
| | | | | | - Johann Haber
- Deutsches Elektronen-Synchrotron DESY, Hamburg, Germany
| | | | | | - Rudolf Rüffer
- The European Synchrotron Radiation Facility (ESRF), Grenoble, France
| | | | - Ralf Röhlsberger
- Deutsches Elektronen-Synchrotron DESY, Hamburg, Germany
- The Hamburg Centre for Ultrafast Imaging, Hamburg, Germany
- Helmholtz-Institut Jena, Jena, Germany
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
- Institut für Optik und Quantenelektronik, Friedrich-Schiller-Universität Jena, Jena, Germany
| | | | - Jörg Evers
- Max-Planck-Institut für Kernphysik, Heidelberg, Germany.
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4
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Hudl M, d'Aquino M, Pancaldi M, Yang SH, Samant MG, Parkin SSP, Dürr HA, Serpico C, Hoffmann MC, Bonetti S. Nonlinear Magnetization Dynamics Driven by Strong Terahertz Fields. PHYSICAL REVIEW LETTERS 2019; 123:197204. [PMID: 31765192 DOI: 10.1103/physrevlett.123.197204] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.2] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 03/21/2019] [Indexed: 06/10/2023]
Abstract
We present a comprehensive experimental and numerical study of magnetization dynamics in a thin metallic film triggered by single-cycle terahertz pulses of ∼20 MV/m electric field amplitude and ∼1 ps duration. The experimental dynamics is probed using the femtosecond magneto-optical Kerr effect, and it is reproduced numerically using macrospin simulations. The magnetization dynamics can be decomposed in three distinct processes: a coherent precession of the magnetization around the terahertz magnetic field, an ultrafast demagnetization that suddenly changes the anisotropy of the film, and a uniform precession around the equilibrium effective field that is relaxed on the nanosecond time scale, consistent with a Gilbert damping process. Macrospin simulations quantitatively reproduce the observed dynamics, and allow us to predict that novel nonlinear magnetization dynamics regimes can be attained with existing tabletop terahertz sources.
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Affiliation(s)
- Matthias Hudl
- Department of Physics, Stockholm University, 106 91 Stockholm, Sweden
| | | | - Matteo Pancaldi
- Department of Physics, Stockholm University, 106 91 Stockholm, Sweden
| | - See-Hun Yang
- IBM Almaden Research Center, San Jose, California 95120, USA
| | - Mahesh G Samant
- IBM Almaden Research Center, San Jose, California 95120, USA
| | - Stuart S P Parkin
- IBM Almaden Research Center, San Jose, California 95120, USA
- Max-Planck Institut für Mikrostrukturphysik, 06120 Halle, Germany
| | - Hermann A Dürr
- Department of Physics and Astronomy, Uppsala University, 751 20 Uppsala, Sweden
| | - Claudio Serpico
- DIETI, University of Naples Federico II, 80125 Naples, Italy
| | | | - Stefano Bonetti
- Department of Physics, Stockholm University, 106 91 Stockholm, Sweden
- Department of Molecular Sciences and Nanosystems, Ca' Foscari University of Venice, 30172 Venezia Mestre, Italy
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5
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Quantum Phonon Transport in Nanomaterials: Combining Atomistic with Non-Equilibrium Green's Function Techniques. ENTROPY 2019; 21:e21080735. [PMID: 33267449 PMCID: PMC7515264 DOI: 10.3390/e21080735] [Citation(s) in RCA: 4] [Impact Index Per Article: 0.7] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 07/01/2019] [Revised: 07/23/2019] [Accepted: 07/25/2019] [Indexed: 11/16/2022]
Abstract
A crucial goal for increasing thermal energy harvesting will be to progress towards atomistic design strategies for smart nanodevices and nanomaterials. This requires the combination of computationally efficient atomistic methodologies with quantum transport based approaches. Here, we review our recent work on this problem, by presenting selected applications of the PHONON tool to the description of phonon transport in nanostructured materials. The PHONON tool is a module developed as part of the Density-Functional Tight-Binding (DFTB) software platform. We discuss the anisotropic phonon band structure of selected puckered two-dimensional materials, helical and horizontal doping effects in the phonon thermal conductivity of boron nitride-carbon heteronanotubes, phonon filtering in molecular junctions, and a novel computational methodology to investigate time-dependent phonon transport at the atomistic level. These examples illustrate the versatility of our implementation of phonon transport in combination with density functional-based methods to address specific nanoscale functionalities, thus potentially allowing for designing novel thermal devices.
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Seifert TS, Jaiswal S, Barker J, Weber ST, Razdolski I, Cramer J, Gueckstock O, Maehrlein SF, Nadvornik L, Watanabe S, Ciccarelli C, Melnikov A, Jakob G, Münzenberg M, Goennenwein STB, Woltersdorf G, Rethfeld B, Brouwer PW, Wolf M, Kläui M, Kampfrath T. Femtosecond formation dynamics of the spin Seebeck effect revealed by terahertz spectroscopy. Nat Commun 2018; 9:2899. [PMID: 30042421 PMCID: PMC6057952 DOI: 10.1038/s41467-018-05135-2] [Citation(s) in RCA: 33] [Impact Index Per Article: 4.7] [Reference Citation Analysis] [Abstract] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 12/17/2017] [Accepted: 06/13/2018] [Indexed: 11/09/2022] Open
Abstract
Understanding the transfer of spin angular momentum is essential in modern magnetism research. A model case is the generation of magnons in magnetic insulators by heating an adjacent metal film. Here, we reveal the initial steps of this spin Seebeck effect with <27 fs time resolution using terahertz spectroscopy on bilayers of ferrimagnetic yttrium iron garnet and platinum. Upon exciting the metal with an infrared laser pulse, a spin Seebeck current js arises on the same ~100 fs time scale on which the metal electrons thermalize. This observation highlights that efficient spin transfer critically relies on carrier multiplication and is driven by conduction electrons scattering off the metal–insulator interface. Analytical modeling shows that the electrons’ dynamics are almost instantaneously imprinted onto js because their spins have a correlation time of only ~4 fs and deflect the ferrimagnetic moments without inertia. Applications in material characterization, interface probing, spin-noise spectroscopy and terahertz spin pumping emerge. Probing spin pumping in the terahertz regime allows one to reveal its initial elementary steps. Here, the authors show that the formation of the spin Seebeck current in YIG/Pt critically relies on hot thermalized metal electrons because they impinge on the metal-insulator interface with maximum noise.
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Affiliation(s)
- Tom S Seifert
- Department of Physical Chemistry, Fritz Haber Institute of the Max Planck Society, 14195, Berlin, Germany.,Department of Physics, Freie Universität Berlin, 14195, Berlin, Germany
| | - Samridh Jaiswal
- Institute of Physics, Johannes Gutenberg University Mainz, 55099, Mainz, Germany.,Singulus Technologies AG, 63796, Kahl am Main, Germany
| | - Joseph Barker
- Institute for Materials Research, Tohoku University, Sendai, 980-8577, Japan
| | - Sebastian T Weber
- Department of Physics and Research Center OPTIMAS, Technische Universität Kaiserslautern, 67663, Kaiserslautern, Germany
| | - Ilya Razdolski
- Department of Physical Chemistry, Fritz Haber Institute of the Max Planck Society, 14195, Berlin, Germany
| | - Joel Cramer
- Institute of Physics, Johannes Gutenberg University Mainz, 55099, Mainz, Germany
| | - Oliver Gueckstock
- Department of Physical Chemistry, Fritz Haber Institute of the Max Planck Society, 14195, Berlin, Germany
| | - Sebastian F Maehrlein
- Department of Physical Chemistry, Fritz Haber Institute of the Max Planck Society, 14195, Berlin, Germany
| | - Lukas Nadvornik
- Department of Physical Chemistry, Fritz Haber Institute of the Max Planck Society, 14195, Berlin, Germany.,Department of Physics, Freie Universität Berlin, 14195, Berlin, Germany
| | - Shun Watanabe
- Department of Advanced Materials Science, School of Frontier Sciences, University of Tokyo, Chiba, 277-8561, Japan
| | - Chiara Ciccarelli
- Cavendish Laboratory, University of Cambridge, Cambridge, CB3 0HE, UK
| | - Alexey Melnikov
- Department of Physical Chemistry, Fritz Haber Institute of the Max Planck Society, 14195, Berlin, Germany.,Institute of Physics, Martin-Luther-Universität Halle, 06120, Halle, Germany
| | - Gerhard Jakob
- Institute of Physics, Johannes Gutenberg University Mainz, 55099, Mainz, Germany
| | - Markus Münzenberg
- Institut für Physik, Universität Greifswald, 17489, Greifswald, Germany
| | - Sebastian T B Goennenwein
- Institut für Festkörper- und Materialphysik, Technische Universität Dresden, 01062, Dresden, Germany
| | - Georg Woltersdorf
- Institute of Physics, Martin-Luther-Universität Halle, 06120, Halle, Germany
| | - Baerbel Rethfeld
- Department of Physics and Research Center OPTIMAS, Technische Universität Kaiserslautern, 67663, Kaiserslautern, Germany
| | - Piet W Brouwer
- Department of Physics, Freie Universität Berlin, 14195, Berlin, Germany
| | - Martin Wolf
- Department of Physical Chemistry, Fritz Haber Institute of the Max Planck Society, 14195, Berlin, Germany
| | - Mathias Kläui
- Institute of Physics, Johannes Gutenberg University Mainz, 55099, Mainz, Germany
| | - Tobias Kampfrath
- Department of Physical Chemistry, Fritz Haber Institute of the Max Planck Society, 14195, Berlin, Germany. .,Department of Physics, Freie Universität Berlin, 14195, Berlin, Germany.
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