Yao Han, Wang Sicong, Wei Chen, et al. Microscopic three-temperature model for all-optical switching in GdFeCo[J]. Opto-Electronic Engineering, 2019, 46(3): 180629. doi: 10.12086/oee.2019.180629
Citation: Yao Han, Wang Sicong, Wei Chen, et al. Microscopic three-temperature model for all-optical switching in GdFeCo[J]. Opto-Electronic Engineering, 2019, 46(3): 180629. doi: 10.12086/oee.2019.180629

Microscopic three-temperature model for all-optical switching in GdFeCo

    Fund Project: Supported by National Natural Science Foundation of China (NSFC) (11604123, 61522504, 61432007), the Fundamental Research Funds for the Central Universities (21616338), and Guangdong Provincial Innovation and Entrepreneurship Project (Grant 2016ZT06D081)
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  • Compared with magnetic switching by an external magnetic field or by a heat-assisted manner, all-optical switching (AOS) can complete the switching process within 100 ps, which has attracted extensive attention from researchers. Among the magneto-optical materials which can realize AOS, the ferrimagnetic GdFeCo has the ability to realize single-shot AOS and possesses great potential in all-optical magnetic storage. In this paper, a microscopic three-temperature model (M3TM) is utilized to simulate the AOS process of GdFeCo, which is also demonstrated experimentally, under the excitation of a single laser pulse based on the heating effect. By using this M3TM, the AOS dynamics and the final magnetization states of GdFeCo induced by single laser pulses with different energy and pulse widths are calculated and analyzed concretely. Compared with the atomic spin model and the Landau- Lifshitz-Bloch (LLB) model, M3TM provides a more concise time-varying expression of the magnetization of GdFeCo and explicitly addresses the dissipation of angular momentum after the laser-pulse excitation, which enables faster calculations of the heat-induced magnetization dynamics in magneto-optical materials with large areas.
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  • [1] Iwasaki S. Perpendicular magnetic recording - Evolution and future[J]. IEEE Transactions on Magnetics, 1984, 20(5): 657-662. doi: 10.1109/TMAG.1984.1063563

    CrossRef Google Scholar

    [2] Schewe H, Stephani D. Thin-film inductive heads for perpendicular recording[J]. IEEE Transactions on Magnetics, 1990, 26(6): 2966-2971. doi: 10.1109/20.102874

    CrossRef Google Scholar

    [3] Nakamura Y, Iwasaki S. On the resolution of perpendicular magnetic head[J]. IEEE Transactions on Magnetics, 1984, 20(1): 105-107. doi: 10.1109/TMAG.1984.1063024

    CrossRef Google Scholar

    [4] Cumpson S R, Hidding P, Coehoorn R. A hybrid recording method using thermally assisted writing and flux sensitive detection[J]. IEEE Transactions on Magnetics, 2000, 36(5): 2271-2275. doi: 10.1109/20.908391

    CrossRef Google Scholar

    [5] Rottmayer R E, Batra S, Buechel D, et al. Heat-assisted magnetic recording[J]. IEEE Transactions on Magnetics, 2006, 42(10): 2417-2421. doi: 10.1109/TMAG.2006.879572

    CrossRef Google Scholar

    [6] Kirilyuk A, Kimel A V, Rasing T. Ultrafast optical manipulation of magnetic order[J]. Reviews of Modern Physics, 2010, 82(3): 2731-2784. doi: 10.1103/RevModPhys.82.2731

    CrossRef Google Scholar

    [7] Stanciu C D, Hansteen F, Kimel A V, et al. All-optical magnetic recording with circularly polarized light[J]. Physical Review Letters, 2007, 99(4): 047601. doi: 10.1103/PhysRevLett.99.047601

    CrossRef Google Scholar

    [8] Ostler T A, Barker J, Evans R F L, et al. Ultrafast heating as a sufficient stimulus for magnetization reversal in a ferrimagnet[J]. Nature Communications, 2012, 3: 666. doi: 10.1038/ncomms1666

    CrossRef Google Scholar

    [9] Gerrits T, van den Berg H A M, Hohlfeld J, et al. Ultrafast precessional magnetization reversal by picosecond magnetic field pulse shaping[J]. Nature, 2002, 418(6897): 509-512. doi: 10.1038/nature00905

    CrossRef Google Scholar

    [10] Scholl A, Baumgarten L, Jacquemin R, et al. Ultrafast spin dynamics of ferromagnetic thin films observed by fs spin-resolved two-photon photoemission[J]. Physical Review Letters, 1997, 79(22): 5146-5149. doi: 10.1103/PhysRevLett.79.5146

    CrossRef Google Scholar

    [11] Gilbert L T. A lagrangian formulation of the gyromagnetic equation of the magnetization field[J]. Physical Review, 1955, 100: 1243.

    Google Scholar

    [12] Landau L D, Lifshitz E. On the theory of the dispersion of magnetic permeability in ferromagnetic bodies[M]. Perspectives in Theoretical Physics. Pergamon, 1992: 51-65.

    Google Scholar

    [13] Gilbert L T, Kelly M J. Proceedings of the Pittsburgh Conference on Magnetism and Magnetic Materials[M]. New York: American Institute of Electrical Engineers, 1955: 253.

    Google Scholar

    [14] Dillon F J, Jr. Magnetism Ⅱ[M]. New York: Academic Press, 1963.

    Google Scholar

    [15] Kazantseva N, Hinzke D, Nowak U, et al. Towards multiscale modeling of magnetic materials: simulations of FePt[J]. Physical Review B, 2008, 77(18): 184428. doi: 10.1103/PhysRevB.77.184428

    CrossRef Google Scholar

    [16] Garanin A D. Generalized equation of motion for a ferromagnet[J]. Physica A: Statistical Mechanics and its Applications, 1991, 172(3): 470-491. doi: 10.1016/0378-4371(91)90395-S

    CrossRef Google Scholar

    [17] Rebei A, Simionato M. Fluctuations of the magnetization in thin films due to conduction electrons[J]. Physical Review B, 2005, 71(17): 174415. doi: 10.1103/PhysRevB.71.174415

    CrossRef Google Scholar

    [18] Kuiper C K, Roth T, Schellekens J A. Spin-orbit enhanced demagnetization rate in Co/Pt-multilayers[J]. Applied Physics Letters, 2014, 105(20): 202402. doi: 10.1063/1.4902069

    CrossRef Google Scholar

    [19] Koopmans B, Malinowski G, Dalla Longa F, et al. Explaining the paradoxical diversity of ultrafast laser-induced demagnetization[J]. Nature Materials, 2009, 9(3): 259-265. doi: 10.1038/nmat2593

    CrossRef Google Scholar

    [20] Cornelissen T D, Córdoba R, Koopmans B. Microscopic model for all optical switching in ferromagnets[J]. Applied Physics Letters, 2016, 108(14): 142405. doi: 10.1063/1.4945660

    CrossRef Google Scholar

    [21] Khorsand R A, Savoini M, Kirilyuk A. Role of magnetic circular dichroism in all-optical magnetic recording[J]. Physical Review Letters, 2012, 108(12): 127205. doi: 10.1103/PhysRevLett.108.127205

    CrossRef Google Scholar

    [22] Wang S C, Wei C, Feng Y H. All-optical helicity-dependent magnetic switching by first-order azimuthally polarized vortex beams[J]. Physical Review Letters, 2018, 113(17): 171108.

    Google Scholar

    [23] Wang S C, Cao Y Y, Li X P. Generation of uniformly oriented in-plane magnetization with near-unity purity in 4π microscopy[J]. Optics Letters, 2017, 42(23): 5050-5053. doi: 10.1364/OL.42.005050

    CrossRef Google Scholar

    [24] Wang S C, Li X P, Zhou J Y, et al. Ultralong pure longitudinal magnetization needle induced by annular vortex binary optics[J]. Optics Letters, 2014, 39(17): 5022-5025. doi: 10.1364/OL.39.005022

    CrossRef Google Scholar

    [25] Wang S C, Li X P, Zhou J Y, et al. All-optically configuring the inverse Faraday effect for nanoscale perpendicular magnetic recording[J]. Optics Express, 2015, 23(10): 13530-13536. doi: 10.1364/OE.23.013530

    CrossRef Google Scholar

    [26] Wang S C, Luo J J, Zhu Z Q, et al. All-optical generation of magnetization with arbitrary three-dimensional orientations[J]. Optics Letters, 2018, 43(22): 5551-5554. doi: 10.1364/OL.43.005551

    CrossRef Google Scholar

    [27] Radu I, Vahaplar K, Stamm C, et al. Transient ferromagnetic-like state mediating ultrafast reversal of antiferromagnetically coupled spins[J]. Nature, 2011, 472(7342): 205-208. doi: 10.1038/nature09901

    CrossRef Google Scholar

    [28] Evans R F L, Fan W J, Chureemart P. Atomistic spin model simulations of magnetic nanomaterials[J]. Journal of Physics: Condensed Matter, 2014, 26(10): 103202. doi: 10.1088/0953-8984/26/10/103202

    CrossRef Google Scholar

    [29] Atxitia U, Chubykalo-Fesenko O. Ultrafast magnetization dynamics rates within the Landau-Lifshitz-Bloch model[J]. Physical Review B, 2011, 84(14): 144414. doi: 10.1103/PhysRevB.84.144414

    CrossRef Google Scholar

    [30] Kazantseva N. Dynamic response of the magnetisation to picosecond heat pulses[D]. York, UK: The University of York, 2008: 1-128.10.2147/OPTH.S23381

    Google Scholar

  • Overview: All-optically manipulating the orientations of the magnetization or the spins in magnetic materials has aroused intensive research interests for the attractive applications in ultrafast data storage, spin dynamics, and magnetic holography. Among these applications, all-optical switching (AOS) has emerged as a promising alternative way to realize ultrafast perpendicular magnetic recording. Compared with magnetic switching by an external magnetic field or by a heat-assisted manner, AOS can complete the switching process within 100 ps, which has attracted extensive attention from researchers. Among the magneto-optical materials which can realize AOS, the ferrimagnetic GdFeCo has the ability to realize single-shot AOS and possesses great potential in all-optical magnetic storage. Currently, the atomic spin model and the Landau-Lifshitz-Bloch (LLB) model are the basic and frequently-used mathematical methods to describe the dynamics of GdFeCo after the laser-pulse excitation. However, these two models only use the damping parameters to phenomenologically describe the transfer process of angular momentum, and hence it is impossible to give the quantized information of angular momentum transfer during the switching process. In 2009, B. Koopmans et al. proposed a simple-form model which is called the microscopic three-temperature model (M3TM) to unify two contradictory ultrafast laser-induced demagnetization processes. This model is especially suitable for magnetic materials with the easy axis perpendicular to the surface and has been applied to calculate the ultrafast dynamics of multisublattice magnets, to demonstrate the spin-orbit enhanced demagnetization rate in Co/Pt-multilayers, and to explain the AOS in ferromagnets. In this model, the switching of electron spins is achieved by emitting or absorbing a phonon with a certain probability and hence the quantized information of angular momentum is explicitly given. In this paper, the M3TM is utilized to simulate the AOS process of GdFeCo, which is also demonstrated experimentally, under the excitation of a single laser pulse based on the heating effect. By using the M3TM, the AOS dynamics and the final magnetization states of GdFeCo induced by single laser pulses with different energy and pulse widths are calculated and analyzed concretely. Compared with the atomic spin model and the LLB model, M3TM provides a more concise time-varying expression of the magnetization of GdFeCo and explicitly addresses the dissipation of angular momentum after the laser-pulse excitation, which enables faster calculations of the heat-induced magnetization dynamics in magneto-optical materials with large areas.

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