2013
DOI: 10.1103/physrevlett.110.266602
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New Concept for Magnetization Switching by Ultrafast Acoustic Pulses

Abstract: It is shown theoretically that a single acoustic pulse, a few picoseconds long, can reverse magnetization in a magnetostrictive material Terfenol-D. Following giant magnetoelastic changes of free energy density, the magnetization vector is ejected from a local in-plane energy minimum and decays into another minimum. For an acoustic pulse duration significantly shorter than magnetization precession period τac≪Tprec, the switching threshold is determined by the acoustic pulse area, i.e., pulse integral in the ti… Show more

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Cited by 118 publications
(119 citation statements)
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“…The opposite effect, inverse magnetostriction, whereby magnetization can be changed upon application of a strain, is particularly relevant to magnetic data storage technologies as a possible route towards induction-free data manipulation when used dynamically. It has been proposed for magnetization switching through resonant [2,3] or nonresonant processes [4,5], the latter possibly at play in early results of surface acoustic wave (SAW)-induced lowering of coercivity in Galfenol films [6]. In the case of precessional (resonant) switching, two features are necessary: sizable magnetoacoustic coupling (to trigger precession), and a highly nonlinear system (to force wide, noncircular precession needed for magnetization reversal).…”
Section: Introductionmentioning
confidence: 99%
“…The opposite effect, inverse magnetostriction, whereby magnetization can be changed upon application of a strain, is particularly relevant to magnetic data storage technologies as a possible route towards induction-free data manipulation when used dynamically. It has been proposed for magnetization switching through resonant [2,3] or nonresonant processes [4,5], the latter possibly at play in early results of surface acoustic wave (SAW)-induced lowering of coercivity in Galfenol films [6]. In the case of precessional (resonant) switching, two features are necessary: sizable magnetoacoustic coupling (to trigger precession), and a highly nonlinear system (to force wide, noncircular precession needed for magnetization reversal).…”
Section: Introductionmentioning
confidence: 99%
“…The elastically generated, out-ofplane torque [14,15] originates from the coupling of in-plane longitudinal strain [16], xx , to in-plane components, M x and M y , of magnetization vector:…”
Section: Experimental Techniquementioning
confidence: 99%
“…Fueled by potential applications in spintronics and sensorics thermal and magnetoelastic driven magnetic dynamics is attacking a great deal of research (Davis et al, 2010;Scherbakov et al, 2010;Roy et al, 2011;Uchida et al, 2011a;Weiler et al, 2011;Azovtsev and Pertsev, 2016). Elastic excitations might be triggered in a variety of ways, for instance via acoustic transducers (Davis et al, 2010;Uchida et al, 2011b;Weiler et al, 2011Weiler et al, , 2012Thevenard et al, 2013) or by optical methods (Scherbakov et al, 2010;Kim et al, 2012;Jäger et al, 2013;Kovalenko et al, 2013;Afanasiev et al, 2014). Optical methods mainly generate elastic excitations via laser heating and thermoelastic effects.…”
Section: Introductionmentioning
confidence: 99%