Abstract:The performance of spintronic devices critically depends on three material parameters, namely, the spin polarization in the current (P), the intrinsic Gilbert damping (α), and the coefficient of the nonadiabatic spin transfer torque (β). However, there has been no method to determine these crucial material parameters in a self-contained manner. Here we show that P, α, and β can be simultaneously determined by performing a single series of time-domain measurements of current-induced spin wave dynamics in a ferr… Show more
“…3 Since the YIG is not compatible with standard silicon integrated circuit (IC) technology, spin wave propagation in ICcompatible materials such as FeNi is of importance for the realization of integrated circuits. [4][5][6][7][8][9][10][11][12][13][14] The magnetostatic surface wave (MSSW) in the FeNi film is the promising mode due to its high propagation velocity and a non-reciprocal character, which was also observed a long time ago in YIG films. [3][4][5] As revealed in the previous letter, 6 the nonreciprocal emission can be utilized for an initial input, since the non-reciprocal parameter (j) is unchanged even if a spin wave propagates a long distance.…”
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confidence: 99%
“…The detail geometry of ACPS and experimental method are the same as reported in the previous letters. 6,7 Spin wave wavevector k $ 0.5 lm À1 is determined by the ACPS geometry, which corresponds to the resonant frequency of approximately x=2p $ 3.6 GHz. The spin wave frequencies were not changed even if we changed the Pt content.…”
“…3 Since the YIG is not compatible with standard silicon integrated circuit (IC) technology, spin wave propagation in ICcompatible materials such as FeNi is of importance for the realization of integrated circuits. [4][5][6][7][8][9][10][11][12][13][14] The magnetostatic surface wave (MSSW) in the FeNi film is the promising mode due to its high propagation velocity and a non-reciprocal character, which was also observed a long time ago in YIG films. [3][4][5] As revealed in the previous letter, 6 the nonreciprocal emission can be utilized for an initial input, since the non-reciprocal parameter (j) is unchanged even if a spin wave propagates a long distance.…”
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confidence: 99%
“…The detail geometry of ACPS and experimental method are the same as reported in the previous letters. 6,7 Spin wave wavevector k $ 0.5 lm À1 is determined by the ACPS geometry, which corresponds to the resonant frequency of approximately x=2p $ 3.6 GHz. The spin wave frequencies were not changed even if we changed the Pt content.…”
“…The experimental results shown in the following are done with a magnetic field applied perpendicular to the film plane. We note that the droplet states can be affected by Joule heating [7], especially the FL precession [27,28]. We, thus, obtain our data by always keeping the electrical current constant and sweeping the magnetic fields.…”
Citation: LENDINEZ, S. ... et al, 2017. Effect of temperature on magnetic solitons induced by spin-transfer torque. Physical Review Applied, 7 (5), 054027.Additional Information:• This paper was accepted for publication in the jour- Spin-transfer torques in a nanocontact to an extended magnetic film can create spin waves that condense to form dissipative droplet solitons. Here we report an experimental study of the temperature dependence of the current and applied field thresholds for droplet soliton formation, as well as the nanocontact's electrical characteristics associated with droplet dynamics. Nucleation requires lower current densities at lower temperatures, in contrast to typical spin-transfer-torque-induced switching between static magnetic states. Magnetoresistance and electrical noise measurements (10 MHz-1 GHz) show that droplet solitons become more stable at lower temperature. These results are of fundamental interest in understanding the influence of thermal noise on droplet solitons and have implications for the design of devices using the spin-transfertorque effects to create and control collective spin excitations.
“…One of the first accomplishments of the stroboscopic methods has been the direct observation of the magnetization relaxation according to the LLG dynamics [18]. By investigating in the frequency range were stroboscopic methods can be applied we observe dynamical effects similar to those we are familiar with in the quasi-static regime, such as domain wall motion or nucleation of domains, but we also encounter new phenomena that require new theoretical approaches, such as fast switching by magnetization precession [19] [20], spin waves (magnetostatic, exchange, ...) [21], (whose spectrum can be continuous, or discrete in structured samples [22]), interaction of spin waves with domain walls and/or with spin polarized currents [23].…”
Section: Fast Magneto-optics: a Direct Approach To The High-frequencymentioning
We present a few significant advances in methods and concepts of magnetic measurements, aimed both at providing novel routes in the characterization of hard and soft magnetic materials and at improving our basic knowledge of the magnetization process. We discuss, in particular, investigation methods and experimental arrangements that have been developed in recent times for: 1) Hysteresis loop determination in extra-hard magnets by means of Pulsed Field Magnetometry; 2) Broadband observation of domain wall dynamics by highspeed stroboscopical Kerr techniques; 3) Entropy measurements in magnetocaloric materials by calorimetry in magnetic field. While pertaining to somewhat independent fields of investigation, all these measuring techniques have in common a solid approach to the underlying physical phenomenology and have a potential for further developments.
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