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Hideo Ohno - One of the best experts on this subject based on the ideXlab platform.

  • electric field effect on spin wave resonance in a nanoscale cofeb mgo Magnetic Tunnel Junction
    Applied Physics Letters, 2017
    Co-Authors: Takaaki Dohi, Shun Kanai, F Matsukura, Hideo Ohno
    Abstract:

    We investigate the electric-field effect on the exchange stiffness constant in a CoFeB/MgO Junction through the observation of the spin-wave resonance in a nanoscale Magnetic Tunnel Junction. We evaluate the electric-field dependence of the stiffness constant from the separation between resonance fields for the Kittel and spin-wave modes under electric fields. The obtained stiffness constant increases when the interfacial electron density is decreased. This dependence is consistent with that determined from the observation of electric-field dependent domain structures.

  • in plane anisotropy of a nano scaled Magnetic Tunnel Junction with perpendicular Magnetic easy axis
    Japanese Journal of Applied Physics, 2015
    Co-Authors: Eriko Hirayama, Shoji Ikeda, Shun Kanai, H Sato, F Matsukura, Koji Sato, Michihiko Yamanouchi, Hideo Ohno
    Abstract:

    We investigate Magnetic properties of a 100-nm-diameter CoFeB/MgO Magnetic Tunnel Junction (MTJ) with perpendicular Magnetic easy axis by homodyne-detected ferroMagnetic resonance (FMR) and Junction resistance measurements. The resonant frequency depends clearly on the direction of the in-plane Magnetic field, which is also the case for the angle dependence of the Junction resistance. A good correspondence between the two independent measurements indicates the presence of unintentionally introduced in-plane Magnetic anisotropy in the present MTJ.

  • magnetization switching in a cofeb mgo Magnetic Tunnel Junction by combining spin transfer torque and electric field effect
    Applied Physics Letters, 2014
    Co-Authors: Shun Kanai, H Sato, M Yamanouchi, F Matsukura, Yoshinobu Nakatani, Hideo Ohno
    Abstract:

    We propose and demonstrate a scheme for magnetization switching in Magnetic Tunnel Junctions, in which two successive voltage pulses are applied to utilize both spin-transfer torque and electric field effect. Under this switching scheme, a CoFeB/MgO Magnetic Tunnel Junction with perpendicular Magnetic easy axis is shown to switch faster than by spin-transfer torque alone and more reliably than that by electric fields alone.

  • wide operational margin capability of 1 kbit spin transfer torque memory array chip with 1 pmos and 1 bottom pin Magnetic Tunnel Junction type cell
    Japanese Journal of Applied Physics, 2014
    Co-Authors: H Koike, Shoji Ikeda, Takashi Ohsawa, Hideo Ohno, Takahiro Hanyu, Hiroaki Honjo, Sadahiko Miura, Tetsuo Endoh
    Abstract:

    This paper discusses the optimal combination of 1 transistor (T) and 1 Magnetic Tunnel Junction (MTJ) type cell for spin transfer torque memory. Taking into consideration of current magnitude for both the T and the MTJ, either PMOS — bottom pin structure or NMOS — top pin structure can be a promising choice. Focusing on the PMOS–bottom pin structure from the viewpoint of avoiding process difficulty, we clarified the condition that the structure would be effective. In order to verify the structure's effectiveness, a stand-alone MTJ test element group and a 1 kbit memory array chip were designed and fabricated with 90 nm CMOS/100 nm MTJ process. With the pass bit percentage measurement of the memory chip, we successfully demonstrated that 1-PMOS and 1-bottom-pin-MTJ has the wide operation margin of 100% pass at near 1.6 V. It will be an effective solution for 1T–1MTJ memories.

  • comprehensive study of cofeb mgo Magnetic Tunnel Junction characteristics with single and double interface scaling down to 1x nm
    International Electron Devices Meeting, 2013
    Co-Authors: H Sato, Naoki Kasai, T Yamamoto, M Yamanouchi, Shunsuke Fukami, Keizo Kinoshita, F Matsukura, Hideo Ohno
    Abstract:

    We study characteristics of CoFeB-MgO Magnetic Tunnel Junction with perpendicular easy-axis (p-MTJ) at a reduced dimension down to 1X nm fabricated by hard-mask process. CoFeB-MgO p-MTJ with double-interface shows higher thermal stability down to 1X nm than that with single-interface. Thermal stability factor of 58 and intrinsic critical current of 24 μA are obtained in the CoFeB-MgO Magnetic Tunnel Junction with perpendicular easy-axis using double-interface structure at a diameter of 20 nmφ.

Shun Kanai - One of the best experts on this subject based on the ideXlab platform.

  • electric field effect on spin wave resonance in a nanoscale cofeb mgo Magnetic Tunnel Junction
    Applied Physics Letters, 2017
    Co-Authors: Takaaki Dohi, Shun Kanai, F Matsukura, Hideo Ohno
    Abstract:

    We investigate the electric-field effect on the exchange stiffness constant in a CoFeB/MgO Junction through the observation of the spin-wave resonance in a nanoscale Magnetic Tunnel Junction. We evaluate the electric-field dependence of the stiffness constant from the separation between resonance fields for the Kittel and spin-wave modes under electric fields. The obtained stiffness constant increases when the interfacial electron density is decreased. This dependence is consistent with that determined from the observation of electric-field dependent domain structures.

  • in plane anisotropy of a nano scaled Magnetic Tunnel Junction with perpendicular Magnetic easy axis
    Japanese Journal of Applied Physics, 2015
    Co-Authors: Eriko Hirayama, Shoji Ikeda, Shun Kanai, H Sato, F Matsukura, Koji Sato, Michihiko Yamanouchi, Hideo Ohno
    Abstract:

    We investigate Magnetic properties of a 100-nm-diameter CoFeB/MgO Magnetic Tunnel Junction (MTJ) with perpendicular Magnetic easy axis by homodyne-detected ferroMagnetic resonance (FMR) and Junction resistance measurements. The resonant frequency depends clearly on the direction of the in-plane Magnetic field, which is also the case for the angle dependence of the Junction resistance. A good correspondence between the two independent measurements indicates the presence of unintentionally introduced in-plane Magnetic anisotropy in the present MTJ.

  • electric field induced ferroMagnetic resonance in a cofeb mgo Magnetic Tunnel Junction under dc bias voltages
    Applied Physics Letters, 2014
    Co-Authors: Shun Kanai, F Matsukura, Daniel C Worledge, Martin Gajek, H Ohno
    Abstract:

    We measure homodyne-detected ferroMagnetic resonance (FMR) induced by the electric-field effect in a CoFeB/MgO/CoFeB Magnetic Tunnel Junction (MTJ) with perpendicular Magnetic easy axis under dc bias voltages up to 0.1 V. From the bias dependence of the resonant frequency, we find that the first order perpendicular Magnetic anisotropy is modulated by the applied electric field, whereas the second order component is virtually independent of the electric field. The lineshapes of the FMR spectra are bias dependent, which are explained by the combination of electric-field effect and reflection of the bias voltage from the MTJ.

  • magnetization switching in a cofeb mgo Magnetic Tunnel Junction by combining spin transfer torque and electric field effect
    Applied Physics Letters, 2014
    Co-Authors: Shun Kanai, H Sato, M Yamanouchi, F Matsukura, Yoshinobu Nakatani, Hideo Ohno
    Abstract:

    We propose and demonstrate a scheme for magnetization switching in Magnetic Tunnel Junctions, in which two successive voltage pulses are applied to utilize both spin-transfer torque and electric field effect. Under this switching scheme, a CoFeB/MgO Magnetic Tunnel Junction with perpendicular Magnetic easy axis is shown to switch faster than by spin-transfer torque alone and more reliably than that by electric fields alone.

  • observation of boron diffusion in an annealed ta cofeb mgo Magnetic Tunnel Junction with standing wave hard x ray photoemission
    Applied Physics Letters, 2012
    Co-Authors: A A Greer, Shun Kanai, A X Gray, Shigenori Ueda, Yoshiyuki Yamashita, A M Kaiser, C Bordel, Gunnar K Palsson, N Maejima, Seehun Yang
    Abstract:

    The CoFeB/MgO system shows promise as a Magnetic Tunnel Junction with perpendicular magnetization and low critical current densities for spin-torque driven magnetization switching. The distribution of B after annealing is believed to be critical to performance. We have studied the distribution of B in a Ta/Co0.2Fe0.6B0.2/MgO sample annealed at 300 °C for 1 h with standing-wave hard x-ray photoemission spectroscopy (SW-HXPS). Comparing experimental rocking curve data to x-ray optical calculations indicates diffusion of 19.5% of the B uniformly into the MgO and of 23.5% into a thin TaB interface layer. SW-HXPS is effective for probing depth distributions in such spintronic structures.

F Matsukura - One of the best experts on this subject based on the ideXlab platform.

H Sato - One of the best experts on this subject based on the ideXlab platform.

M Yamanouchi - One of the best experts on this subject based on the ideXlab platform.

  • magnetization switching in a cofeb mgo Magnetic Tunnel Junction by combining spin transfer torque and electric field effect
    Applied Physics Letters, 2014
    Co-Authors: Shun Kanai, H Sato, M Yamanouchi, F Matsukura, Yoshinobu Nakatani, Hideo Ohno
    Abstract:

    We propose and demonstrate a scheme for magnetization switching in Magnetic Tunnel Junctions, in which two successive voltage pulses are applied to utilize both spin-transfer torque and electric field effect. Under this switching scheme, a CoFeB/MgO Magnetic Tunnel Junction with perpendicular Magnetic easy axis is shown to switch faster than by spin-transfer torque alone and more reliably than that by electric fields alone.

  • comprehensive study of cofeb mgo Magnetic Tunnel Junction characteristics with single and double interface scaling down to 1x nm
    International Electron Devices Meeting, 2013
    Co-Authors: H Sato, Naoki Kasai, T Yamamoto, M Yamanouchi, Shunsuke Fukami, Keizo Kinoshita, F Matsukura, Hideo Ohno
    Abstract:

    We study characteristics of CoFeB-MgO Magnetic Tunnel Junction with perpendicular easy-axis (p-MTJ) at a reduced dimension down to 1X nm fabricated by hard-mask process. CoFeB-MgO p-MTJ with double-interface shows higher thermal stability down to 1X nm than that with single-interface. Thermal stability factor of 58 and intrinsic critical current of 24 μA are obtained in the CoFeB-MgO Magnetic Tunnel Junction with perpendicular easy-axis using double-interface structure at a diameter of 20 nmφ.

  • three terminal Magnetic Tunnel Junction utilizing the spin hall effect of iridium doped copper
    Applied Physics Letters, 2013
    Co-Authors: M Yamanouchi, H Sato, Shunsuke Fukami, F Matsukura, Lin Chen, J Kim, Masamitsu Hayashi, Hideo Ohno
    Abstract:

    We show a three terminal Magnetic Tunnel Junction (MTJ) with a 10-nm thick channel based on an interconnection material Cu with 10% Ir doping. By applying a current density of less than 1012 A m−2 to the channel, depending on the current direction, switching of a MTJ defined on the channel takes place. We show that spin transfer torque (STT) plays a critical role in determining the threshold current. By assuming the spin Hall effect in the channel being the source of the STT, the lower bound of magnitude of the spin Hall angle is evaluated to be 0.03.

  • electric field induced magnetization reversal in a perpendicular anisotropy cofeb mgo Magnetic Tunnel Junction
    Applied Physics Letters, 2012
    Co-Authors: Shun Kanai, Shoji Ikeda, M Yamanouchi, Yoshinobu Nakatani, Hideo Ohno
    Abstract:

    The electric field-induced ∼180° magnetization reversal is realized for a sputtered CoFeB/MgO-based Magnetic Tunnel Junction with perpendicular Magnetic easy axis in a static external Magnetic field. Application of bias voltage with nanoseconds duration results in a temporal change of Magnetic easy axis in the free layer CoFeB to in-plane, which induces precessional motion of magnetization in the free layer. The magnetization reversal takes place when the bias voltage pulse duration is adjusted to a half period of the precession. We show that the back and forth magnetization reversal can be observed by using successive application of half-period voltage pulses.