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Bias-Field-Free Microwave Oscillator Driven by Perpendicularly Polarized Spin Current
In this paper, we propose a novel design of spin-torque-driven microwave oscillator that is free of bias magnetic field. The oscillator consists of a perpendicularly magnetized spin-polarization layer and an oscillating bilayer. The oscillating bilayer comprises a spin-torque-driven layer and a magn...
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Published in: | IEEE transactions on magnetics 2006-10, Vol.42 (10), p.2670-2672 |
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container_title | IEEE transactions on magnetics |
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creator | Zhu, X. Zhu, J.-G. |
description | In this paper, we propose a novel design of spin-torque-driven microwave oscillator that is free of bias magnetic field. The oscillator consists of a perpendicularly magnetized spin-polarization layer and an oscillating bilayer. The oscillating bilayer comprises a spin-torque-driven layer and a magnetic layer of perpendicular anisotropy with adequate interlayer-exchange coupling. The perpendicularly spin-polarized current can yield a sustained stable magnetization oscillation in the oscillating bilayer around the perpendicular easy axis. The oscillating frequency can be tuned from zero to tens of gigahertz by varying the inject current density. The underlying physical mechanism of the oscillation is discussed, and a micromagnetic analysis on the characteristics of the oscillator is reported |
doi_str_mv | 10.1109/TMAG.2006.879722 |
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The oscillator consists of a perpendicularly magnetized spin-polarization layer and an oscillating bilayer. The oscillating bilayer comprises a spin-torque-driven layer and a magnetic layer of perpendicular anisotropy with adequate interlayer-exchange coupling. The perpendicularly spin-polarized current can yield a sustained stable magnetization oscillation in the oscillating bilayer around the perpendicular easy axis. The oscillating frequency can be tuned from zero to tens of gigahertz by varying the inject current density. 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The underlying physical mechanism of the oscillation is discussed, and a micromagnetic analysis on the characteristics of the oscillator is reported</description><subject>Anisotropic magnetoresistance</subject><subject>Couplings</subject><subject>Cross-disciplinary physics: materials science; rheology</subject><subject>Current density</subject><subject>Design engineering</subject><subject>Exact sciences and technology</subject><subject>Frequency</subject><subject>Joining</subject><subject>Magnetic analysis</subject><subject>Magnetic fields</subject><subject>Magnetism</subject><subject>Magnetization</subject><subject>Materials science</subject><subject>Micromagnetic modeling</subject><subject>Micromagnetics</subject><subject>microwave</subject><subject>Microwave oscillators</subject><subject>Oscillating</subject><subject>Oscillations</subject><subject>oscillator</subject><subject>Oscillators</subject><subject>Other topics in materials science</subject><subject>perpendicular magnetic tunnel junction (MTJ)</subject><subject>Physics</subject><subject>Polarization</subject><subject>spin torque</subject><issn>0018-9464</issn><issn>1941-0069</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2006</creationdate><recordtype>article</recordtype><recordid>eNpdkE1LxDAQhoMouK7eBS9FELx0zbRpPo66uirssoJ6Dmk6hUhta7Jd0V9vlgqCp2FmnhleHkJOgc4AqLp6WV3fzzJK-UwKJbJsj0xAMUjjRO2TCaUgU8U4OyRHIbzFlhVAJ-T1xpmQLhw2VbrwiMnKWd99mi0m62Bd05hN55Nb77bYJuVX8oS-x7ZydmiMb2Lfxeq-sUqee9cm88F7bDfH5KA2TcCT3zolr4u7l_lDulzfP86vl6lloDYpClNXKKuiKHMDiiIrualrQ_PCZkKUlcyE4pBVHEqJgmHObYRlwRUYhDyfksvxb--7jwHDRr-7YDGmbrEbggYuIGOqkDSi5__Qt27wbUynJS-YBCUhQnSEooMQPNa69-7d-C8NVO80651mvdOsR83x5OL3rwnWNLU3rXXh705mNM9BRO5s5Bwi_q0FZYzS_AcYIYU3</recordid><startdate>20061001</startdate><enddate>20061001</enddate><creator>Zhu, X.</creator><creator>Zhu, J.-G.</creator><general>IEEE</general><general>Institute of Electrical and Electronics Engineers</general><general>The Institute of Electrical and Electronics Engineers, Inc. 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The oscillator consists of a perpendicularly magnetized spin-polarization layer and an oscillating bilayer. The oscillating bilayer comprises a spin-torque-driven layer and a magnetic layer of perpendicular anisotropy with adequate interlayer-exchange coupling. The perpendicularly spin-polarized current can yield a sustained stable magnetization oscillation in the oscillating bilayer around the perpendicular easy axis. The oscillating frequency can be tuned from zero to tens of gigahertz by varying the inject current density. The underlying physical mechanism of the oscillation is discussed, and a micromagnetic analysis on the characteristics of the oscillator is reported</abstract><cop>New York, NY</cop><pub>IEEE</pub><doi>10.1109/TMAG.2006.879722</doi><tpages>3</tpages></addata></record> |
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subjects | Anisotropic magnetoresistance Couplings Cross-disciplinary physics: materials science rheology Current density Design engineering Exact sciences and technology Frequency Joining Magnetic analysis Magnetic fields Magnetism Magnetization Materials science Micromagnetic modeling Micromagnetics microwave Microwave oscillators Oscillating Oscillations oscillator Oscillators Other topics in materials science perpendicular magnetic tunnel junction (MTJ) Physics Polarization spin torque |
title | Bias-Field-Free Microwave Oscillator Driven by Perpendicularly Polarized Spin Current |
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