2015
DOI: 10.1016/j.sse.2015.05.037
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Integration of GMR-based spin torque oscillators and CMOS circuitry

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Cited by 12 publications
(13 citation statements)
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“…This is because any parasitic will introduce an impedance mismatch much larger than a few Ohms. In this case, rather than maximizing the transferred power, an amplifier with large input impedance is preferable, since it can maximize the AC voltage delivered to the amplifier as well as the signal-to-noise ratio at the output [255].…”
Section: Stno/shno-based Applications: Issues Challenges and Devmentioning
confidence: 99%
“…This is because any parasitic will introduce an impedance mismatch much larger than a few Ohms. In this case, rather than maximizing the transferred power, an amplifier with large input impedance is preferable, since it can maximize the AC voltage delivered to the amplifier as well as the signal-to-noise ratio at the output [255].…”
Section: Stno/shno-based Applications: Issues Challenges and Devmentioning
confidence: 99%
“…Finally, the flip-chip-based integration of GMR spin torque oscillators (STO) onto RF CMOS integrated circuits has been reported in [ 31 ], by following a chip-on-board (CoB) approach, resulting in a GMR STO + CMOS IC pair working in the 8–16 GHz rang with 1.5 nV/ .…”
Section: Gmr Principlesmentioning
confidence: 99%
“…As STT can act as negative spin wave damping, it can realize magnetic systems where spin waves, instead of being damped out, can grow exponentially in amplitude, until additional non-linear damping balances the magnetodynamics and a steady state of intense spin wave generation is realized [4][5][6]. This auto-oscillatory state is the basis for spin torque nanooscillators (STNOs) with promise for use as ultra-broadband, rapidly modulated, truly nanoscopic, and RF CMOS compatible microwave signal generators [5][6][7][8][9][10][11][12][13][14][15][16][17].…”
Section: Introductionmentioning
confidence: 99%