2017
DOI: 10.1088/1361-6463/aa628a
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Imaging magnetisation dynamics in nano-contact spin-torque vortex oscillators exhibiting gyrotropic mode splitting

Abstract: Nano-contact spin-torque vortex oscillators (STVOs) are anticipated to find application as nanoscale sources of microwave emission in future technological applications. Presently the output power and phase stability of individual STVOs are not competitive with existing oscillator technologies. Synchronisation of multiple nano-contact STVOs via magnetisation dynamics has been proposed to enhance the microwave emission. The control of device-todevice variations, such as mode splitting of the microwave emission, … Show more

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Cited by 14 publications
(11 citation statements)
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“…The nanocontact vortex oscillator [23][24][25][26][27][28][29][30] represents an intriguing example, where different commensurate and incommensurate states appear due to competing selfoscillations [27]. The primary oscillation is driven by spin torques and involves self-sustained vortex gyration around the nanocontact [24], which is accompanied by relaxation oscillations in the form of periodic core reversal above a threshold current.…”
mentioning
confidence: 99%
“…The nanocontact vortex oscillator [23][24][25][26][27][28][29][30] represents an intriguing example, where different commensurate and incommensurate states appear due to competing selfoscillations [27]. The primary oscillation is driven by spin torques and involves self-sustained vortex gyration around the nanocontact [24], which is accompanied by relaxation oscillations in the form of periodic core reversal above a threshold current.…”
mentioning
confidence: 99%
“…4(d)]. Such a double-frequency mode has been observed in other STNOs [40][41][42][43][44][45][46], and can either result from the hopping between two frequencies, or from the simultaneous emission of two frequencies. Such cases are discussed in more detail in the following section.…”
Section: Frequency Domain Analysismentioning
confidence: 73%
“…Proof. The estimate (46) follows directly from (37), (42), and (45). For TPS1 and TPS2, also the geometric estimate (33a) is used to conclude that ∂ t m hk L 2 (Ω T ) ≤ C. The convergence (47) for PF-TPS1 follows from Proposition 5.3.…”
Section: Extraction Of Weakly Convergent Subsequencesmentioning
confidence: 98%
“…The presented experiment is a preliminary study to investigate the stability and the dynamics of a skyrmion in the presence of a field pulse. This is done to explore the possibility to use time-resolved scanning Kerr microscopy [37] which is based on the interplay between laser and field pulses to directly map the dynamics of magnetic skyrmions [38].…”
Section: Field-induced Dynamics Of Skyrmions In Nanodisksmentioning
confidence: 99%