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Antiferromagnetic THz-frequency Josephson-like Oscillator Driven by Spin Current
by
Khymyn, Roman
, Lisenkov, Ivan
, Tiberkevich, Vasyl
, Slavin, Andrei
, Ivanov, Boris A.
in
639/766/119/1001
/ 639/766/119/2793
/ 639/766/25
/ Anisotropy
/ Electromagnetism
/ Energy
/ Heavy metals
/ Humanities and Social Sciences
/ Lasers
/ multidisciplinary
/ Oscillations
/ Oscillators
/ Science
/ Temperature effects
2017
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Antiferromagnetic THz-frequency Josephson-like Oscillator Driven by Spin Current
by
Khymyn, Roman
, Lisenkov, Ivan
, Tiberkevich, Vasyl
, Slavin, Andrei
, Ivanov, Boris A.
in
639/766/119/1001
/ 639/766/119/2793
/ 639/766/25
/ Anisotropy
/ Electromagnetism
/ Energy
/ Heavy metals
/ Humanities and Social Sciences
/ Lasers
/ multidisciplinary
/ Oscillations
/ Oscillators
/ Science
/ Temperature effects
2017
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Antiferromagnetic THz-frequency Josephson-like Oscillator Driven by Spin Current
by
Khymyn, Roman
, Lisenkov, Ivan
, Tiberkevich, Vasyl
, Slavin, Andrei
, Ivanov, Boris A.
in
639/766/119/1001
/ 639/766/119/2793
/ 639/766/25
/ Anisotropy
/ Electromagnetism
/ Energy
/ Heavy metals
/ Humanities and Social Sciences
/ Lasers
/ multidisciplinary
/ Oscillations
/ Oscillators
/ Science
/ Temperature effects
2017
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Antiferromagnetic THz-frequency Josephson-like Oscillator Driven by Spin Current
Journal Article
Antiferromagnetic THz-frequency Josephson-like Oscillator Driven by Spin Current
2017
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Overview
The development of compact and tunable room temperature sources of coherent THz-frequency signals would open a way for numerous new applications. The existing approaches to THz-frequency generation based on superconductor Josephson junctions (JJ), free electron lasers, and quantum cascades require cryogenic temperatures or/and complex setups, preventing the miniaturization and wide use of these devices. We demonstrate theoretically that a bi-layer of a heavy metal (Pt) and a bi-axial antiferromagnetic (AFM) dielectric (NiO) can be a source of a coherent THz signal. A spin-current flowing from a DC-current-driven Pt layer and polarized along the hard AFM anisotropy axis excites a non-uniform in time precession of magnetizations sublattices in the AFM, due to the presence of a weak easy-plane AFM anisotropy. The frequency of the AFM oscillations varies in the range of 0.1–2.0 THz with the driving current in the Pt layer from 10
8
A/cm
2
to 10
9
A/cm
2
. The THz-frequency signal from the AFM with the amplitude exceeding 1 V/cm is picked up by the inverse spin-Hall effect in Pt. The operation of a room-temperature AFM THz-frequency oscillator is similar to that of a cryogenic JJ oscillator, with the energy of the easy-plane magnetic anisotropy playing the role of the Josephson energy.
Publisher
Nature Publishing Group UK,Nature Publishing Group
Subject
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