1963
DOI: 10.1109/t-ue.1963.29301
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Microwave Photon Generation by Thin Magnetic Films

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1965
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Cited by 18 publications
(2 citation statements)
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“…This indicates that the high-frequency mode originates from the coherent LA phonon generation in GaAs buffer, and the low-frequency mode should be associated with the coherent LA phonon generation in Co 2 FeAl layer [38,40] . Recall that the optical penetration depth at 800 nm for Co 2 FeAl is only ~ 17.6 nm [47] , the greatly attenuated pumping intensity passing through a thick Co 2 FeAl (45 nm) layer will be too weak to optically excite coherent phonons in the underneath GaAs, thus the detected coherent phonon responses from a thick Co 2 FeAl layer and its underneath GaAs buffer should mainly arise from the magnetoelastic coupling [48][49][50][51][52][53] . As for the mode with a frequency of ~34 GHz, its negligible frequency dependence on the probe wavelength suggests that this mode may not be the coherent acoustic phonon response in Co 2 FeAl/GaAs heterostructure.…”
Section: Resultsmentioning
confidence: 99%
“…This indicates that the high-frequency mode originates from the coherent LA phonon generation in GaAs buffer, and the low-frequency mode should be associated with the coherent LA phonon generation in Co 2 FeAl layer [38,40] . Recall that the optical penetration depth at 800 nm for Co 2 FeAl is only ~ 17.6 nm [47] , the greatly attenuated pumping intensity passing through a thick Co 2 FeAl (45 nm) layer will be too weak to optically excite coherent phonons in the underneath GaAs, thus the detected coherent phonon responses from a thick Co 2 FeAl layer and its underneath GaAs buffer should mainly arise from the magnetoelastic coupling [48][49][50][51][52][53] . As for the mode with a frequency of ~34 GHz, its negligible frequency dependence on the probe wavelength suggests that this mode may not be the coherent acoustic phonon response in Co 2 FeAl/GaAs heterostructure.…”
Section: Resultsmentioning
confidence: 99%
“…The landmark is probably the seminal paper of Kittel [75], who explained the benefits of coupling acoustic-waves (AW) with spin-waves (SW) in order to confer to the former waveform a tunable and non-reciprocal character. Since then, the subject has accumulated a vast amount of literature that spans a wide range of ferromagnetic materials from metals [108], to magnetic semiconductors [109,110], and electrical insulators [111,112,113]. From the start, ferrite garnets [114] have been the subject of an intense focus because of their ultra-low internal frictions.…”
Section: Magneto-elastic Couplingmentioning
confidence: 99%

Spin Insulatronics

Brataas,
van Wees,
Klein
et al. 2020
Preprint