2018
DOI: 10.1103/physrevmaterials.2.051401
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Strongly extended diffusion length for the nonequilibrium magnons in Y3Fe5O12 by photoexcitation

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Cited by 14 publications
(8 citation statements)
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“…To study the system frequency response to a direct excitation of the material like that related to the searched particle in ferromagnetic haloscopes, we photoexcite the material with 1064-nm wavelength, 11-ps duration laser pulses and measure the power stored in the HS modes for several values of applied magnetic field. At 1064 nm, the absorption coefficient of YIG is ~10 cm −1 64-66 , corresponding to the transition 6 A 1g ( 6 S) → 4 T 1g ( 4 G) between electronic levels in the octaedral crystal field configuration 67 . In addition, the laser beam is focused within the sphere and we can thus reasonably assume that the 0.1 mJ energy of the pulse is almost entirely absorbed in the material.…”
Section: Resultsmentioning
confidence: 99%
“…To study the system frequency response to a direct excitation of the material like that related to the searched particle in ferromagnetic haloscopes, we photoexcite the material with 1064-nm wavelength, 11-ps duration laser pulses and measure the power stored in the HS modes for several values of applied magnetic field. At 1064 nm, the absorption coefficient of YIG is ~10 cm −1 64-66 , corresponding to the transition 6 A 1g ( 6 S) → 4 T 1g ( 4 G) between electronic levels in the octaedral crystal field configuration 67 . In addition, the laser beam is focused within the sphere and we can thus reasonably assume that the 0.1 mJ energy of the pulse is almost entirely absorbed in the material.…”
Section: Resultsmentioning
confidence: 99%
“…To study the system frequency response to a direct excitation of the material like that related to the searched particle in ferromagnetic haloscopes, we photoexcite the material with 1064 nm-wavelength, 11 ps-duration laser pulses and measure the power stored in the HS modes for several values of applied magnetic field. At 1064 nm, the absorption coefficient of YIG is ∼ 10 cm −164-66 , corresponding to the transition 6 A 1g ( 6 S) → 4 T 1g ( 4 G) between electronic levels in the octaedral crystal field configuration 67 . In addition, the laser beam is focused within the sphere and we can thus reasonably assume that the 0.1 mJ energy of the pulse is almost entirely absorbed in the material.…”
Section: Experimental Validationmentioning
confidence: 99%
“…Another work indicates that light-thermally induced temperature gradients (i.e., SSE) can excite magnons in YIG. Furthermore, the long-wavelength light causes the Fe 3+ ions in the octahedra FeO 6 from a high-spin state to a low-spin state, which increases the magnetization of YIG and subsequently enhances the magnon diffusion length 13 . In addition, a solution that separates the interface temperature gradient and bulk temperature gradients has been provided to analyze their contributions to spin currents 14 .…”
Section: Introductionmentioning
confidence: 99%