1977
DOI: 10.1088/0022-3719/10/8/034
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The dielectric constant of gadolinium gallium garnet and α -Al2O3single crystals

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Cited by 19 publications
(7 citation statements)
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“…The saturation magnetization is µ 0 M s ≃ 175 mT for YIG [30], where the frequency corresponding to magnetization is ω M = gµ B µ 0 M s / ≃ 4.89 × 2π GHz. µ B is the Bohr magneton, the g-factor is g = 2, and the coherence length of the exchange interaction is λ ex ≃ 1.76×10 −8 m. The dielectric constant is ǫ M = 15 for YIG [31] and ǫ b = 12 for GGG [32].…”
Section: Resultsmentioning
confidence: 99%
“…The saturation magnetization is µ 0 M s ≃ 175 mT for YIG [30], where the frequency corresponding to magnetization is ω M = gµ B µ 0 M s / ≃ 4.89 × 2π GHz. µ B is the Bohr magneton, the g-factor is g = 2, and the coherence length of the exchange interaction is λ ex ≃ 1.76×10 −8 m. The dielectric constant is ǫ M = 15 for YIG [31] and ǫ b = 12 for GGG [32].…”
Section: Resultsmentioning
confidence: 99%
“…Literature survey shows that the work on electrical properties on garnets is limited. Electrical conductivity in GGG was reported by Krishan Lal and Jhans [8]. Dielectric constants on several gallium garnets at room temperature were reported by Shannon et.…”
Section: Introductionmentioning
confidence: 89%
“…While Pt has a strong optical absorption (~10 7 cm -1 ) 28 , enhanced by the Etalon effect 29 , the absorption in GGG|YIG (10 cm -1 ) is essentially negligible. 30,31 The electrons in Pt are heated within a few tens of femtoseconds 18 . At the short timescales after laser absorption (~ 1 ps) probed in our measurement, thermalisation of these hot electrons mainly occurs via two mechanisms.…”
Section: Takedownmentioning
confidence: 99%
“…The Pt layer has a strong optical absorption (~10 ] cm <`)28 that is enhanced by the Etalon effect 29 , while the absorption in GGG|YIG (10 cm <`) is essentially negligible. 30,31 We estimate that for an absorbed fluence of 0.15 mJ/cm 2 ∆ , bc ~200 K at 10 K 18 , taking the electron-phonon coupling constant M <de = 10 `f W • m <i K <` and the electron heat capacity j / = 750 J • m <i K <C . 32 To understand the origin of the temperature dependence of the picosecond LSSE in Fig.…”
mentioning
confidence: 99%