1964
DOI: 10.1103/physrev.134.a734
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Selection Rules and Angular Dependence in Paramagnetic Acoustic Resonance

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Cited by 75 publications
(16 citation statements)
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“…form of the phenomenological spin-phonon interaction Hamiltonian for these ions has been found in agreement with experiments 11,12 and is also well justified theoretically by the work of Van Vleck 13 and Mattuck and Strandberg. 14 In analogy with the spin Hamiltonian 3C.=/9H-g-S+S-D-S (1) the spin-phonon Hamiltonian is written…”
Section: Introductionsupporting
confidence: 81%
“…form of the phenomenological spin-phonon interaction Hamiltonian for these ions has been found in agreement with experiments 11,12 and is also well justified theoretically by the work of Van Vleck 13 and Mattuck and Strandberg. 14 In analogy with the spin Hamiltonian 3C.=/9H-g-S+S-D-S (1) the spin-phonon Hamiltonian is written…”
Section: Introductionsupporting
confidence: 81%
“…The similar results of Dobrov [43] and Tucker [37] strictly hold only for purely longitudinal phonons since CO~k had not been included in the denominator. In (8), the doublet excited state of the I A M] = 1 transition is already accounted for by a factor 2.…”
Section: W~-i(~l'l~t:1ltfi)12g(v)/(zh) 2 Where G(v)supporting
confidence: 61%
“…which is zero for local Ca symmetry [43] so that this transition should be forbidden. Eventually for transverse phonons along the c-axis (T 3):…”
Section: W~-i(~l'l~t:1ltfi)12g(v)/(zh) 2 Where G(v)mentioning
confidence: 97%
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