1974
DOI: 10.1103/physrevb.9.4512
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Scattering tensors and Clebsch-Gordan coefficients in crystals

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Cited by 35 publications
(11 citation statements)
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“…[see e.g. Birman & Berenson (1974) and Cracknell (1974)]. The essential step of the selection-rules derivations consists in the reduction of Kronecker products of space-group representations into irreducible .…”
Section: Direct Product Of Representations 41 the Problemmentioning
confidence: 99%
“…[see e.g. Birman & Berenson (1974) and Cracknell (1974)]. The essential step of the selection-rules derivations consists in the reduction of Kronecker products of space-group representations into irreducible .…”
Section: Direct Product Of Representations 41 the Problemmentioning
confidence: 99%
“…Raman tensors give the relative intensities of the same phonon in different scattering geometries. It has been shown that the Raman tensors are Clebsch-Gordon coefficients [16].…”
Section: Raman Effect For Ordinary Lightmentioning
confidence: 99%
“…We write the first-order Raman scattering tensor according to eq. (A4) of Birman and Berenson [21] as proportional to the CGcs rrz'| ~,z~ with a proportionality factor C(l'l"l) dependent on the representation labels l', l" and l. For the excitation of simmetry specified by representation l and representation row ~ the scattering tensor is…”
Section: -The First-order Raman Scattering Tensor In Hexagonal Icementioning
confidence: 99%
“…Birman and Berenson [21] have shown that elements of the first-order (one-excitation) scattering tensor P~(~) (jr) are appropriate Clebsch-Gordan coefficients or in case of multiplicity greater than one prescribed linear combinations; the elements (2) 9 ., P~ (jz; 3 r') of the second-order (two-excitation) scattering tensor are a particular sum of products of Clebsch-Gordan coefficients for reduction of the symmetrized square of vector representation into irreducible representations of the excitations involved in the scattering process [22,23]. In space group D~h of the uniaxial crystal of h.c.p, structure the vector representation is the direct sum of the unitary irreducible representations/'6-(Elu) and/'2-(A2,~) where we write the representation labels of ML [9] and add those of Herzberg [19] in the brackets:…”
Section: ~2=-~ (Jr) El~l 2 mentioning
confidence: 99%
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