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Volumn 63, Issue 24, 2001, Pages

Theory of resonant Raman scattering of tetrahedral amorphous carbon

Author keywords

[No Author keywords available]

Indexed keywords

CARBON;

EID: 0034907347     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.63.245415     Document Type: Article
Times cited : (34)

References (22)
  • 6
    • 85038277752 scopus 로고    scopus 로고
    • Here and in the following we will use atomic units, with which (formula presented)
    • Here and in the following we will use atomic units, with which (formula presented).
  • 7
    • 0000088041 scopus 로고
    • E. Marx, Akademische Verlagsgesellschaft, Leipzig, in, edited by, p
    • G. Placzek, in Handbuch der Radiologie, edited by E. Marx (Akademische Verlagsgesellschaft, Leipzig, 1934), Vol. 6, p. 209.
    • (1934) Handbuch der Radiologie , vol.6 , pp. 209
    • Placzek, G.1
  • 11
    • 0003444152 scopus 로고
    • Clarendon Press and Oxford University Press, New York
    • R. Loudon, The Quantum Theory of Light (Clarendon Press and Oxford University Press, New York, 1983).
    • (1983) The Quantum Theory of Light
    • Loudon, R.1
  • 19
    • 85038346417 scopus 로고    scopus 로고
    • To perform the projection we have defined for each bond a ‘stretching’ vector in the space of the (formula presented) displacements. The components of each vector involve the displacement of two atoms in the direction of the bond and with opposite orientations. We use these vectors as a (non-orthonormal) basis of the stretching subspace. We define the bending subspace as the complement of the stretching subspace
    • To perform the projection we have defined for each bond a ‘stretching’ vector in the space of the (formula presented) displacements. The components of each vector involve the displacement of two atoms in the direction of the bond and with opposite orientations. We use these vectors as a (non-orthonormal) basis of the stretching subspace. We define the bending subspace as the complement of the stretching subspace.
  • 22
    • 85038270529 scopus 로고    scopus 로고
    • In the expression of intensity, Eq. (12), (formula presented) where the contributions (formula presented) and (formula presented) are obtained substituting in Eq. (14) the vibrational eigenvector (formula presented) with its projections in the stretching and bending subspaces, respectively. The intensity is then proportional to (formula presented). The first two terms correspond to the contributions of stretching and bending modes, respectively, whereas the last term corresponds to the overlap term. A similar repartition is used to define the (formula presented) and (formula presented) contributions
    • In the expression of intensity, Eq. (12), (formula presented) where the contributions (formula presented) and (formula presented) are obtained substituting in Eq. (14) the vibrational eigenvector (formula presented) with its projections in the stretching and bending subspaces, respectively. The intensity is then proportional to (formula presented). The first two terms correspond to the contributions of stretching and bending modes, respectively, whereas the last term corresponds to the overlap term. A similar repartition is used to define the (formula presented) and (formula presented) contributions.


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