1999
DOI: 10.1134/1.558909
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Lattice vibrations of α′-NaV2O5

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Cited by 28 publications
(39 citation statements)
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“…The opening of a gap in the magnetic excitation spectrum below T c leads to a vanishing of a low-frequency continuum and to the appropriate transformation of the line shapes. Subsequent structure redetermination for the HT phase of α ′ -NaV 2 O 5 [2][3][4][5] does not, however, allow to ascribe E a polarized spectral continuum to a pure twospinon absorption. Symmetry considerations show that for both HT-and LT-structure of α ′ -NaV 2 O 5 the two-spinon (two-magnon) absorption is allowed only in E c polarization [33,34].…”
Section: Resultsmentioning
confidence: 99%
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“…The opening of a gap in the magnetic excitation spectrum below T c leads to a vanishing of a low-frequency continuum and to the appropriate transformation of the line shapes. Subsequent structure redetermination for the HT phase of α ′ -NaV 2 O 5 [2][3][4][5] does not, however, allow to ascribe E a polarized spectral continuum to a pure twospinon absorption. Symmetry considerations show that for both HT-and LT-structure of α ′ -NaV 2 O 5 the two-spinon (two-magnon) absorption is allowed only in E c polarization [33,34].…”
Section: Resultsmentioning
confidence: 99%
“…2c represents the spectra of a 150 µm thick sample). The a-polarized FIR absorption continuum extends to about 1500 cm −1 and consists of two bands centered at 300 and 1100 cm −1 [31,5,32]. Drastic changes occur in the spectra of NaV 2 O 5 at the transition temperature.…”
Section: Resultsmentioning
confidence: 99%
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