2012
DOI: 10.1088/0953-8984/24/10/104011
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Zero-phonon lines of systems with different dimensions and unconventional vibronic interactions

Abstract: The standard theory of the optical spectra of impurity centres in solids predicts the Lorentzian shape of the zero-phonon lines to have temperature-dependent position and width. However, in recent years different systems, including ones of reduced dimension, have been found, in which remarkable deviations from the standard laws have been observed. Generalizations of the theory to these systems are presented. Among other things, the quantum liquid 3He doped by optical centres is considered.

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Cited by 7 publications
(6 citation statements)
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“…5(a),(b) that linear Holstein coupling can consequently lead to a temperaturedependent zero-phonon line if there is a large density of low frequency (long wavelength) phonon modes with ω k < γ which is the case in 1D but not in higher dimensions. This peculiarity of dephasing in 1D has already been discussed in the literature [68,69,73]. It is however also well established within the literature that the major contribution of the experimentally observed broadening of the zero-phonon line is caused by a higher-order electron-phonon interaction of the form [70,[73][74][75]]…”
Section: Dephasingsupporting
confidence: 51%
See 1 more Smart Citation
“…5(a),(b) that linear Holstein coupling can consequently lead to a temperaturedependent zero-phonon line if there is a large density of low frequency (long wavelength) phonon modes with ω k < γ which is the case in 1D but not in higher dimensions. This peculiarity of dephasing in 1D has already been discussed in the literature [68,69,73]. It is however also well established within the literature that the major contribution of the experimentally observed broadening of the zero-phonon line is caused by a higher-order electron-phonon interaction of the form [70,[73][74][75]]…”
Section: Dephasingsupporting
confidence: 51%
“…In the continuum limit considered here, this spectral density would lead to a divergence of the integral in Eq. ( 24) due to the high density of low-frequency phonons, which is a well known problem for 1D crystals [68,69]. This issue can be resolved by considering only a finite-sized 1D crystal with a minimum phonon frequency ω min > 0.…”
Section: B Phonon Imprint On Spectramentioning
confidence: 99%
“…2). Acceptable fitting could not be achieved by the conventional T 4 dependence but required additional T 2 term to take into account softening of bonds in the excited electronic state in accordance of a modified model of the ZPL of impurity centers in solids [4].…”
Section: Methodsmentioning
confidence: 99%
“…5(a) and 5(b), we can see that linear Holstein coupling can consequently lead to a temperaturedependent zero-phonon line if there is a large density of low frequency (long wavelength) phonon modes with ω k < γ which is the case in 1D but not in higher dimensions. This peculiarity of dephasing in 1D has already been discussed in the literature [49,50,54]. It is however also well established within the literature that the major contribution of the experimentally observed temperature-dependent broadening of the zero-phonon line is caused by a higher-order electron-phonon interaction of the form [51,[54][55][56]]…”
Section: Dephasingmentioning
confidence: 53%
“…In the continuum limit considered here, this spectral density would lead to a divergence of the integral in Eq. (24) due to the high density of low-frequency phonons, which is a well known problem for 1D crystals [49,50]. This issue can be addressed by considering only a finite-sized 1D crystal with a minimum phonon frequency cutoff ω min > 0.…”
Section: B Phonon Imprint On Spectramentioning
confidence: 99%