2002
DOI: 10.1002/1521-3951(200211)234:2<644::aid-pssb644>3.0.co;2-e
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Zero-Phonon Lines: The Effect of a Strong Softening of Elastic Springs in the Excited State

Abstract: PACS: 63.20.Pw; 78.20.Ci The optical dephasing, caused by a quadratic interaction with acoustic phonons, is studied on the basis of the nonperturbative theory. The effect of a strong weakening of the elastic springs on the electronic transition is studied. It is found that, if the weakening brings the system close to the dynamical instability, then the usual / T 7 dependence of the homogeneous width of a zero-phonon line (ZPL) is replaced by the / T 3 dependence in a broad temperature interval. An equation … Show more

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Cited by 53 publications
(68 citation statements)
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“…The sum of the first and second terms, T 7 and T 3 , reflects the impact of electron-phonon coupling in the case of degenerate electronic states including the effect of softening of bonds in the colour centre excited state. At the same time, the dominance of the T 3 term was verified for N-V centre [26]. The third term T 5 is characteristic for the temperature dependence of the ZPL width under the action of dynamic Jahn-Teller effect in the involved degenerate electronic state.…”
Section: Lorentzian and Two Gaussian Curvesmentioning
confidence: 67%
“…The sum of the first and second terms, T 7 and T 3 , reflects the impact of electron-phonon coupling in the case of degenerate electronic states including the effect of softening of bonds in the colour centre excited state. At the same time, the dominance of the T 3 term was verified for N-V centre [26]. The third term T 5 is characteristic for the temperature dependence of the ZPL width under the action of dynamic Jahn-Teller effect in the involved degenerate electronic state.…”
Section: Lorentzian and Two Gaussian Curvesmentioning
confidence: 67%
“…PL data for the NV 0 center are reported again for comparison. The T 3 dependence of the FWHM peaks, highlighted by the fitting lines, is associated with the softening of the chemical bonds of the defect complex and results in a stronger coupling of its excited state with lattice phonons [23]. The FWHM increase versus temperature is less pronounced for HR centers with respect to the NV 0 emission, indicating that the former are characterized by a lower phonon coupling, as confirmed by their weaker phonon sidebands.…”
Section: Figure 2(b)mentioning
confidence: 92%
“…The adiabatic potential of the E-state is given by the matrix V 2 in the diagonal representation; it has the form of the Mexican hat [15,[9][10][11]. The vibronic E-state is invariant with respect to the rotation of the q 1 ; q 2 -surface through an arbitrary angle f with the simultaneous rotation of the electronic basis states on the angle 2j: In polar coordinates r ¼ ðq 2 1 þ q 2 2 Þ 1=2 and f ¼ arctanðq 2 =q 1 Þ the adiabatic potentials do not depend on j:…”
Section: A 1 -And E-electronic Statesmentioning
confidence: 99%
“…: If one takes into account also the quadratic vibronic interaction in the E-state, then the f-dependent term appears in the APES of this state [15,[9][10][11] …”
Section: A 1 -And E-electronic Statesmentioning
confidence: 99%
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