2004
DOI: 10.1103/physrevb.69.121414
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Phonon and plasmon excitation in inelastic electron tunneling spectroscopy of graphite

Abstract: The inelastic electron tunneling spectrum ͑IETS͒ of highly oriented pyrolitic graphite has been measured with scanning tunneling spectroscopy ͑STS͒ at 6 K. The observed spectral features are in very good agreement with the vibrational density of states of graphite calculated from first principles. We discuss the enhancement of certain phonon modes by phonon-assisted tunneling in STS based on the restrictions imposed by the electronic structure of graphite. We also demonstrate the local excitation of surface pl… Show more

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Cited by 89 publications
(79 citation statements)
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References 30 publications
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“…56͒ and for oscillations perpendicular to the layers are ប c = 45-50 meV. 42,[56][57][58] These values for ប a and ប c agree reasonably well with our derived value considering that we make the crude estimation of ប a and ប c at 0 K while experiments were carried out at room temperature. We also used average effective masses of the electron pocket in order to determine the plasmon frequency, while in fact there is a k z dependence ͑see Fig.…”
Section: Discussionsupporting
confidence: 89%
“…56͒ and for oscillations perpendicular to the layers are ប c = 45-50 meV. 42,[56][57][58] These values for ប a and ប c agree reasonably well with our derived value considering that we make the crude estimation of ប a and ប c at 0 K while experiments were carried out at room temperature. We also used average effective masses of the electron pocket in order to determine the plasmon frequency, while in fact there is a k z dependence ͑see Fig.…”
Section: Discussionsupporting
confidence: 89%
“…Due to the conservation of momentum, the effective barrier height of the tunneling junction is enhanced byh 2 K 2 /2m ≈ 11eV , so the probability of the elastic tunneling is reduced. [25][26][27] In inelastic tunneling, an electron at energy 67meV above the Fermi level can tunnel through the barrier with zero in plane momentum, through the emission of a K point out-of-plane phonon. [23] The barrier height for the inelastic tunneling is reduced by 11eV compared to that for the elastic tunneling, enhancing the probability of inelastic tunneling.…”
Section: Pacs Numbersmentioning
confidence: 99%
“…Using the graphite phonon density of states [35], we calculated the e-ph contribution to ImΣ (figure 3, green curve) with the standard formalism [36] and find an e-ph coupling constant λ ≈ 0.3. Although this is a factor of 5 larger than predicted [37] for n = 5.6 × 10 13 cm −2 , comparison with the experimental data shows that this provides an accurate description of ImΣ in region I.…”
Section: Many Body Interactions At Low Energy Scalesmentioning
confidence: 99%