2015
DOI: 10.1016/j.physleta.2014.11.044
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Wake effect in the interaction of slow correlated charges with supported graphene due to plasmon–phonon hybridization

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Cited by 11 publications
(10 citation statements)
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“…is the background dielectric function due to the substrate [63] described by a frequency-dependent dielectric function ε s (u) which is modeled in the local approximation (i.e., by neglecting spatial dispersion in the substrate) as a set of DrudeeLorentz oscillators,…”
Section: Theoretical Modelmentioning
confidence: 99%
“…is the background dielectric function due to the substrate [63] described by a frequency-dependent dielectric function ε s (u) which is modeled in the local approximation (i.e., by neglecting spatial dispersion in the substrate) as a set of DrudeeLorentz oscillators,…”
Section: Theoretical Modelmentioning
confidence: 99%
“…Gray (red) dashed lines mark the curves ω=0.5v F q, ω=2v F q, and ω=4v F q q c , and hence, it may also be accessed by the resonance condition for the lower speed of v=0.5v F , which falls in the subthreshold region of projectile speeds, v<v F . It was shown recently that this phonon branch survives Landau damping in the intra-band SPEs region and gives rise to a subthreshold wake effect due to plasmon-phonon hybridization in the graphene/SiO 2 system [42].…”
Section: Resultsmentioning
confidence: 97%
“…We have recently shown that the narrow localization of the wake pattern seen in Fig. 2b due to the plasmon-phonon hybrid mode may give rise to strong directionality in the interactions between two slow charges, which move over supported graphene at a finite distance from each other [42].…”
Section: Resultsmentioning
confidence: 99%
“…In the nanoscale devices, graphene layers typically appear in stacks [12,15] or sandwichlike structures [16] with insulating spacers between them made of polar materials, which often support strong Fuchs-Kliewer (FK), or surface optical phonon modes in the THz to mid-IR frequency range [17]. Those surface phonons strongly interact with longitudinal plasmon modes, and may therefore completely change the dispersion and damping of the Dirac plasmons in graphene [18][19][20][21], thereby seriously affecting its tunability for optoelectronic [12,17,[20][21][22] and plasmonic [23][24][25] applications in the range of frequencies of technological interest. While this provides strong motivation for a theoretical study of plasmon-phonon hybridization between graphene and the nearby polar insulator(s), a question arises as to how one can most effectively probe the hybridized plasmon-phonon modes.…”
Section: Introductionmentioning
confidence: 99%
“…Similar theoretical investigations were already conducted in Refs. [18,19], where the authors investigated hybridized plasmon-phonon modes in single-layer graphene deposited on an (experimentally often used) SiO 2 semi-infinite substrate.…”
Section: Introductionmentioning
confidence: 99%