2013
DOI: 10.1109/jproc.2013.2260115
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Plasmons in Graphene: Fundamental Properties and Potential Applications

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Cited by 233 publications
(186 citation statements)
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“…In this context, we notice that the ČR rate increases for higher frequencies (ČR is even observed in the x-ray range at narrow spectral windows [53]), where the difference between the quantum and the conventional ČR effects is considerably larger. A different alternative would be to use artificial materials with a very high index of refraction [54], or to use materials like graphene, where very high refractive indices already exist, reaching 200-300 for plasmons propagating in it [55]. Intriguingly, the quantum ČR becomes of great importance for bound charge carriers that cross the Čerenkov velocity threshold inside a medium [56] because their effective mass can be very low, thus making the ratio ℏω=E i significantly larger, even going above unity.…”
Section: Quantum Derivation: the Rate Of Emissionmentioning
confidence: 99%
“…In this context, we notice that the ČR rate increases for higher frequencies (ČR is even observed in the x-ray range at narrow spectral windows [53]), where the difference between the quantum and the conventional ČR effects is considerably larger. A different alternative would be to use artificial materials with a very high index of refraction [54], or to use materials like graphene, where very high refractive indices already exist, reaching 200-300 for plasmons propagating in it [55]. Intriguingly, the quantum ČR becomes of great importance for bound charge carriers that cross the Čerenkov velocity threshold inside a medium [56] because their effective mass can be very low, thus making the ratio ℏω=E i significantly larger, even going above unity.…”
Section: Quantum Derivation: the Rate Of Emissionmentioning
confidence: 99%
“…26 In the above, E F is the Fermi energy of the graphene substrate, which is directly related to the electron carrier density, and τ is the empirical relaxation time corresponding to losses that can generally be a function of frequency and vary with the Fermi energy. 26 In this work we neglect the dependence of τ on E F but it can be accounted for using results of density functional theory analysis.…”
Section: Methodsmentioning
confidence: 99%
“…26 In the above, E F is the Fermi energy of the graphene substrate, which is directly related to the electron carrier density, and τ is the empirical relaxation time corresponding to losses that can generally be a function of frequency and vary with the Fermi energy. 26 In this work we neglect the dependence of τ on E F but it can be accounted for using results of density functional theory analysis. 27 While the local model is more precise and has been demonstrated to well-describe flourescence quenching experiments in graphene, 28 we also consider the Drude model to connect to other 2D metals and also other Drude metals featuring high local density of states.…”
Section: Methodsmentioning
confidence: 99%
“…The confinement of GPs to plasmon wavelengths over 200 times smaller than the free space wavelength has been predicted [1,[26][27][28], with very recent work suggesting that much higher confinements are also achievable [29]. Importantly, the observed plasmon lifetimes are gradually improving due to higher quality samples and fabrications of Van der Waals heterostructures [3], and are expected to increase further with advances in fabrication techniques (e.g., [30]).…”
mentioning
confidence: 96%
“…Looking beyond graphene, the concept presented here is applicable to other 2D materials that support surface plasmons. Examples include bi-layer graphene [50], and single atomic layers of silver and gold, which have been shown in very recent works to have high confinement factors while also having higher frequencies than GPs [1].…”
mentioning
confidence: 99%