Kuzmenko A B, Benfatto L, Cappelluti E, Crassee I, van der Marel D, Blake P, Novoselov K S, Geim A K
Département de Physique de la Matière Condensée, Université de Genève, CH-1211 Genève 4, Switzerland.
Phys Rev Lett. 2009 Sep 11;103(11):116804. doi: 10.1103/PhysRevLett.103.116804. Epub 2009 Sep 10.
We observe a giant increase of the infrared intensity and a softening of the in-plane antisymmetric phonon mode E(u) ( approximately 0.2 eV) in bilayer graphene as a function of the gate-induced doping. The phonon peak has a pronounced Fano-like asymmetry. We suggest that the intensity growth and the softening originate from the coupling of the phonon mode to the narrow electronic transition between parallel bands of the same character, while the asymmetry is due to the interaction with the continuum of transitions between the lowest hole and electron bands. The growth of the peak can be interpreted as a "charged-phonon" effect observed previously in organic chain conductors and doped fullerenes, which can be tuned in graphene with the gate voltage.
我们观察到,随着栅极诱导掺杂的变化,双层石墨烯中的红外强度大幅增加,面内反对称声子模式E(u)(约0.2电子伏特)发生软化。声子峰具有明显的类法诺不对称性。我们认为,强度增长和软化源于声子模式与相同性质平行能带之间狭窄电子跃迁的耦合,而不对称性则是由于与最低空穴带和电子带之间连续跃迁的相互作用。峰的增长可以解释为先前在有机链导体和掺杂富勒烯中观察到的“带电声子”效应,这种效应在石墨烯中可以通过栅极电压进行调节。