Dipartimento di Fisica, Universitá di Roma La Sapienza", Rome, I-00185, Italy.
Istituto Italiano di Tecnologia, Center for Life Nano Science @Sapienza, Rome, I-00161, Italy.
Nat Commun. 2018 Jan 22;9(1):308. doi: 10.1038/s41467-017-02508-x.
The equilibrium optical phonons of graphene are well characterized in terms of anharmonicity and electron-phonon interactions; however, their non-equilibrium properties in the presence of hot charge carriers are still not fully explored. Here we study the Raman spectrum of graphene under ultrafast laser excitation with 3 ps pulses, which trade off between impulsive stimulation and spectral resolution. We localize energy into hot carriers, generating non-equilibrium temperatures in the ~1700-3100 K range, far exceeding that of the phonon bath, while simultaneously detecting the Raman response. The linewidths of both G and 2D peaks show an increase as function of the electronic temperature. We explain this as a result of the Dirac cones' broadening and electron-phonon scattering in the highly excited transient regime, important for the emerging field of graphene-based photonics and optoelectronics.
石墨烯的平衡光学声子在非谐性和电子-声子相互作用方面得到了很好的描述;然而,在存在热载流子的情况下,它们的非平衡性质仍未得到充分探索。在这里,我们研究了超快激光激发下石墨烯的喇曼光谱,使用的是 3 ps 脉冲,这种方法在脉冲激发和光谱分辨率之间进行了权衡。我们将能量局域到热载流子中,在~1700-3100 K 的范围内产生非平衡温度,远远超过声子浴的温度,同时检测喇曼响应。G 和 2D 峰的线宽都随着电子温度的增加而增加。我们将其解释为狄拉克锥展宽和在高度激发的瞬态状态下电子-声子散射的结果,这对于基于石墨烯的光子学和光电子学这一新兴领域非常重要。