Alexey B. Kuzmenko - Optics @ Unige - Université de Genève
Alexey B. Kuzmenko - Optics @ Unige - Université de Genève
Alexey B. Kuzmenko - Optics @ Unige - Université de Genève
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Couplings between charge, spin, orbital and lattice <strong>de</strong>grees of freedom in solids<br />
Superconductivity<br />
Most significant scientific results<br />
Discovery of a giant Faraday rotation (up to 6 <strong>de</strong>grees) in single atomic graphene layer on SiC and its<br />
explanation as due to the cyclotron resonance [I. Crassee et al. arxiv: 1007:5286, submitted to Nature<br />
Physics].<br />
First observation of a strong doping <strong>de</strong>pen<strong>de</strong>nce of the intensity and the Fano asymmetry of the<br />
infrared phonon G-peak in electrostatically gated bilayer graphene. An explanation of this effect<br />
using the theories of Fano and Rice.This can be used for a contact-free characterization of graphene<br />
[A.B.<strong>Kuzmenko</strong> et al., Phys. Rev. Lett. 103, 116804 (2009); E.Cappelluti et al., Phys. Rev. B 82<br />
041402(R) (2010)].<br />
Optical measurement of the electric-field induced bandgap in gated bilayer graphene [A.B.<br />
<strong>Kuzmenko</strong> et al., Phys. Rev. B 80 165406 (2009)]. The existence of this gap is extremely important<br />
for applications of graphene in electronics. Our paper appeared simultaneously with two other<br />
in<strong>de</strong>pen<strong>de</strong>nt papers reporting similar results [K.F. Mak et al. Rev. Lett. 102, 256405 (2009) and Y.<br />
Zhang et al.Nature 459, 820 (2009)]. However, in contrast to other papers, we extracted selfconsistently<br />
all tight-binding (SWMcC) parameters from the same set of optical data.<br />
2<br />
Experimental <strong>de</strong>monstration that the optical conductivity of graphite is equal to e / 4h<br />
[A.B.<br />
<strong>Kuzmenko</strong> et al., Phys. Rev. Lett. 100, 117401 (2008)], which is the universal value expected for<br />
monolayer graphene. In the same paper we predicted that the optical transmission of monolayer<br />
graphene should be <strong>de</strong>pen<strong>de</strong>nt only on the fine-structure constant: T = 1−<br />
πα . This was in<strong>de</strong>ed<br />
experimentally found in the group of A.K. Geim [R.R: Nair et al., Science 320, 1308 (2008)]. This<br />
universal behaviour is of fundamental importance for the optical applications of graphene.<br />
Establishing the two-band nature of the superconductivity in MgB2 using optical measurements [A.B.<br />
<strong>Kuzmenko</strong> et al., Solid State Commun.121, 479 (2002)] and theoretical input [I.I. Mazin et al., Phys.<br />
Rev. Lett. 89, 107002 (2002)].<br />
Systematic study of the optical sum rules in a high-temperature superconductor Bi2212 as function of<br />
doping [A.B. <strong>Kuzmenko</strong> et al. Phys. Rev. B. 72, 144503 (2005), F, Carbone et al., Phys. Rev. B. 74,<br />
064510 (2006)]. It was shown that in the optimally and un<strong>de</strong>rdoped regime the total Dru<strong>de</strong> weight<br />
increases when entering the superconducting state, which implies a possible lowering of the<br />
electronic kinetic energy below the SC transition, contrary to the predictions of the BCS theory.<br />
However, in the overdoped regime, the BCS-like behaviour is observed. These finding have<br />
important implications for the mechanism of superconductivity in the high-Tc cuprates, which is not<br />
yet un<strong>de</strong>rstood.<br />
Development of a novel Kramers-Kronig constrained variational method of the analysis of optical<br />
spectra [A.B. <strong>Kuzmenko</strong>, Rev. Sci. Instrum.76, 083108 (2005)], allowing the analysis of a great<br />
variety of spectroscopic data. This method I implemented in a freely available program RefFIT<br />
[http://optics.unige.ch/alexey/reffit.html], used at present by more the 50 optics groups in the world.<br />
Observation of a strong spin-phonon coupling and an anomalous phonon softening in cupric oxi<strong>de</strong><br />
CuO [Phys. Rev. B 63, 094303 (2001)], which was found later to be multiferroic. This material is a<br />
parent compound of high-Tc cuprates. It is also wi<strong>de</strong>ly used in the production of various<br />
nanostructures.<br />
References