Magneto-optical conductivity in graphene
By Valery P. Gusynin, S. Sharapov, J. P. Carbotte. 2007
1,010 citations recorded by the source corpus.
Landau level quantization in graphene reflects the Dirac nature of its quasiparticles and has been found to exhibit an unusual integer quantum Hall effect. In particular, the lowest Landau level can be thought of as shared equally by electrons and holes, and this leads to characteristic behaviour of the magneto-optical conductivity as a function of frequency Ω for various values of the chemical potential μ. Particular attention is paid to the optical spectral weight under various absorption peaks and its redistribution as μ is varied. We also provide results for magnetic field B as well as chemical potential sweeps at selected fixed frequencies, which can be particularly useful for possible measurements in graphene. Both diagonal and Hall conductivities are considered.
Subfields: Atomic and Molecular Physics, and Optics, Materials Chemistry, Physical and Theoretical Chemistry
View Paper: https://www.semanticscholar.org/paper/9eca743bf8ba831c3eeab526584397a8c1f517dd
How researchers see this paper
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In Atomic and Molecular Physics, and Optics
- N. M. R. Peres
- K. Novoselov
- A.K. Geim
- Francisco Guinea
- A. C. Castro Neto
- M. Potemski
- M. Orlita
- Xiaodai Dong
In Materials Chemistry
- N. M. R. Peres
- K. Novoselov
- Francisco Guinea
- A. C. Castro Neto
- A.K. Geim
- M. Potemski
- M. Orlita
- M. Goerbig
In Physical and Theoretical Chemistry
- N. M. R. Peres
- Xiaodai Dong
- A. C. Castro Neto
- M. Orlita
- Zhengji Xu
- Jens Bornemann
- K. Novoselov
- Francisco Guinea
Citations in the corpus
- Design of a Reconfigurable MIMO System for THz Communications Based on Graphene Antennas (2014, methodology): “Therefore, we can use the results from the Kubo formula [28]”
- Dirac electronic states in graphene systems: optical spectroscopy studies (2010, background): “The matrix elements of the velocity operators v̂+ = (v̂x − iv̂y)/ √ 2 and v̂− = (v̂x + iv̂y)/ √ 2 are |〈m|v̂+|n〉| = αδ|m|,|n|+1 and |〈m|v̂−|n〉| = αδ|m|,|n|−1, respectively, with α = v2 F / 2 if n or m equals zero, and otherwise α = v2 F / 4 [76, 79, 81, 87].”
- The electronic properties of graphene (2007, background): “In addition to phases with enhan ed ferromag-netism or with broken valley symmetry, intera tionsat high magneti elds an lead to ex itoni instabil-ities (Gusynin et al., 2006) and Wigner rystal phases(Zhang and Joglekar, 2007).”