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Graphene's Hall conductivity is = (+ /) /, where N is the Landau level and the double valley and double spin degeneracies give the factor of 4. [2] These anomalies are present not only at extremely low temperatures but also at room temperature, i.e. at roughly 20 °C (293 K).
The effects of Landau levels may only be observed when the mean thermal energy kT is smaller than the energy level separation, , meaning low temperatures and strong magnetic fields. Each Landau level is degenerate because of the second quantum number k y {\displaystyle k_{y}} , which can take the values k y = 2 π N L y , {\displaystyle k_{y ...
The graphene sheet thus displays a semimetallic (or zero-gap semiconductor) character. Two of the six Dirac points are independent, while the rest are equivalent by symmetry. In the vicinity of the K-points the energy depends linearly on the wave vector, similar to a relativistic particle.
English: Landau levels in graphene appear at energies proportional to √N, in contrast to the standard sequence that goes as N+½. After Geim and Novoselov arXiv:cond-mat/0702595 After Geim and Novoselov arXiv:cond-mat/0702595
(b) Landau levels have a non-zero width in a more realistic picture and overlap if <. (c) The levels become distinct when >. In order to get the number of occupied Landau levels, one defines the so-called filling factor as the ratio between the density of states in a 2DEG and the density of states in the Landau levels.
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