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V.E. Bisti Institute of Solid State Physics RAS, Chernogolovka, Russia N. N. Kirova LPS, Universite Paris Sud, Orsay, France COULOMB INTERACTION AND ELECTRON-HOLE.

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Presentation on theme: "V.E. Bisti Institute of Solid State Physics RAS, Chernogolovka, Russia N. N. Kirova LPS, Universite Paris Sud, Orsay, France COULOMB INTERACTION AND ELECTRON-HOLE."— Presentation transcript:

1 V.E. Bisti Institute of Solid State Physics RAS, Chernogolovka, Russia N. N. Kirova LPS, Universite Paris Sud, Orsay, France COULOMB INTERACTION AND ELECTRON-HOLE ASYMMETRY IN CYCLOTRON RESONANCE OF BILAYER GRAPHENE IN HIGH MAGNETIC FIELD

2 Asymmetry in bilayer graphene

3 Layer asymmetry Nearest neighbour transitions Layer asymmetry

4 Electron-hole asymmetry Next- nearest neighbour transitions Energy difference between dimer and non-dimer sites

5 Layer asymmetry (red) Layer and e-h asymmetry (black)

6 Landau Levels with electron-hole and layer asymmetry

7 Excitations Integer filling Half-filling

8 Coulomb interaction

9 Cyclotron transitions

10 Cyclotron transitions at lower magnetic fields

11 Cyclotron transitions at higher magnetic fields

12 Symmetric bilayer graphene Monolayer graphene

13 Full-symmetric case (half-filling) – – splitting due to Coulomb interaction Electron-hole asymmetry – no splitting Asymmetric case (low field) – splitting die to electron-hole asymmetry Asymmetric case (high field) – splitting die to Coulomb interaction and layer asymmetry Summary V.E. Bisti, N.N. Kirova. JETP Letters 90, v.2, 2009, 130-133. V.E. Bisti, N.N. Kirova. arXiv: 1102.2638v1, 20011.

14 Monolayer: Independent of H Bilayer: for H=40T

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18 Landau Levels with layer asymmetry

19 Asymmetric bilayer


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