Magneto-spectroscopy of multilayer epitaxial graphene, of graphite and of graphene

Transcription

1 Magneto-spectroscopy of multilayer epitaxial graphene, of graphite and of graphene Marek Potemski Grenoble High Magnetic Field Laboratory, Centre National de la Recherche Scientifique Grenoble, France Outline: - introduction - magneto-spectroscopy - inter Landau level transitions - magneto-raman scattering of optical phonons - discussion - band structure parameters and scattering efficiency - electron-phonon coupling - electron-electron interactions - conclusions and acknowledgments

2 Graphene, Dirac-like energy bands, inter Landau level transitions if only γ ~ 0 c = 3a0γ 0 r r E( k ) = ± c~ hk E / 2h Oscillator strength ( fn fm ) E ( hω + i ) 2 B *, n vˆ ± m m vˆ ± m, n m n 4G e σ± ( ω B) = ω E γ E 0 B Selection rules : n Transition energies : m Cyclotron resonance like : Interband like : c ~ 2e h = ±1 B (σ + ) (σ - ) ( ) n +1 n n ( ) n +1 n c ~ 2eh B + Multimode spectrum sqrt(b) rules 0 Re σ xx de e 2 4G B h π tr 1 4 c ~ Broadening ~ scattering efficiency 2 n + 1 B ± n

3 Graphene bilayer, massive Dirac fermions Brillouin zone: Parabolic dispersion: γ γ 3, 4 = 0 Parabolic dispersion: Doubly degenerated 0 th LL Density of states: Optically active transitions : -/+ 1 = m - n

4 Multilayer epitaxial graphene : quasi neutral layers on C-face SiC C-terminated SiC surface multilayer graphene hω Our samples, experiments (Essentially) neutral, majority graphene layers probed in transmission (these experiments) SiC substrate Si layer C layer } Highly conducting layers at the interface probed in electric transport e.g., C. Berger et al., Science (2006) T T ( hω, B) ( hω, B = 0)

5 Magneto-spectroscopy of multilayer graphene (on SiC, C-face) Dirac-like bands in many layer system!!! Landau Level Spectroscopy of Ultrathin Graphite Layers, M.L. Sadowski, G. Martinez, M. Potemski, C. Berger, and W. A. de Heer, Phys. Rev. Lett. 97, (2006) Magneto-transmission: Fourier transform spectroscopy ~ 5GL on SiC B Relative transmission 1,00 0,98 (A) (B) Relative transmission 1,00 0, T 0.3T 0.5T 0.7T 0.4T 8.4 T (C) 12 T 1,00 0,99 0,98 0,97 (D) T T ( ω, B) ( ω, B = 0) 0, T 1.9 K 0,90 1 T 2T 4T Energy (mev) Energy (mev)

6 Multilayer epitaxial graphene : quasi neutral layers on C-face SiC Accurateness of the Dirac cone? Far- and near-infrared magneto-optics Multilayer graphene on SiC Energy (mev) c* = 1.02 x 10 6 m/s CDEFGHI J K LM N O PQR A B S TUVWXYZ AG AHAI AJ AEAF AAABAC AD L L L Deviations from linearity ( L 4 3 ) ( L ) 3 L4 L 2 L3 3 L2 ( L ) 1 L2 2 L1 0 Substrate opacity B 1/2 ( T 1/2 ) L ( L ) 0 L1 1 L0 High-Energy Limit of Massless Dirac Fermions in Multilayer Graphene, P. Plochocka, C. Faugeras, M. Orlita, M.L. Sadowski, G. Martinez, M. Potemski, M.O. Goerbig, J.-N. Fuchs,C. Berger, and W.A. de Heer, Phys. Rev. Lett. 100, (2008)

7 High energy limits of Dirac like electron dispersions + next nearest neighbor hopping In magnetic fields : graphene : tight binding (t) next nearest neighbor (t`/t ~ 0.1) E±,n = ± E0 n m E 0 3w n ~ a 3t ~ a n + E0 n l B 2t l B ± E = 9t a~ m 2 l 2 Deviation from linear dependence (mev) aw ~ + 64h 2 B v F w = Transition energy (mev) ( 0 ) 3 Electron-hole asymmetry: small and not seen! High-Energy Limit of Massless Dirac Fermions in Multilayer Graphene, P. Plochocka, C. Faugeras, M. Orlita, M.L. Sadowski, G. Martinez, M. Potemski, M.O. Goerbig, J.-N. Fuchs,C. Berger, and W.A. de Heer, Phys. Rev. Lett. 100, (2008) n

8 Multilayer epitaxial graphene : quasi neutral layers on C-face SiC quality of electronic states? Carrier scattering from cyclotron resonance measurements σ 10e 2 / ω τ = 1 τ = 200 fs h no temperature activated scattering µ B > 1 µ > cm Vs ne cm, EF 6meV Record RT-mobility! Ultrahigh mobility in multilayered epitaxial graphene: a step towards graphene based electronics, M. Orlita, C. Faugeras,P. Plochocka, P. Neugebauer, G. Martinez, D.K. Maude, A.-L. Barra, M. Sprinkle C. Berger, W.A. de Heer, M. Potemski, Phys. Rev. Lett. 100, (2008).

9 Multilayer epitaxial graphene : quasi neutral layers on C-face SiC C-terminated SiC surface Multilayered graphene Intensity HOPG graphite 2nm-thick graphite grey sea white flakes "exfoliated" graphene Raman shift (1/cm) FGL on SiC C. Faugeras et al., APL, 2007 Raman scattering : fingerprint of simple, (Dirac like?) band + graphite inclusions blue shift as compared to graphene (smaller c *?) Bernal AB turbostratic AA bilayer Rotational stacking!!! (not Bernal) (misoriented, turbostratic, incommensurate) of graphene layers with electronic bands of a single sheet! (but slightly smaller c*?) J. Haas et al., PRL (2007) J.M.B. Lopes dos Santos et al., PRL (2008) S. Latil et al., PRB (2008) Z. Ni et al., PRB (2008)

10 Multilayer epitaxial graphene : quasi neutral layers on C-phase SiC Latest confirmations of Dirac-like electronic bands Cond/mat, 30 July 2009

11 Electron-phonon interaction

12 Electron-phonon interaction hω vs. 2 G E F hω G 2E F

13 Tuning electron-phonon coupling with magnetic field in graphene G-phonon couples to inter Landau level transitions which follow the same selection rules as optically active transitions

14 Tuning electron-phonon coupling with magnetic field in graphene valley asymmetric inter-landau level transitions optically inactive g = 0.2 ev A n 2 = 1 if if n n = 0 0

15 Tuning electron-phonon coupling with magnetic field Magneto-Raman scattering experiments Multilayer epitaxial graphene : quasi neutral layers on C-face SiC C. Faugeras et al., cond/mat, 2009 Experiment on multilayer epitaxial graphene (C-face of SiC) Oscillatory (~ 40%) + Field independent component

16 Tuning electron-phonon coupling with magnetic field Multilayer epitaxial graphene : quasi neutral layers on C-face SiC C. Faugeras et al., cond/mat, 2009 Oscillatory component E T 2 T 1 T 0 B E F (ν = 0)

17 Tuning electron-phonon coupling with magnetic field Multilayer epitaxial graphene : quasi neutral layers on C-face SiC C. Faugeras et al., cond/mat, 2009 Oscillatory component E T 2 T 1 T 0 B E F (ν = 0)

18 Tuning electron-phonon coupling with magnetic field Multilayer epitaxial graphene : quasi neutral layers on C-face SiC C. Faugeras et al., cond/mat, 2009

19 Cleaner systems? Digression on (Bulk) graphite? higher mobilities, controversial reports more complex, 3D material

20 (Bulk) graphite? : higher mobilities, controversial reports more complex, 3D material J. C. Slonczewski and P. R. Weiss, Phys. Rev. 109, 272 (1958). J.W. McClure (1964) parabolic bilayer linear monolayer

21 What about graphite: more complex 3D material Dispersion of Landau bands across the layers (z-direction) Nakao, JAP, 1976 Transport (SdH oscillations): spectroscopy : E F maxima in density of states Landau level spectroscopy : maxima in joint density of states

22 Graphite: SdH pattern, consistent with SWM model J.M. Schneider, M. Orlita, M. Potemski, D.K. Maude, PRL 102, (2009)

23 Graphite: simplified model: effective graphene bilayer Onlyγ 0 and γ 1 E 1 E 3 E 2 2 γ 1 H K H M o m e n t u m k z

24 Graphite from viewpoint of Landau level spectroscopy: An effective graphene bilayer and monolayer Abergel, Falko (2007) Transmission spectra For a bilayer : M. Koshino and T. Ando, Phys. Rev. B (2008) M. Orlita, C. Faugeras, J. M. Schneider, G. Martinez, D. K. Maude, and M. Potemski, PRL 102, (2009) K point H point

25 Natural graphite probed with more subtle tools E exc ~ 1meV, very low fields (EPR-type spectroscopy) All but 3N harmonics of K-point electron cyclotron resonance (due to trigonal warping) J.K. Galt et al., (1956) P. Nozieres (1958) Expected also for graphene bilayer: Abergel, Falko (2007)

26 The cleanest, ever seen Dirac-like system On graphite surface

27 Natural graphite probed with more subtle tools E exc ~ 1meV, very low fields (EPR-type spectroscopy) Grahene flakes on graphite!!! G. Li et al., Phys. Rev. Lett. 102, (2009) Harmonics of K-electron CR P. Neugebauer, M. Orlita, C. Faugeras, A-L. Barra, and M. Potemski, Cond/Mat (2009)

28 Grahene flakes on graphite!!! 1 mt Gap < 1 mev (0.4 K)

29 Grahene flakes on graphite!!! Landau level quantisation down to B = 1 mt σ 400e 2 / h?? 1.3 x 10-3 m 0 B Earth ~ Also at 50 K

30 Grahene flakes on graphite? H-point of graphite? Extremely unlikely: pseudogap ~ 5meV, E f ~ 20 mev, T-dependence Several samples investigated Seen for different frequencies Fast thermal cooling helps (enhanced signal)

31 Collective excitations? Simple, one particle approach is applicable? Magneto-plasmons (e.g., size confined modes) (apparent under similar conditions in a 2DEG in GaAs) Very likely not seen here, but...?? is likely of collective origin E exc ~ B/T Collective but magnetic???

32 Why single particle approach works so well? It does not work e-e interactions leads to modification of dispersion relations at B=0 c ~ 0.86x10 6 m/s (expected) c*~1.02x10 6 m/s (experiment) magnetic field acts on modified dispersions (approach characteristic for dirty systems or for electrons with linear dispersions?) New Kohn theorem cancellation rules? (specific of Dirac electrons ) restoring the one particle character of inter Landau level transitions? E n ~ const ( ~ n for a " conventional" 2DEG) kin EF ~ = E 1 int n rs E 01 B hωc ~ = const ~ B for a " conventional" 2DEG 2 2 e B e κl B κlb Abstract : EP2DS-2009-Kobe

33 Conclusions Magneto-spectroscopy helps to understand the electronic properties of two-dimensional carbon allotropes Not much of electron-electron interactions in graphene as far But clear effects of electron-phonon interaction Acknowledgements Milan ORLITA, Clement FAUGERAS, Paulina PLOCHOCKA, Johannes SCHNEIDER, Petr NEUGEBAUER Marcin SADOWSKI, Duncan.K. MAUDE, Anne-Laure BARRA, Gerad MARTINEZ Mark O. GOERBIG, Jean-Noel FUCHS Claire BERGER, Walt A. DE HEER, Eric DUJARDIN, Yuri LATYSHEV