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Igor Lukyanchuk Amiens University Quantum Oscillations and Magnetic Properties of Graphene-related nanostructures How to identify Dirac Fermions ???
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Graphite …
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Unusual electronic phenomena in Graphite
Y. Kopelevich et al. Phys. Rev. Lett. 87, (2001) 93, (2004) Weak ferromagnetism MIT transition Linear magnetoresistance (old problem) Quantum Hall 35K Superconductivity in Graphite-S
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(2D graphite monolayer, Semimetal)
Graphene: (2D graphite monolayer, Semimetal) Brillouin zone Special points of Brillouin zone Linear Dirac spectrum 4-component (Dirac) wave function
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Graphite: Band structure: Slonczewski-McClure Model Fitting parameters
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holes Is it real ???? electrons
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Problems with band interpretation
Sh > Se Problems with band interpretation 1) Se > Sh 2) H: point Dirac Spectrum Phase volume ~0 holes no Dirac Fermions should be seen in experiment Normal Spectrum electrons Another possibility: Independent layers ???
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ρc/ ρa > 50000 (instead of 300 in Kish) ρa ~ 3 μΩ cm (300K)
ρ(T), HOPG In best samples ρc/ ρa > (instead of 300 in Kish) ρa ~ 3 μΩ cm (300K) n3D~3x1018 cm-3 n2D~1011 cm-2 ( in Graphene) Mobility: μ~107cm2/Vs (105 in Graphene) Metals: 300μΩ cm, Ioffe-Regel μΩ cm
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Dirac Fermions vs Normal Carriers ?
Graphite: 2D vs 3D ? Dirac Fermions vs Normal Carriers ? Tools: Quantum oscillations I. Lukyanchuk, Y. Kopelevich et al. - Phys. Rev. Lett. 93, (2004) - Phys. Rev. Lett. 97, (2006)
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Landau quantization: Normal vs Dirac
Normal electrons ‘’gap’’ Dirac electrons no ‘’gap’’ !!!
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F Magnetic Quantum oscillations
► Susceptibility (H) : de Haas–van Alphen (dHvA) etc… …due to Landau quantization of Density of States Clean 2D Quasi 2D 3D or dirty t, hc F H
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Transport properties: Shubnikov de Haas (SdH) oscillations
► Hall Resistance Rxy(H) : In-field resistivity measurements… In bulk sample ► Resistance Rxx(H) In 2D film: Quantum Hall effect
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and Phase ??? … difficult to extract
Quantum oscillations: What is usually studied ? Profile: Information about e-e interaction (in 2D) Damping: Information about e-scattering (Dingle factor G ) Period: Information about Fermi surface cross section S(e) and Phase ??? … difficult to extract We propose the method.!!!
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► 2D + 3D case, normal spectrum
dHvA oscillations ► 3D case, arbitrary spectrum ► 2D case, normal spectrum ► 2D D case, normal spectrum ► 2D case, Dirac spectrum
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g is extracted from phase !!!
More general… 3D spectrum, model In terms of extremal cross sections ( arbitrary ) Bohr-Sommerfeld quantization Topological index : Mikitik, Sharlai, Phys. Rev. Lett. 82, 2147 (1999) ► for Normal electrons g is extracted from phase !!! ► for Dirac electrons
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Generalized formula: 2D, 3D, arbitrary spectrum
I. Luk’yanchuk and Y. Kopelevich Phys. Rev. Lett. 93, (2004) where Normal: Dirac: Fermi surface cross section Limit cases 3D : => Lifshitz-Kosevich => Shoenberg 2D :
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{ { SdH: Oscillations of xx (H) (1st harmonic)
Phase depends on : Normal: = 1/2 Dirac: = 0 ► Spectrum : { 2D: = 0 3D: = ± 1/8 ► Dimensionality : { dHvA: Oscillations of (H) (1st harmonic)
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Quantum oscillations in Graphite
Resistance Rxy (H) Susceptibility c(H) T. Berlincourt et al. Phys. Rev. 98, 956 (1955) Hall effect Rxy(H) in 2D Graphene Hall effect Rxy(H) Y. Kopelevich et al. Phys. Rev. Lett. 90, (2003) Novoselov, K. S. et al. Nature 438, 197 (2005); Zhang, Y. et al. Nature 438, 201 (2005).
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Quantum oscillations in Graphite:
Fermi surface Y. Kopelevich high fields SdH spectrum dHvA low fields minority majority
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Pass-band filtering Comparison of dHvA and SdH SdH dHvA dHvA SdH
high fields spectrum electrons holes low fields holes (?)
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Fan Diagram for SdH oscillations in Graphite
Dirac Normal Novoselov, 2005 Multilayer 5nm graphite graphene
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QHE and DF
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2005: Discovery of Quantum Hall Effect in 2D Graphene
Due to Dirac fermions … From: - phase analysis - semi-integerr QHE Novoselov, K. S. et al. Nature 438, 197 (2005); Zhang, Y. et al. Nature 438, 201 (2005).
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sxy sxy QHE effect : Normal vs Dirac Normal electrons,
Dirac- like electrons (expected for graphene) sxy 1 / H
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« Dirac » QHE Hall effect in Graphene monolayer n
Novoselov, K. S. et al. Nature 438, 197 (2005); Zhang, Y. et al. Nature 438, 201 (2005). « Dirac » QHE n
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QHE effect in 2-layer graphite film
(K.Novoselov et al, cond-mat 2005, Nature-Physics) -sxy 12T 1 / H « Normal » QHE due to normal electrons
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Graphite, Quantum Hall Effect, different samples Kopelevich, (2003)
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QHE: Graphite vs multi graphene
HOPG, Y. Kopelevich et al. PRL´2003 QHE: Graphite vs multi graphene B0 = 4.68 T . Few Layer Graphite (FLG) K.S.Novoselov et al., Science´2004 B0= 20 T, = > n ~ 2x1012 cm-2
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Filtering Normal (Integer QHE) GRAPHITE: Normal vs Dirac
carriers separation Lukyanchuk, Kopelevich - Phys. Rev. Lett. 97, (2006) Rxy Dirac (Semi-integer QHE) Rxx Filtering B (T)
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FQHE in Graphite
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Rxy Rxx Rxy Rxy Rxx
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Another manifestations
of DF in Graphite
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2006 Confirmation: Angle Resolved Photoemission Spectroscopy
(ARPES) Dirac holes Normal electrons
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Another confirmation of Dirac fermions:
Dirac+Normal fermions in HOPG TEM results: C. Li and E. Andrei. 2007, Nature Phys.
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Interlayer tunneling spectroscopy of Landau levels in graphite
Yu. I. Latyshev1, A. P. Orlov1, V. A. Volkov1, A. V. Irzhak2, D. Vignolles3, J. Marcus4 and T. Fournier4
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INFRARED SPECTROSCOPY
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2006 Graphite, interpretation, ??? =>
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RAMAN SPECTROSCOPY
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Raman spectra of graphite
double-resonant graphite 2.33 eV D G D‘ G‘
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RAMAN SPECTROSCOPY « Graphene Fingerprint »
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HOPG-Graphite, Raman, Peak 2G
I. Lukyanchuk, M. El Marssi, Y. Kopelevich Physica B, 2009 Trace of graphene
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model
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B As in bilayer ?
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Nernst-Ettingshausen (NE) Quantum Oscillations
Graphite, Graphene, Bismuth… Perpendicular magnetic field NE - effect Temperature gradient V, Potential difference
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NE coefficient: Advantages: - oscillations have the thermodynamic origin, related with and - can be measured in films
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NE oscillations, calculated from thermodynamics
for:
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Results: 2D 3D Giant !!! (even in 3D) Phase shift
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As function of gate voltage …
Normal Dirac …
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EXPERIMENT Graphene, DF
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Graphite, ?? Transport Nernst Giant (!), 3D (?), Phase ???
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Bismuth Giant (!), 3D (?), Phase ???
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