Electronic Cooling in Multilayer Epitaxial Graphene
|
|
|
- Fay Fox
- 5 years ago
- Views:
Transcription
1 1
2 Electronic Cooling in Multilayer Epitaxial Graphene Reza Asgari Workshop on Nanoscale heat transport th April
3 My purpose I: 63 layers 93 mev 140 mev 218 mev 360 mev LD HD SiC n < cm 2 n > cm 2 M. Mihney, J. Tolsma, C. David, D. Sun. R. Asgari, M. Polini, C. Berger, W. A. de Heer, A. H. MacDonald, T. Norris, Nature Commuin. (2015) 3
4 My purpose II: Electronic cooling life time M. Mihney, J. Tolsma, C. David, D. Sun. R. Asgari, M. Polini, C. Berger, W. A. de Heer, A. H. MacDonald, T. Norris, Nature Commuin. (2015) 4
5 Outlook 1. Introduction brief overview on electronic cooling and ultrafast spectroscopy 2. Electronic cooling and different mechanisms electron-phonon interactions electron-impurity interactions electron-electron interactions Multilayer epitaxial graphene 3. Conclusion 5
6 Ultrafast Spectroscopy W. S. Yun, et al, Phys. Rev. B 85, (2012) 6
7 Ultrafast Spectroscopy Di Xiao, et al, Phys. Rev. Lett. 108, (2012) 7
8 Ultrafast Spectroscopy 8
9 Ultrafast Spectroscopy Thermalization of the hot electron 9
10 Outlook 1. Introduction brief overview on electronic cooling and ultrafast spectroscopy 2. Electronic cooling and different mechanisms electron-phonon interactions electron-impurity interactions electron-electron interactions Multilayer epitaxial graphene 3. Conclusion 10
11 Electron-phonon interactions Heat transfer rate δ = 5 δ = 6 δ = 3 3D metals, F. Wellstood, et al, PRB 49, 5942 (1994) Discorded thin film, Sergeev and Mitin, PRB 61, 6041 (2000) Clamped 3D but vibrations are 1D, Hekkila, PRB 77, (2008) δ =2+d 11
12 Electron-phonon interactions: graphene δ =4 2D graphene, Kubakadda, PRB 79, (2009) 2D graphene, Bistritzer and MacDonald PRL 102, (2009) 12
13 Electron-phonon interactions: Graphene Classical Boltzmann equation Scattering integral Golden-rule scattering rate Viljas and Heillila Phys. Rev B 81, (2010) 13
14 Electron-phonon interactions: Graphene Electron-phonon Hamiltonian: D is the coupling constant Effective interaction term Viljas and Heillila Phys. Rev B 81, (2010) 14
15 Electron-phonon interactions: Graphene Viljas and Heillila Phys. Rev B 81, (2010) 15
16 Electron-phonon interactions: Graphene Limit of the low temperature Viljas and Heillila Phys. Rev B 81, (2010) 16
17 Electron-phonon interactions: Graphene For high temperature regiem Viljas and Heillila Phys. Rev B 81, (2010) 17
18 Electron-phonon interactions: Exp results Betz et al, Phys. Rev Lett 109, (2012) 18
19 Outlook 1. Introduction brief overview on electronic cooling and ultrafast spectroscopy 2. Electronic cooling and different mechanisms electron-phonon interactions electron-impurity interactions electron-electron interactions Multilayer epitaxial graphene 3. Conclusion 19
20 Electron-impurity interactions: supercollision Song, Reizer and Levitov Phys. Rev Lett, 109, (2012) 20
21 Electron-impurity interactions: Evidences! Graham et al Nature Physics (2012) Betz et al Nature Physics (2012) 21
22 Electron-electron interactions Brida, et al, Nature Commuin, DOI (2013) Butscher, et al App. Phys. Lett 91, (2007) Sun et al, Phys. Rev. B 85, (2012) 22
23 Electron-electron interactions Semiclassical Boltzmann equation Collision integral Brida, et al, Nature Commuin, DOI (2013) Butscher, et al App. Phys. Lett 91, (2007) Sun et al, Phys. rev. B 85, (2012) E = ε 1 + ε 2 Q = k 1 +k 2 23
24 Electron-electron interactions Brida, et al, Nature Commuin, DOI (2013) Butscher, et al App. Phys. Lett 91, (2007) Sun et al, Phys. Rev. B 85, (2012) 24
25 Electron-electron interactions: Delay time Brida, et al, Nature Commuin, DOI (2013) 25
26 Electron-electron interactions: interlayer Wang and Lima, Phys. Rev. B 63, (2001) Senger and Tanatar SSC 121, 61 (2002) 26
27 Electron-electron interactions: Interlayer Cooling power rate transferred between layers Wang and Lima, Phys. Rev. B 63, (2001) Flensberg and Hu, Phys. Rev. B 52, (1995) 27
28 Electron-electron interactions Ramezanali, Vaziefeh, Asgari, Polini, MacDonald, J. Phys. A 42, (2009) Faridi, Pashangpour, Asgari, Phys. Rev. B 85, (2012) 28
29 Electron specific heat and spin susceptibility at low temperature Ramezanali, Vaziefeh, Asgari, Polini, MacDonald, J. Phys. A 42, (2009) Faridi, Pashangpour, Asgari, Phys. Rev. B 85, (2012) 29
30 Outlook 1. Introduction brief overview on electronic cooling and ultrafast spectroscopy 2. Electronic cooling and different mechanisms electron-phonon interactions electron-impurity interactions electron-electron interactions Multilayer epitaxial graphene 3. Conclusion 30
31 Epitaxial graphene on C-terminated SiC Hass, et al Phys. Rev. Lett 100, (2008) 31
32 Epitaxial MLG on C-face SiC Charge distributions: Sun, et al Phys. Rev. Lett 104, (2010) Sprinkle, et al Phys. Rev. Lett 103, (2009) 32
33 Electron-electron interactions: Two-layers M. Mihney, J. Tolsma, C. David, D. Sun. R. Asgari, M. Polini, C. Berger, W. A. de Heer, A. H. MacDonald, T. Norris, Nature Commuin. (2015) 33
34 Electron-electron interactions: two layers 34
35 Electron-electron interactions: Interlayer M. Mihney, J. Tolsma, C. David, D. Sun. R. Asgari, M. Polini, C. Berger, W. A. de Heer, A. H. MacDonald, T. Norris, Nature Commuin. (2015) 35
36 Cooling lifetime in MEG 36
37 Power rate in MEG 63 layers 93 mev LD n < cm mev 218 mev 360 mev SiC HD n > cm 2 37
38 Cooling in multilayer: approximation 38
39 T(t) in MEG 39
40 T(t) in MEG 40
41 Cooling lifetime in MEG M. Mihney, J. Tolsma, C. David, D. Sun. R. Asgari, M. Polini, C. Berger, W. A. de Heer, A. H. MacDonald, T. Norris, Nature Commuin. (2015) 41
42 Conclusions Electron cooling mechanisms: e-ph, e-imp and e-e interactions δ =2+d? Epitaxila graphene: C-face multilayer graphene on SiC substrate electronic cooling times ranging from a few to hundreds of picoseconds that strongly depend on the lattice temperature and the number of epitaxial graphene layers Developed a theory of hot-carrier equilibration based on interlayer energy transfer via screened Coulomb interactions Energy transfer between the LD layers is much stronger than between LD and HD layers The theoretically calculated thermal equilibration times are free of any fitting parameters, compare closely with the experimental relaxation times 42
43 Thanks for your attention 43
Ultrafast Electron-Electron Dynamics in Graphene Daniele Brida
Ultrafast Electron-Electron Dynamics in Graphene Ultrafast Spectroscopy Light-matter interaction on timescale of fundamental physical processes: electron scattering, phonon emission, energy transfer D.
In recent years, graphene has gathered much interest for electrical
pubs.acs.org/nanolett Very Slow Cooling Dynamics of Photoexcited Carriers in Graphene Observed by Optical-Pump Terahertz-Probe Spectroscopy Jared H. Strait,* Haining Wang, Shriram Shivaraman, Virgil Shields,
Supplementary Figures
Supplementary Figures Supplementary Figure 1: Heating and cooling pathways of hot carriers in graphene. a) Schematics illustrating the cooling pathway of photoexcited carriers. Detailed descriptions are
Soft Carrier Multiplication by Hot Electrons in Graphene
Soft Carrier Multiplication by Hot Electrons in Graphene Anuj Girdhar 1,3 and J.P. Leburton 1,2,3 1) Department of Physics 2) Department of Electrical and Computer Engineering, and 3) Beckman Institute
Infrared magneto-spectroscopy of graphene-based systems
Infrared magneto-spectroscopy of graphene-based systems M. Orlita, C. Faugeras, G. Martinez P. Neugebauer, M. Potemski Laboratoire National des Champs Magnétiques Intenses CNRS, Grenoble, France Collaborators:
THz Spectroscopy of Nanoscale Materials
THz Spectroscopy of Nanoscale Materials Frontiers of THz Science Stanford, Sept. 5, 2012 Tony F. Heinz Columbia University New York, NY 10027 http://heinz.phys.columbia.edu tony.heinz@columbia.edu Thanks
TOPOLOGICAL BANDS IN GRAPHENE SUPERLATTICES
TOPOLOGICAL BANDS IN GRAPHENE SUPERLATTICES 1) Berry curvature in superlattice bands 2) Energy scales for Moire superlattices 3) Spin-Hall effect in graphene Leonid Levitov (MIT) @ ISSP U Tokyo MIT Manchester
Supplementary Figure 1: A potential scheme to electrically gate the graphene-based metamaterial. Here density. The voltage equals, where is the DC
Supplementary Figure 1: A potential scheme to electrically gate the graphene-based metamaterial. Here density. The voltage equals, where is the DC permittivity of the dielectric. is the surface charge
Electronic thermal transport in nanoscale metal layers
Electronic thermal transport in nanoscale metal layers David Cahill, Richard Wilson, Wei Wang, Joseph Feser Department of Materials Science and Engineering Materials Research Laboratory University of Illinois
Magneto-spectroscopy of multilayer epitaxial graphene, of graphite and of graphene
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
ELECTRONS AND PHONONS IN SEMICONDUCTOR MULTILAYERS
ELECTRONS AND PHONONS IN SEMICONDUCTOR MULTILAYERS В. К. RIDLEY University of Essex CAMBRIDGE UNIVERSITY PRESS Contents Introduction 1 Simple Models of the Electron-Phonon Interaction 1.1 General remarks
arxiv: v3 [cond-mat.mes-hall] 22 Jul 2008
![arxiv: v3 [cond-mat.mes-hall] 22 Jul 2008](/thumbs/83/88787233.jpg "arxiv: v3 [cond-mat.mes-hall] 22 Jul 2008")
Ultrafast Optical-Pump Terahertz-Probe Spectroscopy of the Carrier Relaxation and Recombination Dynamics in Epitaxial Graphene Paul A. George, Jared Strait, Jahan Dawlaty, Shriram Shivaraman, Mvs Chandrashekhar,
Graphene for THz technology
Graphene for THz technology J. Mangeney1, J. Maysonnave1, S. Huppert1, F. Wang1, S. Maero1, C. Berger2,3, W. de Heer2, T.B. Norris4, L.A. De Vaulchier1, S. Dhillon1, J. Tignon1 and R. Ferreira1 1 Laboratoire
SUPPLEMENTARY INFORMATION
DOI: 1.138/NNANO.215.33 Epitaxial graphene quantum dots for high-performance terahertz bolometers Abdel El Fatimy *, Rachael L. Myers-Ward, Anthony K. Boyd, Kevin M. Daniels, D. Kurt Gaskill, and Paola
Ultrafast Lateral Photo-Dember Effect in Graphene. Induced by Nonequilibrium Hot Carrier Dynamics
1 Ultrafast Lateral Photo-Dember Effect in Graphene Induced by Nonequilibrium Hot Carrier Dynamics Chang-Hua Liu, You-Chia Chang, Seunghyun Lee, Yaozhong Zhang, Yafei Zhang, Theodore B. Norris,*,, and
Ultrafast Optical-Pump Terahertz-Probe Spectroscopy of the Carrier Relaxation and Recombination Dynamics in Epitaxial Graphene
Letter Subscriber access provided by CORNELL UNIV Ultrafast Optical-Pump Terahertz-Probe Spectroscopy of the Carrier Relaxation and Recombination Dynamics in Epitaxial Graphene Paul A. George, Jared Strait,
SUPPLEMENTARY FIGURES
SUPPLEMENTARY FIGURES THz sampling Supplementary Figure 1. Schematic representation of the high-field THz spectroscopy setup. Supplementary Figure 2. The measured Raman spectrum (with 532 nm pump) of the
The Physics of Nanoelectronics
The Physics of Nanoelectronics Transport and Fluctuation Phenomena at Low Temperatures Tero T. Heikkilä Low Temperature Laboratory, Aalto University, Finland OXFORD UNIVERSITY PRESS Contents List of symbols
ELECTRONIC TRANSPORT IN GRAPHENE
ELECTRONIC TRANSPORT IN GRAPHENE J. González Instituto de Estructura de la Materia, CSIC, Spain 1985 1991 4 ELECTRONIC TRANSPORT IN GRAPHENE Graphene has opened the way to understand the behaior of an
ARPES experiments on 3D topological insulators. Inna Vishik Physics 250 (Special topics: spectroscopies of quantum materials) UC Davis, Fall 2016
ARPES experiments on 3D topological insulators Inna Vishik Physics 250 (Special topics: spectroscopies of quantum materials) UC Davis, Fall 2016 Outline Using ARPES to demonstrate that certain materials
Ultrafast Dynamics in Complex Materials
Ultrafast Dynamics in Complex Materials Toni Taylor MPA CINT, Center for Integrated Nanotechnologies Materials Physics and Applications Division Los Alamos National Laboratory Workshop on Scientific Potential
SUPPLEMENTARY INFORMATION
DOI: 1.138/NPHOTON.212.314 Supplementary Information: Photoconductivity of biased graphene Marcus Freitag, Tony Low, Fengnian Xia, and Phaedon Avouris IBM T.J. Watson Research Center, Yorktown Heights,
Supplementary Figure 1 Magneto-transmission spectra of graphene/h-bn sample 2 and Landau level transition energies of three other samples.
Supplementary Figure 1 Magneto-transmission spectra of graphene/h-bn sample 2 and Landau level transition energies of three other samples. (a,b) Magneto-transmission ratio spectra T(B)/T(B 0 ) of graphene/h-bn
Low Bias Transport in Graphene: An Introduction
Lecture Notes on Low Bias Transport in Graphene: An Introduction Dionisis Berdebes, Tony Low, and Mark Lundstrom Network for Computational Nanotechnology Birck Nanotechnology Center Purdue University West
Out-of-plane heat transfer in van der Waals stacks through electron hyperbolic phonon coupling
SUPPLEMENTARY INFORMATION Letters https://doi.org/.38/s4565-7-8-8 In the format provided by the authors and unedited. Out-of-plane heat transfer in van der Waals stacks through electron hyperbolic phonon
Density-matrix theory for time-resolved dynamics of superconductors in non-equilibrium
Max Planck Institute for Solid State Research Density-matrix theory for time-resolved dynamics of superconductors in non-equilibrium co-workers and papers: (1) (2) (3) (4) Dirk Manske A. Knorr (TU Berlin),
Quantum Confinement in Graphene
Quantum Confinement in Graphene from quasi-localization to chaotic billards MMM dominikus kölbl 13.10.08 1 / 27 Outline some facts about graphene quasibound states in graphene numerical calculation of
Imaging electrostatically confined Dirac fermions in graphene
Imaging electrostatically confined Dirac fermions in graphene quantum dots 3 4 5 Juwon Lee, Dillon Wong, Jairo Velasco Jr., Joaquin F. Rodriguez-Nieva, Salman Kahn, Hsin- Zon Tsai, Takashi Taniguchi, Kenji
Reduction of Fermi velocity in folded graphene observed by resonance Raman spectroscopy
Reduction of Fermi velocity in folded graphene observed by resonance Raman spectroscopy Zhenhua Ni, Yingying Wang, Ting Yu, Yumeng You, and Zexiang Shen* Division of Physics and Applied Physics, School
NONLOCAL TRANSPORT IN GRAPHENE: VALLEY CURRENTS, HYDRODYNAMICS AND ELECTRON VISCOSITY
NONLOCAL TRANSPORT IN GRAPHENE: VALLEY CURRENTS, HYDRODYNAMICS AND ELECTRON VISCOSITY Leonid Levitov (MIT) Frontiers of Nanoscience ICTP Trieste, August, 2015 Boris @ 60 2 Boris @ 60 3 Boris Blinks the
Spin-orbit effects in graphene and graphene-like materials. Józef Barnaś
Spin-orbit effects in graphene and graphene-like materials Józef Barnaś Faculty of Physics, Adam Mickiewicz University, Poznań & Institute of Molecular Physics PAN, Poznań In collaboration with: A. Dyrdał,
Identify two CDW amplitude modes with extremely small energy scales in LaAgSb2 by ultrafast pump-probe measurement
IMPACT 2016, Cargese, France ICQM International Center for Quantum Materials Identify two CDW amplitude modes with extremely small energy scales in LaAgSb2 by ultrafast pump-probe measurement Nan-Lin Wang
Supplementary Figure 2 Photoluminescence in 1L- (black line) and 7L-MoS 2 (red line) of the Figure 1B with illuminated wavelength of 543 nm.
PL (normalized) Intensity (arb. u.) 1 1 8 7L-MoS 1L-MoS 6 4 37 38 39 4 41 4 Raman shift (cm -1 ) Supplementary Figure 1 Raman spectra of the Figure 1B at the 1L-MoS area (black line) and 7L-MoS area (red
Introductory lecture on topological insulators. Reza Asgari
Introductory lecture on topological insulators Reza Asgari Workshop on graphene and topological insulators, IPM. 19-20 Oct. 2011 Outlines -Introduction New phases of materials, Insulators -Theory quantum
Magneto-plasmonic effects in epitaxial graphene
Magneto-plasmonic effects in epitaxial graphene Alexey Kuzmenko University of Geneva Graphene Nanophotonics Benasque, 4 March 13 Collaborators I. Crassee, N. Ubrig, I. Nedoliuk, J. Levallois, D. van der
Transient lattice dynamics in fs-laser-excited semiconductors probed by ultrafast x-ray diffraction
Transient lattice dynamics in fs-laser-excited semiconductors probed by ultrafast x-ray diffraction K. Sokolowski-Tinten, M. Horn von Hoegen, D. von der Linde Inst. for Laser- and Plasmaphysics, University
arxiv: v1 [cond-mat.mes-hall] 25 Oct 2012
![arxiv: v1 [cond-mat.mes-hall] 25 Oct 2012](/thumbs/73/69020402.jpg "arxiv: v1 [cond-mat.mes-hall] 25 Oct 2012")
Supercollision cooling in undoped graphene A. C. Betz,, S. H. Jhang,, E. Pallecchi,, R. Feirrera, G. Fève, J.-M. Berroir, and B. Plaçais, Laboratoire Pierre Aigrain, ENS-CNRS UMR 855, Universités P. et
Photexcitation cascade and multiple hot-carrier generation in graphene
Photexcitation cascade and multiple hot-carrier generation in graphene K.J. Tielrooij, 1, J.C.W. Song, 2, 3 S.A. Jensen, 4, 5 A. Centeno, 6 A. Pesquera, 6 A. Zurutuza Elorza, 6 M. Bonn, 4 L.S. Levitov,
Self-assembled SiGe single hole transistors
Self-assembled SiGe single hole transistors G. Katsaros 1, P. Spathis 1, M. Stoffel 2, F. Fournel 3, M. Mongillo 1, V. Bouchiat 4, F. Lefloch 1, A. Rastelli 2, O. G. Schmidt 2 and S. De Franceschi 1 1
Supplementary material for High responsivity mid-infrared graphene detectors with antenna-enhanced photo-carrier generation and collection
Supplementary material for High responsivity mid-infrared graphene detectors with antenna-enhanced photo-carrier generation and collection Yu Yao 1, Raji Shankar 1, Patrick Rauter 1, Yi Song 2, Jing Kong
SUPPLEMENTARY INFORMATION
doi:10.1038/nature11231 Materials and Methods: Sample fabrication: Highly oriented VO 2 thin films on Al 2 O 3 (0001) substrates were deposited by reactive sputtering from a vanadium target through reactive
Minimal Update of Solid State Physics
Minimal Update of Solid State Physics It is expected that participants are acquainted with basics of solid state physics. Therefore here we will refresh only those aspects, which are absolutely necessary
Atomic collapse in graphene
Atomic collapse in graphene Andrey V. Shytov (BNL) Work done in collaboration with: L.S. Levitov MIT M.I. Katsnelson University of Nijmegen, Netherlands * Phys. Rev. Lett. 99, 236801; ibid. 99, 246802
Graphene, a single layer of carbon atoms arranged in
pubs.acs.org/nanolett Controlling Graphene Ultrafast Hot Carrier Response from Metal-like to Semiconductor-like by Electrostatic Gating S.-F. Shi,*,, T.-T. Tang, B. Zeng, L. Ju, Q. Zhou, A. Zettl,,, and
Graphene: massless electrons in flatland.
Graphene: massless electrons in flatland. Enrico Rossi Work supported by: University of Chile. Oct. 24th 2008 Collaorators CMTC, University of Maryland Sankar Das Sarma Shaffique Adam Euyuong Hwang Roman
Ultrafast carrier dynamics in InGaN MQW laser diode
Invited Paper Ultrafast carrier dynamics in InGaN MQW laser diode Kian-Giap Gan* a, Chi-Kuang Sun b, John E. Bowers a, and Steven P. DenBaars a a Department of Electrical and Computer Engineering, University
The loss of excess energy by hot carriers, driven out of
pubs.acs.org/nanolett Fast Energy Relaxation of Hot Carriers Near the Dirac Point of Graphene R. Somphonsane, H. Ramamoorthy, G. Bohra, G. He, D. K. Ferry,, Y. Ochiai, N. Aoki, and J. P. Bird*,, Department
Out-of-equilibrium electron dynamics in photoexcited topological insulators studied by TR-ARPES
Cliquez et modifiez le titre Out-of-equilibrium electron dynamics in photoexcited topological insulators studied by TR-ARPES Laboratoire de Physique des Solides Orsay, France June 15, 2016 Workshop Condensed
Superconductivity and spin excitations in orbitally ordered FeSe
Superconductivity and spin excitations in orbitally ordered FeSe Andreas Kreisel, Brian M. Andersen Niels Bohr Institute, University of Copenhagen, 2100 København, Denmark Peter J. Hirschfeld Department
Electronic Origin of High-Temperature Superconductivity in Single-Layer FeSe Superconductor*
Electronic Origin of High-Temperature Superconductivity in Single-Layer FeSe Superconductor* Team #1 - Jyoti Aneja, Brian Busemeyer, Mindy Cartolano, David Casavant Physics 596 Journal Club Presentation
arxiv: v3 [cond-mat.mtrl-sci] 16 Aug 2008
![arxiv: v3 [cond-mat.mtrl-sci] 16 Aug 2008](/thumbs/86/93290957.jpg "arxiv: v3 [cond-mat.mtrl-sci] 16 Aug 2008")
Measurement of the Optical Absorption Spectra of Epitaxial Graphene from Terahertz to Visible Jahan M. Dawlaty, Shriram Shivaraman, Jared Strait, Paul George, Mvs Chandrashekhar, Farhan Rana, and Michael
Title: Ultrafast photocurrent measurement of the escape time of electrons and holes from
Title: Ultrafast photocurrent measurement of the escape time of electrons and holes from carbon nanotube PN junction photodiodes Authors: Nathaniel. M. Gabor 1,*, Zhaohui Zhong 2, Ken Bosnick 3, Paul L.
Dirac matter: Magneto-optical studies
Dirac matter: Magneto-optical studies Marek Potemski Laboratoire National des Champs Magnétiques Intenses Grenoble High Magnetic Field Laboratory CNRS/UGA/UPS/INSA/EMFL MOMB nd International Conference
M R S Internet Journal of Nitride Semiconductor Research
M R S Internet Journal of Nitride Semiconductor Research Volume 2, Article 25 Properties of the Biexciton and the Electron-Hole-Plasma in Highly Excited GaN J.-Chr. Holst, L. Eckey, A. Hoffmann, I. Broser
Lecture 22: Ionized Impurity Scattering
ECE-656: Fall 20 Lecture 22: Ionized Impurity Scattering Mark Lundstrom Purdue University West Lafayette, IN USA 0/9/ scattering of plane waves ψ i = Ω ei p r U S ( r,t) incident plane wave ( ) = 2π H
Supporting Information. by Hexagonal Boron Nitride
Supporting Information High Velocity Saturation in Graphene Encapsulated by Hexagonal Boron Nitride Megan A. Yamoah 1,2,, Wenmin Yang 1,3, Eric Pop 4,5,6, David Goldhaber-Gordon 1 * 1 Department of Physics,
Time-resolved photoelectron spectroscopy: An ultrafast clock to study electron dynamics at surfaces, interfaces and condensed matter
Time-resolved photoelectron spectroscopy: An ultrafast clock to study electron dynamics at surfaces, interfaces and condensed matter Benjamin Stadtmüller Department of Physics and Research Center OPTIMAS,
Pseudospin Magnetism in Graphene
Title Phys. Rev. B 77, 041407 (R) (008) Pseudospin Magnetism in Graphene Hongi Min 1, Giovanni Borghi, Marco Polini, A.H. MacDonald 1 1 Department of Physics, The University of Texas at Austin, Austin
Branislav K. Nikolić
First-principles quantum transport modeling of thermoelectricity in nanowires and single-molecule nanojunctions Branislav K. Nikolić Department of Physics and Astronomy, University of Delaware, Newark,
Graphene Helicoid: The Distinct Properties Promote Application of Graphene Related Materials in Thermal Management
Supporting Information Graphene Helicoid: The Distinct Properties Promote Application of Graphene Related Materials in Thermal Management Haifei Zhan 1,2, Gang Zhang 3,*, Chunhui Yang 1, and Yuantong Gu
Temperature Dependent Optical Band Gap Measurements of III-V films by Low Temperature Photoluminescence Spectroscopy
Temperature Dependent Optical Band Gap Measurements of III-V films by Low Temperature Photoluminescence Spectroscopy Linda M. Casson, Francis Ndi and Eric Teboul HORIBA Scientific, 3880 Park Avenue, Edison,
ELECTRONS AND PHONONS IN SEMICONDUCTOR MULTILAYERS
ELECTRONS AND PHONONS IN SEMICONDUCTOR MULTILAYERS Second Edition B.K. RIDLEY University of Essex CAMBRIDGE UNIVERSITY PRESS Contents Preface Introduction 1 Simple Models of the Electron-Phonon Interaction
Relativistic magnetotransport in graphene
Relativistic magnetotransport in graphene Markus Müller in collaboration with Lars Fritz (Harvard) Subir Sachdev (Harvard) Jörg Schmalian (Iowa) Landau Memorial Conference June 6, 008 Outline Relativistic
Electronic Properties of Hydrogenated Quasi-Free-Standing Graphene
GCOE Symposium Tohoku University 2011 Electronic Properties of Hydrogenated Quasi-Free-Standing Graphene Danny Haberer Leibniz Institute for Solid State and Materials Research Dresden Co-workers Supervising
What is a topological insulator? Ming-Che Chang Dept of Physics, NTNU
What is a topological insulator? Ming-Che Chang Dept of Physics, NTNU A mini course on topology extrinsic curvature K vs intrinsic (Gaussian) curvature G K 0 G 0 G>0 G=0 K 0 G=0 G
Nature, Vol 458, 2009 Leon Camenzind FMM University of Basel,
Nature, Vol 458, 2009 Leon Camenzind University of Basel, 17.6.2011 Outlook Part I: Transient (Spin)-Grating Spectroscopy Part II: Theory of Persistent Spin Helix (PSH) Experimental results Part I Transient
Conductivity of a disordered ferromagnetic monoatomic film
Materials Science-Poland, Vol. 6, No. 4, 008 Conductivity of a disordered ferromagnetic monoatomic film A. PAJA *, B. J. SPISAK Faculty of Physics and Applied Computer Science, AGH University of Science
Multiple Exciton Generation in Quantum Dots. James Rogers Materials 265 Professor Ram Seshadri
Multiple Exciton Generation in Quantum Dots James Rogers Materials 265 Professor Ram Seshadri Exciton Generation Single Exciton Generation in Bulk Semiconductors Multiple Exciton Generation in Bulk Semiconductors
Journal of Atoms and Molecules
Research article Journal of Atoms and Molecules An International Online Journal ISSN 77 147 Hot Electron Transport in Polar Semiconductor at Low Lattice Temperature A. K. Ghorai Physics Department, Kalimpong
ᣂቇⴚ㗔 䇸䉮䊮䊏䊠䊷䊁䉞䉪䉴䈮䉋䉎 䊂䉱䉟䊮䋺ⶄว 㑐䈫㕖ᐔⴧ䉻䉟䊅䊚䉪䉴䇹 ᐔᚑ22ᐕᐲ ળ䇮2011ᐕ3 4ᣣ䇮 ੩ᄢቇᧄㇹ䉨䊞䊮䊌䉴 㗄 A02 ኒᐲ 㑐ᢙᴺℂ 䈮ၮ䈨䈒㕖ᐔⴧ 䊅䊉䉴䉬䊷䊦㔚 વዉ䉻䉟䊅䊚䉪䉴 ઍ ᄢᎿ ㆺ
22201134 A02 GCOE Si device (further downsizing) Novel nanostructures (such as atomic chain) Nanoscale multi-terminal resistance measurement Carbon nanotube transistor Atomic switch Interplay:l Dynamics:
Condensed Matter Physics 2016 Lecture 13/12: Charge and heat transport.
Condensed Matter Physics 2016 Lecture 13/12: Charge and heat transport. 1. Theoretical tool: Boltzmann equation (review). 2. Electrical and thermal conductivity in metals. 3. Ballistic transport and conductance
PG5295 Muitos Corpos 1 Electronic Transport in Quantum dots 2 Kondo effect: Intro/theory. 3 Kondo effect in nanostructures
PG5295 Muitos Corpos 1 Electronic Transport in Quantum dots 2 Kondo effect: Intro/theory. 3 Kondo effect in nanostructures Prof. Luis Gregório Dias DFMT PG5295 Muitos Corpos 1 Electronic Transport in Quantum
QS School Summary
2018 NSF/DOE/AFOSR Quantum Science Summer School June 22, 2018 QS 3 2018 School Summary Kyle Shen (Cornell) Some Thank yous! A Big Thanks to Caroline Brockner!!! Also to our fantastic speakers! Kavli Institute
Organic Molecular Solids
Markus Schwoerer, Hans Christoph Wolf Organic Molecular Solids BICENTENNIAL BICENTENNIAL WILEY-VCH Verlag GmbH & Co. KGaA VII Contents 1 Introduction 1 1.1 What are Organic Solids? 1 1.2 What are the Special
The many-body interactions in graphene at the charge-neutrality
Many-body interactions in quasifreestanding graphene David A. Siegel a,b, Cheol-Hwan Park a, Choongyu Hwang b, Jack Deslippe a,b, Alexei V. Fedorov c, Steven G. Louie a,b, and Alessandra Lanzara a,b,1
Observation of Intra- and Inter-band Transitions in the Optical Response of Graphene
Observation of Intra- and Inter-band Transitions in the Optical Response of Graphene Leandro M. Malard 1, Kin Fai Mak 1, A. H. Castro Neto 2,3, N. M. R. Peres 4, and Tony F. Heinz 1 1 Departments of Physics
SIGNATURES OF SPIN-ORBIT DRIVEN ELECTRONIC TRANSPORT IN TRANSITION- METAL-OXIDE INTERFACES
SIGNATURES OF SPIN-ORBIT DRIVEN ELECTRONIC TRANSPORT IN TRANSITION- METAL-OXIDE INTERFACES Nicandro Bovenzi Bad Honnef, 19-22 September 2016 LAO/STO heterostructure: conducting interface between two insulators
UvA-DARE (Digital Academic Repository) Charge carrier dynamics in photovoltaic materials Jensen, S.A. Link to publication
UvA-DARE (Digital Academic Repository) Charge carrier dynamics in photovoltaic materials Jensen, S.A. Link to publication Citation for published version (APA): Jensen, S. A. (2014). Charge carrier dynamics
Valley Hall effect in electrically spatial inversion symmetry broken bilayer graphene
NPSMP2015 Symposium 2015/6/11 Valley Hall effect in electrically spatial inversion symmetry broken bilayer graphene Yuya Shimazaki 1, Michihisa Yamamoto 1, 2, Ivan V. Borzenets 1, Kenji Watanabe 3, Takashi
Kondo Physics in Nanostructures. A.Abdelrahman Department of Physics University of Basel Date: 27th Nov. 2006/Monday meeting
Kondo Physics in Nanostructures A.Abdelrahman Department of Physics University of Basel Date: 27th Nov. 2006/Monday meeting Kondo Physics in Nanostructures Kondo Effects in Metals: magnetic impurities
Magnetic properties of spherical fcc clusters with radial surface anisotropy
Magnetic properties of spherical fcc clusters with radial surface anisotropy D. A. Dimitrov and G. M. Wysin Department of Physics Kansas State University Manhattan, KS 66506-2601 (December 6, 1994) We
Scaling Anomaly and Atomic Collapse Collective Energy Propagation at Charge Neutrality
Scaling Anomaly and Atomic Collapse Collective Energy Propagation at Charge Neutrality Leonid Levitov (MIT) Electron Interactions in Graphene FTPI, University of Minnesota 05/04/2013 Scaling symmetry:
Supplementary Information Supplementary Figures
Supplementary Information Supplementary Figures Supplementary Fig S1: Multilayer MoS 2 FETs on SiO2/Si substrates, and contact resistance effects. (Left): Transfer curves and effective mobility of multilayer
arxiv: v1 [cond-mat.mes-hall] 19 Sep 2012
![arxiv: v1 [cond-mat.mes-hall] 19 Sep 2012](/thumbs/96/127246005.jpg "arxiv: v1 [cond-mat.mes-hall] 19 Sep 2012")
Photo-excited Carrier Dynamics and Impact Excitation Cascade in Graphene Justin C. W. Song,, Klaas J. Tielrooij 3, Frank H. L. Koppens 3, and Leonid S. Levitov Department of Physics, Massachusetts Institute
PRESENTED BY: PROF. S. Y. MENSAH F.A.A.S; F.G.A.A.S UNIVERSITY OF CAPE COAST, GHANA.
SOLAR CELL AND ITS APPLICATION PRESENTED BY: PROF. S. Y. MENSAH F.A.A.S; F.G.A.A.S UNIVERSITY OF CAPE COAST, GHANA. OUTLINE OF THE PRESENTATION Objective of the work. A brief introduction to Solar Cell
Klein tunneling in graphene p-n-p junctions
10.1149/1.3569920 The Electrochemical Society Klein tunneling in graphene p-n-p junctions E. Rossi 1,J.H.Bardarson 2,3,P.W.Brouwer 4 1 Department of Physics, College of William and Mary, Williamsburg,
ANISOTROPIC TRANSPORT IN THE IRON PNICTIDES
ANISOTROPIC TRANSPORT IN THE IRON PNICTIDES JÖRG SCHMALIAN AMES LABORATORY AND IOWA STATE UNIVERSITY Collaborators theory Ames: Rafael Fernandes Rutgers: Premala Chandra UCLA: Elihu Abrahams experiment
Cooperative Phenomena
Cooperative Phenomena Frankfurt am Main Kaiserslautern Mainz B1, B2, B4, B6, B13N A7, A9, A12 A10, B5, B8 Materials Design - Synthesis & Modelling A3, A8, B1, B2, B4, B6, B9, B11, B13N A5, A7, A9, A12,
Summary lecture VII. Boltzmann scattering equation reads in second-order Born-Markov approximation
Summary lecture VII Boltzmann scattering equation reads in second-order Born-Markov approximation and describes time- and momentum-resolved electron scattering dynamics in non-equilibrium Markov approximation
Thermoelectric Properties Modeling of Bi2Te3
Thermoelectric Properties Modeling of Bi2Te3 Seungwon Lee and Paul von Allmen Jet propulsion Laboratory, California Institute of Technology Funded by DARPA PROM program Overview Introduce EZTB a modeling
Basic Semiconductor Physics
Chihiro Hamaguchi Basic Semiconductor Physics With 177 Figures and 25 Tables Springer 1. Energy Band Structures of Semiconductors 1 1.1 Free-Electron Model 1 1.2 Bloch Theorem 3 1.3 Nearly Free Electron
Nonequilibrium Physics of Correlated Electron Materials IV: Nonequilibrium Phase Transitions
Nonequilibrium Physics of Correlated Electron Materials IV: Nonequilibrium Phase Transitions! A. J. Millis College de France Oct 12, 2015 Two classes of nonequilibrium manybody phenomena 1. Steady state
Ultrafast surface carrier dynamics in topological insulators: Bi 2 Te 3. Marino Marsi
Ultrafast surface carrier dynamics in topological insulators: Bi 2 Te 3 Marino Marsi Laboratoire de Physique des Solides CNRS UMR 8502 - Université Paris-Sud IMPACT, Orsay, September 2012 Outline Topological
Intermediate valence in Yb Intermetallic compounds
Intermediate valence in Yb Intermetallic compounds Jon Lawrence University of California, Irvine This talk concerns rare earth intermediate valence (IV) metals, with a primary focus on certain Yb-based
Ground state of 2D Graphene in presence of Random Charged impurities
Ground state of 2D Graphene in presence of Random Charged impurities Enrico Rossi.. APS March Meeting, Pittsburgh 2009 Session H1. Collaborators Sankar Das Sarma Shaffique Adam. Euyheon Hwang http://www.physics.umd.edu/cmtc/
Graphene. Tianyu Ye November 30th, 2011
Graphene Tianyu Ye November 30th, 2011 Outline What is graphene? How to make graphene? (Exfoliation, Epitaxial, CVD) Is it graphene? (Identification methods) Transport properties; Other properties; Applications;
Scanning tunneling microscopy and spectroscopy of graphene layers on graphite
Scanning tunneling microscopy and spectroscopy of graphene layers on graphite Adina Luican, Guohong Li and Eva Y. Andrei Department of Physics and Astronomy, Rutgers University, Piscataway, New Jersey
Rashba spin-orbit coupling in the oxide 2D structures: The KTaO 3 (001) Surface
Rashba spin-orbit coupling in the oxide 2D structures: The KTaO 3 (001) Surface Sashi Satpathy Department of Physics University of Missouri, Columbia, USA E Ref: K. V. Shanavas and S. Satpathy, Phys. Rev.
Tuning magnetic anisotropy, Kondo screening and Dzyaloshinskii-Moriya interaction in pairs of Fe adatoms
Tuning magnetic anisotropy, Kondo screening and Dzyaloshinskii-Moriya interaction in pairs of Fe adatoms Department of Physics, Hamburg University, Hamburg, Germany SPICE Workshop, Mainz Outline Tune magnetic
Quantum Impurities In and Out of Equilibrium. Natan Andrei
Quantum Impurities In and Out of Equilibrium Natan Andrei HRI 1- Feb 2008 Quantum Impurity Quantum Impurity - a system with a few degrees of freedom interacting with a large (macroscopic) system. Often