The Physics of Graphene

Total Page:16

File Type:pdf, Size:1020Kb

The Physics of Graphene Proposal for a Workshop at the Aspen Center for Physics Summer 2008 Organizers: Prof. Antonio H. Castro Neto (contact person) Department of Physics Boston University 590 Commonwealth Ave. Boston, MA, 02215 Phone: 617-353-6116 Email: [email protected] Prof. Alessandra Lanzara (responsible for working to ensure diversity) Department of Physics University of California Berkeley 321 Birge Hall Berkeley, CA 94720-7300 USA Phones: (510) 642-4863 (campus) (510) 486-5303 (LBL) Email: [email protected] Prof. Allan MacDonald Department of Physics University of Texas at Austin 1 University Station C1600 Austin, Tx 78712-0264 Phone: 512-232-9113 Email: [email protected] Title: The Physics of Graphene Rationale: The discovery of an anomalous integer quantum Hall effect in graphene (a form of two-dimensional carbon) by two independent groups (K.S. Novoselov et al., Nature 438, 197 (2005), and Yuanbo Zhang et al., Nature 438, 201 (2005)) has stirred a lot of interest in the scientific community (see, for instance, Nature “News and Views“ by C. Kane, Nature 438, 168 (2005), and http://physicsweb.org/articles/news/9/11/6/1) as well as in the international media (see, for instance, a BBC News Report on the subject: http://news.bbc.co.uk/1/hi/sci/tech/3944651.stm). The excitement behind this discovery has two main driven forces: basic science, and technological implications. The excitement on graphene can be measured by the numbers of manuscripts written on the subject. In Fig.1.1 we show the number of articles posted on the cond-mat arXiv.org server from 1998 till 2007 containing the word of graphene in the abstract. One can clearly see that there is an exponential growth in the literature since the publication of the papers by Geim and Kim’s groups. Graphene is a condensed matter realization of the Dirac equation since the electronic dispersion close to the Brillouin zone edges are conical with a Fermi-Dirac velocity of order of one hundredth of the velocity of light (see, for instance, Drawing conclusions from graphene by A. H. Castro Neto, F. Guinea and N.M. R. Peres, Physics World 19, 33 (2006), http://physicsweb.org/articles/world/19/11/7/1). Hence, unlike most of other solids, graphene electrons cannot be described in terms of an effective mass. This fact has strong implications in many of the physical properties of these systems: the electronic density of states vanishes at the Fermi level, there is very poor screening of the Coulomb interaction, the Dirac fermions interact very strongly with disorder such as vacancies, and Landau’s Fermi liquid theory is not applicable. That is, graphene is a non- Fermi liquid system. In fact, graphene share many properties with quasi-two-dimensional d-wave superconductors (such as superconducting cuprates) who can also be described in terms of Dirac-like excitations. As a result of this exotic behavior, graphene has unusual collective excitations (such as zero modes), and an anomalous integer quantum Hall effect with a finite Berry’s phase. There has been an intense experimental effort in recent months in graphene research. Cutting-edge research techniques such as infrared absorption, angle resolved photo-emission (ARPES), scanning tunneling microscopy (STM), and neutron scattering, are being used to study this system. Some of these techniques that have been used so successfully in high temperature superconductivity research, can be directly applied to these materials that also show layered structure. Because of its high electronic mobility, structural flexibility, and capability of being tuned from p-type to n-type doping by the application of a gate voltage (see, K. S. Novoselov et al., Science 306, 666 (2004)), graphene is being considered a breakthrough in terms of carbon-based nano-electronics. In fact, unlike carbon-nanotubes, graphene can be easily patterned with standard lithographic techniques and does not present problems with electric contacts. With the predicted saturation in silicon-based technology due to limitations in miniaturization, integration, yield enhancement, and inter- connectivity (see, for instance, the International Technology Roadmap for Semiconductors, http://www.itrs.net/Common/2004Update/2004Update.htm), there is a growing interest by technology development companies in graphene research. The interest in the anomalous properties of graphene only adds to the intriguing discovery that graphite (a crystal made out a stack of graphene layers) can be made ferromagnetic when sufficiently disordered (see, for instance, the focus page of American Physical Society in 2003, http://focus.aps.org/story/v12/st20). This discovery still remains unexplained theoretically (even in fact of many proposals) and has drawn a lot of attention to modern carbon research (see http://physicsweb.org/article/news/5/12/11\#11, and http://nanotechweb.org/articles/news/3/3/13 ). It is quite clear to us that graphene research is in exponential growth. Because of its tradition, infrastructure, and location, the Aspen Center for Physics is in a special position to host the first international workshop in graphene research in the summer of 2008. We have assembled a list of participants that represents respected scientists who are currently doing significant in the field. We expect that this list will change with time until the date of the workshop. Proposed dates: 16 June – 4 July (preferred); 23 June – 11 July (acceptable); 14 July – 8 August (acceptable). Proposed Participants (in alphabetical order): B. L. Altshuler (Columbia University, USA); T. Ando (Tokyo Institute of Technology, Japan); Eva Andrei (Rutgers University, USA); Reza Asgari (Tehran); Alexander Balatsky (LANL, USA); G. Baskaran (IMS, India); Dmitri Basov (University of California at San Diego, USA); Yarsilav Blanter (Delft, The Netherlands); Carlo Beenakker (Leiden, The Netherlands); Claire Berger (Laboratoire d'Études des Propriétés Électroniques des Solides, France); Arne Brataas (Trondheim); Luiz Brey (ICCM, Spain); J. P. Carbotte (McMaster, Canada); M.W.C. Dharma-wardana (NRC-Canada) Walt de Heer (Georgia Institute of Technology, USA); Millie Dresselhaus (MIT, USA); Konstantin Efetov (Bochum, Germany); W. Falko (Lancaster University, UK); Eduardo Fradkin (University of Illinois at Urbana-Champaing, USA); Andre Ferrari (Oxford, England); Herb Fertig (Indiana University, USA); H. Fukuyama (University of Tokyo, Japan); Victor Galitski (University of Maryland, USA); Andre Geim (University of Manchester, UK); Mark Goerbig (Orsay, France); Bennett Goldberg (Boston University, USA); Francisco Guinea (Instituto de Ciencia de Materiales de Madrid, Spain); G.-H. Gweon (University of California at Berkeley, USA); Duncan Haldane (Princeton University, USA); Ayako Hashimoto (Tsukuba University, Japan); Igor Herbut (Simon Fraser, Canada); Euyheon Hwang (University of Maryland, USA); Mihail Katsnelson (Nejimegen, The Netherlands); Eun-Ah Kim (Stanford University, USA); Philip Kim (Columbia University, USA); D. Khveshchenko (Chapel Hill, USA); Valeri Kotov (Boston University, USA); Yakov Kopelevich (Unicamp, Brazil); Jeannie Lau (University of California at Riverside, USA); Patrick A. Lee (MIT, USA); L. S. Levitov (MIT, USA); S. Louie (University of California at Berkeley, USA); Maria Pilar Lopez-Sancho (ICCM, Spain); Charles Marcus (Harvard, USA); Ivar Martin (LANL, USA); P. L. McEuen (Cornell, USA); A. Morpurgo (Delft, The Netherlands); Y. Niimi (University of Tokyo, Japan); Cristiane Morais-Smith (Utrecht, The Netherlands); E. Mucciolo (Central Florida University, USA); Kentaro Nomura (University of Texas at Austin, USA); K. Novoselov (University of Manchester, UK); J. Nilsson (Leiden, The Netherlands); Tami Pereg-Barnea (University of Texas at Austin, USA); Vitor Pereira (Boston University, USA); Nuno Peres (University of Minho, Portugal); F. M. Peeters (Antwerpen, Belgium); Aron Pinczuk (Columbia University, USA); Marco Polini (INFM, Italy); Elsa Prada (Karlshure, Germany); Subir Sachdev (Harvard University, USA); K. Sengupta (Saha Institute, India); Sankar das Sarma (University of Maryland, USA); Ramamurti Shankar (Yale University, USA); Elena Stolyarov (Columbia University, USA); Y.-W. Son (Berkeley, USA); Joao Lopes dos Santos (University of Porto, Portugal); S. G. Sharapov (MacMaster University, CA); Manfred Sigrist (ETH, Zurich); H. L. Stormer (Columbia University, USA); Anna Swan (Boston University, USA); Shan-Wen Tsai (University of California at Riverside, USA); B. Uchoa (Boston University, USA); Oskar Vafek (Florida State University, USA); Maria Vozmediano (ICCM, Spain); Katsunori Wakabayashi (Hiroshima University, Japan); Y. Zhang (Berkeley, USA); S. Zhou (University of California at Berkeley, USA); K. Ziegler (Augsburg, Germany). .
Recommended publications
  • Joaquin M. Luttinger 1923–1997
    Joaquin M. Luttinger 1923–1997 A Biographical Memoir by Walter Kohn ©2014 National Academy of Sciences. Any opinions expressed in this memoir are those of the author and do not necessarily reflect the views of the National Academy of Sciences. JOAQUIN MAZDAK LUTTINGER December 2, 1923–April 6, 1997 Elected to the NAS, 1976 The brilliant mathematical and theoretical physicist Joaquin M. Luttinger died at the age of 73 years in the city of his birth, New York, which he deeply loved throughout his life. He had been in good spirits a few days earlier when he said to Walter Kohn (WK), his longtime collaborator and friend, that he was dying a happy man thanks to the loving care during his last illness by his former wife, Abigail Thomas, and by his stepdaughter, Jennifer Waddell. Luttinger’s work was marked by his exceptional ability to illuminate physical properties and phenomena through Visual Archives. Emilio Segrè Photograph courtesy the use of appropriate and beautiful mathematics. His writings and lectures were widely appreciated for their clarity and fine literary quality. With Luttinger’s death, an By Walter Kohn influential voice that helped shape the scientific discourse of his time, especially in condensed-matter physics, was stilled, but many of his ideas live on. For example, his famous 1963 paper on condensed one-dimensional fermion systems, now known as Tomonaga-Luttinger liquids,1, 2 or simply Luttinger liquids, continues to have a strong influence on research on 1-D electronic dynamics. In the 1950s and ’60s, Luttinger also was one of the great figures who helped construct the present canon of classic many-body theory while at the same time laying founda- tions for present-day revisions.
    [Show full text]
  • Arxiv:Cond-Mat/0106256 V1 13 Jun 2001
    Quantum Phenomena in Low-Dimensional Systems Michael R. Geller Department of Physics and Astronomy, University of Georgia, Athens, Georgia 30602-2451 (June 18, 2001) A brief summary of the physics of low-dimensional quantum systems is given. The material should be accessible to advanced physics undergraduate students. References to recent review articles and books are provided when possible. I. INTRODUCTION transverse eigenfunction and only the plane wave factor changes. This means that motion in those transverse di- A low-dimensional system is one where the motion rections is \frozen out," leaving only motion along the of microscopic degrees-of-freedom, such as electrons, wire. phonons, or photons, is restricted from exploring the full This article will provide a very brief introduction to three dimensions of our world. There has been tremen- the physics of low-dimensional quantum systems. The dous interest in low-dimensional quantum systems dur- material should be accessible to advanced physics under- ing the past twenty years, fueled by a constant stream graduate students. References to recent review articles of striking discoveries and also by the potential for, and and books are provided when possible. The fabrication of realization of, new state-of-the-art electronic device ar- low-dimensional structures is introduced in Section II. In chitectures. Section III some general features of quantum phenomena The paradigm and workhorse of low-dimensional sys- in low dimensions are discussed. The remainder of the tems is the nanometer-scale semiconductor structure, or article is devoted to particular low-dimensional quantum semiconductor \nanostructure," which consists of a com- systems, organized by their \dimension." positionally varying semiconductor alloy engineered at the atomic scale [1].
    [Show full text]
  • Shaffique Adam a Self-Consistent Theory for Graphene Transport
    A self-consistent theory for graphene transport Shaffique Adam Collaborators: Sankar Das Sarma, Piet Brouwer, Euyheon Hwang, Michael Fuhrer, Enrico Rossi, Ellen Williams, Philip Kim, Victor Galitski, Masa Ishigami, Jian-Hao Chen, Sungjae Cho, and Chaun Jang. Schematic 1. Introduction - Graphene transport mysteries - Need for a hirarchy of approximations - Sketch of self-consistent theory: discussion of ansatz and its predictions 2. Characterizing the Dirac Point - What the Dirac point really looks like - Comparison of self-consistent theory and energy functional minimization results 3. Quantum to classical crossover 4. Effective medium theory 5. Comparison with experiments Introduction to graphene transport mysteries High Density Low Density Hole carriers Electron carriers E electrons kx ky holes n Figure from Novoselov et al. (2005) Vg n Fuhrer group (unpublished) 2006 ∝ - Constant (and high) mobility over a wide range of density. Dominant scattering mechanism? - Minimum conductivity plateau ? - Mechanism for conductivity without carriers? What could be going on? Graphene - Honeycomb lattice: Dirac cone with trigonal warping, - Disorder: missing atoms, ripples, edges, impurities (random or correlated) - Interactions: screening, exchange, correlation, velocity/disorder renormalization - Phonons - Localization: quantum interference - Temperature - ... Exact solution is impossible -> reasonable hierarchy of approximations Any small parameters? - For transport, we can use a low energy effective theory i.e. Dirac Hamiltonian. Corrections,
    [Show full text]
  • Chicago Physics One
    CHICAGO PHYSICS ONE 3:25 P.M. December 02, 1942 “All of us... knew that with the advent of the chain reaction, the world would never be the same again.” former UChicago physicist Samuel K. Allison Physics at the University of Chicago has a remarkable history. From Albert Michelson, appointed by our first president William Rainey Harper as the founding head of the physics department and subsequently the first American to win a Nobel Prize in the sciences, through the mid-20th century work led by Enrico Fermi, and onto the extraordinary work being done in the department today, the department has been a constant source of imagination, discovery, and scientific transformation. In both its research and its education at all levels, the Department of Physics instantiates the highest aspirations and values of the University of Chicago. Robert J. Zimmer President, University of Chicago Welcome to the inaugural issue of Chicago Physics! We are proud to present the first issue of Chicago Physics – an annual newsletter that we hope will keep you connected with the Department of Physics at the University of Chicago. This newsletter will introduce to you some of our students, postdocs and staff as well as new members of our faculty. We will share with you good news about successes and recognition and also convey the sad news about the passing of members of our community. You will learn about the ongoing research activities in the Department and about events that took place in the previous year. We hope that you will become involved in the upcoming events that will be announced.
    [Show full text]
  • Electronic Structure of Full-Shell Inas/Al Hybrid Semiconductor-Superconductor Nanowires: Spin-Orbit Coupling and Topological Phase Space
    Electronic structure of full-shell InAs/Al hybrid semiconductor-superconductor nanowires: Spin-orbit coupling and topological phase space Benjamin D. Woods,1 Sankar Das Sarma,2 and Tudor D. Stanescu1, 2 1Department of Physics and Astronomy, West Virginia University, Morgantown, WV 26506, USA 2Condensed Matter Theory Center and Joint Quantum Institute, Department of Physics, University of Maryland, College Park, Maryland, 20742-4111, USA We study the electronic structure of full-shell superconductor-semiconductor nanowires, which have recently been proposed for creating Majorana zero modes, using an eight-band ~k · ~p model within a fully self-consistent Schrodinger-Poisson¨ scheme. We find that the spin-orbit coupling induced by the intrinsic radial electric field is generically weak for sub-bands with their minimum near the Fermi energy. Furthermore, we show that the chemical potential windows consistent with the emergence of a topological phase are small and sparse and can only be reached by fine tunning the diameter of the wire. These findings suggest that the parameter space consistent with the realization of a topological phase in full-shell InAs/Al nanowires is, at best, very narrow. Hybrid semiconductor-superconductor (SM-SC) nanowires butions) and ii) the electrostatic effects (by self-consistently have recently become the subject of intense research in the solving a Schrodinger-Poisson¨ problem). We note that these context of the quest for topological Majorana zero modes are crucial issues for the entire research field of SM-SC hy- (MZMs) [1,2]. Motivated by the promise of fault-tolerant brid nanostructures, but they have only recently started to be topological quantum computation [3,4] and following con- addressed, and only within single-orbital approaches [27–30].
    [Show full text]
  • Sankar Das Sarma 3/11/19 1 Curriculum Vitae
    Sankar Das Sarma 3/11/19 Curriculum Vitae Sankar Das Sarma Richard E. Prange Chair in Physics and Distinguished University Professor Director, Condensed Matter Theory Center Fellow, Joint Quantum Institute University of Maryland Department of Physics College Park, Maryland 20742-4111 Email: [email protected] Web page: www.physics.umd.edu/cmtc Fax: (301) 314-9465 Telephone: (301) 405-6145 Published articles in APS journals I. Physical Review Letters 1. Theory for the Polarizability Function of an Electron Layer in the Presence of Collisional Broadening Effects and its Experimental Implications (S. Das Sarma) Phys. Rev. Lett. 50, 211 (1983). 2. Theory of Two Dimensional Magneto-Polarons (S. Das Sarma), Phys. Rev. Lett. 52, 859 (1984); erratum: Phys. Rev. Lett. 52, 1570 (1984). 3. Proposed Experimental Realization of Anderson Localization in Random and Incommensurate Artificial Structures (S. Das Sarma, A. Kobayashi, and R.E. Prange) Phys. Rev. Lett. 56, 1280 (1986). 4. Frequency-Shifted Polaron Coupling in GaInAs Heterojunctions (S. Das Sarma), Phys. Rev. Lett. 57, 651 (1986). 5. Many-Body Effects in a Non-Equilibrium Electron-Lattice System: Coupling of Quasiparticle Excitations and LO-Phonons (J.K. Jain, R. Jalabert, and S. Das Sarma), Phys. Rev. Lett. 60, 353 (1988). 6. Extended Electronic States in One Dimensional Fibonacci Superlattice (X.C. Xie and S. Das Sarma), Phys. Rev. Lett. 60, 1585 (1988). 1 Sankar Das Sarma 7. Strong-Field Density of States in Weakly Disordered Two Dimensional Electron Systems (S. Das Sarma and X.C. Xie), Phys. Rev. Lett. 61, 738 (1988). 8. Mobility Edge is a Model One Dimensional Potential (S.
    [Show full text]
  • Table of Contents (Print)
    NEWSPAPER 97 Kinetic energy (vertical) of deuterons after fragmentation of deuterium molecules in a pump-probe experiment, for a given time delay (horizontal) between the pump and the probe pulses. Colors denote the number of deuterons, with orange-yellow being the highest. See article 193001. PHYSICAL REVIEW LETTERS PRL 97 (19), 190201– 199901, 10 November 2006 (280 total pages) Contents Articles published 4 November–10 November 2006 VOLUME 97, NUMBER 19 10 November 2006 General Physics: Statistical and Quantum Mechanics, Quantum Information, etc. Quantum Feedback Control for Deterministic Entangled Photon Generation .......................................... 190201 Masahiro Yanagisawa General Approach to Quantum-Classical Hybrid Systems and Geometric Forces ..................................... 190401 Qi Zhang and Biao Wu Condensation of N Interacting Bosons: A Hybrid Approach to Condensate Fluctuations ............................. 190402 Anatoly A. Svidzinsky and Marlan O. Scully Dipole Polarizability of a Trapped Superfluid Fermi Gas . ............................................................ 190403 A. Recati, I. Carusotto, C. Lobo, and S. Stringari Loschmidt Echo in a System of Interacting Electrons ................................................................ 190404 G. Manfredi and P.-A. Hervieux Detection Scheme for Acoustic Quantum Radiation in Bose-Einstein Condensates . ................................. 190405 Ralf Schu¨tzhold Quantum Stripe Ordering in Optical Lattices . ........................................................................
    [Show full text]
  • A DIALOGUE on the THEORY of HIGH Tc
    A DIALOGUE ON THE THEORY OF HIGH Tc Superconducting Bi2Sr2CaCu2O,, as seen with reflected differential interference contrast microscopy. This view of the ab plane surface of a platelet of the ceramic material shows this high-temperature superconductor's strong planar structure. (Photomicrograph by Michael W. Davidson, W. Jack Rink and Joseph B. Schlenoff, Florida State University.) Figure 1 5 4 PHYSICS TODAY JUNE 1991 The give-and-take between two solid-state theorists offers insight into materials with high superconducting transition temperatures and illustrates the kind of thinking that goes into developing a new theory. Philip W. Anderson and Robert Schrieffer Although ideas that would explain the behavior of the formalism to do their calculations.' I believe they are high-temperature superconducting materials have been wrong. I'd like to hear your opinion, but first let me say a offered almost since their discovery, high-Tt. theory is still couple of things that bear on this question. In the first very much in flux. Two of the leading figures in condensed place, I think few people realize that we now know of at matter theory are Philip Anderson, the Joseph Henry least six different classes of electron superconductors, and Professor of Physics at Princeton University, and Robert two other BCS fluids as well. Out of these only one obeys Schrieffer, Chancellor's Professor at the University of the so-called conventional theory—that is, BCS with California, Santa Barbara. Anderson's ideas have fo- phonons that fit unmodified versions of Eliashberg's cused, in his own words, "on a non-Fermi-liquid normal equations.
    [Show full text]
  • Theory and Modeling in Nanoscience
    Theory and Modeling in Nanoscience Report of the May 10–11, 2002, Workshop Conducted by the Basic Energy Sciences and Advanced Scientific Computing Advisory Committees to the Office of Science, Department of Energy Cover illustrations: TOP LEFT: Ordered lubricants confined to nanoscale gap (Peter Cummings). BOTTOM LEFT: Hypothetical spintronic quantum computer (Sankar Das Sarma and Bruce Kane). TOP RIGHT: Folded spectrum method for free-standing quantum dot (Alex Zunger). MIDDLE RIGHT: Equilibrium structures of bare and chemically modified gold nanowires (Uzi Landman). BOTTOM RIGHT: Organic oligomers attracted to the surface of a quantum dot (F. W. Starr and S. C. Glotzer). Theory and Modeling in Nanoscience Report of the May 10–11, 2002, Workshop Conducted by the Basic Energy Sciences and Advanced Scientific Computing Advisory Committees to the Office of Science, Department of Energy Organizing Committee C. William McCurdy Co-Chair and BESAC Representative Lawrence Berkeley National Laboratory Berkeley, CA 94720 Ellen Stechel Co-Chair and ASCAC Representative Ford Motor Company Dearborn, MI 48121 Peter Cummings The University of Tennessee Knoxville, TN 37996 Bruce Hendrickson Sandia National Laboratories Albuquerque, NM 87185 David Keyes Old Dominion University Norfolk, VA 23529 This work was supported by the Director, Office of Science, Office of Basic Energy Sciences and Office of Advanced Scientific Computing Research, of the U.S. Department of Energy. Table of Contents Executive Summary.......................................................................................................................1
    [Show full text]
  • Emergence and Reductionism: an Awkward Baconian Alliance
    Emergence and Reductionism: an awkward Baconian alliance Piers Coleman1;3 1Center for Materials Theory, Department of Physics and Astronomy, Rutgers University, 136 Frelinghuysen Rd., Piscataway, NJ 08854-8019, USA and 2 Department of Physics, Royal Holloway, University of London, Egham, Surrey TW20 0EX, UK. Abstract This article discusses the relationship between emergence and reductionism from the perspective of a condensed matter physicist. Reductionism and emergence play an intertwined role in the everyday life of the physicist, yet we rarely stop to contemplate their relationship: indeed, the two are often regarded as conflicting world-views of science. I argue that in practice, they compliment one-another, forming an awkward alliance in a fashion envisioned by the philosopher scientist, Francis Bacon. Looking at the historical record in classical and quantum physics, I discuss how emergence fits into a reductionist view of nature. Often, a deep understanding of reductionist physics depends on the understanding of its emergent consequences. Thus the concept of energy was unknown to Newton, Leibniz, Lagrange or Hamilton, because they did not understand heat. Similarly, the understanding of the weak force awaited an understanding of the Meissner effect in superconductivity. Emergence can thus be likened to an encrypted consequence of reductionism. Taking examples from current research, including topological insulators and strange metals, I show that the convection between emergence and reductionism continues to provide a powerful driver for frontier scientific research, linking the lab with the cosmos. Article to be published by Routledge (Oxford and New York) as part of a volume entitled arXiv:1702.06884v2 [physics.hist-ph] 7 Dec 2017 \Handbook of Philosophy of Emergence", editors Sophie Gibb, Robin Hendry and Tom Lancaster.
    [Show full text]
  • 2016 Annual Report Vision
    “Perimeter Institute is now one of the world’s leading centres in theoretical physics, if not the leading centre.” – Stephen Hawking, Emeritus Lucasian Professor, University of Cambridge 2016 ANNUAL REPORT VISION To create the world's foremostcentre for foundational theoretlcal physics, uniting publlc and private partners, and the world's best scientific minds, in a shared enterprise to achieve breakthroughs that will transform ourfuture CONTENTS Welcome . .2 Message from the Board Chair . 4 Message from the Institute Director . 6 Research . .8 At the Quantum Frontier . 10 Exploring Exotic Matter . .12 A New Window to the Cosmos . .14 A Holographic Revolution . .16 Honours, Awards, and Major Grants . .18 Recruitment . 20 Research Training . .24 Research Events . 26 Linkages . 28 Educational Outreach and Public Engagement . 30 Advancing Perimeter’s Mission . .36 Blazing New Paths . 38 Thanks to Our Supporters . .40 Governance . 42 Facility . 46 Financials . .48 Looking Ahead: Priorities and Objectives for the Future . 53 Appendices . 54 This report covers the activities and finances of Perimeter Institute for Theoretical Physics from August 1, 2015, to July 31, 2016 . Photo credits The Royal Society: Page 5 Istock by Getty Images: 11, 13, 17, 18 Adobe Stock: 23, 28 NASA: 14, 36 WELCOME Just one breakthrough in theoretical physics can change the world. Perimeter Institute is an independent research centre located in Waterloo, Ontario, Canada, which was created to accelerate breakthroughs in our understanding of the cosmos. Here, scientists seek to discover how the universe works at all scales – from the smallest particle to the entire cosmos. Their ideas are unveiling our remote past and enabling the technologies that will shape our future.
    [Show full text]
  • Popular Science Background
    THE NOBEL PRIZE IN PHYSICS 2016 POPULAR SCIENCE BACKGROUND Strange phenomena in matter’s fatlands This year’s Laureates opened the door on an unknown world where matter exists in strange states. The Nobel Prize in Physics 2016 is awarded with one half to David J. Thouless, University of Washington, Seattle, and the other half to F. Duncan M. Haldane, Princeton University, and J. Michael Kosterlitz, Brown Univer- sity, Providence. Their discoveries have brought about breakthroughs in the theoretical understanding of matter’s mysteries and created new perspectives on the development of innovative materials. David Thouless, Duncan Haldane, and Michael Kosterlitz have used advanced mathematical methods to explain strange phenomena in unusual phases (or states) of matter, such as superconductors, super- fuids or thin magnetic flms. Kosterlitz and Thouless have studied phenomena that arise in a fat world – on surfaces or inside extremely thin layers that can be considered two-dimensional, compared to the three dimensions (length, width and height) with which reality is usually described. Haldane has also studied matter that forms threads so thin they can be considered one-dimensional. The physics that takes place in the fatlands is very dif- ferent to that we recognise in the world around us. Even if very thinly distributed matter consists of millions of atoms, and even if each atom’s behaviour can be explai- Plasma ned using quantum physics, atoms display completely diferent properties when lots of them come together. New collective phenomena are being continually disco- vered in these fatlands, and condensed matter physics is now one of the most vibrant felds in physics.
    [Show full text]