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Abstracts of Talks in Parallel Sessions
CCP2014 XXVI IUPAP Conference on Computational Physics August 11-14; Boston, USA Abstracts / Parallel Sessions CONTENTS Monday, Parallel Sessions 1, 13:30-15:15 Materials Science and Nanoscience 1 ................................................................................................... 3 Soft Matter and Biological Physics 1 ..................................................................................................... 6 Fluid Dynamics 1 ................................................................................................................................. 10 Quantum Many-Body Physics 1 .......................................................................................................... 14 Monday, Parallel Sessions 2, 15:45-17:30 Soft Matter and Biological Physics 2 ................................................................................................... 16 Statistical Physics 1: Networks ............................................................................................................ 18 Fluid Dynamics 2 ................................................................................................................................. 20 Novel Computing Paradigms 1 ............................................................................................................ 24 Tuesday, Parallel Sessions 1, 13:30-15:15 Soft Matter and Biological Physics 3 ................................................................................................... 26 Statistical Physics 2: Jamming, Hard -
WHAT IS...A Quasicrystal?, Volume 53, Number 8
?WHAT IS... a Quasicrystal? Marjorie Senechal The long answer is: no one is sure. But the short an- diagrams? The set of vertices of a Penrose tiling does— swer is straightforward: a quasicrystal is a crystal that was known before Shechtman’s discovery. But with forbidden symmetry. Forbidden, that is, by “The what other objects do, and how can we tell? The ques- Crystallographic Restriction”, a theorem that confines tion was wide open at that time, and I thought it un- the rotational symmetries of translation lattices in two- wise to replace one inadequate definition (the lattice) and three-dimensional Euclidean space to orders 2, 3, with another. That the commission still retains this 4, and 6. This bedrock of theoretical solid-state sci- definition today suggests the difficulty of the ques- ence—the impossibility of five-fold symmetry in crys- tion we deliberately but implicitly posed. By now a tals can be traced, in the mineralogical literature, back great many kinds of aperiodic crystals have been to 1801—crumbled in 1984 when Dany Shechtman, a grown in laboratories around the world; most of them materials scientist working at what is now the National are metals, alloys of two or three kinds of atoms—bi- Institute of Standards and Technology, synthesized nary or ternary metallic phases. None of their struc- aluminium-manganese crystals with icosahedral sym- tures has been “solved”. (For a survey of current re- metry. The term “quasicrystal”, hastily coined to label search on real aperiodic crystals see, for example, the such theretofore unthinkable objects, suggests the website of the international conference ICQ9, confusions that Shechtman’s discovery sowed. -
Quasicrystals a New Kind of Symmetry Sandra Nair First, Definitions
Quasicrystals A new kind of symmetry Sandra Nair First, definitions ● A lattice is a poset in which every element has a unique infimum and supremum. For example, the set of natural numbers with the notion of ordering by magnitude (1<2). For our purposes, we can think of an array of atoms/molecules with a clear sense of assignment. ● A Bravais lattice is a discrete infinite array of points generated by linear integer combinations of 3 independent primitive vectors: {n1a1 + n2a2 + n3a3 | n1, n2, n3 ∈ Z}. ● Crystal structures = info of lattice points + info of the basis (primitive) vectors. ● Upto isomorphism of point groups (group of isometries leaving at least 1 fixed point), 14 different Bravais lattice structures possible in 3D. Now, crystals... ● Loosely speaking, crystals are molecular arrangements built out of multiple unit cells of one (or more) Bravais lattice structures. ● Crystallographic restriction theorem: The rotational symmetries of a discrete lattice are limited to 2-, 3-, 4-, and 6-fold. ● This leads us to propose a “functional” definition: A crystal is a material that has a discrete diffraction pattern, displaying rotational symmetries of orders 2, 3, 4 and 6. ● Note: Order 5 is a strictly forbidden symmetry → important for us. Tessellations aka tilings Now that we have diffraction patterns to work with, we consider the question of whether a lattice structure tiles or tessellates the plane. This is where the order of the symmetry plays a role. The crystals are special, as they display translational symmetries. As such, the tiling of their lattice structures (which we could see thanks to diffraction patterns) are periodic- they repeat at regular intervals. -
Cond-Mat.Soft
Spatial correlations of mobility and immobility in a glassforming Lennard-Jones liquid Claudio Donati1, Sharon C. Glotzer1, Peter H. Poole2, Walter Kob3, and Steven J. Plimpton4 1 Polymers Division and Center for Theoretical and Computational Materials Science, NIST, Gaithersburg, Maryland, USA 20899 2Department of Applied Mathematics, University of Western Ontario, London, Ontario N6A 5B7, Canada 3 Institut f¨ur Physik, Johannes Gutenberg Universit¨at, Staudinger Weg 7, D-55099 Mainz, Germany 4 Parallel Computational Sciences Department, Sandia National Laboratory, Albuquerque, NM 87185-1111 (February 1, 2008) Using extensive molecular dynamics simulations of an equilibrium, glass-forming Lennard-Jones mixture, we characterize in detail the local atomic motions. We show that spatial correlations exist among particles undergoing extremely large (“mobile”) or extremely small (“immobile”) displace- ments over a suitably chosen time interval. The immobile particles form the cores of relatively compact clusters, while the mobile particles move cooperatively and form quasi-one-dimensional, string-like clusters. The strength and length scale of the correlations between mobile particles are found to grow strongly with decreasing temperature, and the mean cluster size appears to diverge at the mode-coupling critical temperature. We show that these correlations in the particle displace- ments are related to equilibrium fluctuations in the local potential energy and local composition. PACS numbers: 02.70.Ns, 61.20.Lc, 61.43.Fs I. INTRODUCTION ment over some time) to subsets of extreme mobility or immobility, and (2) to establish connections between this The bulk dynamical properties of many cold, dense “dynamical heterogeneity” and local structure. liquids differ dramatically from what might be expected This paper is organized as follows. -
A Review of Transmission Electron Microscopy of Quasicrystals—How Are Atoms Arranged?
crystals Review A Review of Transmission Electron Microscopy of Quasicrystals—How Are Atoms Arranged? Ruitao Li 1, Zhong Li 1, Zhili Dong 2,* and Khiam Aik Khor 1,* 1 School of Mechanical & Aerospace Engineering, Nanyang Technological University, 50 Nanyang Avenue, Singapore 639798, Singapore; [email protected] (R.L.); [email protected] (Z.L.) 2 School of Materials Science and Engineering, Nanyang Technological University, 50 Nanyang Avenue, Singapore 639798, Singapore * Correspondence: [email protected] (Z.D.); [email protected] (K.A.K.); Tel.: +65-6790-6727 (Z.D.); +65-6592-1816 (K.A.K.) Academic Editor: Enrique Maciá Barber Received: 30 June 2016; Accepted: 15 August 2016; Published: 26 August 2016 Abstract: Quasicrystals (QCs) possess rotational symmetries forbidden in the conventional crystallography and lack translational symmetries. Their atoms are arranged in an ordered but non-periodic way. Transmission electron microscopy (TEM) was the right tool to discover such exotic materials and has always been a main technique in their studies since then. It provides the morphological and crystallographic information and images of real atomic arrangements of QCs. In this review, we summarized the achievements of the study of QCs using TEM, providing intriguing structural details of QCs unveiled by TEM analyses. The main findings on the symmetry, local atomic arrangement and chemical order of QCs are illustrated. Keywords: quasicrystal; transmission electron microscopy; symmetry; atomic arrangement 1. Introduction The revolutionary discovery of an Al–Mn compound with 5-fold symmetry by Shechtman et al. [1] in 1982 unveiled a new family of materials—quasicrystals (QCs), which exhibit the forbidden rotational symmetries in the conventional crystallography. -
Some Considerations Relating to the Dynamics of Quasicrystals
Some considerations relating to the dynamics of quasicrystals M. Pitk¨anen Email: [email protected]. http://tgdtheory.com/public_html/. November 12, 2012 Contents 1 The dynamics of quasicrystals, the dynamics of K¨ahleraction, symbolic dynamics, and the dynamics of self-organization 1 1.1 The non-determinism for the dynamics of quasicrystals contra non-determinism of K¨ahleraction . .1 1.2 The dynamics of quasicrystals as a model for fundamental dynamics or high level sym- bolic dynamics? . .2 1.3 Could ordered water layers around biomolecules be modelled as quasicrystal like structure?3 2 What could be the variational principle behind self-organization? 4 2.1 Why Negentropy Maximization Principle should favor quasicrystals? . .5 2.2 Maximal capacity to represent information with minimal metabolic energy costs as a basic variational principle? . .5 2.3 A possible realization for 4-D dynamics favoring quasicrystal like structures . .6 2.4 Summary . .7 1 The dynamics of quasicrystals, the dynamics of K¨ahlerac- tion, symbolic dynamics, and the dynamics of self-organization The dynamics of quasicrystals looks to me very interesting because it shares several features of the dynamics of K¨ahleraction defining the basic variational principle of classical TGD and defining the dynamics of space-time surfaces. In the following I will compare the basic features of the dynamics of quasicrystals to the dynamics of preferred extremals of K¨ahleraction [K1]. Magnetic body carrying dark matter is the fundamental intentional agent in TGD inspired quantum biology and the cautious proposal is that magnetic flux sheets could define the grid of 3-planes (or more general 3-surfaces) defining quasi-periodic background fields favoring 4-D quasicrystals or more general structures in TGD Universe. -
Quasicrystals
Volume 106, Number 6, November–December 2001 Journal of Research of the National Institute of Standards and Technology [J. Res. Natl. Inst. Stand. Technol. 106, 975–982 (2001)] Quasicrystals Volume 106 Number 6 November–December 2001 John W. Cahn The discretely diffracting aperiodic crystals Key words: aperiodic crystals; new termed quasicrystals, discovered at NBS branch of crystallography; quasicrystals. National Institute of Standards and in the early 1980s, have led to much inter- Technology, disciplinary activity involving mainly Gaithersburg, MD 20899-8555 materials science, physics, mathematics, and crystallography. It led to a new un- Accepted: August 22, 2001 derstanding of how atoms can arrange [email protected] themselves, the role of periodicity in na- ture, and has created a new branch of crys- tallography. Available online: http://www.nist.gov/jres 1. Introduction The discovery of quasicrystals at NBS in the early Crystal periodicity has been an enormously important 1980s was a surprise [1]. By rapid solidification we had concept in the development of crystallography. Hau¨y’s made a solid that was discretely diffracting like a peri- hypothesis that crystals were periodic structures led to odic crystal, but with icosahedral symmetry. It had long great advances in mathematical and experimental crys- been known that icosahedral symmetry is not allowed tallography in the 19th century. The foundation of crys- for a periodic object [2]. tallography in the early nineteenth century was based on Periodic solids give discrete diffraction, but we did the restrictions that periodicity imposes. Periodic struc- not know then that certain kinds of aperiodic objects can tures in two or three dimensions can only have 1,2,3,4, also give discrete diffraction; these objects conform to a and 6 fold symmetry axes. -
Istec Distinguished Lectures, Colorado State University, Istec
Colorado State University’s Information Science and Technology Center (ISTeC) presents two lectures by Sharon Glotzer University of Michigan, Ann Arbor Stuart W. Churchill Collegiate Professor of Chemical Engineering, and Professor of Materials Science and Engineering, Physics ISTeC Distinguished Lecture in conjunction with the Electrical and Computer Engineering Department and Computer Science Department Seminar Series “All Hail the GPU: How the Video Game Industry is Transforming Molecular and Materials Simulation” Monday, May 3, 2010 Reception: 10:30 a.m., Computer Science Room CS305 Lecture: 11:00 – 12:00 noon Location: Computer Science 130 • Department of Chemistry Special Lecture sponsored by ISTeC “From Aristotle to Onsager: Packing and Assembling Tetrahedra” Monday, May3, 2010 Reception: 3:45 p.m. Chemistry Building Room B204 Lecture: 4:00 – 4:50 p.m. Location: Chemistry Building Room B202 ABSTRACTS “All Hail the GPU: How the Video Game Industry is Transforming Molecular and Materials Simulation” Graphics processors (GPUs) traditionally developed for video games are now accessible for use by scientific simulation codes. With speeds reaching 2 teraflop/s on a single chip, GPUs are far faster than today’s CPUs for highly data parallel problems. In this talk, we describe their emerging importance for molecular and materials simulation, what they can do, how they’re being used, and how you can learn to use them. We also discuss current trends, challenges, and recent initiatives in computational science and engineering research and education. “From Aristotle to Onsager: Packing and Assembling Tetrahedra” The packing of shapes has interested humankind for millennia. We investigate the packing of hard, regular tetrahedra and show that entropy alone can order them into thermodynamically stable structures both simple and unexpectedly complex. -
Conformal Quasicrystals and Holography
Conformal Quasicrystals and Holography Latham Boyle1, Madeline Dickens2 and Felix Flicker2;3 1Perimeter Institute for Theoretical Physics, Waterloo, Ontario N2L 2Y5, Canada, N2L 2Y5 2Department of Physics, University of California, Berkeley, California 94720, USA 3Rudolf Peierls Centre for Theoretical Physics, University of Oxford, Department of Physics, Clarendon Laboratory, Parks Road, Oxford, OX1 3PU, United Kingdom Recent studies of holographic tensor network models defined on regular tessellations of hyperbolic space have not yet addressed the underlying discrete geometry of the boundary. We show that the boundary degrees of freedom naturally live on a novel structure, a conformal quasicrystal, that pro- vides a discrete model of conformal geometry. We introduce and construct a class of one-dimensional conformal quasicrystals, and discuss a higher-dimensional example (related to the Penrose tiling). Our construction permits discretizations of conformal field theories that preserve an infinite discrete subgroup of the global conformal group at the cost of lattice periodicity. I. INTRODUCTION dom [12{24]. Meanwhile, quantum information theory provides a unifying language for these studies in terms of entanglement, quantum circuits, and quantum error A central topic in theoretical physics over the past two correction [25]. decades has been holography: the idea that a quantum These investigations have gradually clarified our un- theory in a bulk space may be precisely dual to another derstanding of the discrete geometry in the bulk. There living on the boundary of that space. The most concrete has been a common expectation, based on an analogy and widely-studied realization of this idea has been the with AdS/CFT [1{3], that TNs living on discretizations AdS/CFT correspondence [1{3], in which a gravitational of a hyperbolic space define a lattice state of a critical theory living in a (d + 1)-dimensional negatively-curved system on the boundary and vice-versa. -
2007 136Th Annual Meeting & Exhibition Linking Science and Technology for Global Solutions
2007 136th Annual Meeting & Exhibition Linking Science and Technology for Global Solutions Technical Program Program-at-a-Glance ..............................................................2 Session Listing .......................................................................8 Monday AM ...........................................................................16 Monday PM ............................................................................63 Tuesday AM .........................................................................117 Tuesday PM .........................................................................164 Wednesday AM ...................................................................223 Wednesday PM ...................................................................274 Thursday AM .......................................................................327 General Posters ..................................................................359 Index ....................................................................................363 2007 136th Annual Meeting & Exhibition Monday Tuesday Wednesday Thursday ROOM AM PM AM PM AM PM AM Materials Materials Intellectual Intellectual Materials Materials Materials Processing under Processing under Property in Property in Processing under Processing under Processing under the Influence of the Influence of Materials Materials the Influence of the Influence of the Influence of External Fields: External Fields: Science: Patents, Science: Patents, External Fields: External Fields: -
Speaker and Panelist Bios
Speaker and Panelist Bios Michael A. Meador Michael A. Meador is Director of the National Nanotechnology Coordination Office (NNCO) and leads the NNCO's efforts to promote the goals of the National Nanotechnology Initiative in fostering cutting-edge nanotechnology R&D; establishing world-class testing, characterization and fabrication facilities; facilitating commercialization of nanotechnology-based products; and promoting the responsible development of nanotechnology. He is on detail from the NASA Glenn Research Center where, since 1983, he has been involved in planning, executing, and managing materials R&D including serving as the Chief of the Polymers Branch (1988 to 2011). From 2011 to 2014, he initiated and led a NASA/industry/university project to mature and demonstrate high payoff nanotechnologies for use in future NASA missions under the Space Technology Mission Directorate's Game Changing Development Program. Meador received the NASA Equal Opportunity Employment Medal (2002) for his efforts to increase participation of students and faculty from minority-serving institutions in NASA's materials R&D and the NASA Exceptional Service Medal (2014) in recognition of his proactive leadership of NASA nanotechnology R&D. Dr. Meador is a Fellow of the American Chemical Society, an Adjunct Faculty Member in the Department of Materials Science and Engineering at Clemson University, and serves on several advisory boards for university departments and institutes. He received a BA in Chemistry from Ithaca College and a PhD in Organic Chemistry from Michigan State University. Lisa Friedersdorf Lisa Friedersdorf is Deputy Director of NNCO. She has been involved in nanotechnology for nearly twenty years, with a particular interest in advancing technology commercialization through university-industry-government collaboration. -
Nanotechnology and Quasicrystals: from Self Assembly to Photonic Applications
Nanotechnology and Quasicrystals: From self assembly to photonic applications. Ron Lifshitz Raymond and Beverly Sackler School of Physics & Astronomy Tel Aviv University, 69978 Tel Aviv, Israel. After providing a concise overview on quasicrystals and their discovery more than a quarter of a century ago, I consider the unexpected interplay between nanotechnology and quasiperiodic crystals. Of particular relevance are efforts to fabricate artificial functional micro- or nanostructures, as well as efforts to control the self-assembly of nanostructures, where current knowledge about the possibility of having long-range order without periodicity can provide significant advantages. I discuss examples of systems ranging from artificial metamaterials for photonic applications, through self-assembled soft matter, to surface waves and optically-induced nonlinear photonic quasicrystals. 1 Nanotechnology and quasicrystals? When organizers of the NATO Advanced Research Workshop on nanotechnology, held in St. Petersburg in June 2008, asked me to deliver a keynote lecture on quasicrystals I was certain that they had made a mistake. I have been studying quasicrystals for over 15 years and investigating nanomechanical systems for just about a decade, and although one always finds connections between different scientific fields, I had never expected such an invitation. Nevertheless, the organizers insisted and explained that they wanted to learn about the possibility of exploiting nontrivial symmetries—perhaps imitating what viruses do—and in general, learn the lesson of a scientific community that was forced by nature to keep an open mind and “think outside of the box”. This chapter is motivated by my presentation on quasicrystals at the NATO ARW on nanotechnology in St.