The Adventure of Physics – Vol.Iv the Quantum of Change
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Lecture Notes Are Based on a Series of Lectures Given by Myself from April to June 2009 in the School of Mathematics at Trinity College, Dublin
Introduction to Supersymmetry Christian SÄamann Notes by Anton Ilderton August 24, 2009 1 Contents 1 Introduction 5 1.1 A SUSY toy model ............................... 5 1.2 What is it good for? .............................. 10 2 Spinors 12 2.1 The Poincar¶egroup .............................. 12 2.2 Spin and pin groups .............................. 18 2.3 Summary .................................... 22 3 The SUSY algebra 24 3.1 SUSY algebra on R1;3 ............................. 24 3.2 Representations ................................. 25 3.3 The Wess{Zumino model ........................... 28 4 Superspace and super¯elds 32 4.1 Reminder: Gra¼mann numbers. ........................ 32 4.2 Flat superspace ................................. 33 4.3 Super¯elds ................................... 35 5 SUSY{invariant actions from super¯elds 38 5.1 Actions from chiral s¯elds ........................... 38 5.2 Actions with vector super¯elds ........................ 42 6 SUSY quantum ¯eld theories 49 6.1 Abstract considerations ............................ 49 6.2 S¯eld quantisation of chiral s¯elds ...................... 51 6.3 Quantisation of Super Yang{Mills theory . 58 7 Maximally SUSY Yang{Mills theories 63 7.1 Spinors in arbitrary dimensions ........................ 63 7.2 Actions and constraint equations ....................... 64 7.3 d = 4, N = 4 super Yang{Mills theory .................... 67 8 Seiberg-Witten Theory 72 8.1 The moduli space of pure N = 2 SYM theory . 72 8.2 Duality ..................................... 74 8.3 The exact e®ective action ........................... 75 A Conventions and identities 78 B Solutions to exercises 81 2 Preface Supersymmetry, or SUSY for short, is an extension of the classical symmetries of ¯eld theories. SUSY was discovered in the early 1970's and has attracted growing attention ever since, even though there is still no experimental evidence for its existence up to this day. -
MOTION MOUNTAIN the Adventure of Physics – Vol.Vi the Strand Model – a Speculation on Unification
Christoph Schiller MOTION MOUNTAIN the adventure of physics – vol.vi the strand model – a speculation on unification www.motionmountain.net MOTION MOUNTAIN The Adventure of Physics – Vol. VI The Strand Model – A Speculation on Unification What is the origin of colours? Which problems in physics are unsolved since the year 2000 and what might be their solution? At what distance between two points does it become impossible to find room for a third one in between? Why do change and motion exist? What is the most fantastic voyage possible? Answering these and other questions, this book gives an entertaining and mind-twisting introduction to the search for the final theory of physics. The search leads to the strand model:Basedona simple principle, strands reproduce quantum theory, the standard model of particle physics and general relativity. Strands leave no room for alternative theories, agree with all experimental data and allow estimating the fine structure constant. Christoph Schiller, PhD Université Libre de Bruxelles, is a physicist and physics popularizer. This entertaining book is for students, teachers and anybody interested in modern research about fundamental physics. Pdf file available free of charge at www.motionmountain.net Christoph Schiller Motion Mountain The Adventure of Physics Volume VI The Strand Model – A Speculation on Unification Edition 30, available as free pdf with films at www.motionmountain.net subject index 481 at Planck scales 77 weak bosons 248 world viscous fluids weak charge 246–248 crystal, nematic 299 tangles -
The Structure Lacuna
Int. J. Mol. Sci. 2012, 13, 9081-9096; doi:10.3390/ijms13079081 OPEN ACCESS International Journal of Molecular Sciences ISSN 1422-0067 www.mdpi.com/journal/ijms Article The Structure Lacuna Jan C.A. Boeyens 1;* and Demetrius C. Levendis 2 1 Unit for Advanced Scholarship, University of Pretoria, Lynnwood Road, Pretoria 0002, South Africa 2 Molecular Sciences Institute, School of Chemistry, University of the Witwatersrand, Jan Smuts Avenue, Johannesburg 0001, South Africa; E-Mail: [email protected] * Author to whom correspondence should be addressed; E-Mail: [email protected]; Tel.: +27-12-420-4528; Fax: +27-12-362-5288. Received: 6 June 2012; in revised form: 10 July 2012 / Accepted: 12 July 2012 / Published: 20 July 2012 Abstract: Molecular symmetry is intimately connected with the classical concept of three-dimensional molecular structure. In a non-classical theory of wave-like interaction in four-dimensional space-time, both of these concepts and traditional quantum mechanics lose their operational meaning, unless suitably modified. A required reformulation should emphasize the importance of four-dimensional effects like spin and the symmetry effects of space-time curvature that could lead to a fundamentally different understanding of molecular symmetry and structure in terms of elementary number theory. Isolated single molecules have no characteristic shape and macro-biomolecules only develop robust three-dimensional structure in hydrophobic response to aqueous cellular media. Keywords: golden ratio; molecular symmetry; spin function 1. Introduction Most quantum-theoretical concepts of chemistry have their origin in spectroscopy. The atomic spectroscopy of Kirchhoff, Bunsen, Fraunhofer and others resulted in the formulation of Balmer’s mysterious formula, the direct stimulus for the development of quantum mechanics. -
Spinor - Wikipedia, the Free Encyclopedia Page 1 of 14
Spinor - Wikipedia, the free encyclopedia Page 1 of 14 Spinor From Wikipedia, the free encyclopedia In mathematics and physics, in particular in the theory of the orthogonal groups, spinors are elements of a complex vector space introduced to expand the notion of spatial vector. They are needed because the full structure of the group of rotations in a given number of dimensions requires some extra number of dimensions to exhibit it. More formally, spinors can be defined as geometrical objects constructed from a given vector space endowed with a quadratic form by means of an algebraic [1] or quantization [2] procedure. A given quadratic form may support several different types of spinors. The ensemble of spinors of a given type is itself a vector space on which the rotation group acts, but for an ambiguity in the sign of the action. The space of spinors thus carries a projective representation of the rotation group. One can remove this sign ambiguity by regarding the space of spinors as a (linear) group representation of the spin group Spin(n). In this alternative point of view, many of the intrinsic and algebraic properties of spinors are more clearly visible, but the connection with the original spatial geometry is more obscure. On the other hand the use of complex number scalars can be kept to a minimum. Spinors in general were discovered by Élie Cartan in 1913. [3] Later, spinors were adopted by quantum mechanics in order to study the properties of the intrinsic angular momentum of the electron and other fermions. Today spinors enjoy a wide range of physics applications. -
How Efficiently Can One Untangle a Double-Twist? Waving Is Believing
How efficiently can one untangle a double-twist? Waving is believing! David Pengelley Daniel Ramras∗ Abstract It has long been known to mathematicians and physicists that while a full rotation in three-dimensional Euclidean space causes tan- gling, two rotations can be untangled. Formally, an untangling is a based nullhomotopy of the double-twist loop in the special orthogo- nal group of rotations. We study a particularly simple, geometrically defined untangling procedure, leading to new conclusions regarding the minimum possible complexity of untanglings. We animate and analyze how our untangling operates on frames in 3{space, and teach readers in a video how to wave the nullhomotopy with their hands. 1 Entanglement, efficiency, and aesthetics When an object receives a full rotational turn, it becomes \entangled" with its environment. This is second nature to anyone who winds up a garden hose. As more turns are applied, we feel intuitively that the entanglement magnifies via increasingly wound strings (visible or invisible) connecting the object to fixed surroundings. However, outlandish as it may seem, three-dimensional space doesn't actually behave like this! Mathematicians and physicists have long known that while a single full turn entangles, two turns can be \un- tangled". For physicists this provides an analogy for understanding electron arXiv:1610.04680v2 [math.GT] 10 Nov 2016 spin [8, p. 28f], [9, 10], [16, Fig. 41.6, p. 1149], and for mathematicians it is a statement about the topology of the rotation group SO(3). Visual demonstrations of untanglings [10, 17, 18, 22] often have physi- cal origins, with names like the \Dirac scissors demonstration" [20, p. -
Visualizing Quaternions Course Notes for SIGGRAPH
Visualizing Quaternions Course Notes for SIGGRAPH ’99 Course Organizer Andrew J. Hanson Computer Science Department Indiana University Bloomington, IN 47405 USA Email: [email protected] Abstract This tutorial focuses on establishing an intuitive visual understanding of the relationship between ordinary 3D rotations and their quaternion representations. We begin building this intuition by showing how quaternion-like properties appear and can be exploited even in 2D space. Quater- nions are then introduced in several alternative representations that do not necessarily require ab- stract mathematical constructs for their visualization. We then proceed to develop visualizations of quaternion applications such as orientation splines, streamlines, and optimal orientation frames. Finally, for the strong-hearted, we briefly discuss the problem of generalizing quaternion concepts to higher dimensions using Clifford algebras. Presenter’s Biography Andrew J. Hanson is a professor of computer science at Indiana University, and has regularly taught courses in computer graphics, computer vision, programming languages, and scientific vi- sualization. He received a BA in chemistry and physics from Harvard College in 1966 and a PhD in theoretical physics from MIT in 1971. Before coming to Indiana University, he did research in the- oretical physics at the Institute for Advanced Study, Stanford, and Berkeley, and then in computer vision at the SRI Artificial Intelligence Center. He has published a variety of technical articles on machine vision, computer graphics, and visualization methods. He has also contributed three articles to the Graphics Gems series dealing with user interfaces for rotations and with techniques of N-dimensional geometry. His current research interests include scientific visualization (with applications in mathematics, astrophysics, and string-model physics), machine vision, computer graphics, perception, collaborative methods in virtual reality, and the design of interactive user interfaces for virtual reality and visualization applications.