Fundamental Nature of the Fine-Structure Constant
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From a GOLDEN RECTANGLE to GOLDEN QUADRILATERALS And
An example of constructive defining: TechSpace From a GOLDEN TechSpace RECTANGLE to GOLDEN QUADRILATERALS and Beyond Part 1 MICHAEL DE VILLIERS here appears to be a persistent belief in mathematical textbooks and mathematics teaching that good practice (mostly; see footnote1) involves first Tproviding students with a concise definition of a concept before examples of the concept and its properties are further explored (mostly deductively, but sometimes experimentally as well). Typically, a definition is first provided as follows: Parallelogram: A parallelogram is a quadrilateral with half • turn symmetry. (Please see endnotes for some comments on this definition.) 1 n The number e = limn 1 + = 2.71828 ... • →∞ ( n) Function: A function f from a set A to a set B is a relation • from A to B that satisfies the following conditions: (1) for each element a in A, there is an element b in B such that <a, b> is in the relation; (2) if <a, b> and <a, c> are in the relation, then b = c. 1It is not being claimed here that all textbooks and teaching practices follow the approach outlined here as there are some school textbooks such as Serra (2008) that seriously attempt to actively involve students in defining and classifying triangles and quadrilaterals themselves. Also in most introductory calculus courses nowadays, for example, some graphical and numerical approaches are used before introducing a formal limit definition of differentiation as a tangent to the curve of a function or for determining its instantaneous rate of change at a particular point. Keywords: constructive defining; golden rectangle; golden rhombus; golden parallelogram 64 At Right Angles | Vol. -
Theoretical Physics
IC/80/166 INTERNATIONAL CENTRE FOR THEORETICAL PHYSICS AW EFFICIENT KORRINGA-KOHN-ROSTOKER METHOD FOR "COMPLEX" LATTICES M. Yussouff and INTERNATIONAL ATOMIC ENERGY R. Zeller AGENCY UNITED NATIONS EDUCATIONAL SCIENTIFIC AND CULTURAL ORGANIZATION 19R0 MIRAMARE-TRIESTE IC/90/166 The well known rapid convergence and precision of the KKR- Green's function method (Korringa 1947, Kohn and Rostocker 1954) International Atomic Energy Agency have made it useful for the calculation of the electronic struc- and United Rations Educational Scientific and Cultural Organization ture of perfect as well as disordered solids (Ham and Segall 1961, IHTEBSATIOHAL CENTRE FOR THEORETICAL PHYSICS Ehrenrelch and Schwartz 1976). Although extensive calculations of this kind exist for cubic crystals (Moruzzi, Janak and Williams 1978), there are so far very few calculations for the equally important class of hexagonal close packed solids. This is due to the computational efforts involved in evaluating the KKR matrix AH EFFICIENT KORRIHGA-KOHH-ROSTOKER METHOD FOR "COMPLEX" LATTICES • elements ATT,{k,E) using the conventional KKR for 'complex' lattices, i.e. crystals with several atoms per unit cell- Some simplifications can be achieved (Bhokare and Yussouff 1972, 1974) for k" vectors International Centre for Theoretical Physics, Trieste, Italy, in symmetry directions but the renewed interest in simplifying the and computations (Segall and Yang 19 80) has arisen in connection with self-consistent calcualtions. Here we describe an efficient modi- R. Zeller Institut fur FeBtkorperforschung der Kernforschungsanlage, fication of the KKR method which is particularly useful for 'complex1 D-5170 Jiilieh, Federal Republic of Germany. lattices. ABSTRACT In our approach, the transformed KKR matrix elements are calcu- We present a modification of the exact KKR-band structure method lated directly using reciprocal space summation. -
An Amazing Prime Heuristic.Pdf
This document has been moved to https://arxiv.org/abs/2103.04483 Please use that version instead. AN AMAZING PRIME HEURISTIC CHRIS K. CALDWELL 1. Introduction The record for the largest known twin prime is constantly changing. For example, in October of 2000, David Underbakke found the record primes: 83475759 264955 1: · The very next day Giovanni La Barbera found the new record primes: 1693965 266443 1: · The fact that the size of these records are close is no coincidence! Before we seek a record like this, we usually try to estimate how long the search might take, and use this information to determine our search parameters. To do this we need to know how common twin primes are. It has been conjectured that the number of twin primes less than or equal to N is asymptotic to N dx 2C2N 2C2 2 2 Z2 (log x) ∼ (log N) where C2, called the twin prime constant, is approximately 0:6601618. Using this we can estimate how many numbers we will need to try before we find a prime. In the case of Underbakke and La Barbera, they were both using the same sieving software (NewPGen1 by Paul Jobling) and the same primality proving software (Proth.exe2 by Yves Gallot) on similar hardware{so of course they choose similar ranges to search. But where does this conjecture come from? In this chapter we will discuss a general method to form conjectures similar to the twin prime conjecture above. We will then apply it to a number of different forms of primes such as Sophie Germain primes, primes in arithmetic progressions, primorial primes and even the Goldbach conjecture. -
[Math.AG] 1 Nov 2005 Where Uoopimgop Hscntuto Ensahlmrhcperio Holomorphic a Defines Construction This Group
A COMPACTIFICATION OF M3 VIA K3 SURFACES MICHELA ARTEBANI Abstract. S. Kond¯odefined a birational period map from the moduli space of genus three curves to a moduli space of degree four polarized K3 surfaces. In this paper we extend the period map to a surjective morphism on a suitable compactification of M3 and describe its geometry. Introduction 14 Let V =| OP2 (4) |=∼ P be the space of plane quartics and V0 be the open subvariety of smooth curves. The degree four cyclic cover of the plane branched along a curve C ∈ V0 is a K3 surface equipped with an order four non-symplectic automorphism group. This construction defines a holomorphic period map: P0 : V0 −→ M, where V0 is the geometric quotient of V0 by the action of P GL(3) and M is a moduli space of polarized K3 surfaces. In [15] S. Kond¯oshows that P0 gives an isomorphism between V0 and the com- plement of two irreducible divisors Dn, Dh in M. Moreover, he proves that the generic points in Dn and Dh correspond to plane quartics with a node and to smooth hyperelliptic genus three curves respectively. The moduli space M is an arithmetic quotient of a six dimensional complex ball, hence a natural compactification is given by the Baily-Borel compactification M∗ (see [1]). On the other hand, geometric invariant theory provides a compact pro- jective variety V containing V0 as a dense subset, given by the categorical quotient of the semistable locus in V for the natural action of P GL(3). In this paper we prove that the map P0 can be extended to a holomorphic surjective map P : V −→M∗ on the blowing-up V of V in the point v0 corresponding to the orbit of double arXiv:math/0511031v1 [math.AG] 1 Nov 2005 e conics. -
|||GET||| Can the Laws of Physics Be Unified? 1St Edition
CAN THE LAWS OF PHYSICS BE UNIFIED? 1ST EDITION DOWNLOAD FREE Paul Langacker | 9781400885503 | | | | | Can the Laws of Physics be Unified? Answer Key. In American physicist Sheldon Glashow proposed that the weak nuclear forceelectricity and magnetism could arise Can the Laws of Physics Be Unified? 1st edition a partially unified electroweak theory. Law II: The alteration of motion is ever proportional to the motive force impress'd; and is made in the direction of the right line in which that force is impress'd. In the s Mendel Sachs proposed a generally covariant field theory that did not require recourse to renormalisation or perturbation theory. Discoveries are made; models, theories, and laws are formulated; and the beauty of the physical universe is made more sublime for the insights gained. Download as PDF Printable version. Lots of equations, but not much detail explaining exactly what they mean, for that some background is needed. I find that literally inconceivable. These laws are Can the Laws of Physics Be Unified? 1st edition systematically to topics such as phase equilibria, chemical reactions, external forces, fluid-fluid surfaces and interfaces, and anisotropic crystal-fluid interfaces. Cohen and A. The physical universe is enormously complex in its detail. One of her daughters also won a Nobel Prize. Archived from the original PDF on 31 March Thank you for posting a review! And, whereas a law is a postulate that forms the foundation of the scientific method, a theory is the end result of that process. I know of none whatsoever. Paul Langacker is senior scientist at Princeton University, visitor at the Institute for Advanced Study in Princeton, and professor emeritus of physics at the University of Pennsylvania. -
Shadow of a Cubic Surface
Faculteit B`etawetenschappen Shadow of a cubic surface Bachelor Thesis Rein Janssen Groesbeek Wiskunde en Natuurkunde Supervisors: Dr. Martijn Kool Departement Wiskunde Dr. Thomas Grimm ITF June 2020 Abstract 3 For a smooth cubic surface S in P we can cast a shadow from a point P 2 S that does not lie on one of the 27 lines of S onto a hyperplane H. The closure of this shadow is a smooth quartic curve. Conversely, from every smooth quartic curve we can reconstruct a smooth cubic surface whose closure of the shadow is this quartic curve. We will also present an algorithm to reconstruct the cubic surface from the bitangents of a quartic curve. The 27 lines of S together with the tangent space TP S at P are in correspondence with the 28 bitangents or hyperflexes of the smooth quartic shadow curve. Then a short discussion on F-theory is given to relate this geometry to physics. Acknowledgements I would like to thank Martijn Kool for suggesting the topic of the shadow of a cubic surface to me and for the discussions on this topic. Also I would like to thank Thomas Grimm for the suggestions on the applications in physics of these cubic surfaces. Finally I would like to thank the developers of Singular, Sagemath and PovRay for making their software available for free. i Contents 1 Introduction 1 2 The shadow of a smooth cubic surface 1 2.1 Projection of the first polar . .1 2.2 Reconstructing a cubic from the shadow . .5 3 The 27 lines and the 28 bitangents 9 3.1 Theorem of the apparent boundary . -
Combination of Cubic and Quartic Plane Curve
IOSR Journal of Mathematics (IOSR-JM) e-ISSN: 2278-5728,p-ISSN: 2319-765X, Volume 6, Issue 2 (Mar. - Apr. 2013), PP 43-53 www.iosrjournals.org Combination of Cubic and Quartic Plane Curve C.Dayanithi Research Scholar, Cmj University, Megalaya Abstract The set of complex eigenvalues of unistochastic matrices of order three forms a deltoid. A cross-section of the set of unistochastic matrices of order three forms a deltoid. The set of possible traces of unitary matrices belonging to the group SU(3) forms a deltoid. The intersection of two deltoids parametrizes a family of Complex Hadamard matrices of order six. The set of all Simson lines of given triangle, form an envelope in the shape of a deltoid. This is known as the Steiner deltoid or Steiner's hypocycloid after Jakob Steiner who described the shape and symmetry of the curve in 1856. The envelope of the area bisectors of a triangle is a deltoid (in the broader sense defined above) with vertices at the midpoints of the medians. The sides of the deltoid are arcs of hyperbolas that are asymptotic to the triangle's sides. I. Introduction Various combinations of coefficients in the above equation give rise to various important families of curves as listed below. 1. Bicorn curve 2. Klein quartic 3. Bullet-nose curve 4. Lemniscate of Bernoulli 5. Cartesian oval 6. Lemniscate of Gerono 7. Cassini oval 8. Lüroth quartic 9. Deltoid curve 10. Spiric section 11. Hippopede 12. Toric section 13. Kampyle of Eudoxus 14. Trott curve II. Bicorn curve In geometry, the bicorn, also known as a cocked hat curve due to its resemblance to a bicorne, is a rational quartic curve defined by the equation It has two cusps and is symmetric about the y-axis. -
Quantum Mechanics from General Relativity : Particle Probability from Interaction Weighting
Annales de la Fondation Louis de Broglie, Volume 24, 1999 25 Quantum Mechanics From General Relativity : Particle Probability from Interaction Weighting Mendel Sachs Department of Physics State University of New York at Bualo ABSTRACT. Discussion is given to the conceptual and mathemat- ical change from the probability calculus of quantum mechanics to a weighting formalism, when the paradigm change takes place from linear quantum mechanics to the nonlinear, holistic eld theory that accompanies general relativity, as a fundamental theory of matter. This is a change from a nondeterministic, linear theory of an open system of ‘particles’ to a deterministic, nonlinear, holistic eld the- ory of the matter of a closed system. RESUM E. On discute le changement conceptuel et mathematique qui fait passer du calcul des probabilites de la mecanique quantique a un formalisme de ponderation, quand on eectue le changement de paradigme substituantalam ecanique quantique lineairelatheorie de champ holistique non lineaire qui est associee alatheorie de la relativitegenerale, prise comme theorie fondamentale de la matiere. Ce changement mene d’une theorie non deterministe et lineaire decrivant un systeme ouvert de ‘particules’ a une theorie de champ holistique, deterministe et non lineaire, de la matiere constituant un systeme ferme. 1. Introduction. In my view, one of the three most important experimental discov- eries of 20th century physics was the wave nature of matter. [The other two were 1) blackbody radiation and 2) the bending of a beam of s- tarlight as it propagates past the vicinity of the sun]. The wave nature of matter was predicted in the pioneering theoretical studies of L. -
Fundamental Nature of the Fine-Structure Constant Michael Sherbon
Fundamental Nature of the Fine-Structure Constant Michael Sherbon To cite this version: Michael Sherbon. Fundamental Nature of the Fine-Structure Constant. International Journal of Physical Research , Science Publishing Corporation 2014, 2 (1), pp.1-9. 10.14419/ijpr.v2i1.1817. hal-01304522 HAL Id: hal-01304522 https://hal.archives-ouvertes.fr/hal-01304522 Submitted on 19 Apr 2016 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Distributed under a Creative Commons Attribution| 4.0 International License Fundamental Nature of the Fine-Structure Constant Michael A. Sherbon Case Western Reserve University Alumnus E-mail: michael:sherbon@case:edu January 17, 2014 Abstract Arnold Sommerfeld introduced the fine-structure constant that determines the strength of the electromagnetic interaction. Following Sommerfeld, Wolfgang Pauli left several clues to calculating the fine-structure constant with his research on Johannes Kepler’s view of nature and Pythagorean geometry. The Laplace limit of Kepler’s equation in classical mechanics, the Bohr-Sommerfeld model of the hydrogen atom and Julian Schwinger’s research enable a calculation of the electron magnetic moment anomaly. Considerations of fundamental lengths such as the charge radius of the proton and mass ratios suggest some further foundational interpretations of quantum electrodynamics. -
Tropical Curves
Tropical Curves Nathan Pflueger 24 February 2011 Abstract A tropical curve is a graph with specified edge lengths, some of which may be infinite. Various facts and attributes about algebraic curves have analogs for tropical curves. In this article, we focus on divisors and linear series, and prove the Riemann-Roch formula for divisors on tropical curves. We describe two ways in which algebraic curves may be transformed into tropical curves: by aboemas and by specialization on arithmetic surfaces. We discuss how the study of linear series on tropical curves can be used to obtain results about linear series on algebraic curves, and summarize several recent applications. Contents 1 Introduction 2 2 From curves to graphs 3 2.1 Amoebas of plane curves . .3 2.2 Curves over the field of Puiseux series . .4 2.3 Specialization . .5 3 Metric graphs and tropical curves 6 4 Divisors and linear equivalence on tropical curves 9 4.1 The Riemann-Roch criterion . 12 4.2 Tropical Riemann-Roch . 14 5 Tropical plane curves 17 5.1 Tropical algebra and tropical projective space . 17 5.2 Tropical curves in R2 ................................... 18 5.3 Calculation of the genus . 23 5.4 Stable intersection and the tropical B´ezouttheorem . 24 5.5 Classical B´ezoutfrom tropical B´ezout . 29 5.6 Enumerative geometry of tropical plane curves . 31 6 Tropical curves via specialization 32 6.1 The specialization map and specialization lemma . 32 6.2 The canonical divisor of a graph is canonical . 34 6.3 A tropical proof of the Brill-Noether theorem . 34 1 1 Introduction The origins of tropical geometry lie in the study of tropical algebra, whose basic object is the set R [ {−∞} equipped with the operations x ⊕ y = max(x; y) and x ⊗ y = x + y. -
Foundations of Algebraic Geometry Class 41
FOUNDATIONS OF ALGEBRAIC GEOMETRY CLASS 41 RAVI VAKIL CONTENTS 1. Normalization 1 2. Extending maps to projective schemes over smooth codimension one points: the “clear denominators” theorem 5 Welcome back! Let's now use what we have developed to study something explicit — curves. Our motivating question is a loose one: what are the curves, by which I mean nonsingular irreducible separated curves, finite type over a field k? In other words, we'll be dealing with geometry, although possibly over a non-algebraically closed field. Here is an explicit question: are all curves (say reduced, even non-singular, finite type over given k) isomorphic? Obviously not: some are affine, and some (such as P1) are not. So to simplify things — and we'll further motivate this simplification in Class 42 — are all projective curves isomorphic? Perhaps all nonsingular projective curves are isomorphic to P1? Once again the answer is no, but the proof is a bit subtle: we've defined an invariant, the genus, and shown that P1 has genus 0, and that there exist nonsingular projective curves of non-zero genus. Are all (nonsingular) genus 0 curves isomorphic to P1? We know there exist nonsingular genus 1 curves (plane cubics) — is there only one? If not, “how many” are there? In order to discuss interesting questions like these, we'll develop some theory. We first show a useful result that will help us focus our attention on the projective case. 1. NORMALIZATION I now want to tell you how to normalize a reduced Noetherian scheme, which is roughly how best to turn a scheme into a normal scheme. -
Prime Numbers in Logarithmic Intervals
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by PORTO Publications Open Repository TOrino Prime numbers in logarithmic intervals Danilo Bazzanella Dipartimento di Matematica, Politecnico di Torino, Italy [email protected] Alessandro Languasco Dipartimento di Matematica Pura e Applicata Universit`adi Padova , Italy [email protected] Alessandro Zaccagnini Dipartimento di Matematica Universit`adi Parma, Italy [email protected] First published in Transactions of the American Mathematical Society 362 (2010), no. 5, 2667-2684 published by the American Mathematical Society DOI: 10.1090/S0002-9947-09-05009-0 The original publication is available at http://www.ams.org/ 1 TRANSACTIONS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 362, Number 5, May 2010, Pages 2667–2684 S0002-9947(09)05009-0 Article electronically published on November 17, 2009 PRIME NUMBERS IN LOGARITHMIC INTERVALS DANILO BAZZANELLA, ALESSANDRO LANGUASCO, AND ALESSANDRO ZACCAGNINI Abstract. Let X be a large parameter. We will first give a new estimate for the integral moments of primes in short intervals of the type (p, p + h], where p X is a prime number and h = o(X). Then we will apply this to prove that ≤ for every λ>1/2thereexistsapositiveproportionofprimesp X such that ≤ the interval (p, p+λ log X]containsatleastaprimenumber.Asaconsequence we improve Cheer and Goldston’s result on the size of real numbers λ> 1 with the property that there is a positive proportion of integers m X ≤ such that the interval