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Degenerate Eigenvalue Problem 32.1 Degenerate Perturbation
Physics 342 Lecture 32 Degenerate Eigenvalue Problem Lecture 32 Physics 342 Quantum Mechanics I Wednesday, April 23rd, 2008 We have the matrix form of the first order perturbative result from last time. This carries over pretty directly to the Schr¨odingerequation, with only minimal replacement (the inner product and finite vector space change, but notationally, the results are identical). Because there are a variety of quantum mechanical systems with degenerate spectra (like the Hydrogen 2 eigenstates, each En has n associated eigenstates) and we want to be able to predict the energy shift associated with perturbations in these systems, we can copy our arguments for matrices to cover matrices with more than one eigenvector per eigenvalue. The punch line of that program is that we can use the non-degenerate perturbed energies, provided we start with the \correct" degenerate linear combinations. 32.1 Degenerate Perturbation N×N Going back to our symmetric matrix example, we have A IR , and 2 again, a set of eigenvectors and eigenvalues: A xi = λi xi. This time, suppose that the eigenvalue λi has a set of M associated eigenvectors { that is, suppose a set of eigenvectors yj satisfy: A yj = λi yj j = 1 M (32.1) −! 1 of 9 32.1. DEGENERATE PERTURBATION Lecture 32 (so this represents M separate equations) that are themselves orthonormal1. Clearly, any linear combination of these vectors is also an eigenvector: M M X X A βk yk = λi βk yk: (32.2) k=1 k=1 M PM Define the general combination of yi to be z βk yk, also an f gi=1 ≡ k=1 eigenvector of A with eigenvalue λi. -
How Should the College Teach Analytic Geometry?*
1906.] THE TEACHING OF ANALYTIC GEOMETRY. 493 HOW SHOULD THE COLLEGE TEACH ANALYTIC GEOMETRY?* BY PROFESSOR HENRY S. WHITE. IN most American colleges, analytic geometry is an elective study. This fact, and the underlying causes of this fact, explain the lack of uniformity in content or method of teaching this subject in different institutions. Of many widely diver gent types of courses offered, a few are likely to survive, each because it is best fitted for some one purpose. It is here my purpose to advocate for the college of liberal arts a course that shall draw more largely from projective geometry than do most of our recent college text-books. This involves a restriction of the tendency, now quite prevalent, to devote much attention at the outset to miscellaneous graphs of purely statistical nature or of physical significance. As to the subject matter used in a first semester, one may formulate the question : Shall we teach in one semester a few facts about a wide variety of curves, or a wide variety of propositions about conies ? Of these alternatives the latter is to be preferred, for the educational value of a subject is found less in its extension than in its intension ; less in the multiplicity of its parts than in their unification through a few fundamental or climactic princi ples. Some teachers advocate the study of a wider variety of curves, either for the sake of correlation wTith physical sci ences, or in order to emphasize what they term the analytic method. As to the first, there is a very evident danger of dis sipating the student's energy ; while to the second it may be replied that there is no one general method which can be taught, but many particular and ingenious methods for special problems, whose resemblances may be understood only when the problems have been mastered. -
Greece Part 3
Greece Chapters 6 and 7: Archimedes and Apollonius SOME ANCIENT GREEK DISTINCTIONS Arithmetic Versus Logistic • Arithmetic referred to what we now call number theory –the study of properties of whole numbers, divisibility, primality, and such characteristics as perfect, amicable, abundant, and so forth. This use of the word lives on in the term higher arithmetic. • Logistic referred to what we now call arithmetic, that is, computation with whole numbers. Number Versus Magnitude • Numbers are discrete, cannot be broken down indefinitely because you eventually came to a “1.” In this sense, any two numbers are commensurable because they could both be measured with a 1, if nothing bigger worked. • Magnitudes are continuous, and can be broken down indefinitely. You can always bisect a line segment, for example. Thus two magnitudes didn’t necessarily have to be commensurable (although of course they could be.) Analysis Versus Synthesis • Synthesis refers to putting parts together to obtain a whole. • It is also used to describe the process of reasoning from the general to the particular, as in putting together axioms and theorems to prove a particular proposition. • Proofs of the kind Euclid wrote are referred to as synthetic. Analysis Versus Synthesis • Analysis refers to taking things apart to see how they work, or so you can understand them. • It is also used to describe reasoning from the particular to the general, as in studying a particular problem to come up with a solution. • This is one general meaning of analysis: a way of solving problems, of finding the answers. Analysis Versus Synthesis • A second meaning for analysis is specific to logic and theorem proving: beginning with what you wish to prove, and reasoning from that point in hopes you can arrive at the hypotheses, and then reversing the logical steps. -
DEGENERACY CURVES, GAPS, and DIABOLICAL POINTS in the SPECTRA of NEUMANN PARALLELOGRAMS P Overfelt
DEGENERACY CURVES, GAPS, AND DIABOLICAL POINTS IN THE SPECTRA OF NEUMANN PARALLELOGRAMS P Overfelt To cite this version: P Overfelt. DEGENERACY CURVES, GAPS, AND DIABOLICAL POINTS IN THE SPECTRA OF NEUMANN PARALLELOGRAMS. 2020. hal-03017250 HAL Id: hal-03017250 https://hal.archives-ouvertes.fr/hal-03017250 Preprint submitted on 20 Nov 2020 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. DEGENERACY CURVES, GAPS, AND DIABOLICAL POINTS IN THE SPECTRA OF NEUMANN PARALLELOGRAMS P. L. OVERFELT Abstract. In this paper we consider the problem of solving the Helmholtz equation over the space of all parallelograms subject to Neumann boundary conditions and determining the degeneracies occurring in their spectra upon changing the two parameters, angle and side ratio. This problem is solved numerically using the finite element method (FEM). Specifically for the lowest eleven normalized eigenvalue levels of the family of Neumann parallelograms, the intersection of two (or more) adjacent eigen- value level surfaces occurs in one of three ways: either as an isolated point associated with the special geometries, i.e., the rectangle, the square, or the rhombus, as part of a degeneracy curve which appears to contain an infinite number of points, or as a diabolical point in the Neumann parallelogram spec- trum. -
A Singular One-Dimensional Bound State Problem and Its Degeneracies
A Singular One-Dimensional Bound State Problem and its Degeneracies Fatih Erman1, Manuel Gadella2, Se¸cil Tunalı3, Haydar Uncu4 1 Department of Mathematics, Izmir˙ Institute of Technology, Urla, 35430, Izmir,˙ Turkey 2 Departamento de F´ısica Te´orica, At´omica y Optica´ and IMUVA. Universidad de Valladolid, Campus Miguel Delibes, Paseo Bel´en 7, 47011, Valladolid, Spain 3 Department of Mathematics, Istanbul˙ Bilgi University, Dolapdere Campus 34440 Beyo˘glu, Istanbul,˙ Turkey 4 Department of Physics, Adnan Menderes University, 09100, Aydın, Turkey E-mail: [email protected], [email protected], [email protected], [email protected] October 20, 2017 Abstract We give a brief exposition of the formulation of the bound state problem for the one-dimensional system of N attractive Dirac delta potentials, as an N N matrix eigenvalue problem (ΦA = ωA). The main aim of this paper is to illustrate that the non-degeneracy× theorem in one dimension breaks down for the equidistantly distributed Dirac delta potential, where the matrix Φ becomes a special form of the circulant matrix. We then give elementary proof that the ground state is always non-degenerate and the associated wave function may be chosen to be positive by using the Perron-Frobenius theorem. We also prove that removing a single center from the system of N delta centers shifts all the bound state energy levels upward as a simple consequence of the Cauchy interlacing theorem. Keywords. Point interactions, Dirac delta potentials, bound states. 1 Introduction Dirac delta potentials or point interactions, or sometimes called contact potentials are one of the exactly solvable classes of idealized potentials, and are used as a pedagogical tool to illustrate various physically important phenomena, where the de Broglie wavelength of the particle is much larger than the range of the interaction. -
On the Constructibility of the Axes of an Ellipsoid
ON THE CONSTRUCTIBILITY OF THE AXES OF AN ELLIPSOID. THE CONSTRUCTION OF CHASLES IN PRACTICE AKOS´ G.HORVATH´ AND ISTVAN´ PROK Dedicated to the memory of the teaching of Descriptive Geometry in BME Faculty of Mechanical Engineering Abstract. In this paper we discuss Chasles’s construction on ellipsoid to draw the semi-axes from a complete system of conjugate diameters. We prove that there is such situation when the construction is not planar (the needed points cannot be constructed with compasses and ruler) and give some others in which the construction is planar. 1. Introduction Who interested in conics know the construction of Rytz, namely a construction which determines the axes of an ellipse from a pair of conjugate diameters. Contrary to this very few mathematicians know that in the first half of the nineteens century Chasles (see in [1]) gave a construction in space to the analogous problem. The only reference which we found in English is also in an old book written by Salmon (see in [6]) on the analytic geometry of the three-dimensional space. In [2] the author extracted this analytic method to prove some results on the quadric of n-dimensional space. However, in practice this construction cannot be done using compasses and ruler only as we will see in present paper (Statement 4). On the other hand those steps of the construction which are planar constructions we can draw by descriptive geometry (see the figures in this article). 2. Basic properties The proof of the statements of this section can be found in [2]. -
Attoclock Ultrafast Timing of Inversive Chord-Contact Dynamics
Attoclock Ultrafast Timing of Inversive Chord-Contact Dynamics - A Spectroscopic FFT-Glimpse onto Harmonic Analysis of Gravitational Waves - Walter J. Schempp Lehrstuhl f¨urMathematik I Universit¨atSiegen 57068 Siegen, Germany [email protected] According to Bohr's model of the hydrogen atom, it takes about 150 as for an electron in the ground state to orbit around the atomic core. Therefore, the attosecond (1 as = 10−18s) is the typical time scale for Bloch wave packet dynamics operating at the interface of quantum field theory and relativity theory. Attoclock spectroscopy is mathematically dominated by the spectral dual pair of spin groups with the commuting action of the stabilized symplectic spinor quantization (Mp(2; R); PSO(1; 3; R)) In the context of the Mp(2; R) × PSO(1; 3; R) module structure of the complex Schwartz space 2 2 ∼ S(R ⊕ R ) = S(C ⊕ C) of quantum field theory, the metaplectic Lie group Mp(2; R) is the ∼ two-sheeted covering group Sp(2f ; R) of the symplectic group Sp(2; R) = SL(2; R), where the ∼ special linear group SL(2; R) is a simple Lie group, and the two-cycle rotation group SO(2f ; R) = U(1e ; C) is a maximal compact subgroup of Mp(2; R). The two-fold hyperbolically, respectively ∼ elliptically ruled conformal Lie group SU(1; 1; C) is conjugate to SL(2; R) = Spin(1; 2; R) in the ∼ ∼ complexification SL(2; C) = Spin(1; 3; R); the projective Lorentz-M¨obiusgroup PSO(1; 3; R) = ∼ PSL(2; C) = SL(2; C)=(Z2:id) represents a semi-simple Lie group which is isomorphic to the "+ four-dimensional proper orthochroneous Lorentz group L4 of relativity theory. -
A Survey of the Development of Geometry up to 1870
A Survey of the Development of Geometry up to 1870∗ Eldar Straume Department of mathematical sciences Norwegian University of Science and Technology (NTNU) N-9471 Trondheim, Norway September 4, 2014 Abstract This is an expository treatise on the development of the classical ge- ometries, starting from the origins of Euclidean geometry a few centuries BC up to around 1870. At this time classical differential geometry came to an end, and the Riemannian geometric approach started to be developed. Moreover, the discovery of non-Euclidean geometry, about 40 years earlier, had just been demonstrated to be a ”true” geometry on the same footing as Euclidean geometry. These were radically new ideas, but henceforth the importance of the topic became gradually realized. As a consequence, the conventional attitude to the basic geometric questions, including the possible geometric structure of the physical space, was challenged, and foundational problems became an important issue during the following decades. Such a basic understanding of the status of geometry around 1870 enables one to study the geometric works of Sophus Lie and Felix Klein at the beginning of their career in the appropriate historical perspective. arXiv:1409.1140v1 [math.HO] 3 Sep 2014 Contents 1 Euclideangeometry,thesourceofallgeometries 3 1.1 Earlygeometryandtheroleoftherealnumbers . 4 1.1.1 Geometric algebra, constructivism, and the real numbers 7 1.1.2 Thedownfalloftheancientgeometry . 8 ∗This monograph was written up in 2008-2009, as a preparation to the further study of the early geometrical works of Sophus Lie and Felix Klein at the beginning of their career around 1870. The author apologizes for possible historiographic shortcomings, errors, and perhaps lack of updated information on certain topics from the history of mathematics. -
The Project Gutenberg Ebook #43006: Space–Time–Matter
The Project Gutenberg EBook of Space--Time--Matter, by Hermann Weyl This eBook is for the use of anyone anywhere at no cost and with almost no restrictions whatsoever. You may copy it, give it away or re-use it under the terms of the Project Gutenberg License included with this eBook or online at www.gutenberg.org Title: Space--Time--Matter Author: Hermann Weyl Translator: Henry L. Brose Release Date: June 21, 2013 [EBook #43006] Language: English Character set encoding: ISO-8859-1 *** START OF THIS PROJECT GUTENBERG EBOOK SPACE--TIME--MATTER *** Produced by Andrew D. Hwang, using scanned images and OCR text generously provided by the University of Toronto Gerstein Library through the Internet Archive. transcriber’s note The camera-quality files for this public-domain ebook may be downloaded gratis at www.gutenberg.org/ebooks/43006. This ebook was produced using scanned images and OCR text generously provided by the University of Toronto Gerstein Library through the Internet Archive. Typographical corrections, uniformization of punctuation, and minor presentational changes have been effected without comment. This PDF file is optimized for screen viewing, but may be recompiled for printing. Please consult the preamble of the LATEX source file for instructions and other particulars. SPACE—TIME—MATTER BY HERMANN WEYL TRANSLATED FROM THE GERMAN BY HENRY L. BROSE WITH FIFTEEN DIAGRAMS METHUEN & CO. LTD. 36 ESSEX STREET W.C. LONDON First Published in 1922 FROM THE AUTHOR’S PREFACE TO THE FIRST EDITION Einstein’s Theory of Relativity has advanced our ideas of the structure of the cosmos a step further. -
Circles Associated to Pairs of Conjugate Diameters Paris Pamfilos
INTERNATIONAL JOURNAL OF GEOMETRY Vol. 7 (2018), No. 1, 21 - 36 CIRCLES ASSOCIATED TO PAIRS OF CONJUGATE DIAMETERS PARIS PAMFILOS Abstract. A pair of conjugate diameters of a non-circular ellipse or a hyperbola defines a pair of circles, the points of which are naturally related to the points of the conic of reference by a couple of projective transformations. We prove the existence of these circles and corresponding transformations, as well as some of their fundamental properties. 1Thetwocircles Consider an ellipse κ and a fixed pair of conjugate diameters of it {OS, OS}.Letthe varying tangent tP at P intersect the diameters at the points {T,T }. Joining these with the focal points, we obtain the line intersections {U =(FT,FT ),U =(FT,FT )}.The T τ C S P U F' tP F O U' S' τ' T' κ C' Figure 1: Circles generated by a pair of conjugate diameters discussion in this article is about the geometric loci of these two points, as P varies on the ellipse (conic), proven to be two circles {τ,τ} (See Figure 1). We examine also some of the fundamental geometric properties of these circles. The properties dealt with are about genuine central conics, which are not circles. Below we confine the discussion mainly to the case of hyperbolas, in order to encompass also some special properties related to asymptotes and the conjugate hyperbola of κ. Keywords and phrases: Conic, Hyperbola, Ellipse, Conjugate Diameters (2010)Mathematics Subject Classification: 51N15, 51N20, 53A04, 97G40 Received: 9.11.2017. In revised form: 18.01.2018. -
Triangle-Free Penny Graphs: Degeneracy, Choosability, and Edge Count
Triangle-Free Penny Graphs: Degeneracy, Choosability, and Edge Count David Eppstein 25th International Symposium on Graph Drawing & Network Visualization Boston, Massachusetts, September 2017 Circle packing theorem Contacts of interior-disjoint disks in the plane form a planar graph All planar graphs can be represented this way Unique (up to M¨obius)for triangulated graphs [Koebe 1936; Andreev 1970; Thurston 2002] Balanced circle packing Some planar graphs may require exponentially-different radii a b c d But polynomial radii are e f g h i j k possible for: l m n o I Trees p I Outerpaths I Cactus graphs a I Bounded tree-depth b c d [Alam et al. 2015] j e g h i f m k l p n o Perfect balance Circle packings with all radii equal represent penny graphs [Harborth 1974; Erd}os1987] Penny graphs as proximity graphs Given any finite set of points in the plane Draw an edge between each closest pair of points (Pennies: circles centered at the given points with radius = half the minimum distance) So penny graphs may also be called closest-pair graphs or minimum-distance graphs Penny graphs as optimal graph drawings Penny graphs are exactly graphs that can be drawn I With no crossings I All edges equal length I Angular resolution ≥ π=3 Properties of penny graphs 3-degenerate (convex hull vertices have degree ≤ 3) ) easy proof of 4-color theorem; 4-list-colorable [Hartsfield and Ringel 2003] p Number of edges at most 3n − 12n − 3 Maximized by packing into a hexagon [Harborth 1974; Kupitz 1994] NP-hard to recognize, even for trees [Bowen et al. -
1 CHAPTER 2 CONIC SECTIONS 2.1 Introduction a Particle Moving Under the Influence of an Inverse Square Force Moves in an Orbit T
1 CHAPTER 2 CONIC SECTIONS 2.1 Introduction A particle moving under the influence of an inverse square force moves in an orbit that is a conic section; that is to say an ellipse, a parabola or a hyperbola. We shall prove this from dynamical principles in a later chapter. In this chapter we review the geometry of the conic sections. We start off, however, with a brief review (eight equation-packed pages) of the geometry of the straight line. 2.2 The Straight Line It might be thought that there is rather a limited amount that could be written about the geometry of a straight line. We can manage a few equations here, however, (there are 35 in this section on the Straight Line) and shall return for more on the subject in Chapter 4. Most readers will be familiar with the equation y = mx + c 2.2.1 for a straight line. The slope (or gradient) of the line, which is the tangent of the angle that it makes with the x-axis, is m, and the intercept on the y-axis is c. There are various other forms that may be of use, such as x y +=1 2.2.2 x00y yy− 1 yy21− = 2.2.3 xx− 1 xx21− which can also be written x y 1 x1 y1 1 = 0 2.2.4 x2 y2 1 x cos θ + y sin θ = p 2.2.5 2 The four forms are illustrated in figure II.1. y y slope = m y 0 c x x x0 2.2.1 2.2.2 y y • (x2 , y2 ) • ( x1 , y1 ) p x α x 2.2.3 or 4 2.2.5 FIGURE II.1 A straight line can also be written in the form Ax + By + C = 0.