Geometric Description of Scattering Amplitudes: Exploring The

Total Page:16

File Type:pdf, Size:1020Kb

Geometric Description of Scattering Amplitudes: Exploring The Geometric Description of Scattering Amplitudes Exploring the Amplituhedron Andrea Orta M¨unchen2017 Geometric Description of Scattering Amplitudes Exploring the Amplituhedron Andrea Orta Dissertation an der Fakult¨atf¨urPhysik der Ludwig{Maximilians{Universit¨at M¨unchen vorgelegt von Andrea Orta aus Torino, Italien M¨unchen, den 30. Oktober 2017 Erstgutachterin: Prof. Dr. Livia Ferro Zweitgutachter: Prof. Dr. Dieter L¨ust Tag der m¨undlichen Pr¨ufung:15. Dezember 2017 Contents Zusammenfassung xi Summary xiii Acknowledgements xv 0 Introduction 1 1 Scattering amplitudes in massless quantum field theories 9 1.1 General framework . .9 1.2 Large-N limit and colour decomposition . 14 1.2.1 Properties of tree-level colour-ordered amplitudes . 16 1.3 N = 4 super Yang{Mills . 19 1.3.1 The superspace formalism . 22 2 On-shell methods for N = 4 SYM theory and its symmetries 25 2.1 Spinor-helicity variables . 25 2.2 Symmetries of tree-level superamplitudes and the Yangian . 31 2.2.1 Superconformal symmetry . 31 2.2.2 Dual superconformal symmetry . 33 2.2.3 Yangian symmetry . 36 2.3 Twistor variables . 38 2.3.1 Spacetime supertwistors . 38 2.3.2 Momentum supertwistors . 39 2.3.3 Yangian generators in supertwistor formulation . 42 2.4 BCFW recursion relations . 43 2.5 Grassmannian formulation of scattering amplitudes . 54 viii CONTENTS 2.5.1 Geometric interpretation of momentum conservation . 56 2.5.2 Grassmannian integrals . 58 2.5.3 On-shell diagrams . 63 3 The Amplituhedron proposal 79 3.1 Positive geometry in arbitrary dimensions . 80 3.2 Tree amplituhedron and scattering amplitudes . 85 3.3 Loop-level amplituhedron . 91 3.4 An i-prescription for volume functions . 94 3.4.1 A mathematical prelude: multivariate residues . 94 3.4.2 NMHV amplitudes . 96 3.4.3 N2MHV amplitudes . 105 4 Volume of the dual tree-level amplituhedron 107 4.1 Symmetries of the volume function and the Capelli differential equations . 108 4.2 Solution for the k = 1 case . 110 4.3 Applying the master formula . 114 4.3.1 Volume in the m = 2 case . 114 4.3.2 Volume in the m = 4 case . 117 4.4 Deformations and higher-k amplituhedron volumes . 120 5 Yangian symmetry for the tree-level amplituhedron 123 5.1 The Heisenberg isotropic spin chain and the algebraic Bethe ansatz . 124 5.1.1 Introduction . 124 5.1.2 Lax operators, R-matrices, monodromy and transfer matrix . 128 5.1.3 The ansatz and the Bethe equations . 130 5.2 Construction of amplituhedron volume functions . 133 5.2.1 From scattering amplitudes to the amplituhedron . 134 5.2.2 On-shell diagrammatics . 136 5.3 Spin chain picture for the amplituhedron volume . 139 5.3.1 Proof of the monodromy relation . 143 5.3.2 Yangian invariance for the amplituhedron volume . 144 6 Summary and outlook 147 Contents ix A More on the i-prescription 151 A.1 Even distribution of poles: a proof . 151 A.2 The five-point N2MHV volume function . 154 B Details on the solution of the Heisenberg spin chain 161 B.1 Permutation and shift operators . 162 B.2 UN and HN from the transfer matrix . 163 B.3 On the ansatz and the Bethe equations . 164 C Yangian for the tree amplituhedron 167 C.1 Construction of volume functions . 167 C.2 Seed mutations . 168 C.3 Intertwining relations . 169 C.4 Action of the monodromy matrix on the seed . 170 x Contents Zusammenfassung Die vorliegende Dissertation befasst sich mit einigen der neuesten Entwicklungen im The- mengebiet der Streuamplituden in schwach gekoppelten Eichtheorien. Der traditionelle st¨orungstheoretische Zugang, der Feynman-Diagramme verwendet, hat sich durchgesetzt und großen Erfolg erzielt, jedoch er ist zunehmend ungeeignet geworden, um mit der Komplexit¨atder Pr¨azisionsberechnungen umzugehen, die heutzutage ben¨otigtsind. Neue Techniken, die zusammenfassend als on-shell Methoden bezeichnet werden, sind entwickelt worden, um die Nachteile und Engp¨assedieses Zugangs zu vermeiden. Sie enth¨ullteneine inh¨arente (und manchmal unerwartete) Einfachheit der Streuamplituden, oft in Verbindung zur Symmetrien; daneben, erlaubten sie die Entwicklung eines grundverschiedenen, ge- ometrischen Verst¨andnisvon Amplituden, bei dem Grassmann-Mannigfaltigkeiten eine zentrale Rolle spielen. Dieses Programm hat sich sehr gut im Rahmen eines speziellen Modells bew¨ahrt,der planaren N = 4 super Yang{Mills Theorie. Im Jahr 2013 ist eine be- merkenswerte Vermutung vorgelegt worden, die besagt, dass jede Amplitude ist insgeheim das Volumen eines verallgemeinerten Polytops, das Amplituhedron heißt. In dieser Doktorarbeit, untersuchen wir, nach einer detaillierten Einf¨uhrungin die on-shell Methoden, den Amplituhedron-Vorschlag ausf¨uhrlich auf Baumniveau und wir berichten ¨uber mehrere Ergebnisse, die zusammen mit anderen Mitarbeitern erreicht wor- den sind. Wir f¨uhreneine Formel ein, die NMHV-Baumniveau Volumenfunktionen als Inte- grale ¨uber eine duale Grassmann-Mannigfaltigkeit darstellt, und damit Triangulationen des Amplituhedrons vermeidet; dann leiten wir eine i-Vorschrift her, die uns erlaubt, sie als Summe von Residuen eines Grassmannschen Integrals aufzubauen, das im Geiste ¨ahnlich zu dem f¨urAmplituden relevanten ist. Anschließend, angeregt von den Schwierigkeiten bei der Verallgemeinerung unserer Ergebnisse, suchen wir nach einer Realisation der Yangschen Symmetrie im Rahmen des Amplituhedrons. Wir zeigen, dass mit den Volumenfunktio- nen eng verwandte Objekte wirklich invariant unter den Transformationen des Yangians Y gl(m + k) sind und denken ¨uber die Implikationen davon nach. xii 0. Zusammenfassung Summary This dissertation is concerned with some of the most recent developments in the under- standing of gauge theory scattering amplitudes at weak coupling. The traditional pertur- bative approach in terms of Feynman diagrams is well established and has achieved great triumphs, however it has become increasingly unsuited to handle the complexity of the precision calculations needed nowadays. In looking for new ways to avoid its drawbacks and bottlenecks, new techniques have been developed, collectively going under the name of on-shell methods. Beyond unveiling an inherent (and at times unexpected) simplicity of scattering amplitudes { often in connection to symmetries { they helped the rise of a rad- ically different, geometric understanding of them, in which Grassmannian manifolds play a central role. This program has proven very successful in the context of a special model, planar N = 4 super Yang{Mills theory. In 2013 a striking conjecture was put forward, stating that every amplitude is secretly the volume of a generalised polytope, called the amplituhedron. In this thesis, after providing a broad introduction about on-shell methods, we investi- gate this proposal at tree-level in detail and report on several new results that were obtained in collaboration with other authors. In particular, we present a closed formula for express- ing NMHV tree-level volume functions as integrals over a dual Grassmannian, avoiding triangulations of the amplituhedron; we subsequently derive an i-prescription that allows to alternatively construct them as a sum of residues of a Grassmannian integral, similar in spirit to the one relevant for scattering amplitudes. Motivated by the difficulties in mov- ing to more general tree-level volume functions, we then look for a realisation of Yangian symmetry in the framework of the amplituhedron. We prove that objects closely related to the volume functions are in fact invariant under the Yangian Y gl(m + k) and ponder on the implications of this result. xiv 0. Summary Acknowledgements First and foremost, I am very grateful to my supervisor, Livia Ferro, who introduced me to a thriving field to investigate a fascinating problem. Beyond always being available to answer my questions and sharing her deep knowledge, she was supportive and encouraging throughout the difficulties of my first research experiences. Moreover, she gave me the opportunity to travel to attend schools and conferences, where I had the opportunity to learn from numerous outstanding scientists: in relation to this, I would like to thank Nima Arkani-Hamed for a kind invitation to the IAS in Princeton. It has been a pleasure to share my research projects with TomekLukowski, whose expertise and insight have been of inspiration and who contributed to create a pleasant atmosphere throughout our collaborations. I also want to thank Matteo Parisi for the many fruitful discussions that improved my understanding. This dissertation has been heavily influenced by many people: I am indebted to Reinke Isermann for helping me gain familiarity with the on-shell methods; to Jos`eFrancisco Morales and Congkao Wen for collaborating on my first project; to Nils Kanning for sharing his knowledge on integrability and proofreading the Zusammenfassung of this thesis (any remaining mistake is of course my own!). I also wish to thank Jake Bourjaily, Hugh Thomas and Jaroslav Trnka for useful discussions about details of this work; finally, I owe Matteo Rosso and especially Michela Amicone for helping me code a complicated matrix in LATEX. I thoroughly enjoyed my time in Munich, also thanks to the lively atmosphere created by all members of the Mathematical physics and String theory research group. I want to personally thank for the time spent together my fellow PhD students Enrico Brehm, Fabrizio Cordonier-Tello, Nicol´asGonzalez, Daniel Jaud, Benedikt Richter and the Post- Docs Reinke Isermann, Daniel Junghans, Nils Kanning, Emanuel Malek, Stefano Massai, Christoph Mayrhofer, Erik Plauschinn, Felix Rudolph, Cornelius Schmidt-Colinet, Angnis Schmidt-May, as well as Michael Haack for the friendly help and advice on many techni- cal issues. Finally, I express my gratitude to Dieter L¨ust,for agreeing to be my second xvi 0. Acknowledgements Gutachter. I would like to thank Ruth Britto for giving me the chance to continue my career in Dublin as a PostDoc. In this regard, I am grateful to Livia Ferro, Lorenzo Magnea, Dieter L¨ustand TomekLukowski for supporting my applications with their recommenda- tion letters, as well as to Reinke Isermann, Matteo Rosso, Cornelius Schmidt-Colinet and Johannes Broedel for sharing their experience and offering me their friendly advice on the matter.
Recommended publications
  • Beyond Feynman Diagrams Lecture 2
    Beyond Feynman Diagrams Lecture 2 Lance Dixon Academic Training Lectures CERN April 24-26, 2013 Modern methods for trees 1. Color organization (briefly) 2. Spinor variables 3. Simple examples 4. Factorization properties 5. BCFW (on-shell) recursion relations Beyond Feynman Diagrams Lecture 2 April 25, 2013 2 How to organize gauge theory amplitudes • Avoid tangled algebra of color and Lorentz indices generated by Feynman rules structure constants • Take advantage of physical properties of amplitudes • Basic tools: - dual (trace-based) color decompositions - spinor helicity formalism Beyond Feynman Diagrams Lecture 2 April 25, 2013 3 Color Standard color factor for a QCD graph has lots of structure constants contracted in various orders; for example: Write every n-gluon tree graph color factor as a sum of traces of matrices T a in the fundamental (defining) representation of SU(Nc): + all non-cyclic permutations Use definition: + normalization: Beyond Feynman Diagrams Lecture 2 April 25, 2013 4 Double-line picture (’t Hooft) • In limit of large number of colors Nc, a gluon is always a combination of a color and a different anti-color. • Gluon tree amplitudes dressed by lines carrying color indices, 1,2,3,…,Nc. • Leads to color ordering of the external gluons. • Cross section, summed over colors of all external gluons = S |color-ordered amplitudes|2 • Can still use this picture at Nc=3. • Color-ordered amplitudes are still the building blocks. • Corrections to the color-summed cross section, can be handled 2 exactly, but are suppressed by 1/ Nc Beyond Feynman Diagrams Lecture 2 April 25, 2013 5 Trace-based (dual) color decomposition For n-gluon tree amplitudes, the color decomposition is momenta helicities color color-ordered subamplitude only depends on momenta.
    [Show full text]
  • Maximally Helicity Violating Amplitudes
    Maximally Helicity Violating amplitudes Andrew Lifson ID:22635416 Supervised by Assoc. Prof. Peter Skands School of Physics & Astronomy A thesis submitted in partial fulfilment for the degree of Bachelor of Science Advanced with Honours November 13, 2015 Abstract An important aspect in making quantum chromodynamics (QCD) predictions at the Large Hadron Collider (LHC) is the speed of the Monte Carlo (MC) event generators which are used to calculate them. MC event generators simulate a pure QCD collision at the LHC by first using fixed-order perturbation theory to calculate the hard (i.e. energetic) 2 ! n scatter, and then adding radiative corrections to this with a parton shower approximation. The 2 ! n scatter is traditionally calculated by summing Feynman diagrams, however the number of Feynman diagrams has a stronger than factorial growth with the number of final-state particles, hence this method quickly becomes infeasible. We can simplify this calculation by considering helicity amplitudes, in which each particle has its spin either aligned or anti-aligned with its direction of motion i.e. each particle has a specific helicity. In particular, it is well-known that the helicity amplitude for the maximally helicity violating (MHV) configuration is remarkably simple to calculate. In this thesis we describe the physics of the MHV amplitude, how we could use it within a MC event generator, and describe a program we wrote called VinciaMHV which calculates the MHV amplitude for the process qg ! q + ng for n = 1; 2; 3; 4. We tested the speed of VinciaMHV against MadGraph4 and found that VinciaMHV calculates the MHV amplitude significantly faster, especially for high particle multiplicities.
    [Show full text]
  • MHV Amplitudes in N=4 SUSY Yang-Mills Theory and Quantum Geometry of the Momentum Space
    Outline Introduction and tree MHV amplitudes BDS conjecture and amplitude - Wilson loop correspondence c=1 string example and fermionic representation of amplitudes Quantization of the moduli space On the fermionic representation of the loop MHV amplitudes Towards the stringy interpretation of the loop MHV amplitudes. MHV amplitudes in N=4 SUSY Yang-Mills theory and quantum geometry of the momentum space Alexander Gorsky ITEP GGI, Florence - 2008 (to appear) Alexander Gorsky MHV amplitudes in N=4 SUSY Yang-Mills theory and quantum geometry of the momentum space Outline Introduction and tree MHV amplitudes BDS conjecture and amplitude - Wilson loop correspondence c=1 string example and fermionic representation of amplitudes Quantization of the moduli space On the fermionic representation of the loop MHV amplitudes Towards the stringy interpretation of the loop MHV amplitudes. Introduction and tree MHV amplitudes BDS conjecture and amplitude - Wilson loop correspondence c=1 string example and fermionic representation of amplitudes Quantization of the moduli space On the fermionic representation of the loop MHV amplitudes Towards the stringy interpretation of the loop MHV amplitudes. Alexander Gorsky MHV amplitudes in N=4 SUSY Yang-Mills theory and quantum geometry of the momentum space Outline Introduction and tree MHV amplitudes BDS conjecture and amplitude - Wilson loop correspondence c=1 string example and fermionic representation of amplitudes Quantization of the moduli space On the fermionic representation of the loop MHV amplitudes
    [Show full text]
  • Emergent Unitarity from the Amplituhedron Arxiv:1906.10700V2
    Prepared for submission to JHEP Emergent Unitarity from the Amplituhedron Akshay Yelleshpur Srikant Department of Physics, Princeton University, NJ, USA Abstract: We present a proof of perturbative unitarity for planar N = 4 SYM, following from the geometry of the amplituhedron. This proof is valid for amplitudes of arbitrary multiplicity n, loop order L and MHV degree k. arXiv:1906.10700v2 [hep-th] 26 Dec 2019 Contents 1 Introduction2 2 Review of the topological definition of An;k;L 3 2.1 Momentum twistors3 2.2 Topological definition4 2.2.1 Tree level conditions4 2.2.2 Loop level conditions5 2.2.3 Mutual positivity condition6 2.3 Amplitudes and integrands as Canonical Forms6 2.4 Unitarity and the Optical theorem7 3 Proof for 4 point Amplitudes9 4 Proof for MHV amplitudes of arbitrary multiplicity 12 4.1 Left and right Amplituhedra 12 4.1.1 The left amplituhedron An1;0;L1 12 4.1.2 The right Amplituhedron An2;0;L2 14 4.2 Factorization on the unitarity cut 15 4.2.1 Trivialized mutual positivity 16 5 Proof for higher k sectors 17 5.1 The left and right amplituhedra 18 5.1.1 The left amplituhedron AL 18 n1;kL;L1 5.1.2 The right amplituhedron AR 20 n2;kR;L2 5.2 Factorization of the external data 21 5.3 Factorization of loop level data 24 5.4 Mutual positivity 25 6 Conclusions 25 A Restricting flip patterns 26 { 1 { 1 Introduction Unitarity is at the heart of the traditional, Feynman diagrammatic approach to cal- culating scattering amplitudes.
    [Show full text]
  • Implications of Perturbative Unitarity for Scalar Di-Boson Resonance Searches at LHC
    Implications of perturbative unitarity for scalar di-boson resonance searches at LHC Luca Di Luzio∗1,2, Jernej F. Kameniky3,4, and Marco Nardecchiaz5,6 1Dipartimento di Fisica, Universit`adi Genova and INFN, Sezione di Genova, via Dodecaneso 33, 16159 Genova, Italy 2Institute for Particle Physics Phenomenology, Department of Physics, Durham University, DH1 3LE, United Kingdom 3JoˇzefStefan Institute, Jamova 39, 1000 Ljubljana, Slovenia 4Faculty of Mathematics and Physics, University of Ljubljana, Jadranska 19, 1000 Ljubljana, Slovenia 5DAMTP, University of Cambridge, Wilberforce Road, Cambridge CB3 0WA, United Kingdom 6CERN, Theoretical Physics Department, Geneva, Switzerland Abstract We study the constraints implied by partial wave unitarity on new physics in the form of spin-zero di-boson resonances at LHC. We derive the scale where the effec- tive description in terms of the SM supplemented by a single resonance is expected arXiv:1604.05746v3 [hep-ph] 2 Apr 2019 to break down depending on the resonance mass and signal cross-section. Likewise, we use unitarity arguments in order to set perturbativity bounds on renormalizable UV completions of the effective description. We finally discuss under which condi- tions scalar di-boson resonance signals can be accommodated within weakly-coupled models. ∗[email protected] [email protected] [email protected] 1 Contents 1 Introduction3 2 Brief review on partial wave unitarity4 3 Effective field theory of a scalar resonance5 3.1 Scalar mediated boson scattering . .6 3.2 Fermion-scalar contact interactions . .8 3.3 Unitarity bounds . .9 4 Weakly-coupled models 12 4.1 Single fermion case . 15 4.2 Single scalar case .
    [Show full text]
  • Quantum Circuits Synthesis Using Householder Transformations Timothée Goubault De Brugière, Marc Baboulin, Benoît Valiron, Cyril Allouche
    Quantum circuits synthesis using Householder transformations Timothée Goubault de Brugière, Marc Baboulin, Benoît Valiron, Cyril Allouche To cite this version: Timothée Goubault de Brugière, Marc Baboulin, Benoît Valiron, Cyril Allouche. Quantum circuits synthesis using Householder transformations. Computer Physics Communications, Elsevier, 2020, 248, pp.107001. 10.1016/j.cpc.2019.107001. hal-02545123 HAL Id: hal-02545123 https://hal.archives-ouvertes.fr/hal-02545123 Submitted on 16 Apr 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. Quantum circuits synthesis using Householder transformations Timothée Goubault de Brugière1,3, Marc Baboulin1, Benoît Valiron2, and Cyril Allouche3 1Université Paris-Saclay, CNRS, Laboratoire de recherche en informatique, 91405, Orsay, France 2Université Paris-Saclay, CNRS, CentraleSupélec, Laboratoire de Recherche en Informatique, 91405, Orsay, France 3Atos Quantum Lab, Les Clayes-sous-Bois, France Abstract The synthesis of a quantum circuit consists in decomposing a unitary matrix into a series of elementary operations. In this paper, we propose a circuit synthesis method based on the QR factorization via Householder transformations. We provide a two-step algorithm: during the rst step we exploit the specic structure of a quantum operator to compute its QR factorization, then the factorized matrix is used to produce a quantum circuit.
    [Show full text]
  • New Exciting Approaches to Scattering Amplitudes
    New Exciting Approaches to Scattering Amplitudes Henriette Elvang University of Michigan Aspen Center for Physics Colloquium July 16, 2015 In the news… #10 Using only pen and paper, he [Arkani-Hamed & Trnka] discovered a new kind of geometric shape called an amplituhedron […] The shape’s dimensions – length width, height and other parameters […] – represent information about the colliding particles […] Using only pen and paper, he [Arkani-Hamed & Trnka] discovered a new kind of geometric shape called an amplituhedron […] The shape’s dimensions – length width, height and other parameters […] – represent information about the colliding particles […] “We’ve known for decades that spacetime is doomed,” says Arkani-Hamed. Amplituhedrons? Spacetime doomed?? What in the world is this all about??? The story begins with scattering amplitudes in particle physics 1 Introduction 1 Introduction 2 pi =0 In a traditional quantum field theory (QFT) course, you learn to extract Feynman rules from a Lagrangian and use them to calculate a scattering amplitude A as a sum of Feynman dia- Scattering Amplitudes! grams organized perturbatively in the loop-expansion. From the amplitude you calculate the Scatteringdi↵erential amplitudes cross-section, ! dσ A 2, which — if needed — includes a suitable spin-sum average. encode the processes of! d⌦ / | | elementaryFinally particle the cross-sectioninteractions! σ can be found by integration of dσ/d⌦ over angles, with appropriate ! forsymmetry example! factors included for identical final-state particles. The quantities σ and dσ/d⌦ are electrons, photons, quarks,…! the observables of interest for particle physics experiments, but the input for computing them Comptonare thescattering:gauge invariant on-shell scattering amplitudes A.
    [Show full text]
  • Twistor-Strings, Grassmannians and Leading Singularities
    Twistor-Strings, Grassmannians and Leading Singularities Mathew Bullimore1, Lionel Mason2 and David Skinner3 1Rudolf Peierls Centre for Theoretical Physics, 1 Keble Road, Oxford, OX1 3NP, United Kingdom 2Mathematical Institute, 24-29 St. Giles', Oxford, OX1 3LB, United Kingdom 3Perimeter Institute for Theoretical Physics, 31 Caroline St., Waterloo, ON, N2L 2Y5, Canada Abstract We derive a systematic procedure for obtaining explicit, `-loop leading singularities of planar = 4 super Yang-Mills scattering amplitudes in twistor space directly from their momentum spaceN channel diagram. The expressions are given as integrals over the moduli of connected, nodal curves in twistor space whose degree and genus matches expectations from twistor-string theory. We propose that a twistor-string theory for pure = 4 super Yang-Mills | if it exists | is determined by the condition that these leading singularityN formulæ arise as residues when an unphysical contour for the path integral is used, by analogy with the momentum space leading singularity conjecture. We go on to show that the genus g twistor-string moduli space for g-loop Nk−2MHV amplitudes may be mapped into the Grassmannian G(k; n). For a leading singularity, the image of this map is a 2(n 2)-dimensional subcycle of G(k; n) and, when `primitive', it is of exactly the type found from− the Grassmannian residue formula of Arkani-Hamed, Cachazo, Cheung & Kaplan. Based on this correspondence and the Grassmannian conjecture, we deduce arXiv:0912.0539v3 [hep-th] 30 Dec 2009 restrictions on the possible leading singularities of multi-loop NpMHV amplitudes. In particular, we argue that no new leading singularities can arise beyond 3p loops.
    [Show full text]
  • Path Integral for the Hydrogen Atom
    Path Integral for the Hydrogen Atom Solutions in two and three dimensions Vägintegral för Väteatomen Lösningar i två och tre dimensioner Anders Svensson Faculty of Health, Science and Technology Physics, Bachelor Degree Project 15 ECTS Credits Supervisor: Jürgen Fuchs Examiner: Marcus Berg June 2016 Abstract The path integral formulation of quantum mechanics generalizes the action principle of classical mechanics. The Feynman path integral is, roughly speaking, a sum over all possible paths that a particle can take between fixed endpoints, where each path contributes to the sum by a phase factor involving the action for the path. The resulting sum gives the probability amplitude of propagation between the two endpoints, a quantity called the propagator. Solutions of the Feynman path integral formula exist, however, only for a small number of simple systems, and modifications need to be made when dealing with more complicated systems involving singular potentials, including the Coulomb potential. We derive a generalized path integral formula, that can be used in these cases, for a quantity called the pseudo-propagator from which we obtain the fixed-energy amplitude, related to the propagator by a Fourier transform. The new path integral formula is then successfully solved for the Hydrogen atom in two and three dimensions, and we obtain integral representations for the fixed-energy amplitude. Sammanfattning V¨agintegral-formuleringen av kvantmekanik generaliserar minsta-verkanprincipen fr˚anklassisk meka- nik. Feynmans v¨agintegral kan ses som en summa ¨over alla m¨ojligav¨agaren partikel kan ta mellan tv˚a givna ¨andpunkterA och B, d¨arvarje v¨agbidrar till summan med en fasfaktor inneh˚allandeden klas- siska verkan f¨orv¨agen.Den resulterande summan ger propagatorn, sannolikhetsamplituden att partikeln g˚arfr˚anA till B.
    [Show full text]
  • Twistor Theory and Differential Equations
    IOP PUBLISHING JOURNAL OF PHYSICS A: MATHEMATICAL AND THEORETICAL J. Phys. A: Math. Theor. 42 (2009) 404004 (19pp) doi:10.1088/1751-8113/42/40/404004 Twistor theory and differential equations Maciej Dunajski Department of Applied Mathematics and Theoretical Physics, University of Cambridge, Wilberforce Road, Cambridge CB3 0WA, UK E-mail: [email protected] Received 31 January 2009, in final form 17 March 2009 Published 16 September 2009 Online at stacks.iop.org/JPhysA/42/404004 Abstract This is an elementary and self-contained review of twistor theory as a geometric tool for solving nonlinear differential equations. Solutions to soliton equations such as KdV,Tzitzeica, integrable chiral model, BPS monopole or Sine–Gordon arise from holomorphic vector bundles over T CP1. A different framework is provided for the dispersionless analogues of soliton equations, such as dispersionless KP or SU(∞) Toda system in 2+1 dimensions. Their solutions correspond to deformations of (parts of) T CP1, and ultimately to Einstein– Weyl curved geometries generalizing the flat Minkowski space. A number of exercises are included and the necessary facts about vector bundles over the Riemann sphere are summarized in the appendix. PACS number: 02.30.Ik (Some figures in this article are in colour only in the electronic version) 1. Introduction Twistor theory was created by Penrose [19] in 1967. The original motivation was to unify general relativity and quantum mechanics in a non-local theory based on complex numbers. The application of twistor theory to differential equations and integrability has been an unexpected spin off from the twistor programme.
    [Show full text]
  • Twistor Theory at Fifty: from Rspa.Royalsocietypublishing.Org Contour Integrals to Twistor Strings Michael Atiyah1,2, Maciej Dunajski3 and Lionel Review J
    Downloaded from http://rspa.royalsocietypublishing.org/ on November 10, 2017 Twistor theory at fifty: from rspa.royalsocietypublishing.org contour integrals to twistor strings Michael Atiyah1,2, Maciej Dunajski3 and Lionel Review J. Mason4 Cite this article: Atiyah M, Dunajski M, Mason LJ. 2017 Twistor theory at fifty: from 1School of Mathematics, University of Edinburgh, King’s Buildings, contour integrals to twistor strings. Proc. R. Edinburgh EH9 3JZ, UK Soc. A 473: 20170530. 2Trinity College Cambridge, University of Cambridge, Cambridge http://dx.doi.org/10.1098/rspa.2017.0530 CB21TQ,UK 3Department of Applied Mathematics and Theoretical Physics, Received: 1 August 2017 University of Cambridge, Cambridge CB3 0WA, UK Accepted: 8 September 2017 4The Mathematical Institute, Andrew Wiles Building, University of Oxford, Oxford OX2 6GG, UK Subject Areas: MD, 0000-0002-6477-8319 mathematical physics, high-energy physics, geometry We review aspects of twistor theory, its aims and achievements spanning the last five decades. In Keywords: the twistor approach, space–time is secondary twistor theory, instantons, self-duality, with events being derived objects that correspond to integrable systems, twistor strings compact holomorphic curves in a complex threefold— the twistor space. After giving an elementary construction of this space, we demonstrate how Author for correspondence: solutions to linear and nonlinear equations of Maciej Dunajski mathematical physics—anti-self-duality equations e-mail: [email protected] on Yang–Mills or conformal curvature—can be encoded into twistor cohomology. These twistor correspondences yield explicit examples of Yang– Mills and gravitational instantons, which we review. They also underlie the twistor approach to integrability: the solitonic systems arise as symmetry reductions of anti-self-dual (ASD) Yang–Mills equations, and Einstein–Weyl dispersionless systems are reductions of ASD conformal equations.
    [Show full text]
  • Less Decoherence and More Coherence in Quantum Gravity, Inflationary Cosmology and Elsewhere
    Less Decoherence and More Coherence in Quantum Gravity, Inflationary Cosmology and Elsewhere Elias Okon1 and Daniel Sudarsky2 1Instituto de Investigaciones Filosóficas, Universidad Nacional Autónoma de México, Mexico City, Mexico. 2Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México, Mexico City, Mexico. Abstract: In [1] it is argued that, in order to confront outstanding problems in cosmol- ogy and quantum gravity, interpretational aspects of quantum theory can by bypassed because decoherence is able to resolve them. As a result, [1] concludes that our focus on conceptual and interpretational issues, while dealing with such matters in [2], is avoidable and even pernicious. Here we will defend our position by showing in detail why decoherence does not help in the resolution of foundational questions in quantum mechanics, such as the measurement problem or the emergence of classicality. 1 Introduction Since its inception, more than 90 years ago, quantum theory has been a source of heated debates in relation to interpretational and conceptual matters. The prominent exchanges between Einstein and Bohr are excellent examples in that regard. An avoid- ance of such issues is often justified by the enormous success the theory has enjoyed in applications, ranging from particle physics to condensed matter. However, as people like John S. Bell showed [3], such a pragmatic attitude is not always acceptable. In [2] we argue that the standard interpretation of quantum mechanics is inadequate in cosmological contexts because it crucially depends on the existence of observers external to the studied system (or on an artificial quantum/classical cut). We claim that if the system in question is the whole universe, such observers are nowhere to be found, so we conclude that, in order to legitimately apply quantum mechanics in such contexts, an observer independent interpretation of the theory is required.
    [Show full text]