Studies in Field Theories: Mhv Vertices, Twistor Space, Recursion Relations and Chiral Rings
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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. -
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. -
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 -
Magnetic Vortices in Gauge/Gravity Duality
Magnetic Vortices in Gauge/Gravity Duality Dissertation by Migael Strydom Magnetic Vortices in Gauge/Gravity Duality Dissertation an der Fakult¨atf¨urPhysik der Ludwig{Maximilians{Universit¨at M¨unchen vorgelegt von Migael Strydom aus Pretoria M¨unchen, den 20. Mai 2014 Dissertation submitted to the faculty of physics of the Ludwig{Maximilians{Universit¨atM¨unchen by Migael Strydom supervised by Prof. Dr. Johanna Karen Erdmenger Max-Planck-Institut f¨urPhysik, M¨unchen 1st Referee: Prof. Dr. Johanna Karen Erdmenger 2nd Referee: Prof. Dr. Dieter L¨ust Date of submission: 20 May 2014 Date of oral examination: 18 July 2014 Zusammenfassung Wir untersuchen stark gekoppelte Ph¨anomene unter Verwendung der Dualit¨at zwischen Eich- und Gravitationstheorien. Dabei liegt ein besonderer Fokus einer- seits auf Vortex L¨osungen, die von einem magnetischem Feld verursacht werden, und andererseits auf zeitabh¨angigen Problemen in holographischen Modellen. Das wichtigste Ergebnis ist die Entdeckung eines unerwarteten Effektes in einem ein- fachen holografischen Modell: ein starkes nicht abelsches magnetisches Feld verur- sacht die Entstehung eines Grundzustandes in der Form eines dreieckigen Gitters von Vortices. Die Dualit¨at zwischen Eich- und Gravitationstheorien ist ein m¨achtiges Werk- zeug welches bereits verwendet wurde um stark gekoppelte Systeme vom Quark- Gluonen Plasma in Teilchenbeschleunigern bis hin zu Festk¨orpertheorien zu be- schreiben. Die wichtigste Idee ist dabei die der Dualit¨at: Eine stark gekoppelte Quantenfeldtheorie kann untersucht werden, indem man die Eigenschaften eines aus den Einsteinschen Feldgleichungen folgenden Gravitations-Hintergrundes be- stimmt. Eine der Gravitationstheorien, die in dieser Arbeit behandelt werden, ist ei- ne Einstein{Yang{Mills Theorie in einem AdS{Schwarzschild Hintergrund mit SU(2)-Eichsymmetrie. -
Jhep05(2018)208
Published for SISSA by Springer Received: March 12, 2018 Accepted: May 21, 2018 Published: May 31, 2018 Hidden conformal symmetry in tree-level graviton JHEP05(2018)208 scattering Florian Loebbert,a Matin Mojazab and Jan Plefkaa aInstitut f¨urPhysik and IRIS Adlershof, Humboldt-Universit¨atzu Berlin, Zum Großen Windkanal 6, 12489 Berlin, Germany bMax-Planck-Institut f¨urGravitationsphysik, Albert-Einstein-Institut, Am M¨uhlenberg 1, 14476 Potsdam, Germany E-mail: [email protected], [email protected], [email protected] Abstract: We argue that the scattering of gravitons in ordinary Einstein gravity possesses a hidden conformal symmetry at tree level in any number of dimensions. The presence of this conformal symmetry is indicated by the dilaton soft theorem in string theory, and it is reminiscent of the conformal invariance of gluon tree-level amplitudes in four dimensions. To motivate the underlying prescription, we demonstrate that formulating the conformal symmetry of gluon amplitudes in terms of momenta and polarization vectors requires man- ifest reversal and cyclic symmetry. Similarly, our formulation of the conformal symmetry of graviton amplitudes relies on a manifestly permutation symmetric form of the ampli- tude function. Keywords: Conformal and W Symmetry, Scattering Amplitudes ArXiv ePrint: 1802.05999 Open Access, c The Authors. https://doi.org/10.1007/JHEP05(2018)208 Article funded by SCOAP3. Contents 1 Introduction1 2 Poincar´eand conformal symmetry in momentum space3 3 Conformal symmetry of Yang-Mills -
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. -
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. -
Arxiv:Hep-Th/0611273V2 18 Jan 2007
CORE Metadata, citation and similar papers at core.ac.uk Provided by CERN Document Server hep-th/0611273; DAMTP-2006-116; SPHT-T06/156; UB-ECM-PF-06-40 Ultraviolet properties of Maximal Supergravity Michael B. Green Department of Applied Mathematics and Theoretical Physics Wilberforce Road, Cambridge CB3 0WA, UK Jorge G. Russo Instituci´oCatalana de Recerca i Estudis Avan¸cats (ICREA), University of Barcelona, Av.Diagonal 647, Barcelona 08028 SPAIN Pierre Vanhove Service de Physique Th´eorique, CEA/Saclay, F-91191Gif-sur-Yvette, France (Dated: January 19, 2007) We argue that recent results in string perturbation theory indicate that the four-graviton am- plitude of four-dimensional N = 8 supergravity might be ultraviolet finite up to eight loops. We similarly argue that the h-loop M-graviton amplitude might be finite for h< 7+ M/2. PACS numbers: 11.25.-w,04.65.+e,11.25.Db Maximally extended supergravity has for a long time gravity and this ignorance was parameterized by an un- held a privileged position among supersymmetric field limited number of unknown coefficients of counterterms. theories. Its four-dimensional incarnation as N = 8 su- Nevertheless, requiring the structure of the amplitude to pergravity [1] initially raised the hope of a perturbatively be consistent with string theory led to interesting con- finite quantum theory of gravity while its origin in N =1 straints. Among these were strong nonrenormalization eleven-dimensional supergravity [2] provided the impetus conditions in the ten-dimensional type IIA string theory for the subsequent development of M-theory, or the non- limit – where the eleven-dimensional theory is compact- perturbative completion of string theory. -
Loop Amplitudes from MHV Diagrams - Part 1
Loop Amplitudes from MHV Diagrams - part 1 - Gabriele Travaglini Queen Mary, University of London Brandhuber, Spence, GT hep-th/0407214, hep-th/0510253 Bedford, Brandhuber, Spence, GT hep-th/0410280, hep-th/0412108 Brandhuber, McNamara, Spence, GT in progress 2 HP Workshop, Zürich, September 2006 Outline • Motivations and basic formalism • MHV diagrams (Cachazo, Svrcek,ˇ Witten) - Loop MHV diagrams (Brandhuber, Spence, GT) - Applications: One-loop MHV amplitudes in N=4, N=1 & non-supersymmetric Yang-Mills • Proof at one-loop: Andreas’s talk on Friday Motivations • Simplicity of scattering amplitudes unexplained by textbook Feynman diagrams - Parke-Taylor formula for Maximally Helicity Violating amplitude of gluons (helicities are a permutation of −−++ ....+) • New methods account for this simplicity, and allow for much more efficient calculations • LHC is coming ! Towards simplicity • Colour decomposition (Berends, Giele; Mangano, Parke, Xu; Mangano; Bern, Kosower) • Spinor helicity formalism (Berends, Kleiss, De Causmaecker, Gastmans, Wu; De Causmaecker, Gastmans, Troost, Wu; Kleiss, Stirling; Xu, Zhang, Chang; Gunion, Kunszt) Colour decomposition • Main idea: disentangle colour • At tree level, Yang-Mills interactions are planar tree a a A ( p ,ε ) = Tr(T σ1 T σn) A(σ(p ,ε ),...,σ(p ,ε )) { i i} ∑ ··· 1 1 n n σ Colour-ordered partial amplitude - Include only diagrams with fixed cyclic ordering of gluons - Analytic structure is simpler • At loop level: multi-trace contributions - subleading in 1/N Spinor helicity formalism • Consider a null vector p µ µ µ = ( ,! ) • Define p a a ˙ = p µ σ a a ˙ where σ 1 σ • If p 2 = 0 then det p = 0 ˜ ˜ Hence p aa˙ = λaλa˙ · λ (λ) positive (negative) helicity • spinors a b a˙ b˙ Inner products 12 : = ε ab λ λ , [12] := ε ˙λ˜ λ˜ • ! " 1 2 a˙b 1 2 Parke-Taylor formula 4 + + i j A (1 ...i− .. -
Localization of Gauge Theories on the Three-Sphere
Localization of Gauge Theories on the Three-Sphere Thesis by Itamar Yaakov In Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy California Institute of Technology Pasadena, California 2012 (Defended May 14, 2012) ii c 2012 Itamar Yaakov All Rights Reserved iii Acknowledgements I would like to thank my research adviser, Professor Anton Kapustin, for his continuing support. His mentorship, foresight, intuition and collaboration were the keys to my having a successful graduate career. The work described here was done in collaboration with Brian Willett and much of the credit for successful completion of this work is duly his. I would also like to express my deep appreciation to the California Institute of Technology, and especially the professors and staff of the physics department for a thoroughly enjoyable and interesting five years of study. Special thanks to Frank Porter, Donna Driscoll, Virginio Sannibale, and Carol Silberstein. I am grateful to Mark Wise, John Schwarz, Hirosi Ooguri, and Frank Porter for serving on my candidacy and defense committees. I benefited from discussions along the way with Ofer Aharony, John Schwarz, Sergei Gukov, Hirosi Ooguri, David Kutasov, Zohar Komargodski, Daniel Jafferis, and Jaume Gomis. I would like to thank the organizers and lecturers of the PITP 2010 summer school at the Institute for Advanced study for an impeccably produced learning experience. My thanks also to Gregory Moore and Nathan Seiberg for taking the time to discuss my research while at the school. I would like to thank UCLA, especially Yu-tin Huang, and the Perimeter Institute and Jaume Gomis for allowing me to present my work there. -
Pos(HEP2005)146
GL(1) Charged States in Twistor String Theory PoS(HEP2005)146 Dimitri Polyakovy Center for Advanced Mathematical Studies and Department of Physics American University of Beirut Beirut, Lebanon Abstract We discuss the appearance of the GL(1) charged physical operators in the twistor string theory. These operators are shown to be BRST-invariant and non-trivial and some of their correlators and conformal β-functions are computed. Remarkably, the non- conservation of the GL(1) charge in interactions involving these operators, is related to the anomalous term in the Kac-Moody current algebra. While these operators play no role in the maximum helicity violating (MHV) amplitudes, they are shown to contribute nontrivially to the non-MHV correlators in the presence of the worldsheet instantons. We argue that these operators describe the non-perturbative dynamics of solitons in conformal supergravity. The exact form of such solitonic solutions is yet to be determined. y Presented at International Europhysics Conference i High Energy Physics, July 21st-27th 2005 Lisboa, Portugal Introduction The hypothesis of the gauge-string correspondence, attempting to relate the gauge- theoretic and string degrees of freedom, is a long-standing problem of great importance. Remarkably, such a correspondence can be shown to occur both in the strongly coupled and the perturbative limits of Yang-Mills theory. Firstly, it is well-known that the AdS/CFT correspondence (e.g. see [1], [2], [3]) implies the isomorphism between vertex operators of string theory in the -
Unitarity Methods for Scattering Amplitudes in Perturbative Gauge Theories
Unitarity Methods for Scattering Amplitudes in Perturbative Gauge Theories by MASSIMILIANO VINCON A report presented for the examination for the transfer of status to the degree of Doctor of Philosophy of the University of London Thesis Supervisor DR ANDREAS BRANDHUBER Centre for Research in String Theory Department of Physics Queen Mary University of London Mile End Road London E1 4NS United Kingdom The strong do what they want and the weak suffer as they must.1 1Thucydides. Declaration I hereby declare that the material presented in this thesis is a representation of my own personal work unless otherwise stated and is a result of collaborations with Andreas Brandhuber and Gabriele Travaglini. Massimiliano Vincon Abstract In this thesis, we discuss novel techniques used to compute perturbative scattering am- plitudes in gauge theories. In particular, we focus on the use of complex momenta and generalised unitarity as efficient and elegant tools, as opposed to standard textbook Feynman rules, to compute one-loop amplitudes in gauge theories. We consider scatter- ing amplitudes in non-supersymmetric and supersymmetric Yang-Mills theories (SYM). After introducing some of the required mathematical machinery, we give concrete exam- ples as to how generalised unitarity works in practice and we correctly reproduce the n- gluon one-loop MHV amplitude in non-supersymmetric Yang-Mills theory with a scalar running in the loop, thus confirming an earlier result obtained using MHV diagrams: no independent check of this result had been carried out yet. Non-supersymmetric scat- tering amplitudes are the most difficult to compute and are of great importance as they are part of background processes at the LHC.