How I learned to stop worrying and love the tachyon

Size: px
Start display at page:

Download "How I learned to stop worrying and love the tachyon"

Transcription

1 love the tachyon Max Planck Institute for Gravitational Physics Potsdam 6-October-2008

2 Historical background Open string field theory Closed string field theory

3 Experimental Hadron physics Mesons mass spectrum obeys the Regge trajectory m 2 = α 0 + α 1 J Four-point functions have an s/t duality The Veneziano amplitude has both properties String scattering gives the Veneziano amplitude There is only one free parameter the string tension QCD turned out as a better model for hadronic physics Yet string theory predicts gravity

4 Strings are the fundamental objects (instead of point particles) Strings span a worldsheet (instead of a worldline) The string action is proportional to the worldsheet area L = 1 2πα dσ 2 h h ab g µν a X µ b X ν a, b = 0, 1 µ, ν = 0,..., 25(D 1) String equation of motion ( X µ 2 = 2 τ 2 2 σ ) X µ = 0

5 Classic relativistic massless strings Open string spectrum (Neuman boundary conditions) p A µ 1, p Aµ 2, p Closed string spectrum (periodical boundary conditions) p A (L)µ 1, A (R)ν 1, p A (L)µ 2, A (R)ν 2, p

6 Quantum relativistic massless strings Open string spectrum 0, p a µ 1 0, p a µ 2 0, p m 2 = 1 m 2 = 0 m 2 = 1 Closed string spectrum 0, p a (L)µ 1 a (R)ν 1 0, p a (L)µ 2 a (R)ν 2 0, p m 2 = 2 m 2 = 0 m 2 = 2

7 Vacuum state Vacuum energy 0 a 1 2 (D 2) n=1 D 1 n=1 µ=2 0 µ n n = D 2 24 D=26 1 Using zeta function regularization n=1 n = 1 Regge spectrum m 2 = a spin m 2 = a + 1 spin 1 a µ 1 0 (D 2) m 2 = a + 2 spin 2 a µ 1 a ν (D 2)(D 1) m 2 = a + 2 spin 1 a µ (D 2) The last two sum-up to a spin-2 representation of SO(D 1) 12

8 Current inventory Meson spectrum, string tension related to Regge slope T s Ms 2 = MQCD 2 (100MeV )2 Gravitons, string tension related to gravitational constant G 1 N = M2 Planck = g sm 2 s (10 19 GeV ) 2 Gauge bosons, string tension related to regularization scale M 2 s > M 2 GUT (1016 GeV ) 2 g s = g 2 YM dimensions No fermions A tachyon

9 Add supersymmetry to the string worldsheet Down to 10 dimension The tachyon is projected out Space-time fermions Consistent chiral models Space-time supersymmetry D-branes mutli-dimensional non-perturbative objects

10 String theory is defined perturbatively The perturbative vacuum is not stable (SFT) is a non-perturbative formulation of String theory We need an action principle for the string field instead of the worldsheet action

11 s worldline action is its proper time L = ds = dτ g µν Ẋ µẋ ν Equation of motion E 2 = p 2 + m 2 First quantization gives the Klein-Gordon equation Φ + m 2 Φ = 0 This is a classical scalar field

12 Scalar field with Higgs-like potential example L = 1 2 µφ µ Φ m2 Φ λφ4 Feynman diagrams Equation of motion Φ m 2 Φ + λφ 3 = 0 Static solutions Φ = 0 Φ = 0 or Φ = ± m λ

13 Open Bosonic Cubic The string field is a functional from the string configuration to a scalar value Ψ[X µ (σ)] In mode-expansion we get Ψ = dp T (p) 0, p + A µ (p)a µ 1 0, p +... The action is Equation of motion S = 1 2 Ψ (p2 + m 2 ) Ψ + g s 3 Ψ 3 (p 2 + m 2 )Ψ + Ψ 2 = 0

14 Open strings must end on a D-brane has a space-time filling D25-brane The tachyon signifies the instability of the D25-brane A solution to the E.O.M would correspond to annihilation of the D25-brane The potential height would be exactly the D25-brane energy E = V 25 T 25 There would be no open-string degrees of freedom around the solution

15 Closed string field theory Seems redundant open string field theory already contains closed strings at one-loop Seems necessarily because of the closed string tachyon No equivalent to

16 Subjects not covered Black hole entropy Holography AdS/CFT correspondence Super Open questions Is the tachyon related to the Higgs boson? Is the tachyon related to the inflaton field? Does string theory describe hadron physics after all? Is string theory the theory of everything?

1/N Expansions in String and Gauge Field Theories. Adi Armoni Swansea University

1/N Expansions in String and Gauge Field Theories. Adi Armoni Swansea University 1/N Expansions in String and Gauge Field Theories Adi Armoni Swansea University Oberwoelz, September 2010 1 Motivation It is extremely difficult to carry out reliable calculations in the strongly coupled

More information

The Gauge/Gravity correspondence: linking General Relativity and Quantum Field theory

The Gauge/Gravity correspondence: linking General Relativity and Quantum Field theory The Gauge/Gravity correspondence: linking General Relativity and Quantum Field theory Alfonso V. Ramallo Univ. Santiago IFIC, Valencia, April 11, 2014 Main result: a duality relating QFT and gravity Quantum

More information

Particles and Strings Probing the Structure of Matter and Space-Time

Particles and Strings Probing the Structure of Matter and Space-Time Particles and Strings Probing the Structure of Matter and Space-Time University Hamburg DPG-Jahrestagung, Berlin, March 2005 2 Physics in the 20 th century Quantum Theory (QT) Planck, Bohr, Heisenberg,...

More information

Exercise 1 Classical Bosonic String

Exercise 1 Classical Bosonic String Exercise 1 Classical Bosonic String 1. The Relativistic Particle The action describing a free relativistic point particle of mass m moving in a D- dimensional Minkowski spacetime is described by ) 1 S

More information

String / gauge theory duality and ferromagnetic spin chains

String / gauge theory duality and ferromagnetic spin chains String / gauge theory duality and ferromagnetic spin chains M. Kruczenski Princeton Univ. In collaboration w/ Rob Myers, David Mateos, David Winters Arkady Tseytlin, Anton Ryzhov Summary Introduction mesons,,...

More information

Gravity, Strings and Branes

Gravity, Strings and Branes Gravity, Strings and Branes Joaquim Gomis International Francqui Chair Inaugural Lecture Leuven, 11 February 2005 Fundamental Forces Strong Weak Electromagnetism QCD Electroweak SM Gravity Standard Model

More information

Large-N QCD, Veneziano Amplitude, and Holography. Adi Armoni Swansea University CAQCD 2016, May 13, 2016

Large-N QCD, Veneziano Amplitude, and Holography. Adi Armoni Swansea University CAQCD 2016, May 13, 2016 Large-N QCD, Veneziano Amplitude, and Holography Adi Armoni Swansea University CAQCD 2016, May 13, 2016 A. A., Phys.Lett. B756 (2016) 328-331 A. A., Edwin Ireson, work in progress 1 Introduction The 1968

More information

String/gauge theory duality and QCD

String/gauge theory duality and QCD String/gauge theory duality and QCD M. Kruczenski Purdue University ASU 009 Summary Introduction String theory Gauge/string theory duality. AdS/CFT correspondence. Mesons in AdS/CFT Chiral symmetry breaking

More information

γγ αβ α X µ β X µ (1)

γγ αβ α X µ β X µ (1) Week 3 Reading material from the books Zwiebach, Chapter 12, 13, 21 Polchinski, Chapter 1 Becker, Becker, Schwartz, Chapter 2 Green, Schwartz, Witten, chapter 2 1 Polyakov action We have found already

More information

2T-physics and the Standard Model of Particles and Forces Itzhak Bars (USC)

2T-physics and the Standard Model of Particles and Forces Itzhak Bars (USC) 2T-physics and the Standard Model of Particles and Forces Itzhak Bars (USC) hep-th/0606045 Success of 2T-physics for particles on worldlines. Field theory version of 2T-physics. Standard Model in 4+2 dimensions.

More information

AdS/CFT duality. Agnese Bissi. March 26, Fundamental Problems in Quantum Physics Erice. Mathematical Institute University of Oxford

AdS/CFT duality. Agnese Bissi. March 26, Fundamental Problems in Quantum Physics Erice. Mathematical Institute University of Oxford AdS/CFT duality Agnese Bissi Mathematical Institute University of Oxford March 26, 2015 Fundamental Problems in Quantum Physics Erice What is it about? AdS=Anti de Sitter Maximally symmetric solution of

More information

8.821 String Theory Fall 2008

8.821 String Theory Fall 2008 MIT OpenCourseWare http://ocw.mit.edu 8.821 String Theory Fall 2008 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms. 8.821 F2008 Lecture 02: String theory

More information

Gravity, Strings and Branes

Gravity, Strings and Branes Gravity, Strings and Branes Joaquim Gomis Universitat Barcelona Miami, 23 April 2009 Fundamental Forces Strong Weak Electromagnetism QCD Electroweak SM Gravity Standard Model Basic building blocks, quarks,

More information

Large Extra Dimensions and the Hierarchy Problem

Large Extra Dimensions and the Hierarchy Problem Large Extra Dimensions and the Hierarchy Problem The Hierarchy Problem - At Planck energies (M P L 10 19 GeV ) all four forces have the same strength. -At the Electroweak scale (M EW 1T ev ) the four forces

More information

Physics 4213/5213 Lecture 1

Physics 4213/5213 Lecture 1 August 28, 2002 1 INTRODUCTION 1 Introduction Physics 4213/5213 Lecture 1 There are four known forces: gravity, electricity and magnetism (E&M), the weak force, and the strong force. Each is responsible

More information

Fundamental Physics: Quantum Field Theory

Fundamental Physics: Quantum Field Theory Mobolaji Williams (mwilliams@physics.harvard.edu x) First Version: June 1, 216 Fundamental Physics: Quantum Field Theory What is the topic? Quantum field theory refers to the quantum theory of fields in

More information

Théorie des cordes: quelques applications. Cours II: 4 février 2011

Théorie des cordes: quelques applications. Cours II: 4 février 2011 Particules Élémentaires, Gravitation et Cosmologie Année 2010-11 Théorie des cordes: quelques applications Cours II: 4 février 2011 Résumé des cours 2009-10: deuxième partie 04 février 2011 G. Veneziano,

More information

If I only had a Brane

If I only had a Brane If I only had a Brane A Story about Gravity and QCD. on 20 slides and in 40 minutes. AdS/CFT correspondence = Anti de Sitter / Conformal field theory correspondence. Chapter 1: String Theory in a nutshell.

More information

A Brief Introduction to AdS/CFT Correspondence

A Brief Introduction to AdS/CFT Correspondence Department of Physics Universidad de los Andes Bogota, Colombia 2011 Outline of the Talk Outline of the Talk Introduction Outline of the Talk Introduction Motivation Outline of the Talk Introduction Motivation

More information

Putting String Theory to the Test with AdS/CFT

Putting String Theory to the Test with AdS/CFT Putting String Theory to the Test with AdS/CFT Leopoldo A. Pando Zayas University of Iowa Department Colloquium L = 1 4g 2 Ga µνg a µν + j G a µν = µ A a ν ν A a µ + if a bc Ab µa c ν, D µ = µ + it a

More information

Gauge/String Duality and Quark Anti-Quark Potential

Gauge/String Duality and Quark Anti-Quark Potential Gauge/String Duality and Quark Anti-Quark Potential Nelson R. F. Braga, Universidade Federal do Rio de Janeiro Summary Historical facts relating String theory to Strong interactions AdS/CFT, gauge string

More information

String Theory in a Nutshell. Elias Kiritsis

String Theory in a Nutshell. Elias Kiritsis String Theory in a Nutshell Elias Kiritsis P R I N C E T O N U N I V E R S I T Y P R E S S P R I N C E T O N A N D O X F O R D Contents Preface Abbreviations xv xvii Introduction 1 1.1 Prehistory 1 1.2

More information

Gauge/Gravity Duality: An introduction. Johanna Erdmenger. Max Planck Institut für Physik, München

Gauge/Gravity Duality: An introduction. Johanna Erdmenger. Max Planck Institut für Physik, München .. Gauge/Gravity Duality: An introduction Johanna Erdmenger Max Planck Institut für Physik, München 1 Outline I. Foundations 1. String theory 2. Dualities between quantum field theories and gravity theories

More information

Final Exam: Sat. Dec. 18, 2:45-4:45 pm, 1300 Sterling Exam is cumulative, covering all material. From last time

Final Exam: Sat. Dec. 18, 2:45-4:45 pm, 1300 Sterling Exam is cumulative, covering all material. From last time Final Exam: Sat. Dec. 18, 2:45-4:45 pm, 1300 Sterling Exam is cumulative, covering all material From last time Quantum field theory is a relativistic quantum theory of fields and interactions. Fermions

More information

3. Open Strings and D-Branes

3. Open Strings and D-Branes 3. Open Strings and D-Branes In this section we discuss the dynamics of open strings. Clearly their distinguishing feature is the existence of two end points. Our goal is to understand the e ect of these

More information

Gauge/Gravity Duality: Applications to Condensed Matter Physics. Johanna Erdmenger. Julius-Maximilians-Universität Würzburg

Gauge/Gravity Duality: Applications to Condensed Matter Physics. Johanna Erdmenger. Julius-Maximilians-Universität Würzburg Gauge/Gravity Duality: Applications to Condensed Matter Physics. Johanna Erdmenger Julius-Maximilians-Universität Würzburg 1 New Gauge/Gravity Duality group at Würzburg University Permanent members 2 Gauge/Gravity

More information

Outline 1. Introduction 1.1. Historical Overview 1.2. The Theory 2. The Relativistic String 2.1. Set Up 2.2. The Relativistic Point Particle 2.3. The

Outline 1. Introduction 1.1. Historical Overview 1.2. The Theory 2. The Relativistic String 2.1. Set Up 2.2. The Relativistic Point Particle 2.3. The Classical String Theory Proseminar in Theoretical Physics David Reutter ETH Zürich April 15, 2013 Outline 1. Introduction 1.1. Historical Overview 1.2. The Theory 2. The Relativistic String 2.1. Set Up

More information

Supersymmetry, Dark Matter, and Neutrinos

Supersymmetry, Dark Matter, and Neutrinos Supersymmetry, Dark Matter, and Neutrinos The Standard Model and Supersymmetry Dark Matter Neutrino Physics and Astrophysics The Physics of Supersymmetry Gauge Theories Gauge symmetry requires existence

More information

QFT Dimensional Analysis

QFT Dimensional Analysis QFT Dimensional Analysis In the h = c = 1 units, all quantities are measured in units of energy to some power. For example m = p µ = E +1 while x µ = E 1 where m stands for the dimensionality of the mass

More information

Particle Physics. experimental insight. Paula Eerola Division of High Energy Physics 2005 Spring Semester Based on lectures by O. Smirnova spring 2002

Particle Physics. experimental insight. Paula Eerola Division of High Energy Physics 2005 Spring Semester Based on lectures by O. Smirnova spring 2002 experimental insight e + e - W + W - µνqq Paula Eerola Division of High Energy Physics 2005 Spring Semester Based on lectures by O. Smirnova spring 2002 Lund University I. Basic concepts Particle physics

More information

TOPIC VII ADS/CFT DUALITY

TOPIC VII ADS/CFT DUALITY TOPIC VII ADS/CFT DUALITY The conjecture of AdS/CFT duality marked an important step in the development of string theory. Quantum gravity is expected to be a very complicated theory. String theory provides

More information

Hadronic phenomenology from gauge/string duality

Hadronic phenomenology from gauge/string duality Hadronic phenomenology from gauge/string duality Modern Trends in Field Theory, Joã o Pessoa 09/2006 Nelson R. F. Braga, IF, UFRJ String Theory Strong Interactions Experimental observation ( 1960) of an

More information

Light Cone Gauge Quantization of Strings, Dynamics of D-brane and String dualities.

Light Cone Gauge Quantization of Strings, Dynamics of D-brane and String dualities. Light Cone Gauge Quantization of Strings, Dynamics of D-brane and String dualities. Muhammad Ilyas Department of Physics Government College University Lahore, Pakistan Abstract This review aims to show

More information

String Theory I Mock Exam

String Theory I Mock Exam String Theory I Mock Exam Ludwig Maximilians Universität München Prof. Dr. Dieter Lüst 15 th December 2015 16:00 18:00 Name: Student ID no.: E-mail address: Please write down your name and student ID number

More information

Chapter 2: Deriving AdS/CFT

Chapter 2: Deriving AdS/CFT Chapter 8.8/8.87 Holographic Duality Fall 04 Chapter : Deriving AdS/CFT MIT OpenCourseWare Lecture Notes Hong Liu, Fall 04 Lecture 0 In this chapter, we will focus on:. The spectrum of closed and open

More information

Scattering Vector Mesons in D4/D8 model

Scattering Vector Mesons in D4/D8 model Scattering Vector Mesons in D4/D8 model Marcus A. C. Torres C. A. Ballon Bayona H. Boschi-Filho N. Braga Instituto de Física Universidade Federal do Rio de Janeiro Light-Cone 2009: Relativistic Hadronic

More information

Super Yang-Mills Theory in 10+2 dims. Another Step Toward M-theory

Super Yang-Mills Theory in 10+2 dims. Another Step Toward M-theory 1 Super Yang-Mills Theory in 10+2 dims. Another Step Toward M-theory Itzhak Bars University of Southern California Talk at 4 th Sakharov Conference, May 2009 http://physics.usc.edu/~bars/homepage/moscow2009_bars.pdf

More information

Effective Field Theory

Effective Field Theory Effective Field Theory Iain Stewart MIT The 19 th Taiwan Spring School on Particles and Fields April, 2006 Physics compartmentalized Quantum Field Theory String Theory? General Relativity short distance

More information

Planar diagrams in light-cone gauge

Planar diagrams in light-cone gauge Planar diagrams in light-cone gauge M. Kruczenski Purdue University Based on: hep-th/0603202 Summary Introduction Motivation: large-n, D-branes, AdS/CFT, results D-brane interactions: lowest order, light-cone

More information

Strings, gauge theory and gravity. Storrs, Feb. 07

Strings, gauge theory and gravity. Storrs, Feb. 07 Strings, gauge theory and gravity Storrs, Feb. 07 Outline Motivation - why study quantum gravity? Intro to strings Gravity / gauge theory duality Gravity => gauge: Wilson lines, confinement Gauge => gravity:

More information

Théorie des cordes: une introduction Cours I&II: 29 janvier 2010

Théorie des cordes: une introduction Cours I&II: 29 janvier 2010 Particules Élémentaires, Gravitation et Cosmologie Année 2009-10 Théorie des cordes: une introduction Cours I&II: 29 janvier 2010 Les interactions fortes dans les années 60 Introduction et programme du

More information

Quantum Field Theory 2 nd Edition

Quantum Field Theory 2 nd Edition Quantum Field Theory 2 nd Edition FRANZ MANDL and GRAHAM SHAW School of Physics & Astromony, The University of Manchester, Manchester, UK WILEY A John Wiley and Sons, Ltd., Publication Contents Preface

More information

arxiv:hep-ph/ v1 8 Feb 2000

arxiv:hep-ph/ v1 8 Feb 2000 Gravity, Particle Physics and their Unification 1 J. M. Maldacena Department of Physics Harvard University, Cambridge, Massachusetts 02138 arxiv:hep-ph/0002092v1 8 Feb 2000 1 Introduction Our present world

More information

New Phenomena in 2d String Theory

New Phenomena in 2d String Theory New Phenomena in 2d String Theory Nathan Seiberg Rutgers 2005 N.S. hep-th/0502156 J.L. Davis, F. Larsen, N.S. hep-th/0505081, and to appear J. Maldacena, N.S. hep-th/0506141 1 Low Dimensional String Theories

More information

QFT Dimensional Analysis

QFT Dimensional Analysis QFT Dimensional Analysis In h = c = 1 units, all quantities are measured in units of energy to some power. For example m = p µ = E +1 while x µ = E 1 where m stands for the dimensionality of the mass rather

More information

Holographic study of magnetically induced ρ meson condensation

Holographic study of magnetically induced ρ meson condensation Holographic study of magnetically induced ρ meson condensation Nele Callebaut Ghent University November 13, 2012 QCD in strong magnetic fields, Trento Overview 1 Introduction 2 Holographic set-up The Sakai-Sugimoto

More information

Linear Confinement from AdS/QCD. Andreas Karch, University of Washington work with Ami Katz, Dam Son, and Misha Stephanov.

Linear Confinement from AdS/QCD. Andreas Karch, University of Washington work with Ami Katz, Dam Son, and Misha Stephanov. Linear Confinement from AdS/QCD Andreas Karch, University of Washington work with Ami Katz, Dam Son, and Misha Stephanov. Excited Rho Mesons 6 (from PARTICLE DATA BOOK) Experiment 0.933 n 5 m 2 n, GeV

More information

INTRODUCTION TO THE STANDARD MODEL OF PARTICLE PHYSICS

INTRODUCTION TO THE STANDARD MODEL OF PARTICLE PHYSICS INTRODUCTION TO THE STANDARD MODEL OF PARTICLE PHYSICS Class Mechanics My office (for now): Dantziger B Room 121 My Phone: x85200 Office hours: Call ahead, or better yet, email... Even better than office

More information

Introduction to String Theory ETH Zurich, HS11. 9 String Backgrounds

Introduction to String Theory ETH Zurich, HS11. 9 String Backgrounds Introduction to String Theory ETH Zurich, HS11 Chapter 9 Prof. N. Beisert 9 String Backgrounds Have seen that string spectrum contains graviton. Graviton interacts according to laws of General Relativity.

More information

Review: Modular Graph Functions and the string effective action

Review: Modular Graph Functions and the string effective action Review: Modular Graph Functions and the string effective action Jan E. Gerken Max-Planck-Institute for Gravitational Physics Albert-Einstein Institute Potsdam Golm Germany International School of Subnuclear

More information

String Phenomenology ???

String Phenomenology ??? String Phenomenology Andre Lukas Oxford, Theoretical Physics d=11 SUGRA IIB M IIA??? I E x E 8 8 SO(32) Outline A (very) basic introduction to string theory String theory and the real world? Recent work

More information

Dynamics of heavy quarks in charged N = 4 SYM plasma

Dynamics of heavy quarks in charged N = 4 SYM plasma Dynamics of heavy quarks in charged N = 4 SYM plasma Aleksi Vuorinen University of Washington, Seattle & Technical University of Vienna C. Herzog and AV, arxiv:0708:0609 [hep-th] Outline N = 4 SYM and

More information

Lectures on gauge-gravity duality

Lectures on gauge-gravity duality Lectures on gauge-gravity duality Annamaria Sinkovics Department of Applied Mathematics and Theoretical Physics Cambridge University Tihany, 25 August 2009 1. Review of AdS/CFT i. D-branes: open and closed

More information

8.821 String Theory Fall 2008

8.821 String Theory Fall 2008 MIT OpenCourseWare http://ocw.mit.edu 8.821 String Theory Fall 2008 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms. 8.821 F2008 Lecture 03: The decoupling

More information

Symmetries, Groups Theory and Lie Algebras in Physics

Symmetries, Groups Theory and Lie Algebras in Physics Symmetries, Groups Theory and Lie Algebras in Physics M.M. Sheikh-Jabbari Symmetries have been the cornerstone of modern physics in the last century. Symmetries are used to classify solutions to physical

More information

Citation for published version (APA): de Wit, T. C. (2003). Domain-walls and gauged supergravities Groningen: s.n.

Citation for published version (APA): de Wit, T. C. (2003). Domain-walls and gauged supergravities Groningen: s.n. University of Groningen Domain-walls and gauged supergravities de Wit, Tim Cornelis IMPORTANT NOTE: You are advised to consult the publisher's version (publisher's PDF) if you wish to cite from it. Please

More information

Introduction to Particle Physics. HST July 2016 Luis Alvarez Gaume 1

Introduction to Particle Physics. HST July 2016 Luis Alvarez Gaume 1 Introduction to Particle Physics HST July 2016 Luis Alvarez Gaume 1 Basics Particle Physics describes the basic constituents of matter and their interactions It has a deep interplay with cosmology Modern

More information

Non-locality in QFT due to Quantum Effects in Gravity

Non-locality in QFT due to Quantum Effects in Gravity Non-locality in QFT due to Quantum Effects in Gravity Xavier Calmet Physics & Astronomy University of Sussex 1 Effective action for GR How can we describe general relativity quantum mechanically? Well

More information

Fundamental Forces. David Morrissey. Key Concepts, March 15, 2013

Fundamental Forces. David Morrissey. Key Concepts, March 15, 2013 Fundamental Forces David Morrissey Key Concepts, March 15, 2013 Not a fundamental force... Also not a fundamental force... What Do We Mean By Fundamental? Example: Electromagnetism (EM) electric forces

More information

Introduction to AdS/CFT

Introduction to AdS/CFT Introduction to AdS/CFT D-branes Type IIA string theory: Dp-branes p even (0,2,4,6,8) Type IIB string theory: Dp-branes p odd (1,3,5,7,9) 10D Type IIB two parallel D3-branes low-energy effective description:

More information

Coordinate/Field Duality in Gauge Theories: Emergence of Matrix Coordinates

Coordinate/Field Duality in Gauge Theories: Emergence of Matrix Coordinates Coordinate/Field Duality in Gauge Theories: Emergence of Matrix Coordinates Amir H. Fatollahi Department of Physics, Alzahra University, P. O. Box 19938, Tehran 91167, Iran fath@alzahra.ac.ir Abstract

More information

Field Theory: The Past 25 Years

Field Theory: The Past 25 Years Field Theory: The Past 25 Years Nathan Seiberg (IAS) The Future of Physics A celebration of 25 Years of October, 2004 The Nobel Prize in Physics 2004 David J. Gross, H. David Politzer and Frank Wilczek

More information

Lectures on Chiral Perturbation Theory

Lectures on Chiral Perturbation Theory Lectures on Chiral Perturbation Theory I. Foundations II. Lattice Applications III. Baryons IV. Convergence Brian Tiburzi RIKEN BNL Research Center Chiral Perturbation Theory I. Foundations Low-energy

More information

Lecture 9: RR-sector and D-branes

Lecture 9: RR-sector and D-branes Lecture 9: RR-sector and D-branes José D. Edelstein University of Santiago de Compostela STRING THEORY Santiago de Compostela, March 6, 2013 José D. Edelstein (USC) Lecture 9: RR-sector and D-branes 6-mar-2013

More information

An Introduction to Particle Physics

An Introduction to Particle Physics An Introduction to Particle Physics The Universe started with a Big Bang The Universe started with a Big Bang What is our Universe made of? Particle physics aims to understand Elementary (fundamental)

More information

Cosmological Signatures of Brane Inflation

Cosmological Signatures of Brane Inflation March 22, 2008 Milestones in the Evolution of the Universe http://map.gsfc.nasa.gov/m mm.html Information about the Inflationary period The amplitude of the large-scale temperature fluctuations: δ H =

More information

Introduction to Orientifolds.

Introduction to Orientifolds. Introduction to Orientifolds http://www.physto.se/~mberg Overview Orientability in Quantum Field Theory: spinors S R(2π) ψ = ψ Orientability in Quantum Field Theory: spinors (S R(2π) ) 2 ψ =+ ψ S R(2π)

More information

9 Quantum Field Theory for Children

9 Quantum Field Theory for Children 101 9 Quantum Field Theory for Children The theories (known and hypothetical) needed to describe the (very) early universe are quantum field theories (QFT). The fundamental entities of these theories are

More information

Quantum Field Theory. and the Standard Model. !H Cambridge UNIVERSITY PRESS MATTHEW D. SCHWARTZ. Harvard University

Quantum Field Theory. and the Standard Model. !H Cambridge UNIVERSITY PRESS MATTHEW D. SCHWARTZ. Harvard University Quantum Field Theory and the Standard Model MATTHEW D. Harvard University SCHWARTZ!H Cambridge UNIVERSITY PRESS t Contents v Preface page xv Part I Field theory 1 1 Microscopic theory of radiation 3 1.1

More information

QCD Amplitudes Superstrings Quantum Gravity Black holes Gauge/gravity duality

QCD Amplitudes Superstrings Quantum Gravity Black holes Gauge/gravity duality Formal Theory Nick Evans QCD Amplitudes Superstrings Quantum Gravity Black holes Gauge/gravity duality Breaking News The Nobel Prize in Physics 2016 was divided, one half awarded to David J. Thouless,

More information

A New Regulariation of N = 4 Super Yang-Mills Theory

A New Regulariation of N = 4 Super Yang-Mills Theory A New Regulariation of N = 4 Super Yang-Mills Theory Humboldt Universität zu Berlin Institut für Physik 10.07.2009 F. Alday, J. Henn, J. Plefka and T. Schuster, arxiv:0908.0684 Outline 1 Motivation Why

More information

Tachyon Condensation in String Theory and Field Theory

Tachyon Condensation in String Theory and Field Theory Tachyon Condensation in String Theory and Field Theory N.D. Lambert 1 and I. Sachs 2 1 Dept. of Physics and Astronomy Rutgers University Piscataway, NJ 08855 USA nlambert@physics.rutgers.edu 2 School of

More information

Gauge coupling unification without leptoquarks Mikhail Shaposhnikov

Gauge coupling unification without leptoquarks Mikhail Shaposhnikov Gauge coupling unification without leptoquarks Mikhail Shaposhnikov March 9, 2017 Work with Georgios Karananas, 1703.02964 Heidelberg, March 9, 2017 p. 1 Outline Motivation Gauge coupling unification without

More information

Seminar presented at the Workshop on Strongly Coupled QCD: The Confinement Problem Rio de Janeiro UERJ November 2011

Seminar presented at the Workshop on Strongly Coupled QCD: The Confinement Problem Rio de Janeiro UERJ November 2011 and and Seminar presented at the Workshop on Strongly Coupled QCD: The Problem Rio de Janeiro UERJ 28-30 November 2011 Work done in collaboration with: N.R.F. Braga, H. L. Carrion, C. N. Ferreira, C. A.

More information

De la corde hadronique à la gravitation quantique... et retour

De la corde hadronique à la gravitation quantique... et retour Fédération de recherche André Marie Ampère Cours du Collège de France 2011-12 Gabriele Veneziano De la corde hadronique à la gravitation quantique... et retour Cours III : 5 mars 2012 Cordes et gravitation

More information

Effective field theory for axion monodromy inflation

Effective field theory for axion monodromy inflation Effective field theory for axion monodromy inflation Albion Lawrence Brandeis University Based on work in progress with Nemanja Kaloper and L.orenzo Sorbo Outline I. Introduction and motivation II. Scalar

More information

The AdS/CFT correspondence and applications to QCD

The AdS/CFT correspondence and applications to QCD The AdS/CFT correspondence and applications to QCD Philip Fol October 8, 2013 Contents 1 Introduction 1 2 The AdS/CFT correspondence 4 2.1 The concept of a dual theory.......................... 4 2.2 The

More information

Introduction to AdS/CFT

Introduction to AdS/CFT Introduction to AdS/CFT Who? From? Where? When? Nina Miekley University of Würzburg Young Scientists Workshop 2017 July 17, 2017 (Figure by Stan Brodsky) Intuitive motivation What is meant by holography?

More information

Light-Front Quantization Approach to the Gauge/Gravity Correspondence and Strongly Coupled Dynamics

Light-Front Quantization Approach to the Gauge/Gravity Correspondence and Strongly Coupled Dynamics Light-Front Quantization Approach to the Gauge/Gravity Correspondence and Strongly Coupled Dynamics Guy F. de Téramond University of Costa Rica Instituto Tecnológico de Aeronáutica São José dos Campos,

More information

Lecture 8: 1-loop closed string vacuum amplitude

Lecture 8: 1-loop closed string vacuum amplitude Lecture 8: 1-loop closed string vacuum amplitude José D. Edelstein University of Santiago de Compostela STRING THEORY Santiago de Compostela, March 5, 2013 José D. Edelstein (USC) Lecture 8: 1-loop vacuum

More information

A BRIEF TOUR OF STRING THEORY

A BRIEF TOUR OF STRING THEORY A BRIEF TOUR OF STRING THEORY Gautam Mandal VSRP talk May 26, 2011 TIFR. In the beginning... The 20th century revolutions: Special relativity (1905) General Relativity (1915) Quantum Mechanics (1926) metamorphosed

More information

Théorie des Cordes: une Introduction Cours VII: 26 février 2010

Théorie des Cordes: une Introduction Cours VII: 26 février 2010 Particules Élémentaires, Gravitation et Cosmologie Année 2009-10 Théorie des Cordes: une Introduction Cours VII: 26 février 2010 Généralisations de Neveu-Schwarz & Ramond Classical vs. quantum strings

More information

Strings and the Cosmos

Strings and the Cosmos Strings and the Cosmos Yeuk-Kwan Edna Cheung Perimeter Institute for Theoretical Physics University of Science and Technology, China May 27th, 2005 String Theory as a Grand Unifying Theory 60 s: theory

More information

Théorie des cordes: quelques applications. Cours IV: 11 février 2011

Théorie des cordes: quelques applications. Cours IV: 11 février 2011 Particules Élémentaires, Gravitation et Cosmologie Année 2010-11 Théorie des cordes: quelques applications Cours IV: 11 février 2011 Résumé des cours 2009-10: quatrième partie 11 février 2011 G. Veneziano,

More information

Overview. The quest of Particle Physics research is to understand the fundamental particles of nature and their interactions.

Overview. The quest of Particle Physics research is to understand the fundamental particles of nature and their interactions. Overview The quest of Particle Physics research is to understand the fundamental particles of nature and their interactions. Our understanding is about to take a giant leap.. the Large Hadron Collider

More information

Elementary particles and typical scales in high energy physics

Elementary particles and typical scales in high energy physics Elementary particles and typical scales in high energy physics George Jorjadze Free University of Tbilisi Zielona Gora - 23.01.2017 GJ Elementary particles and typical scales in HEP Lecture 1 1/18 Contents

More information

POMERON and AdS/CFT CORRESPONDENCE FOR QCD. Chung-I Tan. Physics Department, Brown University, Providence RI 02912, USA,

POMERON and AdS/CFT CORRESPONDENCE FOR QCD. Chung-I Tan. Physics Department, Brown University, Providence RI 02912, USA, POMERON and AdS/CFT CORRESPONDENCE FOR QCD Chung-I Tan Physics Department, Brown University, Providence RI 02912, USA, E-mail: tan@het.brown.edu The Maldacena conjecture that QCD is holographically dual

More information

e θ 1 4 [σ 1,σ 2 ] = e i θ 2 σ 3

e θ 1 4 [σ 1,σ 2 ] = e i θ 2 σ 3 Fermions Consider the string world sheet. We have bosons X µ (σ,τ) on this world sheet. We will now also put ψ µ (σ,τ) on the world sheet. These fermions are spin objects on the worldsheet. In higher dimensions,

More information

Anomalous Strong Coupling

Anomalous Strong Coupling Simons Center for Geometry and Physics, Stony Brook based on [Brenno Carlini Vallilo, LM, arxiv:1102.1219 [hep-th] ] for a pedagogical review, [LM, arxiv:1104.2604][hep-th] ] XI Workshop on Nonperturbative

More information

Spinning strings and QED

Spinning strings and QED Spinning strings and QED James Edwards Oxford Particles and Fields Seminar January 2015 Based on arxiv:1409.4948 [hep-th] and arxiv:1410.3288 [hep-th] Outline Introduction Various relationships between

More information

Cordes et Branes: des outils pour la cosmologie primordiale. Strings & branes: tools for primordial cosmology. Dan Israël, iap

Cordes et Branes: des outils pour la cosmologie primordiale. Strings & branes: tools for primordial cosmology. Dan Israël, iap Cordes et Branes: des outils pour la cosmologie primordiale Strings & branes: tools for primordial cosmology Dan Israël, iap D. Israël, Strings & branes 1 Preamble Despite its exotic aspects, string theory

More information

Strings, Branes and Extra Dimensions

Strings, Branes and Extra Dimensions arxiv:hep-th/0110055 v3 3 Jan 2002 Strings, Branes and Extra Dimensions Stefan Förste Physikalisches Institut, Universität Bonn Nussallee 12, D-53115 Bonn, Germany Abstract This review is devoted to strings

More information

Quark-gluon plasma from AdS/CFT Correspondence

Quark-gluon plasma from AdS/CFT Correspondence Quark-gluon plasma from AdS/CFT Correspondence Yi-Ming Zhong Graduate Seminar Department of physics and Astronomy SUNY Stony Brook November 1st, 2010 Yi-Ming Zhong (SUNY Stony Brook) QGP from AdS/CFT Correspondence

More information

V Finite T, probe branes, quarks, other extensions

V Finite T, probe branes, quarks, other extensions Introduction to the AdS/CFT correspondence Outline I CFT review II AdS/CFT correspondence III Large N review IV D3 branes and AdS 5 S 5 V Finite T, probe branes, quarks, other extensions 1 0 References

More information

Théorie des cordes: quelques applications. Cours III: 11 février 2011

Théorie des cordes: quelques applications. Cours III: 11 février 2011 Particules Élémentaires, Gravitation et Cosmologie Année 2010-11 Théorie des cordes: quelques applications Cours III: 11 février 2011 Résumé des cours 2009-10: troisième partie 11 février 2011 G. Veneziano,

More information

Speculations on extensions of symmetry and interctions to GUT energies Lecture 16

Speculations on extensions of symmetry and interctions to GUT energies Lecture 16 Speculations on extensions of symmetry and interctions to GUT energies Lecture 16 1 Introduction The use of symmetry, as has previously shown, provides insight to extensions of present physics into physics

More information

Contact interactions in string theory and a reformulation of QED

Contact interactions in string theory and a reformulation of QED Contact interactions in string theory and a reformulation of QED James Edwards QFT Seminar November 2014 Based on arxiv:1409.4948 [hep-th] and arxiv:1410.3288 [hep-th] Outline Introduction Worldline formalism

More information

BEYOND THE SM (II) Kaustubh Agashe (University of Maryland)

BEYOND THE SM (II) Kaustubh Agashe (University of Maryland) BEYOND THE SM (II) Kaustubh Agashe (University of Maryland) ierarchy problems (from lecture 1) Planck-weak hierarchy problem Flavor (hierarchy) puzzle...extra dimensions can address both... Extra dimensions:

More information

Quantum Field Theory. Kerson Huang. Second, Revised, and Enlarged Edition WILEY- VCH. From Operators to Path Integrals

Quantum Field Theory. Kerson Huang. Second, Revised, and Enlarged Edition WILEY- VCH. From Operators to Path Integrals Kerson Huang Quantum Field Theory From Operators to Path Integrals Second, Revised, and Enlarged Edition WILEY- VCH WILEY-VCH Verlag GmbH & Co. KGaA I vh Contents Preface XIII 1 Introducing Quantum Fields

More information

Holographic study of magnetically induced QCD effects:

Holographic study of magnetically induced QCD effects: Holographic study of magnetically induced QCD effects: split between deconfinement and chiral transition, and evidence for rho meson condensation. Nele Callebaut, David Dudal, Henri Verschelde Ghent University

More information