Introduction to String Theory & AdS/CFT Justin Frantz Nuclear Lunch 09/09/09 From a non-expert!!!!
Introduction String Theory is not just one theory but has evolved into a both a set of theories set of techniques AdS/CFT is one such sub-theory/technique that has recently found an application to Physics of the Strong Force This week: start w/ general intro to String Theory – Next week discuss AdS/CFT again in more detail…
Forces and General Relativity Four Forces: Electromagnetic,Weak, Strong, Gravity – In fact EM & Weak are currently fully unified as one theory (one force) Both E&M and Gravity follow inverse square laws to good approximation – Current understanding: “accident” First, Gravity is best explained (on large length scales) by General Relativity LHS Curvature of space-time itself (R == Ricci Tensor) RHS Presence of Matter/Energy (T = Energy/Mom Tensor) Form of matter not specified
Standard Model and QCD Standard model particles Hadrons QED-ElectroWeak, QCD: Quantum field theories – Using Perturbation Theory Approximation Strong Force – Quantum ChromoDynamics – Confinement/ Asymptotic Freedom – Low energy QCD Perturbation theory fails: “uncalculable” – Not motivation for String Theory itself but is motivation for use of AdS/CFT Notice that Gravity is absent: – However, SM “proposes” the existence of the mediator graviton which couples w/ all particles – Does not specifiy any details Microscopically includes the what the forces act upon….
Quantum Field Theory/GR Quantum Field Theory – Particles (e.g. electrons) and Forces (via “mediating particles” e.g. photons) treated “equally” as fields – Quantized: 2 electrons -- |2> state (uses creation anniliation operators like for the QM Simple Harmonic Oscillator) – Perturbation Theory: Power Series of more and more complicated transitions (2- >2, + 2->3+ …) sum to “total probability” more complicated less important Because of Uncertainty Principle implied by QM Location fuzzy GR Curvature goes “haywire” – So GR and QFT are not compatible w/ current formulations QED Lagrangian fermion-- 4 spinor dimensions 4 spacial dimensions Photon
String Theory Edward Witten – Intellectual Leader of String Theory – Regarded by some as “Einstein” or our generation – I’ve heard: can do pages and pages of calc’s in his head – “Downloading from the Mothership” Nice simple introduction/presentation at –
String Theory Currently need >= 10 dimensions (9 space 1 time) to fit all SM particles, including new “SuperSymmetric” SUSY particles ~6 different versions of the theory SUSY solves Hierarchy Problem : -Why is Gravity so weak (vs 3 other Forces)? Compactification: why we don’t see the other dimensions M-theory : Witten discovered one 11-D theory which includes others strings branes Duality / Holographic Principle Recent Advancement leading to recent AdS/CFT activity and other things – Like Gauss’ Law or Curl Theorem: – All information in any volume (n-D space) is reflected on the surface of that volume E.g. all interactions reflected on surface as some kind of fluctuation on that surface. – Theory of the volume and theory of the surface same mathematical object
Basic Idea For “AdS/CFT” Certain configuration in Higher Dimensional “AdS” Space dual to a Quantum (Conformal) Field Theory on some surface in that space Some complicated Field theory calculations become simple “geometric’ problems in higher dimensions
Dam Thanh Son Talk: A field theory much like QCD Strongly Coupled Problem: no confinement though
Dam Thanh Son Talk:
Reminder: still just a hypothesis Not proven Why is it useful? At minimum can provide insights about which directions to take field theory calc benefit from the field theory calc…
Results For Heavy Ions, where we think we create a hot plasma of raw QCD fields w/ very low viscosity – e.g. has yielded a conjectured lower bound for the viscosity of ANY quantum fluid that is compatible w/ data…among many other calculations Easy way to calculate energy loss of certain (heavy) quarks in strongly coupled quantum medium – Some predictions that can be tested! Has also been applied to models of hadrons