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Euclidean Wilson loops and Riemann theta functions. M. Kruczenski. Purdue University. Based on: arXiv:1104.3567 (w/ R. Ishizeki, S. Ziama). Great Lakes 2011. Summary ● Introduction String / gauge theory duality ( AdS/CFT ) Wilson loops in AdS/CFT
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Euclidean Wilson loops and Riemann theta functions M. Kruczenski Purdue University Based on: arXiv:1104.3567(w/ R. Ishizeki, S. Ziama) Great Lakes 2011
Summary ●Introduction String / gauge theory duality (AdS/CFT) Wilson loops in AdS/CFT Theta functions associated w/ Riemann surfaces Main Properties and some interesting facts.
●Minimal area surfaces in Euclidean AdS3 Equations of motion and Pohlmeyer reduction Theta functions solving e.o.m. (*) Formula for the renormalized area. ● Closed Wilson loops for g=3 Particular solutions, plots, etc. ● Conclusions
AdS/CFT correspondence(Maldacena, GKP, Witten) Gives a precise example of the relation between strings and gauge theory. Gauge theory N = 4 SYM SU(N) on R4 Aμ , Φi, Ψa Operators w/ conf. dim. String theory IIB on AdS5xS5 radius R String states w/ λ large → string th. λ small → field th. fixed
Wilson loops in the AdS/CFT correspondence (Maldacena, Rey, Yee) Euclidean, Wilson loops with constant scalar = Minimal area surfaces in Euclidean AdS3 Closed curves: circularlens-shaped Berenstein Corrado Fischler Maldacena Gross Ooguri, Erickson Semenoff Zarembo Drukker Gross, Pestun Drukker Giombi Ricci Trancanelli
Multiple curves: Drukker Fiol concentric circles Euclidean, open Wilson loops: Maldacena, Rey Yee parallel lines Drukker Gross Ooguri cusp
Many interesting and important results for Wilson loops with non-constant scalar and for Minkowski Wilson loops (lots of recent activity related to light-like cusps and their relation to scattering amplitudes). As shown later, more generic examples for Euclidean Wilson loops can be found using Riemann theta functions. Babich, Bobenko. (our case) Dorey, Vicedo. (Minkowski space-time) Sakai, Satoh. (Minkowski space-time)
Theta functions associated with Riemann surfaces Riemann surface: a2 b2 a1 b2 a2 b1 a3 b1 b3 a1 a3 b3 b1 b3 a1 a3 b2 a2
Holomorphic differentials and period matrix: Theta functions:
Theta functions with characteristics: Simple properties: Symmetry: Periodicity Antisymmetry and
Special functions Algebraic problems: Roots of polynomial in terms of coefficients. Square root: quadratic equations (compass and straight edge or ruler) sin a sin(a/2) [sin a sin(a/3)] Exponential and log: generic roots, allows solutions of cubic and quartic eqns. Theta functions: Solves generic polynomial.
Differential Equations sin, cos, exp: harmonic oscillator (Klein-Gordon). theta functions: sine-Gordon, sinh-Gordon, cosh-Gordon. Trisecant identity:
Derivatives: cosh-Gordon:
Minimal Area surfaces in AdS3 Equations of motion and Pohlmeyer reduction
We can also use: X hermitian can be solved by: Global and gauge symmetries:
The currents: satisfy:
Up to a gauge transformation (rotation) A is given by: Then:
Summary Solve plug it in A, B giving: Solve:
Theta functions solve e.o.m. Hyperelliptic Riemann surface
Example of closed Wilson loop for g=3 Hyperelliptic Riemann surface
Computation of area: Using previous formula Direct computation: Circular Wilson loops , maximal area for fixed length. (Alexakis, Mazzeo)
Map from Wilson loop into the Riemann surface Zeros determine shape of the WL. z can be written as:
Conclusions We argue that there is an infinite parameter family of closed Wilson loops whose dual surfaces can be found analytically. The world-sheet has the topology of a disk and the renormalized area is found as a finite one dimensional contour integral over the world-sheet boundary. We showed specific examples for g=3. Integrability properties of Euclidean Wilson loops deserve further study.