Slide 1NP-complete Problems and Physical Reality Scott Aaronson Institute for Advanced Study Slide 2 What could we do if we could solve NP-complete problems? Proof of Riemann…

ar X iv :h ep -th /9 81 02 40 v5 2 8 Fe b 20 01 IFT-UAM/CSIC-98-2 String Primer Enrique Alvarez∗ and Patrick Meessen† Instituto de F´ısica Teo´rica, C-XVI Universidad…

Slide 1 A Matrix Model for Black Hole Thermalization Joseph Polchinski Kavli Institute for Theoretical Physics University of California at Santa Barbara N. Iizuka & JP,…

Slide 1 Spectrum of CHL Dyons (I) Tata Institute of Fundamental Research First Asian Winter School Seoul Atish Dabholkar Slide 2 Motivation Exact BPS spectrum gives valuable…

Slide 1 Anisotropic holography and the microscopic entropy of Lifshitz black holes in 3D of Lifshitz black holes in 3D Ricardo Troncoso Ricardo Troncoso In collaboration…

Slide 1 Hyeong-Chan Kim* (Yonsei Univ. Korea) Jae-Weon Lee (KIAS Korea), Jungjai Lee (Daejin Univ. Korea), KITPC “String Theory and Cosmology” 2007, Oct. 10 Based on…

A Matrix Model for Black Hole Thermalization Joseph Polchinski Kavli Institute for Theoretical Physics University of California at Santa Barbara N. Iizuka & JP, arXiv…

Cosmological Constant Problem: Rethinking Quantum & Gravity Missing Baryons!! Gonzalez, Zaritsky, & Zabludoff 2007 NA, Lin, Nagai, & Sanderson 2007 27% § 8%…

Gauge/Gravity Duality Joseph Polchinski From Black Holes and the Quark Gluon Plasma to Condensed Matter Physics and the Big Bang Which of these interactions doesnât belong?…