PPT-Gauge Theory duals of Null and Space-like Singularities

Sumit R Das SRD J Michelson K Narayan and S Trivedi PRD 74 2006 026002 SRD J Michelson K Narayan and S Trivedi PRD 74 2007 026002 A Awad SRD K Narayan. and UV Properties. TexPoint. fonts used in EMF. . Read the . TexPoint. manual before you delete this box. .: . A. A. A. A. A. A. A. A. Amplitudes 2011. November . 13, 2011. Zvi. . Bern, . UCLA. ZB, J. J.M. Carrasco, L. Dixon, H. Johansson, and R. . , David Marcos, . Marcello . Dalmonte. , Peter . Zoller. . (. IQOQI, Innsbruck). Brighton, 18.12.2013. Phys. Rev. X 3, 041018 (2013). Experimental input:. Christian . Roos. , Ben Lanyon, Christian . Existence of the Gauge Particles. Gauge transformations are like “rotations”. How do functions transform under “rotations”?. How can we generalize to rotations in “strange” spaces. (. A picture book. Closed strings and SUGRA. Closed string theory in background X . Infinite tower of vibrational modes M. 2. ~ n/. ℓ. s . String interaction through 3-vertex g. s. String length. /. gravity. and . condensed. matter. How string theory might say something about strong coupling. Wilke. van der Schee. June. 24, 2011. Outline. Introduction . AdS. /CFT. Gauge/gravity in general. Conformally. Static Space-Times . Debbie Konkowski (USNA) . & Tom . . Helliwell. . (HMC) . Ae100prg – Prague, Czech Republic – June 25-29, 2012. 1. . Singularities . . a. . Classical . formulation. of . Double. . Field. . Theory. . Quantum . Gravity. in . the. . Southern. . Cone. VI. . Maresias. , . September. 2013. Carmen Núñez. 関係式とその一般化に向けて. (String Advanced Lectures No.22). 高エネルギー加速器研究機構. (KEK). 素粒子原子核研究所. (IPNS). 柴　正太郎. 2010. 年. 7. 月. 5. 日（月） . How string theory might say something about strong coupling. Wilke. van der Schee. June 29, 2011. Outline. Introduction . AdS. /CFT. Sample calculation: drag force. Out of equilibrium dynamics and elliptic flow. Task Priority Redundancy Resolution . for. Real-time Kinematic Control . of. Robot Manipulators. Stefano . Chiaverini. Outline. R. edundancy. Inverse . d. ifferential . k. inematic . c. ontrol . . The matrix . C. has . M. rows and . N. columns, . M. < . N. If we have set this up correctly, the rows of . C. are independent. Nonholonomic (including the pseudo ones) constraints. (If not, do a row reduction and rewrite the constraints) . and UV Properties. TexPoint. fonts used in EMF. . Read the . TexPoint. manual before you delete this box. .: . A. A. A. A. A. A. A. A. Amplitudes 2011. November . 13, 2011. Zvi. . Bern, . UCLA. ZB, J. J.M. Carrasco, L. Dixon, H. Johansson, and R. . Rodney G. Roberts. Anthony . Maciejewski. Presenter: . Karthik. . Sheshadri. Introduction. =J. Solution is of the form. , with JG=I.. For a repeatable strategy, no end effector movement => no joint movement.. Six-Dimensional Supergravity. Gregory Moore. Rutgers University. MIT, May 16, 2018. . DANIEL PARK & SAMUEL MONNIER. . Work in progress with SAMUEL MONNIER. . 2. Quantization Of Anomaly Coefficients. .