Chern Simons Bose Fermi Duality in the Condensed Phase (Remote Talk) by Shiraz Minwalla
307 views · Published 23 October 2018 · 1:15:26 · Indexed 29 September 2026
Channel: International Centre for Theoretical Sciences · 2018 · Science & Technology
ORGANIZERS : Pallab Basu, Avinash Dhar, Rajesh Gopakumar, R. Loganayagam, Gautam Mandal, Shiraz Minwalla, Suvrat Raju, Sandip Trivedi and Spenta Wadia DATE : 21 May 2018 to 02 June 2018 VENUE : Ramanujan Lecture Hall, ICTS Bangalore In the past twenty years, the discovery of the AdS/CFT correspondence has revolutionized the study of string theory and quantum gravity. The correspondence has also led to the discovery of far-reaching connections between string theory and other seemingly unrelated areas of physics, including the study of strongly correlated condensed matter systems and fluid dynamics. This meeting is a celebration of 20 years of the AdS/CFT correspondence, and will bring together experts in this area to take stock of the progress that has been made, and identify promising directions for future research in this area. The Infosys-ICTS Chandrasekhar Lectures by Juan Maldacena will also be part of this discussion meeting. PROGRAM LINK : https://www.icts.res.in/discussion-meeting/adscft20 Table of Contents (powered by https://videoken.com) 0:00:00 ICTS 0:00:05 AdS/CFT at 20 and beyond ... 0:00:23 Chem Simon Bose Fermi Duality in the Condensed Phase 0:01:51 Based on 0:02:27 Introduction 0:11:03 Intro: The 'standard' Bose Fermi duality Reg Fermions: SU(N)(k-1) + J #D," 0:13:22 Intro: The 'standard' Bose Fermi duality Reg Fermions: SU(N)(k-1) + J &Dad 0:17:25 Intro: How the conjecture was arrived at 0:20:46 Intro: How the conjecture was arrived at Giombi and Yin in 2009: 0:23:45 Intro: Concrete conjecture and its evidence 0:25:01 Intro: Additional Evidence and finite N. 0:26:13 Intro: Massive deformations and phases. 0:32:34 Intro: Matching of Excitations 0:36:44 Intro: Spins of Excitations 0:39:45 Theories 0:40:16 Thermal partition functions at large N 0:42:54 Duality Map Parameter Map KF = -kg, XF = -sgn(g) + B 0:43:02 Setting up the computation 0:46:36 Linearized solutions 0:46:44 Unitary Gauge and bosons 0:47:16 Integrating out and A 0:48:31 Action for singlets Next we introduce two bilocal singlet fields, 0:49:49 Action for singlets Next we introduce two bilocal singlet fields, and a into the 0:50:16 Action in terms of singlets: contd The action is now quadratic in W. 0:51:08 Gap Equations 0:52:01 Gap equations contd 0:55:07 Solution 0:57:22 Soln Contd 0:57:33 Discussion 0:59:03 Though I have not emphasized this in the talk, 1:00:51 As we have explained in the intro,
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