Vacuum SuperString Field Theory I.Ya. Aref'eva Steklov Mathematical Institute Based on : I.A., D. Belov, A.Giryavets, A.Koshelev, hep-th/0112214, hep-th/0201197,

Slides:



Advertisements
Similar presentations
4.1 Introduction to Matrices
Advertisements

Instantons in Deformed Supersymmetric Gauge Theories Shin Sasaki (University of Helsinki) Based on the work [hep-th/ JHEP 07 (2007) 068 ] [hep-th/ ,
Summing planar diagrams
Construction of BPS Solitons via Tachyon Condensation So RIKEN based on the work with T. Asakawa and K. Ohta hep-th/0603***
String Theory A picture book.
The Topological G 2 String Asad Naqvi (University of Amsterdam) (in progress) with Jan de Boer and Assaf Shomer hep-th/0506nnn.
Magnetic Monopoles E.A. Olszewski Outline I. Duality (Bosonization) II. The Maxwell Equations III. The Dirac Monopole (Wu-Yang) IV. Mathematics Primer.
Solitons in Matrix model and DBI action Seiji Terashima (YITP, Kyoto U.) at KEK March 14, 2007 Based on hep-th/ , and hep-th/ ,
Open String Tachyon in Supergravity Solution
Making Precise the Nothing at the Beginning of the Universe Yu Nakayama, hep-th/ (Collaboration with S.J. Rey, Y. Sugawara)
Algebra Recap Solve the following equations (i) 3x + 7 = x (ii) 3x + 1 = 5x – 13 (iii) 3(5x – 2) = 4(3x + 6) (iv) 3(2x + 1) = 2x + 11 (v) 2(x + 2)
Random Matrix Theory Workshop NBIA May 2007 Large N double scaling limits in Gauge Theories and Matrix Models Gaetano Bertoldi Swansea University.
1 Interacting Higher Spins on AdS(D) Mirian Tsulaia University of Crete.
Light-like tachyon condensation in OSFT Martin Schnabl (IAS) Rutgers University, 02/26/2008 Rutgers University, 02/26/2008 Rutgers University, 2008.
Planar diagrams in light-cone gauge hep-th/ M. Kruczenski Purdue University Based on:
Nonlocal Dynamics in String Field Theory and cosmological applications Liudmila Joukovskaya, CTC, DAMTP, University of Cambridge 21 January, Imperial College.
Strings and Black Holes David Lowe Brown University AAPT/APS Joint Fall Meeting.
String Theory Books MBG 60 April 7, Chronology JHS: , Princeton U. MBG: , IAS 1972: JHS to Caltech, MBG to England 1979: Begin collaboration.
Field Theory: The Past 25 Years Nathan Seiberg (IAS) The Future of Physics October, 2004 A celebration of 25 Years of.
Intersections between Open String Field Theory and condensed matter
Thinking Mathematically Algebra: Graphs, Functions and Linear Systems 7.3 Systems of Linear Equations In Two Variables.
Unit 1 Test Review Answers
Charting the OSFT landscape: Boundary state from classical solutions Carlo Maccaferri Torino University (with M. Kudrna and M. Schnabl) & Work.
Irina Arefeva Steklov Mathematical Institute, RAS String Field Theory: from High Energy Physics to Cosmology.
August 6, 2007 基研研究会@近畿大学 1 Comments on Solutions for Nonsingular Currents in Open String Field Theories Isao Kishimoto I. K., Y. Michishita, arXiv:
as holographic description of String Field Theory inspired models
Gaussian Brane and Open String Tachyon Condensation Shinpei Kobayashi ( RESCEU, The University of Tokyo ) Tateyama, Chiba Yoshiaki Himemoto.
x x x < 1or x < 3 x < 3.
GASYUKU2002,Kyoto-U @ KAGA 1 Computing Feynman Graphs in MSFT Isao Kishimoto (Univ. of Tokyo) based on Collaboration with I.Bars and Y.Matsuo [ hep-th/ ]
Brane-Antibrane at Finite Temperature in the Framework of Thermo Field Dynamics Hokkaido Univ. Kenji Hotta.
Minkyoo Kim (Wigner Research Centre for Physics) 9th, September, 2013 Seminar in KIAS.
Surface States Global coordinates Local coordinate Surface state is a bra = lim.
Puzzles with tachyon in SSFT and Cosmological Applications I. Aref'eva Steklov Mathematical Institute, Moscow String Field Theory 2010 Kyoto, Japan
Rolling Tachyon and Vacuum SuperString Field Theory I.Ya. Aref'eva Steklov Mathematical Institute Based on : I.A., D. Belov, A.Giryavets, A.Koshelev,
STRING FIELD THEORY EFFECTIVE ACTION FORTHE TACHYON AND GAUGE FIELDS FOR THE TACHYON AND GAUGE FIELDS secondo incontro del P.R.I.N. “TEORIA DEI CAMPI SUPERSTRINGHE.
1 Superstring vertex operators in type IIB matrix model arXiv: [hep-th], [hep-th] Satoshi Nagaoka (KEK) with Yoshihisa Kitazawa (KEK &
A.Sako S.Kuroki T.Ishikawa Graduate school of Mathematics, Hiroshima University Graduate school of Science, Hiroshima University Higashi-Hiroshima ,Japan.
Holographic cold nuclear matter as dilute instanton gas 1.Introduction 2.Model of Baryon system 3.D8 brane embedding 4.Chemical potential and phase transition.
Creation of D9-brane — anti-D9-brane Pairs from Hagedorn Transition of Closed Strings Hokkaido Univ. Kenji Hotta.
Univ.1 Idempotency Equation and Boundary States in Closed String Field Theory Isao Kishimoto (Univ. of Tokyo → KEK) Collaboration.
Martin Schnabl Institute of Physics, Prague Academy of Sciences of the Czech Republic ICHEP, July 22, 2010.
Notes Over 3.1 Solving a System Graphically Graph the linear system and estimate the solution. Then check the solution algebraically.
EXAMPLE 1 Solve a system graphically Graph the linear system and estimate the solution. Then check the solution algebraically. 4x + y = 8 2x – 3y = 18.
Algebra Review. Systems of Equations Review: Substitution Linear Combination 2 Methods to Solve:
Ramond-Ramond Couplings of D-branes Collaborators: Koji Hashimoto (Osaka Univ.) Seiji Terashima (YITP Kyoto) Sotaro Sugishita (Kyoto Univ.) JHEP1503(2015)077.
ArXiv: (hep-th) Toshiaki Fujimori (Tokyo Institute of Technology) Minoru Eto, Sven Bjarke Gudnason, Kenichi Konishi, Muneto Nitta, Keisuke Ohashi.
Search for Catalysis of Black Holes Formation in Hight Energy Collisions Irina Aref’eva Steklov Mathematical Institute, Moscow Kolomna, QUARKS’2010, June.
ADHM is a Tachyon Condensation --- Stringy Derivation of the ADHM Construction --- Koji Hashimoto (U. of Tokyo, Komaba) 30 Oct Hawaii meeting hep-th/ ,
Martin Schnabl Collaborators: T. Erler, C. Maccaferri, M. Murata, M. Kudrna, Y. Okawa and M. Rapčák Institute of Physics AS CR SPC2013, Sichuan University,
Analytic Results in Open String Field Theory
PHY 745 Group Theory 11-11:50 AM MWF Olin 102 Plan for Lecture 36:
STRING THEORY AND M-THEORY: A Modern Introduction
Tachyon condensation and Vacuum SuperString Field Theory
Vacuum Super String Field Theory
Tachyon vacuum in Schnabl gauge in level truncation
Solve a system of linear equation in two variables
D-branes and KW-dualities in (p,q) minimal superstring theory
Solving Equations with variables on each side
Analytic Solutions in Open String Field Theory
Linear Equations in One Variable and Problem Solving
Algebra II Honors/Gifted
(Cubic SSFT) Super String Field Theory (Lecture II) I.Ya. Aref'eva
Noncommutative Shift Invariant Quantum Field Theory
Solving Systems of Linear and Quadratic Equations
SECTION 2-4 : SOLVING EQUATIONS WITH THE VARIABLE ON BOTH SIDES
Solving Equations 3x+7 –7 13 –7 =.
Theory and applications of Boundary Sine-Gordon Theory
Bellwork 1) Multiply. 3) Find the determinant. 2) Multiply.
Solving Linear Equations
Warm- Up: Solve by Substitution
Presentation transcript:

Vacuum SuperString Field Theory I.Ya. Aref'eva Steklov Mathematical Institute Based on : I.A., D. Belov, A.Giryavets, A.Koshelev, hep-th/ , hep-th/ , hep-th/ , hep-th/ (Lecture III)

OUTLOOK i) New BRST charge ii) Special solutions - sliver, lump, etc.: algebraic; surface states; Moyal representation Vacuum SuperString Field Theory Conclusion

Sen’s conjectures = NO OPEN STRING EXCITATIONS CLOSED STRING EXCITATIONS (?) Our calculations:

NO OPEN STRING EXCITATIONS VSFT

String Field Theory on a non-BPS brane Parity GSO odd + even -

Vacuum String Field Theory on a non-BPS brane I.A., Belov, Giryavets (2002)

Structure of new Q solution to E.O.M SFT in the background field Ohmori

E.O.M. Analog of Noncommutative Soliton in Strong Coupling Limit Gopakumar, Minwalla,Strominger

Methods of solving Algebraic method Surface states method Moyal representation Half-strings Auxiliary linear system

Algebraic Method I.A., Giryavets, Medvedev; Marino, Schiappa Identities for squeezed states Bosonic sliver Rastelli, Sen, Zwiebach; Kostelecky, Potting...

Conformal Sliver Conformal map Comparison with algebraic sliver

Universality of Conformal Sliver Conformal definition of surface states Sliver conformal map Surface states conformal vacuum Sliver projection equation

Open Superstring Star in Diagonal Basis Diagonal basis Three-string vertex in diagonal basis Identity and sliver in diagonal basis Spectrum of identity and sliver I.A.,A.Giryavets hep-th/

Sliver in the Moyal representation Identity Sliver

Twisted SuperSliver Superghost twisted sliver Superghost twisted sliver equation Sliver with insertion Picture changing I.A., Giryavets,Koshelev, hep-th/

Tests Solution to VSFT E.O.M

Conclusion What we know What we have got Open problems

What we know Two sets of basis: SSFT proposes a hard, but a surmountable way to get answers concerning non-perturbative phenomena i) related with spectrum of free string ii) related with "strong coupling “ regime (may be suitable for study VSFT)

What we have got in cubic SSFT Tachyon condensation Rolling tachyon near the top Vacuum SSFT and some solutions

Open Problems More tests for checking validity of VSSFT Other solutions (lump, kink solutions); especially with time dependence Classification of projectors in open string field algebra and its physical meaning Use the Moyal basis to construct the tachyon condensate and other solutions Closed string excitations in VSSFT