Nonlocal Dynamics in String Field Theory and cosmological applications Liudmila Joukovskaya, CTC, DAMTP, University of Cambridge 21 January, Imperial College.

Slides:



Advertisements
Similar presentations
The Nuts and Bolts of Inflation Richard Barrett. Dark Energy SeminarGlasgow 29/11/2003 Inflation What is inflation? What is dark energy? Why was inflation.
Advertisements

Quantum Field Theory for Gravity and Dark Energy Sang Pyo Kim Kunsan Nat’l Univ. & APCTP Co sPA2009, U. Melbourne, 2009.
Brane-World Inflation
Testing CPT with CMB 李明哲 University of Bielefeld 2008 年 4 月 28 日.
Intersecting membrane and an anisotropic models of dark energy Dmitry G. Orlov (NCU, Taiwan; VNIIMS, Russia) 1st June, 2008NDHU, Taiwan.
Observed Features of the Universe Universe is homogeneous and isotropic on lengths > 100 Mpc Universe expanding uniformly ordinary matter is more abundant.
Miami Miami 2012 Tirtho Biswas Stringy Nonlocal Theories.
Neutrino Mass due to Quintessence and Accelerating Universe Gennady Y. Chitov Laurentian University, Canada.
Physics 133: Extragalactic Astronomy ad Cosmology Lecture 5; January
Cosmic challenges for fundamental physics Diederik Roest December 9, 2009 Symposium “The Quantum Universe”
Physical Constraints on Gauss-Bonnet Dark Energy Cosmologies Ishwaree Neupane University of Canterbury, NZ University of Canterbury, NZ DARK 2007, Sydney.
The Statistically Anisotropic Curvature Perturbation from Vector Fields Mindaugas Karčiauskas Dimopoulos, MK, JHEP 07 (2008) Dimopoulos, MK, Lyth, Rodriguez,
Lecture 1: Basics of dark energy Shinji Tsujikawa (Tokyo University of Science) ``Welcome to the dark side of the world.”
Analytical and numerical aspects of tachyonic inflation Goran S. Djordjević SEEMET-MTP Office & Department of Physics, Faculty of Science and Mathematics.
Based on Phys.Rev.D84:043515,2011,arXiv: &JCAP01(2012)016 Phys.Rev.D84:043515,2011,arXiv: &JCAP01(2012)016.
THE GRACEFUL EXIT FROM INFLATION AND DARK ENERGY By Tomislav Prokopec Publications: Tomas Janssen and T. Prokopec, arXiv: ; Tomas Janssen, Shun-Pei.
Dynamical solutions in intersecting brane systems Kunihito Uzawa Osaka City University Advanced Mathematical Institute.
Emergent Universe Scenario
BRANEWORLD COSMOLOGICAL PERTURBATIONS
Qing-Guo Huang based on arXiv: (to appear in PLB) done with F.L.Lin Institute of High Energy Physics, CAS State Key Laboratory of Theoretical.
Lecture 3: Modified matter models of dark energy Shinji Tsujikawa (Tokyo University of Science)
Cosmology, Inflation & Compact Extra Dimensions Chad A. Middleton Mesa State College March 1, 2007 Keith Andrew and Brett Bolen, Western Kentucky University.
Dark Energy & High-Energy Physics Jérôme Martin Institut d’Astrophysique de Paris.
Quintom Bounce with a Galileon Model Chung-Yuan Christian University, Taiwan & Institute of High Energy Physics, Beijing Based on Collaborated.
1 Parametric resonance with Multi-frequencies in preheating José Pedro Mimoso University of Lisboa Collaboration with: Ana Nunes Tiago Charters ERE08 –Salamanca:
Stabilizing moduli with flux in brane gas cosmology Jin Young Kim (Kunsan National Univ.) CosPA 2009, Melbourne Based on arXiv: [hep-th]; PRD 78,
Yugo Abe (Shinshu University) July 10, 2015 In collaboration with T. Inami (NTU), Y. Kawamura (Shinshu U), Y. Koyama (NCTS) YA, T. Inami,
Adventures in Superspace McGill University, 2013 Tirtho Biswas Towards Consistent Nonlocal Theories of Gravity.
Dark energy: the greatest mystery of the universe Syksy Räsänen Department of Physics and Helsinki Institute of Physics Arkadia.
Notes on Real and p-Adic Inflation Spring School on Strings, Cosmology and Particles SSSCP2009 Nis, 4 April 2009 Goran S. Djordjević In Collaboration with.
Irina Arefeva Steklov Mathematical Institute, RAS String Field Theory: from High Energy Physics to Cosmology.
Quintom Cosmology Tao-Tao Qiu & Yi-Fu Cai, IHEP (邱涛涛、蔡一夫, 中科院高能所) ( “ 精灵 ” 宇宙学)
P-adic Strings: Thermal Duality & the Cosmological Constant Tirthabir Biswas Loyola University, New Orleans PRL 104, (2010) JHEP 1010:048, (2010)
The physics of inflation and dark energy 1.3 Dark energy: some evidence (short list) Ages of glob. clusters/galaxies at z~2-3:  m 0.6 SN Ia:   -
Inflationary Attractor Zong-Kuan Guo (advisor: Yuan-Zhong Zhang) Institute of Theoretical Physics, Chinese Academy of Sciences, P.O. Box 2735, Beijing.
Thermodynamics of Apparent Horizon & Dynamics of FRW Spacetime Rong-Gen Cai (蔡荣根) Institute of Theoretical Physics Chinese Academy of Sciences.
as holographic description of String Field Theory inspired models
Extranatural Inflation Nuno M. C. Santos CFTP - IST Centro de Física Teórica de Partículas Instituto Superior Técnico - Universidade Técnica de Lisboa.
Cosmology and Tachyonic Inflation on Non-Archimedean Spaces Goran S. Djordjević SEEMET-MTP Office & Department of Physics, Faculty of Science and Mathematics.
Derivation of the Friedmann Equations The universe is homogenous and isotropic  ds 2 = -dt 2 + a 2 (t) [ dr 2 /(1-kr 2 ) + r 2 (dθ 2 + sinθ d ɸ 2 )] where.
The false vacuum bubble : - formation and evolution - in collaboration with Bum-Hoon Lee, Chul H. Lee, Siyong Nam, and Chanyong Park Based on PRD74,
Tachyon-Dilaton driven Inflation as an α'-non perturbative solution in first quantized String Cosmology Anna Kostouki, King’s College London DISCRETE ’08,
Brane Gravity and Cosmological Constant Tetsuya Shiromizu Tokyo Institute of Technology Tokyo Institute of Technology 白水 White Water.
Cosmological Perturbations in the brane worlds Kazuya Koyama Tokyo University JSPS PD fellow.
Interaction between dark energy and dark matter Bin Wang Shanghai Jiao TongUniversity collaborated with Elcio Abdalla.
Bin Wang Fudan University Shanghai Signature on the interaction between dark energy and dark matter.
Anisotropic Evolution of D-Dimensional FRW Spacetime
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/ ,
Surface States Global coordinates Local coordinate Surface state is a bra = lim.
The dark side of the Universe: dark energy and dark matter Harutyun Khachatryan Center for Cosmology and Astrophysics.
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,
Role of Backreaction in an accelerating universe Archan S. Majumdar S. N. Bose National Centre for Basic Sciences Kolkata.
Holographic Dark Energy and Anthropic Principle Qing-Guo Huang Interdisciplinary Center of Theoretical Studies CAS
Cosmological evolution of regularized branes in 6D warped flux compactifications Masato Minamitsuji (ASC, LMU, Munich) With David Langlois (APC, Paris)
Interaction between dark energy and dark matter Bin Wang Shanghai JiaotongUniversity.
Quintessence Dark Energy & Acceleration of the Universe B URIN G UMJUDPAI The Tah Poe Academia Institute for Theoretical Physics & Cosmology Department.
Gravity effects to the Vacuum Bubbles Based on PRD74, (2006), PRD75, (2007), PRD77, (2008), arXiv: [hep-th] & works in preparation.
On the Lagrangian theory of cosmological density perturbations Isolo di San Servolo, Venice Aug 30, 2007 V. Strokov Astro Space Center of the P.N. Lebedev.
In Dynamic Dark Energy Models. 1. Accelerating expansion & interpretation 2. What is Dynamic dark energy model 3. recent observational results.
Spherical Collapse and the Mass Function – Chameleon Dark Energy Stephen Appleby, APCTP-TUS dark energy workshop 5 th June, 2014 M. Kopp, S.A.A, I. Achitouv,
FAILURES OF HOMOGENEOUS & ISOTROPIC COSMOLOGIES IN EXTENDED QUASI-DILATON MASSIVE GRAVITY (arXiv: ) Saurabh Kumar, Department of Physics, Case.
Vacuum Super String Field Theory
Recent status of dark energy and beyond
Conclusion of Last Class: Hubble’s Law (that far away galaxies recede faster) implies that the universe is expanding uniformly in all directions, like.
Notes on non-minimally derivative coupling
Lecture 41 – Cosmology- Final Remarks
(Cubic SSFT) Super String Field Theory (Lecture II) I.Ya. Aref'eva
Dynamics in Nonlocal Cosmological Models
6D Standing Wave Braneworld
Presentation transcript:

Nonlocal Dynamics in String Field Theory and cosmological applications Liudmila Joukovskaya, CTC, DAMTP, University of Cambridge 21 January, Imperial College London

Plan of the talk General Motivations Construction of rolling solutions in the truncated SFT a) Truncated SFT (nonlocality) b) Space homogeneous rolling solutions Cosmological motivations for nonlocal theories SFT as a possible framework for cosmology Rolling cosmological solutions

Motivations Cosmological Motivations Theoretical Motivations String Field Theory as a possible framework for Cosmology

Cubic Fermionic String Field Theory Witten’s Cubic Open String Field Theory I.Aref’eva, P.Medvedev, A.Zubarev Phys.Lett. B240 (1990)356 C.Preitschopf, C.Thorn, S.Yost, Nucl. Phys. B337 (1990) 363 I.Arefeva, D.Belov, A.Koshelev, P.Medvedev, Nucl.Phys.B638 (2002)3 E. Witten, Nucl. Phys. B 268 (1986) 253 V.A. Kostelecky, S.Samuel, Phys. Lett. B 207 (1988) 169 V.A. Kostelecky,S.Samuel, Phys. Lett. B 207 (1988) 169, P.West, Phys.Lett.B548:92-96,2002 N. Moeller, A. Sen, B. Zwiebach, JHEP, 08 (2000) 039

In the approximation u=U we have a more simple approximate action

Covariant String Field Theory Level truncation

Spatially-Homogeneous Configurations

Stress Tensor N. Moeller, B. Zwiebach, JHEP, 10 (2002) 034 H. Yang, JHEP 11 (2002) 007 I. Aref’eva, L.J., A. Koshelev, JHEP, 09 (2003) 012

Intuition about possible solutions

Solution construction for Minkowski case Ya. Volovich, JPA, 2003; Ya. Volovich, V.S. Vladimirov, Theor. Math. Phys. 2004; L.J., Theor. Math. Phys or arxiv: [hep-th]; V.S. Vladimirov, arxiv: D. V. Prokhorenko, math-ph/ ; G. Calcagni, G. Nardelli, arxiv:

Solution of Equation of Motion

Standard Cosmological Concordance Model is emerging during the last 10 years …

Big Bang/Inflationary Cosmology Picture taken from: cosmology.berkeley.edu

Cyclic/Ekpyrotic Cosmology N. Turok, P.J. Steinhardt, J. Khoury, B. Ovrut

A great discovery of the last few years is the discovery of the current accelerated expansion of the Universe Observations (1998) of very distant supernovae demonstrated that the Universe is expanding with an acceleration. Ia Supernovae: S.Perlmutter et al., A.Riess et al., 1998; This acceleration seems to be explicable by the presence of a new component of matter called dark energy (DE). DE is a special unknown form of matter with negative pressure and it provides universal repulsive forces (antigravity).

Picture taken from: map.gsfc.nasa.gov

One more reason to work on new inflationary candidates

String Field Theory as a possible cosmological framework Standard Cosmological Concordance Model is emerging during the last 10 years…

Non-locality and Cosmology Non-local gravity ad-hoc: Non-local SFT: Arkani-Hamed at al hep-th/ ; Khoury, hep-th/ ; T.Biswas, A.Mazumdar, W.Siegel, hep-th/ , G.Dvali, S. Hofmann, JKhoury, hep-th/ G.Dvali, S. Hofmann, J Khoury, hep-th/ S.Deser, R.Woodard, arXiv S. S.Deser, R.Woodard, arXiv: S. I.Aref’eva, LJ, A.Koshelev, JHEP, 2003; I.Aref’eva, LJ, JHEP, 2005 G.Calcagni, JHEP, 2005 LJ, PRD 2007 G. Calcagni, M.Montobbio, G.Nardelli; PRD 2007 N. Barnaby, T. Biswas, J.M. Cline, JHEP 2007 J.Lidsey, PRD 2007; D. Mulryne, N. Nunes, PRD 2008

Friedmann Cosmology Einstein equations + Cosmological principle Homogeneous Isotropic K=+1 (3-sphere), k=0 (plane), k=-1 (3-hyperboloid)

Intuition about possible solutions

L.J., PRD 2007

Two fields case

Second possibility

Numerical Scheme for Solution Construction II

Numerical Scheme for Solution Construction II - continuation

Numerical Solution

Does exist the rolling tachyon solution in the case of cubic potential?

Coupling to the gravity / FRW case

Do we have the rolling tachyon solution in this case?

L.J., arxiv:

Numerical solutions a. b.

Energy and pressure for Rolling Tachyon Solutions a. b.

Main results presented in this talk: Construction of rolling cosmological solutions for: Tachyon field describing non-BPS branes in Friedmann-Robertson-Walker background ( Does exist in Minkowski case AJK ) Tachyon field of open bosonic string in Friedmann-Robertson-Walker background ( Does not exist in the Minkowski case (Moeller, Zwiebach) )

Conclusions and further directions

Thank you for the attention!