Theoretical Aspects of Dark Energy Models Rong-Gen Cai Institute of Theoretical Physics Chinese Academy of Sciences CCAST, July 4, 2005.

Slides:



Advertisements
Similar presentations
Theories of gravity in 5D brane-world scenarios
Advertisements

Massive Gravity and the Galileon Claudia de Rham Université de Genève Work with Gregory Gabadadze, Lavinia Heisenberg, David Pirtskhalava and Andrew Tolley.
BRANE SOLUTIONS AND RG FLOW UNIVERSIDADE FEDERAL DE CAMPINA GRANDE September 2006 FRANCISCO A. BRITO.
Dark Energy. Conclusions from Hubble’s Law The universe is expanding Space itself is expanding Galaxies are held together by gravity on “small” distance.
P ROBING SIGNATURES OF MODIFIED GRAVITY MODELS OF DARK ENERGY Shinji Tsujikawa (Tokyo University of Science)
Dark Energy and Extended Gravity theories Francesca Perrotta (SISSA, Trieste)
University of Texas at San Antonio Arthur Lue Dark Energy or Modified Gravity?
L. Perivolaropoulos Department of Physics University of Ioannina Open page.
Quintessence and the Accelerating Universe
José Beltrán and A. L. Maroto Dpto. Física teórica I, Universidad Complutense de Madrid XXXI Reunión Bienal de Física Granada, 11 de Septiembre de 2007.
Dark energy II : Models of dark energy Shinji Tsujikawa (Tokyo University of Science)
Physical Constraints on Gauss-Bonnet Dark Energy Cosmologies Ishwaree Neupane University of Canterbury, NZ University of Canterbury, NZ DARK 2007, Sydney.
Dark Energy Perturbations 李明哲 南京大学物理学院 中国科技大学交叉学科理论研究中心 合肥.
Quintessence – Phenomenology. How can quintessence be distinguished from a cosmological constant ?
COSMO 2006, Lake Tahoe 9/28/2006 Cuscuton Cosmology: Cuscuton Cosmology: Dark Energy meets Modified Gravity Niayesh Afshordi Institute for Theory and Computation.
Bright High z SnIa: A Challenge for LCDM? Arman Shafieloo Particle Physics Seminar, 17 th February 09 Oxford Theoretical Physics Based on arXiv:
Dark Energy from Backreaction Thomas Buchert Thomas Buchert LMU-ASC Munich, Germany LMU-ASC Munich, Germany Toshifumi Futamase (Sendai, Japan): Averaging.
L. Perivolaropoulos Department of Physics University of Ioannina Open page.
Bin Wang (王斌) Fudan University WHAT COULD w BE?. Outline Dark energy: Discords of Concordance Cosmology What is w? Could we imagine w
Near-Horizon Solution to DGP Perturbations Ignacy Sawicki, Yong-Seon Song, Wayne Hu University of Chicago astro-ph/ astro-ph/
1 f(R) Gravity and its relation to the interaction between DE and DM Bin Wang Shanghai Jiao Tong University.
Chaplygin gas in decelerating DGP gravity Matts Roos University of Helsinki Department of Physics and and Department of Astronomy 43rd Rencontres de Moriond,
Emergent Universe Scenario
Large distance modification of gravity and dark energy
Dark Energy and Modified Gravity IGC Penn State May 2008 Roy Maartens ICG Portsmouth R Caldwell.
Modified (dark) gravity Roy Maartens, Portsmouth or Dark Gravity?
BRANEWORLD COSMOLOGICAL PERTURBATIONS
1 Edmund Bertschinger MIT Department of Physics and Kavli Institute for Astrophysics and Space Research Testing Gravity on Large Scales Dekel 1994 Ann.
Cascading gravity and de gravitation Claudia de Rham Perimeter Institute/McMaster Miami 2008 Dec, 18 th 2008.
Lecture 3: Modified matter models of dark energy Shinji Tsujikawa (Tokyo University of Science)
Dilaton quantum gravity and cosmology. Dilaton quantum gravity Functional renormalization flow, with truncation :
Dark Energy & High-Energy Physics Jérôme Martin Institut d’Astrophysique de Paris.
Dark Energy The first Surprise in the era of precision cosmology?
Ilya Gurwich and Aharon Davidson Physics department Ben-Gurion University 1 Radiation Driven Inflation - Ilya Gurwich Aharon Davidson and I.G., JCAP06(2008)01.
Effective Action for Gravity and Dark Energy Sang Pyo Kim Kunsan Nat’l Univ. COSMO/Co sPA, Sept. 30, 2010 U. Tokyo.
Some Remarks on Dark Energy Rong-Gen Cai Institute of Theoretical Physics Chinese Academy of Sciences ( Huangshan, April 9, 2011)
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)
Dilaton quantum gravity and cosmology. Dilaton quantum gravity Functional renormalization flow, with truncation :
Inflationary Attractor Zong-Kuan Guo (advisor: Yuan-Zhong Zhang) Institute of Theoretical Physics, Chinese Academy of Sciences, P.O. Box 2735, Beijing.
DARK ENERGY PARTICLE PHYSICS PROBLEMS STEEN HANNESTAD UNIVERSITY OF AARHUS NBI, 27 AUGUST 2007.
Dark Energy and Modified Gravity Shinji Tsujikawa (Gunma National College of Technology ) Collaborations with L. Amendola, S. Capozziello, R. Gannouji,
Big bang or freeze ?. conclusions Big bang singularity is artefact Big bang singularity is artefact of inappropriate choice of field variables – of inappropriate.
Michael Doran Institute for Theoretical Physics Universität Heidelberg Time Evolution of Dark Energy (if any …)
Dark energy from various approaches Archan S. Majumdar S. N. Bose National Centre for Basic Sciences BSM, Quy nhon, vietnam.
Some Remarks on Dark Energy Rong-Gen Cai Institute of Theoretical Physics Chinese Academy of Sciences ( Nov.6, 2010)
Recent Progress on Dark Energy Study Xinmin Zhang IHEP
Big bang or freeze ?. conclusions Big bang singularity is artefact Big bang singularity is artefact of inappropriate choice of field variables – of inappropriate.
ERE 2008September 15-19, Spanish Relativity Meeting 2008, Salamanca, September (2008) Avoiding the DARK ENERGY coincidence problem with a COSMIC.
Holographic Dark Energy and Anthropic Principle Qing-Guo Huang Interdisciplinary Center of Theoretical Studies CAS
Theory Department, Lebedev Physics Institute, Moscow
Dark Energy in the Early Universe Joel Weller arXiv:gr-qc/
Interaction between dark energy and dark matter Bin Wang Shanghai JiaotongUniversity.
Understanding the Dark Energy From Holography
Quintessence Dark Energy & Acceleration of the Universe B URIN G UMJUDPAI The Tah Poe Academia Institute for Theoretical Physics & Cosmology Department.
Determination of cosmological parameters Gong-Bo Zhao, Jun-Qing Xia, Bo Feng, Hong Li Xinmin Zhang IHEP, Beijing
THE DARK SIDE OF THE UNIVERSE Amna Ali Saha Institute of Nuclear Physics Kolkata, India 9/07/2012 LPNHE,PARIS.
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,
Causality Problem in Holographic Dark Energy Hyeong-Chan Kim Korea National University of Transportation, with Jungjai Lee (Daejin U.) and Jae-Weon Lee.
Cosmology in a brane-induced gravity model with trace-anomaly terms
Phantom Dark Energy Zong-Kuan Guo (advisor: Yuan-Zhong Zhang)
INDUCED COSMOLOGY ON A CODIMENSION-2 BRANE IN A CONICAL BULK
``Welcome to the dark side of the world.”
Recent status of dark energy and beyond
Overview of Dark Energy Theory
The Cosmological Constant Problem & Self-tuning Mechanism
Centre for Theoretical Physics Jamia Millia University New Delhi
Stealth Acceleration and Modified Gravity
43rd Rencontres de Moriond La Thuile (Val d'Aosta, Italy)
Cosmological Scaling Solutions
Presentation transcript:

Theoretical Aspects of Dark Energy Models Rong-Gen Cai Institute of Theoretical Physics Chinese Academy of Sciences CCAST, July 4, 2005

Cosmic Acceleration? Dynamics equations: (Violate the Strong Energy Condition: exotic energy component)

Dark Energy? Observation Data Theoretical Assumptions General RelativityCosmo Principle Model IModel II Model III

Model I: Modifications of Gravitational Theory 1) GR’s test UV: ~ 1 mm IR: ~ solar scale 2) Modify GR UV: quantum gravity effect IR: cosmos scale Brane World Scenario

Modifying GR in IR: 1)“ Ghost Condensation and a Consistent Infrared Modification of Gravity” by N. arkani-Hamed et al, hep-th/ ,JHEP 0405 (2004) 074.

Consider a ghost field with a wrong-sign kinetic term:

Suppose the scalar field has a constant velocity: The low-energy effective action for the fluctuation has an usual form:

2) “ Is Cosmic Speed-up due to New Gravitational Physics ” by S. M. Carroll et al. astro-ph/ , Phys.Rev. D70 (2004) Consider a modification becoming important at extremely low curvature

Making a conformal transformation yields a scalar field with potential: (1) Eternal de Sitter; (2) power-law acceleration; (3) future singularity

General case:

More general case: hep-th/ , PR D71:063513,2005 Consider:

3) Brane World Scenario: y 1) N. Arkani-Hamed et al, 1998 factorizable product 2) L. Randall and R. Sundrum, 1999 warped product in AdS_5 RS1: RS2: 3) DGP model, 2000 a brane embedded in a Minkovski space

a) A popular model: RS scenario where = 0 Fine-Tuning

2) “Dark Energy” on the brane world scenario “Braneworld models of dark energy” by V. Sahni and Y. Shtanov, astro-ph/ , JCAP 0311 (2003) 014 When m=0:

In general they have two branches:

Current value of the effective equation of state of “dark energy”

The acceleration can be a transient phenomenon: Brane 2

However, w crosses –1, the phantom divide? D. Huterer and A. Cooray, astro-ph/040462; Phys.Rev. D71 (2005)

“Crossing w=-1 in Gauss-Bonnet Brane World with Induced Gravity ” by R.G. Cai,H.S. Zhang and A. Wang, hep-th/ Consider the model

The equations of motion:

The effective equation of state of “dark energy”: Where the Gauss-Bonnet term in the bulk and bulk mass play a curial role.

Model III: Back Reaction of Fluctuations “Cosmological influence of super-Hubble perturbations” by E.W. Kolb, S. Matarrese, A. Notari and A. Riotto, astro-ph/ ; “Primordial inflation explains why the universe is accelerating today” by E.W. Kolb, S. Matarrese, A. Notari and A. Riotto, hep-th// ; “On cosmic acceleration without dark energy” by E.W. Kolb, S. Matarrese, and A. Riotto, astro-ph/

Inflation produces super-horizon perturbations!

Consider the presence of cosmic perturbations, Split the gravitational potential to two parts

A local observer within the Hubble volume will see cosmological constant

which indicates the SHCDM with is indistinguishable from LCDM model.

Another scenario:

Beyond the super-horizon mode’s cut-off, the bulk universe is There is a super-horizon sized underdense bubble containing the observable universe, with matter density equal to the average matter density we measure locally

Model II: Various Dark Energy Models: Acts as Source of E’eq (1)Cosmological constant: w=-1 (2) Holographic energy (3) Quintessence: -1<w<0 (4) K-essence: -1 <w<0 (5) Chaplygin gas: p=- A/rho (6) Phantom: w<-1 (7) Quintom (8) Chameleon, K-Chameleon various generalization and mixture……..

QFT, a very successful theory (1) a very tiny positive cosmological constant ? Variable cosmological constant? Interaction?

(2) Holographic Energy? E,S V,A R i) Bekenstein Bound: ii) Holographic Bound: iii) UV/IR Mixture: (Cohen et al, Hsu, Li….)

(3) Quintessence: a very slowly varying scalar field? Tracker Potential: (4) K-essence (Born-Infeld Scalar Field):

(5) Chaplygin gas ? Generalizations:

(6) Phantom (Caldwell, 1999) -1<w<0, if s=1 w<-1, if s=-1

(7) Quintom: normal scalar field plus phantom field W cross the phantom divide, w=-1 (8) Chameleon, K-Chameleon Hessence ?

Acceleration Deceleration Distance between galaxies Time (Age of universe) Beginning Now (13.7 billion years) Inflation (acceleration) Closed, rho<0 Acc.(-1 <w<-1/3) Super Acc. (w<-1) ? Expand, but w>0 The fate of our universe depends on the nature of dark energy, not only the geometry Radiation + dust) (dark energy dominated)

Thanks!