Self accelerating universe from nonlinear massive gravity Chunshan - - PowerPoint PPT Presentation

self accelerating universe from nonlinear massive gravity
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Self accelerating universe from nonlinear massive gravity Chunshan - - PowerPoint PPT Presentation

Self accelerating universe from nonlinear massive gravity Chunshan Lin Outline Introduction; The nonlinear massive gravity theory Self accelerating solutions in open FRW universe; Conclusion and Discussion Cosmological


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Self–accelerating universe from nonlinear massive gravity

Chunshan Lin

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Outline

Introduction; Self–accelerating solutions in open FRW universe;

Conclusion and Discussion

  • The nonlinear massive gravity theory
  • Cosmological perturbations
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Introduction

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Introduction

Cosmic acceleration

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Introduction

Can we give graviton a mass?

  • Fierz and Pauli 1939
  • Vainshtein 1972 non–linear interactions
  • Boulware–Deser (BD) ghost 1972

van Dam–Veltman–Zakharov discontinuity

Lack of Hamiltonian constrain and momentum constrain 6 degrees of freedom Helicity ±2, ±1, 0 5 dof 6th dof is BD ghost!

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Introduction

Whether there exist a nonlinear model without ghost?

  • N. Arkani–Hamed et al 2002

decoupling limit

  • C. de Rham and G. Gabadadze 2010

Mass terms Boundary

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Introduction

  • C. de Rham, G. Gabadadze and A. Tolly 2011

It is often called fiducial metric

  • Automatically produce the “appropriate coefficients” to eliminate BD ghost

at any order in decoupling limit !

  • Free of BD ghost away from the decoupling limit, at fully nolinear level

Stukelberg fields

Hassan, Rosen ’11

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Self–accelerating solutions

A.Emir Gumrukcuoglu, Chunshan Lin, Shinji Mukohyama arXiv:1109.3845

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Self–accelerating solutions

No go result for flat FRW solution (G. D’Amico et al 2011 Aug.) However… (A.Gumrukcuoglu, C. Lin, S. Mukohyama: 1109.3845) It does not extend to

  • pen FRW universe

The 4 Stukelberg scalars

Minkowski metric Open FRW chart

motivated by…

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Fiducial metric respect FRW symmetry

  • (0i) –components of the equation of motion for are trivially

satisfied;

  • Evolution equations for cosmic perturbations fully respect

homogeneity and isotropy at any order.

Self–accelerating solutions

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Constraint from Stuckelberg scalars:

  • Branch I
  • Branch

Please notice that these 2 solutions do not exist when K=0.

Self–accelerating solutions

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Freedmann equation

Self–accelerating solutions

where The effective cosmological constant

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Self–accelerating solutions

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The nonlinear massive gravity theory For Minkowski fiducial metric, only K<0 FRW solution exists Extensions of the theory with generic fiducial metric Cosmological perturbations

Conclusion and discussion

  • Scalar sector & vector sector
  • Tensor sector

Hassan, Rosen, 11

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