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Konstantinos Dimopoulos

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Title: Slide 1 Author: dimopok1 Last modified by: dimopok1 Created Date: 11/8/2006 4:24:57 PM Document presentation format: On-screen Show Company – PowerPoint PPT presentation

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Title: Konstantinos Dimopoulos


1
Cosmological Perturbations
from a Vector Field
Konstantinos Dimopoulos
Lancaster University
2
Scalar vs Vector Fields
  • Scalar fields employed to address many open
    issues inflationary paradigm, dark energy
    (quintessence) baryogenesis (Affleck-Dine)
  • Scalar fields are ubiquitous in theories beyond
    the standard model such as Supersymmetry (scalar
    partners) or string theory (moduli)
  • However, no scalar field has ever been observed
  • Designing models using unobserved scalar fields
    undermines their predictability and
    falsifiability, despite the recent precision data
  • The latest theoretical developments (string
    landscape) offer too much freedom for
    model-building
  • Can we do Cosmology without scalar fields?
  • Some topics are OK

Baryogenesis
, Dark Matter
, Dark Energy (?CDM)
  • Inflationary expansion without scalar fields is
    also possible
  • However, to date, no mechanism for the generation
    of the curvature/density perturbation without a
    scalar field exists

3
Why not Vector Fields?
  • Inflation homogenizes Vector Fields
  • To affect / generate the curvature perturbation a
    Vector Field needs to (nearly) dominate the
    Universe
  • Homogeneous Vector Field in general anisotropic
  • Basic Problem the generatation of a large-scale
    anisotropy is in conflict with CMB observations
  • However, An oscillating massive vector field can
    avoid excessive large-scale anisotropy
  • Also, some weak large-scale anisotropy might be
    present in the CMB (Axis of Evil)

4
Massive Abelian Vector Field
  • To retain isotropy the vector field must not
    drive inflation

Vector Inflation Golovnev et al. (2008) uses
100s of vector fields
5
Vector Curvaton
  • Vector field can be curvaton if safe domination
    of Universe is possible

Pressureless and Isotropic
  • Vector field domination can occur without
    introducing significant anisotropy. The curvature
    perturbation is imposed at domination

6
Particle Production of Vector Fields
  • Breakdown of conformality of massless vector
    field is necessary

Conformal Invariance vector field does not
couple to metric (virtual particles not pulled
outside Horizon during inflation)
7
Particle Production of Vector Fields
  • Cases AB vector curvaton subdominant
    statistical anisotropy only

8
Non-minimally coupled Vector Curvaton
9
Non-minimally coupled Vector Curvaton
  • Longitudinal component
  • The vector curvaton can be the cause of
    statistical anisotropy

saturates observational bound
10
Statistical Anisotropy and non-Gaussianity
  • Non Gaussianity in vector curvaton scenario
  • Non-Gaussianity correlated with statistical
    anisotropy

Smoking gun
11
Conclusions
  • A vector field can contribute to the curvature
    perturbation
  • In this case, the vector field undergoes rapid
    harmonic oscillations during which it acts as a
    pressureless isotropic fluid
  • Hence, when the oscillating vector field
    dominates, it introduces negligible anisotropy
    (Axis of Evil?)
  • If particle production is isotropic then the
    vector curvaton can alone generate the curvature
    perturbation in the Universe
  • If particle production is anisotropic then the
    vector curvaton can give rise to statistical
    anisotropy, potentially observable by Planck
  • Correlation of statistical anisotropy and
    non-Gaussianity in the CMB is the smoking gun for
    the vector curvaton scenario
  • The challenge is to obtain candidates in theories
    beyond the standard model, which can play the
    role of the vector curvaton

Physical Review D 74 (2006) 083502
hep-ph/0607229
arXiv0806.4680 hep-ph
Physical Review D 76 (2007) 063506 0705.3334
hep-ph
arXiv0809.1055 astro-ph
Journal of High Energy Physics 07 (2008) 119
0803.3041 hep-th
arXiv0812.0264 astro-ph
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