Discrete Chebyshev polynomials: Difference between revisions

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'''Non-minimally coupled inflation''' is an [[cosmic inflation|inflationary]] model in which the constant which couples [[gravity]] to the [[inflaton field]] is not small. The [[coupling constant]] is usually represented by <math>\xi</math> ([[Xi (letter)|Xi]]), which features in the [[action (physics)|action]] (constructed by modifying the [[Einstein-Hilbert action]]):<ref name=hertzberg12>Hertzberg (2010-02-16), p. 1&ndash;2</ref>
 
<math>
S = \int d^4x \sqrt{-g} \left[{m_P^2 \over 2} R - {1 \over 2}
  \partial^{\mu}\phi \partial_{\mu}\phi - V(\phi) - {\xi \over 2} R
    \phi^2\right]
</math>
 
<math>\xi</math> represents the strength of the interaction between <math>R</math> and <math>\phi</math>, which relate to the curvature of space and the magnitude of the inflaton field respectively.
 
==References==
<references/>
 
==Bibliography==
*{{Cite arxiv
| last = Hertzberg | first = Mark P
| year =
| title = On Inflation with Non-minimal Coupling
| class =
| arxiv = 1002.2995
}}
 
[[Category:Cosmic inflation]]
 
 
{{physics-stub}}

Revision as of 18:34, 23 January 2014

Non-minimally coupled inflation is an inflationary model in which the constant which couples gravity to the inflaton field is not small. The coupling constant is usually represented by ξ (Xi), which features in the action (constructed by modifying the Einstein-Hilbert action):[1]

S=d4xg[mP22R12μϕμϕV(ϕ)ξ2Rϕ2]

ξ represents the strength of the interaction between R and ϕ, which relate to the curvature of space and the magnitude of the inflaton field respectively.

References

  1. Hertzberg (2010-02-16), p. 1–2

Bibliography


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