2013
DOI: 10.1103/physrevd.88.021302
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Gauge fields and inflation: Chiral gravitational waves, fluctuations, and the Lyth bound

Abstract: Models of inflation involving non-Abelian gauge field backgrounds can produce gravitational waves at an observable level with a preferred handedness. This asymmetry comes about because the non-Abelian background generates parity-violation in the action for perturbations. In the specific model we study, Chromo-Natural Inflation, these gravitational waves can be produced at observable levels even when no field makes a super-Planckian field excursion, thus evading a common formulation of the Lyth bound. Unfortuna… Show more

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Cited by 167 publications
(237 citation statements)
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References 11 publications
(19 reference statements)
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“…To complete our leptogenesis model, now we need to determine net lepton and photons number densities predicted by these models. , H 10 −6 and γ = 9 (which has highly chiral gravitational waves in this γ) [17,23]. The analytical approximation and numerical solution perfectly overlaid each other on sub-horizon scalesτ 5, while as getting closer to the horizon crossing pointτ = 1, they eventually start to deviate from each other.…”
Section: Confronting With the Observationmentioning
confidence: 74%
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“…To complete our leptogenesis model, now we need to determine net lepton and photons number densities predicted by these models. , H 10 −6 and γ = 9 (which has highly chiral gravitational waves in this γ) [17,23]. The analytical approximation and numerical solution perfectly overlaid each other on sub-horizon scalesτ 5, while as getting closer to the horizon crossing pointτ = 1, they eventually start to deviate from each other.…”
Section: Confronting With the Observationmentioning
confidence: 74%
“…That leads to rightand left-handed super-horizon power spectrums which are different from the standard prediction of scalar inflationary models [17,23].…”
Section: Confronting With the Observationmentioning
confidence: 78%
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“…We consider weak distortions of the spacetime metric and the gauge field, δg µν = a 2 h µν and δ A µ · e ν = ay µν , where h µν , y µν are transverse, traceless, and synchronous. Since the Yang-Mills coupling breaks the chiral symmetry of left-and right-circular polarizations [17], it is practical to express the gravitational and gauge field waves with amplitudes h p , y pn in a chiral basis with p = L, R for n = 1, 2, ... , N. A further change of variables, h = H √ 2/aM P and y = Y / √ 2a, puts the action into canonical form. The Lagrangian for gravitational and gauge field waves, propagating with Fourier wave number k much greater than both the expansion rate and the gauge field time rate of change, is given by…”
mentioning
confidence: 99%