2021
DOI: 10.1007/jhep12(2021)098
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Missing scalars at the cosmological collider

Abstract: Light scalar fields typically develop spatially varying backgrounds during inflation. Very often they do not directly affect the density perturbations, but interact with other fields that do leave nontrivial signals in primordial perturbations. In this sense they become “missing scalars” at the cosmological collider. We study potentially observable signals of these missing scalars, focusing on a special example where a missing scalar distorts the usual oscillatory features in the squeezed bispectrum. The disto… Show more

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Cited by 36 publications
(21 citation statements)
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“…The exponent N is an integer, while L is in general a real number. When ω = 0, the exponent L is often an integer or halfinteger, although exceptions exist [54]. In the nonanalytic piece, we see the characteristic oscillatory dependence on , described by two parameters, the frequency ω and the phase ϕ.…”
Section: Observablesmentioning
confidence: 92%
“…The exponent N is an integer, while L is in general a real number. When ω = 0, the exponent L is often an integer or halfinteger, although exceptions exist [54]. In the nonanalytic piece, we see the characteristic oscillatory dependence on , described by two parameters, the frequency ω and the phase ϕ.…”
Section: Observablesmentioning
confidence: 92%
“…(See the next section for details.) Furthermore, a loop-induced mass correction to the intermediate particle can introduce noninteger correction to α [42], a fact sometimes interpreted as particle decay width [1].…”
Section: Dissecting Cosmological Collider Signalsmentioning
confidence: 99%
“…These additional parameters can be used to extract more information from the observed signal. For instance, it was known that the scaling power α can be used to distinguish between tree and 1-loop signals [57], or to tell loop corrected masses from tree-level masses [42].…”
Section: Introductionmentioning
confidence: 99%
“…Said another way, if Q commutes with the Hamiltonian for a Lorentz invariant system, the Lagrangian (not the Lagrangian density) is invariant. 56 Now consider the case when the symmetry δφ does contain the time coordinate, but not time derivatives. Such charges typically do not commute with the Hamiltonian.…”
Section: B2 Symmetry Generatorsmentioning
confidence: 99%
“…The general recursion formula is given in equation (4.14), and is obtained by deforming the kinematics that the wavefunction depends on into the complex plane. The recursion relations as a sort of cosmological collider [23,34,35,[46][47][48][49][50][51][52][53][54][55][56][57]. 2 Scattering amplitudes can also satisfy soft theorems when there are cubic vertices present that are compatible with the nonlinearly realized symmetries, for example in the conformal dilaton [61], or in non-relativistic cases [62] (see also [63] for another relativistic example).…”
Section: Introductionmentioning
confidence: 99%