Abstract:We study the evolution of cosmological perturbations generated during de
Sitter inflation in the singleton gravity theory. This theory is composed of a
dipole ghost pair in addition to tensor. We obtain the singleton power spectra
which show that the de Sitter/logarithmic conformal field theory (dS/LCFT)
correspondence works for computing the power spectra in the superhorizon limit.
Also we compute the spectral indices for light singleton which contains a
logarithmic correction.Comment: 1+18 pages, no figures,… Show more
“…µ is just a parameter of connecting φ 2 with φ 1 to get the fourth-order derivative equation for φ 2 from a mixed kinetic term. If one wishes to have a massive singleton, one has to include a potential term of m 2 φ 1 φ 2 [4]: (∇ 2 − m 2 )ϕ 1 = 0, (∇ 2 − m 2 )ϕ 2 = µϕ 1 , (∇ 2 − m 2 ) 2 ϕ 2 = 0.…”
Section: Discussionmentioning
confidence: 99%
“…It was given by R = −Hδφ/ φ for the single-field inflation in spatially flat gauge, while it takes the form of R S = −H[ϕ 1 / φ1 + ϕ 2 / φ2 ] for the singleton inflation. For example, the power spectrum appeared in dS spacetime with φ1 = φ2 = 0 [3,4] was given by P m ϕ 2 ϕ 2 ∼ z 2w (1 + 2 ln[z]) with w = 3/2 − 9/4 − m 2 /H 2 in the superhorizon limit. However, we remain "cosmological perturbations of the Einstein-singleton theory around the slow-roll inflation" as a future work, worrying about the appearance of the ghost states.…”
Section: Discussionmentioning
confidence: 99%
“…It seems appropriate to comment that Eqs. ( 14)-( 16) are different from those of a massive singleton in [4]:…”
Section: Einstein-singleton Theorymentioning
confidence: 92%
“…Instead, the authors in [3] have investigated the massive singleton to show the dS/LCFT correspondence in the superhorizon limit of z → 0 as an extension to the dS/CFT correspondence. Recently, two of us have shown that the momentum correlators of LCFT take the same form as the power spectra ×k 3 in the superhorizon limit [4]. This might show that the dS/LCFT correspondence works for obtaining the power spectra in the superhorizon limit.…”
We study the Einstein-singleton theory during de Sitter inflation since it provides a way of degenerate fourth-order scalar theory. We obtain an exact solution expressed in terms of the exponential-integral function by solving the degenerate fourth-order scalar equation in de Sitter spacetime. Furthermore, we find that its power spectrum blows negatively up in the superhorizon limit, while it is negatively scale-invariant in the subhorizon limit. This suggests that the Einstein-singleton theory contains the ghost-instability and thus, it is not suitable for developing a slow-roll inflation model.
“…µ is just a parameter of connecting φ 2 with φ 1 to get the fourth-order derivative equation for φ 2 from a mixed kinetic term. If one wishes to have a massive singleton, one has to include a potential term of m 2 φ 1 φ 2 [4]: (∇ 2 − m 2 )ϕ 1 = 0, (∇ 2 − m 2 )ϕ 2 = µϕ 1 , (∇ 2 − m 2 ) 2 ϕ 2 = 0.…”
Section: Discussionmentioning
confidence: 99%
“…It was given by R = −Hδφ/ φ for the single-field inflation in spatially flat gauge, while it takes the form of R S = −H[ϕ 1 / φ1 + ϕ 2 / φ2 ] for the singleton inflation. For example, the power spectrum appeared in dS spacetime with φ1 = φ2 = 0 [3,4] was given by P m ϕ 2 ϕ 2 ∼ z 2w (1 + 2 ln[z]) with w = 3/2 − 9/4 − m 2 /H 2 in the superhorizon limit. However, we remain "cosmological perturbations of the Einstein-singleton theory around the slow-roll inflation" as a future work, worrying about the appearance of the ghost states.…”
Section: Discussionmentioning
confidence: 99%
“…It seems appropriate to comment that Eqs. ( 14)-( 16) are different from those of a massive singleton in [4]:…”
Section: Einstein-singleton Theorymentioning
confidence: 92%
“…Instead, the authors in [3] have investigated the massive singleton to show the dS/LCFT correspondence in the superhorizon limit of z → 0 as an extension to the dS/CFT correspondence. Recently, two of us have shown that the momentum correlators of LCFT take the same form as the power spectra ×k 3 in the superhorizon limit [4]. This might show that the dS/LCFT correspondence works for obtaining the power spectra in the superhorizon limit.…”
We study the Einstein-singleton theory during de Sitter inflation since it provides a way of degenerate fourth-order scalar theory. We obtain an exact solution expressed in terms of the exponential-integral function by solving the degenerate fourth-order scalar equation in de Sitter spacetime. Furthermore, we find that its power spectrum blows negatively up in the superhorizon limit, while it is negatively scale-invariant in the subhorizon limit. This suggests that the Einstein-singleton theory contains the ghost-instability and thus, it is not suitable for developing a slow-roll inflation model.
“…The HP phase transition has been extensively studied in Refs. [13,14,15,16,17,18,19,20] and with curvature terms in higher dimensions [21,22,23,24,25].…”
We study the thermodynamic properties of a black hole and the Hawking-Page phase transition in the asymptotically anti-de Sitter spacetime in the dilatonic Einstein-Gauss-Bonnet theory of gravitation. We show how the higher-order curvature terms can influence both the thermodynamic properties and the phase transition. We evaluate both heat capacity and free energy difference to determine the local and global thermodynamic stabilities, respectively. We find that the phase transition occurs from the thermal anti-de Sitter to a small spherical black hole geometry and occurs to a hyperbolic black hole geometry in the (dilatonic) Einstein-Gauss-Bonnet theory of gravitation unlike those in Einstein's theory of gravitation.
Abstract. We investigate cosmological perturbations generated during de Sitter inflation in the three-coupled scalar theory. This theory is composed of three coupled scalars (φ p , p = 1, 2, 3) to give a sixth-order derivative scalar theory for φ 3 , in addition to tensor. Recovering the power spectra between scalars from the LCFT correlators in momentum space indicates that the de Sitter/logarithmic conformal field theory (dS/LCFT) correspondence works in the superhorizon limit. We use LCFT correlators derived from the dS/LCFT differentiate dictionary to compare cosmological correlators (power spectra) and find also LCFT correlators by making use of extrapolate dictionary. This is because the former approach is more conventional than the latter. A bulk version dual to the truncation process to find a unitary CFT in the LCFT corresponds to selecting a physical field φ 2 with positive norm propagating on the dS spacetime.
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