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Quasinormal modes of D-dimensional de Sitter spacetime
General Relativity and Quantum Cosmology · Submitted 4 May 2006
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We calculate the exact values of the quasinormal frequencies for an electromagnetic field and a gravitational perturbation moving in $D$-dimensional de Sitter spacetime ($D \geq 4$).
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The abstract, sentence by sentence
We calculate the exact values of the quasinormal frequencies for an electromagnetic field and a gravitational perturbation moving in $D$-dimensional de Sitter spacetime ($D \geq 4$). We also study the quasinormal modes of a real massive scalar field and we compare our results with those of other references.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We calculate the exact values of the quasinormal frequencies for an electromagnetic field and a gravitational perturbation moving in $D$-dimensional de Sitter spacetime ($D \geq 4$). | contribution 0.69 | 0.97 | 0.67 | asserted 1.00 |
| s1 | We also study the quasinormal modes of a real massive scalar field and we compare our results with those of other references. | contribution 1.00 | 0.92 | 0.11 | asserted 0.98 |
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The paper
Original abstract
We calculate the exact values of the quasinormal frequencies for an electromagnetic field and a gravitational perturbation moving in $D$-dimensional de Sitter spacetime ($D \geq 4$). We also study the quasinormal modes of a real massive scalar field and we compare our results with those of other references.
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References
How later papers used it
61 later papers cite it
4 later papers by other authors are listed below: 1 used its method or tool, 1 used its data or values and 3 compared their own results with it. 1 of them appears under more than one label.
Uses its method or tool 1 of 5 papers with this label
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Followed the steps in this paper to show that the radial equation can be transformed into the HDE by a change of variable.
Quasinormal modes of accelerating spacetime (2024) · 1.00 · paraphrased: the licence does not allow quoting
Uses its data or values 1 of 7 papers with this label
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The value of $μ_c$ depends on the cosmological constant, and for the de Sitter case (with $M=0$) they correspond to [equation] Although such an explicit form is not attainable for the SdS case, the result for the de Sitter spacetime presented in Ref. [ref] and [ref] provides a good estimate for our purposes.
Quasibound state reminiscent in de-Sitter black holes: Quasinormal modes and the decay of massive fields (2024) · Results · 0.85
Compares with it 3 of 10 papers with this label
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Employed this method to calculate dS modes and compared its own results with those in this paper to validate its approach.
Quasinormal modes of accelerating spacetime (2024) · 1.00 · paraphrased: the licence does not allow quoting
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Noted that its scalar spectra coincide with those of this paper's Physical modes I, while its vector ones coincide with Physical modes II.
De Sitter Horizon Edge Partition Functions (2025) · 0.90 · paraphrased: the licence does not allow quoting
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Retrieved a set of modes that approximate the quasinormal modes of the static patch given in this paper, in the worldline limit of the cosmic patch.
Cosmological Observatories (2024) · 0.80 · paraphrased: the licence does not allow quoting
How the literature uses it
59 arXiv papers cite this in 159 sentences
Papers citing it · 101 sentences without a confident label
Contests it 1 paper
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Thus for these values of the parameters we find that the formula (51) of Ref. [ref] does not give valid QNF of the de Sitter spacetime.
On the quasinormal modes of the de Sitter spacetime · On the de Sitter QNF of the Klein-Gordon field with $q=0$, $μ^2 = 2$, and $D=4$ · contest 0.95
Builds on it 1 paper
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So we provide additional perturbations for which their QN frequencies can be exactly calculated in this background and therefore we extend the results of Refs. [ref] , [ref] .
Electromagnetic quasinormal modes of D-dimensional black holes II · QN frequencies of $D$-dimensional Nariai solution · 1.00
Uses its method or tool 4 papers
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To solve Eq. ([ref]) we make the change of variable $y = r^2$ [ref] , [ref] to obtain [equation] Proposing that the function $U$ takes the form [equation] we find that if the quantities $E$ and $C$ are solutions of the equations [equation] then the function $U_2$ must be a solution of the differential equation [equation] which is a hypergeometric type differential equation [ref] , [ref] [equation]
On the quasinormal modes of the de Sitter spacetime · Gravitational QNM of the de Sitter spacetime · 0.97
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We follow the steps in [ref] to show that the radial equation [ref] can be transformed into the HDE by a change of variable.
Quasinormal modes of accelerating spacetime · Direct conversion to HDEs · 1.00
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The quasinormal modes of massive fields on de Sitter are found directly from the equations of motion of the field in the manner of [ref] .
Spinning up the spool: Massive spinning fields in 3d quantum gravity · DHS for massive spinning fields on S3 · 0.93
Uses its data or values 7 papers
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In this section our aim is to use the ideas by Hod, Kunstatter, and Maggiore to find the quantum of area for $D$-dimensional de Sitter horizon, hence we note that the QNF of the gravitational perturbations (GP) in $D$-dimensional de Sitter spacetime are equal to [ref] , [ref] [equation] where $n = 0, 1,…$, $q=0$ for tensor type GP, $q=1$ for vector type GP, $q=2$ for scalar type GP, and $l$ is the orbital angular momentum number.[The QNF of the boson and fermion fields in $D$-dimensional de Sitter spacetime for $D ≥3$ were calculated exactly in Refs. [ref] – [ref] .
Area spectrum of the D-dimensional de Sitter spacetime · Quantum of area for $D$-dimensional de Sitter horizon · 0.94
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For example, for a massive field of mass $m^2 = Δ(d-1-Δ)$ minimally coupled to gravity the answer [There is also the second branch $ω_k = -i ( l + Δ+ 2k + d-1)κ_c$. ] [ref] is
On scrambling, tomperature and superdiffusion in de Sitter space · Superdiffusion · 0.91
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For the electromagnetic field, the effective potentials of the modes $I$ and $II$ in $D$-dimensional de Sitter spacetime are equal to (Table 1 of Ref. [ref] ) [equation] with $x=r_*/L$.
Dirac quasinormal modes of D-dimensional de Sitter spacetime · Effective potentials · 0.81
Compares with it 9 papers
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It is convenient to notice that the quantities $i ω̃$ of formula ([ref]) are integers for odd $p$ and half-integers for even $p$, as the de Sitter QN frequencies of a massless Klein-Gordon coupled to curvature with coupling constant $ξ=(D-1)/(4D)$ (see expression (55) of [ref] ).
Dirac quasinormal modes of D-dimensional de Sitter spacetime · Massless Dirac field · 0.83
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To validate our approach, we employ this method to calculate dS modes and compare our results with those in [ref] .
Quasinormal modes of accelerating spacetime · INTRODUCTION · 1.00
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Our results coincide with those of Ref. [ref] , but the method of Sect.
On the quasinormal modes of the de Sitter spacetime · Summary · 1.00
Cites it as support 1 paper
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In fact, the $Φ_ω, k$ are exactly (up to normalization) the quasi-normal modes of dS$_3$ [ref] .
Gravitational Wilson Lines in 3D de Sitter · Wick rotation and quasi-normal modes · 0.97
Cites it as background 14 papers
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In this finite region, we find two families of modes in the spectrum, namely the PS modes [ref] and the dS modes [ref] .
Spectral (in)stability of quasinormal modes and strong cosmic censorship · SdS BHs · 0.90
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Second, there is a set of purely imaginary modes (non-oscillatory damped modes) associated to the presence of the cosmological horizon, referred to as de Sitter (dS) modes [ref] .
Pseudospectrum of de Sitter black holes · Introduction · 0.98
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In the presence of a cosmological constant, a new class of modes also emerges, e.g., besides the well-known photon sphere modes, there are purely imaginary de Sitter modes for Schwazrschild-de Sitter black holes [ref] .
Perturbing the perturbed: Stability of quasinormal modes in presence of a positive cosmological constant · Introduction · 0.83
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