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Gravitational Waves From the End of Inflation: Computational Strategies
Astrophysics · Submitted 18 Dec 2007
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim These models have a very short and intense period of resonance which is qualitatively different from previous examples studied in this context, but we find that they lead to a similar spectrum of gravitational radiation.
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The abstract, sentence by sentence
Parametric resonance or preheating is a plausible mechanism for bringing about the transition between the inflationary phase and a hot, radiation dominated universe. This epoch results in the rapid production of heavy particles far from thermal equilibrium and could source a significant stochastic background of gravitational radiation. Here, we present a numerical algorithm for computing the contemporary power spectrum of gravity waves generated in this post-inflationary phase transition for a large class of scalar-field driven inflationary models. We explicitly calculate this spectrum for both quartic and quadratic models of chaotic inflation, and low-scale hybrid models. In particular, we consider hybrid models with an ``inverted'' potential. These models have a very short and intense period of resonance which is qualitatively different from previous examples studied in this context, but we find that they lead to a similar spectrum of gravitational radiation.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Parametric resonance or preheating is a plausible mechanism for bringing about the transition between the inflationary phase and a hot, radiation dominated universe. | background 1.00 | 0.05 | 0.03 | hedged possibility 0.99 |
| s1 | This epoch results in the rapid production of heavy particles far from thermal equilibrium and could source a significant stochastic background of gravitational radiation. | background 0.99 | 0.07 | 0.09 | hedged possibility 0.99 |
| s2 | Here, we present a numerical algorithm for computing the contemporary power spectrum of gravity waves generated in this post-inflationary phase transition for a large class of scalar-field driven inflationary models. | contribution 0.81 | 0.95 | 0.16 | asserted 1.00 |
| s3 | We explicitly calculate this spectrum for both quartic and quadratic models of chaotic inflation, and low-scale hybrid models. | contribution 0.87 | 0.96 | 0.10 | asserted 1.00 |
| s4 | In particular, we consider hybrid models with an ``inverted'' potential. | contribution 0.86 | 0.50 | 0.05 | asserted 0.97 |
| s5 | These models have a very short and intense period of resonance which is qualitatively different from previous examples studied in this context, but we find that they lead to a similar spectrum of gravitational radiation. | result 0.94 | 0.95 | 0.47 | asserted 1.00 |
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The paper
Original abstract
Parametric resonance or preheating is a plausible mechanism for bringing about the transition between the inflationary phase and a hot, radiation dominated universe. This epoch results in the rapid production of heavy particles far from thermal equilibrium and could source a significant stochastic background of gravitational radiation. Here, we present a numerical algorithm for computing the contemporary power spectrum of gravity waves generated in this post-inflationary phase transition for a large class of scalar-field driven inflationary models. We explicitly calculate this spectrum for both quartic and quadratic models of chaotic inflation, and low-scale hybrid models. In particular, we consider hybrid models with an ``inverted'' potential. These models have a very short and intense period of resonance which is qualitatively different from previous examples studied in this context, but we find that they lead to a similar spectrum of gravitational radiation.
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References
How later papers used it
49 later papers cite it
5 papers by the same authors are listed below: 5 used its method or tool.
Uses its method or tool 5 of 11 papers with this label · 5 by the same authors
By the same authors
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Invoked Parseval's theorem, citing this paper, to rewrite its gravitational wave energy density expression.
Gravitational Waves from Global Second Order Phase Transitions (2011) (same authors) · 0.91 · paraphrased: the licence does not allow quoting
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Computed the transverse-traceless part of the first order perturbative metric using the method described in this paper, evolving Fourier modes in Fourier space with a fourth-order-in-time Runge-Kutta scheme.
Gravitational Waves from Oscillon Preheating (2013) (same authors) · 1.00 · paraphrased: the licence does not allow quoting
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Computed gravitational waves by solving the sourced, inhomogeneous linear partial differential equation for the transverse-traceless part of the metric in momentum space, similar to the implementation in this paper.
Gravitational waves from gauge preheating (2018) (same authors) · 1.00 · paraphrased: the licence does not allow quoting
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Calculated the power in gravitational waves by passively calculating tensor perturbations of the metric, following the basic procedure of this paper.
Gravitational Waves from Kinetic Preheating (2024) (same authors) · 1.00 · paraphrased: the licence does not allow quoting
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Computed the gravitational wave spectrum passively, citing this paper, by calculating the transverse-traceless parts of the matter stress tensor.
Gauge preheating with full general relativity (2023) (same authors) · 0.93 · paraphrased: the licence does not allow quoting
How the literature uses it
47 arXiv papers cite this in 72 sentences
Papers citing it · 35 sentences without a confident label
Builds on it 1 paper
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Because fields decay throughout inflation, we expect an additional gravitational wave spectrum resulting from the superposition of spectra similar to the ones found in [ref] ; since the process operates within the horizon, the peaks of the spectra are always generated at the same fraction of the Hubble radius whenever a field decays.
Multi-Field Inflation on the Landscape · Outlook · 0.84
Uses its method or tool 11 papers
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We couple LatticeEasy to a code that evolves the metric perturbation using the methods of [ref] .
Gravitational Waves from Global Second Order Phase Transitions · Gravitational Waves · 1.00
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The transverse-traceless part of the first order perturbative metric is computed using the method described in [ref] – with the Fourier modes of the metric perturbations (and their sources in $T_μν$) evolved in Fourier space, via a fourth-order-in-time Runge-Kutta scheme.
Gravitational Waves from Oscillon Preheating · Gravitational Waves: Numerical simulations · 1.00
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We followed [ref] to compute the transverse-traceless part of the first-order metric perturbation.
Detectable Gravitational Waves from preheating probes non-thermal Dark Matter · Gravitational Waves Generated During Preheating · 1.00
Compares with it 2 papers
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While the detailed mechanism is different, this signal has much in common with the gravitational wave background that can be generated during preheating or parametric resonance [ref] .
Thermal Inflation and the Gravitational Wave Background · Discussion · 0.96
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We note that lattice studies of GW production from preheating with quartic inflaton potentials have a long history [ref] , and our results for the spectator-sourced signal are qualitatively consistent with the enhanced amplitudes found in those works for the inflaton-sourced case.
Gravitational Waves from Matter Perturbations of Spectator Scalar Fields · Gravitational Waves with Quartic Inflaton Potential · 0.96
Cites it as support 1 paper
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The GW signal is therefore expected to be significantly enhanced in this case [ref] .
Gravitational Waves from Matter Perturbations of Spectator Scalar Fields · Gravitational Waves with Quartic Inflaton Potential · 0.96
Cites it as background 19 papers
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These include from preheating at the end of inflation [ref] scalar-induced gravitational waves [ref] , bubble collisions [ref] or phase transitions [ref] .
CMB and energy conservation limits on nanohertz gravitational waves · Introduction · 0.94
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The production of gravitational waves from preheating was originally studied in [ref] for chaotic inflation, and recently by several groups in [ref] .
Gravity Waves from Tachyonic Preheating after Hybrid Inflation · Introduction · 1.00
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The production of such SGWB signals has been studied in literature over the years in various contexts such as single-field chaotic inflation [ref] , preheating after hybrid inflation [ref] , including production of gauge fields during preheating [ref] , and for GWs production from oscillons from inflationary potentials that `opens up' away from the minimum [ref] .
Detectable Gravitational Waves from preheating probes non-thermal Dark Matter · Introduction · 0.98
What it cites · 42 sentences without a confident label
Uses the method or tool of 2 papers
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The field evolution was computed using LATTICEEASY [ref] , which uses a staggered leapfrog integrator.
LATTICEEASY: A Program for Lattice Simulations of Scalar Fields in an Expanding Universe · Evolution of the Perturbation · 1.00
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We could further improve matters by only evolving a subset of the Fourier modes of the $h_ij$ (a strategy employed by [ref] ) – the only downside to these approaches is that, if carried too far, the spectrum acquires significant stochastic noise, since it is being computed from a small sample of total set of modes.
Theory and Numerics of Gravitational Waves from Preheating after Inflation · Numerical Issues · 0.96
Uses data or values from 3 papers
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The $n=1$ term has an amplitude of $0.9550$ and dominates this series (see [ref] for full analysis).
Structure of Resonance in Preheating after Inflation · Parametric Resonance and Preheating · 0.80
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Current data for the CMB B-mode suggests that $r≲.3$, which already rules out well-known models of inflation [ref] .
Wilkinson Microwave Anisotropy Probe (WMAP) Three Year Results: Implications for Cosmology · Introduction · 0.92
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Current data for the CMB B-mode suggests that $r≲.3$, which already rules out well-known models of inflation [ref] .
Slow Roll Reconstruction: Constraints on Inflation from the 3 Year WMAP Dataset · Introduction · 0.92
Compares with 7 papers
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The box method (as implemented in [ref] ) yields spectra with a significantly higher amplitude than those found with the spectral or Green's function methods, but that the latter methods agree very closely with each other.
Stochastic Gravitational Wave Production After Inflation · Introduction · 0.92
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In addition to the previous work of the current authors [ref] , two other independent codes have been recently been developed to address this problem [ref] and we explicitly compare the results of our spectral algorithm that the Green's function algorithm of [ref] , showing that the difference between the computed spectra is of the same order as that introduced by the finite resolution of the underlying spatial lattice.
Gravitational Wave Production At The End Of Inflation · Discussion · 0.98
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In addition to the previous work of the current authors [ref] , two other independent codes have been recently been developed to address this problem [ref] and we explicitly compare the results of our spectral algorithm that the Green's function algorithm of [ref] , showing that the difference between the computed spectra is of the same order as that introduced by the finite resolution of the underlying spatial lattice.
A Gravitational Wave Background from Reheating after Hybrid Inflation · Discussion · 0.98
Cites as background 14 papers
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The overall scaling properties of any stochastic spectrum produced as inflation ends and the universe reheats were first conjectured in [ref] .
Stochastic Gravitational Wave Production After Inflation · Discussion · 0.95
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In [ref] , Garcia-Bellido and Figueroa restated the scaling argument of [ref] and computed the gravitational waves sourced by bubble-collisions at a variety of scales.
A stochastic background of gravitational waves from hybrid preheating · Introduction · 0.81
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We now review parametric resonance of scalar fields [ref] .
Inflation Dynamics and Reheating · Parametric Resonance and Preheating · 1.00
Discussion
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