Shape of the acoustic gravitational wave power spectrum from a first order phase transition
By M. Hindmarsh, S. Huber, K. Rummukainen, D. Weir. 2017
392 citations recorded by the source corpus.
We present results from large-scale numerical simulations of a first order thermal phase transition in the early Universe, in order to explore the shape of the acoustic gravitational wave and the velocity power spectra. We compare the results with the predictions of the recently proposed sound shell model. For the gravitational wave power spectrum, we find that the predicted k−3 behavior, where k is the wave number, emerges clearly for detonations. The power spectra from deflagrations show similar features, but exhibit a steeper high-k decay and an extra feature not accounted for in the model. There are two independent length scales: the mean bubble separation and the thickness of the sound shell around the expanding bubble of the low temperature phase. It is the sound shell thickness which sets the position of the peak of the power spectrum. The low wave number behavior of the velocity power spectrum is consistent with a causal k3, except for the thinnest sound shell, where it is steeper. We present parameters for a simple broken power law fit to the gravitational wave power spectrum for wall speeds well away from the speed of sound where this form can be usefully applied. We examine the prospects for the detection, showing that a LISA-like mission has the sensitivity to detect a gravitational wave signal from sound waves with an RMS fluid velocity of about 0.05c, produced from bubbles with a mean separation of about 10−2 of the Hubble radius. The shape of the gravitational wave power spectrum depends on the bubble wall speed, and it may be possible to estimate the wall speed, and constrain other phase transition parameters, with an accurate measurement of a stochastic gravitational wave background.
View Paper: https://www.semanticscholar.org/paper/6beb3cfc06ff61ac3074253160461b6efb43c9c8
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
Citations in the corpus
- Towards an all-orders calculation of the electroweak bubble wall velocity (2020, background): “For instance, bubble collisions stir up the charged constituents of the plasma [78], and the associated magnetohydrodynamic turbulence leads to a magnetic field with coherence on the scale of the bubble radius.”
- Gravitational waves from first order cosmological phase transitions in the Sound Shell Model (2019, methodology): “Based on the results of numerical simulations [10–12], it is justifiable to assume that the velocity field is irrotational and statistically homogeneous, in which case the the two-point function can be written 〈 ṽ q1(t1)ṽ ∗j q2(t2) 〉 = q̂ 1q̂ j 1G(q1, t1, t2)(2π) δ(q1 − q2).”
- Gravitational waves from first-order cosmological phase transitions: lifetime of the sound wave source (2020, methodology): “(5)The results of numerical lattice simulations show that Ū(2) f from a single expanding bubble very closely matches the results from an ensemble of overlapping bubbles during gravitational wave production at the end of the phase transition [17, 19].”
- Matter-wave Atomic Gradiometer Interferometric Sensor (MAGIS-100) (2021, unknown): “The reason for this is that gravitational waves produced in thermal phase transitions primarily arise from a combination of long-lasting sound wave and turbulent bulk fluid motions of the plasma acting on far sub-horizon length scales [81, 84, 85, 87, 93, 94].”
- Gravitational waves from bubble dynamics: beyond the envelope (2017, background): “♦11 Though sound waves might be damped by viscosity at late times, the timescale of such an effect can be larger than the Hubble time [24].”
- Updated predictions for gravitational waves produced in a strongly supercooled phase transition (2020, background): “First there is the sound wave period observed in numerical lattice simulations involving the relativistic fluid and field bubbles [84, 97, 98].”
- Dark, cold, and noisy: constraining secluded hidden sectors with gravitational waves (2018, background): “[56] M.”
- Phase transitions in an expanding universe: stochastic gravitational waves in standard and non-standard histories (2020, methodology): “[49, 50] still give a faithful account of the first step for an expanding universe.”
- Reconstructing the spectral shape of a stochastic gravitational wave background with LISA (2019, background): “a kination dominated phase [46–50], non-perturbative particle production phenomena [51–62], oscillon dynamics [63–67], strong first order phase transitions [68–81], or cosmic defect networks [82–93].”
- Model-independent energy budget of cosmological first-order phase transitions—A sound argument to go beyond the bag model (2020, methodology): “• A numerical prefactor that is obtained from lattice simulations [21–24].”
- Theoretical uncertainties for cosmological first-order phase transitions (2020, background): “[93, 94], is determined by the difference in the trace anomaly, Θ, between the two phases,”
- Challenges and opportunities of gravitational-wave searches at MHz to GHz frequencies (2020, background): “However, in field theory simulations of string networks (Vincent et al. 1998; Hindmarsh et al. 2009; Daverio et al. 2016; Hindmarsh et al. 2017b), the network of infinite strings reaches a scaling regime thanks to energy loss into classical radiation of the fields involved in the simulations.”
- Gravitational wave energy budget in strongly supercooled phase transitions (2019, background): “This gives rise to sound waves propagating in the plasma after the transition that source GWs [59–62].”
- Detecting gravitational waves from cosmological phase transitions with LISA: an update (2019, methodology): “Note that for producing the SNR curves the duration of the source is taken to be the Hubble time or the fluid turnover time, whichever is shorter, as the most conservative estimate possible [17, 20].”