Searcharxiv⌕ Search

arXiv · 2610.24283

How accurate is Spectral Einstein Code (SpEC)? And what limits its accuracy?

Abstract

The improved sensitivity of upcoming gravitational-wave detectors will require correspondingly more accurate binary black hole (BBH) simulations. Given the high cost of such simulations, it is essential to understand their sources of error and use computational resources efficiently. We study sources of error in BBH simulations performed with the Spectral Einstein Code (SpEC) and seek to understand what limits their accuracy. In particular, we focus on the inspiral phase because it is the longest-running part of the simulation and accounts for the majority of the waveform error. We find that targeted changes to simulation parameters and resolution in different parts of the computational domain reduce constraint violations and gravitational waveform differences. We also discuss more fundamental limitations on our accuracy that become important at higher resolutions: floating-point errors and large differences in the scales of the fundamental variables. Addressing these limitations will require substantial changes to both the SpEC code and the formulation it uses to evolve Einstein's equations. Many of the improvements and changes discussed in this paper are likely to be relevant to other numerical relativity codes.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Himanshu Chaudhary, Mark A. Scheel, Robert Owen, Saul A. Teukolsky, Michael Boyle, Lawrence E. Kidder, Harald P. Pfeiffer. 2026-10-16. How accurate is Spectral Einstein Code (SpEC)? And what limits its accuracy?. https://arxiv.org/abs/2610.24283

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Demagnetizing KBR and New Ricci-flat Rotating Metric

We construct a new Ricci-flat metric by demagnetizing the recently reported Kerr-Bertotti-Robinson (KBR) solution. The metric is a deformation of the Kerr metric characterized by a parameter $B$, so that the asymptotic Kerr becomes a regular dome of spindle shape with north and south poles. Despite lacking an asymptotically-flat region, we find that the first law of black hole thermodynamics can be established. Some thermodynamic relations are identical to those of the Kerr black hole, as if the constant $B$ is absent. Our Ricci-flat rotating metric serves a neutral seed for a variety of inequivalent schemes of magnetizing the Schwarzschild and Kerr black holes.

gr-qc↗

The efficiency gap of two-step forecasts for stochastic gravitational wave background searches

The stochastic gravitational-wave background is targeted by the millihertz observatories LISA, Taiji and TianQin, and its forecast precision rests on a Whittle approximation to the periodogram likelihood. The quoted scale is that of a joint fit a two-step forecast need not reach. We show that the residual risk of a two-step forecast lies in the estimator route rather than in the likelihood. At the exact Whittle form we separate the forecast error into a deterministic bias $\mathbf{b}$ and an efficiency gap $\mathbf{C}_b$, both in closed form. We find that this gap is governed by the span of the first-step nuisance fit. It decreases substantially as the span increases and vanishes when the first-step fit spans the entire band or when the response exhibits no within-bin structure. The gap does not arise as a cost of the prior. Across the LISA band the gap spans more than an order of magnitude, the amplitude and tilt inflation falling from about thirty and twenty to unity at a band-wide first step. A foreground from the released LDC2a population moves the mid-band gap by an order of magnitude. A two-step forecast should therefore report the span of its first-step fit with its intervals, since that span decides whether they sit at the Fisher scale or an order of magnitude above it.

gr-qc↗

Semiclassical Cosmological Constant in Anti-de Sitter and de Sitter Spacetimes

We investigate the semiclassical Einstein equation for a quantized scalar field in four-dimensional anti-de Sitter (AdS) and de Sitter (dS) spacetimes. We first determine self-consistent configurations by fixing the bare cosmological constant to its geometric value, requiring the renormalized vacuum stress-energy tensor to vanish. In AdS, the resulting mass-curvature relations depend on the curvature coupling and boundary conditions; one formal Neumann root for minimal coupling is excluded by the admissible parameter range, whereas both Dirichlet and Neumann solutions are allowed for conformal coupling. In dS, we recover the known self-consistent solution for a minimally coupled massive field. We then evaluate the effective cosmological constant on prescribed backgrounds in four massless configurations. In each case, it takes the form \(Λ_{\mathrm{eff}}=A/\ell^2+B/\ell^4\). The competition between classical curvature and vacuum polarization produces a minimum and a zero in the minimally coupled AdS case, while the other configurations are monotonic. Finally, the formal continuation \(\ell\rightarrow i\ell\) fails to reproduce the directly calculated quantum coefficients: their AdS-to-dS ratios are \(29/61\) for minimal coupling and \(-1\) for conformal coupling. These results show that continuation of the curvature scale alone does not establish equivalence between the semiclassical vacuum contributions in AdS and dS.

gr-qc↗