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Inflationary theory and pulsar timing investigations of primordial black holes and gravitational waves

Nicholas Orlofsky, Aaron Pierce, James D. Wells

TL;DR

The paper probes whether LIGO-detected mergers could originate from primordial black holes formed by inflationary perturbations, and whether the associated secondary gravitational waves are observable with pulsar timing arrays. It develops a framework linking the primordial curvature spectrum to PBH abundance and to a SGW background from second-order tensor modes, then compares predictions across several inflationary scenarios to current PTA data. It finds that models with broad or extended primordial spectra are largely excluded by PTAs, while highly peaked spectra—such as those arising from parametric resonance in double inflation—remain testable with continued PTA observations, whereas some postinflation scenarios like the axion-curvaton generically push SGWs to frequencies PTAs cannot probe. Overall, PTAs provide a powerful, inflation-model-sensitive probe to discriminate PBH formation mechanisms and illuminate early-universe physics, complementary to LIGO observations.

Abstract

The gravitational waves measured at LIGO are presumed here to come from merging primordial black holes. We ask how these primordial black holes could arise through inflationary models while not conflicting with current experiments. Among the approaches that work, we investigate the opportunity for corroboration through experimental probes of gravitational waves at pulsar timing arrays. We provide examples of theories that are already ruled out, theories that will soon be probed, and theories that will not be tested in the foreseeable future. The models that are most strongly constrained are those with a relatively broad primordial power spectrum.

Inflationary theory and pulsar timing investigations of primordial black holes and gravitational waves

TL;DR

The paper probes whether LIGO-detected mergers could originate from primordial black holes formed by inflationary perturbations, and whether the associated secondary gravitational waves are observable with pulsar timing arrays. It develops a framework linking the primordial curvature spectrum to PBH abundance and to a SGW background from second-order tensor modes, then compares predictions across several inflationary scenarios to current PTA data. It finds that models with broad or extended primordial spectra are largely excluded by PTAs, while highly peaked spectra—such as those arising from parametric resonance in double inflation—remain testable with continued PTA observations, whereas some postinflation scenarios like the axion-curvaton generically push SGWs to frequencies PTAs cannot probe. Overall, PTAs provide a powerful, inflation-model-sensitive probe to discriminate PBH formation mechanisms and illuminate early-universe physics, complementary to LIGO observations.

Abstract

The gravitational waves measured at LIGO are presumed here to come from merging primordial black holes. We ask how these primordial black holes could arise through inflationary models while not conflicting with current experiments. Among the approaches that work, we investigate the opportunity for corroboration through experimental probes of gravitational waves at pulsar timing arrays. We provide examples of theories that are already ruled out, theories that will soon be probed, and theories that will not be tested in the foreseeable future. The models that are most strongly constrained are those with a relatively broad primordial power spectrum.

Paper Structure

This paper contains 10 sections, 15 equations, 2 figures.

Figures (2)

  • Figure 1: Gravitational wave abundance for an idealized delta function scalar spectrum peaked at the scale $k_f$ corresponding to PBH mass $30M_{\astrosun}$ according to Eq. (\ref{['eqn:MPBH']}) and normalized so that $\Omega_{\rm PBH}=\Omega_{\rm DM}$
  • Figure 2: Gravitational wave abundance (envelopes) as a function of frequency assuming $\Omega_{\rm PBH}=\Omega_{\rm DM}$. The PBH abundance spectrum is peaked at 30 (left) or 10 (right) $M_{\astrosun}$. We display SGW for a top-hat spectrum with width set by expectations from parametric resonance (green "PR" curve), a red-tilted scalar spectrum with spectral index $n_s=-1$ supplemented by a cutoff at a minimum frequency (red "No PR" curve), and the spectrum from the running mass model (purple curve). Black solid lines are current spectrum-independent bounds from EPTA (upper) Lentati:2015qwp, NANOGrav (middle) Arzoumanian:2015liz, and PPTA (lower) Shannon:2015ect. The black dashed line is a projection for bounds from SKA Janssen:2014dka. The top axis indicates the approximate observing time $T$ to be sensitive to a given minimum frequency $f_{\rm min} \sim 1/T$.