<p>Stellar theory predicts a forbidden range of black-hole masses between approximately 50 <i>M</i><sub>⊙</sub>&#xa0;and 130 <i>M</i><sub>⊙</sub> owing to pair-instability supernovae<sup><CitationRef AdditionalCitationIDS="CR2 CR3 CR4 CR5 CR6" CitationID="CR1">1</CitationRef>–<CitationRef CitationID="CR7">7</CitationRef></sup>, but evidence for such a gap in the mass distribution from gravitational-wave astronomy has proved elusive. Early hints of a cut-off in black-hole masses at about 45 <i>M</i><sub>⊙</sub> disappeared with the subsequent discovery of more massive binary black holes<sup><CitationRef CitationID="CR8">8</CitationRef>,<CitationRef CitationID="CR9">9</CitationRef></sup>. Here we report evidence of the pair-instability gap in LIGO–Virgo–KAGRA’s fourth Gravitational-Wave Transient Catalog (GWTC-4), with a lower boundary of <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(4{4}_{-4}^{+5}\,{M}_{\odot }\)</EquationSource> <EquationSource Format="MATHML"><math> <mn>4</mn> <msubsup> <mrow> <mn>4</mn> </mrow> <mrow> <mo>−</mo> <mn>4</mn> </mrow> <mrow> <mo>+</mo> <mn>5</mn> </mrow> </msubsup> <mspace width="0.25em" /> <msub> <mrow> <mi>M</mi> </mrow> <mrow> <mo>⊙</mo> </mrow> </msub> </math></EquationSource> </InlineEquation> (90% credibility). Although the gap is not present in the distribution of primary masses <i>m</i><sub>1</sub> (the bigger of the two black holes in a binary system), it appears unambiguously in the distribution of secondary masses <i>m</i><sub>2</sub>, in which <i>m</i><sub>2</sub> ≤ <i>m</i><sub>1</sub>. The location of the gap lines up well with a previously identified transition in the binary black-hole spin distribution; binaries with primary components in the gap tend to spin more rapidly than those below the gap. We interpret these findings as evidence for a subpopulation of hierarchical mergers: binaries in which the primary component is the product of a previous black-hole merger and thus populates the gap. Our measurement of the location of the pair-instability gap constrains the <i>S</i>-factor for <sup>12</sup>C(<i>α</i>, <i>γ</i>)<sup>16</sup>O at 300 keV to <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(26{0}_{-108}^{+190}\,{\rm{keV}}\,{\rm{barns}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mn>26</mn> <msubsup> <mrow> <mn>0</mn> </mrow> <mrow> <mo>−</mo> <mn>108</mn> </mrow> <mrow> <mo>+</mo> <mn>190</mn> </mrow> </msubsup> <mspace width="0.25em" /> <mrow> <mrow> <mi mathvariant="normal">keV</mi> </mrow> </mrow> <mspace width="0.25em" /> <mrow> <mrow> <mi mathvariant="normal">barns</mi> </mrow> </mrow> </math></EquationSource> </InlineEquation>.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Evidence of the pair-instability gap from black-hole masses

  • Hui Tong,
  • Maya Fishbach,
  • Eric Thrane,
  • Matthew Mould,
  • Thomas A. Callister,
  • Amanda M. Farah,
  • Nir Guttman,
  • Sharan Banagiri,
  • Daniel Beltran-Martinez,
  • Ben Farr,
  • Shanika Galaudage,
  • Jaxen Godfrey,
  • Jack Heinzel,
  • Marios Kalomenopoulos,
  • Simona J. Miller,
  • Aditya Vijaykumar

摘要

Stellar theory predicts a forbidden range of black-hole masses between approximately 50 M and 130 M owing to pair-instability supernovae17, but evidence for such a gap in the mass distribution from gravitational-wave astronomy has proved elusive. Early hints of a cut-off in black-hole masses at about 45 M disappeared with the subsequent discovery of more massive binary black holes8,9. Here we report evidence of the pair-instability gap in LIGO–Virgo–KAGRA’s fourth Gravitational-Wave Transient Catalog (GWTC-4), with a lower boundary of \(4{4}_{-4}^{+5}\,{M}_{\odot }\) 4 4 4 + 5 M (90% credibility). Although the gap is not present in the distribution of primary masses m1 (the bigger of the two black holes in a binary system), it appears unambiguously in the distribution of secondary masses m2, in which m2 ≤ m1. The location of the gap lines up well with a previously identified transition in the binary black-hole spin distribution; binaries with primary components in the gap tend to spin more rapidly than those below the gap. We interpret these findings as evidence for a subpopulation of hierarchical mergers: binaries in which the primary component is the product of a previous black-hole merger and thus populates the gap. Our measurement of the location of the pair-instability gap constrains the S-factor for 12C(α, γ)16O at 300 keV to \(26{0}_{-108}^{+190}\,{\rm{keV}}\,{\rm{barns}}\) 26 0 108 + 190 keV barns .