<p>Laboratory and astrophysical tests of “constant variation” have so far concentrated on the <i>dimensionless</i> fine-structure constant <i>α</i> and on the electron or quark mass ratios <i>X</i><sub><i>e</i>,<i>q</i></sub> = <i>m</i><sub><i>e</i>,<i>q</i></sub>/Λ<sub>QCD</sub>, treating the QCD scale Λ<sub>QCD</sub> as unchangeable. Certain beyond Standard Model frameworks, most notably those with a dark matter or dark energy scalar field <i>ϕ</i> coupling with the gluon field, would make Λ<sub>QCD</sub> itself time dependent while leaving <i>α</i> and the electron mass untouched. Under the minimal assumption that this gluonic channel is the sole <i>ϕ</i> interaction, we recast state-of-the-art atomic clock comparisons into <InlineEquation ID="IEq1"> <EquationSource Format="MATHML"><math display="inline"> <msub> <mover accent="true"> <mi mathvariant="normal">Λ</mi> <mo>̇</mo> </mover> <mi>QCD</mi> </msub> <mo>/</mo> <msub> <mi mathvariant="normal">Λ</mi> <mi>QCD</mi> </msub> </math></EquationSource> <EquationSource Format="TEX">\( {\dot{\Lambda}}_{\textrm{QCD}}/{\Lambda}_{\textrm{QCD}} \)</EquationSource> </InlineEquation> = (3.2 ± 3.5) × 10<sup>−17</sup> yr<sup>−1</sup> limits, translate the isotope yields of the 1.8-Gyr-old Oklo natural reactor into a complementary geophysical limit of |<i>δ</i>Λ<sub>QCD</sub>/Λ<sub>QCD</sub>| &lt; 2 × 10<sup>−9</sup> over that time span, corresponding to the linear drift limit <InlineEquation ID="IEq2"> <EquationSource Format="MATHML"><math display="inline"> <mfenced close="|" open="|"> <mrow> <msub> <mover accent="true"> <mi mathvariant="normal">Λ</mi> <mo>̇</mo> </mover> <mi>QCD</mi> </msub> <mo>/</mo> <msub> <mi mathvariant="normal">Λ</mi> <mi>QCD</mi> </msub> </mrow> </mfenced> </math></EquationSource> <EquationSource Format="TEX">\( \left|{\dot{\Lambda}}_{\textrm{QCD}}/{\Lambda}_{\textrm{QCD}}\right| \)</EquationSource> </InlineEquation> &lt; 1 × 10<sup>−18</sup>yr<sup>−1</sup>, and show that the proposed 8<i>.</i>4 eV <sup>229</sup>Th nuclear clock would amplify a putative Λ<sub>QCD</sub> drift by four orders of magnitude compared with present atomic clocks. We also obtain constraints from quasar absorption spectra and Big Bang Nucleosynthesis data.</p>

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Constraints on the variation of the QCD interaction scale ΛQCD

  • V. V. Flambaum,
  • A. J. Mansour

摘要

Laboratory and astrophysical tests of “constant variation” have so far concentrated on the dimensionless fine-structure constant α and on the electron or quark mass ratios Xe,q = me,qQCD, treating the QCD scale ΛQCD as unchangeable. Certain beyond Standard Model frameworks, most notably those with a dark matter or dark energy scalar field ϕ coupling with the gluon field, would make ΛQCD itself time dependent while leaving α and the electron mass untouched. Under the minimal assumption that this gluonic channel is the sole ϕ interaction, we recast state-of-the-art atomic clock comparisons into Λ ̇ QCD / Λ QCD \( {\dot{\Lambda}}_{\textrm{QCD}}/{\Lambda}_{\textrm{QCD}} \) = (3.2 ± 3.5) × 10−17 yr−1 limits, translate the isotope yields of the 1.8-Gyr-old Oklo natural reactor into a complementary geophysical limit of |δΛQCDQCD| < 2 × 10−9 over that time span, corresponding to the linear drift limit Λ ̇ QCD / Λ QCD \( \left|{\dot{\Lambda}}_{\textrm{QCD}}/{\Lambda}_{\textrm{QCD}}\right| \) < 1 × 10−18yr−1, and show that the proposed 8.4 eV 229Th nuclear clock would amplify a putative ΛQCD drift by four orders of magnitude compared with present atomic clocks. We also obtain constraints from quasar absorption spectra and Big Bang Nucleosynthesis data.