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Constraints on the Variation of the QCD Interaction Scale $Λ_{\text{QCD}}$

V. V. Flambaum, A. J. Mansour

TL;DR

The work addresses whether the QCD scale $Λ_{\text{QCD}}$ can drift in time due to a gluon-coupled scalar field, and develops a framework to translate diverse data sets into limits on $\dot{Λ}_{\text{QCD}}/Λ_{\text{QCD}}$ using dimensionless combinations. It analyzes atomic clock frequency ratios, hyperfine and nuclear observables, a proposed $^{229}$Th nuclear clock, Big Bang Nucleosynthesis, the Oklo reactor, and quasar absorption spectra to derive complementary constraints. Key results include $\dot{Λ}_{\text{QCD}}/Λ_{\text{QCD}}=(3.2±3.5)×10^{-17}$ yr$^{-1}$ from atomic clocks, $|δΛ_{\text{QCD}}/Λ_{\text{QCD}}|<2×10^{-9}$ over 1.8 Gyr from Oklo, and a four-order-of-magnitude enhancement in sensitivity for the $^{229}$Th nuclear clock, with additional bounds from BBN and quasar data. Collectively, the paper demonstrates the extreme stability of $Λ_{\text{QCD}}$ over cosmological timescales within this beyond-Standard-Model framework and highlights the potential of nuclear-clock and astrophysical probes as powerful cross-checks.

Abstract

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 $X_{e,q}=m_{e,q}/Λ_{\text{QCD}}$, treating the QCD scale $Λ_{\text{QCD}}$ 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 $Λ_{\text{QCD}}$ 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 $\dotΛ_{\text{QCD}}/Λ_{\text{QCD}}=(3.2 \pm 3.5) \times 10^{-17} \ \text{yr}^{-1}$ limits, translate the isotope yields of the 1.8-Gyr-old Oklo natural reactor into a complementary geophysical limit of $|δΛ_{\text{QCD}}/Λ_{\text{QCD}}|<2\times10^{-9}$ over that time span, corresponding to the linear drift limit $|\dotΛ_{\text{QCD}}/Λ_{\text{QCD}}|<1\times10^{-18} \text{yr}^{-1}$, and show that the proposed $8.4$ eV $^{229}$Th nuclear clock would amplify a putative $Λ_{\text{QCD}}$ drift by four orders of magnitude compared with present atomic clocks. We also obtain constraints from quasar absorption spectra and Big Bang Nucleosynthesis data.

Constraints on the Variation of the QCD Interaction Scale $Λ_{\text{QCD}}$

TL;DR

The work addresses whether the QCD scale can drift in time due to a gluon-coupled scalar field, and develops a framework to translate diverse data sets into limits on using dimensionless combinations. It analyzes atomic clock frequency ratios, hyperfine and nuclear observables, a proposed Th nuclear clock, Big Bang Nucleosynthesis, the Oklo reactor, and quasar absorption spectra to derive complementary constraints. Key results include yr from atomic clocks, over 1.8 Gyr from Oklo, and a four-order-of-magnitude enhancement in sensitivity for the Th nuclear clock, with additional bounds from BBN and quasar data. Collectively, the paper demonstrates the extreme stability of over cosmological timescales within this beyond-Standard-Model framework and highlights the potential of nuclear-clock and astrophysical probes as powerful cross-checks.

Abstract

Laboratory and astrophysical tests of ''constant variation'' have so far concentrated on the dimensionless fine-structure constant and on the electron or quark mass ratios , treating the QCD scale as unchangeable. Certain beyond Standard Model frameworks, most notably those with a dark matter or dark energy scalar field coupling with the gluon field, would make itself time dependent while leaving and the electron mass untouched. Under the minimal assumption that this gluonic channel is the sole interaction, we recast state-of-the-art atomic clock comparisons into limits, translate the isotope yields of the 1.8-Gyr-old Oklo natural reactor into a complementary geophysical limit of over that time span, corresponding to the linear drift limit , and show that the proposed eV Th nuclear clock would amplify a putative drift by four orders of magnitude compared with present atomic clocks. We also obtain constraints from quasar absorption spectra and Big Bang Nucleosynthesis data.

Paper Structure

This paper contains 10 sections, 41 equations, 3 tables.