[Paper Review] Magnetic dipole and electric quadrupole moments of the 229Th nucleus
This paper determines the magnetic dipole (μ = 0.360(7) μB) and electric quadrupole (Q = 3.11(6) eb) moments of the 229Th nucleus with 2% uncertainty by combining high-precision relativistic all-order atomic structure calculations with measured hyperfine constants in 229Th³⁺. The method achieves fivefold improved accuracy over prior values and establishes a benchmark for future nuclear moment determinations in other systems.
We calculate the A and B hyperfine constants for the low-lying states of 229Th3+ using a high-precision relativistic all-order approach. By combining these calculations with measurements of the 6d and 5f hyperfine constants [C. J. Campbell et al., Phys. Rev. Lett. 106, 223001 (2011)], we determine the magnetic dipole μ=0.360(7)μ_B and the electric-quadrupole Q=3.11(6) eb moments of the 229Th nucleus. Our value for μis five times more accurate and is 22% smaller than the best previous value μ=0.46(4) μ_B [S. Gerstenkorn et al., J. Phys. (Paris) 35, 483 (1974)], while our value for Q is the same, but 2.5 times more accurate than the 2011 result. A systematic study of hyperfine structure in eight other monovalent atoms supports our claim of 2% level uncertainty for $μ$ and Q in 229Th+3.
Motivation & Objective
- Determine the magnetic dipole and electric quadrupole moments of the 229Th nucleus with high precision to support nuclear clock development.
- Establish a reliable theoretical framework for calculating hyperfine constants in heavy, open-shell ions like 229Th³⁺.
- Benchmark the accuracy of relativistic all-order methods using hyperfine constants in other monovalent atoms (e.g., Ba⁺, Ra⁺, Fr).
- Enable future extraction of the nuclear magnetic octupole moment through high-resolution spectroscopy of hyperfine intervals.
- Improve constraints on temporal variations of fundamental constants using 229Th-based systems.
Proposed method
- Employ a relativistic linearized coupled-cluster (all-order) method including single, double, and partial triple excitations to compute hyperfine matrix elements.
- Calculate theoretical ratios (A/μ)th and (B/Q)th for 229Th³⁺ states using high-precision atomic structure calculations.
- Combine these theoretical ratios with measured hyperfine constants (Aexp and Bexp) from laser spectroscopy of 6d and 5f states in 229Th³⁺ to extract μ and Q.
- Validate the method by comparing theoretical hyperfine constants with experimental values in 133Cs, 137Ba⁺, 201Hg⁺, 210Fr, and 226Ra⁺, achieving agreement within 1–3%.
- Assess uncertainty through correlation corrections and spread across multiple states (6d₃/₂, 5f₅/₂, 5f₇/₂), confirming 2% uncertainty for μ and Q.
- Estimate finite magnetization distribution effects for 7s and 7p₁/₂ states, finding potential overestimation but consistent with 1% uncertainty when scaled.
Experimental results
Research questions
- RQ1What are the magnetic dipole and electric quadrupole moments of the 229Th nucleus with sub-2% uncertainty?
- RQ2Can the relativistic all-order method reliably predict hyperfine constants in Th³⁺ and other monovalent ions with high accuracy?
- RQ3How do correlation corrections and state-dependent effects influence the uncertainty in extracted nuclear moments?
- RQ4What is the potential for measuring the nuclear magnetic octupole moment in 229Th³⁺ using high-resolution microwave spectroscopy?
- RQ5To what extent can improved hyperfine measurements reduce uncertainty in μ and Q beyond the current 2% level?
Key findings
- The magnetic dipole moment of 229Th is determined as μ = 0.360(7) μB, five times more precise and 22% smaller than the previous best value of 0.46(4) μB.
- The electric quadrupole moment is found to be Q = 3.11(6) eb, with 2.5 times better precision than the prior 2011 result.
- The uncertainty in both μ and Q is estimated at 2%, validated by consistency across multiple electronic states and benchmarking against other ions.
- Correlation corrections for hyperfine constants vary significantly between 6d₃/₂, 5f₅/₂, and 5f₇/₂ states, with relative corrections ranging from -1.3% to +1.3%.
- Improved measurements of hyperfine intervals in 6d₃/₂ and 5f₅/₂ states to 0.3% accuracy could reduce the uncertainty in μ to 1% or better.
- Theoretical predictions for the 7s and 7p₁/₂ states suggest finite magnetization distribution corrections of 3.1% and 1.1%, respectively, but these may be overestimated; scaled values support 1% uncertainty.
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This review was created by AI and reviewed by human editors.