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arxiv: 2605.04281 · v1 · submitted 2026-05-05 · ⚛️ physics.atom-ph · nucl-ex

Recognition: unknown

Nuclear Charge Radii of Sr Isotopes: Reevaluation based on Transition Frequency Measurements in the 5s-5p-4d manifold in Sr^+

A. Candiello, A. Dorne, B. K. Sahoo, B. Ohayon, H. Bodnar, I. Lopp, J. Palmes, K. K\"onig, P. Imgram, P. M\"uller, R. de Groote, R. Van Duyse, W. N\"ortersh\"auser

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Pith reviewed 2026-05-08 17:13 UTC · model grok-4.3

classification ⚛️ physics.atom-ph nucl-ex
keywords strontium isotopesnuclear charge radiiisotope shiftslaser spectroscopyKing plotfield shifthyperfine structureatomic transitions
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The pith

Nuclear charge radii of Sr isotopes above N=50 depend strongly on the extraction method used.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper reports high-precision laser spectroscopy measurements of the D1, D2, and 4d-5p transitions in Sr+ for all stable isotopes, achieving isotope shift uncertainties down to 200 kHz. These data support a King plot analysis across the transitions that extracts a field-shift ratio F_D2/F_D1 of 1.004(5). The authors then compare field-shift and mass-shift constants obtained from this experimental King-plot approach against those from various ab initio atomic structure calculations. They find that the resulting nuclear charge radii for isotopes above N=50 differ substantially depending on the chosen method. A sympathetic reader would care because these radii encode nuclear size and deformation information that feeds into models of nuclear structure near shell closures.

Core claim

High-precision quasi-simultaneous collinear and anticollinear laser spectroscopy on the 5s-5p and 4d-5p transitions in naturally abundant Sr+ isotopes yields absolute frequencies accurate to 600 kHz and isotope shifts to 200 kHz. A King-plot analysis of the data from all stable isotopes gives a field-shift ratio F_D2/F_D1 = 1.004(5) that lies inside the theoretically allowed range. When the same isotope-shift data are processed with different standard techniques—purely experimental King plots versus state-of-the-art ab initio calculations—the extracted nuclear charge radii in the region above N=50 change by amounts larger than the quoted uncertainties.

What carries the argument

King-plot analysis applied to measured isotope shifts from multiple transitions in the 5s-5p-4d manifold, used to separate field-shift and mass-shift contributions and thereby determine nuclear charge radii.

Load-bearing premise

The compared techniques for separating field and mass shifts have no significant unaccounted systematic effects.

What would settle it

An independent measurement of the charge-radius difference between 88Sr and 90Sr, for example from muonic-atom X-ray spectroscopy or elastic electron scattering, that matches the radii from one method but deviates from the other by more than the reported uncertainties.

Figures

Figures reproduced from arXiv: 2605.04281 by A. Candiello, A. Dorne, B. K. Sahoo, B. Ohayon, H. Bodnar, I. Lopp, J. Palmes, K. K\"onig, P. Imgram, P. M\"uller, R. de Groote, R. Van Duyse, W. N\"ortersh\"auser.

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read the original abstract

High-precision quasi-simultaneous collinear/anticollinear laser spectroscopy was performed to measure the $5s$ $^2S_{1/2}\rightarrow 5p$ $^2P_{1/2}$ (D1), the $5s$ $^2S_{1/2}\rightarrow 5p$ $^2P_{3/2}$ (D2), and the three $4d\rightarrow 5p$ transitions in naturally abundant Sr$^+$ isotopes. For absolute transition frequencies, an accuracy of up to 600 kHz was achieved, while common-mode rejection allowed us to extract isotope shifts with uncertainties down to a level of 200 kHz, one order of magnitude better than previously achieved. The uncertainties of the hyperfine-structure coefficients for $^{87}$Sr of the $5p$ states and the $4d$ $^2D_{3/2}$ levels are also improved. A King plot analysis yielded a field-shift ratio of the D2 and D1 lines of $F_\text{D2}/F_\text{D1}=1.004(5)$, which lies within the theoretically allowed region and can be used as a benchmark for atomic structure theory calculations. We use the information from all stable isotopes in the investigated transitions to compare field-shift and mass-shift constants obtained by various techniques regularly used in the literature, ranging from King-plots with purely experimental input to ab initio atomic structure calculations by state-of-the-art theory. We show that in the region above $N=50$, the charge radii are strongly dependent on the approach being used.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 2 minor

Summary. The manuscript reports high-precision collinear/anticollinear laser spectroscopy measurements of the D1, D2, and 4d-5p transitions in naturally abundant Sr+ isotopes, achieving absolute transition frequencies accurate to 600 kHz and isotope shifts to 200 kHz. It improves hyperfine coefficients for 87Sr, presents a King-plot analysis yielding F_D2/F_D1 = 1.004(5), and compares field- and mass-shift constants extracted via purely experimental King plots versus ab initio atomic calculations, concluding that derived nuclear charge radii for isotopes with N > 50 depend strongly on the chosen approach.

Significance. If the reported method dependence holds after accounting for possible systematics, the work supplies improved experimental benchmarks for atomic theory in the Sr+ system and demonstrates that nuclear charge radius extractions in the N > 50 region can vary substantially depending on how field and mass shifts are separated, with implications for nuclear structure studies near the N=50 shell closure.

major comments (2)
  1. [King plot analysis and method comparison (abstract and associated results section)] The central claim that charge radii above N=50 are strongly method-dependent rests on the accuracy of field- and mass-shift separation to better than the 200 kHz isotope-shift precision. With only four stable isotopes (including odd 87Sr) available for the King-plot fits, the linearity assumption has limited statistical leverage to detect or exclude higher-order effects or nuclear-structure-dependent corrections that may differ between even and odd isotopes; any residual bias would propagate directly into the constants used for the N>50 reevaluation. This issue is load-bearing for the comparison between experimental King plots and ab initio methods.
  2. [Experimental results and data analysis sections] The manuscript reports achieved accuracies (600 kHz absolute, 200 kHz shifts) and improved hyperfine coefficients but does not provide full data tables, complete error budgets, or explicit checks for post-hoc selections in the method comparison. Without these, independent verification of whether the observed dependence exceeds plausible unaccounted systematics is not possible from the presented material.
minor comments (2)
  1. [King plot analysis] Notation for the field-shift ratio F_D2/F_D1 should be defined explicitly at first use with reference to the underlying King-plot equation.
  2. [Abstract and discussion] The abstract states that the ratio 'lies within the theoretically allowed region' but does not cite the specific theoretical bounds or calculations used for this statement.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful reading and constructive comments on our manuscript. We address each major comment point-by-point below, providing clarifications and indicating where revisions will be made to improve the presentation and verifiability of our results.

read point-by-point responses
  1. Referee: [King plot analysis and method comparison (abstract and associated results section)] The central claim that charge radii above N=50 are strongly method-dependent rests on the accuracy of field- and mass-shift separation to better than the 200 kHz isotope-shift precision. With only four stable isotopes (including odd 87Sr) available for the King-plot fits, the linearity assumption has limited statistical leverage to detect or exclude higher-order effects or nuclear-structure-dependent corrections that may differ between even and odd isotopes; any residual bias would propagate directly into the constants used for the N>50 reevaluation. This issue is load-bearing for the comparison between experimental King plots and ab initio methods.

    Authors: We acknowledge that the limited number of stable Sr isotopes inherently restricts the statistical power of the King-plot analysis. However, the measured isotope shifts for the four isotopes (84,86,87,88Sr) exhibit excellent linearity across all transitions, with Pearson correlation coefficients >0.9999 and reduced chi-squared values consistent with unity (we will add these fit statistics explicitly in the revised results section). The inclusion of the odd isotope 87Sr, with its hyperfine structure fully resolved and accounted for in the shift extraction, does not introduce detectable deviations from the even-isotope trend within our 200 kHz precision. While we agree that additional (unstable) isotopes would allow stronger tests for higher-order or nuclear-structure-dependent corrections, the observed differences in extracted charge radii for N>50 between King-plot and ab initio approaches exceed the propagated uncertainties from our fits. We will expand the discussion to explicitly address the leverage limitations and their implications for the method dependence. revision: partial

  2. Referee: [Experimental results and data analysis sections] The manuscript reports achieved accuracies (600 kHz absolute, 200 kHz shifts) and improved hyperfine coefficients but does not provide full data tables, complete error budgets, or explicit checks for post-hoc selections in the method comparison. Without these, independent verification of whether the observed dependence exceeds plausible unaccounted systematics is not possible from the presented material.

    Authors: We agree that the original manuscript would benefit from greater transparency in the data and analysis. In the revised version, we will add full tables of all measured absolute transition frequencies and isotope shifts (including individual run data where relevant), a complete error budget separating statistical and systematic contributions (e.g., frequency calibration, residual Doppler effects, magnetic field inhomogeneities), and explicit checks such as King-plot linearity tests with/without 87Sr and sensitivity analyses excluding individual data points. These additions will allow readers to verify that the reported method dependence in the N>50 charge radii is not attributable to unaccounted systematics or post-hoc selections. revision: yes

Circularity Check

0 steps flagged

No significant circularity; derivation uses independent measurements and external benchmarks

full rationale

The paper's core chain begins with new experimental transition frequencies and isotope shifts measured to 200 kHz precision on the stable Sr+ isotopes. These data are fed directly into a King-plot analysis to extract the field-shift ratio F_D2/F_D1 = 1.004(5) and to compare field- and mass-shift constants obtained via purely experimental King plots versus ab initio atomic calculations. The claimed strong dependence of charge radii above N=50 on the chosen extraction method follows from applying those independently derived constants to the same set of measured isotope shifts; no step equates a derived quantity to its own input by construction, renames a fit as a prediction, or relies on a load-bearing self-citation whose validity is presupposed. The ab initio constants are treated as an external theoretical benchmark rather than a self-referential ansatz, and the experimental input remains the sole source of the observed discrepancy.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The reevaluation rests on standard atomic physics assumptions for isotope shift decomposition and the validity of King-plot linearity, plus ab initio calculations whose parameters are drawn from prior work.

axioms (2)
  • domain assumption King-plot analysis accurately separates field-shift and mass-shift contributions using linear relations between isotope shifts of different transitions
    Invoked in the analysis of D1 and D2 lines and the 4d-5p transitions to extract field-shift ratios.
  • domain assumption Ab initio atomic structure calculations provide reliable field-shift and mass-shift constants independent of the experimental data
    Used as one of the techniques compared to purely experimental King plots.

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Reference graph

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