Large quadrupole deformation in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mmultiscripts> <mml:mi>Ne</mml:mi> <mml:mprescripts/> <mml:none/> <mml:mn>20</mml:mn> </mml:mmultiscripts> </mml:math> challenges rotor model and modern theory
Bibliographic record
Abstract
The spectroscopic quadrupole moment of the first excited state, ${Q}_{{}_{S}}({2}_{1}^{+})$, at 1.634 MeV in $^{20}\mathrm{Ne}$ was determined from sensitive reorientation-effect Coulomb-excitation measurements using a heavy target and safe energies well below the Coulomb barrier. Particle-$\ensuremath{\gamma}$ coincidence measurements were collected at iThemba LABS with a digital data-acquisition system using the AFRODITE array coupled to an annular, doubled-sided silicon detector. A precise value of ${Q}_{{}_{S}}({2}_{1}^{+})=\ensuremath{-}0.22(2)\phantom{\rule{0.16em}{0ex}}e\mathrm{b}$ was determined at backward angles in agreement with the only safe-energy measurement prior to this work, ${Q}_{{}_{S}}({2}_{1}^{+})=\ensuremath{-}0.23(8)\phantom{\rule{0.16em}{0ex}}e\mathrm{b}$. This result adopts $1\ensuremath{\hbar}\ensuremath{\omega}$ shell-model calculations of the nuclear dipole polarizability of the ${2}_{1}^{+}$ state that contributes to the effective quadrupole interaction and determination of ${Q}_{{}_{S}}({2}_{1}^{+})$. It disagrees, however, with the ideal rotor model for axially symmetric nuclei by almost $3\ensuremath{\sigma}$. Larger discrepancies are computed by modern state-of-the-art calculations performed in this and prior work, including ab initio shell model with chiral effective interactions and the multireference relativistic energy density functional (MR-EDF) model. The intrinsic nucleon density of the ${2}_{1}^{+}$ state in $^{20}\mathrm{Ne}$ calculated with the MR-EDF model illustrates the presence of $\ensuremath{\alpha}$ clustering, which explains the largest discrepancy with the rotor model found in the nuclear chart and motivates the explicit inclusion of $\ensuremath{\alpha}$ clustering for full convergence of $E2$ collective properties.
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How this classification was reachedexpand
Full frame machine prediction
Teacher imitationNot calibrated prevalence, not ground truth. Human validation pending. The Gemma side is a direct model label for every work in the frame, read from the title-only record. The Codex side is a classifier learned from the 10,348 direct Codex labels and calibrated to design-weighted sample rates; fields without enough sample support carry no Codex call. Candidate is the union of the two sides; consensus is their intersection. These outputs are machine_predicted_unvalidated and are not human labels.
Distilled classifier scores by category (both heads)
| Category | Codex | Gemma |
|---|---|---|
| Metaresearch | 0.001 | 0.001 |
| Meta-epidemiology (narrow) | 0.001 | 0.000 |
| Meta-epidemiology (broad) | 0.000 | 0.000 |
| Bibliometrics | 0.001 | 0.001 |
| Science and technology studies | 0.001 | 0.000 |
| Scholarly communication | 0.001 | 0.002 |
| Open science | 0.001 | 0.001 |
| Research integrity | 0.001 | 0.001 |
| Insufficient payload (model declined to judge) | 0.144 | 0.034 |
Machine scores (provisional)
The two teacher heads of the student model, read on this work. A score orders the frame for review; it never asserts a category, and the validation status ships verbatim with every row.
Baseline scores from an immature model (maturity gate not passed, 7 training rounds). Scores rank; they never assert a category.
score_only:v0-immature-baseline · verbatim from the scoring run: score_only means the number may rank works, and no category label ships from itClassification
machine, unvalidatedMachine predicted; a candidate call from one source (direct Gemma or distilled Codex), not a consensus.
How this classification was reached, model by model and score by score, is at the end of the page under "How this classification was reached".