研究 Ru 和 Pd 同位素的精确质量测量对机器学习质量建模的影响

W. S. Porter, B. Liu, D. Ray, A. A. Valverde, M. Li, M. R. Mumpower, M. Brodeur, D. P. Burdette, N. Callahan, A. Cannon, J. A. Clark, D. E. M. Hoff, A. M. Houff, F. G. Kondev, A. E. Lovell, A. T. Mohan, G. E. Morgan, C. Quick, G. Savard, K. S. Sharma, T. M. Sprouse, L. Varriano
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引用次数: 0

摘要

原子质量是我们理解核结构、天体物理学和基本对称性的基础量。然而,为原子核结合能创建一个预测性全局模型的长期目标仍然是一个重大挑战,这促使我们需要对原子质量进行精确测量,以作为模型开发的锚点。我们介绍了在阿贡国家实验室的加利福尼亚稀有同位素育种升级设施中使用加拿大潘宁陷阱质谱仪对富含中子的 Ru 和 Pd 同位素进行的精确质量测量。通过相位-成像-共振技术测量了^{108}$Ru、^{110}$Ru 和^{116}$Pd 的质量,其相对质量精度大约为 10^{-8}。这些质量数据与物理可解释机器学习(PIML)模型结合使用,该模型使用混合密度神经网络,通过高斯分布的混合来模拟质量的增加。本文介绍了新的质量数据对贝叶斯更新 PIML 模型的影响。
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Investigating the effects of precise mass measurements of Ru and Pd isotopes on machine learning mass modeling
Atomic masses are a foundational quantity in our understanding of nuclear structure, astrophysics and fundamental symmetries. The long-standing goal of creating a predictive global model for the binding energy of a nucleus remains a significant challenge, however, and prompts the need for precise measurements of atomic masses to serve as anchor points for model developments. We present precise mass measurements of neutron-rich Ru and Pd isotopes performed at the Californium Rare Isotope Breeder Upgrade facility at Argonne National Laboratory using the Canadian Penning Trap mass spectrometer. The masses of $^{108}$Ru, $^{110}$Ru and $^{116}$Pd were measured to a relative mass precision $\delta m/m \approx 10^{-8}$ via the phase-imaging ion-cyclotron-resonance technique, and represent an improvement of approximately an order of magnitude over previous measurements. These mass data were used in conjunction with the physically interpretable machine learning (PIML) model, which uses a mixture density neural network to model mass excesses via a mixture of Gaussian distributions. The effects of our new mass data on a Bayesian-updating of a PIML model are presented.
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Investigating the effects of precise mass measurements of Ru and Pd isotopes on machine learning mass modeling Addendum: Dielectron production in proton-proton and proton-lead collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV Coherent J/$ψ$ photoproduction at midrapidity in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV First measurement of $\mathrm{D_{s1}}(1^{+})(2536)^+$ and $\mathrm{D_{s2}^{*}(2^{+})(2573)^+}$ production in proton--proton collisions at $\sqrt{s} = 13$ TeV at the LHC Measurement of f$_{1}$(1285) production in pp collisions at $\mathbf{\sqrt{\textit s}}$ = 13 TeV
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