PaperPanorama

Nuclear Theory·nucl-th

Wednesday·February 19, 2025

6 papers4 primary·2 cross-listed

  1. 05

    A Precise Determination of from the Heavy Jet Mass Distribution

    Miguel A. Benitez🇪🇸 · Arindam Bhattacharya🇺🇸 · Andre H. Hoang🇦🇹 · Vicent Mateu🇪🇸 · Matthew D. Schwartz🇺🇸 · Iain W. Stewart🇦🇹 · Xiaoyuan Zhang🇺🇸

    A global fit for is performed on available data for the heavy jet mass distribution. The state-of-the-art theory prediction includes fixed-order results, NLL dijet resummation, NLL Sudakov shoulder resummation, and a first-principles treatment of power corrections in the dijet region. Theoretical correlations are incorporated through a flat random-scan covariance matrix. The global fit results in , compatible with similar determinations from thrust and -parameter. Dijet resummation is essential for a robust fit, as it engenders insensitivity to the fit-range lower cutoff; without resummation the fit-range sensitivity is overwhelming. In addition, we find evidence for a negative power correction in the trijet region if and only if Sudakov shoulder resummation is included.

    hep-phhep-exnucl-exnucl-th29 citations
  2. 06

    Extreme Shape Coexistence Observed in Co

    Cade Dembski · Artemis Spyrou · B. Alex Brown · Sean N. Liddick · Hannah C. Berg · Darren L. Bleuel · Katherine Childers · Benjamin P. Crider · Alexander C. Dombos · Erin C. Good · Caley Harris · Ann-Cecilie Larsen and 13 other authors

    The shape of the atomic nucleus is a property which underpins our understanding of nuclear systems, impacts the limits of nuclear existence, and enables probes of physics beyond the Standard Model. Nuclei can adopt a variety of shapes, including spheres, axially deformed spheroids, and pear shapes. In some regions of the nuclear chart where a spherical nucleus would naively be expected, deformed nuclear states can result from collective action of constituent protons and neutrons. In a small subset of nuclei both spherical and deformed nuclear states have been experimentally observed, a phenomenon termed shape coexistence. We present spectroscopic evidence for the coexistence of spherical and deformed states in Co, separated by less than 275~keV. This close degeneracy of levels with the same and different shapes demonstrates an extreme example of shape coexistence resulting from the interplay of independent particle motion and collective behavior in highly unstable nuclear systems and identifies the Co isotopes as a transition point between deformed ground states observed in the Cr isotopes and spherical configurations observed in the closed-shell Ni isotopes.

    nucl-exnucl-thCommun.Phys.(2025)·1 citation

Affiliations

first authorsco-authorsvia INSPIRE