Nuclear Science
Parent: Physical Sciences
eScholarship stats: History by Item for March through June, 2026
| Item | Title | Total requests | 2026-06 | 2026-05 | 2026-04 | 2026-03 |
|---|---|---|---|---|---|---|
| 2dj9p3h4 | ENDF/B-VIII.0: The 8th Major Release of the Nuclear Reaction Data Library with CIELO-project Cross Sections, New Standards and Thermal Scattering Data | 837 | 196 | 233 | 224 | 184 |
| 3tr0t9cz | Differential measurements of jet substructure and partonic energy loss in Au + Au collisions at sNN=200 GeV | 782 | 253 | 231 | 187 | 111 |
| 5vj6n2qt | Measurement of an excess of B¯→D(*)τ-ν¯τ decays and implications for charged Higgs bosons | 761 | 156 | 229 | 194 | 182 |
| 3pw5g035 | Final Result of the Majorana Demonstrator’s Search for Neutrinoless Double-β Decay in Ge76 | 687 | 140 | 167 | 201 | 179 |
| 2z08p1g4 | Constraints for stellar electron-capture rates on Kr86 via the Kr86(t,He3+γ)Br86 reaction and the implications for core-collapse supernovae | 679 | 38 | 128 | 267 | 246 |
| 68n4j65r | Centrality dependence of inclusive J/ψ production in p-Pb collisions at sNN=5.02 TeV | 655 | 91 | 184 | 169 | 211 |
| 8br9m8hw | Deep Underground Science and Engineering Laboratory - Preliminary Design Report | 653 | 132 | 185 | 175 | 161 |
| 3vj2n57d | In situ diagnostics of the crystal-growth process through neutron imaging: application to scintillators | 616 | 48 | 504 | 42 | 22 |
| 92h5v1x8 | PRODUCTION AND DECAY OF * (1820) | 566 | 5 | 527 | 16 | 18 |
| 0g69b4vb | SEARCHES FOR TIME-DEPENDENT NEUTRINO SOURCES WITH ICECUBE DATA FROM 2008 TO 2012 | 548 | 47 | 44 | 394 | 63 |
| 8sq6520t | Heavy quarkonium: progress, puzzles, and opportunities | 520 | 111 | 140 | 125 | 144 |
| 4cf804vw | Constraints on jet quenching in p–Pb collisions at s NN = 5.02 TeV measured by the event-activity dependence of semi-inclusive hadron-jet distributions | 518 | 106 | 99 | 110 | 203 |
| 80x9f381 | Lawson Criterion for Ignition Exceeded in an Inertial Fusion Experiment | 506 | 161 | 128 | 124 | 93 |
| 4384w4mw | Search for the W-exchange decays B0→Ds(*)-Ds(*)+ | 487 | 133 | 140 | 133 | 81 |
| 2r68z2db | The Present and Future of QCD | 483 | 92 | 92 | 146 | 153 |
| 11k10948 | The Physics of the B Factories | 477 | 109 | 110 | 95 | 163 |
| 7jm9d65z | Physics with CEBAF at 12 GeV and future opportunities | 461 | 113 | 120 | 113 | 115 |
| 3fh431f8 | All-sky Neutrino Point-source Search with IceCube Combined Track and Cascade Data | 412 | 81 | 104 | 102 | 125 |
| 14q1319v | Secondary neutron production from thick target deuteron breakup | 393 | 88 | 135 | 79 | 91 |
| 7vz406nv | Nanodiamond-Rich Layer across Three Continents Consistent with Major Cosmic Impact at 12,800 Cal BP | 386 | 87 | 131 | 85 | 83 |
| 4qk062kd | RADAI: A Large-Scale Realistic Dataset for Radiation Detection Algorithm Development | 362 | 94 | 84 | 93 | 91 |
| 78f398d8 | Search for Neutrino Doublets and Triplets Using 11.4 yr of IceCube Data | 361 | 117 | 83 | 82 | 79 |
| 6zs3247s | Dynamics and observational signatures of core-collapse supernovae with central engines: hydrodynamics simulations with Monte Carlo post-processing | 354 | 70 | 121 | 163 | |
| 4866b17x | Hot QCD White Paper | 352 | 75 | 85 | 95 | 97 |
| 7xn8533z | Superconducting ECR ion source: From 24-28 GHz SECRAL to 45 GHz fourth generation ECR | 351 | 99 | 116 | 77 | 59 |
| 8t67641k | Abundances of Uranium and Thorium Elements in Earth Estimated by Geoneutrino Spectroscopy | 351 | 68 | 102 | 95 | 86 |
| 17n103v7 | Combined Measurement of the Higgs Boson Mass in pp Collisions at s=7 and 8 TeV with the ATLAS and CMS Experiments | 346 | 48 | 88 | 101 | 109 |
| 4s1159jr | Real-Time, Adaptive Radiological Anomaly Detection and Isotope Identification Using Non-Negative Matrix Factorization | 346 | 49 | 182 | 56 | 59 |
| 0tc9r96f | Enhanced Isomer Population via Direct Irradiation of Solid-Density Targets Using a Compact Laser-Plasma Accelerator | 342 | 81 | 92 | 83 | 86 |
| 7xr7v8xh | Explaining machine-learning models for gamma-ray detection and identification | 339 | 61 | 90 | 119 | 69 |
| 3398k4bn | Semi-automatic image annotation using 3D LiDAR projections and depth camera data | 336 | 86 | 123 | 70 | 57 |
| 9mb0s0p8 | Review of Particle Physics | 335 | 118 | 76 | 85 | 56 |
| 14z1h9gr | Web‐based visual data exploration for improved radiological source detection | 334 | 96 | 109 | 69 | 60 |
| 06w3q8dx | ANTARES and IceCube Combined Search for Neutrino Point-like and Extended Sources in the Southern Sky | 333 | 98 | 114 | 56 | 65 |
| 0d03d73k | The STAR Forward Silicon Tracker | 331 | 35 | 55 | 189 | 52 |
| 4739131k | On the discovery of new elements (IUPAC/IUPAP Provisional Report) | 330 | 39 | 199 | 45 | 47 |
| 5sg13227 | Interpolation of computed gamma-ray detector response functions | 328 | 37 | 103 | 76 | 112 |
| 0p92q5md | Toward the Discovery of New Elements: Production of Livermorium (Z=116) with Ti50 | 327 | 65 | 103 | 95 | 64 |
| 61v754fp | Solar fusion cross sections. II. The pp chain and CNO cycles | 326 | 66 | 107 | 97 | 56 |
| 72r616tm | Physics case for quarkonium studies at the Electron Ion Collider | 323 | 82 | 91 | 92 | 58 |
| 48d093gz | Characterization of the Thermal Properties of Ir/Pt Bilayer Transition Edge Sensors | 322 | 93 | 86 | 86 | 57 |
| 5q04m7cg | Prompt and non-prompt J/ψ production and nuclear modification at mid-rapidity in p–Pb collisions at sNN=5.02 TeV | 321 | 49 | 137 | 97 | 38 |
| 5k06s976 | The Gerda experiment for the search of 0νββ decay in 76Ge | 319 | 105 | 78 | 81 | 55 |
| 8833b038 | Review of Particle Physics | 319 | 113 | 55 | 60 | 91 |
| 00g7374m | Combined search for neutrinos from dark matter self-annihilation in the Galactic Center with ANTARES and IceCube | 318 | 99 | 89 | 72 | 58 |
| 69t5z366 | Initial measurement of reactor antineutrino oscillation at SNO+ | 311 | 87 | 80 | 75 | 69 |
| 8dp1z4bh | Gluons and the quark sea at high energies: distributions, polarization, tomography | 308 | 89 | 78 | 53 | 88 |
| 1q8770f0 | Probing quantum phenomena through photoproduction in relativistic heavy-ion collisions | 307 | 63 | 93 | 77 | 74 |
| 0vj1047r | Chiral Effective Field Theory and the High-Density Nuclear Equation of State | 306 | 51 | 77 | 100 | 78 |
| 2px009hq | Achievement of Target Gain Larger than Unity in an Inertial Fusion Experiment | 306 | 65 | 94 | 83 | 64 |
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