Nuclear Science
Parent: Physical Sciences
eScholarship stats: Breakdown by Item for August through November, 2024
Item | Title | Total requests | Download | View-only | %Dnld |
---|---|---|---|---|---|
8833b038 | Review of Particle Physics | 177 | 43 | 134 | 24.3% |
12q424wz | Search for Continuous and Transient Neutrino Emission Associated with IceCube’s Highest-energy Tracks: An 11 yr Analysis | 159 | 118 | 41 | 74.2% |
4k96h755 | A CUPID Li2100MoO4 scintillating bolometer tested in the CROSS underground facility | 159 | 1 | 158 | 0.6% |
5zr5w6xb | IceCat-1: The IceCube Event Catalog of Alert Tracks | 146 | 123 | 23 | 84.2% |
3z96h3pc | Search for Correlations of High-energy Neutrinos Detected in IceCube with Radio-bright AGN and Gamma-Ray Emission from Blazars | 137 | 119 | 18 | 86.9% |
8m8301pk | Constraining High-energy Neutrino Emission from Supernovae with IceCube | 137 | 114 | 23 | 83.2% |
17g5t56q | Searches for Neutrinos from Large High Altitude Air Shower Observatory Ultra-high-energy γ-Ray Sources Using the IceCube Neutrino Observatory | 134 | 119 | 15 | 88.8% |
17p1277m | A Search for IceCube Sub-TeV Neutrinos Correlated with Gravitational-wave Events Detected By LIGO/Virgo | 130 | 114 | 16 | 87.7% |
1s79s9bj | Thermal conductivity measurements of PTFE and Al2O3 ceramic at sub-Kelvin temperatures | 125 | 13 | 112 | 10.4% |
11k10948 | The Physics of the B Factories | 116 | 9 | 107 | 7.8% |
7bd5z9hj | Constraints on Populations of Neutrino Sources from Searches in the Directions of IceCube Neutrino Alerts | 115 | 96 | 19 | 83.5% |
7d8274zw | Limits on Neutrino Emission from GRB 221009A from MeV to PeV Using the IceCube Neutrino Observatory | 115 | 105 | 10 | 91.3% |
18w717zp | Search for sub-TeV Neutrino Emission from Novae with IceCube-DeepCore | 110 | 87 | 23 | 79.1% |
3k1843rw | Bulk properties of the system formed in Au+Au collisions at sNN=14.5 GeV at the BNL STAR detector | 103 | 18 | 85 | 17.5% |
9fb704x9 | Comparative scintillation performance of EJ-309, EJ-276, and a novel organic glass | 102 | 20 | 82 | 19.6% |
7sr999w8 | Machine Learning Techniques for Pile-Up Rejection in Cryogenic Calorimeters | 100 | 24 | 76 | 24.0% |
8rq0t2fp | CUORE opens the door to tonne-scale cryogenics experiments | 99 | 8 | 91 | 8.1% |
0mx946m8 | Search for GeV-scale dark matter annihilation in the Sun with IceCube DeepCore | 97 | 15 | 82 | 15.5% |
79g6x7k4 | Characterization of cubic Li2100MoO4 crystals for the CUPID experiment | 97 | 16 | 81 | 16.5% |
1pp29372 | Multihadronic events at Ec.m.=29 GeV and predictions of QCD models from Ec.m.=29 GeV to Ec.m.=93 GeV | 96 | 7 | 89 | 7.3% |
8bd7v3bb | KamLAND’s search for correlated low-energy electron antineutrinos with astrophysical neutrinos from IceCube | 95 | 16 | 79 | 16.8% |
6831d5df | Spectroscopic study of a possible Λnn resonance and a pair of ΣNN states using the (e,e′K+) reaction with a tritium target | 94 | 12 | 82 | 12.8% |
79f5x4p5 | Strange hadron production in Au+Au collisions at sNN=7.7, 11.5, 19.6, 27, and 39 GeV | 94 | 14 | 80 | 14.9% |
2xr183nn | Measurement of the W+W- cross section in pp collisions at s=8 TeVand limits on anomalous gauge couplings | 93 | 3 | 90 | 3.2% |
5p28d02g | Measurement of R=σL/σT and the separated longitudinal and transverse structure functions in the nucleon-resonance region | 93 | 16 | 77 | 17.2% |
61v5b2r5 | Probing criticality with deep learning in relativistic heavy-ion collisions | 93 | 16 | 77 | 17.2% |
7mw4z049 | Coherent diffractive photoproduction of $ρ^{0}$ mesons on gold nuclei at RHIC | 93 | 4 | 89 | 4.3% |
5m605672 | Detailed analysis of excited state systematics in a lattice QCD calculation of $g_A$ | 91 | 13 | 78 | 14.3% |
58r3c4sx | Can We Detect the Quantum Nature of Weak Gravitational Fields? | 89 | 14 | 75 | 15.7% |
6j8510dj | Initial performance of the CUORE-0 experiment | 89 | 11 | 78 | 12.4% |
7dj1d5sr | Design of the Superconducting Magnet System for a 45 GHz ECR Ion Source | 89 | 13 | 76 | 14.6% |
3fs0d0q3 | Status and prospects for CUORE | 88 | 15 | 73 | 17.0% |
82x5v66c | ADC Nonlinearity Correction for the Majorana Demonstrator | 88 | 11 | 77 | 12.5% |
8pp9z5bd | Precise measurement of 2νββ decay of 100Mo with the CUPID-Mo detection technology | 88 | 8 | 80 | 9.1% |
9q3550m0 | Three-pion Hanbury-Brown-Twiss correlations in relativistic heavy-ion collisions from the STAR experiment | 88 | 2 | 86 | 2.3% |
09v3h754 | Effect of event selection on jetlike correlation measurement in d+Au collisions at sNN=200 GeV | 87 | 6 | 81 | 6.9% |
9cr1b30s | Modification of Z 0 leptonic invariant mass in ultrarelativistic heavy ion collisions as a measure of the electromagnetic field | 87 | 11 | 76 | 12.6% |
70w6x41n | The BABAR detector | 86 | 63 | 23 | 73.3% |
4040k5mh | Dielectron production in proton-proton and proton-lead collisions at sNN=5.02TeV | 85 | 6 | 79 | 7.1% |
4sf7n3pc | Nuclear Physics Network Requirements Review: One-Year Update | 85 | 39 | 46 | 45.9% |
68g1b51r | Measurement of transverse single-spin asymmetries of π0 and electromagnetic jets at forward rapidity in 200 and 500 GeV transversely polarized proton-proton collisions | 85 | 5 | 80 | 5.9% |
7qh3z1dc | Measurements of the branching fractions of exclusive charmless B meson decays with eta(') or omega mesons. | 85 | 1 | 84 | 1.2% |
3tr0t9cz | Differential measurements of jet substructure and partonic energy loss in Au + Au collisions at sNN=200 GeV | 84 | 17 | 67 | 20.2% |
5mv3x1v4 | Search for Multi-flare Neutrino Emissions in 10 yr of IceCube Data from a Catalog of Sources | 84 | 57 | 27 | 67.9% |
8r37x6z9 | Constraints on neutrino emission from nearby galaxies using the 2MASS redshift survey and IceCube | 84 | 23 | 61 | 27.4% |
99q7p65m | First neutrinoless double beta decay results from CUORE-0 | 84 | 3 | 81 | 3.6% |
07j5920q | Searches for Neutrinos from Gamma-Ray Bursts Using the IceCube Neutrino Observatory | 83 | 76 | 7 | 91.6% |
2qm3f1tr | Lattice determination of I=0 and 2 ππ scattering phase shifts with a physical pion mass | 82 | 12 | 70 | 14.6% |
9sw1s6k8 | Search for lepton-flavor-violating decays D0→X0e±μ∓ | 82 | 12 | 70 | 14.6% |
5wr6s8xd | B-meson decays to η′ρ, η′f0, and η′K* | 81 | 2 | 79 | 2.5% |
Note: Due to the evolving nature of web traffic, the data presented here should be considered approximate and subject to revision. Learn more.