First Kaonic Boron Isotopes Measurements with SIDDHARTA-2 at DAΦNEA precision measurement of X-ray transitions in kaonic boron, performed by the SIDDHARTA-2 collaboration at the DAΦNE collider, is reported. The energies and yields of the 5g→4f and…D Sirghi, M Iliescu, F Sgaramella et al.·Jul 1, 2026SaveLearn
New limits on the Pauli forbidden transitions in 12C nuclei obtained with the complete Borexino datasetThe Pauli exclusion principle (PEP) was tested for nucleons in 12C nuclei using the Borexino dataset from 2007 to 2021. %the complete Borexino detector data. The approach consists of…Borexino collaboration, D. Basilico, G. Bellini et al.·Jul 1, 2026SaveLearn
Precision measurement of radiative neutron eta-decay: methodology and systematic effectsIn the Standard Model the free neutron decays to a proton, an electron, and an antineutrino along with a continuous spectrum of photons. In 2016 the RDK II collaboration reported on a measurement of…J. S. Nico, R. Alarcon, M. J. Bales et al.·Jun 29, 2026SaveLearn
Dineutron clustersThe dineutron is a spatially compact two-neutron cluster, which is expected to appear in a low-density part of nuclei. In recent years, there has been rapid progress in experimental and theoretical…Takashi Nakamura, Kouichi Hagino, Yosuke Kondo·Jun 27, 2026SaveLearn
Multiplicity dependence of the size of the common hadron emission source in pp collisions at the LHCFemtoscopic analysis can shed light on hadron production in pp collisions. In this paper, proton-proton correlations measured in collisions at s=13.6 TeV recorded with the ALICE detector at…ALICE Collaboration·Jun 26, 2026SaveLearn
Half-Life Measurements of 110Sn, 113Sn, 117mSn, and 123mSn Produced via Photon Activation of Natural TinWe report independent determinations of the ground-state half-lives of 110Sn, 113Sn, and the isomeric states 117mSn (Jπ = 11/2-) and 123mSn (J$π =…O Nusair, D Devries, M Toto-Gonzalez·Jun 25, 2026SaveLearn
Shape Coexistence in 94Zr from a Model-Independent AnalysisLow-lying states of 94Zr were investigated via low-energy multi-step Coulomb excitation. From the measured γ-ray yields, black16 reduced blackE2 transition…N. Marchini, M. Rocchini, M. Zielinska et al.·Jun 25, 2026SaveLearn
Low lying excitations in 150PmThe low lying excitations in odd-odd 150Pm have been studied through proton induced reaction with an array of five Compton suppressed Clover HPGe and one segmented planar Ge detectors. The…A. Pal, S. Basak, T. Bhattacharjee et al.·Jun 23, 2026SaveLearn
Measurements of Bremsstrahlung-Averaged Cross Sections for Reactions on Natural Nickel Targets at Eendpoint = 40MeVBremsstrahlung activation measurements were performed to study the production of 57Ni, 56Ni, 58Co, 57Co, 56Co, and…O. Nusair, N. Solomon, M. Toro-Gonzalez et al.·Jun 22, 2026SaveLearn
Single Particle Excitations, Band Structures and Octupole Correlation in 65ZnThe excitation scheme of the 65Zn (Z = 30, N = 35) nucleus has been probed following its population in the 63Cu(α,pn) reaction at Ebeam = 30 MeV and using an array of Compton…Anil Sharma, S. Nandi, S. S. Dutta et al.·Jun 22, 2026SaveLearn
Development of a Neural Network-Based Background Suppression Technique for ΣN Cusp Spectroscopy at J-PARCA clear spectral enhancement, known as the ``ΣN cusp'', has been observed near the ΣN threshold in the d(K-, π-) reaction. To understand the dynamical origin of this enhancement, the…K. Amemiya, Y. Ichikawa, S. H. Hayakawa et al.·Jun 22, 2026SaveLearn
Hyper-Nuclei 4ΛHe Production in sNN = 3 GeV Au+Au collisions at RHICThe STAR experiment reports the first measurement of the 4ΛHe hyper-nuclei yield as a function of rapidity and transverse momentum in 0-50% central Au+Au collisions at $sNN…The STAR Collaboration·Jun 21, 2026SaveLearn
Evidence for parton energy loss in oxygen-oxygen collisions at s NN=5.36 TeVUltra-relativistic heavy-ion collisions create a hot and dense medium of deconfined quarks and gluons, the quark-gluon plasma (QGP), in which parton energy loss ("jet quenching") is a key…ALICE Collaboration·Jun 19, 2026SaveLearn
Scaling Properties of the Δγ Correlator: Constraints on Background and CME-Sensitive Charge Separation in Heavy-Ion CollisionsThe scaling properties of the Δγ correlator are used to investigate charge separation associated with the chiral magnetic effect (CME) in p+Au, d+Au, Ru+Ru, Zr+Zr, and Au+Au collisions at…Roy A. Lacey, Niseem Magdy·Jun 19, 2026SaveLearn
Observation of centrality-dependent dijet transverse momentum imbalance in O+O and Ne+Ne collisions at sNN = 5.36 TeV with the ATLAS detectorThe ATLAS experiment presents an observation of a centrality-dependent dijet transverse momentum imbalance in O+O and Ne+Ne collisions at a nucleon-nucleon center-of-mass energy of 5.36 TeV at the…ATLAS Collaboration·Jun 18, 2026SaveLearn
Measurements of charged-particle pseudorapidity and transverse momentum distributions in O+O and Ne+Ne collisions at s_NN = 5.36 TeV with the ATLAS detectorMeasurements of charged-particle transverse momentum spectra, multiplicity, and mean transverse momentum are presented as a function of pseudorapidity and collision centrality in O+O and Ne+Ne…ATLAS Collaboration·Jun 18, 2026SaveLearn
Probing Strange-Quark Hadronization via (Multi-)Strange Hadron Multiplicity Distributions in Small Collision Systems with ALICEStrangeness enhancement is defined as the increased relative production of strange hadrons in heavy-ion collisions compared to proton--proton (pp) interactions. It was originally proposed as one of…Sara Pucillo·Jun 18, 2026SaveLearn
Precision mass measurements of multistrange baryons and their antiparticlesThe Ω- baryon, composed of three strange quarks (sss), was predicted by the quark model and discovered in 1964, playing a pivotal role in establishing quarks as fundamental constituents of matter.…ALICE Collaboration·Jun 18, 2026SaveLearn
Modification of jet-energy flow in heavy-ion collisionsThe ALICE Collaboration presents the first measurements of the jet-energy flow (Δp T) observable in proton-proton and heavy-ion collisions. Jets are excellent probes for the quark-gluon…ALICE Collaboration·Jun 18, 2026SaveLearn
Probing flavor effects in the QCD parton shower using D0-tagged jet angularities in proton-proton collisions at s = 5.02 TeVThe ALICE Collaboration presents the first measurements of D0-tagged jet angularities in proton-proton (pp) collisions at s = 5.02 TeV. Jet angularities are powerful substructure…ALICE Collaboration·Jun 18, 2026SaveLearn
Direct Measurement of the 212Pb and 214Pb β Decay Branching Ratios with the XENONnT ExperimentWe present precision measurements of 212Pb and 214Pb β decay branching ratios using 220Rn and 222Rn calibration data from the XENONnT…E. Aprile, J. Aalbers, K. Abe et al.·Jun 18, 2026SaveLearn
First direct measurement of 48Ca single β-decay Q value with the TITAN Penning trapNeutrinoless double β-decay (0νββ), if observed, would provide unequivocal evidence of physics beyond the Standard Model. 48Ca is an interesting candidate system to study because it has the…S. Kakkar, D. Perera, J. Ash et al.·Jun 18, 2026SaveLearn
Hofstadter-Herman Visualization as a Diagnostic Tool for Systematic Effects in Electromagnetic Form Factor ExtractionsThe internal charge and magnetization distributions of the proton are characterized by electromagnetic form factors GE and GM. They are experimentally extracted via Rosenbluth separation, which…Tyler Williams, Jennifer Rittenhouse West, Douglas W. Higinbotham et al.·Jun 18, 2026SaveLearn
The electromagnetic decay of 250mNo and the stability of neutron deficient Rf isotopesThe electromagnetic decay of the ≈40 μs isomer of 250No has been investigated using the Geant4 toolkit for the simulations of the interaction of particles through matter. It…A. Lopez-Martens, K. Hauschild, R. Chakma et al.·Jun 17, 2026SaveLearn
Azimuthal Anisotropy Scaling Functions for Identified Particle and Anti-Particle Species across Beam Energies: Insights into Baryon Junction EffectsAzimuthal anisotropy scaling functions are constructed from species-resolved anisotropy measurements in Pb+Pb (sNN=2.76, 5.02~TeV) and Au+Au (sNN=7.7--200~GeV) collisions to…Roy A. Lacey·Jun 17, 2026SaveLearn