Odd-odd neutron-rich rhodium isotopes studied with the double Penning trap JYFLTRAPPrecision mass measurements of neutron-rich rhodium isotopes have been performed at the JYFLTRAP Penning trap mass spectrometer at the Ion Guide Isotope Separator On-Line (IGISOL) facility. We report…M. Hukkanen, W. Ryssens, P. Ascher et al.·Oct 19, 2022SaveLearn
First Simultaneous K-p → (0/) \, π0 Cross Sections Measurements at 98 MeV/cWe report the first simultaneous and independent measurements of the K-p → 0 \, π0 and K-p → \, π0 cross sections around 100 MeV/c kaon…Kristian Piscicchia, Magdalena Skurzok, Michael Cargnelli et al.·Oct 19, 2022SaveLearn
Collision-Induced Dissociation at TRIUMF's Ion Trap for Atomic and Nuclear scienceThe performance of high-precision mass spectrometry of radioactive isotopes can often be hindered by large amounts of contamination, including molecular species, stemming from the production of the…A. Jacobs, C. Andreoiu, J. Bergmann et al.·Oct 18, 2022SaveLearn
Measurements of azimuthal anisotropies at forward and backward rapidity with muons in high-multiplicity p-Pb collisions at s NN = 8.16 TeVThe study of the azimuthal anisotropy of inclusive muons produced in p-Pb collisions at s NN = 8.16 TeV, using the ALICE detector at the LHC is reported. The measurement of the…ALICE Collaboration·Oct 17, 2022SaveLearn
(2S) suppression in Pb-Pb collisions at the LHCThe production of the (2S) charmonium state was measured with ALICE in Pb-Pb collisions at s NN=5.02 TeV, in the dimuon decay channel. A significant signal was observed for the…ALICE Collaboration·Oct 17, 2022SaveLearn
(2S) production as a function of charged-particle multiplicity in pp collisions at s= 13 TeV and p--Pb collisions at sNN= 8.16 TeV with ALICE at the LHCThe self-normalised (2S) yields as a function of charged-particle multiplicity in pp collisions at s = 13 TeV and p--Pb collisions at sNN= 8.16 TeV, using the…Theraa Tork·Oct 17, 2022SaveLearn
Shake-up and shake-off effects in neutrinoless double-beta decayWe revisit the role of shake-up and shake-off effects in neutrinoless double-beta decay, following earlier work by Drukarev et al. We find in agreement with Drukarev et al. that the Q value of the…J. A. Detwiler, R. G. H. Robertson·Oct 17, 2022SaveLearn
Intermittency analysis of charged hadrons generated in Pb-Pb collisions at sNN= 2.76 TeV and 5.02 TeV using PYTHIA8/AngantyrLocal density fluctuations are expected to scale as a universal power-law when the system approaches critical point. Such power-law fluctuations are studied within the framework of intermittency…Salman Khurshid Malik, Ramni Gupta·Oct 14, 2022SaveLearn
Quasi-free (p,2p) reactions in inverse kinematics for studying the fission yield dependence on temperatureDespite the recent experimental and theoretical progress in the investigation of the nuclear fission process, a complete description still represents a challenge in nuclear physics because it is a…A. Graña-González, J. L. Rodríguez-Sánchez, J. Benlliure et al.·Oct 12, 2022SaveLearn
Comprehensive investigation of fission yields by using spallation- and (p,2p)-induced fission reactions in inverse kinematicsIn the last decades, measurements of spallation, fragmentation and Coulex induced fission reactions in inverse kinematics have provided valuable data to accurately investigate the fission dynamics…J. L. Rodríguez-Sánchez, A. Graña-González, J. Benlliure et al.·Oct 10, 2022SaveLearn
Quarkonium production in p-Pb collisions with ALICEALICE has measured quarkonium production in p-Pb collisions at backward (-4.46 < y cms < -2.96), mid (-1.37 < y cms < 0.43) and forward (2.03 < y cms < 3.53)…Biswarup Paul·Oct 10, 2022SaveLearn
Recent ALICE results on quarkonium production in nuclear collisionsQuarkonium production has long been regarded as a potential signature of deconfinement in nucleus-nucleus collisions. Recently, the production of J/ via regeneration within the quark-gluon…Biswarup Paul·Oct 9, 2022SaveLearn
(2S) production and nuclear modification factor in nucleus--nucleus collisions with ALICECharmonium production is a probe sensitive to deconfinement in nucleus--nucleus collisions. The production of J/ via regeneration within the QGP or at the phase boundary has been identified as…Biswarup Paul·Oct 9, 2022SaveLearn
Photonuclear reactions cross-sections at energies up to 100 MeV for different experimental setupsIn experiments on the electron linac LUE-40 of RDC "Accelerator" NSC KIPT, the flux-averaged cross-sections σ(Eγ max)exp of photonuclear reactions…O. S. Deiev, I. S. Timchenko, S. M. Olejnik et al.·Oct 9, 2022SaveLearn
Revealing the short-range structure of the "mirror nuclei" 3H and 3HeWhen protons and neutrons (nucleons) are bound into atomic nuclei, they are close enough together to feel significant attraction, or repulsion, from the strong, short-distance part of the…S. Li, R. Cruz-Torres, N. Santiesteban et al.·Oct 9, 2022SaveLearn
Deep underground laboratory measurement of 13C(α,n)16O in the Gamow windows of the s- and i-processesThe 13C(α,n)16O reaction is the main neutron source for the slow-neutron-capture (s-) process in Asymptotic Giant Branch stars and for the intermediate (i-) process. Direct…B. Gao, T. Y. Jiao, Y. T. Li et al.·Oct 6, 2022SaveLearn
Study of path-length dependent energy loss of jets in p--Pb and Pb--Pb collisions with ALICEJet quenching, a standard signature of quark--gluon plasma (QGP) formation in which jets lose energy by traversing the medium, comprises a well-studied set of observables in heavy-ion collisions.…Caitlin Beattie·Oct 6, 2022SaveLearn
Hadronic resonance production with ALICE at the LHCWe present recent results on short-lived hadronic resonances obtained by the ALICE experiment at LHC energies. Results include system-size and collision-energy evolution of transverse momentum…Sergey Kiselev·Oct 6, 2022SaveLearn
K*0 production in Au+Au collisions at s NN = 7.7, 11.5, 14.5, 19.6, 27 and 39 GeV from RHIC beam energy scanWe report the measurement of K*0 meson at midrapidity (|y|< 1.0) in Au+Au collisions at s NN~=~7.7, 11.5, 14.5, 19.6, 27 and 39 GeV collected by the STAR experiment during the…STAR Collaboration, M. S. Abdallah, B. E. Aboona et al.·Oct 6, 2022SaveLearn
Charge radii of 55,56Ni reveal a surprisingly similar behavior at N=28 in Ca and Ni isotopesNuclear charge radii of 55,56Ni were measured by collinear laser spectroscopy. The obtained information completes the behavior of the charge radii at the shell closure of the doubly magic…F. Sommer, K. König, D. M. Rossi et al.·Oct 4, 2022SaveLearn
Exploiting dissipative reactions to perform in-beam γ-ray spectroscopy of the neutron-deficient isotopes 38,39CaThe neutron-deficient Ca isotopes continue to attract attention due to their importance for testing isospin symmetry and their relevance in capture reactions of interest for nova nucleosynthesis and…A. Gade, D. Weisshaar, B. A. Brown et al.·Oct 3, 2022SaveLearn
Fissile isotopes antineutrino spectra: summation method and direct experimentNew antineutrino spectra of fissile isotopes (235U, 238U, 239Pu and 241Pu) which are containing in a nuclear reactor fuel have been obtained. A combined technique was used:…P. Naumov, S. Silaeva, V. Sinev et al.·Oct 3, 2022SaveLearn
Flow and transverse momentum correlation in Pb+Pb and Xe+Xe collisions with ATLAS: assessing the initial condition of the QGPOne important challenge in our field is to understand the initial condition of the QGP and constrain it using sensitive experimental observables. Recent studies show that the Pearson Correlation…Somadutta Bhatta·Oct 1, 2022SaveLearn
Photon-photon fusion and tau g-2 measurement in ATLASRelativistic heavy-ion beams at the LHC are accompanied by a large flux of equivalent photons. New measurements of exclusive dilepton production (electron, muon, and tau pairs) performed by the ATLAS…Agnieszka Ogrodnik·Sep 30, 2022SaveLearn
Laser Spectroscopy for the Study of Exotic NucleiInvestigation into the properties and structure of unstable nuclei far from stability remains a key avenue of research in modern nuclear physics. These efforts are motivated by the continual…X. F. Yang, S. J. Wang, S. G. Wilkins et al.·Sep 30, 2022SaveLearn