50Ti(d,p)51Ti, single neutron energies in the N=29 isotones and the N=32 subshell closureA measurement of the 50Ti(d,p)51Ti reaction at 16 MeV was performed using a Super Enge Split Pole Spectrograph to measure the magnitude of the N=32 subshell gap in Ti. Seven states…L. A. Riley, 1 J. M. Nebel-Crosson, 1 K. T. Macon et al.·Jun 10, 2021SaveLearn
Direct observation of the dead-cone effect in QCDIn particle collider experiments, elementary particle interactions with large momentum transfer produce quarks and gluons (known as partons) whose evolution is governed by the strong force, as…ALICE Collaboration·Jun 10, 2021SaveLearn
Elastic scattering measurements for the 10C + 208Pb system at E lab = 66 MeVBackground: The influence of halo structure of 6He, 8B, 11Be and 11Li nuclei in several mechanisms such as direct reactions and fusion is already established, although not completely…R Linares, Mandira Sinha, E N Cardozo et al.·Jun 10, 2021SaveLearn
Evidence against the wobbling nature of low-spin bands in 135PrThe electromagnetic character of the I=1 transitions connecting the one- to zero-phonon and the two- to one-phonon wobbling bands should be dominated by an E2 component, due to the…B. F. Lv, C. M. Petrache, E. A. Lawrie et al.·Jun 9, 2021SaveLearn
Measurement and Modeling of Proton-Induced Reactions on Arsenic from 35 to 200 MeV72As is a promising positron emitter for diagnostic imaging that can be employed locally using a 72Se generator. However, current reaction pathways to 72Se have insufficient nuclear…Morgan B. Fox, Andrew S. Voyles, Jonathan T. Morrell et al.·Jun 8, 2021SaveLearn
Measurement of the transverse polarization of electrons emitted in neutron decay -- nTRV experimentThis paper recalls the main achievements of the nTRV experiment which measured two components of the transverse polarization (σT1, σT2) of electrons emitted in the…K. Bodek, A. Kozela·Jun 7, 2021SaveLearn
Precise Measurements of the Decay of Free NeutronsThe impact of new and highly precise neutron eta decay data is reviewed. We focus on recent results from neutron lifetime, eta asymmetry, and electron-neutrino correlation experiments. From…Dirk Dubbers, Bastian Märkisch·Jun 4, 2021SaveLearn
Isomers in 203Tl and core excitations built on a five-nucleon-hole structureIsomers with three- and five-nucleon-hole configurations have been established in 203Tl. These include newly identified levels with a three-nucleon structure: Iπ = (15/2-)…V. Bothe, S. K. Tandel, S. G. Wahid et al.·Jun 4, 2021SaveLearn
Neutron occupancies and single-particle energies across the stable tin isotopesThe occupancies and vacancies of the valence neutron orbitals across the stable tin isotopic chain from 112≤ A≤ 124 have been determined. These were inferred from the cross sections of…S. V. Szwec, D. K. Sharp, B. P. Kay et al.·Jun 3, 2021SaveLearn
A new method in the production of Ac-227, Ra-228, Th-228 and U-232 on Thorium target from different perspective for use in Radioisotope Power Systems and Nuclear BatteriesWe recommended a new method from different perspective for the production of Ac-227, Ra-228, Th-228 and U-232 radioisotopes which have an important potential for use in radioisotope power systems…O. Artun·Jun 3, 2021SaveLearn
Nuclear reaction measurements of 80.5 MeV/u 12C beam bombarding on C, W, Cu, Au, Pb targetsTo get the energy spectrum distribution and cross-sections of emitted light charged particles and explore the nuclear reaction, a experiment of 80.5 MeV/u 12C beam bombarding on C, W, Cu, Au, Pb…Zhichao Gao, Xueying Zhang, Yongqin Ju et al.·Jun 2, 2021SaveLearn
The extremes of neutron richnessA neutron star is pictured as a gigantic nucleus overwhelmed by the number of neutrons, unlike real atomic nuclei, that have a similar number of neutrons and protons. Is this true? What if we could…F. Miguel Marqués·Jun 1, 2021SaveLearn
Measurement of the Sixth-Order Cumulant of Net-Proton Multiplicity Distributions in Au+Au Collisions at s NN= 27, 54.4, and 200 GeV at RHICAccording to first principle Lattice QCD calculations, the transition from quark-gluon plasma to hadronic matter is a smooth crossover in the region μ B≤ Tc. In this range the ratio,…STAR Collaboration, M. S. Abdallah, J. Adam et al.·May 31, 2021SaveLearn
Probing dense QCD matter: Muon measurements with the CBM experiment at FAIRThe Compressed Baryonic Matter (CBM) experiment at the future Facility for Antiproton and Ion Research (FAIR) in Darmstadt is designed to investigate the properties of high-density QCD matter with…Anna Senger, Peter Senger·May 29, 2021SaveLearn
Peculiar features of missing mass distributions in studies of exclusive reactionsThis study examines the influence of the following five factors on missing mass distributions, radiative effects, admixtures from other channels, detector resolution, Fermi smearing, and final state…Iu. A. Skorodumina, G. V. Fedotov, R. W. Gothe·May 28, 2021SaveLearn
Radioactive ion beam production at the Gamma FactoryA very intense gamma beam of the Gamma Factory facility proposed at CERN can be used to generate radioactive ion beams (RIBs) with high production yields and study the structure of exotic…Dragos Nichita, Dimiter Balabanski, Paul Constantin et al.·May 27, 2021SaveLearn
Cross-sections for the 27\!al(γ,x)22na multichannel reaction with the 28.3 mev difference of the reaction thresholdsThe bremsstrahlung flux-averaged cross-sections σ(Eγ max) and the cross-sections per equivalent photon σ(Eγ max)Q were…O. S. Deiev, I. S. Timchenko, S. N. Olejnik et al.·May 26, 2021SaveLearn
An experimental review of open heavy flavor and quarkonium production at RHICOpen heavy flavor and quarkonium are unique probes of the hot-dense medium produced in heavy-ion collisions. Their production in p+p collisions also provide important test of QCD. In this paper, we…Zebo Tang, Wangmei Zha, Yifei Zhang·May 25, 2021SaveLearn
Resonance-like structure near the η d threshold in the γdπ0ηd reactionTo investigate the interaction between the nucleon N and nucleon resonance N(1535)1/2-, the η d threshold structure connected to the isoscalar S-wave N-N(1535)1/2- system has been…T. Ishikawa, H. Fujimura, H. Fukasawa et al.·May 23, 2021SaveLearn
Isotope Shifts of Radium Monofluoride MoleculesIsotope shifts of 223-226,228Ra19F were measured for different vibrational levels in the electronic transition A21/2← X2+. The observed isotope…S. M. Udrescu, A. J. Brinson, R. F. Garcia Ruiz et al.·May 21, 2021SaveLearn
Nucleon-Nucleon Interaction ib the Singlet State at Low EnergyIt is possible to describe the scattering and the radiative capture with help of a Breit-Wigner resonance with negative energy.S. B. Borzakov·May 21, 2021SaveLearn
Symmetry energy at high densities from neutron/proton flow excitation functionsDetermination of the high density behavior of the symmetry energy through the simultaneous measurement of elliptic flow excitation functions of neutrons, protons and light clusters is proposed. The…P. Russotto, A. Le Fèvre, J. Łukasik et al.·May 19, 2021SaveLearn
Measurements of (1530)0 and (1530)0 production in proton-proton interactions at sNN = 17.3 GeV in the NA61/SHINE experimentDouble-differential yields of (1530)0 and (1530)0 resonances produced in interactions were measured at a laboratory beam momentum of 158~.…A. Acharya, H. Adhikary, K. K. Allison et al.·May 19, 2021SaveLearn
An overview of STAR jet and high pT resultsThese proceeding present recent measurements by the STAR Collaboration of jet production in p+p and Au+Au collisions at sqrt(sNN) = 200 GeV. We focus on jet yields, substructure, and heavy-flavor…Saehanseul Oh·May 18, 2021SaveLearn
Flow harmonics in heavy ion physics at CMS and ATLASHow can we gain a detailed insight into the hydrodynamic response of the system created in heavy ion collisions to the fluctuating initial geometry and viscous effects? Do we create a strongly…Georgios Konstantinos Krintiras·May 15, 2021SaveLearn