An Isotensor Dibaryon in the pp ppπ+π- Reaction?Exclusive measurements of the quasi-free pp ppπ+π- reaction have been carried out at WASA@COSY by means of pd collisions at Tp = 1.2 GeV. Total and differential cross sections have been…P. Adlarson, W. Augustyniak, W. Bardan et al.·Mar 8, 2018SaveLearn
On the Production of an Isotensor Dibaryon in the pp ppπ+π- ReactionExclusive measurements of the quasi-free pp ppπ+π- reaction have been performed by means of pd collisions at Tp = 1.2 GeV using the WASA detector setup at COSY. Total and differential…P. Adlarson, W. Augustyniak, W. Bardan et al.·Mar 8, 2018SaveLearn
Isospin influence on dynamical production of Intermediate Mass Fragments at Fermi EnergiesThe Intermediate Mass Fragments emission probability from Projectile-Like Fragment break-up in semi-peripheral reactions has been measured in collisions of 124Xe projectiles with two different…P. Russotto, E. De Filippo, E. V. Pagano et al.·Mar 8, 2018SaveLearn
The kaonic atoms research program at DAΦNE: from SIDDHARTA to SIDDHARTA-2The interaction of antikaons with nucleons and nuclei in the low-energy regime represents an active research field in hadron physics with still many important open questions. The investigation of…A. Scordo, A. Amirkhani, M. Bazzi et al.·Mar 7, 2018SaveLearn
Examination of the observability of a chiral magnetically-driven charge-separation difference in collisions of the 9644Ru +\, 9644Ru and 9640Zr +\, 9640Zr isobars at energies available at RHICAnomalous Viscous Fluid Dynamics (AVFD) model calculations for 9644Ru +\, 9644Ru and 9640Zr +\, 9640Zr collisions (s NN = 200 GeV) are…Niseem Magdy, Shuzhe Shi, Jinfeng Liao et al.·Mar 6, 2018SaveLearn
Beam energy dependence of squeeze-out effect on the directed and elliptic flow in Au+Au collisions at high baryon density regionWe present a detailed analysis of the beam energy dependence of the mechanisms for the generation of directed and elliptic flows in Au+Au collisions focusing on the role of hadronic rescattering and…Chao Zhang, Jiamin Chen, Xiaofeng Luo et al.·Mar 6, 2018SaveLearn
Probing the N = 14 subshell closure: g factor of the 26Mg(2+1) stateThe first-excited state g~factor of 26Mg has been measured relative to the g factor of the 24Mg(2+1) state using the high-velocity transient-field technique, giving…B. P. McCormick, A. E. Stuchbery, T. Kibédi et al.·Mar 6, 2018SaveLearn
Halo structure of 8B determined from intermediate energy proton elastic scattering in inverse kinematicsThe absolute differential cross section for small-angle proton elastic scattering on the proton-rich 8B nucleus has been measured in inverse kinematics for the first time. The experiment was…G. A. Korolev, A. V. Dobrovolsky, A. G. Inglessi et al.·Mar 6, 2018SaveLearn
First Measurement of the Ti(e,e) X Cross Section at Jefferson LabTo probe CP violation in the leptonic sector using GeV energy neutrino beams in current and future experiments using argon detectors, precise models of the complex underlying neutrino and…H. Dai, M. Murphy, V. Pandey et al.·Mar 5, 2018SaveLearn
Robust extraction of proton charge radius from electron-proton scattering dataExtracting the proton charge radius from electron scattering data requires determining the slope of the charge form factor at Q2 of zero. But as experimental data never reach that limit, numerous…Xuefei Yan, Douglas W. Higinbotham, Dipangkar Dutta et al.·Mar 5, 2018SaveLearn
Charm Program of NA61/SHINE: Motivation and MeasurementsRecently, the NA61/SHINE experiment at the CERN SPS has extended its program on physics of strong interactions by measurements of charm hadron production in nucleus-nucleus collisions. This charm…Aleksandra Snoch, the NA61/SHINE collaboration·Mar 5, 2018SaveLearn
On the possibility to observe neutron dark decay in nucleiAs proposed recently by Fornal and Grinstein, neutrons can undergo a dark matter decay mode which was not observed before. Such a decay could explain the existing discrepancy between two different…Marek Pfützner, Karsten Riisager·Mar 4, 2018SaveLearn
Study of the γp π0ηp reaction with the A2 setup at MAMIThe data available from the A2 Collaboration at MAMI were analyzed to select the γp π0ηp reaction on an event-by-event basis, which allows for partial-wave analyses of three-body final states…V. Sokhoyan, S. Prakhov, A. Fix et al.·Mar 2, 2018SaveLearn
Identification of significant E0 strength in the 2+2 → 2+1 transitions of 58, 60, 62NiThe E0 transition strength in the 2+2 → 2+1 transitions of 58,60,62Ni have been determined for the first time following a series of measurements at the Australian National…L. J. Evitts, A. B. Garnsworthy, T. Kibédi et al.·Mar 2, 2018SaveLearn
Jet properties in PbPb and pp collisions at sNN = 5.02 TeVModifications of the properties of jets in PbPb collisions, relative to those in pp collisions, are studied at a nucleon-nucleon center-of-mass energy of sNN = 5.02 TeV via…CMS Collaboration·Feb 28, 2018SaveLearn
Measurement of the full excitation spectrum of the 7Li(p,γ)αα reaction at 441 keVA current challenge for ab initio calculations is systems that contain large continuum contributions such as 8Be. We report on new measurements of radiative decay widths in this nucleus that test…Michael Munch, Oliver Sølund Kirsebom, Jacobus Andreas Swartz et al.·Feb 28, 2018SaveLearn
Re-examining the transition into the N=20 island of inversion: structure of 30MgIntermediate energy single-neutron removal from 31Mg has been employed to investigate the transition into the N=20 island of inversion. Levels up to 5~MeV excitation energy in 30Mg were…B. Fernández-Domínguez, B. Pietras, W. N. Catford et al.·Feb 27, 2018SaveLearn
Transverse momentum spectra and nuclear modification factors of charged particles in pp, p-Pb and Pb-Pb collisions at the LHCWe report the measured transverse momentum (p T) spectra of primary charged particles from pp, p-Pb and Pb-Pb collisions at a center-of-mass energy s NN = 5.02 TeV in the…ALICE Collaboration·Feb 26, 2018SaveLearn
Measurement of the D-meson nuclear modification factor and elliptic flow in Pb-Pb collisions at sNN = 5.02 TeV with ALICE at the LHCHeavy-flavour hadrons are effective probes to study the Quark-Gluon Plasma (QGP) formed in ultra-relativistic heavy-ion collisions. The ALICE Collaboration measured the D-mesons (D0, D+,…Syaefudin Jaelani·Feb 26, 2018SaveLearn
Constraining the optical potential in the search for eta-mesic 4HeA consistent description of the d d → 4-0.03cmHe η and d d → (4Heη)bound → X cross sections was recently proposed with a broad…M. Skurzok, P. Moslal, N. G. Kelkar et al.·Feb 23, 2018SaveLearn
Search for time modulations in the decay constant of 40K and 226Ra at the underground Gran Sasso LaboratoryTime modulations at per mil level have been reported to take place in the decay constant of several nuclei with period of one year (most cases) but also of about one month or one day. On the other…E. Bellotti, C. Broggini, G. Di Carlo et al.·Feb 23, 2018SaveLearn
Measurement of the normalized 238U(n,f)/235U(n,f) cross section ratio from threshold to 30 MeV with the fission Time Projection ChamberThe normalized 238U(n,f)/235U(n,f) cross section ratio has been measured using the NIFFTE fission Time Projection Chamber from the reaction threshold to 30~MeV. The fissionTPC is a…R. J. Casperson, D. M. Asner, J. Baker et al.·Feb 23, 2018SaveLearn
Results of the first user program on the Homogenous Thermal Neutron Source HOTNES (ENEA / INFN)The HOmogeneous Thermal NEutron Source (HOTNES) is a new type of thermal neutron irradiation assembly developed by the ENEA-INFN collaboration. The facility is fully characterized in terms of neutron…A. Sperduti, M. Angelone, R. Bedogni et al.·Feb 22, 2018SaveLearn
First Result on the Neutrinoless Double Beta Decay of 82Se with CUPID-0We report the result of the search for neutrinoless double beta decay of 82Se obtained with CUPID-0, the first large array of scintillating Zn82Se cryogenic calorimeters implementing…0 collaboration, O. Azzolini, M. T. Barrera et al.·Feb 21, 2018SaveLearn
Physics at the Munich Tandem Accelerator LaboratoryThis review reports on the science performed in various fields at the Munich tandem accelerator during the past decade. It covers nuclear structure studies, also with respect to astro- and particle…Günther Dollinger, Thomas Faestermann·Feb 20, 2018SaveLearn