Femtoscopy of Proton, Light nuclei, and Strange hadrons in Au+Au Collisions at STARIn these proceedings, we present the measurements of proton, light nuclei, and strange particle with neutral kaons correlation functions in Au+Au collisions at the BES program and top RHIC energy.…Ke Mi·Aug 11, 2022SaveLearn
Higher-order Proton Cumulants in Au+Au Collisions at s NN = 3 GeV from RHIC-STARIn these proceedings, we present the higher-order cumulants of proton multiplicity distributions of the fixed-target (FXT) run in Au+Au collisions at s NN = 3.0 GeV. The cumulant…Yu Zhang·Aug 11, 2022SaveLearn
Characterization of electroless nickel-phosphorus plating for ultracold-neutron storageElectroless nickel plating is an established industrial process that provides a robust and relatively low-cost coating suitable for transporting and storing ultracold neutrons (UCN). Using roughness…H. Akatsuka, T. Andalib, B. Bell et al.·Aug 10, 2022SaveLearn
Heavy-ion physics with the ALICE detectorSelection of recent (in March 2022) results from the heavy-ion experiment ALICE at the CERN LHC, chosen to address various stages of the nucleus-nucleus reaction.Dariusz Miskowiec·Aug 10, 2022SaveLearn
An improved method to access initial states in relativistic heavy-ion collisionsObservables in heavy-ion collisions are generally categorized into centralities, which reflect an average over events within a range of impact parameter including a wide variety of initial state…Somadutta Bhatta, Vipul Bairathi·Aug 10, 2022SaveLearn
Excitation and probing of low-energy nuclear states at high-energy storage rings229Th with a low-lying nuclear isomeric state is an essential candidate for a nuclear clock as well as many other applications. Laser excitation of the isomeric state has been a long-standing…Junlan Jin, Hendrik Bekker, Tobias Kirschbaum et al.·Aug 9, 2022SaveLearn
Measurements of groomed-jet substructure of charm jets tagged by D0 mesons in proton-proton collisions at s = 13 TeVUnderstanding the role of parton mass and Casimir colour factors in the quantum chromodynamics parton shower represents an important step in characterising the emission properties of heavy quarks.…ALICE Collaboration·Aug 9, 2022SaveLearn
Measurement of Light Nuclei Production in Heavy-ion Collisions by the STAR experimentIn these proceedings, we present the measurements of centrality, transverse momentum and rapidity dependences of proton (p) and light nuclei (d (d), t, 3He…Hui Liu·Aug 9, 2022SaveLearn
Searching for New Physics with DarkLight at the ARIEL Electron-LinacThe search for a dark photon holds considerable interest in the physics community. Such a force carrier would begin to illuminate the dark sector. Many experiments have searched for such a particle,…The DarkLight Collaboration, E. Cline, R. Corliss et al.·Aug 8, 2022SaveLearn
Proton, deuteron and triton flow measurements in Au+Au collisions at sNN = 2.4 GeVHigh precision measurements of flow coefficients vn (n = 1 - 4) for protons, deuterons and tritons relative to the first-order spectator plane have been performed in Au+Au collisions at…HADES collaboration, J. Adamczewski-Musch, O. Arnold et al.·Aug 4, 2022SaveLearn
Advances and new ideas for neutron-capture astrophysics experiments at CERN nTOFThis article presents a few selected developments and future ideas related to the measurement of (n,γ) data of astrophysical interest at CERN nTOF. The MC-aided analysis methodology for the…C. Domingo-Pardo, V. Babiano-Suarez, J. Balibrea-Correa et al.·Aug 3, 2022SaveLearn
Model-independent determination of the dipole response of 66Zn using quasi-monoenergetic and linearly-polarized photon beams[Background] Photon strength functions are an important ingredient in calculations relevant for the nucleosynthesis of heavy elements. The relation to the photoabsorption cross section allows to…D. Savran, J. Isaak, R. Schwengner et al.·Aug 3, 2022SaveLearn
The splitting of directed flow for identified light hadrons (K and p) and strange baryons ( and ) in Au+Au collisions at STARThe first measurements for rapidity-odd directed flow of and in Au+Au collisions at s NN= 27 and 200 GeV are reported. The coalescence sum rule is examined with…Ashik Ikbal Sheikh·Aug 2, 2022SaveLearn
Measurement of charged-particle jet properties in p--Pb collisions at s NN = 5.02 TeV with ALICEWe present the measurement of charged-particle jet properties in minimum bias p--Pb collisions at s NN = 5.02 TeV in ALICE. Jets are reconstructed from charged particles at midrapidity…Prottoy Das·Aug 2, 2022SaveLearn
Pion, kaon, and (anti-)proton production in U+U Collisions at sNN = 193 GeV measured with the STAR detectorWe present the first measurements of transverse momentum spectra of π, K, p(p) at midrapidity (|y| < 0.1) in U+U collisions at sNN = 193 GeV with the STAR…STAR Collaboration, M. S. Abdallah, B. E. Aboona et al.·Aug 1, 2022SaveLearn
An Investigation of Charm Quark Jet Spectrum and Shape Modifications in Au+Au Collisions at sNN = 200 GeVPartons in heavy-ion collisions interact strongly with the Quark-Gluon Plasma (QGP), and hence have their energy and shower structure modified compared to those in vacuum. Theoretical calculations…Diptanil Roy·Jul 29, 2022SaveLearn
Measurements and computational analysis on the natural decay of 176LuMainly because of its long half-life and despite its scientific relevance, spectroscopic measurements of 176Lu forbidden β-decays are very limited and lack formulation of shape factors. A…F. G. A. Quarati, G. Bollen, P. Dorenbos et al.·Jul 28, 2022SaveLearn
Charm production: constraints to transport models and charm diffusion coefficient with ALICEIn this contribution, the nuclear modification factor and azimuthal anisotropy of prompt charm mesons and baryons in Pb-Pb collisions at sNN=5.02 TeV by the ALICE Collaboration are…Luuk Vermunt·Jul 28, 2022SaveLearn
Resonant behavior of the pp \pp\s π0 reaction at the energy s = 2.65 GeVWe report on measurements of the differential cross section dσ/d in the energy region of s = 2.5-2.9 GeV of the reaction pp \pp\s π0 where \pp\s is a 1\!S0…Dmitry Tsirkov, Bota Baimurzinova, Vladimir I. Komarov et al.·Jul 27, 2022SaveLearn
An enhancement of formation of unstable 8Be nucleus with the growth of α-particle multiplicity in fragmentation of relativistic nucleiIn this paper, the correlation between the formation of the unstable 8Be nucleus and accompanying α particles in the fragmentation of relativistic 16O, 22Ne, 28Si, and…A. A. Zaitsev, P. I. Zarubin, N. G. Peresadko·Jul 27, 2022SaveLearn
Charmonium production as a function of charged-particle multiplicity in pp and p--Pb collisions with ALICE at the LHCHeavy quarkonium production is an excellent tool to test both perturbative and non-perturbative QCD, as perturbative QCD can describe the heavy quark production process, while the formation of the…Theraa Tork·Jul 27, 2022SaveLearn
Exclusive dielectron production in ultraperipheral Pb+Pb collisions at s_NN = 5.02 TeV with ATLASExclusive production of dielectron pairs, γγ→ e+e-, is studied using Lint=1.72\; nb-1 of data from ultraperipheral collisions of lead nuclei…ATLAS Collaboration·Jul 26, 2022SaveLearn
Measurement of the Parity-Odd Angular Distribution of Gamma Rays From Polarized Neutron Capture on 35ClWe report a measurement of two energy-weighted gamma cascade angular distributions from polarized slow neutron capture on the 35Cl nucleus, one parity-odd correlation proportional to…N. Fomin, R. Alarcon, L. Alonzi et al.·Jul 22, 2022SaveLearn
The use of a novel gradient heat flux sensor for characterization of reflux condensationIn this paper we present the developments in heat flux measurements using gradient heat flux sensors (GHFS). The GHFS is a sensor made of artificially created material with anisotropic…Filip Janasz, Horst-Michel Prasser, Detlef Suckow et al.·Jul 22, 2022SaveLearn
Study of elastic and inelastic scattering of 7Be + 12C at 35 MeVThe elastic and inelastic scattering of 7Be from 12C have been measured at an incident energy of 35 MeV. The inelastic scattering leading to the 4.439 MeV excited state of 12C has been…K. Kundalia, D. Gupta, Sk M. Ali et al.·Jul 22, 2022SaveLearn