6533b7cffe1ef96bd1258622
RESEARCH PRODUCT
Comparing proton momentum distributions in A = 2 and 3 nuclei via 2H 3H and 3He (e,e′p) measurements
Z. YeB. SchmooklerJ. P. ChenG. M. UrciuoliDiego LonardoniDiego LonardoniP. M. KingHongbang LiuR. MichaelsD. KingM. OlsonDarko AndroićS. CovrigToshiyuki GogamiPete MarkowitzS. PaulWeidong LiM. VivianiWhitney ArmstrongP. E. ReimerLarry WeinsteinT. SuM. PatsyukH. AtacB. DongwiOr HenN. SantiestebanB. SawatzkyT. KutzV. BelliniR. I. PomatsalyukH. BhattI. KoroverS. A. WoodR. ObrechtS. RiordanV. PandeyE. FucheyShanfeng LiA. BeckM. HattawyJohn ArringtonS. Mey-tal BeckZ. YeAndrew PuckettD. BulumullaBogdan WojtsekhowskiAditya R. KhanalF. HauensteinSimon ŠIrcaA. ShahinyanM. N. H. RashadAxel SchmidtCynthia KeppelM. KhachatryanJ. GomezN. Lashley-colthirstD. BlythJ. CastellanosRuprecht MachleidtR. SuleimanH. AlbatainehD. BhetuwalV. KhachatryanKondo GnanvoEliahu CohenF. TortoriciJ. RocheV. A. PunjabiN. NuruzzamanS. AlsalmiM. NyczH. Szumila-vanceB. DuranG. G. PetratosZ. E. MezianiC. GalVladimir NelyubinG. LaskarisL. TangW. TiremanM. MihovilovicM. MihovilovicA. KarkiRonald RansomeD. G. MeekinsA. T. KatramatouOlfred HansenW. U. BoeglinNilanga LiyanageD. BiswasC. Ayerbe GayosoJiawen ZhangS. PremathilakeD. NguyenX. BaiE.p. SegarraSiyu JianElliot HughesR. Cruz-torresDouglas HiginbothamL. OuS. BarcusV. OwenJ. BaneA. S. TadepalliR. E. McclellanA. HabarakadaSylvester JoostenK. CraycraftH. F. IbrahimB. KarkiDipangkar DuttaLaura Elisa MarcucciM. DuerT. GautamB. PandeyShalev GiladA. PapadopoulouK. A. AniolA. CamsonneD. AbramsS. ParkF. SammarrucaN. SparverisE. PiasetzkyC. GuT. HagueT. AverettC. E. Hydesubject
production [pi]Nuclear and High Energy Physicsdata analysis methodPhotonNuclear TheoryNuclear TheoryinterferenceFOS: Physical sciencesElectronImpulse (physics)Inelastic scattering01 natural sciencesxperimental results | Jefferson Lab | electron p: scattering | parity: violation | inelastic scattering | structure function | interference | photon | Z0 | pi: production | spin: asymmetry | data analysis methodNuclear Theory (nucl-th)structure function0103 physical sciencesZ0Nuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentPhysics010308 nuclear & particles physicsMomentum transferphotoninelastic scatteringscattering [electron p]Eikonal approximationNATURAL SCIENCES. Physics.lcsh:QC1-999PRIRODNE ZNANOSTI. Fizika.Deuteriumxperimental resultsHigh Energy Physics::Experimentviolation [parity]Atomic physicsNucleonasymmetry [spin]lcsh:PhysicsJefferson Labdescription
We report the first measurement of the $(e,e'p)$ reaction cross-section ratios for Helium-3 ($^3$He), Tritium ($^3$H), and Deuterium ($d$). The measurement covered a missing momentum range of $40 \le p_{miss} \le 550$ MeV$/c$, at large momentum transfer ($\langle Q^2 \rangle \approx 1.9$ (GeV$/c$)$^2$) and $x_B>1$, which minimized contributions from non quasi-elastic (QE) reaction mechanisms. The data is compared with plane-wave impulse approximation (PWIA) calculations using realistic spectral functions and momentum distributions. The measured and PWIA-calculated cross-section ratios for $^3$He$/d$ and $^3$H$/d$ extend to just above the typical nucleon Fermi-momentum ($k_F \approx 250$ MeV$/c$) and differ from each other by $\sim 20\%$, while for $^3$He/$^3$H they agree within the measurement accuracy of about 3\%. At momenta above $k_F$, the measured $^3$He/$^3$H ratios differ from the calculation by $20\% - 50\%$. Final state interaction (FSI) calculations using the generalized Eikonal Approximation indicate that FSI should change the $^3$He/$^3$H cross-section ratio for this measurement by less than 5\%. If these calculations are correct, then the differences at large missing momenta between the $^3$He/$^3$H experimental and calculated ratios could be due to the underlying $NN$ interaction, and thus could provide new constraints on the previously loosely-constrained short-distance parts of the $NN$ interaction.
year | journal | country | edition | language |
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2019-10-01 | Physics Letters B |