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Electroproduction of the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi mathvariant="normal">Λ</mml:mi><mml:mtext>/</mml:mtext><mml:msup><mml:mi mathvariant="normal">Σ</mml:mi><mml:mn>0</mml:mn></mml:msup></mml:math> hyperons at <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msup><mml:mi>Q</mml:mi><mml:mn>2</mml:mn></mml:msup><mml:mo>≃</mml:mo><mml:mn>0.5</mml:mn></mml:mrow></mml:math> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:mi>GeV</mml:mi><mml:mo>/</mml:mo><mml:mi>c</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mn>2</mml:mn></mml:msup></mml:math> at forward angles

K. OkuyamaTohoku UniversityKosuke ItabashiKEKS. NagaoThe University of TokyoSeitaro NakamuraThe University of TokyoK. N. SuzukiKyoto UniversityT. GogamiKyoto UniversityB. PandeyVirginia Military InstituteL. TangHampton UniversityP. BydžovskýNuclear Physics InstituteD. SkoupilNuclear Physics InstituteT. MartUniversitas IndonesiaD. AbramsUniversity of VirginiaTetsuya AkiyamaTohoku UniversityD. AndroićUniversity of ZagrebK. AniolCalifornia State University, Los AngelesC. Ayerbe GayosoWilliam and MaryJ. BaneUniversity of Tennessee, KnoxvilleS. BarcusWilliam and MaryJ. BarrowUniversity of Tennessee, KnoxvilleVincenzo BelliniIstituto Nazionale di Fisica Nucleare, Sezione di RomaH. BhattMississippi State UniversityD. BhetuwalMississippi State UniversityDiptaparna BiswasHampton UniversityA. CamsonneThomas Jefferson National Accelerator FacilityJ. CastellanosFlorida International UniversityJ.-P. ChenDepartment of PhysicsJ. ChenThomas Jefferson National Accelerator FacilityS. CovrigThomas Jefferson National Accelerator FacilityD. ChrismanMichigan State UniversityR. Cruz-TorresMassachusetts Institute of TechnologyRasel DasState University of New YorkE. FucheyUniversity of Connecticut, StorrsK. GnanvoUniversity of VirginiaF. GaribaldiInstituto Superiore di SanitàT. GautamHampton UniversityJ. GómezThomas Jefferson National Accelerator FacilityP. GuèyeMichigan State UniversityThe HagueKent State UniversityO. HansenThomas Jefferson National Accelerator FacilityW. HenryThomas Jefferson National Accelerator FacilityF. HauensteinOld Dominion UniversityD. W. HiginbothamThomas Jefferson National Accelerator FacilityC. E. Hyde-WrightOld Dominion UniversityM. KanetaTohoku UniversityC. E. KeppelThomas Jefferson National Accelerator FacilityT. KutzDepartment of Physics, State University of New York, Stony Brook, New York 11794, USAN. Lashley-ColthirstHampton UniversityS. LiDepartment of Physics, University of New Hampshire, Durham, New Hampshire 03824, USAHaibo LiuColumbia UniversityJ. MammeiUniversity of ManitobaP. MarkowitzFlorida International UniversityR. E. McClellanThomas Jefferson National Accelerator FacilityF. MeddiSapienza University of RomeD. MeekinsThomas Jefferson National Accelerator FacilityR. MichaelsThomas Jefferson National Accelerator FacilityM. MihovilovičUniversity of LjubljanaA. MoyerChristopher Newport UniversityD. NguyenHue UniversityM. NyczKent State UniversityV. OwenDepartment of PhysicsC. PalatchiUniversity of VirginiaS. ParkStony BrookTea PetkovićUniversity of ZagrebS. PremathilakeUniversity of VirginiaP. E. ReimerArgonne National LaboratoryJ. ReinholdFlorida International UniversityS. RiordanArgonne National LaboratoryV. M. RodriguezUniversidad Ana G. MéndezC. SamantaVirginia Military InstituteS. N. SantiestebanDepartment of Physics, University of New Hampshire, Durham, New Hampshire 03824, USAB. SawatzkyThomas Jefferson National Accelerator FacilityS. ŠircaUniversity of LjubljanaK. SliferDepartment of Physics, University of New Hampshire, Durham, New Hampshire 03824, USAT. SuKent State UniversityY. TianSyracuse UniversityYuichi ToyamaTohoku UniversityK. UeharaTohoku UniversityG. M. UrciuoliIstituto Nazionale di Fisica Nucleare, Sezione di RomaD. VotawNational Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USAJeffrey F. WilliamsonUniversity of GlasgowB. WojtsekhowskiThomas Jefferson National Accelerator FacilityStephen A. WoodThomas Jefferson National Accelerator FacilityB. YaleDepartment of Physics, University of New Hampshire, Durham, New Hampshire 03824, USAZ. YeArgonne National LaboratoryJ. ZhangUniversity of VirginiaXiaowei ZhengUniversity of Virginia
Physical review. Cjournal2024lv

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In 2018, the E12-17-003 experiment was conducted at the Thomas Jefferson National Accelerator Facility (JLab) to explore the possible existence of an $nn\mathrm{\ensuremath{\Lambda}}$ state in the reconstructed missing mass distribution from a tritium gas target [K. N. Suzuki et al., Prog. Theor. Exp. Phys. 2022, 013D01 (2022); B. Pandey et al., Phys. Rev. C 105, L051001 (2022)]. As part of this investigation, data were also collected using a gaseous hydrogen target, not only for a precise absolute mass scale calibration but also for the study of $\mathrm{\ensuremath{\Lambda}}/{\mathrm{\ensuremath{\Sigma}}}^{0}$ electroproduction. This dataset was acquired at ${Q}^{2}\ensuremath{\simeq}0.5$ ${(\mathrm{GeV}/c)}^{2}$, $W=2.14$ GeV, and ${\ensuremath{\theta}}_{\ensuremath{\gamma}\mathrm{K}}^{\mathrm{c}.\mathrm{m}.}\ensuremath{\simeq}{8}^{\ensuremath{\circ}}$. It covers forward angles where photoproduction data are scarce and a low-${Q}^{2}$ region that is of interest for hypernuclear experiments. On the other hand, this kinematic region is at a slightly higher ${Q}^{2}$ than previous hypernuclear experiments, thus providing crucial information for understanding the ${Q}^{2}$ dependence of the differential cross sections for $\mathrm{\ensuremath{\Lambda}}/{\mathrm{\ensuremath{\Sigma}}}^{0}$ hyperon electroproduction. This paper reports on the ${Q}^{2}$ dependence of the differential cross section for the $e+p\ensuremath{\rightarrow}{e}^{\ensuremath{'}}+{K}^{+}+\mathrm{\ensuremath{\Lambda}}/{\mathrm{\ensuremath{\Sigma}}}^{0}$ reaction at $0.2--0.8$ ${(\mathrm{GeV}/c)}^{2}$, and provides comparisons with the currently available theoretical models.

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