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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. PandeyHampton UniversityL. TangHampton UniversityP. BydžovskýNuclear Physics InstituteD. SkoupilNuclear Physics InstituteT. MartUniversitas IndonesiaD. AbramsUniversity of VirginiaTetsuya AkiyamaTohoku UniversityD. AndroićUniversity of ZagrebK. AniolCalifornia State University, Los AngelesC. Ayerbe GayosoDepartment of PhysicsJ. BaneUniversity of Tennessee, KnoxvilleS. BarcusDepartment of PhysicsJ. 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. ChenDepartment of PhysicsS. 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. GuèyeHampton 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. KutzState University of New YorkN. Lashley-ColthirstHampton UniversityS. LiLawrence Berkeley National LaboratoryHaibo LiuColumbia UniversityJ. MammeiUniversity of ManitobaP. MarkowitzFlorida International UniversityR. E. McClellanThomas Jefferson National Accelerator FacilityF. MeddiIstituto Nazionale di Fisica Nucleare, Sezione di RomaD. MeekinsThomas Jefferson National Accelerator FacilityR. MichaelsThomas Jefferson National Accelerator FacilityM. MihovilovičInstitut für KernphysikA. MoyerChristopher Newport UniversityD. NguyenHue UniversityM. NyczKent State UniversityV. OwenDepartment of PhysicsC. PalatchiUniversity of VirginiaS. ParkState University of New YorkTea 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. SantiestebanUniversity of New HampshireB. SawatzkyThomas Jefferson National Accelerator FacilityS. ŠircaJožef Stefan InstituteK. SliferUniversity of New HampshireT. SuKent State UniversityY. TianSyracuse UniversityYuichi ToyamaTohoku UniversityK. UeharaTohoku UniversityG. M. UrciuoliIstituto Nazionale di Fisica Nucleare, Sezione di RomaD. VotawMichigan State UniversityJeffrey F. WilliamsonUniversity of GlasgowB. WojtsekhowskiThomas Jefferson National Accelerator FacilityStephen A. WoodThomas Jefferson National Accelerator FacilityB. YaleUniversity of New HampshireZ. YeArgonne National LaboratoryJ. ZhangUniversity of VirginiaXiaowei ZhengUniversity of Virginia
Physical review. Cjournal2024lv
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Annotatsiya

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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