Total and differential cross sections of the dp→He3η reaction at excess energies between 1 and 15 MeV

C. Fritzsch, S. Barsov, I. Burmeister, S. Dymov, R. Gebel, M. Hartmann, A. Kacharava, A. Khoukaz, V. Komarov, P. Kulessa, A. Kulikov, A. Lehrach, B. Lorentz, D. Mchedlishvili, T. Mersmann, M. Mielke, S. Mikirtychiants, M. Nioradze, H. Ohm, M. Papenbrock, D. Prasuhn, V. Serdyuk, H. Ströher, A. Täschner, Y. Valdau, C. Wilkin
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Abstract

New high precision total and differential cross sections are reported for the $dp\to {}^3\textrm{He}\,\eta$ reaction close to threshold. The measurements were performed using the magnetic spectrometer ANKE, which is an internal fixed target facility at the COSY cooler synchrotron. The data were taken for deuteron beam momenta between $3.14641~\textrm{GeV}/c$ and $3.20416~\textrm{GeV}/c$, which corresponds to the range in excess energy $Q$ for this reaction between $1.14~\textrm{MeV}$ and $15.01~\textrm{MeV}$. The normalization was established through the measurement in parallel of deuteron-proton elastic scattering and this was checked through the study of the $dp\to {}^3\textrm{He}\,\pi^0$ reaction. The previously indicated possible change of sign of the slope of the differential cross sections near the production threshold, which could be explained by a rapid variation of the $s$- and $p$-wave interference term, is not confirmed by the new data. The energy dependence of the total cross section and the $90^{\circ}$ slope parameter are well explained by describing the final state interaction in terms of a complex Jost function and the results are significant in the discussion of $\eta$-mesic nuclei. In combination with recently published WASA-at-COSY data [P. Adlarson $et\, al.$, Phys. Lett. B 782, 297 (2018)], a smooth variation of the slope parameter is achieved up to an excess energy of $80.9~\textrm{MeV}$.
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dp→He3η反应在过剩能量1 ~ 15mev时的总截面和微分截面
在接近阈值的$dp\to {}^3\textrm{He}\,\eta$反应中,报告了新的高精度总和微分截面。测量是使用ANKE磁谱仪进行的,ANKE是在COSY冷却器同步加速器的内部固定目标设施。氘核束动量在$3.14641~\textrm{GeV}/c$和$3.20416~\textrm{GeV}/c$之间,对应于该反应的多余能量$Q$在$1.14~\textrm{MeV}$和$15.01~\textrm{MeV}$之间。通过平行测量氘核-质子弹性散射建立了归一化,并通过研究$dp\to {}^3\textrm{He}\,\pi^0$反应验证了这一点。先前指出的在生产阈值附近的微分截面斜率的符号可能发生变化,这可以通过$s$和$p$波干涉项的快速变化来解释,但新数据并未证实。用复约斯特函数描述终态相互作用,很好地解释了总截面和$90^{\circ}$斜率参数的能量依赖性,其结果对讨论$\eta$-介核具有重要意义。结合最近公布的WASA-at-COSY数据[P。Adlarson $et\, al.$,物理学。列托人。[B][782, 297(2018)],斜率参数的平滑变化达到多余能量$80.9~\textrm{MeV}$。
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