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首页> 外文期刊>Nuclear Physics, A: Journal Devoted to the Experimental Study of the Fundamental Constituents of Matter and Their Actions >Exclusive scalar f(0)(1500) meson production for energy ranges available at the GSI Facility for Antiproton and Ion Research (GSI-FAIR) and at the Japan Proton Accelerator Research Complex (J-PARC)
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Exclusive scalar f(0)(1500) meson production for energy ranges available at the GSI Facility for Antiproton and Ion Research (GSI-FAIR) and at the Japan Proton Accelerator Research Complex (J-PARC)

机译:可在GSI反质子和离子研究设施(GSI-FAIR)和日本质子加速器研究中心(J-PARC)获得能量范围的独家标量f(0)(1500)介子生产

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摘要

We evaluate differential distributions for exclusive scalar f(0)(1500) meson (glueball candidate) production for p (p) over bar -> N-1 N-2 f(0)(FAIR@GSI) and pp -> pp f(0)(J-PARC@Tokai). Both QCD diffractive, pion-pion meson exchange current (MEC) components as well as double-diffractive mechanism with intermediate pionic loop are calculated for the first time in the literature. The pion-pion component, which can be reliably calculated. dominates close to the threshold while the diffractive component may take over only for larger energies. At the moment only upper limit for the QCD-diffractive component can be obtained. The diffractive component is calculated based on two-gluon impact factors as well as in the framework of Khoze-Martin-Ryskin approach proposed for diffractive Higgs boson production. Different unintegrated gluon distribution functions (UGDFs) from the literature are used. Rather large cross sections due to pion-pion fusion are predicted for PANDA energies, where the gluonic mechanism is shown to be negligible. The production of f(0)(1500) close to threshold could limit the so-called pi N N form factor in the region of larger pion viriualities. We discuss in detail the two-pion background to the production of the f(0)(1500) meson. (C) 2009 Elsevier B.V. All rights reserved.
机译:我们在bar-> N-1 N-2 f(0)(FAIR @ GSI)和pp-> pp f上评估p(p)的排他标量f(0)(1500)介子(胶球候选)的差分分布(0)(J-PARC @ Tokai)。文献中首次计算了QCD的衍射,π-π介子交换电流(MEC)分量以及带有中间离子回路的双衍射机理。 pion-pion分量,可以可靠地计算。在接近阈值的情况下,晶格占主导地位,而衍射分量可能仅在更大的能量上占据。目前,只能获得QCD衍射分量的上限。衍射分量是基于两胶子影响因子以及在提出的用于产生希格斯玻色子衍射的Khoze-Martin-Ryskin方法的框架中计算的。使用了来自文献的不同的非积分胶子分布函数(UGDF)。对于PANDA能量,预测了由于pion-pion融合而产生的较大横截面,其中胶合子机理可忽略不计。 f(0)(1500)接近阈值的产生可能会限制较大的pion病毒性区域中的所谓pi N N形状因子。我们将详细讨论产生f(0)(1500)介子的两点背景。 (C)2009 Elsevier B.V.保留所有权利。

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