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首页> 外文期刊>Physics Reports: A Review Section of Physics Letters (Section C) >Pentaquark Theta(+)(1540) production in gamma N -> K(K)overbar N reactions
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Pentaquark Theta(+)(1540) production in gamma N -> K(K)overbar N reactions

机译:Pentaquark Theta(+)(1540)在N N-> K(K)Overbar N反应中的产生

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摘要

Recent developments in the search of exotic pentaquark hadrons are briefly reviewed. We then focus on investigating how the exotic pentaquark Theta(1540) baryon production can be identified in the gamma N -> K (K) over barN reactions, focusing on the influence of the background (non-Theta production) mechanisms. By imposing the SU(3) symmetry and using various quark model predictions, we are able to fix the coupling constants for evaluating the kaon backgrounds, the K (K) over bar production through the intermediate vector meson and tensor meson photoproduction, and the mechanisms involving intermediate A(I 116), A(1405), A (1520), Sigma(1 193), Sigma(1 385), and A (1232) states. The vector meson photoproduction part is calculated from a phenomenological model which describes well the experimental data at low energies. We point out that the neutral tensor meson production cannot be due to pi(0)-exchange as done by Dzierba et al. [Phys. Rev. D 69 (2004) 051901] because of C parity. The neutral tensor meson production is estimated by considering the vector meson exchange and found to be too weak to generate any peak at the position near Theta(1540). For Theta(1540) production, we assume that it is an isoscalar and hence can only be produced in gamma n K(+)K(-)n and gamma p -> K-0(K) over bar (0)p reactions, but not in gamma p -> K(+)K(-)p and gamma n -> K-0(K) over bar (0)n. The total cross section data of gamma p -> K(+)K(-)p is thus used to fix the form factors which regularize the background amplitudes so that the signal of Theta(1540) in gamma n -> K(+)K(-)n and gamma p -> K-0(K) over bar (0)p cross sections can be predicted. We find that the predicted K+K- and K(+)n invariant mass distributions of the gamma n -> K(+)K(-)n reaction can qualitatively reproduce the shapes of the JLab data. However, the predicted Theta(1540) peak cannot be identified unambiguously with the data. High statistics experiments are needed to resolve the problem. We also find that an even-parity Theta is more likely to be detected, while it will be difficult to identify an odd-parity Theta, even if it exists, from the background continuum, if its coupling constants are small as in the present quark model predictions. (c) 2005 Elsevier B.V. All rights reserved.
机译:简要回顾了寻找奇异的五夸克强子的最新进展。然后,我们着重研究如何通过barN反应在伽马N-> K(K)中识别奇异的五夸克Theta(1540)重子产生,重点是背景(非Theta产生)机制的影响。通过施加SU(3)对称性并使用各种夸克模型预测,我们能够固定耦合常数,以通过中间矢量介子和张量介子光产生来评估kaon背景,K(K)超过条形产生以及机制涉及中间体A(I 116),A(1405),A(1520),Sigma(1 193),Sigma(1 385)和A(1232)状态。矢量介子光产生部分是根据现象模型计算的,该模型很好地描述了低能量下的实验数据。我们指出,中性张量介子的产生不能归因于Dzierba等人所做的pi(0)交换。 [物理Rev. D 69(2004)051901]。中性张量介子的产生是通过考虑矢量介子交换来估算的,发现它太弱而无法在Theta(1540)附近的位置产生任何峰值。对于Theta(1540)的生成,我们假设它是等量的,因此只能在bar(0)p反应上以γn K(+)K(-)n和γp-> K-0(K)生成。 ,但不在(0)n上方的γp-> K(+)K(-)p和γn-> K-0(K)中。因此,将γp-> K(+)K(-)p的总横截面数据用于固定使背景振幅规则化的形状因子,以使Theta(1540)的信号在γn-> K(+)中可以预测在(0)p条横截面上的K(-)n和γp-> K-0(K)。我们发现,γn-> K(+)K(-)n反应的预测K + K-和K(+)n不变质量分布可以定性地再现JLab数据的形状。但是,预测的Theta(1540)峰无法与数据明确识别。要解决此问题,需要进行大量的统计实验。我们还发现,偶校验奇偶性更可能被检测到,即使它的耦合常数很小(如在当前夸克中),也很难从背景连续体中识别奇偶校验奇偶性(即使存在)。模型预测。 (c)2005 Elsevier B.V.保留所有权利。

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