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Recent Progress in Few-Body Physics最新文献

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Experimental Study of Few Nucleon Correlations Using Deuteron Beam at Nuclotron 用氘核束在核加速器上进行少核子相关的实验研究
Pub Date : 2018-02-09 DOI: 10.1007/978-3-030-32357-8_81
M. Janek, V. Ladygin, O. Mezhenska, A. Averyanov, E. Chernykh, D. Enache, Y. Gurchin, A. Isupov, J. Karachuk, A. Khrenov, D. Krivenkov, P. Kurilkin, N. Ladygina, A. Livanov, S. Piyadin, S. Reznikov, Y. Skhomenko, A. A. Terekhin, A. V. Tishevsky, T. Uesaka, J. Urban
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引用次数: 0
Approximate Sum Rule for the Electric Dipole Moment of Light Nuclei 轻原子核电偶极矩的近似求和规则
Pub Date : 2018-02-09 DOI: 10.1007/978-3-030-32357-8_58
N. Yamanaka
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引用次数: 0
Hidden-Charm and Bottom Meson-Baryon Molecules Coupled with Five-Quark States 与五夸克态耦合的隐粲和底介子-重子分子
Pub Date : 2017-09-04 DOI: 10.1103/PhysRevD.96.114031
Y. Yamaguchi, A. Giachino, A. Hosaka, E. Santopinto, S. Takeuchi, M. Takizawa
In this paper, we investigate the hidden-charm pentaquarks as $bar{D}^{(ast)}Lambda_{rm c}$ and $bar{D}^{(ast)}Sigma^{(ast)}_{rm c}$ molecules coupled to the five-quark states. Furthermore, we extend our calculations to the hidden-bottom sector. The coupling to the five-quark states is treated as the short range potential, where the relative strength for the meson-baryon channels is determined by the structure of the five-quark states. We found that resonant and/or bound states appear in both the charm and bottom sectors. The five-quark state potential turned out to be attractive and, for this reason, it plays an important role to produce these states. In the charm sector, we need the five-quark potential in addition to the pion exchange potential in producing bound and resonant states, whereas, in the bottom sector, the pion exchange interaction is strong enough to produce states. Thus, from this investigation, it emerges that the hidden-bottom pentaquarks are more likely to form than their hidden-charm counterparts; for this reason, we suggest that the experimentalists should look for states in the bottom sector.
本文研究了与五夸克态耦合的隐粲五夸克分子$bar{D}^{(ast)}Lambda_{rm c}$和$bar{D}^{(ast)}Sigma^{(ast)}_{rm c}$。此外,我们将计算扩展到隐藏底部部门。与五夸克态的耦合被视为短程势,其中介子-重子通道的相对强度由五夸克态的结构决定。我们发现共振和/或束缚状态出现在魅力部门和底层部门。五夸克态势被证明是有吸引力的,因此,它在产生这些态中起着重要的作用。在粲扇区,除了介子交换势外,我们还需要五夸克势来产生束缚态和共振态,而在底扇区,介子交换相互作用足够强,可以产生态。因此,从这项研究中可以发现,隐藏底五夸克比隐藏粲子更容易形成;出于这个原因,我们建议实验学家应该寻找底层部分的状态。
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引用次数: 43
Direct Measurement of the $${^{13}}C(alpha ,n)^{16}O$$ Reaction at LUNA 月球上$${^{13}}C(alpha ,n)^{16}O$$反应的直接测量
Pub Date : 1900-01-01 DOI: 10.1007/978-3-030-32357-8_49
G. F. Ciani, L. Csedreki, J. Balibrea-Correa, A. Best
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引用次数: 0
期刊
Recent Progress in Few-Body Physics
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