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Erratum to: (gamma )-Ray spectroscopy above the 9(^+) isomeric state in the N = Z nucleus (^{66})As 勘误:(gamma ) -射线光谱上的9 (^+)同分异构体状态在N = Z核(^{66}) As
IF 2.8 3区 物理与天体物理 Q2 PHYSICS, NUCLEAR Pub Date : 2025-11-10 DOI: 10.1140/epja/s10050-025-01729-9
Henna Joukainen, Panu Ruotsalainen, Jan Sarén, Praveen C. Srivastava, Deepak Patel, Rauno Julin, Kalle Auranen, Zhuang Ge, Tuomas Grahn, Paul Greenlees, Andres Illana, Henri Jutila, Matti Leino, Jussi Louko, Minna Luoma, Joonas Ojala, Janne Pakarinen, Panu Rahkila, Mikael Sandzelius, Holly Tann, Juha Uusitalo, George L. Zimba
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引用次数: 0
The role of the (f_0(1710)) and (a_0(1710)) resonances in the (D^0 rightarrow rho ^0 phi ), (omega phi ) decays (f_0(1710))和(a_0(1710))共振在(D^0 rightarrow rho ^0 phi )、(omega phi )衰变中的作用
IF 2.8 3区 物理与天体物理 Q2 PHYSICS, NUCLEAR Pub Date : 2025-11-08 DOI: 10.1140/epja/s10050-025-01717-z
Natsumi Ikeno, Wen-Hao Jia, Wei-Hong Liang, Eulogio Oset

We study the (D^0 rightarrow rho ^0 phi ), (omega phi ) decays which proceed in a direct mode via internal emission with equal rates. Yet, the experimental branching ratio for the (rho ^0 phi ) mode is twice as big as that for the (omega phi ) mode. We find a natural explanation based on the extra indirect mechanism where (K^{*+} K^{*-}) is produced via external emission and that channel undergoes final state interaction with other vector–vector channels to lead to the (rho ^0 phi ), (omega phi ) final states, with transition amplitudes dominated by the (a_0(1710)) resonance, recently discovered, and (f_0(1710)) respectively. The large coupling of the (a_0(1710)) to the (rho ^0 phi ) channel is mostly responsible for this large ratio of the production rates.

我们研究了(D^0 rightarrow rho ^0 phi ), (omega phi )衰变,它们通过内部发射以等速率以直接模式进行。然而,(rho ^0 phi )模态的实验分支比(omega phi )模态的实验分支比大两倍。我们发现了一个基于额外间接机制的自然解释,其中(K^{*+} K^{*-})是通过外部发射产生的,并且该通道与其他矢量-矢量通道进行最终状态相互作用,从而导致(rho ^0 phi ), (omega phi )最终状态,其跃迁幅度分别由最近发现的(a_0(1710))共振和(f_0(1710))主导。(a_0(1710))与(rho ^0 phi )通道的大耦合是造成如此大比例生产速率的主要原因。
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引用次数: 0
Retraction Note: A probability of synthesis of the superheavy element Z = 124 注:超重元素合成的概率Z = 124
IF 2.8 3区 物理与天体物理 Q2 PHYSICS, NUCLEAR Pub Date : 2025-11-07 DOI: 10.1140/epja/s10050-025-01735-x
H. C. Manjunatha, K. N. Sridhar
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引用次数: 0
Revisiting the (^{12})C+(^{208})Pb reaction: a comprehensive CRC study with the São Paulo potential 重新审视(^{12}) C+ (^{208}) Pb反应:具有<s:1>圣保罗电位的CRC综合研究
IF 2.8 3区 物理与天体物理 Q2 PHYSICS, NUCLEAR Pub Date : 2025-11-07 DOI: 10.1140/epja/s10050-025-01721-3
L. R. Gasques, J. M. Brandão Neto, L. C. Chamon, V. Scarduelli

We present a comprehensive coupled reaction channels analysis of the (^{12})C+(^{208})Pb system over a broad range of bombarding energies, employing the parameter-free São Paulo potential for the real part of the nuclear interaction. The calculations include couplings to low-lying inelastic states and transfer channels, with no adjustable parameters. Theoretical results are compared with experimental data for elastic scattering, fusion, inelastic excitation, and transfer cross sections. The inclusion of channel couplings significantly improves the agreement with the data. These findings reaffirm the predictive power of the São Paulo potential and underscore the importance of coupled reaction channels calculations in describing heavy-ion collisions, not only near the Coulomb barrier but also at much higher energies.

我们对(^{12}) C+ (^{208}) Pb体系在广泛的轰击能量范围内的耦合反应通道进行了全面的分析,采用无参数圣保罗势作为核相互作用的实部。计算包括与低洼非弹性状态和传输通道的耦合,没有可调参数。对弹性散射、聚变、非弹性激发和转移截面的实验数据进行了比较。信道耦合的加入显著提高了与数据的一致性。这些发现重申了圣保罗势的预测能力,并强调了耦合反应通道计算在描述重离子碰撞中的重要性,不仅在库仑势垒附近,而且在更高的能量下。
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引用次数: 0
Extreme Light Infrastructure - Nuclear Physics: first results 极端光基础设施-核物理:第一个结果
IF 2.8 3区 物理与天体物理 Q2 PHYSICS, NUCLEAR Pub Date : 2025-11-07 DOI: 10.1140/epja/s10050-025-01713-3
C. A. Ur, D. Balabanski, M. Cernăianu, D. Doria, P. Ghenuche, A. Kusoglu, N. Safca, P.-A. Söderstrom, D. Stutman

Extreme Light Infrastructure - Nuclear Physics (ELI-NP) is the nuclear physics pillar of the pan-European project Extreme Light Infrastructure. Started in 2012, the project has accomplished several milestones that have placed it among the most relevant research infrastructures worldwide in nuclear photonics. Two main extreme light sources were included in the ELI-NP project, a 2 x 10 PW laser system and a high intensity gamma beam system. The high power laser system is operational since 2020 and delivers beam time to users. The gamma beam system is still under construction. Several experimental setups have been developed and commissioned for the two extreme light beams. The paper makes an overview of some of the first results obtained with the research infrastructure developed at ELI-NP.

极光基础设施-核物理(ELI-NP)是泛欧项目极光基础设施的核物理支柱。该项目于2012年启动,已经完成了几个里程碑,使其成为核光子学领域全球最相关的研究基础设施之一。ELI-NP项目包括两个主要的极端光源,一个2 x 10 PW激光系统和一个高强度伽马光束系统。高功率激光系统自2020年开始运行,并向用户提供光束时间。伽马光束系统仍在建设中。针对这两种极端光束,已经开发并启用了几个实验装置。本文概述了在ELI-NP开发的研究基础设施获得的一些初步结果。
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引用次数: 0
Retraction Note to: New semi-empirical formula for α-decay half-lives of the heavy and superheavy nuclei 注:重核和超重核α衰变半衰期的新半经验公式
IF 2.8 3区 物理与天体物理 Q2 PHYSICS, NUCLEAR Pub Date : 2025-11-05 DOI: 10.1140/epja/s10050-025-01734-y
H. C. Manjunatha, K. N. Sridhar
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引用次数: 0
Cross section measurement for the (^{16})O(n, ({alpha }_0))(^{13})C reaction in 6.8–11.7 MeV neutron energy region 在6.8-11.7 MeV中子能区(^{16}) O(n, ({alpha }_0)) (^{13}) C反应的截面测量
IF 2.8 3区 物理与天体物理 Q2 PHYSICS, NUCLEAR Pub Date : 2025-11-05 DOI: 10.1140/epja/s10050-025-01730-2
Cong Xia, Zhenpeng Chen, Yiwei Hu, Jie Liu, Zepeng Wu, Haofan Bai, Wenkai Ren, Yu. M. Gledenov, E. Sansarbayar, G. Khuukhenkhuu, L. Krupa, I. Chuprakov, Xichao Ruan, Hanxiong Huang, Jie Ren, Xiaofei Wang, Bin Shao, Li’ao Zhao, Wentian Cao, Tieshuan Fan, Guohui Zhang

Cross sections of the (^{16})O(n, (alpha _0))(^{13})C reaction were measured in the 6.8–11.7 MeV neutron energy region based on the HI-13 tandem accelerator of China Institute of Atomic Energy (CIAE). Two experiments were performed in 2022 and 2023 at total 21 neutron energy points. A gridded ionization chamber (GIC) was used as the charged particle detector, with working gas of 3.0 atm Kr+4.0%CO(_2) in 2022 and 4.0 atm Kr+3.0%CO(_2) in 2023. The oxygen atoms in the CO(_2) were used as the gas sample. A (^{238})U(_3)O(_8) sample inside the GIC was used to determine the neutron fluences and an EJ-309 scintillation detector was placed on the beam line to measure the neutron energy spectra to correct the events induced by the low-energy neutrons. Based on the present measurement cross sections and existing measurement data from the EXFOR library, R-matrix analysis was carried out for the (n + ^{16})O system using the RAC code. Present cross sections are compared with existing measurement data and evaluation data. In the 6.8–9.5 MeV neutron energy region our measurement results are consistent with the evaluation data in the ENDF/B-VIII.1 library. In the 9.5–11.7 MeV neutron energy region, A peak near 10.5 MeV in the excitation function in our measurement and R-matrix calculation results was obtained while the excitation functions given by the evaluations and existing measurements have a valley structure.

利用中国原子能科学研究院的HI-13串列加速器,在6.8 ~ 11.7 MeV中子能量区测量了(^{16}) O(n, (alpha _0)) (^{13}) C反应的截面。在2022年和2023年进行了两次实验,总共有21个中子能量点。采用栅格电离室(GIC)作为带电粒子探测器,工作气体为3.0 atm Kr+4.0%CO(_2) in 2022 and 4.0 atm Kr+3.0%CO(_2) in 2023. The oxygen atoms in the CO(_2) were used as the gas sample. A (^{238})U(_3)O(_8) sample inside the GIC was used to determine the neutron fluences and an EJ-309 scintillation detector was placed on the beam line to measure the neutron energy spectra to correct the events induced by the low-energy neutrons. Based on the present measurement cross sections and existing measurement data from the EXFOR library, R-matrix analysis was carried out for the (n + ^{16})O system using the RAC code. Present cross sections are compared with existing measurement data and evaluation data. In the 6.8–9.5 MeV neutron energy region our measurement results are consistent with the evaluation data in the ENDF/B-VIII.1 library. In the 9.5–11.7 MeV neutron energy region, A peak near 10.5 MeV in the excitation function in our measurement and R-matrix calculation results was obtained while the excitation functions given by the evaluations and existing measurements have a valley structure.
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引用次数: 0
Suppression in compound nuclear fusion at low projectile energies 低抛射能量下复合核聚变的抑制
IF 2.8 3区 物理与天体物理 Q2 PHYSICS, NUCLEAR Pub Date : 2025-11-04 DOI: 10.1140/epja/s10050-025-01725-z
Rajesh K. Sahoo, Dharmendra Singh, Amritraj Mahato, Pankaj K. Giri, Nitin Sharma, Lupteindu Chhura, Rahul Mahato, Sneha B. Linda, Harish Kumar, Suhail A. Tali, Rahbar Ali, M. Afzal Ansari, R. Kumar, S. Muralithar, R. P. Singh

In this study, the excitation functions of evaporation residues produced in the (^{18})O + (^{144})Sm system have been measured through offline (gamma ) ray spectrometry. The statistical model code PACE-4, ALICE91, and EMPIRE 3.2.2 were utilized to distinguish the evaporation residues populated through the compound and non-compound nuclear fusion processes. For a comprehensive investigation of fusion suppression and its correlation with the charge of the target and the (Q_{alpha }) value of the projectile, the compound nuclear fusion cross sections of various projectile-target combinations were analyzed within the framework of the Universal Fusion Function (UFF) reduction method. The study revealed that the measured fusion functions of various systems were suppressed compared to the UFF, where the degree of suppression was dependent on the projectile’s (Q_{alpha }) value. Besides that, an exponential increase in the suppression was further observed with increasing (Q_{alpha }) values, while the target charge had a marginal effect. A generalized formula based on present study has been proposed to estimate fusion suppression of different systems as a function of (Q_{alpha }) value of the projectile. The above observations indicates that the involvement of non-compound nuclear reactions leads to a reduction in the compound nuclear fusion cross section at energies above the Coulomb barrier. This is primarily attributed to the loss of flux in the compound nuclear fusion channel, which is offset by an increased flux in non-compound fusion processes.

在本研究中,通过离线(gamma )射线能谱法测量了(^{18}) O + (^{144}) Sm体系中产生的蒸发残留物的激发函数。利用统计模型代码PACE-4、ALICE91和EMPIRE 3.2.2来区分化合物和非化合物核聚变过程中填充的蒸发残留物。为了全面研究核聚变抑制及其与靶载药量和弹丸(Q_{alpha })值的相关性,在通用聚变函数(UFF)约简法的框架下,分析了不同弹靶组合的复合核聚变截面。研究表明,与UFF相比,各种系统的测量融合函数被抑制,其中抑制程度取决于弹丸的(Q_{alpha })值。此外,随着(Q_{alpha })值的增加,抑制作用呈指数增长,而目标电荷的作用则是边际效应。在本研究的基础上,提出了一个估计不同系统的融合抑制作为弹丸(Q_{alpha })值的函数的广义公式。上述观察结果表明,非复合核反应的参与导致库仑势垒以上能量处复合核聚变截面的减小。这主要是由于复合核聚变通道中通量的损失,而非复合核聚变过程中通量的增加抵消了这一损失。
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引用次数: 0
Deciphering the influence of multi neutron transfer in Si-based fusion reactions around the Coulomb barrier 破解围绕库仑势垒的硅基聚变反应中多中子转移的影响
IF 2.8 3区 物理与天体物理 Q2 PHYSICS, NUCLEAR Pub Date : 2025-11-03 DOI: 10.1140/epja/s10050-025-01720-4
Rinku Prajapat

The enhancement in sub-barrier fusion cross-sections caused by different intrinsic degrees of freedom, such as inelastic excitations and deformations, has been well explored. However, the influence of positive Q-value neutron transfer channels and their microscopic understanding on fusion dynamics have still been far from complete. Therefore, I aim to investigate the role of multi neutron transfer channels on the dynamics of fusion reactions around the Coulomb barrier by judicially selecting 11 different (^{28,30})Si-induced systems. These reactions are chosen in such a way that they possess positive and negative Q-values for neutron transfer channels to make the comparison more apparent. For this purpose, a channel coupling approach within the framework of a semiclassical model is being used to investigate the role of multi-neutron transfer with positive Q-values on fusion phenomena. The sub-barrier fusion enhancement compared to the one-dimensional barrier penetration model (uncoupled) is investigated by considering collective excitations in colliding nuclei and multi-neutron transfer channels with Q > 0 within the channel coupling model. All the fusion excitation functions, except for a few cases, have been successfully explained by the coupled channel calculations using the channel coupling model. Slight deviation from the model calculations is observed for (^{28})Si+(^{90,92})Zr below the Coulomb barrier and (^{28})Si+(^{144})Nd in the above-barrier energy region. Only the significant effect of up to 2n pickup transfer with Q > 0 was found on sub-barrier fusion.

不同的固有自由度(如非弹性激励和变形)引起的亚势垒熔合截面的增强已经得到了很好的探讨。然而,正q值中子传递通道对核聚变动力学的影响及其微观认识还远未完成。因此,我的目的是通过选择11种不同的(^{28,30})硅诱导体系来研究多中子传递通道对库仑势垒周围聚变反应动力学的作用。选择这些反应的方式使它们具有中子传递通道的正q值和负q值,以使比较更加明显。为此,在半经典模型框架内的通道耦合方法被用于研究具有正q值的多中子转移对聚变现象的作用。通过考虑碰撞核的集体激发和通道耦合模型中Q &gt; 0的多中子传递通道,研究了与一维势垒穿透模型(不耦合)相比,亚势垒核聚变的增强。除个别情况外,所有的聚变激发函数都可以用通道耦合模型的耦合通道计算得到解释。对于库仑势垒以下的(^{28}) Si+ (^{90,92}) Zr和势垒以上的(^{28}) Si+ (^{144}) Nd,模型计算略有偏差。在亚势垒聚变中,只有Q &gt; 0的高达2n的拾取转移有显著影响。
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引用次数: 0
Decays of the vector charmonium and bottomonium hybrids 载体夏莫铵和底溴铵杂交体的衰变
IF 2.8 3区 物理与天体物理 Q2 PHYSICS, NUCLEAR Pub Date : 2025-11-02 DOI: 10.1140/epja/s10050-025-01722-2
B. Barsbay

The full widths of the vector charmonium and bottomonium hybrid mesons (H_{ textrm{c}}) and (H_{textrm{b}}), characterized by the quantum numbers (1^{ mathrm {--}}), are determined by analyzing their dominant strong decay modes: (H_{textrm{c}} rightarrow D^{+}D^{-}), (D_{0}overline{D}_{0}), ( D_{s}^{+}D_{s}^{-} ), ( D^{*+}D^{*-} ), ( D^{*0}overline{D}^{*0}), ( D^{*+}D^{-} ), ( D^{*0}overline{D}^{0} ), (D_{s}^{*+}D_{s}^{-} ) and (H_{textrm{b}} rightarrow B^{+}B^{-}), (B_{0}overline{B}_{0}). To evaluate the partial widths of these channels, we employ the QCD three-point sum rule approach, which provides a reliable method for extracting the strong coupling constants at the relevant hybrid-meson–meson interaction vertices. Based on this analysis, the full widths of these hybrid quarkonia are found to be (Gamma _{H_{textrm{c}}} =(309.6pm 39.0)~ textrm{MeV} ) and (Gamma _{H_{textrm{b}}} =(78.8pm 15.4)~textrm{MeV} ). These results are expected to facilitate the interpretation of future experimental data concerning the spectroscopy and decay patterns of exotic charmonium- and bottomonium-like hybrid mesons.

通过分析其优势强衰变模式(H_{textrm{c}} rightarrow D^{+}D^{-})、(D_{0}overline{D}_{0})、( D_{s}^{+}D_{s}^{-} )、( D^{*+}D^{*-} )、( D^{*0}overline{D}^{*0})、( D^{*+}D^{-} )、( D^{*0}overline{D}^{0} )、(D_{s}^{*+}D_{s}^{-} )、(H_{textrm{b}} rightarrow B^{+}B^{-})、(B_{0}overline{B}_{0}),确定了矢量charmonium和bottomonium杂化介子(H_{ textrm{c}})和(H_{textrm{b}})的全宽度,量子数为(1^{ mathrm {--}})。为了评估这些通道的部分宽度,我们采用了QCD三点和规则方法,该方法为提取相关杂介子-介子-介子相互作用顶点的强耦合常数提供了一种可靠的方法。在此基础上,杂交夸克虫的全宽分别为(Gamma _{H_{textrm{c}}} =(309.6pm 39.0)~ textrm{MeV} )和(Gamma _{H_{textrm{b}}} =(78.8pm 15.4)~textrm{MeV} )。这些结果预计将有助于解释未来有关外来类恰蒙和类底铌杂化介子的光谱和衰变模式的实验数据。
{"title":"Decays of the vector charmonium and bottomonium hybrids","authors":"B. Barsbay","doi":"10.1140/epja/s10050-025-01722-2","DOIUrl":"10.1140/epja/s10050-025-01722-2","url":null,"abstract":"<div><p>The full widths of the vector charmonium and bottomonium hybrid mesons <span>(H_{ textrm{c}})</span> and <span>(H_{textrm{b}})</span>, characterized by the quantum numbers <span>(1^{ mathrm {--}})</span>, are determined by analyzing their dominant strong decay modes: <span>(H_{textrm{c}} rightarrow D^{+}D^{-})</span>, <span>(D_{0}overline{D}_{0})</span>, <span>( D_{s}^{+}D_{s}^{-} )</span>, <span>( D^{*+}D^{*-} )</span>, <span>( D^{*0}overline{D}^{*0})</span>, <span>( D^{*+}D^{-} )</span>, <span>( D^{*0}overline{D}^{0} )</span>, <span>(D_{s}^{*+}D_{s}^{-} )</span> and <span>(H_{textrm{b}} rightarrow B^{+}B^{-})</span>, <span>(B_{0}overline{B}_{0})</span>. To evaluate the partial widths of these channels, we employ the QCD three-point sum rule approach, which provides a reliable method for extracting the strong coupling constants at the relevant hybrid-meson–meson interaction vertices. Based on this analysis, the full widths of these hybrid quarkonia are found to be <span>(Gamma _{H_{textrm{c}}} =(309.6pm 39.0)~ textrm{MeV} )</span> and <span>(Gamma _{H_{textrm{b}}} =(78.8pm 15.4)~textrm{MeV} )</span>. These results are expected to facilitate the interpretation of future experimental data concerning the spectroscopy and decay patterns of exotic charmonium- and bottomonium-like hybrid mesons.</p></div>","PeriodicalId":786,"journal":{"name":"The European Physical Journal A","volume":"61 11","pages":""},"PeriodicalIF":2.8,"publicationDate":"2025-11-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145426008","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
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The European Physical Journal A
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