Constraining the DDD* three-body bound state via the Zc(3900) pole

IF 5 2区 物理与天体物理 Q1 Physics and Astronomy
Hai-Xiang Zhu, Lu Meng, Yao Ma, Ning Li, Wei Chen, Shi-Lin Zhu
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The existence of the <g:math xmlns:g=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><g:mi>D</g:mi><g:mi>D</g:mi><g:msup><g:mi>D</g:mi><g:mo>*</g:mo></g:msup></g:math> bound state remains uncertain due to significant variations in the OBE interaction, particularly in the strength of scalar-meson-exchange interactions, which can differ by a factor about 20 between two commonly used OBE models. This discrepancy renders the <i:math xmlns:i=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><i:mi>D</i:mi><i:mi>D</i:mi><i:msup><i:mi>D</i:mi><i:mo>*</i:mo></i:msup></i:math> system highly model-dependent. To address this issue, we constrain the scalar-meson-exchange interaction using the <k:math xmlns:k=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><k:msub><k:mi>Z</k:mi><k:mi>c</k:mi></k:msub><k:mo stretchy=\"false\">(</k:mo><k:mn>3900</k:mn><k:mo stretchy=\"false\">)</k:mo></k:math> pole position, where the pseudoscalar-meson coupling is well-determined, and the <o:math xmlns:o=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><o:mi>ρ</o:mi></o:math>- and <q:math xmlns:q=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><q:mi>ω</q:mi></q:math>-exchange interactions nearly cancel each other out, leaving the coupling constant of the <s:math xmlns:s=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><s:mi>σ</s:mi></s:math>-exchange as the only unknown parameter. Our results indicate that the isospin-<u:math xmlns:u=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><u:mfrac><u:mn>1</u:mn><u:mn>2</u:mn></u:mfrac></u:math> <w:math xmlns:w=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><w:mi>D</w:mi><w:mi>D</w:mi><w:msup><w:mi>D</w:mi><w:mo>*</w:mo></w:msup></w:math> bound states exist when <y:math xmlns:y=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><y:msub><y:mi>Z</y:mi><y:mi>c</y:mi></y:msub><y:mo stretchy=\"false\">(</y:mo><y:mn>3900</y:mn><y:mo stretchy=\"false\">)</y:mo></y:math> is a virtual state of <cb:math xmlns:cb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><cb:mrow><cb:mi>D</cb:mi><cb:msup><cb:mrow><cb:mover accent=\"true\"><cb:mrow><cb:mi>D</cb:mi></cb:mrow><cb:mrow><cb:mo stretchy=\"false\">¯</cb:mo></cb:mrow></cb:mover></cb:mrow><cb:mrow><cb:mo>*</cb:mo></cb:mrow></cb:msup><cb:mo>/</cb:mo><cb:mover accent=\"true\"><cb:mrow><cb:mi>D</cb:mi></cb:mrow><cb:mrow><cb:mo stretchy=\"false\">¯</cb:mo></cb:mrow></cb:mover><cb:msup><cb:mrow><cb:mi>D</cb:mi></cb:mrow><cb:mrow><cb:mo>*</cb:mo></cb:mrow></cb:msup></cb:mrow></cb:math> located within approximately <ib:math xmlns:ib=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ib:mo>−</ib:mo><ib:mn>15</ib:mn><ib:mtext> </ib:mtext><ib:mtext> </ib:mtext><ib:mi>MeV</ib:mi></ib:math> of the threshold. However, the three-body bound state is gone when the <kb:math xmlns:kb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><kb:msub><kb:mi>Z</kb:mi><kb:mi>c</kb:mi></kb:msub><kb:mo stretchy=\"false\">(</kb:mo><kb:mn>3900</kb:mn><kb:mo stretchy=\"false\">)</kb:mo></kb:math> virtual state pole is more than 20 MeV away from the threshold. Each experimental progress, either on the <ob:math xmlns:ob=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ob:mi>D</ob:mi><ob:mi>D</ob:mi><ob:msup><ob:mi>D</ob:mi><ob:mo>*</ob:mo></ob:msup></ob:math> state or the <qb:math xmlns:qb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><qb:msub><qb:mi>Z</qb:mi><qb:mi>c</qb:mi></qb:msub><qb:mo stretchy=\"false\">(</qb:mo><qb:mn>3900</qb:mn><qb:mo stretchy=\"false\">)</qb:mo></qb:math>, can shed light on the nature of the other state. Another significant outcome is a refined set of OBE model parameters calibrated using the pole positions of <ub:math xmlns:ub=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ub:mi>X</ub:mi><ub:mo stretchy=\"false\">(</ub:mo><ub:mn>3872</ub:mn><ub:mo stretchy=\"false\">)</ub:mo></ub:math>, <yb:math xmlns:yb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><yb:msub><yb:mi>T</yb:mi><yb:mrow><yb:mi>c</yb:mi><yb:mi>c</yb:mi></yb:mrow></yb:msub><yb:mo stretchy=\"false\">(</yb:mo><yb:mn>3875</yb:mn><yb:mo stretchy=\"false\">)</yb:mo></yb:math>, and <cc:math xmlns:cc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><cc:msub><cc:mi>Z</cc:mi><cc:mi>c</cc:mi></cc:msub><cc:mo stretchy=\"false\">(</cc:mo><cc:mn>3900</cc:mn><cc:mo stretchy=\"false\">)</cc:mo></cc:math>, rigorously addressing the cutoff dependence. These parameters provide a valuable resource for more accurate calculations of systems involving few-body <gc:math xmlns:gc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><gc:mi>D</gc:mi></gc:math>, <ic:math xmlns:ic=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ic:msup><ic:mi>D</ic:mi><ic:mo>*</ic:mo></ic:msup></ic:math>, and their antiparticles. Additionally, we find no evidence of the <kc:math xmlns:kc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><kc:mi>D</kc:mi><kc:mi>D</kc:mi><kc:msup><kc:mi>D</kc:mi><kc:mo>*</kc:mo></kc:msup></kc:math> three-body resonances after extensive search using a combination of the Gaussian expansion method and the complex scaling method. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2025</jats:copyright-year> </jats:permissions> </jats:supplementary-material>","PeriodicalId":20167,"journal":{"name":"Physical Review D","volume":"13 1","pages":""},"PeriodicalIF":5.0000,"publicationDate":"2025-05-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physical Review D","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1103/physrevd.111.094022","RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"Physics and Astronomy","Score":null,"Total":0}
引用次数: 0

Abstract

In this study, we propose using the Zc(3900) pole position to constrain the existence of the DDD* three-body bound state within the one-boson-exchange (OBE) model. The existence of the DDD* bound state remains uncertain due to significant variations in the OBE interaction, particularly in the strength of scalar-meson-exchange interactions, which can differ by a factor about 20 between two commonly used OBE models. This discrepancy renders the DDD* system highly model-dependent. To address this issue, we constrain the scalar-meson-exchange interaction using the Zc(3900) pole position, where the pseudoscalar-meson coupling is well-determined, and the ρ- and ω-exchange interactions nearly cancel each other out, leaving the coupling constant of the σ-exchange as the only unknown parameter. Our results indicate that the isospin-12 DDD* bound states exist when Zc(3900) is a virtual state of DD¯*/D¯D* located within approximately 15 MeV of the threshold. However, the three-body bound state is gone when the Zc(3900) virtual state pole is more than 20 MeV away from the threshold. Each experimental progress, either on the DDD* state or the Zc(3900), can shed light on the nature of the other state. Another significant outcome is a refined set of OBE model parameters calibrated using the pole positions of X(3872), Tcc(3875), and Zc(3900), rigorously addressing the cutoff dependence. These parameters provide a valuable resource for more accurate calculations of systems involving few-body D, D*, and their antiparticles. Additionally, we find no evidence of the DDD* three-body resonances after extensive search using a combination of the Gaussian expansion method and the complex scaling method. Published by the American Physical Society 2025
通过Zc(3900)极点约束DDD*三体束缚态
在本研究中,我们提出使用Zc(3900)极点位置来约束单玻色子交换(OBE)模型中DDD*三体束缚态的存在。DDD*束缚态的存在仍然是不确定的,因为在OBE相互作用中存在显著的变化,特别是在标量-介子交换相互作用的强度上,在两种常用的OBE模型之间可能相差约20倍。这种差异使得DDD*系统高度依赖于模型。为了解决这个问题,我们使用Zc(3900)极点位置来约束标量-介子交换相互作用,其中伪标量-介子耦合是确定的,ρ-和ω-交换相互作用几乎相互抵消,留下σ-交换的耦合常数作为唯一的未知参数。结果表明,当Zc(3900)为DD¯*/D¯D*的虚态时,在阈值的−15 MeV范围内存在同位旋-12 DDD*束缚态。然而,当Zc(3900)虚态极距阈值超过20mev时,三体束缚态消失。无论是DDD*态还是Zc(3900)态,每一个实验进展都能揭示另一种状态的性质。另一个重要的结果是使用X(3872)、Tcc(3875)和Zc(3900)的极点位置校准的一组精细化的OBE模型参数,严格地解决了截止依赖性。这些参数为更精确地计算涉及少体D、D*及其反粒子的系统提供了宝贵的资源。此外,在结合高斯展开法和复标度法进行广泛搜索后,我们没有发现DDD*三体共振的证据。2025年由美国物理学会出版
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来源期刊
Physical Review D
Physical Review D 物理-天文与天体物理
CiteScore
9.20
自引率
36.00%
发文量
0
审稿时长
2 months
期刊介绍: Physical Review D (PRD) is a leading journal in elementary particle physics, field theory, gravitation, and cosmology and is one of the top-cited journals in high-energy physics. PRD covers experimental and theoretical results in all aspects of particle physics, field theory, gravitation and cosmology, including: Particle physics experiments, Electroweak interactions, Strong interactions, Lattice field theories, lattice QCD, Beyond the standard model physics, Phenomenological aspects of field theory, general methods, Gravity, cosmology, cosmic rays, Astrophysics and astroparticle physics, General relativity, Formal aspects of field theory, field theory in curved space, String theory, quantum gravity, gauge/gravity duality.
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