{"title":"(J/ψ,J/ψ)和(ηc,ηc)在 B 工厂的电子-正电子湮灭中通过两个中间光子产生","authors":"Shashank Bhatnagar , Hluf Negash","doi":"10.1016/j.nuclphysa.2024.122969","DOIUrl":null,"url":null,"abstract":"<div><div>We study the processes, <span><math><msup><mrow><mi>e</mi></mrow><mrow><mo>−</mo></mrow></msup><msup><mrow><mi>e</mi></mrow><mrow><mo>+</mo></mrow></msup><mo>→</mo><msup><mrow><mi>γ</mi></mrow><mrow><mo>⁎</mo></mrow></msup><msup><mrow><mi>γ</mi></mrow><mrow><mo>⁎</mo></mrow></msup><mo>→</mo><mi>J</mi><mo>/</mo><mi>ψ</mi><mo>+</mo><mi>J</mi><mo>/</mo><mi>ψ</mi></math></span>, and <span><math><msup><mrow><mi>e</mi></mrow><mrow><mo>−</mo></mrow></msup><msup><mrow><mi>e</mi></mrow><mrow><mo>+</mo></mrow></msup><mo>→</mo><msup><mrow><mi>γ</mi></mrow><mrow><mo>⁎</mo></mrow></msup><msup><mrow><mi>γ</mi></mrow><mrow><mo>⁎</mo></mrow></msup><mo>→</mo><msub><mrow><mi>η</mi></mrow><mrow><mi>c</mi></mrow></msub><mo>+</mo><msub><mrow><mi>η</mi></mrow><mrow><mi>c</mi></mrow></msub></math></span> at <span><math><msqrt><mrow><mi>s</mi></mrow></msqrt><mo>=</mo><mn>10.6</mn></math></span> GeV in the framework of <span><math><mn>4</mn><mo>×</mo><mn>4</mn></math></span> Bethe-Salpeter equation. For <span><math><mi>J</mi><mo>/</mo><mi>ψ</mi><mo>+</mo><mi>J</mi><mo>/</mo><mi>ψ</mi></math></span> production, the dominant contribution is through fragmentation process, while for <span><math><msub><mrow><mi>η</mi></mrow><mrow><mi>c</mi></mrow></msub><mo>+</mo><msub><mrow><mi>η</mi></mrow><mrow><mi>c</mi></mrow></msub></math></span> production, the quark rearrangement diagrams contribute. Our results of cross section for <span><math><mi>J</mi><mo>/</mo><mi>ψ</mi><mo>+</mo><mi>J</mi><mo>/</mo><mi>ψ</mi></math></span> and <span><math><mi>ψ</mi><mo>(</mo><mn>2</mn><mi>S</mi><mo>)</mo><mo>+</mo><mi>ψ</mi><mo>(</mo><mn>2</mn><mi>S</mi><mo>)</mo></math></span> are compatible with the experimental upper limits set by Belle Collaboration, while in the absence of experimental data for <span><math><msub><mrow><mi>η</mi></mrow><mrow><mi>c</mi></mrow></msub><mo>(</mo><mn>1</mn><mi>S</mi><mo>)</mo><mo>+</mo><msub><mrow><mi>η</mi></mrow><mrow><mi>c</mi></mrow></msub><mo>(</mo><mn>1</mn><mi>S</mi><mo>)</mo></math></span>, and <span><math><msub><mrow><mi>η</mi></mrow><mrow><mi>c</mi></mrow></msub><mo>(</mo><mn>2</mn><mi>S</mi><mo>)</mo><mo>+</mo><msub><mrow><mi>η</mi></mrow><mrow><mi>c</mi></mrow></msub><mo>(</mo><mn>2</mn><mi>S</mi><mo>)</mo></math></span> production, we have given theoretical prediction of their cross sections, and compared with NRQCD prediction.</div></div>","PeriodicalId":19246,"journal":{"name":"Nuclear Physics A","volume":"1053 ","pages":"Article 122969"},"PeriodicalIF":1.7000,"publicationDate":"2024-10-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"(J/ψ,J/ψ), and (ηc,ηc) production through two intermediate photons in electron-positron annihilation at B-factories\",\"authors\":\"Shashank Bhatnagar , Hluf Negash\",\"doi\":\"10.1016/j.nuclphysa.2024.122969\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>We study the processes, <span><math><msup><mrow><mi>e</mi></mrow><mrow><mo>−</mo></mrow></msup><msup><mrow><mi>e</mi></mrow><mrow><mo>+</mo></mrow></msup><mo>→</mo><msup><mrow><mi>γ</mi></mrow><mrow><mo>⁎</mo></mrow></msup><msup><mrow><mi>γ</mi></mrow><mrow><mo>⁎</mo></mrow></msup><mo>→</mo><mi>J</mi><mo>/</mo><mi>ψ</mi><mo>+</mo><mi>J</mi><mo>/</mo><mi>ψ</mi></math></span>, and <span><math><msup><mrow><mi>e</mi></mrow><mrow><mo>−</mo></mrow></msup><msup><mrow><mi>e</mi></mrow><mrow><mo>+</mo></mrow></msup><mo>→</mo><msup><mrow><mi>γ</mi></mrow><mrow><mo>⁎</mo></mrow></msup><msup><mrow><mi>γ</mi></mrow><mrow><mo>⁎</mo></mrow></msup><mo>→</mo><msub><mrow><mi>η</mi></mrow><mrow><mi>c</mi></mrow></msub><mo>+</mo><msub><mrow><mi>η</mi></mrow><mrow><mi>c</mi></mrow></msub></math></span> at <span><math><msqrt><mrow><mi>s</mi></mrow></msqrt><mo>=</mo><mn>10.6</mn></math></span> GeV in the framework of <span><math><mn>4</mn><mo>×</mo><mn>4</mn></math></span> Bethe-Salpeter equation. For <span><math><mi>J</mi><mo>/</mo><mi>ψ</mi><mo>+</mo><mi>J</mi><mo>/</mo><mi>ψ</mi></math></span> production, the dominant contribution is through fragmentation process, while for <span><math><msub><mrow><mi>η</mi></mrow><mrow><mi>c</mi></mrow></msub><mo>+</mo><msub><mrow><mi>η</mi></mrow><mrow><mi>c</mi></mrow></msub></math></span> production, the quark rearrangement diagrams contribute. Our results of cross section for <span><math><mi>J</mi><mo>/</mo><mi>ψ</mi><mo>+</mo><mi>J</mi><mo>/</mo><mi>ψ</mi></math></span> and <span><math><mi>ψ</mi><mo>(</mo><mn>2</mn><mi>S</mi><mo>)</mo><mo>+</mo><mi>ψ</mi><mo>(</mo><mn>2</mn><mi>S</mi><mo>)</mo></math></span> are compatible with the experimental upper limits set by Belle Collaboration, while in the absence of experimental data for <span><math><msub><mrow><mi>η</mi></mrow><mrow><mi>c</mi></mrow></msub><mo>(</mo><mn>1</mn><mi>S</mi><mo>)</mo><mo>+</mo><msub><mrow><mi>η</mi></mrow><mrow><mi>c</mi></mrow></msub><mo>(</mo><mn>1</mn><mi>S</mi><mo>)</mo></math></span>, and <span><math><msub><mrow><mi>η</mi></mrow><mrow><mi>c</mi></mrow></msub><mo>(</mo><mn>2</mn><mi>S</mi><mo>)</mo><mo>+</mo><msub><mrow><mi>η</mi></mrow><mrow><mi>c</mi></mrow></msub><mo>(</mo><mn>2</mn><mi>S</mi><mo>)</mo></math></span> production, we have given theoretical prediction of their cross sections, and compared with NRQCD prediction.</div></div>\",\"PeriodicalId\":19246,\"journal\":{\"name\":\"Nuclear Physics A\",\"volume\":\"1053 \",\"pages\":\"Article 122969\"},\"PeriodicalIF\":1.7000,\"publicationDate\":\"2024-10-15\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Nuclear Physics A\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0375947424001519\",\"RegionNum\":4,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"PHYSICS, NUCLEAR\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Nuclear Physics A","FirstCategoryId":"101","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0375947424001519","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"PHYSICS, NUCLEAR","Score":null,"Total":0}
(J/ψ,J/ψ), and (ηc,ηc) production through two intermediate photons in electron-positron annihilation at B-factories
We study the processes, , and at GeV in the framework of Bethe-Salpeter equation. For production, the dominant contribution is through fragmentation process, while for production, the quark rearrangement diagrams contribute. Our results of cross section for and are compatible with the experimental upper limits set by Belle Collaboration, while in the absence of experimental data for , and production, we have given theoretical prediction of their cross sections, and compared with NRQCD prediction.
期刊介绍:
Nuclear Physics A focuses on the domain of nuclear and hadronic physics and includes the following subsections: Nuclear Structure and Dynamics; Intermediate and High Energy Heavy Ion Physics; Hadronic Physics; Electromagnetic and Weak Interactions; Nuclear Astrophysics. The emphasis is on original research papers. A number of carefully selected and reviewed conference proceedings are published as an integral part of the journal.