用QCD求和规则寻找魅力重子和二重子结构

IF 1.5 4区 物理与天体物理 Q3 PHYSICS, PARTICLES & FIELDS
Xiu-Wu Wang, Zhi-Gang wang
{"title":"用QCD求和规则寻找魅力重子和二重子结构","authors":"Xiu-Wu Wang, Zhi-Gang wang","doi":"10.1155/2022/6224597","DOIUrl":null,"url":null,"abstract":"<jats:p>In the present work, we construct eight six-quark currents to study the <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M1\">\n <msub>\n <mrow>\n <mi>Σ</mi>\n </mrow>\n <mrow>\n <mi>c</mi>\n </mrow>\n </msub>\n <msub>\n <mrow>\n <mover accent=\"true\">\n <mi>Σ</mi>\n <mo stretchy=\"true\">¯</mo>\n </mover>\n </mrow>\n <mrow>\n <mi>c</mi>\n </mrow>\n </msub>\n </math>\n </jats:inline-formula> baryonium and <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M2\">\n <msub>\n <mrow>\n <mi>Σ</mi>\n </mrow>\n <mrow>\n <mi>c</mi>\n </mrow>\n </msub>\n <msub>\n <mrow>\n <mi>Σ</mi>\n </mrow>\n <mrow>\n <mi>c</mi>\n </mrow>\n </msub>\n </math>\n </jats:inline-formula> dibaryon states via the QCD sum rules. For either <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M3\">\n <msub>\n <mrow>\n <mi>Σ</mi>\n </mrow>\n <mrow>\n <mi>c</mi>\n </mrow>\n </msub>\n <msub>\n <mrow>\n <mover accent=\"true\">\n <mi>Σ</mi>\n <mo stretchy=\"true\">¯</mo>\n </mover>\n </mrow>\n <mrow>\n <mi>c</mi>\n </mrow>\n </msub>\n </math>\n </jats:inline-formula> baryonium or <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M4\">\n <msub>\n <mrow>\n <mi>Σ</mi>\n </mrow>\n <mrow>\n <mi>c</mi>\n </mrow>\n </msub>\n <msub>\n <mrow>\n <mi>Σ</mi>\n </mrow>\n <mrow>\n <mi>c</mi>\n </mrow>\n </msub>\n </math>\n </jats:inline-formula> dibaryon states, we construct four currents with the <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M5\">\n <msup>\n <mrow>\n <mi>J</mi>\n </mrow>\n <mrow>\n <mi>P</mi>\n </mrow>\n </msup>\n <mo>=</mo>\n <msup>\n <mrow>\n <mn>1</mn>\n </mrow>\n <mrow>\n <mo>−</mo>\n </mrow>\n </msup>\n <mo>,</mo>\n <msup>\n <mrow>\n <mn>1</mn>\n </mrow>\n <mrow>\n <mo>+</mo>\n </mrow>\n </msup>\n <mo>,</mo>\n <msup>\n <mrow>\n <mn>0</mn>\n </mrow>\n <mrow>\n <mo>+</mo>\n </mrow>\n </msup>\n </math>\n </jats:inline-formula> and <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M6\">\n <msup>\n <mrow>\n <mn>0</mn>\n </mrow>\n <mrow>\n <mo>−</mo>\n </mrow>\n </msup>\n </math>\n </jats:inline-formula>. Except the current <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M7\">\n <msup>\n <mrow>\n <mn>1</mn>\n </mrow>\n <mrow>\n <mo>+</mo>\n </mrow>\n </msup>\n </math>\n </jats:inline-formula> of <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M8\">\n <msub>\n <mrow>\n <mi>Σ</mi>\n </mrow>\n <mrow>\n <mi>c</mi>\n </mrow>\n </msub>\n <msub>\n <mrow>\n <mi>Σ</mi>\n </mrow>\n <mrow>\n <mi>c</mi>\n </mrow>\n </msub>\n </math>\n </jats:inline-formula>, we find the Borel windows for the other seven. There are two possible <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M9\">\n <msub>\n <mrow>\n <mi>Σ</mi>\n </mrow>\n <mrow>\n <mi>c</mi>\n </mrow>\n </msub>\n <msub>\n <mrow>\n <mover accent=\"true\">\n <mi>Σ</mi>\n <mo stretchy=\"true\">¯</mo>\n </mover>\n </mrow>\n <mrow>\n <mi>c</mi>\n </mrow>\n </msub>\n </math>\n </jats:inline-formula> molecular states or compact six-quark states with the <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M10\">\n <msup>\n <mrow>\n <mi>J</mi>\n </mrow>\n <mrow>\n <mi>P</mi>\n </mrow>\n </msup>\n <mo>=</mo>\n <msup>\n <mrow>\n <mn>1</mn>\n </mrow>\n <mrow>\n <mo>−</mo>\n </mrow>\n </msup>\n </math>\n </jats:inline-formula> and <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M11\">\n <msup>\n <mrow>\n <mn>0</mn>\n </mrow>\n <mrow>\n <mo>−</mo>\n </mrow>\n </msup>\n </math>\n </jats:inline-formula>. The results of the current <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M12\">\n <msup>\n <mrow>\n <mn>0</mn>\n </mrow>\n <mrow>\n <mo>+</mo>\n </mrow>\n </msup>\n </math>\n </jats:inline-formula> of <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M13\">\n <msub>\n <mrow>\n <mi>Σ</mi>\n </mrow>\n <mrow>\n <mi>c</mi>\n </mrow>\n </msub>\n <msub>\n <mrow>\n <mi>Σ</mi>\n </mrow>\n <mrow>\n <mi>c</mi>\n </mrow>\n </msub>\n </math>\n </jat","PeriodicalId":7498,"journal":{"name":"Advances in High Energy Physics","volume":" ","pages":""},"PeriodicalIF":1.5000,"publicationDate":"2021-10-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"2","resultStr":"{\"title\":\"Search for the Charmed Baryonium and Dibaryon Structures via the QCD Sum Rules\",\"authors\":\"Xiu-Wu Wang, Zhi-Gang wang\",\"doi\":\"10.1155/2022/6224597\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<jats:p>In the present work, we construct eight six-quark currents to study the <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M1\\\">\\n <msub>\\n <mrow>\\n <mi>Σ</mi>\\n </mrow>\\n <mrow>\\n <mi>c</mi>\\n </mrow>\\n </msub>\\n <msub>\\n <mrow>\\n <mover accent=\\\"true\\\">\\n <mi>Σ</mi>\\n <mo stretchy=\\\"true\\\">¯</mo>\\n </mover>\\n </mrow>\\n <mrow>\\n <mi>c</mi>\\n </mrow>\\n </msub>\\n </math>\\n </jats:inline-formula> baryonium and <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M2\\\">\\n <msub>\\n <mrow>\\n <mi>Σ</mi>\\n </mrow>\\n <mrow>\\n <mi>c</mi>\\n </mrow>\\n </msub>\\n <msub>\\n <mrow>\\n <mi>Σ</mi>\\n </mrow>\\n <mrow>\\n <mi>c</mi>\\n </mrow>\\n </msub>\\n </math>\\n </jats:inline-formula> dibaryon states via the QCD sum rules. For either <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M3\\\">\\n <msub>\\n <mrow>\\n <mi>Σ</mi>\\n </mrow>\\n <mrow>\\n <mi>c</mi>\\n </mrow>\\n </msub>\\n <msub>\\n <mrow>\\n <mover accent=\\\"true\\\">\\n <mi>Σ</mi>\\n <mo stretchy=\\\"true\\\">¯</mo>\\n </mover>\\n </mrow>\\n <mrow>\\n <mi>c</mi>\\n </mrow>\\n </msub>\\n </math>\\n </jats:inline-formula> baryonium or <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M4\\\">\\n <msub>\\n <mrow>\\n <mi>Σ</mi>\\n </mrow>\\n <mrow>\\n <mi>c</mi>\\n </mrow>\\n </msub>\\n <msub>\\n <mrow>\\n <mi>Σ</mi>\\n </mrow>\\n <mrow>\\n <mi>c</mi>\\n </mrow>\\n </msub>\\n </math>\\n </jats:inline-formula> dibaryon states, we construct four currents with the <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M5\\\">\\n <msup>\\n <mrow>\\n <mi>J</mi>\\n </mrow>\\n <mrow>\\n <mi>P</mi>\\n </mrow>\\n </msup>\\n <mo>=</mo>\\n <msup>\\n <mrow>\\n <mn>1</mn>\\n </mrow>\\n <mrow>\\n <mo>−</mo>\\n </mrow>\\n </msup>\\n <mo>,</mo>\\n <msup>\\n <mrow>\\n <mn>1</mn>\\n </mrow>\\n <mrow>\\n <mo>+</mo>\\n </mrow>\\n </msup>\\n <mo>,</mo>\\n <msup>\\n <mrow>\\n <mn>0</mn>\\n </mrow>\\n <mrow>\\n <mo>+</mo>\\n </mrow>\\n </msup>\\n </math>\\n </jats:inline-formula> and <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M6\\\">\\n <msup>\\n <mrow>\\n <mn>0</mn>\\n </mrow>\\n <mrow>\\n <mo>−</mo>\\n </mrow>\\n </msup>\\n </math>\\n </jats:inline-formula>. Except the current <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M7\\\">\\n <msup>\\n <mrow>\\n <mn>1</mn>\\n </mrow>\\n <mrow>\\n <mo>+</mo>\\n </mrow>\\n </msup>\\n </math>\\n </jats:inline-formula> of <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M8\\\">\\n <msub>\\n <mrow>\\n <mi>Σ</mi>\\n </mrow>\\n <mrow>\\n <mi>c</mi>\\n </mrow>\\n </msub>\\n <msub>\\n <mrow>\\n <mi>Σ</mi>\\n </mrow>\\n <mrow>\\n <mi>c</mi>\\n </mrow>\\n </msub>\\n </math>\\n </jats:inline-formula>, we find the Borel windows for the other seven. There are two possible <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M9\\\">\\n <msub>\\n <mrow>\\n <mi>Σ</mi>\\n </mrow>\\n <mrow>\\n <mi>c</mi>\\n </mrow>\\n </msub>\\n <msub>\\n <mrow>\\n <mover accent=\\\"true\\\">\\n <mi>Σ</mi>\\n <mo stretchy=\\\"true\\\">¯</mo>\\n </mover>\\n </mrow>\\n <mrow>\\n <mi>c</mi>\\n </mrow>\\n </msub>\\n </math>\\n </jats:inline-formula> molecular states or compact six-quark states with the <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M10\\\">\\n <msup>\\n <mrow>\\n <mi>J</mi>\\n </mrow>\\n <mrow>\\n <mi>P</mi>\\n </mrow>\\n </msup>\\n <mo>=</mo>\\n <msup>\\n <mrow>\\n <mn>1</mn>\\n </mrow>\\n <mrow>\\n <mo>−</mo>\\n </mrow>\\n </msup>\\n </math>\\n </jats:inline-formula> and <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M11\\\">\\n <msup>\\n <mrow>\\n <mn>0</mn>\\n </mrow>\\n <mrow>\\n <mo>−</mo>\\n </mrow>\\n </msup>\\n </math>\\n </jats:inline-formula>. The results of the current <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M12\\\">\\n <msup>\\n <mrow>\\n <mn>0</mn>\\n </mrow>\\n <mrow>\\n <mo>+</mo>\\n </mrow>\\n </msup>\\n </math>\\n </jats:inline-formula> of <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M13\\\">\\n <msub>\\n <mrow>\\n <mi>Σ</mi>\\n </mrow>\\n <mrow>\\n <mi>c</mi>\\n </mrow>\\n </msub>\\n <msub>\\n <mrow>\\n <mi>Σ</mi>\\n </mrow>\\n <mrow>\\n <mi>c</mi>\\n </mrow>\\n </msub>\\n </math>\\n </jat\",\"PeriodicalId\":7498,\"journal\":{\"name\":\"Advances in High Energy Physics\",\"volume\":\" \",\"pages\":\"\"},\"PeriodicalIF\":1.5000,\"publicationDate\":\"2021-10-27\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"2\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Advances in High Energy Physics\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.1155/2022/6224597\",\"RegionNum\":4,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"PHYSICS, PARTICLES & FIELDS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Advances in High Energy Physics","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1155/2022/6224597","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"PHYSICS, PARTICLES & FIELDS","Score":null,"Total":0}
引用次数: 2

摘要

在本工作中,我们构造了八个六夸克流来研究∑c∑c重子和∑通过QCD和的c∑c二核态规则。对于∑c∑?c钡鎓或∑c∑c二核态,我们构造了四个电流,其中J P=1−,1+,0+和0−。除了当前的1+∑c,我们找到了其他七个的Borel窗口。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Search for the Charmed Baryonium and Dibaryon Structures via the QCD Sum Rules
In the present work, we construct eight six-quark currents to study the Σ c Σ ¯ c baryonium and Σ c Σ c dibaryon states via the QCD sum rules. For either Σ c Σ ¯ c baryonium or Σ c Σ c dibaryon states, we construct four currents with the J P = 1 , 1 + , 0 + and 0 . Except the current 1 + of Σ c Σ c , we find the Borel windows for the other seven. There are two possible Σ c Σ ¯ c molecular states or compact six-quark states with the J P = 1 and 0 . The results of the current 0 + of Σ c Σ c
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来源期刊
Advances in High Energy Physics
Advances in High Energy Physics PHYSICS, PARTICLES & FIELDS-
CiteScore
3.40
自引率
5.90%
发文量
55
审稿时长
6-12 weeks
期刊介绍: Advances in High Energy Physics publishes the results of theoretical and experimental research on the nature of, and interaction between, energy and matter. Considering both original research and focussed review articles, the journal welcomes submissions from small research groups and large consortia alike.
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