确定 G(3900) 结构为 P 波 DD¯*/D¯D* 共振

IF 8.1 1区 物理与天体物理 Q1 PHYSICS, MULTIDISCIPLINARY
Zi-Yang Lin, Jun-Zhang Wang, Jian-Bo Cheng, Lu Meng, Shi-Lin Zhu
{"title":"确定 G(3900) 结构为 P 波 DD¯*/D¯D* 共振","authors":"Zi-Yang Lin, Jun-Zhang Wang, Jian-Bo Cheng, Lu Meng, Shi-Lin Zhu","doi":"10.1103/physrevlett.133.241903","DOIUrl":null,"url":null,"abstract":"The BESIII Collaboration recently performed a precise measurement of the e</a:mi>+</a:mo></a:msup>e</a:mi>−</a:mo></a:msup>→</a:mo>D</a:mi>D</a:mi>¯</a:mo></a:mover></a:math> Born cross sections, and confirmed the <f:math xmlns:f=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><f:mi>G</f:mi><f:mo stretchy=\"false\">(</f:mo><f:mn>3900</f:mn><f:mo stretchy=\"false\">)</f:mo></f:math> structure reported by and Belle with high significance. We identify the <j:math xmlns:j=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><j:mi>G</j:mi><j:mo stretchy=\"false\">(</j:mo><j:mn>3900</j:mn><j:mo stretchy=\"false\">)</j:mo></j:math> as the first <n:math xmlns:n=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><n:mi>P</n:mi></n:math>-wave <p:math xmlns:p=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><p:mi>D</p:mi><p:msup><p:mover accent=\"true\"><p:mi>D</p:mi><p:mo stretchy=\"false\">¯</p:mo></p:mover><p:mo>*</p:mo></p:msup><p:mo>/</p:mo><p:mover accent=\"true\"><p:mi>D</p:mi><p:mo stretchy=\"false\">¯</p:mo></p:mover><p:msup><p:mi>D</p:mi><p:mo>*</p:mo></p:msup></p:math> molecular resonance. The experimental and theoretical identification of the <v:math xmlns:v=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><v:mi>P</v:mi></v:math>-wave dimeson state holds paramount importance in enhancing our comprehension of the nonperturbative QCD and few-body physics. Its existence is firmly established in a unified meson-exchange model that simultaneously depicts the features of the <x:math xmlns:x=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><x:msub><x:mi>χ</x:mi><x:mrow><x:mi>c</x:mi><x:mn>1</x:mn></x:mrow></x:msub><x:mo stretchy=\"false\">(</x:mo><x:mn>3872</x:mn><x:mo stretchy=\"false\">)</x:mo></x:math>, <bb:math xmlns:bb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><bb:msub><bb:mi>Z</bb:mi><bb:mi>c</bb:mi></bb:msub><bb:mo stretchy=\"false\">(</bb:mo><bb:mn>3900</bb:mn><bb:mo stretchy=\"false\">)</bb:mo></bb:math>, and <fb:math xmlns:fb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><fb:msub><fb:mi>T</fb:mi><fb:mrow><fb:mi>c</fb:mi><fb:mi>c</fb:mi></fb:mrow></fb:msub><fb:mo stretchy=\"false\">(</fb:mo><fb:mn>3875</fb:mn><fb:mo stretchy=\"false\">)</fb:mo></fb:math>. This scenario can be directly examined in the <jb:math xmlns:jb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><jb:msup><jb:mi>e</jb:mi><jb:mo>+</jb:mo></jb:msup><jb:msup><jb:mi>e</jb:mi><jb:mo>−</jb:mo></jb:msup><jb:mo stretchy=\"false\">→</jb:mo><jb:mi>D</jb:mi><jb:msup><jb:mover accent=\"true\"><jb:mi>D</jb:mi><jb:mo stretchy=\"false\">¯</jb:mo></jb:mover><jb:mo>*</jb:mo></jb:msup><jb:mo>/</jb:mo><jb:mover accent=\"true\"><jb:mi>D</jb:mi><jb:mo stretchy=\"false\">¯</jb:mo></jb:mover><jb:msup><jb:mi>D</jb:mi><jb:mo>*</jb:mo></jb:msup></jb:math> cross section by seeing whether a resonance exists at the threshold. The credibility of the investigations is also ensured by the fact that the <qb:math xmlns:qb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><qb:mi>P</qb:mi></qb:math>-wave interaction dominantly arises from the well-known long-range pion exchange. Additionally, thanks to the centrifugal barrier, it is easier to form resonances in <sb:math xmlns:sb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><sb:mi>P</sb:mi></sb:math>-wave than in <ub:math xmlns:ub=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ub:mi>S</ub:mi></ub:math>-wave. We extensively calculate all systems up to <wb:math xmlns:wb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><wb:mi>P</wb:mi></wb:math>-wave with various quantum numbers and predict a dense population of the <yb:math xmlns:yb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><yb:mi>D</yb:mi><yb:msup><yb:mover accent=\"true\"><yb:mi>D</yb:mi><yb:mo stretchy=\"false\">¯</yb:mo></yb:mover><yb:mo>*</yb:mo></yb:msup><yb:mo>/</yb:mo><yb:mover accent=\"true\"><yb:mi>D</yb:mi><yb:mo stretchy=\"false\">¯</yb:mo></yb:mover><yb:msup><yb:mi>D</yb:mi><yb:mo>*</yb:mo></yb:msup></yb:math> and <ec:math xmlns:ec=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ec:mi>D</ec:mi><ec:msup><ec:mi>D</ec:mi><ec:mo>*</ec:mo></ec:msup></ec:math> states, where the <gc:math xmlns:gc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><gc:mi>S</gc:mi></gc:math>-wave <ic:math xmlns:ic=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ic:mi>D</ic:mi><ic:msup><ic:mover accent=\"true\"><ic:mi>D</ic:mi><ic:mo stretchy=\"false\">¯</ic:mo></ic:mover><ic:mo>*</ic:mo></ic:msup><ic:mo>/</ic:mo><ic:mover accent=\"true\"><ic:mi>D</ic:mi><ic:mo stretchy=\"false\">¯</ic:mo></ic:mover><ic:msup><ic:mi>D</ic:mi><ic:mo>*</ic:mo></ic:msup></ic:math> state with <oc:math xmlns:oc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><oc:msup><oc:mi>I</oc:mi><oc:mi>G</oc:mi></oc:msup><oc:mo stretchy=\"false\">(</oc:mo><oc:msup><oc:mi>J</oc:mi><oc:mrow><oc:mi>P</oc:mi><oc:mi>C</oc:mi></oc:mrow></oc:msup><oc:mo stretchy=\"false\">)</oc:mo><oc:mo>=</oc:mo><oc:msup><oc:mn>0</oc:mn><oc:mo>−</oc:mo></oc:msup><oc:mo stretchy=\"false\">(</oc:mo><oc:msup><oc:mn>1</oc:mn><oc:mrow><oc:mo>+</oc:mo><oc:mo>−</oc:mo></oc:mrow></oc:msup><oc:mo stretchy=\"false\">)</oc:mo></oc:math>, <uc:math xmlns:uc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><uc:mi>P</uc:mi></uc:math>-wave <wc:math xmlns:wc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><wc:mi>D</wc:mi><wc:msup><wc:mover accent=\"true\"><wc:mi>D</wc:mi><wc:mo stretchy=\"false\">¯</wc:mo></wc:mover><wc:mo>*</wc:mo></wc:msup><wc:mo>/</wc:mo><wc:mover accent=\"true\"><wc:mi>D</wc:mi><wc:mo stretchy=\"false\">¯</wc:mo></wc:mover><wc:msup><wc:mi>D</wc:mi><wc:mo>*</wc:mo></wc:msup></wc:math> state with <cd:math xmlns:cd=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><cd:msup><cd:mi>I</cd:mi><cd:mi>G</cd:mi></cd:msup><cd:mo stretchy=\"false\">(</cd:mo><cd:msup><cd:mi>J</cd:mi><cd:mrow><cd:mi>P</cd:mi><cd:mi>C</cd:mi></cd:mrow></cd:msup><cd:mo stretchy=\"false\">)</cd:mo><cd:mo>=</cd:mo><cd:msup><cd:mn>0</cd:mn><cd:mo>+</cd:mo></cd:msup><cd:mo stretchy=\"false\">(</cd:mo><cd:msup><cd:mn>0</cd:mn><cd:mrow><cd:mo>−</cd:mo><cd:mo>+</cd:mo></cd:mrow></cd:msup><cd:mo stretchy=\"false\">)</cd:mo></cd:math>, and <id:math xmlns: display=\"inline\"><id:mi>P</id:mi></id:math>-wave <kd:math xmlns:kd=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><kd:mi>D</kd:mi><kd:msup><kd:mi>D</kd:mi><kd:mo>*</kd:mo></kd:msup></kd:math> state with <md:math xmlns:md=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><md:mi>I</md:mi><md:mo stretchy=\"false\">(</md:mo><md:msup><md:mi>J</md:mi><md:mi>P</md:mi></md:msup><md:mo stretchy=\"false\">)</md:mo><md:mo>=</md:mo><md:mn>0</md:mn><md:mo stretchy=\"false\">(</md:mo><md:msup><md:mn>0</md:mn><md:mo>−</md:mo></md:msup><md:mo stretchy=\"false\">)</md:mo></md:math> are more likely to be observed in experiments. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2024</jats:copyright-year> </jats:permissions> </jats:supplementary-material>","PeriodicalId":20069,"journal":{"name":"Physical review letters","volume":"51 1","pages":""},"PeriodicalIF":8.1000,"publicationDate":"2024-12-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Identification of the G(3900) Structure as the P -Wave DD¯*/D¯D* Resonance\",\"authors\":\"Zi-Yang Lin, Jun-Zhang Wang, Jian-Bo Cheng, Lu Meng, Shi-Lin Zhu\",\"doi\":\"10.1103/physrevlett.133.241903\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The BESIII Collaboration recently performed a precise measurement of the e</a:mi>+</a:mo></a:msup>e</a:mi>−</a:mo></a:msup>→</a:mo>D</a:mi>D</a:mi>¯</a:mo></a:mover></a:math> Born cross sections, and confirmed the <f:math xmlns:f=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><f:mi>G</f:mi><f:mo stretchy=\\\"false\\\">(</f:mo><f:mn>3900</f:mn><f:mo stretchy=\\\"false\\\">)</f:mo></f:math> structure reported by and Belle with high significance. We identify the <j:math xmlns:j=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><j:mi>G</j:mi><j:mo stretchy=\\\"false\\\">(</j:mo><j:mn>3900</j:mn><j:mo stretchy=\\\"false\\\">)</j:mo></j:math> as the first <n:math xmlns:n=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><n:mi>P</n:mi></n:math>-wave <p:math xmlns:p=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><p:mi>D</p:mi><p:msup><p:mover accent=\\\"true\\\"><p:mi>D</p:mi><p:mo stretchy=\\\"false\\\">¯</p:mo></p:mover><p:mo>*</p:mo></p:msup><p:mo>/</p:mo><p:mover accent=\\\"true\\\"><p:mi>D</p:mi><p:mo stretchy=\\\"false\\\">¯</p:mo></p:mover><p:msup><p:mi>D</p:mi><p:mo>*</p:mo></p:msup></p:math> molecular resonance. The experimental and theoretical identification of the <v:math xmlns:v=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><v:mi>P</v:mi></v:math>-wave dimeson state holds paramount importance in enhancing our comprehension of the nonperturbative QCD and few-body physics. Its existence is firmly established in a unified meson-exchange model that simultaneously depicts the features of the <x:math xmlns:x=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><x:msub><x:mi>χ</x:mi><x:mrow><x:mi>c</x:mi><x:mn>1</x:mn></x:mrow></x:msub><x:mo stretchy=\\\"false\\\">(</x:mo><x:mn>3872</x:mn><x:mo stretchy=\\\"false\\\">)</x:mo></x:math>, <bb:math xmlns:bb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><bb:msub><bb:mi>Z</bb:mi><bb:mi>c</bb:mi></bb:msub><bb:mo stretchy=\\\"false\\\">(</bb:mo><bb:mn>3900</bb:mn><bb:mo stretchy=\\\"false\\\">)</bb:mo></bb:math>, and <fb:math xmlns:fb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><fb:msub><fb:mi>T</fb:mi><fb:mrow><fb:mi>c</fb:mi><fb:mi>c</fb:mi></fb:mrow></fb:msub><fb:mo stretchy=\\\"false\\\">(</fb:mo><fb:mn>3875</fb:mn><fb:mo stretchy=\\\"false\\\">)</fb:mo></fb:math>. This scenario can be directly examined in the <jb:math xmlns:jb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><jb:msup><jb:mi>e</jb:mi><jb:mo>+</jb:mo></jb:msup><jb:msup><jb:mi>e</jb:mi><jb:mo>−</jb:mo></jb:msup><jb:mo stretchy=\\\"false\\\">→</jb:mo><jb:mi>D</jb:mi><jb:msup><jb:mover accent=\\\"true\\\"><jb:mi>D</jb:mi><jb:mo stretchy=\\\"false\\\">¯</jb:mo></jb:mover><jb:mo>*</jb:mo></jb:msup><jb:mo>/</jb:mo><jb:mover accent=\\\"true\\\"><jb:mi>D</jb:mi><jb:mo stretchy=\\\"false\\\">¯</jb:mo></jb:mover><jb:msup><jb:mi>D</jb:mi><jb:mo>*</jb:mo></jb:msup></jb:math> cross section by seeing whether a resonance exists at the threshold. The credibility of the investigations is also ensured by the fact that the <qb:math xmlns:qb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><qb:mi>P</qb:mi></qb:math>-wave interaction dominantly arises from the well-known long-range pion exchange. Additionally, thanks to the centrifugal barrier, it is easier to form resonances in <sb:math xmlns:sb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><sb:mi>P</sb:mi></sb:math>-wave than in <ub:math xmlns:ub=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><ub:mi>S</ub:mi></ub:math>-wave. We extensively calculate all systems up to <wb:math xmlns:wb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><wb:mi>P</wb:mi></wb:math>-wave with various quantum numbers and predict a dense population of the <yb:math xmlns:yb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><yb:mi>D</yb:mi><yb:msup><yb:mover accent=\\\"true\\\"><yb:mi>D</yb:mi><yb:mo stretchy=\\\"false\\\">¯</yb:mo></yb:mover><yb:mo>*</yb:mo></yb:msup><yb:mo>/</yb:mo><yb:mover accent=\\\"true\\\"><yb:mi>D</yb:mi><yb:mo stretchy=\\\"false\\\">¯</yb:mo></yb:mover><yb:msup><yb:mi>D</yb:mi><yb:mo>*</yb:mo></yb:msup></yb:math> and <ec:math xmlns:ec=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><ec:mi>D</ec:mi><ec:msup><ec:mi>D</ec:mi><ec:mo>*</ec:mo></ec:msup></ec:math> states, where the <gc:math xmlns:gc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><gc:mi>S</gc:mi></gc:math>-wave <ic:math xmlns:ic=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><ic:mi>D</ic:mi><ic:msup><ic:mover accent=\\\"true\\\"><ic:mi>D</ic:mi><ic:mo stretchy=\\\"false\\\">¯</ic:mo></ic:mover><ic:mo>*</ic:mo></ic:msup><ic:mo>/</ic:mo><ic:mover accent=\\\"true\\\"><ic:mi>D</ic:mi><ic:mo stretchy=\\\"false\\\">¯</ic:mo></ic:mover><ic:msup><ic:mi>D</ic:mi><ic:mo>*</ic:mo></ic:msup></ic:math> state with <oc:math xmlns:oc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><oc:msup><oc:mi>I</oc:mi><oc:mi>G</oc:mi></oc:msup><oc:mo stretchy=\\\"false\\\">(</oc:mo><oc:msup><oc:mi>J</oc:mi><oc:mrow><oc:mi>P</oc:mi><oc:mi>C</oc:mi></oc:mrow></oc:msup><oc:mo stretchy=\\\"false\\\">)</oc:mo><oc:mo>=</oc:mo><oc:msup><oc:mn>0</oc:mn><oc:mo>−</oc:mo></oc:msup><oc:mo stretchy=\\\"false\\\">(</oc:mo><oc:msup><oc:mn>1</oc:mn><oc:mrow><oc:mo>+</oc:mo><oc:mo>−</oc:mo></oc:mrow></oc:msup><oc:mo stretchy=\\\"false\\\">)</oc:mo></oc:math>, <uc:math xmlns:uc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><uc:mi>P</uc:mi></uc:math>-wave <wc:math xmlns:wc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><wc:mi>D</wc:mi><wc:msup><wc:mover accent=\\\"true\\\"><wc:mi>D</wc:mi><wc:mo stretchy=\\\"false\\\">¯</wc:mo></wc:mover><wc:mo>*</wc:mo></wc:msup><wc:mo>/</wc:mo><wc:mover accent=\\\"true\\\"><wc:mi>D</wc:mi><wc:mo stretchy=\\\"false\\\">¯</wc:mo></wc:mover><wc:msup><wc:mi>D</wc:mi><wc:mo>*</wc:mo></wc:msup></wc:math> state with <cd:math xmlns:cd=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><cd:msup><cd:mi>I</cd:mi><cd:mi>G</cd:mi></cd:msup><cd:mo stretchy=\\\"false\\\">(</cd:mo><cd:msup><cd:mi>J</cd:mi><cd:mrow><cd:mi>P</cd:mi><cd:mi>C</cd:mi></cd:mrow></cd:msup><cd:mo stretchy=\\\"false\\\">)</cd:mo><cd:mo>=</cd:mo><cd:msup><cd:mn>0</cd:mn><cd:mo>+</cd:mo></cd:msup><cd:mo stretchy=\\\"false\\\">(</cd:mo><cd:msup><cd:mn>0</cd:mn><cd:mrow><cd:mo>−</cd:mo><cd:mo>+</cd:mo></cd:mrow></cd:msup><cd:mo stretchy=\\\"false\\\">)</cd:mo></cd:math>, and <id:math xmlns: display=\\\"inline\\\"><id:mi>P</id:mi></id:math>-wave <kd:math xmlns:kd=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><kd:mi>D</kd:mi><kd:msup><kd:mi>D</kd:mi><kd:mo>*</kd:mo></kd:msup></kd:math> state with <md:math xmlns:md=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><md:mi>I</md:mi><md:mo stretchy=\\\"false\\\">(</md:mo><md:msup><md:mi>J</md:mi><md:mi>P</md:mi></md:msup><md:mo stretchy=\\\"false\\\">)</md:mo><md:mo>=</md:mo><md:mn>0</md:mn><md:mo stretchy=\\\"false\\\">(</md:mo><md:msup><md:mn>0</md:mn><md:mo>−</md:mo></md:msup><md:mo stretchy=\\\"false\\\">)</md:mo></md:math> are more likely to be observed in experiments. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2024</jats:copyright-year> </jats:permissions> </jats:supplementary-material>\",\"PeriodicalId\":20069,\"journal\":{\"name\":\"Physical review letters\",\"volume\":\"51 1\",\"pages\":\"\"},\"PeriodicalIF\":8.1000,\"publicationDate\":\"2024-12-13\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Physical review letters\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.1103/physrevlett.133.241903\",\"RegionNum\":1,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"PHYSICS, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physical review letters","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1103/physrevlett.133.241903","RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"PHYSICS, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0

摘要

本文章由计算机程序翻译,如有差异,请以英文原文为准。
Identification of the G(3900) Structure as the P -Wave DD¯*/D¯D* Resonance
The BESIII Collaboration recently performed a precise measurement of the e+e−→DD¯ Born cross sections, and confirmed the G(3900) structure reported by and Belle with high significance. We identify the G(3900) as the first P-wave DD¯*/D¯D* molecular resonance. The experimental and theoretical identification of the P-wave dimeson state holds paramount importance in enhancing our comprehension of the nonperturbative QCD and few-body physics. Its existence is firmly established in a unified meson-exchange model that simultaneously depicts the features of the χc1(3872), Zc(3900), and Tcc(3875). This scenario can be directly examined in the e+eDD¯*/D¯D* cross section by seeing whether a resonance exists at the threshold. The credibility of the investigations is also ensured by the fact that the P-wave interaction dominantly arises from the well-known long-range pion exchange. Additionally, thanks to the centrifugal barrier, it is easier to form resonances in P-wave than in S-wave. We extensively calculate all systems up to P-wave with various quantum numbers and predict a dense population of the DD¯*/D¯D* and DD* states, where the S-wave DD¯*/D¯D* state with IG(JPC)=0(1+), P-wave DD¯*/D¯D* state with IG(JPC)=0+(0+), and P-wave DD* state with I(JP)=0(0) are more likely to be observed in experiments. Published by the American Physical Society 2024
求助全文
通过发布文献求助,成功后即可免费获取论文全文。 去求助
来源期刊
Physical review letters
Physical review letters 物理-物理:综合
CiteScore
16.50
自引率
7.00%
发文量
2673
审稿时长
2.2 months
期刊介绍: Physical review letters(PRL)covers the full range of applied, fundamental, and interdisciplinary physics research topics: General physics, including statistical and quantum mechanics and quantum information Gravitation, astrophysics, and cosmology Elementary particles and fields Nuclear physics Atomic, molecular, and optical physics Nonlinear dynamics, fluid dynamics, and classical optics Plasma and beam physics Condensed matter and materials physics Polymers, soft matter, biological, climate and interdisciplinary physics, including networks
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术官方微信