Full-heavy tetraquarks in constituent quark models
The full-heavy tetraquarks b b b ¯ b ¯ and c c c ¯ c ¯ are systematically investigated within the chiral quark model and the quark delocalization color screening model. Two structures, meson–meson and diquark–antidiquark, are considered. For the full-beauty b b b ¯ b ¯ systems, there is no any bound...
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| creator | Jin, Xin Xue, Yaoyao Huang, Hongxia Ping, Jialun |
| description | The full-heavy tetraquarks
b
b
b
¯
b
¯
and
c
c
c
¯
c
¯
are systematically investigated within the chiral quark model and the quark delocalization color screening model. Two structures, meson–meson and diquark–antidiquark, are considered. For the full-beauty
b
b
b
¯
b
¯
systems, there is no any bound state or resonance state in two structures in the chiral quark model, while the wide resonances with masses around
19.1
-
19.4
GeV and the quantum numbers
J
P
=
0
+
,
1
+
, and
2
+
are possible in the quark delocalization color screening model. For the full-charm
c
c
c
¯
c
¯
systems, the results are qualitative consistent in two quark models. No bound state can be found in the meson–meson configuration, while in the diquark–antidiquark configuration there may exist the resonance states, with masses range between 6.2 to 7.4 GeV, and the quantum numbers
J
P
=
0
+
,
1
+
, and
2
+
. And the separation between the diquark and the antidiquark indicates that these states may be the compact resonance states. The reported state
X
(6900) is possible to be explained as a compact resonance state with
I
J
P
=
00
+
in present calculation. All these full-charm resonance states are worth searching in the experiments further. |
| doi_str_mv | 10.1140/epjc/s10052-020-08650-z |
| format | Article |
| fullrecord | <record><control><sourceid>gale_proqu</sourceid><recordid>TN_cdi_proquest_journals_2473360092</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><galeid>A650507086</galeid><sourcerecordid>A650507086</sourcerecordid><originalsourceid>FETCH-LOGICAL-c522t-ce020b448d374a09ec27bb70b550ab99279094eb5aa85db138d5d3cb047ec8623</originalsourceid><addsrcrecordid>eNqFkN1LwzAUxYsoOKd_gwWffMh2myZN-ziGH4OB4MdzSNPb2dm1W5KK219vtoqyJ8lDwuGc3Ht-QXAdwSiKGIxxvdRjGwFwSoACgTThQHYnwSBiMSOJ109_34ydBxfWLgGAMkgHAb3v6pq8o_rchg6dUZtOmQ8bVk2o28a6ynXYuPCghqu2wNpeBmelqi1e_dzD4O3-7nX6SOZPD7PpZE40p9QRjX6bnLG0iAVTkKGmIs8F5JyDyrOMigwyhjlXKuVFHsVpwYtY58AE6jSh8TC46f9dm3bToXVy2Xam8SMlZSKOE4Bs7xr1roWqUVZN2foS2p8CV5WvgGXl9YlnwkF4Nj5wexTwHodfbqE6a-Xs5fnYK3qvNq21Bku5NtVKma2MQO7pyz192dOXvq880Jc7n0z7pPWJZoHmb_n_ot8WW4ot</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>2473360092</pqid></control><display><type>article</type><title>Full-heavy tetraquarks in constituent quark models</title><source>Springer Nature - Complete Springer Journals</source><source>DOAJ Directory of Open Access Journals</source><source>Elektronische Zeitschriftenbibliothek - Frei zugängliche E-Journals</source><source>Springer Nature OA Free Journals</source><creator>Jin, Xin ; Xue, Yaoyao ; Huang, Hongxia ; Ping, Jialun</creator><creatorcontrib>Jin, Xin ; Xue, Yaoyao ; Huang, Hongxia ; Ping, Jialun</creatorcontrib><description>The full-heavy tetraquarks
b
b
b
¯
b
¯
and
c
c
c
¯
c
¯
are systematically investigated within the chiral quark model and the quark delocalization color screening model. Two structures, meson–meson and diquark–antidiquark, are considered. For the full-beauty
b
b
b
¯
b
¯
systems, there is no any bound state or resonance state in two structures in the chiral quark model, while the wide resonances with masses around
19.1
-
19.4
GeV and the quantum numbers
J
P
=
0
+
,
1
+
, and
2
+
are possible in the quark delocalization color screening model. For the full-charm
c
c
c
¯
c
¯
systems, the results are qualitative consistent in two quark models. No bound state can be found in the meson–meson configuration, while in the diquark–antidiquark configuration there may exist the resonance states, with masses range between 6.2 to 7.4 GeV, and the quantum numbers
J
P
=
0
+
,
1
+
, and
2
+
. And the separation between the diquark and the antidiquark indicates that these states may be the compact resonance states. The reported state
X
(6900) is possible to be explained as a compact resonance state with
I
J
P
=
00
+
in present calculation. All these full-charm resonance states are worth searching in the experiments further.</description><identifier>ISSN: 1434-6044</identifier><identifier>EISSN: 1434-6052</identifier><identifier>DOI: 10.1140/epjc/s10052-020-08650-z</identifier><language>eng</language><publisher>Berlin/Heidelberg: Springer Berlin Heidelberg</publisher><subject>Analysis ; Astronomy ; Astrophysics and Cosmology ; Charm (particle physics) ; Color ; Configurations ; Elementary Particles ; Hadrons ; Heavy Ions ; Measurement Science and Instrumentation ; Nuclear Energy ; Nuclear Physics ; Physics ; Physics and Astronomy ; Quantum Field Theories ; Quantum Field Theory ; Quantum numbers ; Quark models ; Quarks ; Regular Article – Theoretical Physics ; Resonance ; Screening ; String Theory</subject><ispartof>The European physical journal. C, Particles and fields, 2020-11, Vol.80 (11), Article 1083</ispartof><rights>The Author(s) 2020</rights><rights>COPYRIGHT 2020 Springer</rights><rights>The Author(s) 2020. This work is published under http://creativecommons.org/licenses/by/4.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c522t-ce020b448d374a09ec27bb70b550ab99279094eb5aa85db138d5d3cb047ec8623</citedby><cites>FETCH-LOGICAL-c522t-ce020b448d374a09ec27bb70b550ab99279094eb5aa85db138d5d3cb047ec8623</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1140/epjc/s10052-020-08650-z$$EPDF$$P50$$Gspringer$$Hfree_for_read</linktopdf><linktohtml>$$Uhttps://link.springer.com/10.1140/epjc/s10052-020-08650-z$$EHTML$$P50$$Gspringer$$Hfree_for_read</linktohtml><link.rule.ids>314,776,780,860,27901,27902,41096,41464,42165,42533,51294,51551</link.rule.ids></links><search><creatorcontrib>Jin, Xin</creatorcontrib><creatorcontrib>Xue, Yaoyao</creatorcontrib><creatorcontrib>Huang, Hongxia</creatorcontrib><creatorcontrib>Ping, Jialun</creatorcontrib><title>Full-heavy tetraquarks in constituent quark models</title><title>The European physical journal. C, Particles and fields</title><addtitle>Eur. Phys. J. C</addtitle><description>The full-heavy tetraquarks
b
b
b
¯
b
¯
and
c
c
c
¯
c
¯
are systematically investigated within the chiral quark model and the quark delocalization color screening model. Two structures, meson–meson and diquark–antidiquark, are considered. For the full-beauty
b
b
b
¯
b
¯
systems, there is no any bound state or resonance state in two structures in the chiral quark model, while the wide resonances with masses around
19.1
-
19.4
GeV and the quantum numbers
J
P
=
0
+
,
1
+
, and
2
+
are possible in the quark delocalization color screening model. For the full-charm
c
c
c
¯
c
¯
systems, the results are qualitative consistent in two quark models. No bound state can be found in the meson–meson configuration, while in the diquark–antidiquark configuration there may exist the resonance states, with masses range between 6.2 to 7.4 GeV, and the quantum numbers
J
P
=
0
+
,
1
+
, and
2
+
. And the separation between the diquark and the antidiquark indicates that these states may be the compact resonance states. The reported state
X
(6900) is possible to be explained as a compact resonance state with
I
J
P
=
00
+
in present calculation. All these full-charm resonance states are worth searching in the experiments further.</description><subject>Analysis</subject><subject>Astronomy</subject><subject>Astrophysics and Cosmology</subject><subject>Charm (particle physics)</subject><subject>Color</subject><subject>Configurations</subject><subject>Elementary Particles</subject><subject>Hadrons</subject><subject>Heavy Ions</subject><subject>Measurement Science and Instrumentation</subject><subject>Nuclear Energy</subject><subject>Nuclear Physics</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Quantum Field Theories</subject><subject>Quantum Field Theory</subject><subject>Quantum numbers</subject><subject>Quark models</subject><subject>Quarks</subject><subject>Regular Article – Theoretical Physics</subject><subject>Resonance</subject><subject>Screening</subject><subject>String Theory</subject><issn>1434-6044</issn><issn>1434-6052</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2020</creationdate><recordtype>article</recordtype><sourceid>C6C</sourceid><sourceid>BENPR</sourceid><recordid>eNqFkN1LwzAUxYsoOKd_gwWffMh2myZN-ziGH4OB4MdzSNPb2dm1W5KK219vtoqyJ8lDwuGc3Ht-QXAdwSiKGIxxvdRjGwFwSoACgTThQHYnwSBiMSOJ109_34ydBxfWLgGAMkgHAb3v6pq8o_rchg6dUZtOmQ8bVk2o28a6ynXYuPCghqu2wNpeBmelqi1e_dzD4O3-7nX6SOZPD7PpZE40p9QRjX6bnLG0iAVTkKGmIs8F5JyDyrOMigwyhjlXKuVFHsVpwYtY58AE6jSh8TC46f9dm3bToXVy2Xam8SMlZSKOE4Bs7xr1roWqUVZN2foS2p8CV5WvgGXl9YlnwkF4Nj5wexTwHodfbqE6a-Xs5fnYK3qvNq21Bku5NtVKma2MQO7pyz192dOXvq880Jc7n0z7pPWJZoHmb_n_ot8WW4ot</recordid><startdate>20201101</startdate><enddate>20201101</enddate><creator>Jin, Xin</creator><creator>Xue, Yaoyao</creator><creator>Huang, Hongxia</creator><creator>Ping, Jialun</creator><general>Springer Berlin Heidelberg</general><general>Springer</general><general>Springer Nature B.V</general><scope>C6C</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>ISR</scope><scope>7U5</scope><scope>8FD</scope><scope>8FE</scope><scope>8FG</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>ARAPS</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>H8D</scope><scope>HCIFZ</scope><scope>L7M</scope><scope>P5Z</scope><scope>P62</scope><scope>PHGZM</scope><scope>PHGZT</scope><scope>PIMPY</scope><scope>PKEHL</scope><scope>PQEST</scope><scope>PQGLB</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope></search><sort><creationdate>20201101</creationdate><title>Full-heavy tetraquarks in constituent quark models</title><author>Jin, Xin ; Xue, Yaoyao ; Huang, Hongxia ; Ping, Jialun</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c522t-ce020b448d374a09ec27bb70b550ab99279094eb5aa85db138d5d3cb047ec8623</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2020</creationdate><topic>Analysis</topic><topic>Astronomy</topic><topic>Astrophysics and Cosmology</topic><topic>Charm (particle physics)</topic><topic>Color</topic><topic>Configurations</topic><topic>Elementary Particles</topic><topic>Hadrons</topic><topic>Heavy Ions</topic><topic>Measurement Science and Instrumentation</topic><topic>Nuclear Energy</topic><topic>Nuclear Physics</topic><topic>Physics</topic><topic>Physics and Astronomy</topic><topic>Quantum Field Theories</topic><topic>Quantum Field Theory</topic><topic>Quantum numbers</topic><topic>Quark models</topic><topic>Quarks</topic><topic>Regular Article – Theoretical Physics</topic><topic>Resonance</topic><topic>Screening</topic><topic>String Theory</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Jin, Xin</creatorcontrib><creatorcontrib>Xue, Yaoyao</creatorcontrib><creatorcontrib>Huang, Hongxia</creatorcontrib><creatorcontrib>Ping, Jialun</creatorcontrib><collection>Springer Nature OA Free Journals</collection><collection>CrossRef</collection><collection>Gale In Context: Science</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest Central UK/Ireland</collection><collection>Advanced Technologies & Aerospace Collection</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection (ProQuest)</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>Aerospace Database</collection><collection>SciTech Premium Collection</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Advanced Technologies & Aerospace Database</collection><collection>ProQuest Advanced Technologies & Aerospace Collection</collection><collection>ProQuest Central (New)</collection><collection>ProQuest One Academic (New)</collection><collection>Publicly Available Content Database</collection><collection>ProQuest One Academic Middle East (New)</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Applied & Life Sciences</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><jtitle>The European physical journal. C, Particles and fields</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Jin, Xin</au><au>Xue, Yaoyao</au><au>Huang, Hongxia</au><au>Ping, Jialun</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Full-heavy tetraquarks in constituent quark models</atitle><jtitle>The European physical journal. C, Particles and fields</jtitle><stitle>Eur. Phys. J. C</stitle><date>2020-11-01</date><risdate>2020</risdate><volume>80</volume><issue>11</issue><artnum>1083</artnum><issn>1434-6044</issn><eissn>1434-6052</eissn><abstract>The full-heavy tetraquarks
b
b
b
¯
b
¯
and
c
c
c
¯
c
¯
are systematically investigated within the chiral quark model and the quark delocalization color screening model. Two structures, meson–meson and diquark–antidiquark, are considered. For the full-beauty
b
b
b
¯
b
¯
systems, there is no any bound state or resonance state in two structures in the chiral quark model, while the wide resonances with masses around
19.1
-
19.4
GeV and the quantum numbers
J
P
=
0
+
,
1
+
, and
2
+
are possible in the quark delocalization color screening model. For the full-charm
c
c
c
¯
c
¯
systems, the results are qualitative consistent in two quark models. No bound state can be found in the meson–meson configuration, while in the diquark–antidiquark configuration there may exist the resonance states, with masses range between 6.2 to 7.4 GeV, and the quantum numbers
J
P
=
0
+
,
1
+
, and
2
+
. And the separation between the diquark and the antidiquark indicates that these states may be the compact resonance states. The reported state
X
(6900) is possible to be explained as a compact resonance state with
I
J
P
=
00
+
in present calculation. All these full-charm resonance states are worth searching in the experiments further.</abstract><cop>Berlin/Heidelberg</cop><pub>Springer Berlin Heidelberg</pub><doi>10.1140/epjc/s10052-020-08650-z</doi><oa>free_for_read</oa></addata></record> |
| fulltext | fulltext |
| identifier | ISSN: 1434-6044 |
| ispartof | The European physical journal. C, Particles and fields, 2020-11, Vol.80 (11), Article 1083 |
| issn | 1434-6044 1434-6052 |
| language | eng |
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| source | Springer Nature - Complete Springer Journals; DOAJ Directory of Open Access Journals; Elektronische Zeitschriftenbibliothek - Frei zugängliche E-Journals; Springer Nature OA Free Journals |
| subjects | Analysis Astronomy Astrophysics and Cosmology Charm (particle physics) Color Configurations Elementary Particles Hadrons Heavy Ions Measurement Science and Instrumentation Nuclear Energy Nuclear Physics Physics Physics and Astronomy Quantum Field Theories Quantum Field Theory Quantum numbers Quark models Quarks Regular Article – Theoretical Physics Resonance Screening String Theory |
| title | Full-heavy tetraquarks in constituent quark models |
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