Study of the structures of four-quark states in terms of the Born-Oppenheimer approximation
In this work, we use the Born-Oppenheimer approximation, where the potential between atoms can be approximated as a function of distance between the two nuclei, to study the four-quark bound states. By this approximation, Heitler and London calculated the spectrum of the hydrogen molecule, which inc...
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| Published in | Chinese physics C Vol. 39; no. 8; pp. 22 - 31 |
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| Main Author | |
| Format | Journal Article |
| Language | English |
| Published |
01.08.2015
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| Subjects | |
| Online Access | Get full text |
| ISSN | 1674-1137 2058-6132 0254-3052 |
| DOI | 10.1088/1674-1137/39/8/083103 |
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| Abstract | In this work, we use the Born-Oppenheimer approximation, where the potential between atoms can be approximated as a function of distance between the two nuclei, to study the four-quark bound states. By this approximation, Heitler and London calculated the spectrum of the hydrogen molecule, which includes two protons (heavy) and two electrons (light). Cenerally, the observed exotic mesons Zb(10610), ZD(10650), Zc(3900) and Zc(4020) (Zc(4025)) may be molecular states made of two physical mesons and/or diquark-anti-diquark structures. Analogous to the Heitler-London method for calculating the mass of the hydrogen molecule, we investigate whether there exist energy minima for these two structures. Contrary to the hydrogen molecule case where only the spin-triplet possesses an energy minimum, there exist minima for both of these states. This implies that both molecule and tetraquark states can be stable objects. Since they have the same quantum numbers, however, the two states may mix to result in the physical states. A consequence would be that partner exotic states co-existing with ZD(10610), Zb(]0650), Zc(3900) and Zc(4020) (Zc(4025)) are predicted and should be experimentally observed. |
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| AbstractList | In this work, we use the Born-Oppenheimer approximation, where the potential between atoms can be approximated as a function of distance between the two nuclei, to study the four-quark bound states. By this approximation, Heitler and London calculated the spectrum of the hydrogen molecule, which includes two protons (heavy) and two electrons (light). Generally, the observed exotic mesons Z sub(b)(10610), Z sub(b)(10650), Z sub(c)(3900) and Z sub(c)(4020) (Z sub(c)(4025)) may be molecular states made of two physical mesons and/or diquark-anti-diquark structures. Analogous to the Heitler-London method for calculating the mass of the hydrogen molecule, we investigate whether there exist energy minima for these two structures. Contrary to the hydrogen molecule case where only the spin-triplet possesses an energy minimum, there exist minima for both of these states. This implies that both molecule and tetraquark states can be stable objects. Since they have the same quantum numbers, however, the two states may mix to result in the physical states. A consequence would be that partner exotic states co-existing with Z sub(b)(10610), Z sub(b)(10650), Z sub(c)(3900) and Z sub(c)(4020) (Z sub(c) (4025)) are predicted and should be experimentally observed. In this work, we use the Born-Oppenheimer approximation, where the potential between atoms can be approximated as a function of distance between the two nuclei, to study the four-quark bound states. By this approximation, Heitler and London calculated the spectrum of the hydrogen molecule, which includes two protons (heavy) and two electrons (light). Cenerally, the observed exotic mesons Zb(10610), ZD(10650), Zc(3900) and Zc(4020) (Zc(4025)) may be molecular states made of two physical mesons and/or diquark-anti-diquark structures. Analogous to the Heitler-London method for calculating the mass of the hydrogen molecule, we investigate whether there exist energy minima for these two structures. Contrary to the hydrogen molecule case where only the spin-triplet possesses an energy minimum, there exist minima for both of these states. This implies that both molecule and tetraquark states can be stable objects. Since they have the same quantum numbers, however, the two states may mix to result in the physical states. A consequence would be that partner exotic states co-existing with ZD(10610), Zb(]0650), Zc(3900) and Zc(4020) (Zc(4025)) are predicted and should be experimentally observed. |
| Author | 刘学文 柯红卫 丁亦兵 李学潜 |
| AuthorAffiliation | School of Physics, Nankai University, Tianjin 300071, China School of Science, Tianjin University, Tianjin 300072, China School of Physics, University of Chinese Academy of Sciences, Beijing 100049, China |
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| CitedBy_id | crossref_primary_10_1016_j_physrep_2016_05_004 crossref_primary_10_1088_1402_4896_acf0f3 crossref_primary_10_1142_S0217732319502201 crossref_primary_10_1103_PhysRevD_94_054009 crossref_primary_10_1142_S0217751X18500963 crossref_primary_10_1103_PhysRevD_93_074013 crossref_primary_10_1007_s00601_023_01791_3 |
| Cites_doi | 10.1103/PhysRevD.85.054011 10.1140/epja/i2014-14131-9 10.1103/PhysRevD.87.074006 10.1007/JHEP04(2012)056 10.1103/PhysRevD.90.014044 10.1103/PhysRevC.73.045214 10.1140/epja/i2011-11120-6 10.1140/epja/i2003-10128-9 10.1140/epjc/s10052-012-1880-x 10.1103/PhysRevD.87.125018 10.1103/PhysRevD.41.2236 10.1007/JHEP07(2014)106 10.1103/PhysRevC.60.045203 10.1103/PhysRevD.17.3090 10.1016/S0375-9474(99)00321-8 10.1103/PhysRevD.26.3280 10.1140/epjc/s2005-02383-9 10.1140/epjc/s10052-013-2635-z 10.1088/0253-6102/43/2/016 10.1103/PhysRevD.84.054002 10.1103/PhysRevD.35.907 10.1103/PhysRevD.38.146 10.1140/epjc/s10052-013-2561-0 10.1103/PhysRevD.71.014028 10.1103/PhysRevD.27.588 10.1103/PhysRevLett.111.242001 10.1007/BF01397394 10.3390/sym1020155 10.1103/PhysRevD.84.054010 10.1103/PhysRevLett.110.252001 10.1002/andp.19273892002 10.1103/PhysRevD.21.203 10.1103/PhysRevD.87.116004 10.1103/PhysRevLett.113.112001 10.1088/0954-3899/31/5/017 10.1103/PhysRevD.27.233 10.1103/PhysRevD.86.117502 10.1088/0954-3899/25/9/304 |
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| Notes | LIU Xue-Wen, KE Hong-Wei,DING Yi-Bing, LI Xue-Qian( 1 School of Physics, Nankai University, Tianjin 300071, China 2 School of Science, Tianjin University, Tianjin 300072, China 3 School of Physics, University of Chinese Academy of Sciences, Beijing 100049, China) 11-5641/O4 exotic states, Born-Oppenheimer approximation, molecule, tetraquark In this work, we use the Born-Oppenheimer approximation, where the potential between atoms can be approximated as a function of distance between the two nuclei, to study the four-quark bound states. By this approximation, Heitler and London calculated the spectrum of the hydrogen molecule, which includes two protons (heavy) and two electrons (light). Cenerally, the observed exotic mesons Zb(10610), ZD(10650), Zc(3900) and Zc(4020) (Zc(4025)) may be molecular states made of two physical mesons and/or diquark-anti-diquark structures. Analogous to the Heitler-London method for calculating the mass of the hydrogen molecule, we investigate whether there exist energy minima for these two structures. Contrary to the hydrogen molecule case where only the spin-triplet possesses an energy minimum, there exist minima for both of these states. This implies that both molecule and tetraquark states can be stable objects. Since they have the same quantum numbers, however, the two states may mix to result in the physical states. A consequence would be that partner exotic states co-existing with ZD(10610), Zb(]0650), Zc(3900) and Zc(4020) (Zc(4025)) are predicted and should be experimentally observed. ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 23 |
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| References | 22 24 25 26 27 28 29 Shen P N (43) 1999; 25 30 31 10 11 33 12 34 Adachi I (Belle collaboration) (1) 13 35 14 36 15 37 16 38 17 39 18 Vijande J (20) 2005; 31 19 Olive K A (Particle Data Group collaboration) (32) 2014; 38 2 3 5 Ablikim M (BESIII collaboration) (4) 6 7 8 9 40 (41) 2005; 44 42 21 Chang C H (23) 2005; 43 |
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| SubjectTerms | Approximation Born-Oppenheimer approximation Hydrogen Mathematical analysis Mesons Minima Molecular structure Nuclei 双夸克 奇异介子 奥本海默 氢分子 物理状态 能量最小 自旋三重态 近似理论 |
| Title | Study of the structures of four-quark states in terms of the Born-Oppenheimer approximation |
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