001 | 330334 | ||
005 | 20211110142839.0 | ||
020 | _ | _ | |a 978-3-945931-07-3 |
020 | _ | _ | |a 978-3-945931-07-3 |
024 | 7 | _ | |a 10.3204/DESY-PROC-2016-04/Rehman |2 datacite_doi |
024 | 7 | _ | |a 1435-8077 |2 ISSN |
037 | _ | _ | |a PUBDB-2017-06833 |
041 | _ | _ | |a English |
088 | 1 | _ | |a DESY-PROC-2016-04 |
088 | _ | _ | |a DESY-PROC-2016-04 |2 DESY |
100 | 1 | _ | |a Ali, Ahmed |0 P:(DE-H253)PIP1003110 |b 0 |u desy |
111 | 2 | _ | |a Quantum Field Theory at the Limits |c Dubna |d 2016-07-18 - 2016-07-30 |g HQ 2016 |0 C16-07-18.8 |2 inspire |w Russia |
245 | _ | _ | |a Heavy Quark Symmetry and Hidden Charm Pentaquarks |
260 | _ | _ | |a Hamburg |c 2017 |b Verlag Deutsches Elektronen-Synchrotron |
295 | 1 | 0 | |a Ali, Ahmed "Heavy Quark Symmetry and Hidden Charm Pentaquarks" in Proceedings of the Helmholtz International Summer School 2016 (HQ 2016) : Quantum Field Theory at the Limits : from Strong Fields to Heavy Quarks / Ali, Ahmed, Blaschke, David, Issadykov, Aidos, Ivanov, Mikhail (eds.), Verlag Deutsches Elektronen-Synchrotron : 2017 ; HQ 2016 : Helmholtz International Summer School 2016, 2016-07-18 - 2016-07-30, Dubna |
300 | _ | _ | |a 239-245 |
336 | 7 | _ | |a CONFERENCE_PAPER |2 ORCID |
336 | 7 | _ | |a Conference Paper |0 33 |2 EndNote |
336 | 7 | _ | |a INPROCEEDINGS |2 BibTeX |
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336 | 7 | _ | |a Report |0 PUB:(DE-HGF)29 |2 PUB:(DE-HGF) |m report |
336 | 7 | _ | |a Output Types/Conference Paper |2 DataCite |
336 | 7 | _ | |a Contribution to a conference proceedings |b contrib |m contrib |0 PUB:(DE-HGF)8 |s 1499687046_20607 |2 PUB:(DE-HGF) |
336 | 7 | _ | |a Contribution to a book |0 PUB:(DE-HGF)7 |2 PUB:(DE-HGF) |m contb |
490 | 0 | _ | |a DESY-PROC |0 PERI:(DE-600)2450075-6 |
520 | _ | _ | |a We report on the role of the heavy quark symmetry (HQS) in understanding the hidden charm pentaquarks, $P_c^+(4380)$ and $P_c^+(4450)$, observed by LHCb in $\Lambda_b^0 \to J/\psi\; p\; K^-$ decays, in the compact diquark-diquark-antiquark picture. In the HQS-limit, only the state $P_c^+(4450)$ is expected to be produced. Within this picture, we employ $SU(3)_F$ symmetry to discuss the mass spectrum and decays of the related pentaquark states $\bar{c}[cq][q^\prime q^{\prime\prime}]$ with $q, q^{\prime}, q^{\prime \prime} \in [u,d,s]$. Some of these pentaquarks are expected to be produced in $b$-baryon decays and we work out their relative decay widths. |
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693 | _ | _ | |0 EXP:(DE-MLZ)NOSPEC-20140101 |5 EXP:(DE-MLZ)NOSPEC-20140101 |e No specific instrument |x 0 |
700 | 1 | _ | |a Ahmed, Ishtiaq |0 P:(DE-HGF)0 |b 1 |
700 | 1 | _ | |a Aslam, M. Jamil |0 P:(DE-HGF)0 |b 2 |
700 | 1 | _ | |a Rehman, Abdur |0 P:(DE-HGF)0 |b 3 |e Corresponding author |
787 | 0 | _ | |a Ali, Ahmed et. al. |d Verlag Deutsches Elektronen-Synchrotron |i isPartOf |0 PUBDB-2017-01598 |r DESY-PROC-2016-04 |t Proceedings of the Helmholtz International Summer School 2016 (HQ 2016) : Quantum Field Theory at the Limits : from Strong Fields to Heavy Quarks |
856 | 4 | _ | |u https://bib-pubdb1.desy.de/record/330334/files/fulltext.pdf |y OpenAccess |
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910 | 1 | _ | |a National Centre for Physics - Quaid-i-Azam University Campus - Islamabad 45320 - Pakistan |b 0 |
910 | 1 | _ | |a Physics Department - Quaid-i-Azam University - Islamabad 45320 - Pakistan |b 0 |
910 | 1 | _ | |a NCP, Islamabad |0 I:(DE-HGF)0 |b 1 |6 P:(DE-HGF)0 |
910 | 1 | _ | |a Quaid-i-Azam U. |0 I:(DE-HGF)0 |b 2 |6 P:(DE-HGF)0 |
910 | 1 | _ | |a NCP, Islamabad |0 I:(DE-HGF)0 |b 3 |6 P:(DE-HGF)0 |
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914 | 1 | _ | |y 2017 |
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915 | _ | _ | |a Creative Commons Attribution CC BY 4.0 |0 LIC:(DE-HGF)CCBY4 |2 HGFVOC |
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