We systematically study hidden charm pentaquark states in the constituent quark model with a general Hamiltonian for multiquark systems, considering the coupling between the <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:msubsup><a:mi mathvariant="normal">Σ</a:mi><a:mi>c</a:mi><a:mrow><a:mo stretchy="false">(</a:mo><a:mo>*</a:mo><a:mo stretchy="false">)</a:mo></a:mrow></a:msubsup><a:msup><a:mover accent="true"><a:mi>D</a:mi><a:mo stretchy="false">¯</a:mo></a:mover><a:mrow><a:mo stretchy="false">(</a:mo><a:mo>*</a:mo><a:mo stretchy="false">)</a:mo></a:mrow></a:msup></a:math> molecular states and the <j:math xmlns:j="http://www.w3.org/1998/Math/MathML" display="inline"><j:msup><j:mi>q</j:mi><j:mn>3</j:mn></j:msup><j:mi>c</j:mi><j:mover accent="true"><j:mi>c</j:mi><j:mo stretchy="false">¯</j:mo></j:mover></j:math> compact pentaquark states by the one-gluon exchange hyperfine interaction. The ground state hidden-charm pentaquark mass spectra and the strong decay widths are calculated. This work suggests that <n:math xmlns:n="http://www.w3.org/1998/Math/MathML" display="inline"><n:msub><n:mi>P</n:mi><n:mi>c</n:mi></n:msub><n:mo stretchy="false">(</n:mo><n:mn>4312</n:mn><n:mo stretchy="false">)</n:mo></n:math>, <r:math xmlns:r="http://www.w3.org/1998/Math/MathML" display="inline"><r:msub><r:mi>P</r:mi><r:mi>c</r:mi></r:msub><r:mo stretchy="false">(</r:mo><r:mn>4457</r:mn><r:mo stretchy="false">)</r:mo></r:math>, and <v:math xmlns:v="http://www.w3.org/1998/Math/MathML" display="inline"><v:msub><v:mi>P</v:mi><v:mi>c</v:mi></v:msub><v:mo stretchy="false">(</v:mo><v:mn>4380</v:mn><v:mo stretchy="false">)</v:mo></v:math> resonances might be mainly <z:math xmlns:z="http://www.w3.org/1998/Math/MathML" display="inline"><z:msub><z:mi mathvariant="normal">Σ</z:mi><z:mi>c</z:mi></z:msub><z:mover accent="true"><z:mi>D</z:mi><z:mo stretchy="false">¯</z:mo></z:mover></z:math>, <eb:math xmlns:eb="http://www.w3.org/1998/Math/MathML" display="inline"><eb:msub><eb:mi mathvariant="normal">Σ</eb:mi><eb:mi>c</eb:mi></eb:msub><eb:msup><eb:mover accent="true"><eb:mi>D</eb:mi><eb:mo stretchy="false">¯</eb:mo></eb:mover><eb:mo>*</eb:mo></eb:msup></eb:math>, and <jb:math xmlns:jb="http://www.w3.org/1998/Math/MathML" display="inline"><jb:msubsup><jb:mi mathvariant="normal">Σ</jb:mi><jb:mi>c</jb:mi><jb:mo>*</jb:mo></jb:msubsup><jb:mover accent="true"><jb:mi>D</jb:mi><jb:mo stretchy="false">¯</jb:mo></jb:mover></jb:math> hadronic molecules respectively, and <ob:math xmlns:ob="http://www.w3.org/1998/Math/MathML" display="inline"><ob:msub><ob:mi>P</ob:mi><ob:mi>c</ob:mi></ob:msub><ob:mo stretchy="false">(</ob:mo><ob:mn>4440</ob:mn><ob:mo stretchy="false">)</ob:mo></ob:math> might include sizable pentaquark components. Published by the American Physical Society 2024
No takes yet. Share an insight, caveat, or question.
Xu et al. (2024) studied this question.
Synapse has enriched 5 closely related papers on similar clinical questions. Consider them for comparative context: