Mao-Jun Yan

activity

20182026

most citedThe

P_{cs} (4459)

pentaquark from a combined effective field theory and phenomenological perspective

80 citations · 447 across the 19 of their papers we have counts for

collaborators

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19 papers · 1 filter

hep-ph2026

Threshold cusp effects to measure masses of radiatively decaying hadrons: The $B_{s 0}^{*}$ mass from the $Υ ϕ$ spectrum

Hai-Long Fu, Xu Zhang, Feng-Kun Guo +3

Hadrons that decay predominantly into final states containing photons are notoriously difficult to detect at hadron colliders. Prominent examples are the yet-unobserved $B_{s 0}^{*}$ …

hep-ph2026

Decoding the near-threshold $X_{0, 1} (4140)$ and $X_{1} (4685)$ states via OZI-suppressed coupled-channel scattering

Mao-Jun Yan

To decode the near-threshold dynamics of the $X_{0, 1} (4140)$ and $X_{1} (4685)$ states, we investigate the OZI-suppressed $\{D_{s}\bar{D}_{s},\, J/ψϕ,\, D_{s}^{\ast}\bar{D}_{s}^{\…

hep-ph2023★ 20 cited

Molecular charmed baryons and pentaquarks from light-meson exchange saturation

Mao-Jun Yan, Fang-Zheng Peng, Manuel Pavon Valderrama

The spectrum of the $c q q$ baryons contains a few states whose nature is not clearly a three-quark composite and which might have a sizable baryon-meson component. Examples include…

hep-ph2023★ 26 cited

Heavy- and light-flavor symmetry partners of the $T_{cc}^{+} (3875)$ , the $X (3872)$ and the $X (3960)$ from light-meson exchange saturation

Fang-Zheng Peng, Mao-Jun Yan, Manuel Pavon Valderrama

The spectrum of the charmed meson-(anti)meson system is a fundamental tool for disentangling the nature of a few exotic hadrons, including the recently discovered $T_{cc}^{+} (3875)$ …

hep-ph2023★ 13 cited

On the $η_{1} (1855)$ , $π_{1} (1400)$ and $π_{1} (1600)$ as dynamically generated states and their SU(3) partners

Mao-Jun Yan, Jorgivan M. Dias, Adolfo Guevara +2

In this work, we interpret the newly observed $η_{1} (1855)$ resonance with exotic $J^{P C} = 1^{-+}$ quantum numbers in the $I = 0$ sector, reported by the BESIII Collaboration, as a dyna…

hep-ph2022

Rethinking the $P_{c} (4457)^{+}$ as the $P_{ψ}^{Δ^{+}} (4457)$ isoquartet $D ˉ^{*} Σ_{c}$ molecule

Fang-Zheng Peng, Mao-Jun Yan, Mario Sánchez Sánchez +1

The nature of the $P_{c} (4312)$ , $P_{c} (4440)$ and $P_{c} (4457)$ pentaquarks is a fascinating theoretical question. Within the molecular picture their more usual interpretation is that…

hep-ph2022★ 7 cited

Molecular $P_{ψ}$ pentaquarks from light-meson exchange saturation

Zi-Ying Yang, Fang-Zheng Peng, Mao-Jun Yan +2

Theoretical predictions for the spectrum of heavy meson-baryon bound states are a fundamental tool for disentangling the nature of the different pentaquark states that have been ob…

hep-ph2022★ 18 cited

Hadronic decays of the heavy-quark-spin molecular partner of $T_{cc}^{+}$

Zhao-Sai Jia, Mao-Jun Yan, Zhen-Hua Zhang +3

Starting from the hypothesis that the $T_{cc}^{+}$ discovered at LHCb is a $D^{*+} D^{0} / D^{* 0} D^{+}$ hadronic molecule, we consider the partial width of its heavy quark spin part…

hep-ph2022★ 8 cited

Triangle singularity in $B^{0} \to π^{-} K^{+} X (3872)$ via the $D_{s 1} D ˉ D^{*}$ loop and possible precise measurement of the $X (3872)$ mass

Mao-Jun Yan, Ying-Hui Ge, Xiao-Hai Liu

We investigate the $B^{0} \to π^{-} K^{+} X (3872)$ decay via the $D_{s 1} (2536) D ˉ D^{*}$ rescattering diagram. The line shape of the $K^{+} X (3872)$ distribution curve around $D_{s1}(2536)…

hep-ph2022

The $P_{ψ s}^{Λ} (4338)$ pentaquark and its partners in the molecular picture

Mao-Jun Yan, Fang-Zheng Peng, Mario Sánchez Sánchez +1

The LHCb collaboration has detected a new hidden-charm pentaquark with the quantum numbers of a $Λ$ baryon: the $P_{ψ s}^{Λ} (4338)$ . This pentaquark will be interpreted as a $\bar{D}_…

hep-ph2022

Light- and heavy-quark symmetries and the $Y (4230)$ , $Y (4360)$ , $Y (4500)$ , $Y (4620)$ and $X (4630)$ resonances

Fang-Zheng Peng, Mao-Jun Yan, Mario Sánchez Sánchez +1

The heavy hadron spectrum is constrained by symmetries, of which two of the most important ones are heavy-quark spin and SU(3)-flavor symmetries. Here we argue that in the molecula…

hep-ph2021★ 30 cited

Interpretations of the new LHCb $P_{c} (4337)^{+}$ pentaquark state

Mao-Jun Yan, Fang-Zheng Peng, Mario Sánchez Sánchez +1

Recently the LHCb collaboration has observed a new pentaquark state, the $P_{c} (4337)^{+}$ . Owing to its proximity to the $χ_{c 0} (1 S) p$ , $D ˉ^{*} Λ_{c}$ , $D ˉ Σ_{c}$ and $\bar{D} Σ_…

hep-ph2021★ 62 cited

Subleading contributions to the decay width of the $T_{cc}^{+}$ tetraquark

Mao-Jun Yan, Manuel Pavon Valderrama

Recently the LHCb collaboration has announced the discovery of the $T_{cc}^{+}$ tetraquark. Being merely a few hundred $keV$ below the $D^{*+} D^{0}$ threshold, the $T_{cc}^{+}$ is…

hep-ph2021★ 34 cited

Axial meson exchange and the $Z_{c} (3900)$ and $Z_{cs} (3985)$ resonances as heavy hadron molecules

Mao-Jun Yan, Fang-Zheng Peng, Mario Sánchez Sánchez +1

Early speculations about the existence of heavy hadron molecules were grounded on the idea that light-meson exchanges forces could lead to binding. In analogy to the deuteron, the…

hep-ph2021★ 27 cited

Heavy-hadron molecular spectrum from light-meson exchange saturation

Fang-Zheng Peng, Mario Sánchez Sánchez, Mao-Jun Yan +1

If known, the spectrum of heavy-hadron molecules will be a key tool to disentangle the nature of the exotic states that are being discovered in experiments. Here we argue that the…

hep-ph2020★ 80 cited

The $P_{cs} (4459)$ pentaquark from a combined effective field theory and phenomenological perspective

Fang-Zheng Peng, Mao-Jun Yan, Mario Sánchez Sánchez +1

The observation of the $P_{cs} (4459)$ by the LHCb collaboration adds a new member to the set of known hidden-charm pentaquarks, which includes the $P_{c} (4312)$ , $P_{c} (4440)$ and $P_c…

hep-ph2020★ 65 cited

Triangle singularity as the origin of $X_{0} (2900)$ and $X_{1} (2900)$ observed in $B^{+} \to D^{+} D^{-} K^{+}$

Xiao-Hai Liu, Mao-Jun Yan, Hong-Wei Ke +2

The LHCb collaboration reported the observation of a narrow peak in the $D^{-} K^{+}$ invariant mass distributions from the $B^{+} \to D^{+} D^{-} K^{+}$ decay. The peak is parameterized in ter…

hep-ph2020★ 24 cited

Peaks within peaks and the possible two-peak structure of the Pc(4457): the effective field theory perspective

Fang-Zheng Peng, Jun-Xu Lu, Mario Sánchez Sánchez +2

The LHCb pentaquarks -- the $P_{c} (4312)$ , $P_{c} (4440)$ and $P_{c} (4457)$ -- have been theorized to be $Σ_{c} D ˉ$ and $Σ_{c} D ˉ^{*}$ S-wave molecules. Here we explore the possibilit…

hep-ph2018★ 33 cited

New spectrum of negative-parity doubly charmed baryons: Possibility of two quasistable states

Mao-Jun Yan, Xiao-Hai Liu, Sergi Gonzàlez-Solís +4

The discovery of $Ξ_{cc}^{++}$ by the LHCb Collaboration triggers predictions of more doubly charmed baryons. By taking into account both the $P$ -wave excitations between the two c…

Threshold cusp effects to measure masses of radiatively decaying hadrons: The Bs0∗​ mass from the Υϕ spectrum

Decoding the near-threshold X0,1​(4140) and X1​(4685) states via OZI-suppressed coupled-channel scattering

Molecular charmed baryons and pentaquarks from light-meson exchange saturation

Heavy- and light-flavor symmetry partners of the Tcc+​(3875), the X(3872) and the X(3960) from light-meson exchange saturation

On the η1​(1855), π1​(1400) and π1​(1600) as dynamically generated states and their SU(3) partners

Rethinking the Pc​(4457)+ as the PψΔ+​(4457) isoquartet Dˉ∗Σc​ molecule

Molecular Pψ​ pentaquarks from light-meson exchange saturation

Hadronic decays of the heavy-quark-spin molecular partner of Tcc+​

Triangle singularity in B0→π−K+X(3872) via the Ds1​DˉD∗ loop and possible precise measurement of the X(3872) mass

The PψsΛ​(4338) pentaquark and its partners in the molecular picture

Light- and heavy-quark symmetries and the Y(4230), Y(4360), Y(4500), Y(4620) and X(4630) resonances

Interpretations of the new LHCb Pc​(4337)+ pentaquark state

Subleading contributions to the decay width of the Tcc+​ tetraquark

Axial meson exchange and the Zc​(3900) and Zcs​(3985) resonances as heavy hadron molecules

Heavy-hadron molecular spectrum from light-meson exchange saturation

The Pcs​(4459) pentaquark from a combined effective field theory and phenomenological perspective

Triangle singularity as the origin of X0​(2900) and X1​(2900) observed in B+→D+D−K+

Peaks within peaks and the possible two-peak structure of the Pc(4457): the effective field theory perspective

New spectrum of negative-parity doubly charmed baryons: Possibility of two quasistable states

Threshold cusp effects to measure masses of radiatively decaying hadrons: The $B_{s 0}^{*}$ mass from the $Υ ϕ$ spectrum

Decoding the near-threshold $X_{0, 1} (4140)$ and $X_{1} (4685)$ states via OZI-suppressed coupled-channel scattering

Heavy- and light-flavor symmetry partners of the $T_{cc}^{+} (3875)$ , the $X (3872)$ and the $X (3960)$ from light-meson exchange saturation

On the $η_{1} (1855)$ , $π_{1} (1400)$ and $π_{1} (1600)$ as dynamically generated states and their SU(3) partners

Rethinking the $P_{c} (4457)^{+}$ as the $P_{ψ}^{Δ^{+}} (4457)$ isoquartet $D ˉ^{*} Σ_{c}$ molecule

Molecular $P_{ψ}$ pentaquarks from light-meson exchange saturation

Hadronic decays of the heavy-quark-spin molecular partner of $T_{cc}^{+}$

Triangle singularity in $B^{0} \to π^{-} K^{+} X (3872)$ via the $D_{s 1} D ˉ D^{*}$ loop and possible precise measurement of the $X (3872)$ mass

The $P_{ψ s}^{Λ} (4338)$ pentaquark and its partners in the molecular picture

Light- and heavy-quark symmetries and the $Y (4230)$ , $Y (4360)$ , $Y (4500)$ , $Y (4620)$ and $X (4630)$ resonances

Interpretations of the new LHCb $P_{c} (4337)^{+}$ pentaquark state

Subleading contributions to the decay width of the $T_{cc}^{+}$ tetraquark

Axial meson exchange and the $Z_{c} (3900)$ and $Z_{cs} (3985)$ resonances as heavy hadron molecules

The $P_{cs} (4459)$ pentaquark from a combined effective field theory and phenomenological perspective

Triangle singularity as the origin of $X_{0} (2900)$ and $X_{1} (2900)$ observed in $B^{+} \to D^{+} D^{-} K^{+}$