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Tetraquark state X(6900) and the interaction between diquark and antidiquark

The European physical journal. C, Particles and fields, 2021-05, Vol.81 (5), p.1-9, Article 427

2021

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Possible molecular states of D(∗)D(∗) and B(∗)B(∗) within the Bethe–Salpeter framework

The European physical journal. C, Particles and fields, 2022-02, Vol.82 (2), Article 144

2022

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Threshold effects as the origin of Zcs(4000), Zcs(4220) and X(4700) observed in B+→J/ψϕK

The European physical journal. C, Particles and fields, 2021-09, Vol.81 (9)

2021

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Study on Ξcc→Ξc and Ξcc→Ξc′ weak decays in the light-front quark model

The European physical journal. C, Particles and fields, 2020-02, Vol.80 (2)

2020

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Weak decays of the triply heavy baryons in the three-quark picture with the light-front quark model

The European physical journal. C, Particles and fields, 2024-05, Vol.84 (5), p.452-10, Article 452

2024

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Synthesis of Ultrasmall Cu2O Nanocubes and Octahedra with Tunable Sizes for Facet-Dependent Optical Property Examination

Small (Weinheim an der Bergstrasse, Germany), 2016-07, Vol.12 (26), p.3530-3534

2016

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How can X±(5568) escape detection?

Physics letters. B, 2018-10, Vol.785, p.301-303

2018

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The possible Bπ molecular state and its radiative decay

The European physical journal. C, Particles and fields, 2017-05, Vol.77 (5), p.1-7

2017

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Revisiting Λb→Λc and Σb→Σc weak decays in the light-front quark model

The European physical journal. C, Particles and fields, 2019-06, Vol.79 (6)

2019

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Semileptonic and nonleptonic weak decays of Λb0

Physical review. D, 2019-03, Vol.99 (5)

2019

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Study of the strong decays of ϕ ( 2170 ) and the future charm-tau factory

Physical review. D, 2019-02, Vol.99 (3), p.1, Article 036014

2019

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Vertex functions for d-wave mesons in the light-front approach

The European physical journal. C, Particles and fields, 2011-10, Vol.71 (10), p.1-7, Article 1776

2011

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Possibility of Tcs¯(2900) as the resonance-like structure induced by threshold effects

The European physical journal. C, Particles and fields, 2022-10, Vol.82 (10)

2022

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Study on the weak decay between two heavy baryons Bi(12+)→Bf(32+) in the light-front quark model

The European physical journal. C, Particles and fields, 2023-05, Vol.83 (5), p.412

2023

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Facet-Dependent Electrical Conductivity Properties of Cu2O Crystals

Nano letters, 2015-03, Vol.15 (3), p.2155-2160

2015

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

The European physical journal. C, Particles and fields, 2020-12, Vol.80 (12)

2020

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Study on the mixing of Ξ c and Ξ c ′ by the transition Ξ b → Ξ c ( ′ )

Physical review. D, 2024-04, Vol.109 (7), Article 073006

2024

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Applying the Kalman filter particle method to strange and open charm hadron reconstruction in the STAR experiment

Nuclear science and techniques, 2023-10, Vol.34 (10), p.148-157, Article 158

2023

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Searching for doubly charmed tetraquark candidates Tcc and Tccs¯ in Bc decays

The European physical journal. C, Particles and fields, 2023-03, Vol.83 (3), p.258

2023

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Estimating decay rate of X±(5568)→Bsπ± while assuming them to be molecular states

The European physical journal. C, Particles and fields, 2018-05, Vol.78 (5)

2018

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Unified Fano-like interference picture for charmoniumlike states Y ( 4008 ) , Y ( 4260 ) and Y ( 4360 )

Physical review. D, 2016-01, Vol.93 (1), Article 014011

2016

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Exploring open-charm decay mode ΛcΛ¯c of charmonium-like state Y(4630)

The European physical journal. C, Particles and fields, 2016-10, Vol.76 (10)

2016

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An Underlying Symmetry Determines all Elements of CKM and PMNS up to a Universal Constant?

Communications in theoretical physics, 2015-11, Vol.64 (5), p.519-524

2015

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Threshold effects as the origin of $$Z_{cs}(4000)$$, $$Z_{cs}(4220)$$ and X(4700) observed in $$B^+\rightarrow J/\psi \phi K

The European physical journal. C, Particles and fields, 2021-09, Vol.81 (9), Article 854

2021

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Estimating decay rate of X ± ( 5568 ) → B s π ± while assuming them to be molecular states

The European physical journal. C, Particles and fields, 2018-05, Vol.78 (5), p.1-7

2018

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Tetraquark state X(6900) and the interaction between diquark and antidiquark

Possible molecular states of D(∗)D(∗) and B(∗)B(∗) within the Bethe–Salpeter framework

Threshold effects as the origin of Zcs(4000), Zcs(4220) and X(4700) observed in B+→J/ψϕK

Study on Ξcc→Ξc and Ξcc→Ξc′ weak decays in the light-front quark model

Weak decays of the triply heavy baryons in the three-quark picture with the light-front quark model

Synthesis of Ultrasmall Cu2O Nanocubes and Octahedra with Tunable Sizes for Facet-Dependent Optical Property Examination

How can X±(5568) escape detection?

The possible Bπ molecular state and its radiative decay

Revisiting Λb→Λc and Σb→Σc weak decays in the light-front quark model

Semileptonic and nonleptonic weak decays of Λb0

Study of the strong decays of ϕ ( 2170 ) and the future charm-tau factory

Vertex functions for d-wave mesons in the light-front approach

Possibility of Tcs¯(2900) as the resonance-like structure induced by threshold effects

Study on the weak decay between two heavy baryons Bi(12+)→Bf(32+) in the light-front quark model

Facet-Dependent Electrical Conductivity Properties of Cu2O Crystals

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

Study on the mixing of Ξ c and Ξ c ′ by the transition Ξ b → Ξ c ( ′ )

Applying the Kalman filter particle method to strange and open charm hadron reconstruction in the STAR experiment

Searching for doubly charmed tetraquark candidates Tcc and Tccs¯ in Bc decays

Estimating decay rate of X±(5568)→Bsπ± while assuming them to be molecular states

Unified Fano-like interference picture for charmoniumlike states Y ( 4008 ) , Y ( 4260 ) and Y ( 4360 )

Exploring open-charm decay mode ΛcΛ¯c of charmonium-like state Y(4630)

An Underlying Symmetry Determines all Elements of CKM and PMNS up to a Universal Constant?

Threshold effects as the origin of $$Z_{cs}(4000)$$, $$Z_{cs}(4220)$$ and X(4700) observed in $$B^+\rightarrow J/\psi \phi K

Estimating decay rate of X ± ( 5568 ) → B s π ± while assuming them to be molecular states

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