Publication data of Xie, Ju-Jun: Link to Inspire

Created with Highcharts 9.0.1CitationsCitationsw/o self-citaionself-citaion200620082010201220142016201820202022202401000200030004000
Created with Highcharts 9.0.1Publicationspublications per yearPublicationsPublications per yearCumulative publications20062008201020122014201620182020202220240501001502002500612182430
Created with Highcharts 9.0.1h-indexh-indexh-indexh-index w/o self-citaion2006200820102012201420162018202020222024010203040
Created with Highcharts 9.0.1CitationsBreakdown of Most Cited PapersrestThe role of the $N^*(2080)$ resonance in the $ ec{gamma} p o K^+ Lambda(1520)$ reactionThe role of the $N^*(2080)$ resonance in the $ ec{gamma} p o K^+ Lam…$f_0(500)$ , $f_0(980)$ , and $a_0(980)$ production in the $chi _{c1} ightarrow eta pi ^+pi ^-$ reaction$f_0(500)$ , $f_0(980)$ , and $a_0(980)$ production in the $chi _{c1} igh…Determination of the $oldsymbol{eta ^3{ m He}}$ threshold structure from the low energy $oldsymbol{pd o eta ^3{ m He}}$ reactionDetermination of the $oldsymbol{eta ^3{ m He}}$ threshold structure fro…The Role of Delta++*(1620) resonances in pp ---> nK+ Sigma+ reaction and its important implicationsThe Role of Delta++*(1620) resonances in pp ---> nK+ Sigma+ reaction and …Neutral hidden charm pentaquark states $P_c^0(4380)$ and $P_c^0(4450)$ in $pi^-p o J/psi n$ reactionNeutral hidden charm pentaquark states $P_c^0(4380)$ and $P_c^0(4450)…Faddeev fixed center approximation to the $Nar{K}K$ system and the signature of a $N^*(1920)(1/2^+)$ stateFaddeev fixed center approximation to the $Nar{K}K$ system and the sign…Strong decays of ${ar{D}}^{*}K^{*}$ molecules and the newly observed $X_{0,1}$ statesStrong decays of ${ar{D}}^{*}K^{*}$ molecules and the newly observed…Disentangling the hadronic molecule nature of the $P_c(4380)$ pentaquark-like structureDisentangling the hadronic molecule nature of the $P_c(4380)$ pentaquark-…Role of a triangle singularity in the $gamma p ightarrow K^+ Lambda(1405)$ reactionRole of a triangle singularity in the $gamma p ightarrow K^+ Lambda(1405)…Dynamically generated $J^P=1/2^-(3/2^-)$ singly charmed and bottom heavy baryonsDynamically generated $J^P=1/2^-(3/2^-)$ singly charmed and bottom hea…Triangle singularity as the origin of $X_0(2900)$ and $X_1(2900)$ observed in $B^+ o D^+ D^- K^+$Triangle singularity as the origin of $X_0(2900)$ and $X_1(2900)$ observed …The low lying scalar resonances in the $D^0$ decays into $K^0_s$ and $f_0(500)$, $f_0(980)$, $a_0(980)$The low lying scalar resonances in the $D^0$ decays into $K^0_s$ and $f_0…The Role of N*(1535) in pp ---> pp phi and pi- p ---> n phi reactionsThe $Lambda_{b} ightarrow J/psi K^{0}Lambda$ reaction and a hidden-charm pentaquark state with strangenessThe $Lambda_{b} ightarrow J/psi K^{0}Lambda$ reaction and a hidden-ch…Can we understand the decay width of the Tcc+ state?Spin-parities of the $P_c(4440)$ and $P_c(4457)$ in the one-boson-exchange modelSpin-parities of the $P_c(4440)$ and $P_c(4457)$ in the one-boson-exchang…$X_0(2866)$ as a $D^*ar{K}^*$ molecular stateLooking for a hidden-charm pentaquark state with strangeness S=−1 from Ξ$_b^−$ decay into J/ψK$^−$ΛLooking for a hidden-charm pentaquark state with strangeness S=−1 from Ξ…Heavy-quark spin and flavor symmetry partners of the X(3872) revisited: What can we learn from the one boson exchange model?Heavy-quark spin and flavor symmetry partners of the X(3872) revisited: Wh…200620082010201220142016201820202022202401000200030004000
Created with Highcharts 9.0.1Fraction [%]Breakdown of Most Cited Papers (Fraction)The role of the $N^*(2080)$ resonance in the $ ec{gamma} p o K^+ Lambda(1520)$ reactionThe role of the $N^*(2080)$ resonance in the $ ec{gamma} p o K^+ Lam…$f_0(500)$ , $f_0(980)$ , and $a_0(980)$ production in the $chi _{c1} ightarrow eta pi ^+pi ^-$ reaction$f_0(500)$ , $f_0(980)$ , and $a_0(980)$ production in the $chi _{c1} igh…Determination of the $oldsymbol{eta ^3{ m He}}$ threshold structure from the low energy $oldsymbol{pd o eta ^3{ m He}}$ reactionDetermination of the $oldsymbol{eta ^3{ m He}}$ threshold structure fro…The Role of Delta++*(1620) resonances in pp ---> nK+ Sigma+ reaction and its important implicationsThe Role of Delta++*(1620) resonances in pp ---> nK+ Sigma+ reaction and …Neutral hidden charm pentaquark states $P_c^0(4380)$ and $P_c^0(4450)$ in $pi^-p o J/psi n$ reactionNeutral hidden charm pentaquark states $P_c^0(4380)$ and $P_c^0(4450)…Faddeev fixed center approximation to the $Nar{K}K$ system and the signature of a $N^*(1920)(1/2^+)$ stateFaddeev fixed center approximation to the $Nar{K}K$ system and the sign…Strong decays of ${ar{D}}^{*}K^{*}$ molecules and the newly observed $X_{0,1}$ statesStrong decays of ${ar{D}}^{*}K^{*}$ molecules and the newly observed…Disentangling the hadronic molecule nature of the $P_c(4380)$ pentaquark-like structureDisentangling the hadronic molecule nature of the $P_c(4380)$ pentaquark-…Role of a triangle singularity in the $gamma p ightarrow K^+ Lambda(1405)$ reactionRole of a triangle singularity in the $gamma p ightarrow K^+ Lambda(1405)…Dynamically generated $J^P=1/2^-(3/2^-)$ singly charmed and bottom heavy baryonsDynamically generated $J^P=1/2^-(3/2^-)$ singly charmed and bottom hea…Triangle singularity as the origin of $X_0(2900)$ and $X_1(2900)$ observed in $B^+ o D^+ D^- K^+$Triangle singularity as the origin of $X_0(2900)$ and $X_1(2900)$ observed …The low lying scalar resonances in the $D^0$ decays into $K^0_s$ and $f_0(500)$, $f_0(980)$, $a_0(980)$The low lying scalar resonances in the $D^0$ decays into $K^0_s$ and $f_0…The Role of N*(1535) in pp ---> pp phi and pi- p ---> n phi reactionsThe $Lambda_{b} ightarrow J/psi K^{0}Lambda$ reaction and a hidden-charm pentaquark state with strangenessThe $Lambda_{b} ightarrow J/psi K^{0}Lambda$ reaction and a hidden-ch…Can we understand the decay width of the Tcc+ state?Spin-parities of the $P_c(4440)$ and $P_c(4457)$ in the one-boson-exchange modelSpin-parities of the $P_c(4440)$ and $P_c(4457)$ in the one-boson-exchang…$X_0(2866)$ as a $D^*ar{K}^*$ molecular stateLooking for a hidden-charm pentaquark state with strangeness S=−1 from Ξ$_b^−$ decay into J/ψK$^−$ΛLooking for a hidden-charm pentaquark state with strangeness S=−1 from Ξ…Heavy-quark spin and flavor symmetry partners of the X(3872) revisited: What can we learn from the one boson exchange model?Heavy-quark spin and flavor symmetry partners of the X(3872) revisited: Wh…20062008201020122014201620182020202220240255075100
Created with Highcharts 9.0.1Citations/1 YearCitations/PeriodCitations / 1 YearMoving average200620082010201220142016201820202022202402004006008001000