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Related papers: How can $X^{\pm}(5568)$ escape detection?

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Very recently, the D0 collaboration has reported the observation of a narrow structure, $X(5568)$, in the decay process $X(5568)\to B^0_s\pi^\pm$ using the 10.4${\rm fb}^{-1}$ data of $p\bar p$ collision at $\sqrt s= 1.96$ TeV. This…

High Energy Physics - Phenomenology · Physics 2016-07-22 Wei Wang , Ruilin Zhu

The recent observation by the D$\O$ collaboration of the first tetraquark candidate with four different quark flavors $(u, d, s$ and $ b)$ in the $B^0_s\pi^{\pm}$ channel having a narrow structure, has still not been confirmed by other…

High Energy Physics - Phenomenology · Physics 2020-01-08 J. Y. Süngü , A. Türkan , E. Veli Veliev

Discovery of $X(5568)$ brings up a tremendous interest because it is very special, i.e. made of four different flavors. The D0 collaboration claimed that they observed this resonance through portal $X(5568)\to B_s\pi$, but unfortunately,…

High Energy Physics - Phenomenology · Physics 2020-03-17 Hong-Wei Ke , Xue-Qian Li

We investigate the recent evidence for a charged $X(5568)$ meson as an exotic open-flavor tetraquark state $su\bar b\bar d$ with $J^P=0^+/1^+$ in the framework of QCD sum rules. We use the color antisymmetric $[\mathbf{\bar 3_c}]_{su}…

High Energy Physics - Phenomenology · Physics 2016-07-08 Wei Chen , Hua-Xing Chen , Xiang Liu , T. G. Steele , Shi-Lin Zhu

The $S$-wave eigenstates of tetraquarks of type $s u \bar d \bar b$ with J$^{P}$ = 0$^{+}$, 1$^{+}$ and 2$^{+}$ are studied within a simple quark model with chromomagnetic interaction and effective quark masses extracted from meson and…

High Energy Physics - Phenomenology · Physics 2016-08-25 Fl. Stancu

Stimulated by the recent observation of the exotic $X(5568)$ state by D0 Collaboration, we study the four-quark system $us\bar{b}\bar{d}$ with quantum numbers $J^P=0^+$ in the framework of chiral quark model. Two structures,…

High Energy Physics - Phenomenology · Physics 2016-07-20 Xiaoyun Chen , Jialun Ping

Inspired by the report of D0 Collaboration on the state $X(5568)$ with four different flavors, a similar state, $ud\bar{s}\bar{b}$ is investigated in the present work. The advantage of looking for this state over the state $X(5568)$ with…

High Energy Physics - Phenomenology · Physics 2018-10-03 Xiaoyun Chen , Jialun Ping

We report evidence of a narrow structure, $X(5568)$, in the decay sequence $X(5568) \rightarrow B_s^0 \pi^{\pm}$, $B_s^0 \rightarrow J/\psi \phi$, $J/\psi\rightarrow \mu^+ \mu^-$, $\phi \rightarrow K^+K^-$. This is evidence for the first…

High Energy Physics - Experiment · Physics 2016-12-14 D0 Collaboration

Stimulated by the recent observation of the $X(5568)$, we study the $X(5568)$ and its partners under the tetraquark scenario. In the framework of the color-magnetic interaction, we estimate the masses of the partner states of the $X(5568)$…

High Energy Physics - Phenomenology · Physics 2016-04-20 Yan-Rui Liu , Xiang Liu , Shi-Lin Zhu

We use a combination of quark-antiquark and $B^{(*)}K$ interpolating fields to predict the mass of two QCD bound states below the $B^*K$ threshold in the quantum channels $J^P=0^+$ and $1^+$. The mesons correspond to the b-quark cousins of…

High Energy Physics - Lattice · Physics 2016-11-09 Daniel Mohler , C. B. Lang , Sasa Prelovsek

The exotic state $X(5568)$ which was observed by D0 Collaboration is very likely to be a tetraquark state with four different valence quark flavors, though the existence was not confirmed by other collaborations. The possibility of such…

High Energy Physics - Phenomenology · Physics 2019-05-22 Ye Xing , Fu-Sheng Yu , Ruilin Zhu

The parameters, i.e. the mass and current coupling of the exotic $X(5568)$ state observed by the D0 Collaboration as well as the decay width of the process $X \to B_s^{0}\pi^{+}$ are explored using $B\bar{K}$ molecule assumption on its…

High Energy Physics - Phenomenology · Physics 2016-07-01 S. S. Agaev , K. Azizi , H. Sundu

In a one-boson-exchange model, we study molecular states of double-charm baryon ($\Xi_{cc}(3621)$) and a charmed meson ($D$ and $D^*$). Our model indicates that there exist two possible triple-charm molecular pentaquarks, a $\Xi_{cc}D$…

High Energy Physics - Phenomenology · Physics 2018-01-03 Rui Chen , Atsushi Hosaka , Xiang Liu

A variety of options for interpreting the D\O{} state, $X(5568)$, are examined. We find that threshold, cusp, molecular, and tetraquark models are all unfavoured. Several experimental tests for unravelling the nature of the signal are…

High Energy Physics - Phenomenology · Physics 2016-08-24 T. J. Burns , E. S. Swanson

We scrutinize recent QCD spectral sum rules (QSSR) results to lowest order (LO) predicting the masses of the BK molecule and (su)\bar(bd) four-quark states. We improve these results by adding NLO and N2LO corrections to the PT contributions…

High Energy Physics - Phenomenology · Physics 2016-07-01 R. Albuquerque , S. Narison , A. Rabemananjara , D. Rabetiarivony

The $D_s(2320)$ state recently observed by BaBar in the $D_s^+\pi^0$ channel may be the first of a host of $cq\bar q\bar q$ four-quark states. We give a phenomenological account of the masses and decay modes. The isosinglet $D_s(2320)$…

High Energy Physics - Phenomenology · Physics 2008-11-26 Hai-Yang Cheng , Wei-Shu Hou

In the framework of the quark delocalization color screening model, we investigate tetraquarks composed of $us\bar{d}\bar{b}$ and $ud\bar{s}\bar{b}$ in two structures: meson-meson structure and diquark-antidiquark structure. Neither bound…

High Energy Physics - Phenomenology · Physics 2022-10-12 Hongxia Huang , Jialun Ping

We analyze the possibility of the existence of a fully exotic pentaquark state $udsc\bar{b}$, which is made from the five different flavors participarting in the strong interactions. We investigate the coupled channel effects of the…

High Energy Physics - Phenomenology · Physics 2022-06-08 Chao-Wei Shen , Ulf-G. Meißner

Beauty tetraquark states $X(\bar b q'q'' \bar q )$ composed of $ \bar b s u \bar d$, $\bar b d s \bar u$, and $\bar b u d \bar s$, are unique that all the four valence quarks are different. Although the claim of existence of the first two…

High Energy Physics - Phenomenology · Physics 2016-09-21 Xiao-Gang He , Pyungwon Ko

In this article, we take the $X(5568)$ as the diquark-antidiquark type tetraquark state with the spin-parity $J^P=0^+$, construct the scalar-diquark-scalar-antidiquark type current, carry out the operator product expansion up to the vacuum…

High Energy Physics - Phenomenology · Physics 2016-09-21 Zhi-Gang Wang
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