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Related papers: Dimesonic states with the heavy-light flavour meso…

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With a quark level interaction, we give a unified description of the loosely bound molecular systems composed of the heavy flavor hadrons $(\bar{D},\bar{D}^*)$, $(\Lambda_c, \Sigma_c, \Sigma_c^*)$, and $(\Xi_c, \Xi_c^\prime,\Xi_c^*)$. Using…

High Energy Physics - Phenomenology · Physics 2022-07-13 Kan Chen , Rui Chen , Lu Meng , Bo Wang , Shi-Lin Zhu

We investigate the enhancement in the D^0\bar{D}^0\pi^0 final state with the mass M=3875.2\pm 0.7^{+0.3}_{-1.6}\pm 0.8 MeV found recently by the Belle Collaboration in the B\to K D^0\bar{D}^0\pi^0 decay and test the possibility that this is…

High Energy Physics - Phenomenology · Physics 2008-11-26 C. Hanhart , Yu. S. Kalashnikova , A. E. Kudryavtsev , A. V. Nefediev

Pion exchange in S-wave between hadrons that are themselves in a relative S-wave is shown to shift energies by hundreds of MeV, leading to deeply bound quasi-molecular states. In the case of charmed mesons $D^*,D_1$ a spectroscopy arises…

High Energy Physics - Phenomenology · Physics 2010-05-12 Frank Close , Clark Downum , Christopher E. Thomas

Several observed states close to the $D\bar{D}^*$ and $D^*_{(s)}\bar{D}^*_{(s)}$ thresholds, as the X(3872) and some XYZ particles can be described in terms of a two-meson molecule. Furthermore, doubly charmed states are also predicted.…

High Energy Physics - Phenomenology · Physics 2013-11-08 R. Molina , H. Nagahiro , A. Hosaka

In this work we present our model that dynamically generates resonances from charmed and light pseudoscalar and vector mesons. The model generates a rich spectrum of charmed and hidden charm scalar and axial resonances, most of them which…

High Energy Physics - Phenomenology · Physics 2009-05-12 D. Gamermann , E. Oset , B. S. Zou

The bound state problem of $D^0\bar{D}^{\ast0}$ ($\bar{D}^0{D}^{\ast0}$) is relevant to the molecular interpretation of the X(3872). We investigated this problem in a chiral quark model by solving the resonating group method equation. We…

High Energy Physics - Phenomenology · Physics 2009-05-07 Yan-Rui Liu , Zong-Ye Zhang

We study the heavy-light mesons within basis light-front quantization. The resulting mass spectra of $D$, $D_s$, $B$, and $B_s$ agree reasonably well with experiments. We also predict states which could be measured in the near future. In…

Nuclear Theory · Physics 2020-07-15 Shuo Tang , Yang Li , Pieter Maris , James P. Vary

Spectroscopy results for Belle and BaBar are reported. A particular focus is put on new results of the X(3872) state with its radiative decays to $J$/$\psi$$\gamma$ and $\psi'$$\gamma$, its decay into $J$/$\psi$3$\pi$ and the search for…

High Energy Physics - Experiment · Physics 2019-08-13 Jens Sören Lange

We measure the dipion mass spectrum in X(3872)--> J/Psi Pi+ Pi- decays using 360 pb-1 of pbar-p collisions at 1.96 TeV collected with the CDF II detector. The spectrum is fit with predictions for odd C-parity (3S1, 1P1, and 3DJ) charmonia…

High Energy Physics - Experiment · Physics 2010-05-12 A. Abulencia , D. Acosta , J. Adelman

We have studied, using double ratio of QCD (spectral) sum rules, the ratio between the masses of $T_{cc}$ and X(3872) assuming that they are respectively described by the $D-{D}^*$ and $D-\bar{D}^*$ molecular currents. We found (within our…

High Energy Physics - Phenomenology · Physics 2015-05-28 J. M. Dias , S. Narison , F. S. Navarra , M. Nielsen , J. -M. Richard

Recently, LHCb reported the radiative-decay ratio ${\cal R}^{\psi\gamma}\equiv {\cal B}[X(3872)\to \psi'\gamma]/{\cal B}[X(3872)\to J/\psi\gamma]=1.67\pm 0.25$ extracted from $B^+\to K^+(J/\psi\gamma, \psi'\gamma)$. This result differs…

High Energy Physics - Phenomenology · Physics 2026-02-24 Satoshi X. Nakamura

Using the LAMP model for nuclear quark structure, we calculate the binding energy and quark structure of a $B$ meson merging with a $D$ meson. The larger-than-nucleon masses of the two heavy quarks allow for a more reliable application of…

Nuclear Theory · Physics 2015-01-07 T. Goldman , Richard R. Silbar

The possible hadronic molecules in $D_s^{(*)+}\Xi_c^{(',*)}$ systems with $J^P=1/2^-,3/2^-$ and $5/2^-$ are investigated with interactions described by light meson exchanges. By varying the cutoff in a phenomenologically reasonable range of…

High Energy Physics - Phenomenology · Physics 2023-09-06 Nijiati Yalikun , Xiang-Kun Dong , Bing-Song Zou

We study heavy hadron spectroscopy near open bottom thresholds. We employ B and B* mesons as effective degrees of freedom near the thresholds, and consider meson exchange potentials between them. All possible composite states which can be…

High Energy Physics - Phenomenology · Physics 2012-07-18 Shunsuke Ohkoda , Yasuhiro Yamaguchi , Shigehiro Yasui , Kazutaka Sudoh , Atsushi Hosaka

If the recently-discovered charmonium state X(3872) is a loosely-bound S-wave molecule of the charm mesons \bar D^0 D^{*0} or \bar D^{*0} D^0, it can be produced in B meson decay by the coalescence of charm mesons. If this coalescence…

High Energy Physics - Phenomenology · Physics 2008-11-26 Eric Braaten , Masaoki Kusunoki , Shmuel Nussinov

We use QCD spectral sum rules to test the nature of the meson X(3872), assumed to be an exotic four-quark (c\bar{c}q\bar{q}) state with J^{PC}=1^{++}. For definiteness, we work with the current proposed recently by Maiani et al [1], at…

High Energy Physics - Phenomenology · Physics 2008-11-26 R. D. Matheus , S. Narison , M. Nielsen , J. M. Richard

We present that the $X(3872)$ could be represented as a dynamically generated state in the extended Friedrichs scheme, in which the ratio of "elementariness" and "compositeness" of the different components in the $X(3872)$ is about…

High Energy Physics - Phenomenology · Physics 2019-12-06 Meng-Ting Yu , Zhi-Yong Zhou , Zhiguang Xiao

We present a quark model calculation of the charmonium spectrum with self energy corrections due to the coupling to the meson-meson continuum. The bare masses used in the calculation are computed within the relativized quark model by…

High Energy Physics - Phenomenology · Physics 2015-10-05 J. Ferretti , G. Galatà , E. Santopinto

It is pointed out that in the decays $X(3872) \to D {\bar D} \gamma$ the possible `molecular' component of the X(3872) should give rise essentially only to a $D^0 {\bar D}^0 \gamma$ final state with a predictable spectrum, and should yield…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. B. Voloshin

The $D^{*}\bar{D}^{*}$ and $B^{*}\bar{B}^{*}$ systems are studied dynamically in the one boson exchange model, where $\pi$, $\eta$, $\sigma$, $\rho$ and $\omega$ exchanges are taken into account. Ten allowed states with low spin parity are…

High Energy Physics - Phenomenology · Physics 2010-04-15 Gui-Jun Ding
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