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Related papers: X(3872), I^G(J^{PC})=0^+(1^{++}), as the \chi_{1c}…

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We construct spectra of decays of the resonance X(3872) with good analytical and unitary properties which allows to define the branching ratio of the X(3872) \to D^{*0}\bar D^0 + c.c. decay studying only one more decay, for example, the…

High Energy Physics - Phenomenology · Physics 2015-10-27 N. N. Achasov , E. V. Rogozina

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

We re-examine the re-scattering mechanism for the X(3872), as a candidate for the 2P charmonium state $\chi_{c1}(2P)$, decaying to $J/\psi\rho(\omega)$ through exchanging $D^{(*)}$ mesons between intermediate states $D(\bar{D})$ and…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ce Meng , Kuang-Ta Chao

In order to understand the structure of the X(3872), the $c \bar c$ charmonium core state coupling to the $D^0 \bar D^{\ast 0}$ and $D^+ D^{\ast -}$ molecular states are studied. The strengths of the couplings between the charmonium state…

High Energy Physics - Phenomenology · Physics 2014-05-07 Makoto Takizawa , Sachiko Takeuchi

The X(3872) resonance is considered as a hadronic molecule, a loosely-bound state of charmed D0 and D*0 mesons, since its mass is very close to the D*0 barD0 threshold. Assuming structure and quantum numbers of X(3872) as (D0 barD*0 - D*0…

High Energy Physics - Phenomenology · Physics 2008-11-26 Yubing Dong , Amand Faessler , Thomas Gutsche , Valery E. Lyubovitskij

We investigate the decays of $B^0 \to K^0 X(3872)$ and $B^+ \to K^+ X(3872)$ based on the picture where the $X(3872)$ resonance is strongly coupled to the $D\bar{D}^* + c.c.$ channel. In addition to the decay mechanism where the $X(3872)$…

High Energy Physics - Phenomenology · Physics 2022-11-29 Hao-Nan Wang , Li-Sheng Geng , Qian Wang , Ju-Jun Xie

The X(3872) with quantum numbers J(PC) = 1(++) is considered as a composite hadronic state comprised of the dominant molecular D(0) D*(0) component and other hadronic pairs - D(+-) D*(-+), Jpsi omega and Jpsi rho. Applying the compositeness…

High Energy Physics - Phenomenology · Physics 2009-07-30 Yubing Dong , Amand Faessler , Thomas Gutsche , Sergey Kovalenko , Valery E. Lyubovitskij

We study the spectral function of the axial-vector charmonium state $\chi_{c1}(2P)$ coupled to $DD^{\ast}$ mesons, by employing a quantum field theoretical approach: a pronounced enhancement close to the $D^{0}% D^{\ast0}$ threshold, to be…

High Energy Physics - Phenomenology · Physics 2020-01-08 Francesco Giacosa , Milena Piotrowska , Susana Coito

It has been argued that the mystery boson X(3872) is a molecule state consisting of primarily D0-D0*bar + D0bar-D*0. In contrast, apparent puzzles and potential difficulties have been pointed out for the charmonium assignment of X(3872). We…

High Energy Physics - Phenomenology · Physics 2008-11-26 Mahiko Suzuki

Using chiral effective field theory, we predict that there must be isovector charmonium-like $D\bar D^*$ hadronic molecules with $J^{PC}=1^{++}$ denoted as $W_{c1}$. The inputs are the properties of the $X(3872)$, including its mass and the…

High Energy Physics - Phenomenology · Physics 2024-08-29 Zhen-Hua Zhang , Teng Ji , Xiang-Kun Dong , Feng-Kun Guo , Christoph Hanhart , Ulf-G. Meißner , Akaki Rusetsky

Starting from a molecular picture for the X(3872) resonance, this state and its J^{PC}=2++ HQSS partner [X2(4012)] are analyzed within a model which incorporates possible mixings with 2P charmonium states. Since it is reasonable to expect…

High Energy Physics - Phenomenology · Physics 2016-11-23 E. Cincioglu , J. Nieves , A. Ozpineci , A. U. Yilmazer

The 1D2 charmonium assignment for the X(3872) meson is considered, as prompted by a recent result from the BABAR Collaboration, favouring 2-+ quantum numbers for the X. It is shown that established properties of the X(3872) are in a drastic…

High Energy Physics - Phenomenology · Physics 2010-12-23 Yu. S. Kalashnikova , A. V. Nefediev

The X(3872) radiative decay is discussed by employing a two-meson multichannel model with the charmonium components, which explains many of the other observed features of X(3872). We have found that the ratio of the branching fractions of…

High Energy Physics - Phenomenology · Physics 2017-08-02 Sachiko Takeuchi , Makoto Takizawa , Kiyotaka Shimizu

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

Since the discovery of X(3872), its structure has been in ceaseless dispute. The data of $X(3872)\rightarrow \pi^+\pi^-\pi^0 J/\psi$ suggest that X(3872) may be a high-spin charmonium-like of $2^{-+}$. In terms of the light front quark…

High Energy Physics - Phenomenology · Physics 2012-01-04 Hong-Wei Ke , Xue-Qian Li

By describing the $X(3872)$ using the extended Friedrichs scheme, in which $D\bar D^*$ is the dominant component, we calculate the decay rates of the $X(3872)$ to $\pi^0$ and a $P$-wave charmonium $\chi_{cJ}$ state with $J=0,1$, or $2$, and…

High Energy Physics - Phenomenology · Physics 2020-01-07 Zhi-Yong Zhou , Meng-Ting Yu , Zhiguang Xiao

The $X(3872)$, as the first and the most crucial member in the exotic charmoniumlike $XYZ$ family, has been studied for a long time. However, its dynamical origin, whether stemming from a $D\bar{D}^*$ hadronic molecule or the first excited…

High Energy Physics - Phenomenology · Physics 2025-06-10 Jun-Zhang Wang , Zi-Yang Lin , Yan-Ke Chen , Lu Meng , Shi-Lin Zhu

Enfant terrible of charmonium spectroscopy, the resonance $X(3872)$, generated a stream of interpretations and ushered in a new exotic $XYZ$ spectroscopy. In th meantime, many (if not all) characteristics of $X(3872)$ are rather ambiguous.…

High Energy Physics - Phenomenology · Physics 2014-10-31 N. N. Achasov , E. V. Rogozina

Radiative decays of X(3872) with $J^{PC}=1^{++}$ are studied in the coupled-channel approach, where the $c\bar c$ states are described by relativistic string Hamiltonian, while for the decay channels $DD^*$ a string breaking mechanism is…

High Energy Physics - Phenomenology · Physics 2014-01-29 A. M. Badalian , V. D. Orlovsky , Yu. A. Simonov , B. L. G. Bakker

We discuss the possible interpretation of X(3872) as a $DD^{\ast}$ hadronic molecule with $J^{PC} = 2^{-+}$. Using the phenomenological Lagrangian approach, we studied its radiative and strong decay properties. We find that our model with…

High Energy Physics - Phenomenology · Physics 2015-05-20 Masayasu Harada , Yong-Liang Ma
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