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Related papers: Small size pentaquark in QCD sum rule approach

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In this article, we tentatively assign the $P_c(4312)$ to be the $\bar{D}\Sigma_c$ pentaquark molecular state with the spin-parity $J^P={\frac{1}{2}}^-$, and discuss the factorizable and non-factorizable contributions in the two-point QCD…

High Energy Physics - Phenomenology · Physics 2020-09-28 Zhi-Gang Wang , Xu Wang

The QCD up- and down-quark masses are determined from an optimized QCD Finite Energy Sum Rule (FESR) involving the correlator of axial-vector current divergences. In the QCD sector this correlator is known to five loop order in perturbative…

High Energy Physics - Phenomenology · Physics 2019-02-20 C. A. Dominguez , A. Mes , K. Schilcher

We use diquark-antidiquark currents to investigate the masses and partial decay widths of the recently observed mesons $D_{sJ}^{+}(2317)$, $D_0^{*0}(2308)$ and X(3872), considered as four-quark states, in a QCD sum rule approach. In…

High Energy Physics - Phenomenology · Physics 2008-11-26 Marina Nielsen

To better understand the nature and internal structure of the exotic states discovered by many collaborations, more information on their electromagnetic properties and their strong and weak interactions with other hadrons is needed. The…

High Energy Physics - Phenomenology · Physics 2017-05-31 K. Azizi , Y. Sarac , H. Sundu

In this article, we take the point of view that Y(2175) be a tetraquark state which consists of color octet constituents, and calculate its mass and decay constant within the framework of the QCD sum rule approach. We release standard…

High Energy Physics - Phenomenology · Physics 2008-11-26 Zhi-Gang Wang

In multiquark correlator analyses with 1/Nc classifications, it is possible to separate the scattering background and to justify the factorization of condensates, which allows us to achieve an isolated peak saturation in the QCD sum rules…

High Energy Physics - Phenomenology · Physics 2008-09-12 Toru Kojo , Daisuke Jido

In this article, we construct the charmed-diquark-charmed-diquark-charmed-diquark type current to study the axialvector triply-charmed hexaquark state with the QCD sum rules in details. In calculations, we take the energy scale formula…

High Energy Physics - Phenomenology · Physics 2020-06-08 Zhi-Gang Wang

We study the $\sigma$ meson in QCD sum rules using a two quark interpolating field with derivatives. In the constituent quark model, the $\sigma$ meson is composed of a quark and an antiquark in the relative p-wave state and is thus…

High Energy Physics - Phenomenology · Physics 2015-05-13 Su Houng Lee , Kenji Morita , Kazuaki Ohnishi

We use a constituent model to analyze the stability of pentaquark $\bar Q qqqq$ configurations with a heavy antiquark $\bar c$ or $\bar b$, and four light quarks $uuds$, $ddsu$ or $ssud$. The interplay between chromoelectric and…

High Energy Physics - Phenomenology · Physics 2019-01-29 J. -M. Richard , A. Valcarce , J. Vijande

We study a QCD sum rule analysis for an exotic tetraquark ud bar[s] bar[s] of J^P=0^+ and I = 1. We construct q q bar[q] bar[q] currents in a local product form and find that there are five independent currents for this channel. Due to high…

High Energy Physics - Phenomenology · Physics 2009-09-29 Hua-Xing Chen , Atsushi Hosaka , Shi-Lin Zhu

We review the current status of the theoretical pentaquark search from the direct QCD calculation. The works from the QCD sum rule and the lattice QCD in the literature are carefully examined. The importance of the framework which can…

High Energy Physics - Phenomenology · Physics 2008-11-26 Takumi Doi

The consistency of effective models with QCD is investigated through the use of the QCD sum rule. Taking the potential model for the heavy quark system, we apply the method to two phenomenologically successful parameter sets, and obtain the…

High Energy Physics - Phenomenology · Physics 2007-05-23 T. Matsuki , K. Yazaki

We study pentaquark $\Theta^{+} (I=0,J=1/2)$ in the QCD sum rules emphasizing that we can not extract any properties of the pentaquark outside of the Borel window. To find the appropriate Borel window, we prepare a favorable set up of the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Toru Kojo , Daisuke Jido , Arata Hayashigaki

After constructing the possible $J^P=0^-, 0^+, 1^-$ and $1^+$ $QQ\bar{q}\bar{q}$ tetraquark interpolating currents in a systematic way, we investigate the two-point correlation functions and extract the corresponding masses with the QCD sum…

High Energy Physics - Phenomenology · Physics 2013-01-10 Meng-Lin Du , Wei Chen , Xiao-Lin Chen , Shi-Lin Zhu

In this work, we chose three molecular and three diquark-antidiquark currents with the quark content $c\bar{c}s\bar{s}$ and $J^{PC}=0^{++},1^{++},2^{++}$, and estimated the masses and the meson coupling constants of the ground states…

High Energy Physics - Phenomenology · Physics 2019-03-14 Arzu Turkan , Huseyin Dag

By assuming SU(6)_cs symmetry for pentaquark decays one finds a selection rule, which strongly reduces the number of states able to decay into a baryon and a meson final state and allows an intriguing identification for the Theta^+ particle…

High Energy Physics - Phenomenology · Physics 2010-11-05 F. Buccella

We discuss a sum rule satisfied by the correlation function of two particles with small relative momenta. The sum rule, which results from the completeness condition of the quantum states of the two particles, is first derived and then we…

Nuclear Theory · Physics 2009-11-10 Radoslaw Maj , Stanislaw Mrowczynski

There are experimental evidences for the existence of narrow states $\Theta^+$ and $\Theta_c$ with the same quantum numbers of $uudd\bar s$ and $uudd\bar c$ pentaquarks and also $NK^{(*)}$ and $ND^{(*)}$ molecular states. Their masses…

High Energy Physics - Phenomenology · Physics 2014-11-18 Xiao-Gang He , Xue-Qian Li , Xiang Liu , Xiao-Qian Zeng

In the QCD Sum Rule determination of $m_s$ using the two-point correlator of divergences of $\Delta S=1$ vector currents, the final uncertainty on $m_s$ is mainly due to the hadronic spectral function. Using a specific parameterization…

High Energy Physics - Phenomenology · Physics 2008-11-26 P. Colangelo , F. De Fazio , G. Nardulli , N. Paver

We identify essential differences between the pentaquark and chiral soliton models of \10bar$_5$ and {\bf 8}$_5$ pentaquarks and conventional {\bf 8}$_3$ states, which are experimentally measurable. We show how the decays of $\Xi_5$ states…

High Energy Physics - Phenomenology · Physics 2009-11-10 F. E. Close , J. J. Dudek
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