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Related papers: Penta-quark baryon from the QCD Sum Rule

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We study the pentaquark $uudd\bar s$ with $J=3/2$ and I=1 ($\Theta^{++}$) in the QCD sum rule approach. We derive the QCD sum rules for positive and negative parity states of the pentaquark. The QCD sum rule predicts that there exists…

High Energy Physics - Phenomenology · Physics 2009-11-10 Tetsuo Nishikawa , Yoshiko Kanada-En'yo , Osamu Morimatsu , Yoshihiko Kondo

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

We propose a new approach in QCD sum rules applied for exotic hadrons with a number of quarks, exemplifying the pentaquark Theta^{+} (I=0,J=1/2) in the Borel sum rule. Our approach enables reliable extraction of the pentaquark properties…

High Energy Physics - Phenomenology · Physics 2009-11-11 Toru Kojo , Arata Hayashigaki , Daisuke Jido

The QCD sum rule method is formulated for the strangeness +1 pentaquark baryon with isospin I=0 and spin-parity J^P = 3/2^\pm. The spin-3/2 states are considered to be narrower than the spin-1/2 ones, and thus may provide a natural…

High Energy Physics - Phenomenology · Physics 2014-11-18 P. Gubler , D. Jido , T. Kojo , T. Nishikawa , M. Oka

We construct QCD sum rules for the anti-charmed pentaquark $\Theta_c (3099)$, recently reported at HERA. The sum rules are constructed similarly with the $\Theta^+ (1540)$ sum rules using the anti-charmed analogue of the $\Theta^+$…

High Energy Physics - Phenomenology · Physics 2009-11-10 Hungchong Kim , Su Houng Lee , Yongseok Oh

We perform a QCD sum rule analysis for the pentaquark baryon Theta^+ with the non-interacting $KN$ contribution treated carefully. The coupling of the Theta^+ current to the $KN$ state is evaluated by applying the soft kaon theorem and…

High Energy Physics - Phenomenology · Physics 2007-05-23 Youngshin Kwon , Atsushi Hosaka , Su Houng Lee

It is shown, that the small decay width of $\Theta^+ = uudd\bar{s}$ baryon is suppressed by chirality violation. It is shown that $\Theta^+$ decay width $\Gamma$ is proportional to $\alpha^2_s < 0 | \bar{q} q | 0 >^2$, for any pentaquark…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. G. Oganesian

We estimate the mass of the pentaquark state with QCD sum rules and find that pentaquark states with isospin $I=0, 1, 2$ lie close to each other around $(1.55\pm 0.15)$ GeV. The experimentally observed baryon resonance $\Theta^+ (1540)$…

High Energy Physics - Phenomenology · Physics 2007-05-23 Shi-Lin Zhu

We discuss a possible interpretation for the pentaquark baryon $\Theta^+$ which has an exotic quantum number of strangeness $S = +1$. The role of the pion which modifies the structure of single-particle levels of quarks is examined. When…

High Energy Physics - Phenomenology · Physics 2009-11-10 Atsushi Hosaka

In this article, we study the doubly heavy baryon states and pentaquark states with the QCD sum rules by carrying out the operator product expansion up to the vacuum condensates of dimension $7$ and $13$ respectively in a consistent way. In…

High Energy Physics - Phenomenology · Physics 2018-10-17 Zhi-Gang Wang

The QCD sum rule for the pentaquark $\Theta^+$, first analyzed by Sugiyama, Doi and Oka, is reanalyzed with a phenomenological side that explicitly includes the contribution from the two-particle reducible kaon-nucleon intermediate state.…

High Energy Physics - Phenomenology · Physics 2009-11-10 Su Houng Lee , Hungchong Kim , Youngshin Kwon

The QCD sum rule technique is employed to investigate pentaquark states with strangeness S = +1 and IJ^P = 0,1/2^\pm, 1,1/2^\pm, 0,3/2^\pm, 1,3/2^\pm. Throughout the calculation, emphasis is laid on the establishment of a valid Borel…

High Energy Physics - Phenomenology · Physics 2010-01-15 P. Gubler , D. Jido , T. Kojo , T. Nishikawa , M. Oka

A narrow resonance peak was observed at 1.54 +/- 0.01 GeV as an exotic baryon with strangeness S = +1 in the gamma + n going to K^+ + K^- + n reaction on Carbon. The new state have a width smaller than 0.025 GeV and a Gaussian significance…

High Energy Physics - Experiment · Physics 2007-05-23 Yuji Ohashi

The negative-parity baryons are studied by a novel approach in the QCD sum rule. It is found that the parity of the ground-state nucleon is determined by the sign of the quark condensate. We predict the mass of negative-parity nucleon.

High Energy Physics - Phenomenology · Physics 2009-10-28 D. Jido , N. Kodama , M. Oka

QCD sum rules for positive and negative parity heavy baryons in the heavy quark limit are formulated. We apply the method to $\Lambda$ and $\Sigma$ channels. We include the next-to-leading order corrections in $\alpha_s$-expansion to…

High Energy Physics - Phenomenology · Physics 2024-04-16 Tetsuo Nishikawa , Yoshihiko Kondo , Yoshiko Kanada-En'yo

Recent experimental evidence for the Theta^+(1540) has given rise to much theoretical interest in exotic baryons. The Theta^+ is a baryon that has strangeness S=+1, meaning that it contains an anti-strange quark. Thus it cannot be…

High Energy Physics - Phenomenology · Physics 2007-05-23 Margaret E Wessling

The pion-baryon sigma terms and the strange-quark condensates of the octet and the decuplet baryons are calculated by employing the method of quantum chromodynamics (QCD) sum rules. We evaluate the vacuum-to-vacuum transition matrix…

High Energy Physics - Phenomenology · Physics 2010-04-21 G. Erkol , M. Oka , G. Turan

The masses of the flavor octet and singlet baryons with negative parity and spin 1/2 are calculated using the QCD sum rule. We find that the chiral symmetry breaking vacuum condensates cause the mass splitting of the positive and negative…

High Energy Physics - Phenomenology · Physics 2008-02-03 D. Jido , M. Oka

A strangeness +1 exotic baryon Theta^+ has recently been seen in a number of experiments. We demonstrate that in large N_c QCD the existence of such a state implies the existence of S = +1 partner states with various spins and isospins but…

High Energy Physics - Phenomenology · Physics 2015-06-25 Thomas D. Cohen , Richard F. Lebed

Motivated by the recent discovery of the exotic S=+1 narrow baryon resonance Theta^+ at 1540 MeV, with quark content {uudd sbar}, we conjecture the existence of its anti-charmed analogue Theta_c, with quark content {uudd cbar}, and compute…

High Energy Physics - Phenomenology · Physics 2007-05-23 Marek Karliner , Harry J. Lipkin
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