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Related papers: Baryonium X(1835)

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The relativistic six-quark equations including the $u$, $d$ quarks and antiquarks are found. The nonstrange baryonia $B \bar B$ are constructed without the mixing of the quarks and antiquarks. The relativistic six-quark amplitudes of the…

High Energy Physics - Phenomenology · Physics 2011-07-15 S. M. Gerasyuta , E. E. Matskevich

The relativistic six-quark equations are found in the framework of the dispersion relation technique. The strange baryonia are constructed without the mixing of the quarks and antiquarks. The relativistic six-quark amplitudes of the strange…

High Energy Physics - Phenomenology · Physics 2020-08-26 S. M. Gerasyuta , E. E. Matskevich

The relativistic six-quark equations are found in the framework of the dispersion relation technique. The charmed baryonia $B\bar B$ are constructed without the mixing of the quarks and antiquarks. The relativistic six-quark amplitudes of…

High Energy Physics - Phenomenology · Physics 2012-04-02 S. M. Gerasyuta , E. E. Matskevich

The relativistic six-quark amplitudes of the nonstrange baryonia with the open charm are calculated. The poles of these amplitudes determine the masses of baryonia. 9 masses of baryonia are predicted.

High Energy Physics - Phenomenology · Physics 2012-12-04 S. M. Gerasyuta , E. E. Matskevich

The relativistic six-quark equations are constructed in the framework of the dispersion relation technique. The relativistic six-quark amplitudes of dibaryons including the light $u$, $d$ and heavy $c$, $b$ quarks are calculated. The…

High Energy Physics - Phenomenology · Physics 2015-05-30 S. M. Gerasyuta , E. E. Matskevich

The relativistic six-quark equations are found in the framework of the dispersion relation technique. The approximate solutions of these equations using the method based on the extraction of leading singularities of the heavy hexaquark…

High Energy Physics - Phenomenology · Physics 2015-05-28 S. M. Gerasyuta , E. E. Matskevich

The relativistic six-quark equations are found in the framework of the dispersion relation technique. The approximate solutions of these equations using the method based on the extraction of leading singularities of the amplitudes are…

High Energy Physics - Phenomenology · Physics 2014-11-20 S. M. Gerasyuta , E. E. Matskevich

The relativistic five-quark equations are found in the framework of the dispersion relation technique.The five-quark amplitudes for the low-lying exotic baryons including the up and down quarks are calculated.The poles of the five-quark…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. M. Gerasyuta , V. I. Kochkin

The masses of the yet undiscovered baryons containing single $c$ or $b$ quarks are estimated from the known masses using the following rules: equal distances in mass between the isomultiplets forming sextets, equal mass differences between…

High Energy Physics - Phenomenology · Physics 2007-05-23 Agnieszka Zalewska , Kacper Zalewski

Simple and plausible rules are used to correlate the masses of the ground-state baryons containing single heavy ($b$ or $c$) quarks. A comparison with the experimental data shows that the observed mass difference between the $\Sigma_b$ and…

High Energy Physics - Phenomenology · Physics 2008-02-03 Agnieszka Zalewska , Kacper Zalewski

The masses of the ground state heavy baryons consisting of two light (u,d,s) and one heavy (c,b) quarks are calculated in the heavy-quark--light-diquark approximation within the constituent quark model. The light quarks, forming the…

High Energy Physics - Phenomenology · Physics 2009-11-11 D. Ebert , R. N. Faustov , V. O. Galkin

About 120 baryons and baryon resonances are known, from the abundant nucleon with $u$ and $d$ light-quark constituents up to the recently discovered $\Omega_b^-=bss$, and the $\Xi_b^-=bsd$ which contains one quark of each generation. In…

High Energy Physics - Phenomenology · Physics 2010-11-11 Eberhard Klempt , Jean-Marc Richard

The relativistic five-quark equations are found in the framework of the dispersion relation technique. The five-quark amplitude for the N(1688) resonance including u-, d- quarks is calculated. The pole of this amplitude determines the mass…

High Energy Physics - Phenomenology · Physics 2007-07-05 S. M. Gerasyuta , V. I. Kochkin

The masses of negative parity $(70,1^-)$ bottom nonstrange baryons are calculated in the relativistic quark model. The relativistic three-quark equations of the $(70,1^-)$ bottom baryon multiplet are derived in the framework of the…

High Energy Physics - Phenomenology · Physics 2016-04-18 S. M. Gerasyuta , E. E. Matskevich

Supposing quark--diquark structure of baryons, we look for systematics of baryons composed of light quarks ($q=u,d$). We systematize baryons using the notion of two diquarks: (i) axial--vector state, $D^{1}_{1}$, with the spin $S_D=1$ and…

High Energy Physics - Phenomenology · Physics 2014-11-20 A. V. Anisovich , V. V. Anisovich , M. A. Matveev , V. A. Nikonov , A. V. Sarantsev , T. O. Vulfs

The mass spectra of the excited heavy baryons consisting of two light (u,d,s) and one heavy (c,b) quarks are calculated in the heavy-quark--light-diquark approximation within the constituent quark model. The light quarks, forming the…

High Energy Physics - Phenomenology · Physics 2008-11-26 D. Ebert , R. N. Faustov , V. O. Galkin

The Feynman-Hellmann theorem and semiempirical mass formulas are used to predict the masses of baryons containing one or two heavy quarks. In particular, the mass of the $\Lambda_b$ is predicted to be $5620 \pm 40$ MeV, a value consistent…

High Energy Physics - Phenomenology · Physics 2016-09-01 R. Roncaglia , D. B. Lichtenberg , E. Predazzi

We show that $\omega_B$ or $\omega_{\bar B}$, the squared baryon or antibaryon number fluctuation per baryon or antibaryon, is a possible signature for the quark-gluon plasma that is expected to be created in relativistic heavy ion…

Nuclear Theory · Physics 2009-11-07 Zi-wei Lin , C. M. Ko

Properties of a hypothetical baryonium with the quark content ($uds\ov{u}\ov{d}\ov{s}$) are discussed. The MIT bag model predicts its mass to be unexpectedly low, approximately 1210 MeV. Possible hadronic decay modes of this state are…

High Energy Physics - Phenomenology · Physics 2009-11-10 I. N. Mishustin , L. M. Satarov , D. Strottman , W. Greiner

Masses of heavy baryons and tetraquarks are calculated in the relativistic quark model using the heavy-quark--light-diquark and diquark-antidiquark approximations, respectively.

High Energy Physics - Phenomenology · Physics 2007-12-05 D. Ebert , R. N. Faustov , V. O. Galkin
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