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Journal articles on the topic 'Octet decuplet baryons'

Author: Grafiati

Published: 4 June 2021

Last updated: 28 January 2023

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1

OSET, E., S. SARKAR, M. J. VICENTE VACAS, et al. "DYNAMICALLY GENERATED RESONANCES IN THE CHIRAL UNITARY APPROACH TO MESON BARYON INTERACTION." International Journal of Modern Physics A 20, no. 08n09 (2005): 1619–26. http://dx.doi.org/10.1142/s0217751x05023086.

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In this talk we report on the use of a chiral unitary approach for the interaction of the octets of meson and baryon and the octet of mesons with the decuplet of baryons. Two octets of Jπ=1/2- baryon states and a singlet are generated dynamically in the first case, resulting in the case of strangeness S=-1 in two poles of the scattering matrix close to the nominal Λ(1405) resonance. In the second case many resonances are also generated, among them an exotic baryon with S=1 corresponding to a ΔK resonance. We make suggestions of experiments which could show evidence for the existence of these s

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2

Ren, Xiu-Lei, Lisheng Geng, Jie Meng, and Hiroshi Toki. "Lowest-lying octet baryon masses up to $\mathcal{O}(p^4)$ in covariant baryon chiral perturbation theory." International Journal of Modern Physics: Conference Series 29 (January 2014): 1460215. http://dx.doi.org/10.1142/s2010194514602154.

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In this talk, we report on a systematic study of the lowest-lying octet baryon masses in covariant baryon chiral perturbation theory with the extended-on-mass-shell renormalization scheme up to [Formula: see text]. By adjusting the low-energy constants, a reasonable description of the nf = 2 + 1 lattice results is achieved with χ2/d.o.f. about 1. It confirms that the various lattice simulations are consistent with each other. We also find that the virtual decuplet effects on the baryon masses cannot be disentangled from those of the virtual octet baryons and the tree level diagrams.

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3

WANG, FAN, JIA-LUN PING, HOU-RONG PANG, and T. GOLDMAN. "WHICH CONSTITUENT QUARK MODEL IS BETTER?" Modern Physics Letters A 18, no. 02n06 (2003): 356–61. http://dx.doi.org/10.1142/s021773230301048x.

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A comparative study has heen done by calculating the effective baryon-baryon interactions of the 64 lowest channels consisting of octet and decuplet baryons with three constituent quark models: the extended quark gluon exchange model, the Goldstone boson exchange model and the quark gluon meson exchange hybrid model. We find that these three models give similar results for 44 channels. Further tests of these models are discussed.

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4

PANDA, A. R., K. C. ROY, and R. K. SAHOO. "VACUUM STRUCTURE, CHIRAL SYMMETRY BREAKING AND STATIC PROPERTIES OF OCTET AND DECUPLET BARYONS." International Journal of Modern Physics E 05, no. 04 (1996): 649–67. http://dx.doi.org/10.1142/s0218301396000360.

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The static properties of the octet and decuplet baryons are considered within the framework of a quark model of hadrons where the chiral symmetry is broken dynamically through a nontrivial vacuum structure. The pion and kaon being treated consistently within the model yield to the constituent quark wave function approximately same as the wave functions from the gap equations and thus determine consequently the constituent quark field operators. The model was successfully used earlier to study some hadronic phenomena and here also it estimates the static properties of the octet and decuplet bar

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5

FARIA DA VEIGA, PAULO A., and MICHAEL O'CARROLL. "EXACT DYNAMICAL EIGHTFOLD WAY BARYON SPECTRUM AND CONFINEMENT IN STRONGLY COUPLED LATTICE QCD." International Journal of Modern Physics A 24, no. 16n17 (2009): 3053–72. http://dx.doi.org/10.1142/s0217751x09043183.

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We obtain from the quark–gluon dynamics the eightfold way baryon spectrum exactly in an imaginary time functional integral formulation of 3+1 lattice QCD with Wilson's action in the strong coupling regime (small hopping parameter 0 < κ ≪ 1 and much smaller plaquette coupling [Formula: see text]). The model has SU(3)c local gauge and global SU(3)f flavor symmetries. A decoupling of the hyperplane method naturally unveils the form of the baryon composite fields. In the subspace of the physical Hilbert space of vectors with an odd number of quarks, the baryons are associated with isolated disp

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6

Alkofer, Reinhard, Christian S. Fischer, and Hèlios Sanchis-Alepuz. "Electromagnetic transition form factors of baryons in a relativistic Faddeev approach." EPJ Web of Conferences 181 (2018): 01013. http://dx.doi.org/10.1051/epjconf/201818101013.

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The covariant Faddeev approach which describes baryons as relativistic three-quark bound states and is based on the Dyson-Schwinger and Bethe-Salpeter equations of QCD is briefly reviewed. All elements, including especially the baryons’ three-body-wave-functions, the quark propagators and the dressed quark-photon vertex, are calculated from a well-established approximation for the quark-gluon interaction. Selected previous results of this approach for the spectrum and elastic electromagnetic form factors of ground-state baryons and resonances are reported. The main focus of this talk is a pres

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7

ZHENG, W., and H. R. PANG. "MOMENTUM-SPACE FADDEEV CALCULATIONS FOR GROUND-STATE TRIPLY AND DOUBLY HEAVY BARYONS IN THE CONSTITUENT QUARK MODEL." Modern Physics Letters A 25, no. 24 (2010): 2077–88. http://dx.doi.org/10.1142/s0217732310032962.

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In the framework of constituent quark model, mass spectra of the ground-state baryons consisting of three or two heavy (b or c) and one light (u, d or s) quarks are calculated by solving three-body Faddeev equations. The results imply that, it is possible to obtain a unified model to describe heavy baryons spectra, as well as meson and SU(3) octet and decuplet baryon spectra. We find that, when taking into account the relativistic correction quark–diquark approximation and three-body Faddeev approach tend to give similar predictions for heavy–light systems. We also study the spin splitting of

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8

REN, XIU-LEI, LISHENG GENG, JIE MENG, and HIROSHI TOKI. "LOWEST-LYING OCTET BARYON MASSES IN COVARIANT BARYON CHIRAL PERTURBATION THEORY." International Journal of Modern Physics: Conference Series 26 (January 2014): 1460068. http://dx.doi.org/10.1142/s2010194514600684.

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We report on a systematic study of the ground-state octet baryon masses in the covariant baryon chiral perturbation theory with the extended-on-mass-shell renormalization scheme up to next-to-next-to-next-to-leading order, taking into account the contributions of the virtual decuplet baryons. A reasonable description of the lattice results is achieved by fitting simultaneously all the publicly availablenf = 2 + 1lattice QCD data. It confirms that the various lattice simulations are consistent with each other. We stress that a self-consistent treatment of finite-volume corrections is important

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9

Sharma, Neetika, and Harleen Dahiya. "Charge Radii and Quadrupole Moments of the Low-Lying Baryons in the Chiral Constituent Quark Model." Advances in High Energy Physics 2013 (2013): 1–17. http://dx.doi.org/10.1155/2013/756847.

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The chiral constituent quark model (χCQM) with general parameterization method (GPM) has been formulated to calculate the charge radii of the spin1/2+octet and3/2+decuplet baryons and quadrupole moments of the spin3/2+decuplet baryons and spin3/2+→1/2+transitions. The implications of such a model have been investigated in detail for the effects of symmetry breaking and GPM parameters pertaining to the one-, two-, and three-quark contributions. Our results are not only comparable with the latest experimental studies but also agree with other phenomenological models. It is found that theχCQM is

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10

Morpurgo, G. "New mass formula for octet and decuplet baryons." Physical Review Letters 68, no. 2 (1992): 139–41. http://dx.doi.org/10.1103/physrevlett.68.139.

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11

Hanhart, C., and S. Krewald. "Faddeev approach to the octet and decuplet baryons." Physics Letters B 344, no. 1-4 (1995): 55–60. http://dx.doi.org/10.1016/0370-2693(94)01532-h.

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12

INOUE, T., V. E. LYUBOVITSKIJ, TH GUTSCHE, and AMAND FAESSLER. "GROUND-STATE BARYON MASSES IN THE PERTURBATIVE CHIRAL QUARK MODEL." International Journal of Modern Physics E 15, no. 01 (2006): 121–42. http://dx.doi.org/10.1142/s0218301306003862.

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The mass differences of the flavor octet and decuplet ground-state baryons are studied in the perturbative chiral quark model. We present a way to understand the nontrivial spin- and flavor-dependent mass differences, whereby both pseudoscalar mesons and gluons play a significant role.

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13

Chen, Chen. "On SU(3)F positive-parity octet and decuplet baryons." EPJ Web of Conferences 241 (2020): 02002. http://dx.doi.org/10.1051/epjconf/202024102002.

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A continuum approach to the three valence-quark bound-state problem in quantum field theory, employing parametrisations of the necessary kernel elements, is used to compute the spectrum and Poincarö- covariant wave functions for all flavour-SU(3) octet and decuplet baryons and their first positive-parity ex citations. Such analyses predict the existence of nonpointlike, dynamical quark-quark (diquark) correlations within all baryons; and a uniformly sound description of the systems studied is obtained by retaining flavour- antitriplet-scalar and flavour-sextet-pseudovector diquarks. The analys

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14

Morpurgo, G. "Electromagnetic mass differences of the octet and decuplet baryons." Physical Review D 45, no. 5 (1992): 1686–92. http://dx.doi.org/10.1103/physrevd.45.1686.

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15

Choi, Ki-Seok, and Willibald Plessas. "Electromagnetic and Axial Form Factors of Octet and Decuplet Baryons." Few-Body Systems 54, no. 7-10 (2013): 1055–58. http://dx.doi.org/10.1007/s00601-012-0577-x.

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16

Aliev, T. M., K. Azizi, and M. Savcı. "Strong transitions of decuplet to octet baryons and pseudoscalar mesons." Nuclear Physics A 847, no. 1-2 (2010): 101–17. http://dx.doi.org/10.1016/j.nuclphysa.2010.06.013.

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17

Wong, S. M. H. "Color octet contribution in exclusive P-wave charmonium decay into octet and decuplet baryons." European Physical Journal C 14, no. 4 (2000): 643–71. http://dx.doi.org/10.1007/s100520000376.

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18

Aliev, T. M., and A. Ozpineci. "Radiative decays of decuplet to octet baryons in light cone QCD." Nuclear Physics B 732, no. 1-2 (2006): 291–320. http://dx.doi.org/10.1016/j.nuclphysb.2005.07.038.

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19

Carone, Christopher, and Howard Georgi. "Nonrealitivistic chiral expansion and nonleptonic decays of octet and decuplet baryons." Nuclear Physics B 375, no. 2 (1992): 243–62. http://dx.doi.org/10.1016/0550-3213(92)90031-6.

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20

Oettel, M., G. Hellstern, R. Alkofer, and H. Reinhardt. "Octet and decuplet baryons in a covariant and confining diquark-quark model." Physical Review C 58, no. 4 (1998): 2459–77. http://dx.doi.org/10.1103/physrevc.58.2459.

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21

Alkofer, R., S. Ahlig, C. Fischer, M. Oettel, and H. Reinhardt. "Octet and decuplet baryons in a confining and covariant diquark-quark model." Nuclear Physics A 663-664 (January 2000): 683c—686c. http://dx.doi.org/10.1016/s0375-9474(99)00721-6.

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22

SHARMA, NEETIKA, and HARLEEN DAHIYA. "Charge radii of octet and decuplet baryons in chiral constituent quark model." Pramana 81, no. 3 (2013): 449–65. http://dx.doi.org/10.1007/s12043-013-0575-7.

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23

FURUICHI, MIKITO, KIYOTAKA SHIMIZU, and Sachiko Takeuchi. "DESCRIPTION OF SU(3) S-WAVE AND P-WAVE BARYONS." Modern Physics Letters A 18, no. 02n06 (2003): 362–65. http://dx.doi.org/10.1142/s0217732303010491.

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We investigate the structure of the SU(3) octet and decuplet baryons employing a constituent chiral quark model. We study the ground, s-wave and p-wave excited states of the three-quark system with many range gaussian bases. The method, which we employ here, is shown to work quite well in describing the structure of the SU(3) s-wave and p-wave baryons. It is found that the mass differences between positive and negative parity states are well reproduced. It is also found that the pseudoscalar (ps) meson exchange potential plays a very important role in describing the mass of the nucleon resonan

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24

Wakamatsu, M., and N. Kaya. "Magnetic Moments of Octet and Decuplet Baryons in the SU(3) Chiral Quark Soliton Model." Progress of Theoretical Physics 95, no. 4 (1996): 767–78. http://dx.doi.org/10.1143/ptp.95.767.

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25

Buck, A., and H. Reinhardt. "Octet and decuplet baryons in the hadronized Nambu-Jona-Lasinio model with proper spin projection." Physics Letters B 356, no. 2-3 (1995): 168–74. http://dx.doi.org/10.1016/0370-2693(95)00847-e.

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26

Polanco-Euán, E. N., G. Sánchez-Colón, and V. Gupta. "Dibaryon octet strong decay coupling constants sum rules with first-order SU(3) symmetry breaking." Modern Physics Letters A 32, no. 07 (2017): 1750041. http://dx.doi.org/10.1142/s0217732317500419.

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The SU(3) octet states with baryon number B = 2, hexaquark dibaryons, are considered. We extend previous work and determine strong decay coupling constants sum rules with first-order SU(3) symmetry breaking for dibaryon octet into two ordinary baryon octets and into a baryon octet plus a baryon decuplet. Possibilities for the experimental observation of multibaryon and anti-multibaryon states are pointed out.

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27

Cárcamo Hernández, Antonio E. "The Gell-Mann-Okubo and Coleman-Glashow relations for octet and decuplet baryons in the SUq(3) quantum algebra." Journal of Mathematical Physics 47, no. 7 (2006): 073509. http://dx.doi.org/10.1063/1.2218672.

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28

Sánchez-Colón, G., E. N. Polanco-Euán, and C. E. López-Fortín. "Sum rules for strong decays of 10 and 27 dibaryon multiplets in broken SU(3) symmetry." International Journal of Modern Physics A 33, no. 29 (2018): 1850173. http://dx.doi.org/10.1142/s0217751x18501737.

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10 and 27 SU(3) multiplets of hexaquarks states with baryon number [Formula: see text], known as dibaryons, are considered. Previous analyses are complemented and sum rules for strong decay amplitudes with SU(3) symmetry violation up to the first order are determined for the 10 and 27 dibaryon multiplets into a baryon octet plus a baryon decuplet and for the dibaryon 27 into two baryon octets.

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29

Dahiya, Harleen. "Transition magnetic moments of ${J}^{P}={\frac{3}{2}}^{+}$ decuplet to ${J}^{P}={\frac{1}{2}}^{+}$ octet baryons in the chiral constituent quark model." Chinese Physics C 42, no. 9 (2018): 093102. http://dx.doi.org/10.1088/1674-1137/42/9/093102.

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30

VICENTE VACAS, M. J., E. OSET, and SOURAV SARKAR. "BARYONIC RESONANCES FROM BARYON DECUPLET-MESON OCTET INTERACTION." International Journal of Modern Physics A 20, no. 08n09 (2005): 1826–29. http://dx.doi.org/10.1142/s0217751x05023414.

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The s-wave interactions of the baryon decuplet with the octet of pseudoscalar mesons is studied in a unitarized coupled channel approach. We obtain a fair agreement for mass and width of several [Formula: see text] resonances. In particular, the Ξ(1820), the Λ(1520) and the Σ(1670) states are well reproduced. Other resonances are predicted and also the couplings of the observed resonances to the various channels are evaluated.

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31

Sarkar, Sourav, E. Oset, and M. J. Vicente Vacas. "Baryonic resonances from baryon decuplet-meson octet interaction." Nuclear Physics A 750, no. 2-4 (2005): 294–323. http://dx.doi.org/10.1016/j.nuclphysa.2005.01.006.

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32

Roy, T. "A note on mass formula and Quark structure." International Journal of Mathematics and Mathematical Sciences 11, no. 3 (1988): 613–14. http://dx.doi.org/10.1155/s0161171288000730.

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33

Ghosh, Rismita. "Magnetic Moments of The Baryon Anti-decuplet and Octet Pentaquark States." JOURNAL OF ADVANCES IN PHYSICS 7, no. 1 (2015): 1309–15. http://dx.doi.org/10.24297/jap.v7i1.1734.

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The magnetic moments of the baryon anti-decuplet and octet-pentaquark states have been estimated in the framework of diquark-diquark-antiquark configuration using the composite fermion (CF) model of diquark suggested by us. The masses of the diquark have been estimated in the CF approach and subsequently used to estimate the magnetic moments of baryon antidecuplet and octet penta quark states. Results are compared with existing predictions.

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34

Leinweber, Derek B., Terrence Draper, and R. M. Woloshyn. "Baryon octet to decuplet electromagnetic transitions." Physical Review D 48, no. 5 (1993): 2230–49. http://dx.doi.org/10.1103/physrevd.48.2230.

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35

Sarkar, Sourav, E. Oset, and M. J. Vicente Vacas. "Baryonic Resonances from Baryon Decuplet-Meson Octet Interactions and the Exotic Resonance , ,." Nuclear Physics A 755 (June 2005): 665–68. http://dx.doi.org/10.1016/j.nuclphysa.2005.03.091.

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36

Chemtob, Marc. "Skyrme model of baryon octet and decuplet." Nuclear Physics B 256 (January 1985): 600–608. http://dx.doi.org/10.1016/0550-3213(85)90409-2.

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37

Cutkosky, R. E. "Isospin splitting in the baryon octet and decuplet." Physical Review C 47, no. 1 (1993): 367–71. http://dx.doi.org/10.1103/physrevc.47.367.

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38

SAHU, SARIRA. "BARYON MASSES IN COLOR DIELECTRIC MODEL." International Journal of Modern Physics E 03, no. 02 (1994): 801–10. http://dx.doi.org/10.1142/s0218301394000231.

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The non-scaling version of the Color Dielectric Model is used to calculate the SU(3) baryon octet and decuplet masses with the mean-field approximation and momentum projection method of Peierls and Yoccoz. Quantum mechanical treatment of the dielectric field is done by taking the coherent state approximation. For suitable set of parameters it is observed that the masses in the momentum projection method are in better agreement with the observed values than those of the mean-field ones.

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39

STROBEL, GEORGE L. "BARYON MAGNETIC MOMENTS AND SPIN DEPENDENT QUARK FORCES." International Journal of Modern Physics E 11, no. 01 (2002): 71–81. http://dx.doi.org/10.1142/s0218301302000697.

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The J=3/2 Δ, J=1/2 nucleon mass difference shows that quark energies can be spin dependent. It is natural to expect that quark wave functions also depend on spin. In the octet, such spin dependent forces lead to different wave functions for quarks with spin parallel or antiparallel to the nucleon spin. A two component Dirac equation wave function is used for the quarks assuming small current quark masses for the u and d quarks. Then, the neutron/proton magnetic moment ratio, the nucleon axial charge, and the spin content of the nucleon can all be simultaneously fit assuming isospin invariance

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40

Ha, Phuoc. "A parametrization of the baryon octet and decuplet masses." Journal of Physics G: Nuclear and Particle Physics 35, no. 7 (2008): 075006. http://dx.doi.org/10.1088/0954-3899/35/7/075006.

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41

Sarkar, Sourav, Bao-Xi Sun, E. Oset, and M. J. Vicente Vacas. "Dynamically generated resonances from the vector octet-baryon decuplet interaction." European Physical Journal A 44, no. 3 (2010): 431–43. http://dx.doi.org/10.1140/epja/i2010-10956-4.

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42

Bao-Xi, Sun, Sourav Sarkar, E. Oset та M. J. Vicente Vacas. "Dynamically generated resonances from the vector octet-baryon decuplet interaction and their radiative decays into γ-baryon decuplet". Chinese Physics C 33, № 12 (2009): 1366–68. http://dx.doi.org/10.1088/1674-1137/33/12/056.

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43

Sarkar, Sourav, E. Oset, and M. J. Vicente-Vacas. "Erratum to: “Baryonic resonances from baryon decuplet-meson octet interaction” [Nucl. Phys. A 750 (2005) 294]." Nuclear Physics A 780, no. 1-2 (2006): 90. http://dx.doi.org/10.1016/j.nuclphysa.2006.09.019.

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44

Li, Jin-Ping, Mu-Lin Yan, and Rong-Hua Yu. "Higher Order Perturbation Corrections of Rotating Excited States in the Standard SU(3) Skyrme Model to Baryon Mass Spectrum." International Journal of Modern Physics A 12, no. 05 (1997): 873–90. http://dx.doi.org/10.1142/s0217751x97000669.

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The higher order corrections of SU(3) rotating excited states to the Gell-Mann–Okubo Relations (or GOR) are presented in the standard SU(3) Skyrme model. The Improved GOR (or IGOR) are obtained. The results show the IGOR for decuplet up to the third order and for octet up to the second order are much compatible with the experimental data. But things become quite inadequate for the octet to the third order. In order to overcome the inadequacy, a heuristic discussion is presented. The properties of SU(3) rotating excited states 27-let (with spin [Formula: see text] or [Formula: see text]), 10*-l

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45

Duck, Ian. "Octet-decuplet baryon mass splittings from self-consistent one-loop perturbation theory." Zeitschrift f�r Physik A Hadrons and Nuclei 350, no. 1 (1994): 71–88. http://dx.doi.org/10.1007/bf01285055.

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46

K�rner, J. G. "TheN-? transition form factor and anomalous?-decays into octet-decuplet baryon-antibaryon Pairs." Zeitschrift f�r Physik C Particles and Fields 33, no. 4 (1987): 529–35. http://dx.doi.org/10.1007/bf01548265.

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47

Ivanov, A. N., M. Nagy, and N. I. Troitskaya. "Effective quark model with chiralU(3)×U(3)symmetry for baryon octet and decuplet." Physical Review C 59, no. 1 (1999): 451–59. http://dx.doi.org/10.1103/physrevc.59.451.

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48

Semke, A., and M. F. M. Lutz. "On the possibility of a discontinuous quark-mass dependence of baryon octet and decuplet masses." Nuclear Physics A 789, no. 1-4 (2007): 251–59. http://dx.doi.org/10.1016/j.nuclphysa.2007.02.011.

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49

Sinha, Monika, Ashik Iqubal, Mira Dey та Jishnu Dey. "Two new sum rules for octet-baryon magnetic moments (μ) and constraints on QCD sum rules from new experimental determination of μ-s for the decuplet". Physics Letters B 562, № 1-2 (2003): 63–67. http://dx.doi.org/10.1016/s0370-2693(03)00545-8.

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50

Sinha, Monika, Ashik Iqubal, Mira Dey та Jishnu Dey. "Addendum to: “Two new sum rules for octet-baryon magnetic moments (μ) and constraints on QCD sum rules from new experimental determination of μ-s for the decuplet” [Phys. Lett. B 562 (2003) 63]". Physics Letters B 610, № 3-4 (2005): 283–84. http://dx.doi.org/10.1016/j.physletb.2005.02.030.

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