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000291403 0881_ $$aDESY-PROC-2014-04
000291403 088__ $$2DESY$$aDESY-PROC-2014-04
000291403 1001_ $$aBhattacharya, A.$$b0
000291403 1112_ $$aPanic2014$$cHamburg$$d2014-08-25 - 2014-08-29$$gPanic2014$$wGermany
000291403 245__ $$aDiquark and Baryon Masses in Composite Fermion Approach
000291403 260__ $$aHamburg$$bDeutsches Elektronen-Synchrotron, DESY$$c2014
000291403 300__ $$a99-103
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000291403 520__ $$aA model for diquark has been suggested describing it as a Composite Fermion. The masses of the light[$\Lambda^{0}$, $\Sigma^{-}$, $\Xi^{-}$, $\Omega^{-}$], heavy [$\Lambda_{c}^{+}$, $\Sigma_{c}^{+}$, $\Xi_{c}^{0}$, $\Omega_{c}^{-}$ and $\Lambda_{b}^{0}$, $\Sigma_{b}^{0}$, $\Xi_{b}^{0}$, $\Omega_{b}^{-}$], doubly heavy [$\Xi_{cc}^{++}$, $\Xi_{cc}^{+}$, $\Xi_{cb}^{+}$, $\Xi_{cb}^{0}$, $\Xi_{bb}^{0}$, $\Xi_{bb}^{-}$, $\Omega_{cc}^{+}$, $\Omega_{cb}^{0}$, $\Omega_{bb}^{-}$] and triply heavy [$\Omega_{ccc}$, $\Omega_{ccb}$, $\Omega_{bbc}$, $\Omega_{bbb}$] baryons have been studied for J$^{P}$ = $\frac{1}{2}^{+}$ and $\frac{3}{2}^{+}$ states. The results are found to be in good agreement with available experimental data and other theoretical works.
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000291403 650_7 $$2autogen$$afermion: composite
000291403 650_7 $$2autogen$$abaryon: mass
000291403 650_7 $$2autogen$$adiquark
000291403 693__ $$0EXP:(DE-MLZ)NOSPEC-20140101$$5EXP:(DE-MLZ)NOSPEC-20140101$$eNo specific instrument$$x0
000291403 7001_ $$aGhosh, R.$$b1
000291403 7001_ $$aChakrabarti, B.$$b2
000291403 773__ $$a10.3204/DESY-PROC-2014-04/128
000291403 7870_ $$0PUBDB-2015-03603$$aSchmidt, Alexander et.al.$$dHamburg : Deutsches Elektronen-Synchrotron, DESY, Hamburg, 2014$$iIsPartOf$$rDESY-PROC-2014-04$$tProceedings, 20th International Conference on Particles and Nuclei (PANIC 14)
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