000026962 001__ 26962
000026962 005__ 20140130015536.0
000026962 037__ $$9arXiv$$ahep-ex/0403044$$chep-ex
000026962 035__ $$9arXiv$$zoai:arXiv.org:hep-ex/0403044
000026962 035__ $$9DESY$$zD04-09902
000026962 035__ $$9SPIRESTeX$$zAslanyan:2004gs
000026962 100__ $$aAslanyan, P.Zh.$$uYerevan State U.$$uDubna, JINR
000026962 245__ $$aObservation of S = +1 narrow resonances in the system K0(s)p from p + C(3)H(8) collision at 10-GeV/c
000026962 246__ $$9arXiv$$aObservation of S=+1 narrow resonances in the system $K^0_sp$ from p+$C_3H_8$ collision at 10 GeV/c
000026962 269__ $$c2004-03
000026962 300__ $$a8
000026962 520__ $$9arXiv$$aThe 2m propane bubble chamber experimental data have been analyzed to search for an exotic baryon state, the $\Theta^+$ -baryon, in the $pK^0_s$ decay mode for the reaction p+$C_3H_8$ at 10 GeV/c. The $pK^0_s$ invariant mass spectrum shows resonant structures with $M_{K_s^0 p}$=1540$\pm$8, 1613$\pm$10, 1821$\pm$11 MeV/$c^2$ and $\Gamma_{K_s^0 p}$= 9.2$\pm$1.8, 16.1$\pm$4.1, 28.0$\pm$9.4 MeV/$c^2$. The maximal statistical significance of these peaks have been estimated as 5.5$\sigma$,4.8$\sigma$ and 5.0$\sigma$, respectively.
000026962 65017 $$2INSPIRE$$aExperiment-HEP
000026962 690C_ $$2INSPIRE$$aConference Paper
000026962 690C_ $$2INSPIRE$$aPublished
000026962 695__ $$2INSPIRE$$ap p: exclusive reaction
000026962 695__ $$2INSPIRE$$aK0(S): hadroproduction
000026962 695__ $$2INSPIRE$$aLambda: associated production
000026962 695__ $$2INSPIRE$$amass spectrum: (p K0(S))
000026962 695__ $$2INSPIRE$$anarrow resonance: search for
000026962 695__ $$2INSPIRE$$apentaquark
000026962 695__ $$2INSPIRE$$aTheta(1540)
000026962 695__ $$2INSPIRE$$achannel cross section
000026962 695__ $$2INSPIRE$$abubble chamber(heavy liquid): experimental results
000026962 695__ $$2INSPIRE$$aDubna PS
000026962 695__ $$2INSPIRE$$ap p --> Lambda p K0(S)
000026962 695__ $$2INSPIRE$$a10 GeV/c
000026962 700__ $$aEmelyanenko, V.N.$$uDubna, JINR
000026962 700__ $$aRikhkvitzkaya, G.G.$$uDubna, JINR
000026962 773__ $$a10.1016/j.nuclphysa.2005.03.041$$c375-378$$pNucl.Phys.$$vA755$$y2005
000026962 773__ $$wC04/10/25
000026962 8564_ $$uhttp://dx.doi.org/10.1016/j.nuclphysa.2005.03.041$$w10.1016/j.nuclphysa.2005.03.041$$yDOI
000026962 909CO $$ooai:jdsweb.jinr.ru:26962$$pglobal
000026962 961__ $$x2004-03-30
000026962 961__ $$c2008-11-26
000026962 970__ $$aSPIRES-5836492
000026962 980__ $$aConference
000026962 980__ $$aPublished
000026962 980__ $$aarXiv
000026962 980__ $$aCiteable
000026962 980__ $$aCORE
000026962 999C5 $$rhep-ph/9703373$$sZ.Phys.,A359,305
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000026962 999C5 $$rhep-ph/0402260$$sPhys.Lett.,B575,249
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000026962 999C5 $$rhep-ex/0310014$$sPhys.Rev.Lett.,92,042003
000026962 999C5 $$rhep-ex/0301020$$sPhys.Rev.Lett.,91,012002
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000026962 999C5 $$rhep-ex/0312044$$sPhys.Lett.,B585,213
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000026962 999C5 $$sPhys.Rev.,D66,010001
000026962 999C5 $$sComput.Phys.Commun.,71,173
000026962 999C5 $$sJINR Rapid Commun.,6,209