001221239 001__ 1221239
001221239 003__ SzGeCERN
001221239 005__ 20230312215006.0
001221239 0248_ $$aoai:cds.cern.ch:1221239$$pcerncds:FULLTEXT$$pcerncds:CERN:FULLTEXT$$pcerncds:CERN
001221239 035__ $$9arXiv$$aoai:arXiv.org:0911.1951
001221239 035__ $$9SPIRES$$a8460051
001221239 035__ $$9Inspire$$a836575
001221239 037__ $$9arXiv$$aarXiv:0911.1951$$chep-ph
001221239 037__ $$aCERN-PH-TH-2009-214
001221239 041__ $$aeng
001221239 084__ $$2CERN Library$$aTH-2009-214
001221239 088__ $$aCERN-PH-TH-2009-214
001221239 100__ $$aChoi, S.Y.$$uChonbuk Natl. U.
001221239 245__ $$aScalar gluons and Dirac gluinos at the LHC
001221239 260__ $$c2009
001221239 269__ $$c11 Nov 2009
001221239 300__ $$a10 p
001221239 300__ $$a10 p
001221239 500__ $$aComments: 10 pages, 4 figures, presented at the XXXIII International Conference on Theoretical Physics "Matter to the Deepest", Ustron, Poland, September 11-16, 2009. To appear in Acta Physica Polonica B
001221239 520__ $$aThe hybrid N=1/N=2 supersymmetric model predicts scalar gluons (sgluons) as SUSY partners of the Dirac gluino. Their strikingly distinct phenomenology at the CERN Large Hadron Collider is discussed.
001221239 520__ $$9arXiv$$aThe hybrid N=1/N=2 supersymmetric model predicts scalar gluons (sgluons) as SUSY partners of the Dirac gluino. Their strikingly distinct phenomenology at the CERN Large Hadron Collider is discussed.
001221239 595__ $$aLANL EDS
001221239 595__ $$aCERN-TH
001221239 595__ $$aSIS ARXIVPUBL2010
001221239 595__ $$darxiv:0911.1951
001221239 595__ $$aOA
001221239 65017 $$2arXiv$$aParticle Physics - Phenomenology
001221239 690C_ $$aARTICLE
001221239 690C_ $$aCERN
001221239 693__ $$aNot applicable$$eNot applicable
001221239 695__ $$9LANL EDS$$ahep-ph
001221239 700__ $$aKalinowski, J.$$uWarsaw U.
001221239 700__ $$aKim, J.M.$$uBonn U.
001221239 700__ $$aPopenda, E.$$uKIT, Karlsruhe
001221239 710__ $$5PH-TH
001221239 773__ $$c2913-2922$$pActa Phys. Pol. B$$v40$$y2009
001221239 8564_ $$uhttp://th-www.if.uj.edu.pl/acta/vol40/abs/v40p2913.htm$$yActa Physica Polonica Server
001221239 8564_ $$82432560$$s149777$$uhttps://cds.cern.ch/record/1221239/files/arXiv:0911.1951.pdf
001221239 8564_ $$82432554$$s25934$$uhttps://cds.cern.ch/record/1221239/files/sigbr2.png$$y00003 \it Branching ratios for $\sigma$ decays, for $m_{\tilde q_L}$=2$ m_{\tilde g}$=1~TeV (left) and $m_{\tilde g}$ = 2$m_{\tilde q_L}$=1~TeV(right).
001221239 8564_ $$82432555$$s26347$$uhttps://cds.cern.ch/record/1221239/files/sigbr1.png$$y00002 \it Branching ratios for $\sigma$ decays, for $m_{\tilde q_L}$=2$ m_{\tilde g}$=1~TeV (left) and $m_{\tilde g}$ = 2$m_{\tilde q_L}$=1~TeV(right).
001221239 8564_ $$82432556$$s11759$$uhttps://cds.cern.ch/record/1221239/files/lhcsigma.png$$y00004 \it Cross sections for $\sigma$-pair [and $\tilde{q}_3$-pair] production (lines (a) and (b)), as well as for single $\sigma$ production (lines (c) and (d)),at the LHC. The curve (c) is for the mass parameters as in Fig.3 (right), while the dashed (d) for the mSUGRA benchmark point SPS1a$'$.
001221239 8564_ $$82432557$$s3270$$uhttps://cds.cern.ch/record/1221239/files/fig.sqaQ.png$$y00000 \it Cross sections for different-flavor squark production in $q\bar q'\to\tilde{q}\tilde{q}'^\ast$ (left) and $qq'\to\tilde{q}\tilde{q}'$ (right) as afunction of the Dirac/Majorana control parameter~$y$.
001221239 8564_ $$82432558$$s3357$$uhttps://cds.cern.ch/record/1221239/files/fig.sqsQ.png$$y00001 \it Cross sections for different-flavor squark production in $q\bar q'\to\tilde{q}\tilde{q}'^\ast$ (left) and $qq'\to\tilde{q}\tilde{q}'$ (right) as afunction of the Dirac/Majorana control parameter~$y$.
001221239 8564_ $$82432559$$s456956$$uhttps://cds.cern.ch/record/1221239/files/v40p2913.pdf$$yFulltext
001221239 916__ $$sn$$w200945$$ya2009
001221239 960__ $$a13
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001221239 962__ $$b1234875$$k2913-2922$$nustron20090911
001221239 963__ $$aPUBLIC
001221239 970__ $$a002857827CER
001221239 980__ $$aARTICLE
001221239 980__ $$aConferencePaper