000331194 001__ 331194
000331194 003__ SzGeCERN
000331194 005__ 20240824063913.0
000331194 0247_ $$2DOI$$a10.1016/S0370-2693(97)01178-7
000331194 0248_ $$aoai:cds.cern.ch:331194$$pcerncds:hep-ex$$pcerncds:CERN$$pcerncds:CERN:FULLTEXT$$pcerncds:FULLTEXT
000331194 035__ $$9CERN annual report$$a97-1261
000331194 035__ $$9CERCER$$a0254701
000331194 035__ $$9SPIRES$$a3603458
000331194 035__ $$9Inspire$$a446719
000331194 037__ $$9arXiv$$ahep-ex/9708013$$chep-ex
000331194 037__ $$aCERN-PPE-97-084
000331194 037__ $$aCERN-PPE-97-84
000331194 037__ $$aFSU-SCRI-98-11
000331194 041__ $$aeng
000331194 084__ $$2CERN Library$$aPPE-1997-084
000331194 088__ $$aCERN-PPE-97-084
000331194 100__ $$aBarate, R.$$uAnnecy, LAPP
000331194 245__ $$aSearches for scalar top and scalar bottom quarks at LEP2
000331194 260__ $$c1997
000331194 269__ $$aGeneva$$bCERN$$c17 Jul 1997
000331194 300__ $$a16 p
000331194 340__ $$apaper
000331194 490__ $$aALEPH Papers
000331194 500__ $$9arXiv$$aLatex (epsfig): 16 pages including 6 figures Report-no: CERN-PPE/97-084
000331194 520__ $$aSearches for scalar top and bottom quarks have been performed with data collected by the ALEPH detector at LEP. The data sample consists of 21.7 pb^-1 taken at sqrt{s} = 161, 170, and 172~GeV and 5.7 pb^-1 taken at sqrt{s} = 130 and 136~GeV. No evidence for scalar top quarks or scalar bottom quarks was found in the channels stop --> c chi, stop --> b l snu, and sbottom --> b chi. For the channel stop --> c chi a limit of 67 GeV/c^2 has been set on the scalar top quark mass, independent of the mixing angle between the supersymmetric partners of the left and right-handed states of the top quark. This limit assumes a mass difference between the stop and the chi of at least 10 GeV/c^2. For the channel stop --> b l snu the mixing-angle independent scalar top limit is 70 GeV/c^2, assuming a mass difference between the stop and the snu of at least 10 GeV/c^2. For the channel sbottom --> b chi, a limit of 73 GeV/c^2 has been set on the mass of the supersymmetric partner of the left-handed state of the bottom quark. This limit is valid if the mass difference between the sbottom and the chi is at least 10 GeV/c^2.
000331194 520__ $$aSearches for scalar top and bottom quarks have been performed with data collected by the ALEPH detector at LEP. The data sample consists of 21.7 pb^-1 taken at sqrt{s} = 161, 170, and 172~GeV and 5.7 pb^-1 taken at sqrt{s} = 130 and 136~GeV. No evidence for scalar top quarks or scalar bottom quarks was found in the channels stop --> c chi, stop --> b l snu, and sbottom --> b chi. For the channel stop --> c chi a limit of 67 GeV/c^2 has been set on the scalar top quark mass, independent of the mixing angle between the supersymmetric partners of the left and right-handed states of the top quark. This limit assumes a mass difference between the stop and the chi of at least 10 GeV/c^2. For the channel stop --> b l snu the mixing-angle independent scalar top limit is 70 GeV/c^2, assuming a mass difference between the stop and the snu of at least 10 GeV/c^2. For the channel sbottom --> b chi, a limit of 73 GeV/c^2 has been set on the mass of the supersymmetric partner of the left-handed state of the bottom quark. This limit is valid if the mass difference between the sbottom and the chi is at least 10 GeV/c^2.
000331194 520__ $$aSearches for scalar top and bottom quarks have been performed with data collected by the ALEPH detector at LEP. The data sample consists of 21.7 pb^-1 taken at sqrt{s} = 161, 170, and 172~GeV and 5.7 pb^-1 taken at sqrt{s} = 130 and 136~GeV. No evidence for scalar top quarks or scalar bottom quarks was found in the channels stop --> c chi, stop --> b l snu, and sbottom --> b chi. For the channel stop --> c chi a limit of 67 GeV/c^2 has been set on the scalar top quark mass, independent of the mixing angle between the supersymmetric partners of the left and right-handed states of the top quark. This limit assumes a mass difference between the stop and the chi of at least 10 GeV/c^2. For the channel stop --> b l snu the mixing-angle independent scalar top limit is 70 GeV/c^2, assuming a mass difference between the stop and the snu of at least 10 GeV/c^2. For the channel sbottom --> b chi, a limit of 73 GeV/c^2 has been set on the mass of the supersymmetric partner of the left-handed state of the bottom quark. This limit is valid if the mass difference between the sbottom and the chi is at least 10 GeV/c^2.
000331194 520__ $$aSearches for scalar top and bottom quarks have been performed with data collected by the ALEPH detector at LEP. The data sample consists of 21.7 pb^-1 taken at sqrt{s} = 161, 170, and 172~GeV and 5.7 pb^-1 taken at sqrt{s} = 130 and 136~GeV. No evidence for scalar top quarks or scalar bottom quarks was found in the channels stop --> c chi, stop --> b l snu, and sbottom --> b chi. For the channel stop --> c chi a limit of 67 GeV/c^2 has been set on the scalar top quark mass, independent of the mixing angle between the supersymmetric partners of the left and right-handed states of the top quark. This limit assumes a mass difference between the stop and the chi of at least 10 GeV/c^2. For the channel stop --> b l snu the mixing-angle independent scalar top limit is 70 GeV/c^2, assuming a mass difference between the stop and the snu of at least 10 GeV/c^2. For the channel sbottom --> b chi, a limit of 73 GeV/c^2 has been set on the mass of the supersymmetric partner of the left-handed state of the bottom quark. This limit is valid if the mass difference between the sbottom and the chi is at least 10 GeV/c^2.
000331194 520__ $$aSearches for scalar top and bottom quarks have been performed with data collected by the ALEPH detector at LEP. The data sample consists of 21.7 pb^-1 taken at sqrt{s} = 161, 170, and 172~GeV and 5.7 pb^-1 taken at sqrt{s} = 130 and 136~GeV. No evidence for scalar top quarks or scalar bottom quarks was found in the channels stop --> c chi, stop --> b l snu, and sbottom --> b chi. For the channel stop --> c chi a limit of 67 GeV/c^2 has been set on the scalar top quark mass, independent of the mixing angle between the supersymmetric partners of the left and right-handed states of the top quark. This limit assumes a mass difference between the stop and the chi of at least 10 GeV/c^2. For the channel stop --> b l snu the mixing-angle independent scalar top limit is 70 GeV/c^2, assuming a mass difference between the stop and the snu of at least 10 GeV/c^2. For the channel sbottom --> b chi, a limit of 73 GeV/c^2 has been set on the mass of the supersymmetric partner of the left-handed state of the bottom quark. This limit is valid if the mass difference between the sbottom and the chi is at least 10 GeV/c^2.
000331194 520__ $$aSearches for scalar top and bottom quarks have been performed with data collected by the ALEPH detector at LEP. The data sample consists of 21.7 pb^-1 taken at sqrt{s} = 161, 170, and 172~GeV and 5.7 pb^-1 taken at sqrt{s} = 130 and 136~GeV. No evidence for scalar top quarks or scalar bottom quarks was found in the channels stop --> c chi, stop --> b l snu, and sbottom --> b chi. For the channel stop --> c chi a limit of 67 GeV/c^2 has been set on the scalar top quark mass, independent of the mixing angle between the supersymmetric partners of the left and right-handed states of the top quark. This limit assumes a mass difference between the stop and the chi of at least 10 GeV/c^2. For the channel stop --> b l snu the mixing-angle independent scalar top limit is 70 GeV/c^2, assuming a mass difference between the stop and the snu of at least 10 GeV/c^2. For the channel sbottom --> b chi, a limit of 73 GeV/c^2 has been set on the mass of the supersymmetric partner of the left-handed state of the bottom quark. This limit is valid if the mass difference between the sbottom and the chi is at least 10 GeV/c^2.
000331194 520__ $$aSearches for scalar top and bottom quarks have been performed with data collected by the ALEPH detector at LEP. The data sample consists of 21.7 pb^-1 taken at sqrt{s} = 161, 170, and 172~GeV and 5.7 pb^-1 taken at sqrt{s} = 130 and 136~GeV. No evidence for scalar top quarks or scalar bottom quarks was found in the channels stop --> c chi, stop --> b l snu, and sbottom --> b chi. For the channel stop --> c chi a limit of 67 GeV/c^2 has been set on the scalar top quark mass, independent of the mixing angle between the supersymmetric partners of the left and right-handed states of the top quark. This limit assumes a mass difference between the stop and the chi of at least 10 GeV/c^2. For the channel stop --> b l snu the mixing-angle independent scalar top limit is 70 GeV/c^2, assuming a mass difference between the stop and the snu of at least 10 GeV/c^2. For the channel sbottom --> b chi, a limit of 73 GeV/c^2 has been set on the mass of the supersymmetric partner of the left-handed state of the bottom quark. This limit is valid if the mass difference between the sbottom and the chi is at least 10 GeV/c^2.
000331194 520__ $$aSearches for scalar top and bottom quarks have been performed with data collected by the ALEPH detector at LEP. The data sample consists of 21.7 pb^-1 taken at sqrt{s} = 161, 170, and 172~GeV and 5.7 pb^-1 taken at sqrt{s} = 130 and 136~GeV. No evidence for scalar top quarks or scalar bottom quarks was found in the channels stop --> c chi, stop --> b l snu, and sbottom --> b chi. For the channel stop --> c chi a limit of 67 GeV/c^2 has been set on the scalar top quark mass, independent of the mixing angle between the supersymmetric partners of the left and right-handed states of the top quark. This limit assumes a mass difference between the stop and the chi of at least 10 GeV/c^2. For the channel stop --> b l snu the mixing-angle independent scalar top limit is 70 GeV/c^2, assuming a mass difference between the stop and the snu of at least 10 GeV/c^2. For the channel sbottom --> b chi, a limit of 73 GeV/c^2 has been set on the mass of the supersymmetric partner of the left-handed state of the bottom quark. This limit is valid if the mass difference between the sbottom and the chi is at least 10 GeV/c^2.
000331194 520__ $$aSearches for scalar top and bottom quarks have been performed with data collected by the ALEPH detector at LEP. The data sample consists of 21.7 pb^-1 taken at sqrt{s} = 161, 170, and 172~GeV and 5.7 pb^-1 taken at sqrt{s} = 130 and 136~GeV. No evidence for scalar top quarks or scalar bottom quarks was found in the channels stop --> c chi, stop --> b l snu, and sbottom --> b chi. For the channel stop --> c chi a limit of 67 GeV/c^2 has been set on the scalar top quark mass, independent of the mixing angle between the supersymmetric partners of the left and right-handed states of the top quark. This limit assumes a mass difference between the stop and the chi of at least 10 GeV/c^2. For the channel stop --> b l snu the mixing-angle independent scalar top limit is 70 GeV/c^2, assuming a mass difference between the stop and the snu of at least 10 GeV/c^2. For the channel sbottom --> b chi, a limit of 73 GeV/c^2 has been set on the mass of the supersymmetric partner of the left-handed state of the bottom quark. This limit is valid if the mass difference between the sbottom and the chi is at least 10 GeV/c^2.
000331194 520__ $$9Elsevier$$aSearches for scalar top and bottom quarks have been performed with data collected by the ALEPH detector at LEP. The data sample consists of 21.7 pb −1 taken at s = 161, 170 , and 5.7 pb −1 taken at s = 130 and 136 GeV . No evidence for scalar top quarks or scalar bottom quarks was found in the channels t → cχ, t → bℓ ν , and b → bχ. For the channel t → cχ a limit of 67 GeV/ c 2 has been set on the scalar top quark mass, independent of the mixing angle between the supersymmetric partners of the left and right-handed states of the top quark. This limit assumes a mass difference between the t and the χ of at least 10 GeV/ c 2 . For the channel t → bℓ ν the mixing-angle independent scalar top limit is 70 GeV/ c 2 , assuming a mass difference between the t and the ν of at least 10 GeV/ c 2 . For the channel b → bχ, a limit of 73 GeV/ c 2 has been set on the mass of the supersymmetric partner of the left-handed state of the bottom quark. This limit is valid if the mass difference between the b and the χ is at least 10 GeV/ c 2 .
000331194 542__ $$fCopyright @ unknown. Published by Elsevier B.V.
000331194 595__ $$aCERN-PPE
000331194 595__ $$aLANL EDS
000331194 595__ $$aOA
000331194 65017 $$2SzGeCERN$$aParticle Physics - Experiment
000331194 690C_ $$aARTICLE
000331194 690C_ $$aCERN
000331194 693__ $$aCERN LEP$$eALEPH
000331194 695__ $$9MEDLINE$$asearches supersymmetry
000331194 695__ $$9LANL EDS$$aHigh Energy Physics - Experiment
000331194 700__ $$aBuskulic, D.$$uAnnecy, LAPP
000331194 700__ $$aDecamp, D.$$uAnnecy, LAPP
000331194 700__ $$aGhez, Philippe$$uAnnecy, LAPP
000331194 700__ $$aGoy, C.$$uAnnecy, LAPP
000331194 700__ $$aLees, J.P.$$uAnnecy, LAPP
000331194 700__ $$aLucotte, A.$$uAnnecy, LAPP
000331194 700__ $$aMinard, M.N.$$uAnnecy, LAPP
000331194 700__ $$aNief, J.Y.$$uAnnecy, LAPP
000331194 700__ $$aPietrzyk, B.$$uAnnecy, LAPP
000331194 700__ $$aCasado, M.P.$$uBarcelona, Autonoma U.
000331194 700__ $$aChmeissani, M.$$uBarcelona, Autonoma U.
000331194 700__ $$aComas, P.$$uBarcelona, Autonoma U.
000331194 700__ $$aCrespo, J.M.$$uBarcelona, Autonoma U.
000331194 700__ $$aDelfino, M.$$uBarcelona, Autonoma U.
000331194 700__ $$aFernandez, E.$$uBarcelona, Autonoma U.
000331194 700__ $$aFernandez-Bosman, M.$$uBarcelona, Autonoma U.
000331194 700__ $$aGarrido, L.$$uBarcelona, Autonoma U.
000331194 700__ $$aJuste, A.$$uBarcelona, Autonoma U.
000331194 700__ $$aMartinez, M.$$uBarcelona, Autonoma U.
000331194 700__ $$aMerino, G.$$uBarcelona, Autonoma U.
000331194 700__ $$aMiquel, R.$$uBarcelona, Autonoma U.
000331194 700__ $$aMir, L.M.$$uBarcelona, Autonoma U.
000331194 700__ $$aPadilla, C.$$uBarcelona, Autonoma U.
000331194 700__ $$aPark, I.C.$$uBarcelona, Autonoma U.
000331194 700__ $$aPascual, A.$$uBarcelona, Autonoma U.
000331194 700__ $$aPerlas, J.A.$$uBarcelona, Autonoma U.
000331194 700__ $$aRiu, I.$$uBarcelona, Autonoma U.
000331194 700__ $$aSanchez, F.$$uBarcelona, Autonoma U.
000331194 700__ $$aTeubert, F.$$uBarcelona, Autonoma U.
000331194 700__ $$aColaleo, A.$$uBari U.$$uINFN, Bari
000331194 700__ $$aCreanza, D.$$uBari U.$$uINFN, Bari
000331194 700__ $$ade Palma, M.$$uBari U.$$uINFN, Bari
000331194 700__ $$aGelao, G.$$uBari U.$$uINFN, Bari
000331194 700__ $$aIaselli, G.$$uBari U.$$uINFN, Bari
000331194 700__ $$aMaggi, G.$$uBari U.$$uINFN, Bari
000331194 700__ $$aMaggi, M.$$uBari U.$$uINFN, Bari
000331194 700__ $$aMarinelli, N.$$uBari U.$$uINFN, Bari
000331194 700__ $$aNuzzo, S.$$uBari U.$$uINFN, Bari
000331194 700__ $$aRanieri, A.$$uBari U.$$uINFN, Bari
000331194 700__ $$aRaso, G.$$uBari U.$$uINFN, Bari
000331194 700__ $$aRuggieri, F.$$uBari U.$$uINFN, Bari
000331194 700__ $$aSelvaggi, G.$$uBari U.$$uINFN, Bari
000331194 700__ $$aSilvestris, L.$$uBari U.$$uINFN, Bari
000331194 700__ $$aTempesta, P.$$uBari U.$$uINFN, Bari
000331194 700__ $$aTricomi, A.$$uBari U.$$uINFN, Bari$$uCatania U.$$uINFN, Catania
000331194 700__ $$aZito, G.$$uBari U.$$uINFN, Bari
000331194 700__ $$aHuang, X.$$uBeijing, Inst. High Energy Phys.
000331194 700__ $$aLin, J.$$uBeijing, Inst. High Energy Phys.
000331194 700__ $$aOuyang, Q.$$uBeijing, Inst. High Energy Phys.
000331194 700__ $$aWang, T.$$uBeijing, Inst. High Energy Phys.
000331194 700__ $$aXie, Y.$$uBeijing, Inst. High Energy Phys.
000331194 700__ $$aXu, R.$$uBeijing, Inst. High Energy Phys.
000331194 700__ $$aXue, S.$$uBeijing, Inst. High Energy Phys.
000331194 700__ $$aZhang, J.$$uBeijing, Inst. High Energy Phys.
000331194 700__ $$aZhang, L.$$uBeijing, Inst. High Energy Phys.
000331194 700__ $$aZhao, W.$$uBeijing, Inst. High Energy Phys.
000331194 700__ $$aAbbaneo, D.$$uCERN
000331194 700__ $$aAlemany, R.$$uCERN
000331194 700__ $$aBazarko, A.O.$$uCERN
000331194 700__ $$aBecker, U.$$uCERN
000331194 700__ $$aBright-Thomas, P.$$uCERN
000331194 700__ $$aCattaneo, M.$$uCERN
000331194 700__ $$aCerutti, F.$$uCERN
000331194 700__ $$aDissertori, G.$$uCERN
000331194 700__ $$aDrevermann, H.$$uCERN
000331194 700__ $$aForty, R.W.$$uCERN
000331194 700__ $$aFrank, M.$$uCERN
000331194 700__ $$aHagelberg, R.$$uCERN
000331194 700__ $$aHansen, J.B.$$uCERN
000331194 700__ $$aHarvey, John$$uCERN
000331194 700__ $$aJanot, P.$$uCERN
000331194 700__ $$aJost, B.$$uCERN
000331194 700__ $$aKneringer, E.$$uCERN
000331194 700__ $$aKnobloch, J.$$uCERN
000331194 700__ $$aLehraus, I.$$uCERN
000331194 700__ $$aMato, P.$$uCERN
000331194 700__ $$aMinten, A.$$uCERN
000331194 700__ $$aMoneta, L.$$uCERN
000331194 700__ $$aPacheco, A.$$uCERN
000331194 700__ $$aPusztaszeri, J.F.$$uCERN
000331194 700__ $$aRanjard, F.$$uCERN
000331194 700__ $$aRizzo, G.$$uCERN
000331194 700__ $$aRolandi, Gigi$$uCERN
000331194 700__ $$aRousseau, D.$$uCERN
000331194 700__ $$aSchlatter, D.$$uCERN
000331194 700__ $$aSchmitt, M.$$uCERN
000331194 700__ $$aSchneider, O.$$uCERN
000331194 700__ $$aTejessy, W.$$uCERN
000331194 700__ $$aTomalin, I.R.$$uCERN
000331194 700__ $$aWachsmuth, H.$$uCERN
000331194 700__ $$aWagner, A.$$uCERN
000331194 700__ $$aAjaltouni, Z.$$uClermont-Ferrand U.
000331194 700__ $$aBarres, A.$$uClermont-Ferrand U.
000331194 700__ $$aBoyer, C.$$uClermont-Ferrand U.
000331194 700__ $$aFalvard, A.$$uClermont-Ferrand U.
000331194 700__ $$aFerdi, C.$$uClermont-Ferrand U.
000331194 700__ $$aGay, P.$$uClermont-Ferrand U.
000331194 700__ $$aGuicheney, C.$$uClermont-Ferrand U.
000331194 700__ $$aHenrard, P.$$uClermont-Ferrand U.
000331194 700__ $$aJousset, J.$$uClermont-Ferrand U.
000331194 700__ $$aMichel, B.$$uClermont-Ferrand U.
000331194 700__ $$aMonteil, S.$$uClermont-Ferrand U.
000331194 700__ $$aMontret, J.C.$$uClermont-Ferrand U.
000331194 700__ $$aPallin, D.$$uClermont-Ferrand U.
000331194 700__ $$aPerret, P.$$uClermont-Ferrand U.
000331194 700__ $$aPodlyski, F.$$uClermont-Ferrand U.
000331194 700__ $$aProriol, J.$$uClermont-Ferrand U.
000331194 700__ $$aRosnet, P.$$uClermont-Ferrand U.
000331194 700__ $$aRossignol, J.M.$$uClermont-Ferrand U.
000331194 700__ $$aFearnley, T.$$uBohr Inst.
000331194 700__ $$aHansen, J.D.$$uBohr Inst.
000331194 700__ $$aHansen, J.R.$$uBohr Inst.
000331194 700__ $$aHansen, P.H.$$uBohr Inst.
000331194 700__ $$aNilsson, B.S.$$uBohr Inst.
000331194 700__ $$aRensch, B.$$uBohr Inst.
000331194 700__ $$aWaananen, A.$$qWaeaenaenen, A.$$uBohr Inst.
000331194 700__ $$aDaskalakis, G.$$uDemocritos Nucl. Res. Ctr.
000331194 700__ $$aKyriakis, A.$$uDemocritos Nucl. Res. Ctr.
000331194 700__ $$aMarkou, C.$$uDemocritos Nucl. Res. Ctr.
000331194 700__ $$aSimopoulou, E.$$uDemocritos Nucl. Res. Ctr.
000331194 700__ $$aVayaki, A.$$uDemocritos Nucl. Res. Ctr.
000331194 700__ $$aBlondel, A.$$uEcole Polytechnique
000331194 700__ $$aBrient, J.C.$$uEcole Polytechnique
000331194 700__ $$aMachefert, F.$$uEcole Polytechnique
000331194 700__ $$aRouge, A.$$uEcole Polytechnique
000331194 700__ $$aRumpf, M.$$uEcole Polytechnique
000331194 700__ $$aValassi, A.$$uEcole Polytechnique
000331194 700__ $$aVideau, H.$$uEcole Polytechnique
000331194 700__ $$aFocardi, E.$$uFlorence U.$$uINFN, Florence
000331194 700__ $$aParrini, G.$$uFlorence U.$$uINFN, Florence
000331194 700__ $$aZachariadou, K.$$uFlorence U.$$uINFN, Florence
000331194 700__ $$aCavanaugh, R.$$uFlorida State U., SCRI
000331194 700__ $$aCorden, M.$$uFlorida State U., SCRI
000331194 700__ $$aGeorgiopoulos, C.$$uFlorida State U., SCRI
000331194 700__ $$aHuehn, T.$$uFlorida State U., SCRI
000331194 700__ $$aJaffe, D.E.$$uFlorida State U., SCRI
000331194 700__ $$aAntonelli, A.$$uFrascati
000331194 700__ $$aBencivenni, G.$$uFrascati
000331194 700__ $$aBologna, G.$$uFrascati$$uTurin U.
000331194 700__ $$aBossi, F.$$uFrascati
000331194 700__ $$aCampana, P.$$uFrascati
000331194 700__ $$aCapon, G.$$uFrascati
000331194 700__ $$aCasper, D.$$uFrascati
000331194 700__ $$aChiarella, V.$$uFrascati
000331194 700__ $$aFelici, G.$$uFrascati
000331194 700__ $$aLaurelli, P.$$uFrascati
000331194 700__ $$aMannocchi, G.$$uFrascati$$uTurin, Cosmo-Geofisica Lab
000331194 700__ $$aMurtas, F.$$uFrascati
000331194 700__ $$aMurtas, G.P.$$uFrascati
000331194 700__ $$aPassalacqua, L.$$uFrascati
000331194 700__ $$aPepe-Altarelli, M.$$uFrascati
000331194 700__ $$aCurtis, L.$$uGlasgow U.
000331194 700__ $$aDorris, S.J.$$uGlasgow U.
000331194 700__ $$aHalley, A.W.$$uGlasgow U.
000331194 700__ $$aKnowles, I.G.$$uGlasgow U.
000331194 700__ $$aLynch, J.G.$$uGlasgow U.
000331194 700__ $$aO'Shea, V.$$uGlasgow U.
000331194 700__ $$aRaine, C.$$uGlasgow U.
000331194 700__ $$aScarr, J.M.$$uGlasgow U.
000331194 700__ $$aSmith, K.$$uGlasgow U.
000331194 700__ $$aTeixeira-Dias, P.$$uGlasgow U.
000331194 700__ $$aThompson, A.S.$$uGlasgow U.
000331194 700__ $$aThomson, Evelyn J.$$uGlasgow U.
000331194 700__ $$aThomson, F.$$uGlasgow U.
000331194 700__ $$aTurnbull, R.M.$$uGlasgow U.
000331194 700__ $$aBuchmuller, O.$$uHeidelberg U.
000331194 700__ $$aDhamotharan, S.$$uHeidelberg U.
000331194 700__ $$aGeweniger, C.$$uHeidelberg U.
000331194 700__ $$aGraefe, G.$$uHeidelberg U.
000331194 700__ $$aHanke, P.$$uHeidelberg U.
000331194 700__ $$aHansper, G.$$uHeidelberg U.
000331194 700__ $$aHepp, V.$$uHeidelberg U.
000331194 700__ $$aKluge, E.E.$$uHeidelberg U.
000331194 700__ $$aPutzer, A.$$uHeidelberg U.
000331194 700__ $$aSommer, J.$$uHeidelberg U.
000331194 700__ $$aTittel, K.$$uHeidelberg U.
000331194 700__ $$aWerner, S.$$uHeidelberg U.
000331194 700__ $$aWunsch, M.$$uHeidelberg U.
000331194 700__ $$aBeuselinck, R.$$uImperial Coll., London
000331194 700__ $$aBinnie, D.M.$$uImperial Coll., London
000331194 700__ $$aCameron, W.$$uImperial Coll., London
000331194 700__ $$aDornan, P.J.$$uImperial Coll., London
000331194 700__ $$aGirone, M.$$uImperial Coll., London
000331194 700__ $$aGoodsir, S.$$uImperial Coll., London
000331194 700__ $$aMartin, E.B.$$uImperial Coll., London
000331194 700__ $$aMorawitz, P.$$uImperial Coll., London
000331194 700__ $$aMoutoussi, A.$$uImperial Coll., London
000331194 700__ $$aNash, J.$$uImperial Coll., London
000331194 700__ $$aSedgbeer, J.K.$$uImperial Coll., London
000331194 700__ $$aSpagnolo, P.$$uImperial Coll., London
000331194 700__ $$aStacey, A.M.$$uImperial Coll., London
000331194 700__ $$aWilliams, M.D.$$uImperial Coll., London
000331194 700__ $$aGhete, M.$$uInnsbruck U.
000331194 700__ $$aGirtler, P.$$uInnsbruck U.
000331194 700__ $$aKuhn, D.$$uInnsbruck U.
000331194 700__ $$aRudolph, G.$$uInnsbruck U.
000331194 700__ $$aBetteridge, A.P.$$uLancaster U.
000331194 700__ $$aBowdery, C.K.$$uLancaster U.
000331194 700__ $$aColrain, P.$$uLancaster U.
000331194 700__ $$aCrawford, G.$$uLancaster U.
000331194 700__ $$aFinch, A.J.$$uLancaster U.
000331194 700__ $$aFoster, F.$$uLancaster U.
000331194 700__ $$aHughes, G.$$uLancaster U.
000331194 700__ $$aJones, R.W.$$uLancaster U.
000331194 700__ $$aSloan, T.$$uLancaster U.
000331194 700__ $$aWhelan, E.P.$$uLancaster U.
000331194 700__ $$aWilliams, M.I.$$uLancaster U.
000331194 700__ $$aHoffmann, C.$$uMainz U., Inst. Phys.
000331194 700__ $$aJakobs, K.$$uMainz U., Inst. Phys.
000331194 700__ $$aKleinknecht, K.$$uMainz U., Inst. Phys.
000331194 700__ $$aQuast, G.$$uMainz U., Inst. Phys.
000331194 700__ $$aRenk, B.$$uMainz U., Inst. Phys.
000331194 700__ $$aRohne, E.$$uMainz U., Inst. Phys.
000331194 700__ $$aSander, H.G.$$uMainz U., Inst. Phys.
000331194 700__ $$avan Gemmeren, P.$$uMainz U., Inst. Phys.
000331194 700__ $$aZeitnitz, C.$$uMainz U., Inst. Phys.
000331194 700__ $$aAubert, J.J.$$uMarseille, CPPM
000331194 700__ $$aBenchouk, C.$$uMarseille, CPPM
000331194 700__ $$aBonissent, A.$$uMarseille, CPPM
000331194 700__ $$aBujosa, G.$$uMarseille, CPPM
000331194 700__ $$aCarr, J.$$uMarseille, CPPM
000331194 700__ $$aCoyle, P.$$uMarseille, CPPM
000331194 700__ $$aDiaconu, C.$$uMarseille, CPPM
000331194 700__ $$aEalet, A.$$uMarseille, CPPM
000331194 700__ $$aFouchez, D.$$uMarseille, CPPM
000331194 700__ $$aKonstantinidis, N.$$uMarseille, CPPM
000331194 700__ $$aLeroy, O.$$uMarseille, CPPM
000331194 700__ $$aMotsch, F.$$uMarseille, CPPM
000331194 700__ $$aPayre, P.$$uMarseille, CPPM
000331194 700__ $$aTalby, M.$$uMarseille, CPPM
000331194 700__ $$aSadouki, A.$$uMarseille, CPPM
000331194 700__ $$aThulasidas, M.$$uMarseille, CPPM
000331194 700__ $$aTilquin, A.$$uMarseille, CPPM
000331194 700__ $$aTrabelsi, K.$$uMarseille, CPPM
000331194 700__ $$aAleppo, M.$$uMilan U.$$uINFN, Milan
000331194 700__ $$aAntonelli, M.$$uMilan U.$$uINFN, Milan
000331194 700__ $$aRagusa, F.$$uMilan U.$$uINFN, Milan$$uCERN
000331194 700__ $$aBerlich, R.$$uMunich, Max Planck Inst.
000331194 700__ $$aBlum, W.$$uMunich, Max Planck Inst.
000331194 700__ $$aBuescher, Volker$$qBuescher, Volker$$uMunich, Max Planck Inst.
000331194 700__ $$aDietl, H.$$uMunich, Max Planck Inst.
000331194 700__ $$aGanis, G.$$uMunich, Max Planck Inst.
000331194 700__ $$aGotzhein, C.$$uMunich, Max Planck Inst.
000331194 700__ $$aKroha, H.$$uMunich, Max Planck Inst.
000331194 700__ $$aLutjens, G.$$qLuetjens, G.$$uMunich, Max Planck Inst.
000331194 700__ $$aLutz, G.$$uMunich, Max Planck Inst.
000331194 700__ $$aManner, W.$$qMaenner, W.$$uMunich, Max Planck Inst.
000331194 700__ $$aMoser, H.G.$$uMunich, Max Planck Inst.
000331194 700__ $$aRichter, Robert$$iINSPIRE-00120026$$uMunich, Max Planck Inst.
000331194 700__ $$aRosado-Schlosser, A.$$uMunich, Max Planck Inst.
000331194 700__ $$aSchael, S.$$uMunich, Max Planck Inst.
000331194 700__ $$aSettles, R.$$uMunich, Max Planck Inst.
000331194 700__ $$aSeywerd, H.$$uMunich, Max Planck Inst.
000331194 700__ $$aSt. Denis, Richard Dante$$uMunich, Max Planck Inst.
000331194 700__ $$aStenzel, H.$$uMunich, Max Planck Inst.
000331194 700__ $$aWiedenmann, W.$$uMunich, Max Planck Inst.
000331194 700__ $$aWolf, G.$$uMunich, Max Planck Inst.
000331194 700__ $$aBoucrot, J.$$uOrsay, LAL
000331194 700__ $$aCallot, O.$$uOrsay, LAL$$uCERN
000331194 700__ $$aChen, S.$$uOrsay, LAL
000331194 700__ $$aCordier, A.$$uOrsay, LAL
000331194 700__ $$aDavier, M.$$uOrsay, LAL
000331194 700__ $$aDuflot, L.$$uOrsay, LAL
000331194 700__ $$aGrivaz, J.F.$$uOrsay, LAL
000331194 700__ $$aHeusse, P.$$uOrsay, LAL
000331194 700__ $$aHocker, Andreas$$qHoecker, A.$$uOrsay, LAL
000331194 700__ $$aJacholkowska, A.$$uOrsay, LAL
000331194 700__ $$aJacquet, M.$$uOrsay, LAL
000331194 700__ $$aKim, D.W.$$uOrsay, LAL
000331194 700__ $$aLe Diberder, F.$$uOrsay, LAL
000331194 700__ $$aLefrancois, J.$$uOrsay, LAL
000331194 700__ $$aLutz, A.M.$$uOrsay, LAL
000331194 700__ $$aNikolic, Irina$$uOrsay, LAL
000331194 700__ $$aSchune, M.H.$$uOrsay, LAL
000331194 700__ $$aSerin, L.$$uOrsay, LAL
000331194 700__ $$aSimion, S.$$uOrsay, LAL
000331194 700__ $$aTournefier, E.$$uOrsay, LAL
000331194 700__ $$aVeillet, J.J.$$uOrsay, LAL
000331194 700__ $$aVideau, I.$$uOrsay, LAL
000331194 700__ $$aZerwas, D.$$uOrsay, LAL
000331194 700__ $$aAzzurri, P.$$uPisa U.$$uINFN, Pisa$$uPisa, Scuola Normale Superiore
000331194 700__ $$aBagliesi, Giuseppe$$uPisa U.$$uINFN, Pisa$$uPisa, Scuola Normale Superiore
000331194 700__ $$aBettarini, S.$$uPisa U.$$uINFN, Pisa$$uPisa, Scuola Normale Superiore
000331194 700__ $$aBozzi, C.$$uPisa U.$$uINFN, Pisa$$uPisa, Scuola Normale Superiore
000331194 700__ $$aCalderini, G.$$uPisa U.$$uINFN, Pisa$$uPisa, Scuola Normale Superiore
000331194 700__ $$aCiulli, V.$$uPisa U.$$uINFN, Pisa$$uPisa, Scuola Normale Superiore
000331194 700__ $$aDell'Orso, R.$$uPisa U.$$uINFN, Pisa$$uPisa, Scuola Normale Superiore
000331194 700__ $$aFantechi, R.$$uPisa U.$$uINFN, Pisa$$uPisa, Scuola Normale Superiore
000331194 700__ $$aFerrante, I.$$uPisa U.$$uINFN, Pisa$$uPisa, Scuola Normale Superiore
000331194 700__ $$aGiassi, A.$$uPisa U.$$uINFN, Pisa$$uPisa, Scuola Normale Superiore
000331194 700__ $$aGregorio, A.$$uPisa U.$$uINFN, Pisa$$uPisa, Scuola Normale Superiore
000331194 700__ $$aLigabue, F.$$uPisa U.$$uINFN, Pisa$$uPisa, Scuola Normale Superiore
000331194 700__ $$aLusiani, A.$$uPisa U.$$uINFN, Pisa$$uPisa, Scuola Normale Superiore
000331194 700__ $$aMarrocchesi, P.S.$$uPisa U.$$uINFN, Pisa$$uPisa, Scuola Normale Superiore
000331194 700__ $$aMessineo, A.$$uPisa U.$$uINFN, Pisa$$uPisa, Scuola Normale Superiore
000331194 700__ $$aPalla, F.$$uPisa U.$$uINFN, Pisa$$uPisa, Scuola Normale Superiore
000331194 700__ $$aSanguinetti, G.$$uPisa U.$$uINFN, Pisa$$uPisa, Scuola Normale Superiore
000331194 700__ $$aSciaba, A.$$uPisa U.$$uINFN, Pisa$$uPisa, Scuola Normale Superiore
000331194 700__ $$aSguazzoni, G.$$uPisa U.$$uINFN, Pisa$$uPisa, Scuola Normale Superiore
000331194 700__ $$aSteinberger, J.$$uPisa U.$$uINFN, Pisa$$uPisa, Scuola Normale Superiore
000331194 700__ $$aTenchini, R.$$uPisa U.$$uINFN, Pisa$$uPisa, Scuola Normale Superiore
000331194 700__ $$aVannini, C.$$uPisa U.$$uINFN, Pisa$$uPisa, Scuola Normale Superiore
000331194 700__ $$aVenturi, A.$$uPisa U.$$uINFN, Pisa$$uPisa, Scuola Normale Superiore
000331194 700__ $$aVerdini, P.G.$$uPisa U.$$uINFN, Pisa$$uPisa, Scuola Normale Superiore
000331194 700__ $$aBlair, G.A.$$uRoyal Holloway, U. of London
000331194 700__ $$aBryant, L.M.$$uRoyal Holloway, U. of London
000331194 700__ $$aChambers, J.T.$$uRoyal Holloway, U. of London
000331194 700__ $$aGao, Y.$$uRoyal Holloway, U. of London
000331194 700__ $$aGreen, M.G.$$uRoyal Holloway, U. of London
000331194 700__ $$aMedcalf, T.$$uRoyal Holloway, U. of London
000331194 700__ $$aPerrodo, P.$$uRoyal Holloway, U. of London
000331194 700__ $$aStrong, J.A.$$uRoyal Holloway, U. of London
000331194 700__ $$avon Wimmersperg-Toeller, J.H.$$qvon Wimmersperg-Toeller, J.H.$$uRoyal Holloway, U. of London
000331194 700__ $$aBotterill, D.R.$$uRutherford
000331194 700__ $$aClifft, R.W.$$uRutherford
000331194 700__ $$aEdgecock, T.R.$$uRutherford
000331194 700__ $$aHaywood, S.$$uRutherford
000331194 700__ $$aMaley, P.$$uRutherford
000331194 700__ $$aNorton, P.R.$$uRutherford
000331194 700__ $$aThompson, J.C.$$uRutherford
000331194 700__ $$aWright, A.E.$$uRutherford
000331194 700__ $$aBloch-Devaux, Brigitte$$uDAPNIA, Saclay
000331194 700__ $$aColas, P.$$uDAPNIA, Saclay
000331194 700__ $$aFabbro, B.$$uDAPNIA, Saclay
000331194 700__ $$aKozanecki, W.$$uDAPNIA, Saclay
000331194 700__ $$aLancon, E.$$uDAPNIA, Saclay
000331194 700__ $$aLemaire, M.C.$$uDAPNIA, Saclay
000331194 700__ $$aLocci, E.$$uDAPNIA, Saclay
000331194 700__ $$aPerez, P.$$uDAPNIA, Saclay
000331194 700__ $$aRander, J.$$uDAPNIA, Saclay
000331194 700__ $$aRenardy, J.F.$$uDAPNIA, Saclay
000331194 700__ $$aRosowsky, A.$$uDAPNIA, Saclay
000331194 700__ $$aRoussarie, A.$$uDAPNIA, Saclay
000331194 700__ $$aSchuller, J.P.$$uDAPNIA, Saclay
000331194 700__ $$aSchwindling, J.$$uDAPNIA, Saclay
000331194 700__ $$aTrabelsi, A.$$uDAPNIA, Saclay
000331194 700__ $$aVallage, B.$$uDAPNIA, Saclay
000331194 700__ $$aBlack, S.N.$$uUC, Santa Cruz
000331194 700__ $$aDann, J.H.$$uUC, Santa Cruz
000331194 700__ $$aKim, H.Y.$$uUC, Santa Cruz
000331194 700__ $$aLitke, A.M.$$uUC, Santa Cruz
000331194 700__ $$aMcNeil, M.A.$$uUC, Santa Cruz
000331194 700__ $$aTaylor, G.$$uUC, Santa Cruz
000331194 700__ $$aBooth, C.N.$$uSheffield U.
000331194 700__ $$aBoswell, R.$$uSheffield U.
000331194 700__ $$aBrew, C.A.J.$$uSheffield U.
000331194 700__ $$aCartwright, S.$$uSheffield U.
000331194 700__ $$aCombley, F.$$uSheffield U.
000331194 700__ $$aKelly, M.S.$$uSheffield U.
000331194 700__ $$aLehto, M.$$uSheffield U.
000331194 700__ $$aNewton, W.M.$$uSheffield U.
000331194 700__ $$aReeve, J.$$uSheffield U.
000331194 700__ $$aThompson, L.F.$$uSheffield U.
000331194 700__ $$aAffholderbach, K.$$uSiegen U.
000331194 700__ $$aBoehrer, Armin$$qBoehrer, A.$$uSiegen U.
000331194 700__ $$aBrandt, S.$$uSiegen U.
000331194 700__ $$aCowan, G.$$uSiegen U.
000331194 700__ $$aFoss, J.$$uSiegen U.
000331194 700__ $$aGrupen, C.$$uSiegen U.
000331194 700__ $$aLutters, G.$$uSiegen U.
000331194 700__ $$aSaraiva, P.$$uSiegen U.
000331194 700__ $$aSmolik, L.$$uSiegen U.
000331194 700__ $$aStephan, F.$$uSiegen U.
000331194 700__ $$aApollonio, M.$$uTrieste U.$$uINFN, Trieste
000331194 700__ $$aBosisio, L.$$uTrieste U.$$uINFN, Trieste
000331194 700__ $$aDella Marina, R.$$uTrieste U.$$uINFN, Trieste
000331194 700__ $$aGiannini, G.$$uTrieste U.$$uINFN, Trieste
000331194 700__ $$aGobbo, B.$$uTrieste U.$$uINFN, Trieste
000331194 700__ $$aMusolino, G.$$uTrieste U.$$uINFN, Trieste
000331194 700__ $$aPutz, J.$$uWashington U., Seattle
000331194 700__ $$aRothberg, J.$$uWashington U., Seattle
000331194 700__ $$aWasserbaech, S.$$uWashington U., Seattle
000331194 700__ $$aWilliams, R.W.$$uWashington U., Seattle
000331194 700__ $$aArmstrong, S.R.$$uWisconsin U., Madison
000331194 700__ $$aCharles, E.$$uWisconsin U., Madison
000331194 700__ $$aElmer, P.$$uWisconsin U., Madison
000331194 700__ $$aFerguson, D.P.S.$$uWisconsin U., Madison
000331194 700__ $$aGonzalez, S.$$uWisconsin U., Madison
000331194 700__ $$aGreening, T.C.$$uWisconsin U., Madison
000331194 700__ $$aHayes, O.J.$$uWisconsin U., Madison
000331194 700__ $$aHu, H.$$uWisconsin U., Madison
000331194 700__ $$aJin, S.$$uWisconsin U., Madison
000331194 700__ $$aMcNamara, P.A., III$$uWisconsin U., Madison
000331194 700__ $$aNachtman, J.M.$$uWisconsin U., Madison
000331194 700__ $$aNielsen, J.$$uWisconsin U., Madison
000331194 700__ $$aOrejudos, W.$$uWisconsin U., Madison
000331194 700__ $$aPan, Y.B.$$uWisconsin U., Madison
000331194 700__ $$aSaadi, Y.$$uWisconsin U., Madison
000331194 700__ $$aScott, I.J.$$uWisconsin U., Madison
000331194 700__ $$aWalsh, J.$$uWisconsin U., Madison
000331194 700__ $$aWu, Sau Lan$$uWisconsin U., Madison
000331194 700__ $$aWu, X.$$uWisconsin U., Madison
000331194 700__ $$aYamartino, J.M.$$uWisconsin U., Madison
000331194 700__ $$aZobernig, G.$$uWisconsin U., Madison
000331194 710__ $$gALEPH Collaboration
000331194 710__ $$5PPE
000331194 773__ $$c431-446$$pPhys. Lett. B$$v413$$y1997
000331194 852__ $$cCERN ARC Library$$hCERN-PPE-97-084
000331194 852__ $$cCERN Central Library$$hhep-ex/9708013
000331194 859__ [email protected]
000331194 8564_ $$uhttp://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=cern&id=ppe-97-084$$yFulltext
000331194 8564_ $$846368$$s462247$$uhttps://cds.cern.ch/record/331194/files/ppe-97-084.pdf$$yFulltext
000331194 8564_ $$846368$$s171370$$uhttps://cds.cern.ch/record/331194/files/ppe-97-084.ps.gz$$yFulltext
000331194 8564_ $$82316637$$s277388$$uhttps://cds.cern.ch/record/331194/files/arXiv:hep-ex_9708013.pdf
000331194 8564_ $$82316622$$s18672$$uhttps://cds.cern.ch/record/331194/files/AlephStopFig6c.png$$y00015 \rm Excluded regions assuming $\sbot \rightarrow \mathrm{b}\neu$. (a) Excluded region in the $m_{\neu}$ vs $m_{\sbot}$ plane. (b) Excluded region in the $m_{\sbot}$ vs $\mathrm \thetab$ plane. (c) Excluded region in the $m_{\sbot}$ vs $\deltm$ plane. In (a) and (c), excluded regions are given for $0^{\circ}$, corresponding to the maximum $\sbot$-Z coupling, and for $40^{\circ}$.
000331194 8564_ $$82316623$$s19183$$uhttps://cds.cern.ch/record/331194/files/AlephStopFig3a.png$$y00003 \rm Efficiencies as a function of $\deltm$. (a) Efficiency for a 65 $\gev$ stop decaying as $\stop \rightarrow \mathrm{c}\neu$ (solid curve), a 50 $\gev$ stop decaying as $\stop \rightarrow \mathrm{c}\neu$ (dashed curve) and a 60~$\gev$ stop decaying as $\stop \rightarrow \mathrm{b}\ell\tilde{\nu}$ (dotted curve). (b) Efficiency for a 60 $\gev$ sbottom (solid curve) and a 50 $\gev$ sbottom (dashed curve) decaying as $\sbot \rightarrow \mathrm{b}\neu$.
000331194 8564_ $$82316624$$s18948$$uhttps://cds.cern.ch/record/331194/files/AlephStopFig4b.png$$y00007 \rm Excluded regions assuming $\stop \rightarrow \mathrm{c}\neu$. (a) Excluded region in the $m_{\neu}$ vs $m_{\stop}$ plane, including the region excluded by the D0 collaboration. (b) Excluded region in the $m_{\stop}$ vs $\mathrm \thetamix$ plane. (c) Excluded region in the $m_{\stop}$ vs $\deltm$ plane. In (a) and (c), excluded regions are given for $0^{\circ}$, corresponding to the maximum $\stop$-Z coupling, and for $56^{\circ}$, corresponding to the minimum $\stop$-Z coupling.
000331194 8564_ $$82316625$$s16699$$uhttps://cds.cern.ch/record/331194/files/AlephStopFig3b.png$$y00004 \rm Efficiencies as a function of $\deltm$. (a) Efficiency for a 65 $\gev$ stop decaying as $\stop \rightarrow \mathrm{c}\neu$ (solid curve), a 50 $\gev$ stop decaying as $\stop \rightarrow \mathrm{c}\neu$ (dashed curve) and a 60~$\gev$ stop decaying as $\stop \rightarrow \mathrm{b}\ell\tilde{\nu}$ (dotted curve). (b) Efficiency for a 60 $\gev$ sbottom (solid curve) and a 50 $\gev$ sbottom (dashed curve) decaying as $\sbot \rightarrow \mathrm{b}\neu$.
000331194 8564_ $$82316626$$s15369$$uhttps://cds.cern.ch/record/331194/files/AlephStopFig2a.png$$y00001 \rm (a) $\pt$ for $\ggqq$ and $\stop \rightarrow \mathrm{c}\neu$ at $\rts$ = 161~GeV. The solid histogram gives the $\ggqq$ distribution, the dashed histogram gives the signal distribution for \mbox{$\mstop$ = 65 $\gev$} and $\deltm$ = 5 $\gev$, the dotted histogram gives the signal distribution for \mbox{$\mstop$ = 65 $\gev$} and $\deltm$ = 15 $\gev$. The cut $\pt$ $>$ 2\%$\rts$ is indicated by the arrow. (b) $E_{\mathrm{iso}}$/$E_{\mathrm{lepton}}$ for $\qqg$ and $\stop \to \rm{b} \ell \tilde{\nu}$ at $\rts$ = 161~GeV. The solid histogram gives the $\qqg$ distribution, the dashed histogram gives the signal distribution for \mbox{$\mstop$ = 60 $\gev$} and $\deltm$ = 20 $\gev$. The cut $E_{\mathrm{iso}}$/$E_{\mathrm{lepton}}$ $<$ 4 is indicated by the arrow. In (a), the cut $\elow$ = 0 has been applied. In (b), at least one identified electron or muon is required. Normalization for the plots is arbitrary.
000331194 8564_ $$82316627$$s22211$$uhttps://cds.cern.ch/record/331194/files/AlephStopFig5c.png$$y00011 \rm Excluded regions assuming $\stop \rightarrow \mathrm{b}\ell\tilde{\nu}$. (a) Excluded region in the $m_{\tilde{\nu}}$ vs $m_{\stop}$ plane. (b) Excluded region in the $m_{\stop}$ vs $\mathrm \thetamix$ plane. (c) Excluded region in the $m_{\stop}$ vs $\deltm$ plane. In (a), (b) and (c) equal branching fractions for the $\stop$ decay to $\mathrm{e}$, $\mu$ or $\tau$ are assumed. (d) Excluded region in the $m_{\stop}$ vs $\deltm$ plane, assuming a branching ratio of 100\% for the $\stop$ decay to $\tau$. In (a), (c), and (d), excluded regions are given for $0^{\circ}$, corresponding to the maximum $\stop$-Z coupling, and for $56^{\circ}$, corresponding to the minimum $\stop$-Z coupling. Also shown in (a), (c), and (d) is the excluded region from LEP1, obtained from the measurement of the Z lineshape.
000331194 8564_ $$82316628$$s17781$$uhttps://cds.cern.ch/record/331194/files/AlephStopFig5b.png$$y00010 \rm Excluded regions assuming $\stop \rightarrow \mathrm{b}\ell\tilde{\nu}$. (a) Excluded region in the $m_{\tilde{\nu}}$ vs $m_{\stop}$ plane. (b) Excluded region in the $m_{\stop}$ vs $\mathrm \thetamix$ plane. (c) Excluded region in the $m_{\stop}$ vs $\deltm$ plane. In (a), (b) and (c) equal branching fractions for the $\stop$ decay to $\mathrm{e}$, $\mu$ or $\tau$ are assumed. (d) Excluded region in the $m_{\stop}$ vs $\deltm$ plane, assuming a branching ratio of 100\% for the $\stop$ decay to $\tau$. In (a), (c), and (d), excluded regions are given for $0^{\circ}$, corresponding to the maximum $\stop$-Z coupling, and for $56^{\circ}$, corresponding to the minimum $\stop$-Z coupling. Also shown in (a), (c), and (d) is the excluded region from LEP1, obtained from the measurement of the Z lineshape.
000331194 8564_ $$82316629$$s19839$$uhttps://cds.cern.ch/record/331194/files/AlephStopFig5a.png$$y00009 \rm Excluded regions assuming $\stop \rightarrow \mathrm{b}\ell\tilde{\nu}$. (a) Excluded region in the $m_{\tilde{\nu}}$ vs $m_{\stop}$ plane. (b) Excluded region in the $m_{\stop}$ vs $\mathrm \thetamix$ plane. (c) Excluded region in the $m_{\stop}$ vs $\deltm$ plane. In (a), (b) and (c) equal branching fractions for the $\stop$ decay to $\mathrm{e}$, $\mu$ or $\tau$ are assumed. (d) Excluded region in the $m_{\stop}$ vs $\deltm$ plane, assuming a branching ratio of 100\% for the $\stop$ decay to $\tau$. In (a), (c), and (d), excluded regions are given for $0^{\circ}$, corresponding to the maximum $\stop$-Z coupling, and for $56^{\circ}$, corresponding to the minimum $\stop$-Z coupling. Also shown in (a), (c), and (d) is the excluded region from LEP1, obtained from the measurement of the Z lineshape.
000331194 8564_ $$82316630$$s31097$$uhttps://cds.cern.ch/record/331194/files/AlephStopFig4a.png$$y00006 \rm Excluded regions assuming $\stop \rightarrow \mathrm{c}\neu$. (a) Excluded region in the $m_{\neu}$ vs $m_{\stop}$ plane, including the region excluded by the D0 collaboration. (b) Excluded region in the $m_{\stop}$ vs $\mathrm \thetamix$ plane. (c) Excluded region in the $m_{\stop}$ vs $\deltm$ plane. In (a) and (c), excluded regions are given for $0^{\circ}$, corresponding to the maximum $\stop$-Z coupling, and for $56^{\circ}$, corresponding to the minimum $\stop$-Z coupling.
000331194 8564_ $$82316631$$s5687$$uhttps://cds.cern.ch/record/331194/files/AlephStopFig1.png$$y00000 \rm Stop decay diagrams. (a) $\stop \rightarrow \mathrm{c}\neu$. (b) $\stop \to \rm{b} \ell \tilde{\nu}$. (c) $\stop \to \mathrm{b} \mathrm{f}_{1} \mathrm{f}_{2} \neutr$. Decay (c) is not considered in this paper.
000331194 8564_ $$82316632$$s19240$$uhttps://cds.cern.ch/record/331194/files/AlephStopFig4c.png$$y00008 \rm Excluded regions assuming $\stop \rightarrow \mathrm{c}\neu$. (a) Excluded region in the $m_{\neu}$ vs $m_{\stop}$ plane, including the region excluded by the D0 collaboration. (b) Excluded region in the $m_{\stop}$ vs $\mathrm \thetamix$ plane. (c) Excluded region in the $m_{\stop}$ vs $\deltm$ plane. In (a) and (c), excluded regions are given for $0^{\circ}$, corresponding to the maximum $\stop$-Z coupling, and for $56^{\circ}$, corresponding to the minimum $\stop$-Z coupling.
000331194 8564_ $$82316633$$s21339$$uhttps://cds.cern.ch/record/331194/files/AlephStopFig6b.png$$y00014 \rm Excluded regions assuming $\sbot \rightarrow \mathrm{b}\neu$. (a) Excluded region in the $m_{\neu}$ vs $m_{\sbot}$ plane. (b) Excluded region in the $m_{\sbot}$ vs $\mathrm \thetab$ plane. (c) Excluded region in the $m_{\sbot}$ vs $\deltm$ plane. In (a) and (c), excluded regions are given for $0^{\circ}$, corresponding to the maximum $\sbot$-Z coupling, and for $40^{\circ}$.
000331194 8564_ $$82316634$$s14300$$uhttps://cds.cern.ch/record/331194/files/AlephStopFig2b.png$$y00002 \rm (a) $\pt$ for $\ggqq$ and $\stop \rightarrow \mathrm{c}\neu$ at $\rts$ = 161~GeV. The solid histogram gives the $\ggqq$ distribution, the dashed histogram gives the signal distribution for \mbox{$\mstop$ = 65 $\gev$} and $\deltm$ = 5 $\gev$, the dotted histogram gives the signal distribution for \mbox{$\mstop$ = 65 $\gev$} and $\deltm$ = 15 $\gev$. The cut $\pt$ $>$ 2\%$\rts$ is indicated by the arrow. (b) $E_{\mathrm{iso}}$/$E_{\mathrm{lepton}}$ for $\qqg$ and $\stop \to \rm{b} \ell \tilde{\nu}$ at $\rts$ = 161~GeV. The solid histogram gives the $\qqg$ distribution, the dashed histogram gives the signal distribution for \mbox{$\mstop$ = 60 $\gev$} and $\deltm$ = 20 $\gev$. The cut $E_{\mathrm{iso}}$/$E_{\mathrm{lepton}}$ $<$ 4 is indicated by the arrow. In (a), the cut $\elow$ = 0 has been applied. In (b), at least one identified electron or muon is required. Normalization for the plots is arbitrary.
000331194 8564_ $$82316635$$s24687$$uhttps://cds.cern.ch/record/331194/files/AlephStopFig6a.png$$y00013 \rm Excluded regions assuming $\sbot \rightarrow \mathrm{b}\neu$. (a) Excluded region in the $m_{\neu}$ vs $m_{\sbot}$ plane. (b) Excluded region in the $m_{\sbot}$ vs $\mathrm \thetab$ plane. (c) Excluded region in the $m_{\sbot}$ vs $\deltm$ plane. In (a) and (c), excluded regions are given for $0^{\circ}$, corresponding to the maximum $\sbot$-Z coupling, and for $40^{\circ}$.
000331194 8564_ $$82316636$$s21767$$uhttps://cds.cern.ch/record/331194/files/AlephStopFig5d.png$$y00012 \rm Excluded regions assuming $\stop \rightarrow \mathrm{b}\ell\tilde{\nu}$. (a) Excluded region in the $m_{\tilde{\nu}}$ vs $m_{\stop}$ plane. (b) Excluded region in the $m_{\stop}$ vs $\mathrm \thetamix$ plane. (c) Excluded region in the $m_{\stop}$ vs $\deltm$ plane. In (a), (b) and (c) equal branching fractions for the $\stop$ decay to $\mathrm{e}$, $\mu$ or $\tau$ are assumed. (d) Excluded region in the $m_{\stop}$ vs $\deltm$ plane, assuming a branching ratio of 100\% for the $\stop$ decay to $\tau$. In (a), (c), and (d), excluded regions are given for $0^{\circ}$, corresponding to the maximum $\stop$-Z coupling, and for $56^{\circ}$, corresponding to the minimum $\stop$-Z coupling. Also shown in (a), (c), and (d) is the excluded region from LEP1, obtained from the measurement of the Z lineshape.
000331194 8564_ $$82316638$$s9563$$uhttps://cds.cern.ch/record/331194/files/fig00005.png$$y00005 noimgSummary of relative systematic uncertainties on the $\stop$ and $\sbot$ selection efficiencies. The ranges of variation are those used for the low $\deltm$ case.
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