Search for the supersymmetric partner of the top quark in ppbar collisions at sqrt(s) = 1.96 TeV

H. P. Nilles, Phys. Rep. 110

1985

Earlier work this paper cites.

J. Ellis and S. Rudaz, Phys. Lett. B 128

1990

Earlier work this paper cites.

W. Beenakker, M. Kr a ¨ \rm\ddot{a} mer, T. Plehn, M. Spira, and P. M. Zerwas, Nucl. Phys. B 515

1998

Cited alongside, same era.

LEPSUSYWG, ALEPH, DELPHI, L3 and OPAL experiments, note LEPSUSYWG/04-01.1; note LEPSUSYWG/04-02.1; note LEPSUSYWG/01-03.1 (http://lepsusy.web.cern.ch/lepsusy/Welcome.html)

Cited in the paper.

CDF uses a cylindrical coordinate system in which ϕ \phi is the azimuthal angle, r r is the radius from the nominal beam line, and z z points in the proton beam direction. The transverse ( r − ϕ r-\phi ) plane is perpendicular to the z z axis. Transverse momentum and energy are the respective projections of momentum measured in the tracking system and energy measured in the calorimeter system onto the r − ϕ r-\phi plane, and are defined as p T p_{\mathrm{T}} = p ​ sin ⁡ θ p\sin\theta and E T E_{\mathrm{T}} = E ​ sin ⁡ θ E\sin\theta . Here, θ \theta is the polar angle measured with respect to the interaction vertex. Missing transverse energy ( OPEN ) ​ i ​ s ​ d ​ e ​ f ​ i ​ n ​ e ​ d ​ b ​ y )isdefinedby = − Σ i ​ E T i ​ n i → -\Sigma_{i}E_{\mathrm{T}}^{i}\overrightarrow{n_{i}} , where i i is the calorimeter tower and n → i \overrightarrow{n}_{i} is a unit vector perpendicular to the beam axis and pointing at the i i th tower. The pseudorapidity η \eta is defined as -ln(tan( θ / 2 \theta/2 )), where θ \theta is measured with respect to the origin of the detector. We define the magnitude ／ \not E T E_{\mathrm{T}} = | | — . 7 [7] CDF F . A b e e t a l . , N u c l . I n s t r u m . M e t h o d s P h y s . R e s . A 271,387 ( 1988 ) ; D . A m i d e i e t a l . , N u c l . I n s t u m . M e t h o d s P h y s . R e s . A 𝟑𝟓𝟎 , 73 ( 1994 ) ; F . A b e e t a l . , P h y s . R e v . D 𝟓𝟐 , 4784 ( 1995 ) ; P . A z z i e t a l . , N u c l . I n s t r u m . M e t h o d s P h y s . R e s . A 360,137 ( 1995 ) ; T h e C D F I I D e t e c t o r T e c h n i c a l D e s i g n R e p o r t , F e r m i l a b − P u b − 96 / 390 − E ; A . A b u l e n c i a e t a l . , J . P h y s . G N u c l . P a r t . P h y s .34 , 2457 ( 2007 ) . 8 [8] id_effic D . A c o s t a e t a l . , P h y s . R e v . D 𝟕𝟐 , 052003 ( 2005 ) ; T . A a l t o n e n e t a l . , P h y s . R e v . D 𝟕𝟗 , 052004 ( 2009 ) . 9 [9] jes A . B h a t t i e t a l . , N u c l . I n s t r u m . M e t h o d s P h y s . R e s . A 566,375 ( 2006 ) . 10 [10] pythia T . S j ö s t r a n d , L . L ö n n b l a d a n d S . M r e n n a , J . H i g h E n e r g y P h y s .05,026 ( 2006 ) . pythia v e r s i o n 6.126 w a s u s e d i n t h i s a n a l y s i s . 11 [11] geant S . A g o s t i n e l l i e t a l . , N u c l . I n s t r u m . M e t h o d s P h y s . R e s . A 506,250 ( 2003 ) ; J . A l l i s o n e t a l . , I E E E T r a n s . N u c l . S c i .1,270 ( 2006 ) . 12 [12] ttbar M . C a c c i a r i e t a l . , J . H i g h E n e r g y P h y s .04,068 ( 2004 ) . 13 [13] k-factor F . A b e e t a l . , P h y s . R e v . D 𝟓𝟗 , 052002 ( 1999 ) . 14 [14] WW J . M . C a m p b e l l a n d R . K . E l l i s , P h y s . R e v . D 𝟔𝟎 , 113006 ( 1999 ) ; S . E i d e l m a n e t a l . ( P a r t i c l e D a t a G r o u p ) , P h y s . L e t t . B 𝟓𝟗𝟐 , 1 ( 2004 ) . 15 [15] baur U . B a u r a n d E . L . B e r g e r , P h y s . R e v . D 𝟒𝟏 , 1476 ( 1990 ) ; U . B a u r , T . H a n , a n d J . O h n e m u s , P h y s . R e v . D 𝟒𝟖 , 5140 ( 1993 ) . 16 [16] Prospino1 W . B e e n a k k e r , R . H ö p k e r , M . S p i r a , a n d P . M . Z e r w a s , N u c l . P h y s . B 𝟒𝟗𝟐 , 51 ( 1997 ) . 17 [17] prospino W . B e e n a k k e r , R . H ö p k e r , a n d M . S p i r a , a r X i v : h e p − p h / 9611232 v 1 . prospino v e r s i o n 2 w a s u s e d i n t h i s a n a l y s i s . 18 [18] cteq J . P u m p l i n , D . R . S t u m p , J . H u s t o n , H . L . L a i , P . N a d o l s k y , a n d W . K . T u n g , J . H i g h E n e r g y P h y s .07,012 ( 2002 ) , D . S t u m p , J . H u s t o n , J . P u m p l i n , W . K . T u n g , H . L . L a i , S . K u h l m a n n , a n d J . F . O w e n s , J . H i g h E n e r g y P h y s .10,046 ( 2003 ) . 19 [19] Bayes J . C o n w a y , C E R N R e p o r t N o .2000 − 005 , 2000 , p .247 . .\par\par\reset@natbib@cites\@@lbibitem{CDF}\NAT@@wrout{7}{}{}{}{[7]}{CDF}\lx@bibnewblock F.Abe\emph{etal.},Nucl.Instrum.MethodsPhys.Res.A{\bf 271},387(1988);D.Amidei\emph{etal.},Nucl.Instum.MethodsPhys.Res.A{\bf 350},73(1994);F.Abe\emph{etal.},Phys.Rev.D{\bf 52},4784(1995);P.Azzi\emph{etal.},Nucl.Instrum.MethodsPhys.Res.A{\bf 360},137(1995);TheCDFIIDetectorTechnicalDesignReport,Fermilab-Pub-96/390-E;A.Abulencia\emph{etal.},J.Phys.GNucl.Part.Phys.{\bf 34},2457(2007).\par\par\reset@natbib@cites\@@lbibitem{id_effic}\NAT@@wrout{8}{}{}{}{[8]}{id_effic}\lx@bibnewblock D.Acosta\emph{etal.},Phys.Rev.D{\bf 72},052003(2005);T.Aaltonen\emph{etal.},Phys.Rev.D{\bf 79},052004(2009).\par\reset@natbib@cites\@@lbibitem{jes}\NAT@@wrout{9}{}{}{}{[9]}{jes}\lx@bibnewblock A.Bhatti\emph{etal.},Nucl.Instrum.MethodsPhys.Res.A{\bf 566},375(2006).\par\reset@natbib@cites\@@lbibitem{pythia}\NAT@@wrout{10}{}{}{}{[10]}{pythia}\lx@bibnewblock T.Sj\"{o}strand,L.L\"{o}nnbladandS.Mrenna,J.HighEnergyPhys.{\bf 05},026(2006).{\sc pythia}version6.126wasusedinthisanalysis.\par\reset@natbib@cites\@@lbibitem{geant}\NAT@@wrout{11}{}{}{}{[11]}{geant}\lx@bibnewblock S.Agostinelli\emph{etal.},Nucl.Instrum.MethodsPhys.Res.A{\bf 506},250(2003);J.Allison\emph{etal.},IEEETrans.Nucl.Sci.{\bf 1},270(2006).\par\reset@natbib@cites\@@lbibitem{ttbar}\NAT@@wrout{12}{}{}{}{[12]}{ttbar}\lx@bibnewblock M.Cacciari\emph{etal.},J.HighEnergyPhys.{\bf 04},068(2004).\par\reset@natbib@cites\@@lbibitem{k-factor}\NAT@@wrout{13}{}{}{}{[13]}{k-factor}\lx@bibnewblock F.Abe\emph{etal.},Phys.Rev.D{\bf 59},052002(1999).\par\reset@natbib@cites\@@lbibitem{WW}\NAT@@wrout{14}{}{}{}{[14]}{WW}\lx@bibnewblock J.M.CampbellandR.K.Ellis,Phys.Rev.D{\bf 60},113006(1999);S.Eidelman\emph{etal.}(ParticleDataGroup),Phys.Lett.B{\bf 592},1(2004).\par\reset@natbib@cites\@@lbibitem{baur}\NAT@@wrout{15}{}{}{}{[15]}{baur}\lx@bibnewblock U.BaurandE.L.Berger,Phys.Rev.D{\bf 41},1476(1990);U.Baur,T.Han,andJ.Ohnemus,Phys.Rev.D{\bf 48},5140(1993).\par\par\reset@natbib@cites\@@lbibitem{Prospino1}\NAT@@wrout{16}{}{}{}{[16]}{Prospino1}\lx@bibnewblock W.Beenakker,R.H\"{o}pker,M.Spira,andP.M.Zerwas,Nucl.Phys.B{\bf 492},51(1997).\par\par\reset@natbib@cites\@@lbibitem{prospino}\NAT@@wrout{17}{}{}{}{[17]}{prospino}\lx@bibnewblock W.Beenakker,R.H\"{o}pker,andM.Spira,arXiv:hep-ph/9611232v1.{\sc prospino}version2wasusedinthisanalysis.\par\reset@natbib@cites\@@lbibitem{cteq}\NAT@@wrout{18}{}{}{}{[18]}{cteq}\lx@bibnewblock J.Pumplin,D.R.Stump,J.Huston,H.L.Lai,P.Nadolsky,andW.K.Tung,J.HighEnergyPhys.{\bf 07},012(2002),D.Stump,J.Huston,J.Pumplin,W.K.Tung,H.L.Lai,S.Kuhlmann,andJ.F.Owens,J.HighEnergyPhys.{\bf 10},046(2003).\par\par\reset@natbib@cites\@@lbibitem{Bayes}\NAT@@wrout{19}{}{}{}{[19]}{Bayes}\lx@bibnewblock J.Conway,CERNReportNo.2000-005,2000,p.247.\par\endthebibliography\par\par\par\@add@PDF@RDFa@triples\par\end{document}

Cited in the paper.

T. Affolder et al. (CDF Collaboration), Phys. Rev Lett. 84

2004

Later among the works it cites.