arXiv:0712.3805v2 [hep-ex] 18 Feb 2008
Search for squarks and gluinos in events with jets and missing transverse energy
using 2.1 fb
−1of p ¯
p
collision data at
√
s
=1.96 TeV
V.M. Abazov36, B. Abbott76, M. Abolins66, B.S. Acharya29, M. Adams52, T. Adams50, E. Aguilo6, S.H. Ahn31,
M. Ahsan60, G.D. Alexeev36, G. Alkhazov40, A. Alton65,a, G. Alverson64, G.A. Alves2, M. Anastasoaie35,
L.S. Ancu35, T. Andeen54, S. Anderson46, B. Andrieu17, M.S. Anzelc54, Y. Arnoud14, M. Arov61, M. Arthaud18,
A. Askew50, B. ˚Asman41, A.C.S. Assis Jesus3, O. Atramentov50, C. Autermann21, C. Avila8, C. Ay24, F. Badaud13,
A. Baden62, L. Bagby53, B. Baldin51, D.V. Bandurin60, S. Banerjee29, P. Banerjee29, E. Barberis64, A.-F. Barfuss15,
P. Bargassa81, P. Baringer59, J. Barreto2, J.F. Bartlett51, U. Bassler18, D. Bauer44, S. Beale6, A. Bean59,
M. Begalli3, M. Begel72, C. Belanger-Champagne41, L. Bellantoni51, A. Bellavance51, J.A. Benitez66, S.B. Beri27,
G. Bernardi17, R. Bernhard23, I. Bertram43, M. Besan¸con18, R. Beuselinck44, V.A. Bezzubov39, P.C. Bhat51,
V. Bhatnagar27, C. Biscarat20, G. Blazey53, F. Blekman44, S. Blessing50, D. Bloch19, K. Bloom68, A. Boehnlein51,
D. Boline63, T.A. Bolton60, G. Borissov43, T. Bose78, A. Brandt79, R. Brock66, G. Brooijmans71, A. Bross51,
D. Brown82, N.J. Buchanan50, D. Buchholz54, M. Buehler82, V. Buescher22, V. Bunichev38, S. Burdin43,b,
S. Burke46, T.H. Burnett83, C.P. Buszello44, J.M. Butler63, P. Calfayan25, S. Calvet16, J. Cammin72, W. Carvalho3,
B.C.K. Casey51, N.M. Cason56, H. Castilla-Valdez33, S. Chakrabarti18, D. Chakraborty53, K.M. Chan56, K. Chan6,
A. Chandra49, F. Charles19,‡, E. Cheu46, F. Chevallier14, D.K. Cho63, S. Choi32, B. Choudhary28, L. Christofek78,
T. Christoudias44,†, S. Cihangir51, D. Claes68, Y. Coadou6, M. Cooke81, W.E. Cooper51, M. Corcoran81,
F. Couderc18, M.-C. Cousinou15, S. Cr´ep´e-Renaudin14, D. Cutts78, M. ´Cwiok30, H. da Motta2, A. Das46,
G. Davies44, K. De79, S.J. de Jong35, E. De La Cruz-Burelo65, C. De Oliveira Martins3, J.D. Degenhardt65,
F. D´eliot18, M. Demarteau51, R. Demina72, D. Denisov51, S.P. Denisov39, S. Desai51, H.T. Diehl51, M. Diesburg51,
A. Dominguez68, H. Dong73, L.V. Dudko38, L. Duflot16, S.R. Dugad29, D. Duggan50, A. Duperrin15, J. Dyer66,
A. Dyshkant53, M. Eads68, D. Edmunds66, J. Ellison49, V.D. Elvira51, Y. Enari78, S. Eno62, P. Ermolov38,
H. Evans55, A. Evdokimov74, V.N. Evdokimov39, A.V. Ferapontov60, T. Ferbel72, F. Fiedler24, F. Filthaut35,
W. Fisher51, H.E. Fisk51, M. Ford45, M. Fortner53, H. Fox23, S. Fu51, S. Fuess51, T. Gadfort71, C.F. Galea35,
E. Gallas51, E. Galyaev56, C. Garcia72, A. Garcia-Bellido83, V. Gavrilov37, P. Gay13, W. Geist19, D. Gel´e19,
C.E. Gerber52, Y. Gershtein50, D. Gillberg6, G. Ginther72, N. Gollub41, B. G´omez8, A. Goussiou56, P.D. Grannis73,
H. Greenlee51, Z.D. Greenwood61, E.M. Gregores4, G. Grenier20, Ph. Gris13, J.-F. Grivaz16, A. Grohsjean25,
S. Gr¨unendahl51, M.W. Gr¨unewald30, J. Guo73, F. Guo73, P. Gutierrez76, G. Gutierrez51, A. Haas71, N.J. Hadley62,
P. Haefner25, S. Hagopian50, J. Haley69, I. Hall66, R.E. Hall48, L. Han7, P. Hansson41, K. Harder45, A. Harel72,
R. Harrington64, J.M. Hauptman58, R. Hauser66, J. Hays44, T. Hebbeker21, D. Hedin53, J.G. Hegeman34,
J.M. Heinmiller52, A.P. Heinson49, U. Heintz63, C. Hensel59, K. Herner73, G. Hesketh64, M.D. Hildreth56,
R. Hirosky82, J.D. Hobbs73, B. Hoeneisen12, H. Hoeth26, M. Hohlfeld22, S.J. Hong31, S. Hossain76, P. Houben34,
Y. Hu73, Z. Hubacek10, V. Hynek9, I. Iashvili70, R. Illingworth51, A.S. Ito51, S. Jabeen63, M. Jaffr´e16, S. Jain76,
K. Jakobs23, C. Jarvis62, R. Jesik44, K. Johns46, C. Johnson71, M. Johnson51, A. Jonckheere51, P. Jonsson44,
A. Juste51, E. Kajfasz15, A.M. Kalinin36, J.R. Kalk66, J.M. Kalk61, S. Kappler21, D. Karmanov38, P.A. Kasper51,
I. Katsanos71, D. Kau50, R. Kaur27, V. Kaushik79, R. Kehoe80, S. Kermiche15, N. Khalatyan51, A. Khanov77,
A. Kharchilava70, Y.M. Kharzheev36, D. Khatidze71, T.J. Kim31, M.H. Kirby54, M. Kirsch21, B. Klima51,
J.M. Kohli27, J.-P. Konrath23, V.M. Korablev39, A.V. Kozelov39, D. Krop55, T. Kuhl24, A. Kumar70, S. Kunori62,
A. Kupco11, T. Kurˇca20, J. Kvita9,†, F. Lacroix13, D. Lam56, S. Lammers71, G. Landsberg78, P. Lebrun20,
W.M. Lee51, A. Leflat38, F. Lehner42, J. Lellouch17, J. Leveque46, J. Li79, Q.Z. Li51, L. Li49, S.M. Lietti5,
J.G.R. Lima53, D. Lincoln51, J. Linnemann66, V.V. Lipaev39, R. Lipton51, Y. Liu7,†, Z. Liu6, A. Lobodenko40,
M. Lokajicek11, P. Love43, H.J. Lubatti83, R. Luna3, A.L. Lyon51, A.K.A. Maciel2, D. Mackin81, R.J. Madaras47,
P. M¨attig26, C. Magass21, A. Magerkurth65, P.K. Mal56, H.B. Malbouisson3, S. Malik68, V.L. Malyshev36,
H.S. Mao51, Y. Maravin60, B. Martin14, R. McCarthy73, A. Melnitchouk67, L. Mendoza8, P.G. Mercadante5,
M. Merkin38, K.W. Merritt51, J. Meyer22,d, A. Meyer21, T. Millet20, J. Mitrevski71, J. Molina3, R.K. Mommsen45,
N.K. Mondal29, R.W. Moore6, T. Moulik59, G.S. Muanza20, M. Mulders51, M. Mulhearn71, O. Mundal22,
L. Mundim3, E. Nagy15, M. Naimuddin51, M. Narain78, N.A. Naumann35, H.A. Neal65, J.P. Negret8,
P. Neustroev40, H. Nilsen23, H. Nogima3, S.F. Novaes5, T. Nunnemann25, V. O’Dell51, D.C. O’Neil6, G. Obrant40,
P. Padley81, M. Pangilinan78, N. Parashar57, S.-J. Park72, S.K. Park31, J. Parsons71, R. Partridge78, N. Parua55,
A. Patwa74, G. Pawloski81, B. Penning23, M. Perfilov38, K. Peters45, Y. Peters26, P. P´etroff16, M. Petteni44,
R. Piegaia1, J. Piper66, M.-A. Pleier22, P.L.M. Podesta-Lerma33,c, V.M. Podstavkov51, Y. Pogorelov56,
M.-E. Pol2, P. Polozov37, B.G. Pope66, A.V. Popov39, C. Potter6, W.L. Prado da Silva3, H.B. Prosper50,
S. Protopopescu74, J. Qian65, A. Quadt22,d, B. Quinn67, A. Rakitine43, M.S. Rangel2, K. Ranjan28, P.N. Ratoff43,
P. Renkel80, S. Reucroft64, P. Rich45, J. Rieger55, M. Rijssenbeek73, I. Ripp-Baudot19, F. Rizatdinova77,
S. Robinson44, R.F. Rodrigues3, M. Rominsky76, C. Royon18, P. Rubinov51, R. Ruchti56, G. Safronov37,
G. Sajot14, A. S´anchez-Hern´andez33, M.P. Sanders17, A. Santoro3, G. Savage51, L. Sawyer61, T. Scanlon44,
D. Schaile25, R.D. Schamberger73, Y. Scheglov40, H. Schellman54, T. Schliephake26, C. Schwanenberger45,
A. Schwartzman69, R. Schwienhorst66, J. Sekaric50, H. Severini76, E. Shabalina52, M. Shamim60, V. Shary18,
A.A. Shchukin39, R.K. Shivpuri28, V. Siccardi19, V. Simak10, V. Sirotenko51, P. Skubic76, P. Slattery72,
D. Smirnov56, J. Snow75, G.R. Snow68, S. Snyder74, S. S¨oldner-Rembold45, L. Sonnenschein17, A. Sopczak43,
M. Sosebee79, K. Soustruznik9, B. Spurlock79, J. Stark14, J. Steele61, V. Stolin37, D.A. Stoyanova39,
J. Strandberg65, S. Strandberg41, M.A. Strang70, M. Strauss76, E. Strauss73, R. Str¨ohmer25, D. Strom54,
L. Stutte51, S. Sumowidagdo50, P. Svoisky56, A. Sznajder3, M. Talby15, P. Tamburello46, A. Tanasijczuk1,
W. Taylor6, J. Temple46, B. Tiller25, F. Tissandier13, M. Titov18, V.V. Tokmenin36, T. Toole62, I. Torchiani23,
T. Trefzger24, D. Tsybychev73, B. Tuchming18, C. Tully69, P.M. Tuts71, R. Unalan66, S. Uvarov40,
L. Uvarov40, S. Uzunyan53, B. Vachon6, P.J. van den Berg34, R. Van Kooten55, W.M. van Leeuwen34,
N. Varelas52, E.W. Varnes46, I.A. Vasilyev39, M. Vaupel26, P. Verdier20, L.S. Vertogradov36, M. Verzocchi51,
F. Villeneuve-Seguier44, P. Vint44, P. Vokac10, E. Von Toerne60, M. Voutilainen68,e, R. Wagner69, H.D. Wahl50,
L. Wang62, M.H.L.S Wang51, J. Warchol56, G. Watts83, M. Wayne56, M. Weber51, G. Weber24, L. Welty-Rieger55,
A. Wenger42, N. Wermes22, M. Wetstein62, A. White79, D. Wicke26, G.W. Wilson59, S.J. Wimpenny49,
M. Wobisch61, D.R. Wood64, T.R. Wyatt45, Y. Xie78, S. Yacoob54, R. Yamada51, M. Yan62, T. Yasuda51,
Y.A. Yatsunenko36, K. Yip74, H.D. Yoo78, S.W. Youn54, J. Yu79, A. Zatserklyaniy53, C. Zeitnitz26, T. Zhao83,
B. Zhou65, J. Zhu73, M. Zielinski72, D. Zieminska55, A. Zieminski55,‡, L. Zivkovic71, V. Zutshi53, and E.G. Zverev38 (The DØ Collaboration)
1Universidad de Buenos Aires, Buenos Aires, Argentina 2LAFEX, Centro Brasileiro de Pesquisas F´ısicas, Rio de Janeiro, Brazil
3Universidade do Estado do Rio de Janeiro, Rio de Janeiro, Brazil 4Universidade Federal do ABC, Santo Andr´e, Brazil
5Instituto de F´ısica Te´orica, Universidade Estadual Paulista, S˜ao Paulo, Brazil 6University of Alberta, Edmonton, Alberta, Canada,
Simon Fraser University, Burnaby, British Columbia, Canada, York University, Toronto, Ontario, Canada, and McGill University, Montreal, Quebec, Canada
7University of Science and Technology of China, Hefei, People’s Republic of China 8Universidad de los Andes, Bogot´a, Colombia
9Center for Particle Physics, Charles University, Prague, Czech Republic 10Czech Technical University, Prague, Czech Republic
11Center for Particle Physics, Institute of Physics,
Academy of Sciences of the Czech Republic, Prague, Czech Republic 12Universidad San Francisco de Quito, Quito, Ecuador 13LPC, Univ Blaise Pascal, CNRS/IN2P3, Clermont, France 14LPSC, Universit´e Joseph Fourier Grenoble 1, CNRS/IN2P3,
Institut National Polytechnique de Grenoble, France
15CPPM, IN2P3/CNRS, Universit´e de la M´editerran´ee, Marseille, France 16LAL, Univ Paris-Sud, IN2P3/CNRS, Orsay, France
17LPNHE, IN2P3/CNRS, Universit´es Paris VI and VII, Paris, France 18DAPNIA/Service de Physique des Particules, CEA, Saclay, France
19IPHC, Universit´e Louis Pasteur et Universit´e de Haute Alsace, CNRS/IN2P3, Strasbourg, France 20IPNL, Universit´e Lyon 1, CNRS/IN2P3, Villeurbanne, France and Universit´e de Lyon, Lyon, France
21III. Physikalisches Institut A, RWTH Aachen, Aachen, Germany 22Physikalisches Institut, Universit¨at Bonn, Bonn, Germany 23Physikalisches Institut, Universit¨at Freiburg, Freiburg, Germany
24Institut f¨ur Physik, Universit¨at Mainz, Mainz, Germany 25Ludwig-Maximilians-Universit¨at M¨unchen, M¨unchen, Germany
26Fachbereich Physik, University of Wuppertal, Wuppertal, Germany 27Panjab University, Chandigarh, India
28Delhi University, Delhi, India
29Tata Institute of Fundamental Research, Mumbai, India 30University College Dublin, Dublin, Ireland
31Korea Detector Laboratory, Korea University, Seoul, Korea 32SungKyunKwan University, Suwon, Korea
33CINVESTAV, Mexico City, Mexico
34FOM-Institute NIKHEF and University of Amsterdam/NIKHEF, Amsterdam, The Netherlands 35Radboud University Nijmegen/NIKHEF, Nijmegen, The Netherlands
36Joint Institute for Nuclear Research, Dubna, Russia 37Institute for Theoretical and Experimental Physics, Moscow, Russia
38Moscow State University, Moscow, Russia 39Institute for High Energy Physics, Protvino, Russia 40Petersburg Nuclear Physics Institute, St. Petersburg, Russia
41Lund University, Lund, Sweden, Royal Institute of Technology and Stockholm University, Stockholm, Sweden, and Uppsala University, Uppsala, Sweden
42Physik Institut der Universit¨at Z¨urich, Z¨urich, Switzerland 43Lancaster University, Lancaster, United Kingdom
44Imperial College, London, United Kingdom 45University of Manchester, Manchester, United Kingdom
46University of Arizona, Tucson, Arizona 85721, USA
47Lawrence Berkeley National Laboratory and University of California, Berkeley, California 94720, USA 48California State University, Fresno, California 93740, USA
49University of California, Riverside, California 92521, USA 50Florida State University, Tallahassee, Florida 32306, USA 51Fermi National Accelerator Laboratory, Batavia, Illinois 60510, USA
52University of Illinois at Chicago, Chicago, Illinois 60607, USA 53Northern Illinois University, DeKalb, Illinois 60115, USA
54Northwestern University, Evanston, Illinois 60208, USA 55Indiana University, Bloomington, Indiana 47405, USA 56University of Notre Dame, Notre Dame, Indiana 46556, USA
57Purdue University Calumet, Hammond, Indiana 46323, USA 58Iowa State University, Ames, Iowa 50011, USA 59University of Kansas, Lawrence, Kansas 66045, USA 60Kansas State University, Manhattan, Kansas 66506, USA 61Louisiana Tech University, Ruston, Louisiana 71272, USA 62University of Maryland, College Park, Maryland 20742, USA
63Boston University, Boston, Massachusetts 02215, USA 64Northeastern University, Boston, Massachusetts 02115, USA
65University of Michigan, Ann Arbor, Michigan 48109, USA 66Michigan State University, East Lansing, Michigan 48824, USA
67University of Mississippi, University, Mississippi 38677, USA 68University of Nebraska, Lincoln, Nebraska 68588, USA 69Princeton University, Princeton, New Jersey 08544, USA 70State University of New York, Buffalo, New York 14260, USA
71Columbia University, New York, New York 10027, USA 72University of Rochester, Rochester, New York 14627, USA 73State University of New York, Stony Brook, New York 11794, USA
74Brookhaven National Laboratory, Upton, New York 11973, USA 75Langston University, Langston, Oklahoma 73050, USA 76University of Oklahoma, Norman, Oklahoma 73019, USA 77Oklahoma State University, Stillwater, Oklahoma 74078, USA
78Brown University, Providence, Rhode Island 02912, USA 79University of Texas, Arlington, Texas 76019, USA 80Southern Methodist University, Dallas, Texas 75275, USA
81Rice University, Houston, Texas 77005, USA
82University of Virginia, Charlottesville, Virginia 22901, USA and 83University of Washington, Seattle, Washington 98195, USA
(Dated: January 24, 2008)
A data sample corresponding to an integrated luminosity of 2.1 fb−1collected by the D0 detector at the Fermilab Tevatron Collider was analyzed to search for squarks and gluinos produced in p¯p collisions at a center-of-mass energy of 1.96 TeV. No evidence for the production of such particles
was observed in topologies involving jets and missing transverse energy, and 95% C.L. lower limits of 379 GeV and 308 GeV were set on the squark and gluino masses, respectively, within the framework of minimal supergravity with tan β = 3, A0= 0, and µ < 0. The corresponding previous limits are improved by 54 GeV and 67 GeV.
PACS numbers: 14.80.Ly, 12.60.Jv, 13.85.Rm
In supersymmetric models [1], each of the standard model (SM) particles has a partner differing by a half-unit of spin. If R-parity [2] is conserved, supersymmetric particles are produced in pairs, and their decay leads to SM particles and to the lightest supersymmetric particle (LSP), which is stable. Cosmological arguments suggest that the LSP should be neutral and colorless [3]. The lightest neutralino ˜χ0
1, which is a mixture of the
super-partners of the neutral gauge and Higgs bosons, fulfills these conditions. In the following, it is assumed that R-parity is conserved and that ˜χ0
1 is the LSP. Since this
particle is weakly interacting, it escapes detection and provides the classic missing transverse energy ( /ET)
signa-ture at colliders. In p¯p collisions, squarks (˜q) and gluinos (˜g), the superpartners of quarks and gluons, would be abundantly produced, if sufficiently light, by the strong interaction, leading to final states containing jets and
/
ET. The most constraining direct limits on squark and
gluino masses were obtained by the D0 collaboration [4], based on an analysis of 310 pb−1 of data from p¯p
col-lisions at a center-of-mass energy of 1.96 TeV, collected during Run II of the Fermilab Tevatron Collider. In the model of minimal supergravity (mSUGRA) [5], the limits obtained were mq˜> 325 GeV and m˜g> 241 GeV at the
95% C.L., for the set of model parameters detailed below. In this Letter, an update of the D0 search for squarks and gluinos in topologies with jets and large /ET is reported,
using a seven times larger data set of 2.1 fb−1.
A detailed description of the D0 detector can be found in Ref. [6]. The central tracking system consists of a sil-icon microstrip tracker and a central fiber tracker, both located within a 2 T superconducting solenoidal magnet. A liquid-argon and uranium calorimeter covers pseudora-pidities up to |η| ≈ 4.2, where η = − ln [tan (θ/2)], and θ is the polar angle with respect to the proton beam direc-tion. The calorimeter consists of three sections, housed in separate cryostats: the central one covers |η| ∼< 1.1, and the two end sections extend the coverage to larger |η|. The calorimeter is segmented in depth, with four electromagnetic layers followed by up to five hadronic layers. It is also segmented in semi-projective towers of size 0.1 × 0.1 in the (η, φ) plane, where φ is the azimuthal angle in radians. Calorimeter cells are defined by the intersections of towers and layers. Additional sampling is provided by scintillating tiles between cryostats. An outer muon system, covering |η| < 2, consists of a layer of tracking detectors and scintillation trigger counters in front of 1.8 T iron toroids, followed by two similar lay-ers after the toroids. Jets were reconstructed with the
iterative midpoint cone algorithm [7] with cone radius R = p(∆φ)2+ (∆y)2 = 0.5 in azimuthal angle φ and
rapidity y = 1
2ln((E + pz)/(E − pz)). The jet energy
scale (JES) was derived from the transverse momentum balance in photon-plus-jet events. The /ET was
calcu-lated from all calorimeter cells, and corrected for the jet energy scale and for the transverse momenta of recon-structed muons.
The D0 trigger system consists of three levels, L1, L2 and L3. The 1.2 fb−1 of data recorded after 2006
(during the so-called Run IIb) were collected using a significantly upgraded system, in particular a new L1 calorimeter trigger [8] involving a sliding-window algo-rithm which improved the jet triggering efficiency. In ad-dition, /ET was used at L1 to select events, which was not
done during the previous data taking period (Run IIa). Both improvements helped to keep a high trigger effi-ciency despite the increased instantaneous luminosity in Run IIb (up to 2.8 × 1032cm−2s−1, to be compared to
1.6 × 1032cm−2s−1 in Run IIa). The events used in this
analysis were recorded using two categories of triggers [9]. The dijet triggers selected events with two jets and /ET,
while the multijet triggers were optimized for events with at least three jets and /ET.
The SM processes leading to events with jets and real /ET in the final state (“SM backgrounds”) are the
production of W or Z bosons in association with jets (W/Z+jets), of pairs of vector bosons (W W , W Z, ZZ) or top quarks (t¯t), and of single top quarks. The neu-trinos from the decays Z → ν ¯ν and W → lν, with the W boson produced directly or coming from a top quark decay, generate the /ET signature. In this analysis, most
of the W boson leptonic decays leading to an electron or a muon were identified, and the corresponding events rejected. However, a charged lepton from W boson de-cay can be a tau dede-caying hadronically. It can also be an electron or a muon that escapes detection or fails the identification criteria. Such W +jets events therefore ex-hibit the jets plus /ET signature. Finally, multijet
pro-duction also leads to a final state with jets and /ET when
one or more jets are mismeasured (“QCD background”). Events from SM and supersymmetric processes were simulated using Monte Carlo (MC) generators and passed through a full geant3-based [10] simulation of the de-tector geometry and response. They were subsequently processed with the same reconstruction chain as the data. The parton density functions (PDFs) used in the MC generators are the CTEQ6L1 [11] PDFs. A data event from a randomly selected beam crossing was overlaid on
each event to simulate the additional minimum bias in-teractions. The QCD background was not simulated, but estimated directly from data. The alpgen generator [12] was used to simulate W/Z+ jets and t¯t production. It was interfaced with pythia [13] for the simulation of initial and final state radiation (ISR/FSR) and of jet hadronization. Pairs of vector bosons and electroweak top quark production were simulated with pythia and comphep [14], respectively. The next-to-leading order (NLO) cross sections were computed with mcfm 5.1 [15]. Squark and gluino production and decay were simu-lated with pythia. The masses of the supersymmetric particles were calculated with suspect 2.3 [16] from the set of five mSUGRA parameters: m0, the universal scalar
mass at the grand unification scale ΛGUT; m1/2 the
uni-versal gaugino mass at ΛGUT; A0, the universal trilinear
coupling at ΛGUT; tan β, the ratio of the vacuum
ex-pectation values of the two Higgs fields; and µ the sign of the Higgs-mixing mass parameter. The decay widths and branching ratios of all supersymmetric particles were then calculated with sdecay 1.1a [17]. In order to allow for an easier comparison with previous results, the fol-lowing parameters were fixed to the same values as in Ref. [4]: A0 = 0, tan β = 3, and µ < 0. The
produc-tion of scalar top quarks (stops) was ignored, and in the following, the “squark mass” is the average mass of all squarks other than stops. All squark and gluino decay modes were taken into account, including cascade decays through charginos or neutralinos which could addition-ally produce electrons, muons, or taus. The NLO cross sections of the squark and gluino pair production were calculated with prospino 2 [18].
The analysis strategy is the same as in Ref. [4] with three analyses optimized for three benchmark regions of the mSUGRA parameter space. A “dijet” analysis was optimized at low m0 for events containing a pair of
acoplanar jets, as expected from p¯p → ˜q ˜q → q ˜χ0
1q ˜¯χ01 and
p¯p → ˜q ˜q → q ˜χ0
1q ˜χ01. A “gluino” analysis was optimized
at high m0for events with at least four jets, as expected
from p¯p → ˜g˜g → q ¯q ˜χ0
1q ¯q ˜χ01. Finally, a “3-jets” analysis
was optimized for events with at least three jets, as ex-pected from p¯p → ˜q˜g → q ˜χ0
1q ¯q ˜χ01. The benchmark for
this analysis is the case where mq˜= m˜g.
Each analysis required at least two jets and substan-tial /ET (≥ 40 GeV). The acoplanarity, i.e. the azimuthal
angle between the two leading jets, was required to be smaller than 165◦, where the two leading jets are those
with the largest transverse momenta. These leading jets were required: to be in the central region of the calorimeter, |ηdet| < 0.8, where ηdet is the jet
pseudo-rapidity calculated under the assumption that the jet originates from the detector center; to have fractions of energy in the electromagnetic layers of the calorimeter less than 0.95; and to have transverse momenta greater than 35 GeV. The best primary vertex (PV0) was se-lected among all reconstructed primary vertices (PV)
TABLE I: Selection criteria for the three analyses (all energies and momenta in GeV); see the text for further details.
Preselection Cut All Analyses
/
ET ≥ 40
|Vertex z pos.| < 60 cm
Acoplanarity < 165◦
Selection Cut “dijet” “3-jets” “gluino”
Trigger dijet multijet multijet
jet1 pT a ≥ 35 ≥ 35 ≥ 35 jet2 pTa ≥ 35 ≥ 35 ≥ 35 jet3 pT b − ≥ 35 ≥ 35 jet4 pT b − − ≥ 20
Electron veto yes yes yes
Muon veto yes yes yes
∆φ( /ET, jet1) ≥ 90◦ ≥ 90◦ ≥ 90◦
∆φ( /ET, jet2) ≥ 50◦ ≥ 50◦ ≥ 50◦
∆φmin( /ET, any jet) ≥ 40◦ − −
HT ≥ 325 ≥ 375 ≥ 400
/
ET ≥ 225 ≥ 175 ≥ 100
a
First and second jets are also required to be central (|ηdet| < 0.8),
with an electromagnetic fraction below 0.95, and to have CPF0 ≥ 0.75.
b
Third and fourth jets are required to have |ηdet| < 2.5, with an
electromagnetic fraction below 0.95.
as the one with the smallest probability to be due to a minimum bias interaction [19]. Its longitudinal posi-tion with respect to the detector center was restricted to |z| < 60 cm to ensure efficient reconstruction. For each jet, CPF0 is defined as the fraction of track pT sum
as-sociated with the jet which comes from PV0, CPF0= P ptrack
T (PV0)/P ptrackT (any PV). The two leading jets
were required to have CPF0 larger than 0.75. Since jet transverse momenta and /ET were calculated with respect
to PV0, this criterion reduced the background with large /
ET due to an incorrect PV0 selection.
Different selection criteria were applied in the three analyses, as summarized in Table I. Events passing a trigger for acoplanar dijet events were used in the “dijet” analysis, while a multijet and /ET trigger was required in
the “3-jets” and “gluino” analyses. In the “3-jets” and “gluino” analyses, a third and fourth jet were required, respectively. In comparison with the previously pub-lished analysis [4], the |ηdet| upper limit for the third and
fourth jet was increased from 0.8 to 2.5, which consider-ably improved the signal efficiency at high m0. These two
jets also had to have their fraction of energy in the elec-tromagnetic layers of the calorimeter less than 0.95, but no requirement was made on their CPF0. The third and fourth jet transverse momenta were required to exceed 35 GeV and 20 GeV, respectively. In all three analyses, a veto on isolated electrons or muons with pT > 10 GeV
was applied to reject background events containing a lep-tonic W boson decay. The azimuthal angles between the
/
ET and the first jet, ∆φ( /ET, jet1), and the second jet,
en-ergy of one jet was mismeasured, generating /ET aligned
with that jet. In the “dijet” analysis, the minimum az-imuthal angle ∆φmin( /ET, any jet) between the /ET and
any jet with pT > 15 GeV was required to be greater
than 40◦ to further suppress QCD background. This
cri-terion was not used in the “3-jets” and “gluino” analyses because of the higher jet multiplicity in the signal events. The two final cuts on /ET and on HT =PjetspT, where
the sum is over all jets with pT > 15 GeV and |ηdet| < 2.5,
were optimized by minimizing the expected upper limit on the cross section in the absence of signal. Here and in the calculation of the final limits, the modified frequentist CLsmethod [20] was used. The QCD background contri-bution was estimated by fitting the /ET distribution below
60 GeV with an exponential function, after subtraction of the SM background processes, and subsequently extrap-olating this function above the chosen /ET cut value. The
optimal cuts are given in Table I. The /ET distributions
after applying all analysis criteria except the one on /ET
are shown in Fig. 1 for the three analyses.
Table II reports the number of data events and the expected signal and background. The main background contributions are from (Z → ν ¯ν) + jets, (W → lν) + jets, and t¯t → b¯b q ¯q′lν. The QCD background was evaluated
from a fit to the /ET distribution as described above. The
largest QCD contribution of 1.4±0.8 event was estimated in the “gluino” analysis, but was conservatively ignored when setting the limits. It was found to be negligible in the “dijet” and “3-jets” analyses. The signal efficiencies are given in Table II for the three benchmark scenarios, with the corresponding values of m0, m1/2, the squark
and gluino masses, and the NLO cross section.
The uncertainty coming from the JES corrections is typically (10–15)% for the SM backgrounds and (6–11)% for the signal efficiencies. The uncertainties due to the jet energy resolution, to the jet track confirmation, and to jet reconstruction and identification efficiencies range between 2% and 4%. All these uncertainties on jet prop-erties account for differences between data and MC sim-ulation, both for signal efficiencies and background con-tributions. The trigger was found to be fully efficient for the event samples surviving all analysis cuts with an uncertainty of 2%. The uncertainty on the luminosity measurement is 6.1% [21]. All of these uncertainties are fully correlated between signal and SM backgrounds. A 15% systematic uncertainty was set on the W/Z+jets and t¯t NLO cross sections. The uncertainty on the signal acceptance due to the PDF choice was determined to be 6%, using the forty-eigenvector basis of the CTEQ6.1M PDF set [11]. Finally, the effects of ISR/FSR on the signal efficiencies were studied by varying the pythia parameters controlling the QCD scales and the maximal allowed virtualities used in the simulation of the space-like and time-space-like parton showers. The uncertainty on the signal efficiencies was determined to be 6%.
The nominal NLO signal cross sections, σnom, were
computed with the CTEQ6.1M PDF and for the renor-malization and factorization scale µr,f = Q, where Q was
taken to be equal to m˜gfor ˜g˜g production, m˜qfor ˜q ˜q and
˜
q ˜q production, and (mq˜+ mg˜)/2 for ˜q˜g production. The
uncertainty due to the choice of PDF was determined using the full set of CTEQ6.1M eigenvectors, with the individual uncertainties added in quadrature. The ef-fect on the nominal signal cross sections, which varies between 15% and 60%, is dominated by the large uncer-tainty on the gluon distribution at high x. The effect of the renormalization and factorization scale was stud-ied by calculating the signal cross sections for µr,f = Q,
µr,f = Q/2 and µr,f = 2 × Q. The factor of two on
this scale reduces or increases the nominal signal cross sections by (15–20)%. The PDF and µr,f effects were
added in quadrature to compute minimum, σmin, and
maximum, σmax, signal cross sections.
The numbers of events observed in the data are in agreement with the SM background expectation in the three analyses. Therefore, an excluded domain in the gluino-squark mass plane was determined as follows. The three analyses were run over signal MC samples gener-ated in the gluino-squark mass plane to compute signal efficiencies. Then, to take advantage of the different features of the three analyses, seven independent com-binations of the three selections were defined as shown in Table III, which were combined in the limit compu-tations. The number of events passing at least one of the three analyses is 31 while the SM expectation is 32.6 ± 1.7(stat.)+9.0−5.8(syst.) events. Figure 2 shows the
95% C.L. observed and expected upper limits on squark-gluino production cross sections for the three benchmark scenarios. Figure 3 shows the excluded domain in the gluino-squark mass plane.
The absolute lower limits on the squark and gluino masses obtained in the most conservative hypothesis, σmin, are 379 GeV and 308 GeV, respectively. The
corre-sponding expected limits are 377 GeV and 312 GeV. Ta-ble IV summarizes these absolute limits for the three sig-nal cross section hypotheses. Limits were also derived for the particular case mq˜= m˜g. For σmin, squark and gluino
masses below 390 GeV are excluded, while the expected limit is 390 GeV. The observed limit becomes 408 GeV for σnom, and 427 GeV for σmax.
The results of this analysis also constrain the mSUGRA parameters at the grand unification scale. Fig-ure 4 shows the excluded regions in the (m0, m1/2) plane
for tan β = 3, A0 = 0, µ < 0. Although a detailed scan
of the mSUGRA parameter space is beyond the scope of this analysis, it was verified that similar results hold for a large class of parameter sets. In particular, the fact that there is no explicit veto in this analysis on hadron-ically decaying tau leptons mitigates the expected effi-ciency reduction at larger values of tan β. It can be seen in Fig. 4 that the limits from LEP2 chargino and slepton searches [23] are improved for m0 values between 70 and
(GeV) T E 0 50 100 150 200 250 300 350 400 450 500 Events / 20 GeV -1 10 1 10 2 10 (GeV) T E 0 50 100 150 200 250 300 350 400 450 500 Events / 20 GeV -1 10 1 10 2 10 -1 DØ, L=2.1 fb Data SM Background Fitted QCD SUSY (a) (GeV) T E 0 50 100 150 200 250 300 350 400 450 500 Events / 20 GeV -1 10 1 10 2 10 3 10 (GeV) T E 0 50 100 150 200 250 300 350 400 450 500 Events / 20 GeV -1 10 1 10 2 10 3 10 DØ, L=2.1 fb -1 Data SM Background Fitted QCD SUSY (b) (GeV) T E 0 50 100 150 200 250 300 350 400 450 500 Events / 20 GeV -1 10 1 10 2 10 3 10 (GeV) T E 0 50 100 150 200 250 300 350 400 450 500 Events / 20 GeV -1 10 1 10 2 10 3 10 DØ, L=2.1 fb -1 Data SM Background Fitted QCD SUSY (c)
FIG. 1: Distributions of /ETafter applying all analysis criteria except the one on /ETfor the “dijet” (a), “3-jets” (b), and “gluino” (c) analyses; for data (points with error bars), for SM background (full histogram), and for signal MC (dotted histogram on top of SM). The signal drawn corresponds to (m0, m1/2) = (25, 175) GeV, mq˜= m˜g = 410 GeV, and (m0, m1/2) = (500, 110) GeV from left to right. The fitted QCD background contribution is also shown.
TABLE II: For each analysis, information on the signal for which it was optimized (m0, m1/2, m˜g, mq˜, and nominal NLO cross section), signal efficiency, the number of events observed, the number of events expected from SM backgrounds, the number of events expected from signal, and the 95% C.L. signal cross section upper limit. The first uncertainty is statistical and the second is systematic.
Analysis (m0, m1/2) (m˜g, mq˜) σnom ǫsig. Nobs. Nbackgrd. Nsig. σ95
(GeV) (GeV) (pb) (%) (pb)
“dijet” (25,175) (439,396) 0.072 6.8 ± 0.4+1.2−1.2 11 11.1 ± 1.2+2.9−2.3 10.4 ± 0.6+1.8−1.8 0.075 “3-jets” (197,154) (400,400) 0.083 6.8 ± 0.4+1.4−1.3 9 10.7 ± 0.9+3.1−2.1 12.0 ± 0.7+2.5−2.3 0.065 “gluino” (500,110) (320,551) 0.195 4.1 ± 0.3+0.8−0.7 20 17.7 ± 1.1+5.5−3.3 17.0 ± 1.2+3.3−2.9 0.165
TABLE III: Definition of the analysis combinations, and number of events observed in the data and expected from the SM backgrounds.
Selection “dijet” “3-jets” “gluino” Nobs. Nbackgrd.
Combination 1 yes no no 8 9.4 ± 1.2 (stat.) +2.3
−1.8(syst.)
Combination 2 no yes no 2 4.5 ± 0.6 (stat.) +0.7−0.5(syst.)
Combination 3 no no yes 14 12.5 ± 0.9 (stat.) +3.6−1.9(syst.)
Combination 4 yes yes no 1 1.1 ± 0.3 (stat.) +0.5−0.3(syst.)
Combination 5 yes no yes kinematically not allowed
Combination 6 no yes yes 4 4.5 ± 0.6 (stat.) +1.8
−1.3(syst.)
Combination 7 yes yes yes 2 0.6 ± 0.2 (stat.) +0.1
−0.2(syst.)
At least one selection 31 32.6 ± 1.7 (stat.) +9.0−5.8(syst.)
Squark Mass (GeV) 320 340 360 380 400 420 440 Cross Section (pb) 0.1 0.2 0.3 -1 DØ, L=2.1 fb <0 µ )=3, β =0, tan( 0 =25, A 0 m NLO σ Observed limit Expected limit (a)
Squark-Gluino Mass (GeV)
320 340 360 380 400 420 440 Cross Section (pb) 0.1 0.2 0.3 0.4 -1 DØ, L=2.1 fb <0 µ )=3, β =0, tan( 0 , A g ~ =m q ~ m NLO σ Observed limit Expected limit (b)
Gluino Mass (GeV) 240 260 280 300 320 340 360 Cross Section (pb) 0.5 1 1.5 2 -1 DØ, L=2.1 fb <0 µ )=3, β =0, tan( 0 =500, A 0 m NLO σ Observed limit Expected limit (c)
FIG. 2: For tan β = 3, A0 = 0, µ < 0, observed (closed circles) and expected (opened triangles) 95% C.L. upper limits on squark-gluino production cross sections combining the analyses for m0 = 25 GeV (a), mq˜ = mg˜ (b), and m0 = 500 GeV (c). The nominal production cross sections are also shown, with shaded bands corresponding to the PDF and renormalization-and-factorization scale uncertainties.
TABLE IV: Absolute lower limits at the 95% C.L. on the squark and gluino masses (in GeV) as a function of the choice of signal cross section hypothesis as defined in the text. Num-bers in parentheses correspond to the expected limits. These limits are valid for the mSUGRA parameters tan β = 3, A0 = 0, µ < 0.
Hypothesis Gluino mass Squark mass
σmin 308 (312) 379 (377)
σnom 327 (332) 392 (391)
σmax 349 (354) 406 (404)
Gluino Mass (GeV)
0
100 200 300 400 500 600
Squark Mass (GeV)
0
100
200
300
400
500
600
-1DØ, L=2.1 fb
<0
µ
=0,
0=3, A
β
tan
UA1 UA2 LEP CDF IB DØ IA DØ IB DØ II no mSUGRA solution ± χ∼ LEP2 ± l ~ LEP2FIG. 3: In the gluino and squark mass plane, excluded regions at the 95% C.L. by direct searches in the mSUGRA frame-work with tan β = 3, A0= 0, µ < 0. The region excluded by this analysis and previous D0 Run II results [4] in the most conservative hypothesis (σmin) is shown in dark shading. The thick (dotted) line is the limit of the observed (expected) ex-cluded region for the σnomhypothesis. The band delimited by the two dashed lines shows the effect of the PDF choice and of the variation of µr,f by a factor of two. Regions excluded by previous experiments are indicated in light shading [22]. The two thin lines indicate the indirect limits inferred from the LEP2 chargino and slepton searches [23]. The region where no mSUGRA solution can be found is shown hatched.
300 GeV and for m1/2 values between 125 and 165 GeV.
However, the LEP2 Higgs search limits remain more con-straining in a purely mSUGRA scenario [23].
In summary, a search for squarks and gluinos pro-duced in p¯p collisions at 1.96 TeV has been performed in a 2.1 fb−1data sample. The results of three selections of
events with jets and large missing transverse energy are in agreement with the SM background predictions. In the framework of minimal supergravity with tan β = 3,
(GeV)
0m
0
100
200
300
400
500
600
(GeV)
1/2m
0
50
100
150
200
250
(GeV)
0m
0
100
200
300
400
500
600
(GeV)
1/2m
0
50
100
150
200
250
-1DØ, L=2.1 fb
<0
µ
=0,
0=3, A
β
tan
no EWSB ± χ∼ LEP2 ± l ~ LEP2 DØ IIFIG. 4: In the (m0, m1/2) plane, the region excluded by this analysis at the 95% C.L. in the mSUGRA framework for tan β = 3, A0 = 0, µ < 0 is shown in dark shading. The thick line is the limit of the excluded region for the σnom hy-pothesis. The corresponding expected limit is the dashed line. The band delimited by the two dotted lines shows the effect of the PDF choice and of the variation of µr,fby a factor of two. Regions excluded by the LEP2 chargino and slepton searches are indicated in light shading [23]. The region where there is no electroweak symmetry breaking is shown in black.
A0= 0, and µ < 0, 95% C.L. lower limits of 392 GeV and
327 GeV were set on the squark and gluino masses, re-spectively, for the central choice of PDF and for a renor-malization and factorization scale equal to the mass of the squark or gluino produced. Taking into account the PDF uncertainties and allowing for a factor of two in the choice of scale, these limits are reduced to 379 GeV and 308 GeV. They exceed the corresponding previous limits [4] by 54 GeV and 67 GeV and are the most con-straining direct limits on the squark and gluino masses to date.
We thank the staffs at Fermilab and collaborating in-stitutions, and acknowledge support from the DOE and NSF (USA); CEA and CNRS/IN2P3 (France); FASI, Rosatom and RFBR (Russia); CAPES, CNPq, FAPERJ, FAPESP and FUNDUNESP (Brazil); DAE and DST (India); Colciencias (Colombia); CONACyT (Mexico); KRF and KOSEF (Korea); CONICET and UBACyT (Argentina); FOM (The Netherlands); Science and Tech-nology Facilities Council (United Kingdom); MSMT and GACR (Czech Republic); CRC Program, CFI, NSERC and WestGrid Project (Canada); BMBF and DFG (Ger-many); SFI (Ireland); The Swedish Research Council (Sweden); CAS and CNSF (China); and the Alexander von Humboldt Foundation.
[a] Visitor from Augustana College, Sioux Falls, SD, USA. [b] Visitor from The University of Liverpool, Liverpool, UK.
[c] Visitor from ICN-UNAM, Mexico City, Mexico.
[d] Visitor from II. Physikalisches Institut, Georg-August-University, G¨ottingen, Germany.
[e] Visitor from Helsinki Institute of Physics, Helsinki, Fin-land.
[†] Fermilab International Fellow. [‡] Deceased.
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