Search for a dark matter candidate produced in association with a single top quark in pp collisions at √[s]=1.96 TeV.
Aaltonen T,Alvarez González B,Amerio S,Amidei D,Anastassov A,Annovi A,Antos J,Anzá F,Apollinari G,Appel J A,Arisawa T,Artikov A,Asaadi J,Ashmanskas W,Auerbach B,Aurisano A,Azfar F,Badgett W,Bae T,Barbaro-Galtieri A,Barnes V E,Barnett B A,Barria P,Bartos P,Bauce M,Bedeschi F,Behari S,Bellettini G,Bellinger J,Benjamin D,Beretvas A,Bhatti A,Bisello D,Bizjak I,Bland K R,Blumenfeld B,Bocci A,Bodek A,Bortoletto D,Boudreau J,Boveia A,Brigliadori L,Bromberg C,Brucken E,Budagov J,Budd H S,Burkett K,Busetto G,Bussey P,Buzatu A,Calamba A,Calancha C,Camarda S,Campanelli M,Campbell M,Canelli F,Carls B,Carlsmith D,Carosi R,Carrillo S,Carron S,Casal B,Casarsa M,Castro A,Catastini P,Cauz D,Cavaliere V,Cavalli-Sforza M,Cerri A,Cerrito L,Chen Y C,Chertok M,Chiarelli G,Chlachidze G,Chlebana F,Cho K,Chokheli D,Chung W H,Chung Y S,Ciocci M A,Clark A,Clarke C,Compostella G,Convery M E,Conway J,Corbo M,Cordelli M,Cox C A,Cox D J,Crescioli F,Cuevas J,Culbertson R,Dagenhart D,d'Ascenzo N,Datta M,de Barbaro P,Dell'Orso M,Demortier L,Deninno M,Devoto F,d'Errico M,Di Canto A,Di Ruzza B,Dittmann J R,D'Onofrio M,Donati S,Dong P,Dorigo M,Dorigo T,Ebina K,Elagin A,Eppig A,Erbacher R,Errede S,Ershaidat N,Eusebi R,Farrington S,Feindt M,Fernandez J P,Field R,Flanagan G,Forrest R,Frank M J,Franklin M,Freeman J C,Fuks B,Funakoshi Y,Furic I,Gallinaro M,Garcia J E,Garfinkel A F,Garosi P,Gerberich H,Gerchtein E,Giagu S,Giakoumopoulou V,Giannetti P,Gibson K,Ginsburg C M,Giokaris N,Giromini P,Giurgiu G,Glagolev V,Glenzinski D,Gold M,Goldin D,Goldschmidt N,Golossanov A,Gomez G,Gomez-Ceballos G,Goncharov M,González O,Gorelov I,Goshaw A T,Goulianos K,Grinstein S,Grosso-Pilcher C,Group R C,Guimaraes da Costa J,Hahn S R,Halkiadakis E,Hamaguchi A,Han J Y,Happacher F,Hara K,Hare D,Hare M,Harr R F,Hatakeyama K,Hays C,Heck M,Heinrich J,Herndon M,Hewamanage S,Hocker A,Hopkins W,Horn D,Hou S,Hughes R E,Hurwitz M,Husemann U,Hussain N,Hussein M,Huston J,Introzzi G,Iori M,Ivanov A,James E,Jang D,Jayatilaka B,Jeon E J,Jindariani S,Jones M,Joo K K,Jun S Y,Junk T R,Kamon T,Karchin P E,Kasmi A,Kato Y,Ketchum W,Keung J,Khotilovich V,Kilminster B,Kim D H,Kim H S,Kim J E,Kim M J,Kim S B,Kim S H,Kim Y K,Kim Y J,Kimura N,Kirby M,Klimenko S,Knoepfel K,Kondo K,Kong D J,Konigsberg J,Kotwal A V,Kreps M,Kroll J,Krop D,Kruse M,Krutelyov V,Kuhr T,Kurata M,Kwang S,Laasanen A T,Lami S,Lammel S,Lancaster M,Lander R L,Lannon K,Lath A,Latino G,LeCompte T,Lee E,Lee H S,Lee J S,Lee S W,Leo S,Leone S,Lewis J D,Limosani A,Lin C-J,Lindgren M,Lipeles E,Lister A,Litvintsev D O,Liu C,Liu H,Liu Q,Liu T,Lockwitz S,Loginov A,Lucchesi D,Lueck J,Lujan P,Lukens P,Lungu G,Lys J,Lysak R,Madrak R,Maeshima K,Maestro P,Malik S,Manca G,Manousakis-Katsikakis A,Margaroli F,Marino C,Martínez M,Mastrandrea P,Matera K,Mattson M E,Mazzacane A,Mazzanti P,McFarland K S,McIntyre P,McNulty R,Mehta A,Mehtala P,Mesropian C,Miao T,Mietlicki D,Mitra A,Miyake H,Moed S,Moggi N,Mondragon M N,Moon C S,Moore R,Morello M J,Morlock J,Movilla Fernandez P,Mukherjee A,Muller Th,Murat P,Mussini M,Nachtman J,Nagai Y,Naganoma J,Nakano I,Napier A,Nett J,Neu C,Neubauer M S,Nielsen J,Nodulman L,Noh S Y,Norniella O,Oakes L,Oh S H,Oh Y D,Oksuzian I,Okusawa T,Orava R,Ortolan L,Pagan Griso S,Pagliarone C,Palencia E,Papadimitriou V,Paramonov A A,Patrick J,Pauletta G,Paulini M,Paus C,Pellett D E,Penzo A,Phillips T J,Piacentino G,Pianori E,Pilot J,Pitts K,Plager C,Pondrom L,Poprocki S,Potamianos K,Prokoshin F,Pranko A,Ptohos F,Punzi G,Rahaman A,Ramakrishnan V,Ranjan N,Redondo I,Renton P,Rescigno M,Riddick T,Rimondi F,Ristori L,Robson A,Rodrigo T,Rodriguez T,Rogers E,Rolli S,Roser R,Ruffini F,Ruiz A,Russ J,Rusu V,Safonov A,Sakumoto W K,Sakurai Y,Santi L,Sato K,Saveliev V,Savoy-Navarro A,Schlabach P,Schmidt A,Schmidt E E,Schwarz T,Scodellaro L,Scribano A,Scuri F,Seidel S,Seiya Y,Semenov A,Sforza F,Shalhout S Z,Shears T,Shepard P F,Shimojima M,Shochet M,Shreyber-Tecker I,Simonenko A,Sinervo P,Sliwa K,Smith J R,Snider F D,Soha A,Sorin V,Song H,Squillacioti P,Stancari M,St Denis R,Stelzer B,Stelzer-Chilton O,Stentz D,Strologas J,Strycker G L,Sudo Y,Sukhanov A,Suslov I,Takemasa K,Takeuchi Y,Tang J,Tecchio M,Teng P K,Thom J,Thome J,Thompson G A,Thomson E,Toback D,Tokar S,Tollefson K,Tomura T,Tonelli D,Torre S,Torretta D,Totaro P,Trovato M,Ukegawa F,Uozumi S,Varganov A,Vázquez F,Velev G,Vellidis C,Vidal M,Vila I,Vilar R,Vizán J,Vogel M,Volpi G,Wagner P,Wagner R L,Wakisaka T,Wallny R,Wang S M,Warburton A,Waters D,Wester W C,Whiteson D,Wicklund A B,Wicklund E,Wilbur S,Wick F,Williams H H,Wilson J S,Wilson P,Winer B L,Wittich P,Wolbers S,Wolfe H,Wright T,Wu X,Wu Z,Yamamoto K,Yamato D,Yang T,Yang U K,Yang Y C,Yao W-M,Yeh G P,Yi K,Yoh J,Yorita K,Yoshida T,Yu G B,Yu I,Yu S S,Yun J C,Zanetti A,Zeng Y,Zhou C,Zucchelli S,Null Null
Physical review letters(2012)
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摘要
We report a new search for dark matter in a data sample of an integrated luminosity of 7.7 fb-1 of Tevatron pp[over ¯] collisions at √[s]=1.96 TeV, collected by the CDF II detector. We search for production of a dark-matter candidate, D, in association with a single top quark. We consider the hadronic decay mode of the top quark exclusively, yielding a final state of three jets with missing transverse energy. The data are consistent with the standard model; we thus set 95% confidence level upper limits on the cross section of the process pp[over ¯]→t+D as a function of the mass of the dark-matter candidate. The limits are approximately 0.5 pb for a dark-matter particle with mass in the range of 0-150 GeV/c2.