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WillE. WilliamsH.H. WilliamsW. WillisS. WillocqJ.A. WilsonM.G. WilsonA. WilsonI. Wingerter-SeezS. WinkelmannF. WinklmeierM. WittgenM.W. WolterH. WoltersW.C. WongG. WoodenB.K. WosiekJ. WotschackM.J. WoudstraK.W. WozniakK. WraightC. WrightM. WrightB. WronaS.L. WuX. WuY. WuE. WulfR. WunstorfB.M. WynneS. XellaM. XiaoS. XieY. XieC. XuD. XuG. XuB. YabsleyS. YacoobM. YamadaH. YamaguchiA. YamamotoK. YamamotoS. YamamotoT. YamamuraT. YamanakaJ. YamaokaT. YamazakiY. YamazakiZ. YanH. YangU.K. YangY. YangY. YangZ. YangS. YanushY. YaoY. YasuG.V. Ybeles SmitJ. YeS. YeM. YilmazR. YoosoofmiyaK. YoritaR. YoshidaC. YoungC.J. YoungS. YoussefD. YuJ. YuJ. YuL. YuanA. YurkewiczB. ZabinskiV.G. ZaetsR. ZaidanA.M. ZaitsevZ. ZajacovaL. ZanelloA. ZaytsevC. ZeitnitzM. ZellerM. ZemanA. ZemlaC. ZendlerO. ZeninT. ŽenišZ. ZinonosS. ZenzD. ZerwasG. Zevi della PortaZ. ZhanD. ZhangH. ZhangJ. ZhangX. ZhangZ. ZhangL. ZhaoT. ZhaoZ. ZhaoA. ZhemchugovS. ZhengJ. ZhongB. ZhouN. ZhouY. ZhouC.G. ZhuH. ZhuJ. ZhuY. ZhuX. ZhuangV. ZhuravlovD. ZieminskaR. ZimmermannS. ZimmermannS. ZimmermannM. ZiolkowskiR. ZitounL. ŽivkovićV.V. ZmouchkoG. ZobernigA. ZoccoliA. ZseneiM. zur NeddenV. ZutshiL. ZwalinskiSupersymmetryGMSBTau leptonPhysics Letters B 714 (2012) 197-214. doi:10.1016/j.physletb.2012.06.061journalPhysics Letters BPublished by Elsevier B.V.Elsevier B.V.0370-26937142-514 August 20122012-08-14197-21419721410.1016/j.physletb.2012.06.061http://dx.doi.org/10.1016/j.physletb.2012.06.061doi:10.1016/j.physletb.2012.06.061http://vtw.elsevier.com/data/voc/oa/OpenAccessStatus#Full2013-07-16T20:28:17Zhttp://vtw.elsevier.com/data/voc/oa/SponsorType#Otherhttp://creativecommons.org/licenses/by/3.0/

Journals

S300.3

PLB28701S0370-2693(12)00700-910.1016/j.physletb.2012.06.061Experiments

Fig. 1

Output distribution of the BDT used to discriminate W+jets from top-quark events in the low-mT control region, defined as mT<70 GeV. Background distributions are taken from simulation. The yield for W+jets and top backgrounds are taken from a maximum-likelihood fit to this distribution. The solid (red) line with shaded (yellow) error band corresponds to the total SM prediction, while the points are data. (For interpretation of the references to color in this figure, the reader is referred to the web version of this Letter.)

Fig. 2

Distributions of ETmiss, pTτ, and meff for data with all selection requirements except for that on meff, along with the corresponding estimated backgrounds. Backgrounds are taken from simulation and normalized with control regions in data. The solid (red) line with shaded (yellow) error band corresponds to the total SM prediction, while the points are data. The error bands indicate the size of the total (statistical and systematic) uncertainty. The notation GMSB(40,30) stands for the GMSB model with Λ=40 TeV and tanβ=30 and analogously for GMSB(30,20). (For interpretation of the references to color in this figure, the reader is referred to the web version of this Letter.)

Fig. 3

Expected and observed 95% C.L. exclusion limits in the Mmess=250 TeV, N5=3, μ>0, Cgrav=1 slice of GMSB, together with the most stringent previous limits from OPAL [32]. The identity of the NLSP is indicated, with CoNLSP the region where the τ˜ and ℓ˜ are nearly degenerate.

Table 1

Numbers of observed and expected events in the true-τ-dominated W/top control region, defined as mT<70 GeV. The numbers shown for W+jets and top are from Monte Carlo simulation and do not include the correction factors derived from this control region. The correction factors obtained from a fit to data are 1.22±0.13 for top and 0.71±0.03 for W+jets. The true-τ purity is 97% for top, 96% for W+jets and 87% for Z+jets.

TopW+jetsZ+jetsMultijetData186.4 ± 8.4919 ± 4062.2 ± 6.71.8 ± 1.8951Table 2

Numbers of observed and expected events in the fake-τ-enhanced control region. The numbers of expected W+jets and top-quark events have been corrected by the correction factors measured in the true-τ-dominated region. The fake-τ correction factor obtained from data is 0.50±0.08.

True τFake τTotalTop53.3±7.537.8±5.891.1±9.4W+jets80.5±6.933.3±4.1113.8±8.0Z+jets5.1±1.641.5±10.846.6±10.9Multijet0±02.9±1.02.9±1.0Total139±10116±13254±17Data197Table 3

Expected SM background event yields and number of events observed in data after the final requirement on meff. All systematic uncertainties are included here, and the uncertainty on ΣSM, the sum of all SM backgrounds, takes correlations between the individual background uncertainties into account. The true-τ purities are 53% and 64% for the top and W+jets backgrounds, respectively, and are negligible for the Z+jets and multijet backgrounds. For comparison, the estimated event yield for a GMSB signal with Λ=40 TeV, tanβ=30 is an additional 9.1±1.7 events.

TopW+jetsZ+jetsMultijetΣSMData5.6±1.44.7±1.52.4±0.70.5±0.613.2±4.211

☆

Search for supersymmetry with jets, missing transverse momentum and at least one hadronically decaying τ lepton in proton–proton collisions at s=7 TeV with the ATLAS detector

ATLAS Collaboration

⋆

E-mail address:atlas.publications@cern.ch.

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Djobava

51b

M.A.B.

do Vale

23c

Do Valle Wemans

123a

T.K.O.

Doan

Dobbs

Dobinson

⁎

Dobos

Dobson

Dodd

Doglioni

Doherty

Doi

⁎

Dolejsi

125

Dolenc

Dolezal

125

B.A.

Dolgoshein

⁎

Dohmae

154

Donadelli

23d

Donega

119

Donini

Dopke

Doria

101a

Dos Anjos

171

Dosil

Dotti

121a

121b

M.T.

Dova

A.D.

Doxiadis

104

A.T.

Doyle

Drasal

125

Drees

173

Dressnandt

119

Drevermann

Driouichi

Dris

Dubbert

Dube

Duchovni

170

Duckeck

Dudarev

Dudziak

Dührssen

I.P.

Duerdoth

Duflot

114

M-A.

Dufour

Dunford

Duran Yildiz

Duxfield

138

Dwuznik

Dydak

Düren

W.L.

Ebenstein

Ebke

Eckweiler

Edmonds

C.A.

Edwards

N.C.

Edwards

Ehrenfeld

Ehrich

Eifert

142

Eigen

Einsweiler

Eisenhandler

Ekelof

165

El Kacimi

134c

Ellert

165

Elles

Ellinghaus

Ellis

Elmsheuser

Elsing

Emeliyanov

128

Engelmann

147

Engl

Epp

Eppig

Erdmann

Ereditato

Eriksson

145a

Ernst

Ernwein

135

Errede

164

Errede

164

Ertel

Escalier

114

Escobar

122

Espinal Curull

Esposito

Etienne

A.I.

Etienvre

135

Etzion

152

Evangelakou

Evans

Fabbri

19a

19b

Fabre

R.M.

Fakhrutdinov

127

Falciano

131a

Fang

171

Fanti

88a

88b

Farbin

Farilla

133a

Farley

147

Farooque

157

Farrell

162

S.M.

Farrington

117

Farthouat

Fassnacht

Fassouliotis

Fatholahzadeh

157

Favareto

88a

88b

Fayard

114

Fazio

36a

36b

Febbraro

Federic

143a

O.L.

Fedin

120

Fedorko

Fehling-Kaschek

Feligioni

Fellmann

Feng

32d

E.J.

Feng

A.B.

Fenyuk

127

Ferencei

143b

Ferland

Fernando

108

Ferrag

Ferrando

Ferrara

Ferrari

165

Ferrari

104

Ferrari

118a

D.E.

Ferreira de Lima

Ferrer

166

M.L.

Ferrer

Ferrere

Ferretti

Ferretto Parodi

50a

50b

Fiascaris

Fiedler

Filipčič

Filippas

Filthaut

103

Fincke-Keeler

168

M.C.N.

Fiolhais

123a

Fiorini

166

Firan

Fischer

M.J.

Fisher

108

Flechl

Fleck

140

Fleckner

Fleischmann

172

Fleischmann

173

Flick

173

Floderus

L.R.

Flores Castillo

171

M.J.

Flowerdew

Fokitis

Fonseca Martin

D.A.

Forbush

137

Formica

135

Forti

Fortin

158a

J.M.

Foster

Fournier

114

Foussat

A.J.

Fowler

136

Fox

Francavilla

Franchino

118a

118b

Francis

Frank

170

Franklin

Franz

Fraternali

118a

118b

Fratina

119

S.T.

French

Friedrich

Froeschl

Froidevaux

J.A.

Frost

Fukunaga

155

Fullana Torregrosa

B.G.

Fulsom

142

Fuster

166

Gabaldon

Gabizon

170

Gadfort

Gadomski

Gagliardi

50a

50b

Gagnon

Galea

E.J.

Gallas

117

Gallo

B.J.

Gallop

128

Gallus

124

K.K.

Gan

108

Y.S.

Gao

142

V.A.

Gapienko

127

Gaponenko

Garberson

174

Garcia-Sciveres

García

166

J.E.

García Navarro

166

R.W.

Gardner

Garelli

Garitaonandia

104

Garonne

Garvey

Gatti

Gaudio

118a

Gaur

140

Gauthier

135

Gauzzi

131a

131b

I.L.

Gavrilenko

Gay

167

Gaycken

J-C.

Gayde

E.N.

Gazis

32d

Gecse

167

C.N.P.

Gee

128

D.A.A.

Geerts

104

Ch.

Geich-Gimbel

Gellerstedt

145a

145b

Gemme

50a

Gemmell

M.H.

Genest

Gentile

131a

131b

George

Gerlach

173

Gershon

152

Geweniger

58a

Ghazlane

134b

Ghodbane

Giacobbe

19a

Giagu

131a

131b

Giakoumopoulou

Giangiobbe

Gianotti

Gibbard

Gibson

157

S.M.

Gibson

L.M.

Gilbert

117

Gilewsky

Gillberg

A.R.

Gillman

128

D.M.

Gingrich

Ginzburg

152

Giokaris

M.P.

Giordani

163c

Giordano

101a

101b

F.M.

Giorgi

Giovannini

P.F.

Giraud

135

Giugni

88a

Giunta

Giusti

19a

B.K.

Gjelsten

116

L.K.

Gladilin

Glasman

Glatzer

Glazov

K.W.

Glitza

173

G.L.

Glonti

J.R.

Goddard

Godfrey

141

Godlewski

Goebel

Göpfert

Goeringer

Gössling

Göttfert

Goldfarb

Golling

174

Gomes

123a

L.S.

Gomez Fajardo

Gonçalo

Goncalves Pinto Firmino Da Costa

Gonella

Gonidec

Gonzalez

171

González de la Hoz

166

Gonzalez Parra

M.L.

Gonzalez Silva

Gonzalez-Sevilla

J.J.

Goodson

147

Goossens

P.A.

Gorbounov

H.A.

Gordon

Gorelov

102

Gorfine

173

Gorini

71a

71b

Gorišek

Gornicki

V.N.

Goryachev

127

Gosdzik

A.T.

Goshaw

Gosselink

104

M.I.

Gostkin

Gough Eschrich

162

Gouighri

134a

Goujdami

134c

M.P.

Goulette

A.G.

Goussiou

137

Goy

Gozpinar

Grabowska-Bold

Grafström

K-J.

Grahn

Grancagnolo

71a

Grancagnolo

Grassi

147

Gratchev

120

Grau

H.M.

Gray

J.A.

Gray

147

Graziani

133a

O.G.

Grebenyuk

120

Greenshaw

Z.D.

Greenwood

Gregersen

I.M.

Gregor

Grenier

142

Griffiths

137

Grigalashvili

A.A.

Grillo

136

Grinstein

Y.V.

Grishkevich

J.-F.

Grivaz

114

Gross

170

Grosse-Knetter

Groth-Jensen

170

Grybel

140

V.J.

Guarino

Guest

174

Guicheney

Guida

71a

71b

Guindon

Guler

Gunther

124

Guo

157

Guo

Gupta

Gusakov

V.N.

Gushchin

127

Gutierrez

110

Guttman

152

Gutzwiller

171

Guyot

135

Gwenlan

117

C.B.

Gwilliam

Haas

142

Haas

Haber

H.K.

Hadavand

D.R.

Hadley

Haefner

Hahn

Haider

Hajduk

Hakobyan

175

Hall

117

Haller

Hamacher

173

Hamal

112

Hamer

Hamilton

144b

Hamilton

160

Han

32a

Han

32b

Hanagaki

115

Hanawa

159

Hance

Handel

Hanke

58a

J.R.

Hansen

J.B.

Hansen

J.D.

Hansen

P.H.

Hansen

Hansson

142

Hara

159

G.A.

Hare

136

Harenberg

173

Harkusha

Harper

R.D.

Harrington

O.M.

Harris

137

Harrison

Hartert

Hartjes

104

Haruyama

Harvey

Hasegawa

100

Hasegawa

139

Hassani

135

Hatch

Hauff

Haug

Hauschild

Hauser

Havranek

B.M.

Hawes

117

C.M.

Hawkes

R.J.

Hawkings

A.D.

Hawkins

162

Hayakawa

Hayashi

159

Hayden

H.S.

Hayward

S.J.

Haywood

128

Hazen

32d

S.J.

Head

Hedberg

Heelan

Heim

Heinemann

Heisterkamp

Helary

Heller

Hellman

145a

145b

Hellmich

Helsens

R.C.W.

Henderson

Henke

58a

Henrichs

A.M.

Henriques Correia

Henrot-Versille

114

Henry-Couannier

Hensel

Henß

173

C.M.

Hernandez

Hernández Jiménez

166

Herrberg

Herten

Hertenberger

Hervas

G.G.

Hesketh

N.P.

Hessey

104

Higón-Rodriguez

166

Hill

⁎

J.C.

Hill

K.H.

Hiller

Hillert

S.J.

Hillier

Hinchliffe

Hines

119

Hirose

115

Hirsch

Hirschbuehl

173

Hobbs

147

Hod

152

M.C.

Hodgkinson

138

Hodgson

138

Hoecker

M.R.

Hoeferkamp

102

Hoffman

Hoffmann

Hohlfeld

Holder

140

S.O.

Holmgren

145a

Holy

126

J.L.

Holzbauer

Homma

T.M.

Hong

119

Hooft van Huysduynen

107

Horazdovsky

126

Horn

142

Horner

J-Y.

Hostachy

Hou

150

M.A.

Houlden

Hoummada

134a

Howarth

D.F.

Howell

117

Hristova

Hrivnac

114

Hruska

124

Hrynʼova

P.J.

Hsu

S.-C.

Hsu

G.S.

Huang

110

Hubacek

126

Hubaut

Huegging

Huettmann

T.B.

Huffman

117

E.W.

Hughes

R.E.

Hughes-Jones

Huhtinen

Hurst

Hurwitz

Husemann

Huseynov

Huston

Huth

Iacobucci

Iakovidis

Ibbotson

Ibragimov

140

Ichimiya

Iconomidou-Fayard

114

Idarraga

114

Iengo

101a

Igonkina

104

Ikegami

Ikeno

Ilchenko

Iliadis

153

Ilic

157

Imori

154

Ince

Inigo-Golfin

Ioannou

Iodice

133a

Iordanidou

Ippolito

131a

131b

Irles Quiles

166

Isaksson

165

Ishikawa

Ishino

Ishmukhametov

Issever

117

Istin

18a

A.V.

Ivashin

127

Iwanski

Iwasaki

J.M.

Izen

Izzo

101a

Jackson

119

J.N.

Jackson

142

M.R.

Jaekel

Jain

Jakobs

Jakobsen

Jakubek

126

D.K.

Jana

110

Jansen

Jantsch

Janus

Jarlskog

Jeanty

Jelen

Jen-La Plante

Jenni

Jeremie

Jež

Jézéquel

M.K.

Jha

19a

171

Jia

147

Jiang

32b

Jimenez Belenguer

Jin

32b

Jin

32a

Jinnouchi

156

M.D.

Joergensen

Joffe

L.G.

Johansen

145a

145b

K.E.

Johansson

145a

Johansson

138

Johnert

K.A.

Johns

Jon-And

145a

145b

Jones

117

R.W.L.

Jones

T.W.

Jones

T.J.

Jones

Jonsson

Joram

P.M.

Jorge

123a

Joseph

K.D.

Joshi

Jovicevic

146

Jovin

12b

171

C.A.

Jung

R.M.

Jungst

Juranek

124

Jussel

Juste Rozas

V.V.

Kabachenko

127

Kabana

Kaci

166

Kaczmarska

Kadlecik

Kado

114

Kagan

108

Kagan

Kaiser

Kajomovitz

151

Kalinin

173

L.V.

Kalinovskaya

Kama

Kanaya

154

Kaneda

Kaneti

Kanno

156

V.A.

Kantserov

Kanzaki

Kaplan

174

Kapliy

Kaplon

Kar

Karagounis

Karagoz

117

Karnevskiy

Kartvelishvili

A.N.

Karyukhin

127

Kashif

171

Kasieczka

58b

R.D.

Kass

108

Kastanas

Kataoka

154

Katsoufis

Katzy

Kaushik

Kawagoe

Kawamoto

154

Kawamura

M.S.

Kayl

104

V.A.

Kazanin

106

M.Y.

Kazarinov

Keeler

168

Kehoe

Keil

G.D.

Kekelidze

J.S.

Keller

137

Kennedy

Kenyon

Kepka

124

Kerschen

B.P.

Kerševan

Kersten

173

Kessoku

154

Keung

157

Khalil-zada

Khandanyan

164

Khanov

111

Kharchenko

Khodinov

A.G.

Kholodenko

127

Khomich

58a

T.J.

Khoo

Khoriauli

Khoroshilov

173

Khovanskiy

Khramov

Khubua

51b

Kim

145a

145b

M.S.

Kim

S.H.

Kim

159

Kimura

169

Kind

B.T.

King

R.S.B.

King

117

Kirk

128

L.E.

Kirsch

A.E.

Kiryunin

Kishimoto

Kisielewska

Kittelmann

122

A.M.

Kiver

127

Kladiva

143b

Klein

Kleinknecht

Klemetti

Klier

170

Klimek

145a

145b

Klimentov

Klingenberg

J.A.

Klinger

E.B.

Klinkby

Klioutchnikova

P.F.

Klok

103

Klous

104

E.-E.

Kluge

58a

Kluge

Kluit

104

Kluth

N.S.

Knecht

157

Kneringer

Knobloch

E.B.F.G.

Knoops

Knue

B.R.

Kobayashi

154

Kobel

Kocian

142

Kodys

125

Köneke

A.C.

König

103

Koenig

Köpke

Koetsveld

103

Koevesarki

Koffas

Koffeman

104

L.A.

Kogan

117

Kohlmann

173

Kohn

Kohout

126

Kohriki

Koi

142

Kokott

G.M.

Kolachev

106

Kolanoski

Kolesnikov

Koletsou

88a

Koll

Kollefrath

S.D.

Kolya

A.A.

Komar

Komori

154

Kondo

Kono

A.I.

Kononov

Konoplich

107

Konstantinidis

Kootz

173

Koperny

Korcyl

Kordas

153

Koreshev

127

Korn

117

Korol

106

Korolkov

E.V.

Korolkova

138

V.A.

Korotkov

127

Kortner

V.V.

Kostyukhin

M.J.

Kotamäki

Kotov

V.M.

Kotov

Kotwal

Kourkoumelis

Kouskoura

153

Koutsman

158a

Kowalewski

168

T.Z.

Kowalski

Kozanecki

135

A.S.

Kozhin

127

Kral

126

V.A.

Kramarenko

Kramberger

M.W.

Krasny

Krasznahorkay

107

Kraus

J.K.

Kraus

Krejci

126

Kretzschmar

Krieger

157

Kroeninger

Kroha

Kroll

119

Kroseberg

Krstic

12a

Kruchonak

Krüger

Kruker

Krumnack

Z.V.

Krumshteyn

Kruth

Kubota

Kuday

Kuehn

Kugel

58c

Kuhl

Kuhn

Kukhtin

Kulchitsky

Kuleshov

31b

Kummer

Kuna

Kundu

117

Kunkle

119

Kupco

124

Kurashige

Kurata

159

Y.A.

Kurochkin

Kus

124

E.S.

Kuwertz

146

Kuze

156

Kvita

141

Kwee

La Rosa

La Rotonda

36a

36b

Labarga

Labbe

Lablak

134a

Lacasta

166

Lacava

131a

131b

Lacker

Lacour

V.R.

Lacuesta

166

Ladygin

Lafaye

Laforge

Lagouri

Lai

Laisne

Lamanna

Lambourne

C.L.

Lampen

Lampl

Lancon

135

Landgraf

M.P.J.

Landon

J.L.

Lane

Lange

A.J.

Lankford

162

Lanni

Lantzsch

173

Laplace

Lapoire

J.F.

Laporte

135

Lari

88a

A.V.

Larionov

127

Larner

117

Lasseur

Lassnig

Laurelli

Lavorini

36a

36b

Lavrijsen

Laycock

A.B.

Lazarev

Le Dortz

Le Guirriec

Le Maner

157

Le Menedeu

Lebel

LeCompte

Ledroit-Guillon

Lee

104

J.S.H.

Lee

115

S.C.

Lee

150

Lee

174

Lefebvre

168

Legendre

135

Leger

B.C.

LeGeyt

119

Legger

Leggett

Lehmacher

Lehmann Miotto

Lei

M.A.L.

Leite

23d

Leitner

125

Lellouch

170

Leltchouk

Lemmer

Lendermann

58a

K.J.C.

Leney

144b

Lenz

104

Lenzen

173

Lenzi

Leonhardt

Leontsinis

Leroy

J-R.

Lessard

168

Lesser

145a

C.G.

Lester

C.M.

Lester

119

Levêque

Levin

L.J.

Levinson

170

M.S.

Levitski

127

Lewis

117

G.H.

Lewis

107

A.M.

Leyko

Leyton

171

32b

Liang

117

Liao

Liberti

132a

Lichard

Lichtnecker

Lie

164

Liebig

Limbach

Limosani

Limper

S.C.

Lin

150

Linde

104

J.T.

Linnemann

Lipeles

119

Lipinsky

124

Lipniacka

T.M.

Liss

164

Lissauer

Lister

A.M.

Litke

136

Liu

150

Liu

J.B.

Liu

32b

Liu

32b

Livan

118a

118b

S.S.A.

Livermore

117

Lleres

Llorente Merino

S.L.

Lloyd

Lobodzinska

Loch

W.S.

Lockman

136

Loddenkoetter

F.K.

Loebinger

Loginov

174

C.W.

Loh

167

Lohse

Lohwasser

Lokajicek

124

Loken

117

V.P.

Lombardo

R.E.

Long

Lopes

123a

Lopez Mateos

Lorenz

Lorenzo Martinez

114

Losada

161

Loscutoff

Lo Sterzo

131a

131b

M.J.

Losty

158a

Lou

Lounis

114

K.F.

Loureiro

161

Love

P.A.

Love

A.J.

Lowe

142

32a

H.J.

Lubatti

137

Luci

131a

131b

Lucotte

Ludwig

Luehring

Luijckx

104

Lukas

Lumb

Luminari

131a

Lund

116

Lund-Jensen

146

Lundberg

145a

145b

Lundquist

Lungwitz

Lutz

Lynn

Lys

Lytken

L.L.

171

J.A.

Macana Goia

Maccarrone

Macchiolo

Maček

Machado Miguens

123a

Mackeprang

R.J.

Madaras

W.F.

Mader

Maenner

58c

Maeno

Mättig

173

Mättig

Magnoni

Magradze

Mahalalel

152

Mahboubi

Mahmoud

Mahout

Maiani

131a

131b

Maidantchik

23a

Maio

123a

Majewski

Makida

Makovec

114

Mal

135

Malaescu

Pa.

Malecki

V.P.

Maleev

120

Malek

Mallik

Malon

Malone

142

Maltezos

Malyshev

106

Malyukov

Mameghani

Mamuzic

12b

Manabe

Mandelli

88a

Mandić

Mandrysch

Maneira

123a

P.S.

Mangeard

Manhaes de Andrade Filho

23a

I.D.

Manjavidze

Mann

P.M.

Manning

136

Manousakis-Katsikakis

Mansoulie

135

Manz

Mapelli

March

J.F.

Marchand

Marchese

132a

132b

Marchiori

Marcisovsky

124

C.P.

Marino

168

Marroquim

23a

Marshall

F.K.

Martens

157

Marti-Garcia

166

A.J.

Martin

174

Martin

F.F.

Martin

119

J.P.

Martin

Ph.

Martin

T.A.

Martin

V.J.

Martin

Martin dit Latour

Martin-Haugh

148

Martinez

Martinez Outschoorn

A.C.

Martyniuk

168

Marx

Marzano

131a

Marzin

110

Masetti

Mashimo

154

Mashinistov

Masik

A.L.

Maslennikov

106

Massa

19a

19b

Massaro

104

Massol

Mastrandrea

131a

131b

Mastroberardino

36a

36b

Masubuchi

154

Matricon

114

Matsumoto

154

Matsunaga

154

Matsushita

Mattravers

117

J.M.

Maugain

Maurer

S.J.

Maxfield

D.A.

Maximov

106

E.N.

May

Mayne

138

Mazini

150

Mazur

Mazzaferro

132a

132b

Mazzanti

88a

S.P.

Mc Kee

McCarn

164

R.L.

McCarthy

147

T.G.

McCarthy

N.A.

McCubbin

128

K.W.

McFarlane

J.A.

Mcfayden

138

McGlone

Mchedlidze

51b

R.A.

McLaren

Mclaughlan

S.J.

McMahon

128

R.A.

McPherson

168

Meade

Mechnich

104

Mechtel

173

Medinnis

Meera-Lebbai

110

Meguro

115

Mehdiyev

Mehlhase

Mehta

Meier

58a

Meirose

Melachrinos

B.R.

Mellado Garcia

171

Meloni

88a

88b

Mendoza Navas

161

Meng

150

Mengarelli

19a

19b

Menke

Menot

Meoni

K.M.

Mercurio

Mermod

Merola

101a

101b

Meroni

88a

F.S.

Merritt

108

Messina

Metcalfe

102

A.S.

Mete

Meyer

J-P.

Meyer

135

Meyer

172

Meyer

T.C.

Meyer

W.T.

Meyer

Miao

32d

Michal

Micu

25a

R.P.

Middleton

128

Migas

Mijović

Mikenberg

170

Mikestikova

124

Mikuž

D.W.

Miller

R.J.

Miller

W.J.

Mills

167

Mills

Milov

170

D.A.

Milstead

145a

145b

Milstein

170

A.A.

Minaenko

127

Miñano Moya

166

I.A.

Minashvili

A.I.

Mincer

107

Mindur

Mineev

Ming

171

L.M.

Mir

Mirabelli

131a

Miralles Verge

Misiejuk

Mitrevski

136

G.Y.

Mitrofanov

127

V.A.

Mitsou

166

Mitsui

P.S.

Miyagawa

138

Miyazaki

J.U.

Mjörnmark

Moa

145a

145b

Mockett

137

Moed

Moeller

Mönig

Möser

Mohapatra

147

Mohr

Mohrdieck-Möck

Moles-Valls

166

Molina-Perez

Monk

Monnier

Montesano

88a

88b

Monticelli

Monzani

19a

19b

R.W.

Moore

G.F.

Moorhead

Mora Herrera

Moraes

Morange

135

Morel

Morello

36a

36b

Moreno

Moreno Llácer

166

Morettini

50a

Morgenstern

Morii

Morin

A.K.

Morley

Mornacchi

S.V.

Morozov

J.D.

Morris

Morvaj

100

H.G.

Moser

Mosidze

51b

Moss

108

Mount

142

Mountricha

S.V.

Mouraviev

E.J.W.

Moyse

Mudrinic

12b

Mueller

58a

Mueller

122

Mueller

T.A.

Müller

Mueller

Muenstermann

Munwes

152

W.J.

Murray

128

Mussche

104

Musto

101a

101b

A.G.

Myagkov

127

Myska

124

Nadal

Nagai

159

Nagano

Nagarkar

108

Nagasaka

Nagel

A.M.

Nairz

Nakahama

Nakamura

154

Nakamura

154

Nakano

109

Nanava

Napier

160

Narayan

58b

Nash

N.R.

Nation

Nattermann

Naumann

Navarro

161

H.A.

Neal

Nebot

P.Yu.

Nechaeva

T.J.

Neep

Negri

118a

118b

Negri

Nektarijevic

Nelson

162

T.K.

Nelson

142

Nemecek

124

Nemethy

107

A.A.

Nepomuceno

23a

Nessi

M.S.

Neubauer

164

Neusiedl

R.M.

Neves

107

Nevski

P.R.

Newman

Nguyen Thi Hong

135

R.B.

Nickerson

117

Nicolaidou

135

Nicolas

138

Nicquevert

Niedercorn

114

Nielsen

136

Niinikoski

Nikiforou

Nikiforov

Nikolaenko

127

Nikolaev

Nikolic-Audit

Nikolics

Nikolopoulos

Nilsen

Nilsson

Ninomiya

154

Nisati

131a

Nishiyama

Nisius

Nodulman

Nomachi

115

Nomidis

153

Nordberg

P.R.

Norton

128

Novakova

125

Nozaki

Nozka

112

I.M.

Nugent

158a

A.-E.

Nuncio-Quiroz

Nunes Hanninger

Nunnemann

Nurse

B.J.

OʼBrien

S.W.

OʼNeale

⁎

D.C.

OʼNeil

141

OʼShea

L.B.

Oakes

F.G.

Oakham

Oberlack

Ocariz

Ochi

Oda

154

Odaka

Odier

Ogren

S.H.

C.C.

Ohm

145a

145b

Ohshima

100

Ohshita

139

Okada

Okawa

162

Okumura

100

Okuyama

154

Olariu

25a

Olcese

50a

A.G.

Olchevski

S.A.

Olivares Pino

31a

Oliveira

123a

Oliveira Damazio

Oliver Garcia

166

Olivito

119

Olszewski

Olszowska

Omachi

Onofre

123a

P.U.E.

Onyisi

C.J.

Oram

158a

M.J.

Oreglia

Oren

152

Orestano

133a

133b

Orlando

71a

71b

Orlov

106

Oropeza Barrera

R.S.

Orr

157

Osculati

50a

50b

Ospanov

119

Osuna

Otero y Garzon

J.P.

Ottersbach

104

Ouchrif

134d

E.A.

Ouellette

168

Ould-Saada

116

Ouraou

135

Ouyang

32a

Ovcharova

Owen

138

V.E.

Ozcan

18a

Ozturk

Pacheco Pages

Padilla Aranda

Pagan Griso

Paganis

138

Paige

Pais

Pajchel

116

Palacino

158b

C.P.

Paleari

Palestini

Pallin

Palma

123a

J.D.

Palmer

Y.B.

Pan

171

Panagiotopoulou

Panes

31a

Panikashvili

Panitkin

Pantea

25a

Panuskova

124

Paolone

122

Papadelis

145a

Th.D.

Papadopoulou

Paramonov

Paredes Hernandez

Park

M.A.

Parker

Parodi

50a

50b

J.A.

Parsons

Parzefall

Pashapour

Pasqualucci

131a

Passaggio

50a

Passeri

133a

Pastore

133a

133b

Fr.

Pastore

Pásztor

Pataraia

173

Patel

149

J.R.

Pater

Patricelli

101a

101b

Pauly

Pecsy

143a

M.I.

Pedraza Morales

171

S.V.

Peleganchuk

106

Pelikan

165

Peng

32b

Penning

Penson

Penwell

Perantoni

23a

Perez

Perez Cavalcanti

Perez Codina

158a

M.T.

Pérez García-Estañ

166

Perez Reale

Perini

88a

88b

Pernegger

Perrino

71a

Perrodo

Persembe

V.D.

Peshekhonov

Peters

B.A.

Petersen

T.C.

Petersen

Petit

Petridis

153

Petridou

153

Petrolo

131a

Petrucci

133a

133b

Petschull

Petteni

141

Pezoa

31b

Phan

P.W.

Phillips

128

Piacquadio

Picazio

Piccaro

Piccinini

19a

19b

S.M.

Piec

Piegaia

D.T.

Pignotti

108

J.E.

Pilcher

A.D.

Pilkington

Pina

123a

Pinamonti

163a

163c

Pinder

117

J.L.

Pinfold

Ping

32c

Pinto

123a

Pirotte

Pizio

88a

88b

Plamondon

168

M.-A.

Pleier

A.V.

Pleskach

127

Plotnikova

Poblaguev

Poddar

58a

Podlyski

Poggioli

114

Poghosyan

Pohl

Polci

Polesello

118a

Policicchio

36a

36b

Polini

19a

Poll

Polychronakos

D.M.

Pomarede

135

Pomeroy

Pommès

Pontecorvo

131a

B.G.

Pope

G.A.

Popeneciu

25a

D.S.

Popovic

12a

Poppleton

Portell Bueso

Posch

G.E.

Pospelov

Pospisil

126

I.N.

Potrap

C.J.

Potter

148

C.T.

Potter

113

Poulard

Poveda

171

Pozdnyakov

Prabhu

Pralavorio

Pranko

Prasad

Pravahan

Prell

Pretzl

Pribyl

Price

L.E.

Price

M.J.

Price

Prieur

122

Primavera

71a

Prokofiev

107

Prokoshin

31b

Protopopescu

Proudfoot

Prudent

Przybycien

Przysiezniak

Psoroulas

Ptacek

113

Pueschel

Purdham

Purohit

Puzo

114

Pylypchenko

Qian

Qin

Quadt

D.R.

Quarrie

W.B.

Quayle

171

Quinonez

31a

Raas

103

Radescu

Radics

Radloff

113

Rador

18a

Ragusa

88a

88b

Rahal

176

A.M.

Rahimi

108

Rahm

Rajagopalan

Rammensee

Rammes

140

A.S.

Randle-Conde

Randrianarivony

P.N.

Ratoff

Rauscher

T.C.

Rave

Raymond

A.L.

Read

116

D.M.

Rebuzzi

118a

118b

Redelbach

172

Redlinger

Reece

119

Reeves

Reichold

104

Reinherz-Aronis

152

Reinsch

113

Reisinger

Rembser

Z.L.

Ren

150

Renaud

114

Rescigno

131a

Resconi

88a

Resende

135

Reznicek

Rezvani

157

Richards

Richter

Richter-Was

Ridel

Rijpstra

104

Rijssenbeek

147

Rimoldi

118a

118b

Rinaldi

19a

R.R.

Rios

Riu

Rivoltella

88a

88b

Rizatdinova

111

Rizvi

S.H.

Robertson

Robichaud-Veronneau

117

Robinson

J.E.M.

Robinson

Robson

J.G.

Rocha de Lima

105

Roda

121a

121b

Roda Dos Santos

Rodriguez

161

Roe

Røhne

116

Rojo

Rolli

160

Romaniouk

Romano

19a

19b

V.M.

Romanov

Romeo

Romero Adam

166

Roos

Ros

166

Rosati

131a

Rosbach

Rose

148

Rose

G.A.

Rosenbaum

157

E.I.

Rosenberg

P.L.

Rosendahl

Rosenthal

140

Rosselet

Rossetti

Rossi

131a

131b

L.P.

Rossi

50a

Rotaru

25a

Roth

170

Rothberg

137

Rousseau

114

C.R.

Royon

135

Rozanov

Rozen

151

Ruan

32a

Rubbo

Rubinskiy

Ruckert

Ruckstuhl

104

V.I.

Rud

Rudolph

Rühr

Ruggieri

133a

133b

Ruiz-Martinez

Rumiantsev

⁎

Rumyantsev

Runge

Rurikova

N.A.

Rusakovich

J.P.

Rutherfoord

Ruwiedel

Ruzicka

124

Y.F.

Ryabov

120

Ryadovikov

127

Ryan

Rybar

125

Rybkin

114

N.C.

Ryder

117

Rzaeva

A.F.

Saavedra

149

Sadeh

152

H.F-W.

Sadrozinski

136

Sadykov

Safai Tehrani

131a

Sakamoto

154

Salamanna

Salamon

132a

Saleem

110

Salek

Salihagic

Salnikov

142

Salt

166

B.M.

Salvachua Ferrando

Salvatore

36a

36b

Salvatore

148

Salvucci

103

Salzburger

Sampsonidis

153

B.H.

Samset

116

Sanchez

101a

101b

Sanchez Martinez

166

Sandaker

H.G.

Sander

M.P.

Sanders

Sandhoff

173

Sandoval

161

Sandstroem

Sandvoss

173

D.P.C.

Sankey

128

Sansoni

Santamarina Rios

Santoni

Santonico

132a

132b

Santos

123a

J.G.

Saraiva

123a

Sarangi

171

Sarkisyan-Grinbaum

Sarri

121a

121b

Sartisohn

173

Sasaki

Sasao

Satsounkevitch

Sauvage

Sauvan

J.B.

Sauvan

114

Savard

157

Savinov

122

D.O.

Savu

Sawyer

D.H.

Saxon

119

L.P.

Says

Sbarra

19a

Sbrizzi

19a

19b

Scallon

D.A.

Scannicchio

162

Scarcella

149

Schaarschmidt

114

Schacht

Schaefer

119

Schäfer

Schaepe

Schaetzel

58b

A.C.

Schaffer

114

Schaile

R.D.

Schamberger

147

A.G.

Schamov

106

Scharf

58a

V.A.

Schegelsky

120

Scheirich

Schernau

162

M.I.

Scherzer

Schiavi

50a

50b

Schieck

Schioppa

36a

36b

Schlenker

J.L.

Schlereth

Schmidt

Schmieden

Schmitt

58b

Schmitz

Schöning

58b

Schott

Schouten

158a

Schovancova

124

Schram

Schroeder

Schroer

58c

Schuler

M.J.

Schultens

Schultes

173

H.-C.

Schultz-Coulon

58a

Schulz

J.W.

Schumacher

B.A.

Schumm

136

Ph.

Schune

135

Schwanenberger

Schwartzman

142

Ph.

Schwemling

Schwienhorst

Schwierz

Schwindling

135

Schwindt

Schwoerer

Sciolla

W.G.

Scott

128

Searcy

113

Sedov

Sedykh

120

Segura

S.C.

Seidel

102

Seiden

136

Seifert

J.M.

Seixas

23a

Sekhniaidze

101a

S.J.

Sekula

K.E.

Selbach

D.M.

Seliverstov

120

Sellden

145a

Sellers

Seman

143b

Semprini-Cesari

19a

19b

Serfon

Serin

114

Serkin

Seuster

Severini

110

M.E.

Sevior

Sfyrla

Shabalina

Shamim

113

L.Y.

Shan

32a

J.T.

Shank

Q.T.

Shao

Shapiro

P.B.

Shatalov

Shaver

Shaw

163a

163c

Sherman

174

Sherwood

Shibata

107

Shichi

100

Shimizu

Shimojima

Shin

Shiyakova

Shmeleva

M.J.

Shochet

Short

117

Shrestha

Shulga

M.A.

Shupe

Sicho

124

Sidoti

131a

Siegert

Dj.

Sijacki

12a

Silbert

170

Silva

123a

Silver

152

Silverstein

142

S.B.

Silverstein

145a

Simak

126

Simard

135

Lj.

Simic

12a

Simion

114

Simmons

Simoniello

88a

88b

Simonyan

Sinervo

157

N.B.

Sinev

113

Sipica

140

Siragusa

172

Sircar

A.N.

Sisakyan

S.Yu.

Sivoklokov

Sjölin

145a

145b

T.B.

Sjursen

L.A.

Skinnari

H.P.

Skottowe

Skovpen

106

Skubic

110

Skvorodnev

Slater

Slavicek

126

Sliwa

160

Sloper

Smakhtin

170

B.H.

Smart

S.Yu.

Smirnov

L.N.

Smirnova

B.C.

Smith

142

K.M.

Smith

Smizanska

Smolek

126

A.A.

Snesarev

S.W.

Snow

110

Snyder

Soares

123a

Sobie

168

Sodomka

126

Soffer

152

C.A.

Solans

166

Solar

126

Solc

126

Soldatov

Soldevila

166

Solfaroli Camillocci

131a

131b

A.A.

Solodkov

127

O.V.

Solovyanov

127

Soni

Sopko

126

Sopko

126

Sosebee

Soualah

163a

163c

Soukharev

106

Spagnolo

71a

71b

Spanò

Spighi

19a

Spigo

Spila

131a

131b

Spiwoks

Spousta

125

Spreitzer

157

Spurlock

R.D.

St. Denis

Stahlman

119

Stamen

58a

Stanecka

R.W.

Stanek

Stanescu

133a

Stanescu-Bellu

Stapnes

116

E.A.

Starchenko

127

Stark

Staroba

124

Starovoitov

Staude

Stavina

143a

Steele

Steinbach

Steinberg

Stekl

126

Stelzer

141

H.J.

Stelzer

Stelzer-Chilton

158a

Stenzel

Stern

Stevenson

G.A.

Stewart

J.A.

Stillings

M.C.

Stockton

Stoerig

Stoicea

25a

Stonjek

Strachota

125

A.R.

Stradling

Straessner

Strandberg

146

Strandberg

145a

145b

Strandlie

116

Strang

108

Strauss

142

Strauss

110

Strizenec

143b

Ströhmer

172

D.M.

Strom

113

J.A.

Strong

⁎

Stroynowski

Strube

128

Stugu

Stumer

⁎

Stupak

147

Sturm

173

N.A.

Styles

D.A.

Soh

150

142

HS.

Subramania

Succurro

Sugaya

115

Sugimoto

100

Suhr

105

Suita

Suk

125

V.V.

Sulin

Sultansoy

Sumida

Sun

J.E.

Sundermann

Suruliz

138

Sushkov

Susinno

36a

36b

M.R.

Sutton

148

Suzuki

Svatos

124

Yu.M.

Sviridov

127

Swedish

167

Sykora

143a

Sykora

125

Szeless

Sánchez

166

104

Tackmann

Taffard

162

Tafirout

158a

Taiblum

152

Takahashi

100

Takai

Takashima

Takeda

Takeshita

139

Takubo

Talby

Talyshev

106

M.C.

Tamsett

Tanaka

154

Tanaka

114

Tanaka

130

Tanaka

A.J.

Tanasijczuk

141

Tani

Tannoury

G.P.

Tappern

Tapprogge

Tardif

157

Tarem

151

Tarrade

G.F.

Tartarelli

88a

Tas

125

Tasevsky

124

Tassi

36a

36b

Tatarkhanov

Tayalati

134d

Taylor

F.E.

Taylor

G.N.

Taylor

158b

Teinturier

114

Teixeira Dias Castanheira

Teixeira-Dias

K.K.

Temming

Ten Kate

P.K.

Teng

150

Terada

Terashi

154

Terron

Testa

R.J.

Teuscher

157

Thadome

173

Therhaag

Theveneaux-Pelzer

Thioye

174

Thoma

J.P.

Thomas

E.N.

Thompson

P.D.

Thompson

P.D.

Thompson

157

A.S.

Thompson

L.A.

Thomsen

Thomson

119

Thomson

R.P.

Thun

Tian

M.J.

Tibbetts

Tic

124

V.O.

Tikhomirov

Y.A.

Tikhonov

106

Timoshenko

Tipton

174

F.J.

Tique Aires Viegas

Tisserant

Toczek

Todorov

Todorova-Nova

160

Toggerson

162

Tojo

Tokár

143a

Tokunaga

Tokushuku

Tollefson

Tomoto

100

Tompkins

Toms

102

Tong

32a

Tonoyan

Topfel

N.D.

Topilin

Torchiani

Torrence

113

Torres

Torró Pastor

166

Toth

Touchard

D.R.

Tovey

138

Trefzger

172

Tremblet

Tricoli

I.M.

Trigger

158a

Trincaz-Duvoid

T.N.

Trinh

M.F.

Tripiana

Trischuk

157

Trivedi

Trocmé

Troncon

88a

Trottier-McDonald

141

Trzebinski

Trzupek

Tsarouchas

J.C-L.

Tseng

117

Tsiakiris

104

P.V.

Tsiareshka

Tsionou

Tsipolitis

Tsiskaridze

E.G.

Tskhadadze

51a

I.I.

Tsukerman

Tsulaia

J.-W.

Tsung

Tsuno

Tsybychev

147

Tua

138

Tudorache

25a

Tudorache

25a

J.M.

Tuggle

Turala

Turecek

126

Turk Cakir

Turlay

104

Turra

88a

88b

P.M.

Tuts

Tykhonov

Tylmad

145a

145b

Tyndel

128

Tzanakos

Uchida

Ueda

154

Ueno

Ugland

Uhlenbrock

Uhrmacher

Ukegawa

159

Unal

D.G.

Underwood

Undrus

Unel

162

Unno

Urbaniec

Usai

Uslenghi

118a

118b

Vacavant

Vacek

126

Vachon

Vahsen

Valenta

124

Valente

131a

Valentinetti

19a

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Valkar

125

Valladolid Gallego

166

Vallecorsa

151

J.A.

Valls Ferrer

166

van der Graaf

104

van der Kraaij

104

Van Der Leeuw

104

van der Poel

104

van der Ster

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van Gemmeren

van Kesteren

104

van Vulpen

104

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131a

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Varouchas

Vartapetian

K.E.

Varvell

149

V.I.

Vassilakopoulos

Vazeille

Vazquez Schroeder

Vegni

88a

88b

J.J.

Veillet

114

Vellidis

Veloso

123a

Veness

Veneziano

131a

Ventura

71a

71b

Ventura

137

Venturi

157

Vercesi

118a

Verducci

137

Verkerke

104

J.C.

Vermeulen

104

Vest

M.C.

Vetterli

141

Vichou

164

Vickey

144b

O.E.

Vickey Boeriu

144b

G.H.A.

Viehhauser

117

Viel

167

Villa

19a

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Villaplana Perez

166

Vilucchi

M.G.

Vincter

Vinek

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135

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Virzi

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170

Viti

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126

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126

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Volpini

88a

von der Schmitt

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125

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127

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166

Voss

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173

J.H.

Vossebeld

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135

Vranjes Milosavljevic

104

Vrba

124

Vreeswijk

104

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114

Wagner

173

Wagner

119

Wahlen

173

Wakabayashi

100

Walch

Walder

Walker

Walkowiak

140

Wall

174

Waller

Wang

171

Wang

32b

Wang

150

Wang

J.C.

Wang

137

Wang

102

S.M.

Wang

150

Wang

Warburton

C.P.

Ward

Warsinsky

Washbrook

Wasicki

P.M.

Watkins

A.T.

Watson

I.J.

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149

M.F.

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Watts

137

Watts

A.T.

Waugh

149

B.M.

Waugh

Weber

128

M.S.

Weber

A.R.

Weidberg

117

Weigell

Weingarten

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Wellenstein

P.S.

Wells

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Wendland

Wendler

122

Weng

150

Wengler

Wenig

Wermes

Werner

Werth

162

Wessels

58a

Wetter

160

Weydert

Whalen

S.J.

Wheeler-Ellis

162

S.P.

Whitaker

White

M.J.

White

121a

121b

S.R.

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117

Whiteson

162

Whittington

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114

Wicke

173

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128

Wiedenmann

171

Wielers

128

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142

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149

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154

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154

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154

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145a

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142

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117

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105

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127

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127

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174

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127

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121a

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140

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127

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171

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zur Nedden

Zutshi

105

Zwalinski

1University at Albany, Albany, NY, United States2Department of Physics, University of Alberta, Edmonton, AB, Canada3aDepartment of Physics, Ankara University, Ankara, Turkey3bDepartment of Physics, Dumlupinar University, Kutahya, Turkey3cDepartment of Physics, Gazi University, Ankara, Turkey3dDivision of Physics, TOBB University of Economics and Technology, Ankara, Turkey3eTurkish Atomic Energy Authority, Ankara, Turkey4LAPP, CNRS/IN2P3 and Université de Savoie, Annecy-le-Vieux, France5High Energy Physics Division, Argonne National Laboratory, Argonne, IL, United States6Department of Physics, University of Arizona, Tucson, AZ, United States7Department of Physics, The University of Texas at Arlington, Arlington, TX, United States8Physics Department, University of Athens, Athens, Greece9Physics Department, National Technical University of Athens, Zografou, Greece10Institute of Physics, Azerbaijan Academy of Sciences, Baku, Azerbaijan11Institut de Física dʼAltes Energies and Departament de Física de la Universitat Autònoma de Barcelona and ICREA, Barcelona, Spain12aInstitute of Physics, University of Belgrade, Belgrade, Serbia12bVinca Institute of Nuclear Sciences, University of Belgrade, Belgrade, Serbia13Department for Physics and Technology, University of Bergen, Bergen, Norway14Physics Division, Lawrence Berkeley National Laboratory and University of California, Berkeley, CA, United States15Department of Physics, Humboldt University, Berlin, Germany16Albert Einstein Center for Fundamental Physics and Laboratory for High Energy Physics, University of Bern, Bern, Switzerland17School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom18aDepartment of Physics, Bogazici University, Istanbul, Turkey18bDivision of Physics, Dogus University, Istanbul, Turkey18cDepartment of Physics Engineering, Gaziantep University, Gaziantep, Turkey18dDepartment of Physics, Istanbul Technical University, Istanbul, Turkey19aINFN Sezione di Bologna, Italy19bDipartimento di Fisica, Università di Bologna, Bologna, Italy20Physikalisches Institut, University of Bonn, Bonn, Germany21Department of Physics, Boston University, Boston, MA, United States22Department of Physics, Brandeis University, Waltham, MA, United States23aUniversidade Federal do Rio De Janeiro COPPE/EE/IF, Rio de Janeiro, Brazil23bFederal University of Juiz de Fora (UFJF), Juiz de Fora, Brazil23cFederal University of Sao Joao del Rei (UFSJ), Sao Joao del Rei, Brazil23dInstituto de Fisica, Universidade de Sao Paulo, Sao Paulo, Brazil24Physics Department, Brookhaven National Laboratory, Upton, NY, United States25aNational Institute of Physics and Nuclear Engineering, Bucharest, Romania25bUniversity Politehnica Bucharest, Bucharest, Romania25cWest University in Timisoara, Timisoara, Romania26Departamento de Física, Universidad de Buenos Aires, Buenos Aires, Argentina27Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom28Department of Physics, Carleton University, Ottawa, ON, Canada29CERN, Geneva, Switzerland30Enrico Fermi Institute, University of Chicago, Chicago, IL, United States31aDepartamento de Fisica, Pontificia Universidad Católica de Chile, Santiago, Chile31bDepartamento de Física, Universidad Técnica Federico Santa María, Valparaíso, Chile32aInstitute of High Energy Physics, Chinese Academy of Sciences, Beijing, China32bDepartment of Modern Physics, University of Science and Technology of China, Anhui, China32cDepartment of Physics, Nanjing University, Jiangsu, China32dSchool of Physics, Shandong University, Shandong, China33Laboratoire de Physique Corpusculaire, Clermont Université and Université Blaise Pascal and CNRS/IN2P3, Aubiere Cedex, France34Nevis Laboratory, Columbia University, Irvington, NY, United States35Niels Bohr Institute, University of Copenhagen, Kobenhavn, Denmark36aINFN Gruppo Collegato di Cosenza, Italy36bDipartimento di Fisica, Università della Calabria, Arcavata di Rende, Italy37AGH University of Science and Technology, Faculty of Physics and Applied Computer Science, Krakow, Poland38The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Krakow, Poland39Physics Department, Southern Methodist University, Dallas, TX, United States40Physics Department, University of Texas at Dallas, Richardson, TX, United States41DESY, Hamburg and Zeuthen, Germany42Institut für Experimentelle Physik IV, Technische Universität Dortmund, Dortmund, Germany43Institut für Kern- und Teilchenphysik, Technical University Dresden, Dresden, Germany44Department of Physics, Duke University, Durham, NC, United States45SUPA – School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom46Fachhochschule Wiener Neustadt, Johannes Gutenbergstrasse 3 2700 Wiener Neustadt, Austria47INFN Laboratori Nazionali di Frascati, Frascati, Italy48Fakultät für Mathematik und Physik, Albert-Ludwigs-Universität, Freiburg i.Br., Germany49Section de Physique, Université de Genève, Geneva, Switzerland50aINFN Sezione di Genova, Italy50bDipartimento di Fisica, Università di Genova, Genova, Italy51aE.Andronikashvili Institute of Physics, Tbilisi State University, Tbilisi, Georgia51bHigh Energy Physics Institute, Tbilisi State University, Tbilisi, Georgia52II Physikalisches Institut, Justus-Liebig-Universität Giessen, Giessen, Germany53SUPA – School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom54II Physikalisches Institut, Georg-August-Universität, Göttingen, Germany55Laboratoire de Physique Subatomique et de Cosmologie, Université Joseph Fourier and CNRS/IN2P3 and Institut National Polytechnique de Grenoble, Grenoble, France56Department of Physics, Hampton University, Hampton, VA, United States57Laboratory for Particle Physics and Cosmology, Harvard University, Cambridge, MA, United States58aKirchhoff-Institut für Physik, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany58bPhysikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany58cZITI Institut für technische Informatik, Ruprecht-Karls-Universität Heidelberg, Mannheim, Germany59Faculty of Applied Information Science, Hiroshima Institute of Technology, Hiroshima, Japan60Department of Physics, Indiana University, Bloomington, IN, United States61Institut für Astro- und Teilchenphysik, Leopold-Franzens-Universität, Innsbruck, Austria62University of Iowa, Iowa City, IA, United States63Department of Physics and Astronomy, Iowa State University, Ames, IA, United States64Joint Institute for Nuclear Research, JINR Dubna, Dubna, Russia65KEK, High Energy Accelerator Research Organization, Tsukuba, Japan66Graduate School of Science, Kobe University, Kobe, Japan67Faculty of Science, Kyoto University, Kyoto, Japan68Kyoto University of Education, Kyoto, Japan69Instituto de Física La Plata, Universidad Nacional de La Plata and CONICET, La Plata, Argentina70Physics Department, Lancaster University, Lancaster, United Kingdom71aINFN Sezione di Lecce, Italy71bDipartimento di Fisica, Università del Salento, Lecce, Italy72Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom73Department of Physics, Jožef Stefan Institute and University of Ljubljana, Ljubljana, Slovenia74School of Physics and Astronomy, Queen Mary University of London, London, United Kingdom75Department of Physics, Royal Holloway University of London, Surrey, United Kingdom76Department of Physics and Astronomy, University College London, London, United Kingdom77Laboratoire de Physique Nucléaire et de Hautes Energies, UPMC and Université Paris-Diderot and CNRS/IN2P3, Paris, France78Fysiska institutionen, Lunds universitet, Lund, Sweden79Departamento de Fisica Teorica C-15, Universidad Autonoma de Madrid, Madrid, Spain80Institut für Physik, Universität Mainz, Mainz, Germany81School of Physics and Astronomy, University of Manchester, Manchester, United Kingdom82CPPM, Aix-Marseille Université and CNRS/IN2P3, Marseille, France83Department of Physics, University of Massachusetts, Amherst, MA, United States84Department of Physics, McGill University, Montreal, QC, Canada85School of Physics, University of Melbourne, Victoria, Australia86Department of Physics, The University of Michigan, Ann Arbor, MI, United States87Department of Physics and Astronomy, Michigan State University, East Lansing, MI, United States88aINFN Sezione di Milano, Italy88bDipartimento di Fisica, Università di Milano, Milano, Italy89B.I. Stepanov Institute of Physics, National Academy of Sciences of Belarus, Minsk, Belarus90National Scientific and Educational Centre for Particle and High Energy Physics, Minsk, Belarus91Department of Physics, Massachusetts Institute of Technology, Cambridge, MA, United States92Group of Particle Physics, University of Montreal, Montreal, QC, Canada93P.N. Lebedev Institute of Physics, Academy of Sciences, Moscow, Russia94Institute for Theoretical and Experimental Physics (ITEP), Moscow, Russia95Moscow Engineering and Physics Institute (MEPhI), Moscow, Russia96Skobeltsyn Institute of Nuclear Physics, Lomonosov Moscow State University, Moscow, Russia97Fakultät für Physik, Ludwig-Maximilians-Universität München, München, Germany98Max-Planck-Institut für Physik (Werner-Heisenberg-Institut), München, Germany99Nagasaki Institute of Applied Science, Nagasaki, Japan100Graduate School of Science, Nagoya University, Nagoya, Japan101aINFN Sezione di Napoli, Italy101bDipartimento di Scienze Fisiche, Università di Napoli, Napoli, Italy102Department of Physics and Astronomy, University of New Mexico, Albuquerque, NM, United States103Institute for Mathematics, Astrophysics and Particle Physics, Radboud University Nijmegen/Nikhef, Nijmegen, Netherlands104Nikhef National Institute for Subatomic Physics and University of Amsterdam, Amsterdam, Netherlands105Department of Physics, Northern Illinois University, DeKalb, IL, United States106Budker Institute of Nuclear Physics, SB RAS, Novosibirsk, Russia107Department of Physics, New York University, New York, NY, United States108Ohio State University, Columbus, OH, United States109Faculty of Science, Okayama University, Okayama, Japan110Homer L. Dodge Department of Physics and Astronomy, University of Oklahoma, Norman, OK, United States111Department of Physics, Oklahoma State University, Stillwater, OK, United States112Palacký University, RCPTM, Olomouc, Czech Republic113Center for High Energy Physics, University of Oregon, Eugene, OR, United States114LAL, Univ. Paris-Sud and CNRS/IN2P3, Orsay, France115Graduate School of Science, Osaka University, Osaka, Japan116Department of Physics, University of Oslo, Oslo, Norway117Department of Physics, Oxford University, Oxford, United Kingdom118aINFN Sezione di Pavia, Italy118bDipartimento di Fisica, Università di Pavia, Pavia, Italy119Department of Physics, University of Pennsylvania, Philadelphia, PA, United States120Petersburg Nuclear Physics Institute, Gatchina, Russia121aINFN Sezione di Pisa, Italy121bDipartimento di Fisica E. Fermi, Università di Pisa, Pisa, Italy122Department of Physics and Astronomy, University of Pittsburgh, Pittsburgh, PA, United States123aLaboratorio de Instrumentacao e Fisica Experimental de Particulas – LIP, Lisboa, Portugal, Spain123bDepartamento de Fisica Teorica y del Cosmos and CAFPE, Universidad de Granada, Granada, Spain124Institute of Physics, Academy of Sciences of the Czech Republic, Praha, Czech Republic125Faculty of Mathematics and Physics, Charles University in Prague, Praha, Czech Republic126Czech Technical University in Prague, Praha, Czech Republic127State Research Center Institute for High Energy Physics, Protvino, Russia128Particle Physics Department, Rutherford Appleton Laboratory, Didcot, United Kingdom129Physics Department, University of Regina, Regina, SK, Canada130Ritsumeikan University, Kusatsu, Shiga, Japan131aINFN Sezione di Roma I, Italy131bDipartimento di Fisica, Università La Sapienza, Roma, Italy132aINFN Sezione di Roma Tor Vergata, Italy132bDipartimento di Fisica, Università di Roma Tor Vergata, Roma, Italy133aINFN Sezione di Roma Tre, Italy133bDipartimento di Fisica, Università Roma Tre, Roma, Italy134aFaculté des Sciences Ain Chock, Réseau Universitaire de Physique des Hautes Energies – Université Hassan II, Casablanca, Morocco134bCentre National de lʼEnergie des Sciences Techniques Nucleaires, Rabat, Morocco134cFaculté des Sciences Semlalia, Université Cadi Ayyad, LPHEA-Marrakech, Morocco134dFaculté des Sciences, Université Mohamed Premier and LPTPM, Oujda, Morocco134eFaculté des Sciences, Université Mohammed V-Agdal, Rabat, Morocco135DSM/IRFU (Institut de Recherches sur les Lois Fondamentales de lʼUnivers), CEA Saclay (Commissariat a lʼEnergie Atomique), Gif-sur-Yvette, France136Santa Cruz Institute for Particle Physics, University of California Santa Cruz, Santa Cruz, CA, United States137Department of Physics, University of Washington, Seattle, WA, United States138Department of Physics and Astronomy, University of Sheffield, Sheffield, United Kingdom139Department of Physics, Shinshu University, Nagano, Japan140Fachbereich Physik, Universität Siegen, Siegen, Germany141Department of Physics, Simon Fraser University, Burnaby, BC, Canada142SLAC National Accelerator Laboratory, Stanford, CA, United States143aFaculty of Mathematics, Physics & Informatics, Comenius University, Bratislava, Slovak Republic143bDepartment of Subnuclear Physics, Institute of Experimental Physics of the Slovak Academy of Sciences, Kosice, Slovak Republic144aDepartment of Physics, University of Johannesburg, Johannesburg, South Africa144bSchool of Physics, University of the Witwatersrand, Johannesburg, South Africa145aDepartment of Physics, Stockholm University, Sweden145bThe Oskar Klein Centre, Stockholm, Sweden146Physics Department, Royal Institute of Technology, Stockholm, Sweden147Departments of Physics & Astronomy and Chemistry, Stony Brook University, Stony Brook, NY, United States148Department of Physics and Astronomy, University of Sussex, Brighton, United Kingdom149School of Physics, University of Sydney, Sydney, Australia150Institute of Physics, Academia Sinica, Taipei, Taiwan151Department of Physics, Technion: Israel Inst. of Technology, Haifa, Israel152Raymond and Beverly Sackler School of Physics and Astronomy, Tel Aviv University, Tel Aviv, Israel153Department of Physics, Aristotle University of Thessaloniki, Thessaloniki, Greece154International Center for Elementary Particle Physics and Department of Physics, The University of Tokyo, Tokyo, Japan155Graduate School of Science and Technology, Tokyo Metropolitan University, Tokyo, Japan156Department of Physics, Tokyo Institute of Technology, Tokyo, Japan157Department of Physics, University of Toronto, Toronto, ON, Canada158aTRIUMF, Vancouver, BC, Canada158bDepartment of Physics and Astronomy, York University, Toronto, ON, Canada159Institute of Pure and Applied Sciences, University of Tsukuba, 1-1-1 Tennodai, Tsukuba, Ibaraki 305-8571, Japan160Science and Technology Center, Tufts University, Medford, MA, United States161Centro de Investigaciones, Universidad Antonio Narino, Bogota, Colombia162Department of Physics and Astronomy, University of California Irvine, Irvine, CA, United States163aINFN Gruppo Collegato di Udine, Italy163bICTP, Trieste, Italy163cDipartimento di Chimica, Fisica e Ambiente, Università di Udine, Udine, Italy164Department of Physics, University of Illinois, Urbana, IL, United States165Department of Physics and Astronomy, University of Uppsala, Uppsala, Sweden166Instituto de Física Corpuscular (IFIC) and Departamento de Física Atómica, Molecular y Nuclear and Departamento de Ingeniería Electrónica and Instituto de Microelectrónica de Barcelona (IMB-CNM), University of Valencia and CSIC, Valencia, Spain167Department of Physics, University of British Columbia, Vancouver, BC, Canada168Department of Physics and Astronomy, University of Victoria, Victoria, BC, Canada169Waseda University, Tokyo, Japan170Department of Particle Physics, The Weizmann Institute of Science, Rehovot, Israel171Department of Physics, University of Wisconsin, Madison, WI, United States172Fakultät für Physik und Astronomie, Julius-Maximilians-Universität, Würzburg, Germany173Fachbereich C Physik, Bergische Universität Wuppertal, Wuppertal, Germany174Department of Physics, Yale University, New Haven, CT, United States175Yerevan Physics Institute, Yerevan, Armenia176Domaine scientifique de la Doua, Centre de Calcul CNRS/IN2P3, Villeurbanne Cedex, Francea

Also at Laboratorio de Instrumentacao e Fisica Experimental de Particulas – LIP, Lisboa, Portugal.

Also at Faculdade de Ciencias and CFNUL, Universidade de Lisboa, Lisboa, Portugal.

Also at Particle Physics Department, Rutherford Appleton Laboratory, Didcot, United Kingdom.

Also at TRIUMF, Vancouver, BC, Canada.

Also at Department of Physics, California State University, Fresno, CA, United States.

Also at Novosibirsk State University, Novosibirsk, Russia.

Also at Fermilab, Batavia, IL, United States.

Also at Department of Physics, University of Coimbra, Coimbra, Portugal.

Also at Università di Napoli Parthenope, Napoli, Italy.

Also at Institute of Particle Physics (IPP), Canada.

Also at Department of Physics, Middle East Technical University, Ankara, Turkey.

Also at Louisiana Tech University, Ruston, LA, United States.

Also at Department of Physics and Astronomy, University College London, London, United Kingdom.

Also at Group of Particle Physics, University of Montreal, Montreal, QC, Canada.

Also at Department of Physics, University of Cape Town, Cape Town, South Africa.

Also at Institute of Physics, Azerbaijan Academy of Sciences, Baku, Azerbaijan.

Also at Institut für Experimentalphysik, Universität Hamburg, Hamburg, Germany.

Also at Manhattan College, New York, NY, United States.

Also at School of Physics, Shandong University, Shandong, China.

Also at CPPM, Aix-Marseille Université and CNRS/IN2P3, Marseille, France.

Also at School of Physics and Engineering, Sun Yat-sen University, Guanzhou, China.

Also at Academia Sinica Grid Computing, Institute of Physics, Academia Sinica, Taipei, Taiwan.

Also at DSM/IRFU (Institut de Recherches sur les Lois Fondamentales de lʼUnivers), CEA Saclay (Commissariat a lʼEnergie Atomique), Gif-sur-Yvette, France.

Also at Section de Physique, Université de Genève, Geneva, Switzerland.

Also at Departamento de Fisica, Universidade de Minho, Braga, Portugal.

Also at Department of Physics and Astronomy, University of South Carolina, Columbia, SC, United States.

Also at Institute for Particle and Nuclear Physics, Wigner Research Centre for Physics, Budapest, Hungary.

Also at California Institute of Technology, Pasadena, CA, United States.

Also at Institute of Physics, Jagiellonian University, Krakow, Poland.

Also at LAL, Univ. Paris-Sud and CNRS/IN2P3, Orsay, France.

Also at Department of Physics and Astronomy, University of Sheffield, Sheffield, United Kingdom.

Also at Department of Physics, Oxford University, Oxford, United Kingdom.

Also at Institute of Physics, Academia Sinica, Taipei, Taiwan.

Also at Department of Physics, The University of Michigan, Ann Arbor, MI, United States.

Also at Laboratoire de Physique Nucléaire et de Hautes Energies, UPMC and Université Paris-Diderot and CNRS/IN2P3, Paris, France.

⁎

Deceased.

Editor: H. Weerts

Abstract

A search for production of supersymmetric particles in final states containing jets, missing transverse momentum, and at least one hadronically decaying τ lepton is presented. The data were recorded by the ATLAS experiment in s=7 TeV proton–proton collisions at the Large Hadron Collider. No excess above the Standard Model background expectation was observed in 2.05fb−1 of data. The results are interpreted in the context of gauge mediated supersymmetry breaking models with Mmess=250 TeV, N5=3, μ>0, and Cgrav=1. The production of supersymmetric particles is excluded at 95% C.L. up to a supersymmetry breaking scale Λ=30 TeV, independent of tanβ, and up to Λ=43 TeV for large tanβ.

Keywords

SupersymmetryGMSBTau lepton

Introduction

Supersymmetry (SUSY) [1–9] is a well-motivated theoretical concept that introduces a symmetry between bosons and fermions. As a consequence, every Standard Model (SM) particle has a SUSY partner with the same mass and quantum numbers except for the spin which differs by half a unit. Since none of these partners has been observed SUSY must be a broken symmetry if realized in nature. If R-parity is conserved [10–14], SUSY particles can only be produced in pairs and would decay through cascades involving lighter SUSY particles. These decay cascades end in the production of the lightest supersymmetric particle (LSP), which is stable and escapes the detector unseen, giving rise to missing transverse momentum in the detector. SUSY can remedy various shortcomings of the Standard Model, such as the hierarchy problem [14–19], the lack of a dark matter candidate [20,21] and the non-unification of the gauge couplings [22–25]. To achieve this, the masses of at least some SUSY particles must be near the weak scale, and therefore, if weak-scale SUSY is realized in nature, there are good prospects to discover it at the Large Hadron Collider (LHC).In certain SUSY models, large mixing between left and right sfermions, the partners of the left-handed and right-handed SM fermions, implies that the lightest sfermions belong to the third generation. This leads to a large production rate of τ leptons from decays of τ˜ sleptons and gauginos, the partners of the SM gauge bosons, in SUSY cascade decays. For example, in the context of Gauge Mediated SUSY Breaking (GMSB) [26–31] the lighter of the two τ˜ sleptons is the next-to-lightest supersymmetric particle (NLSP) for a large part of the parameter space, and the very light gravitino, G˜, is the LSP. Hence τ˜ sleptons decay to a τ lepton and a gravitino. While this τ˜→τG˜ process is the dominant source of τ leptons from SUSY decays in certain regions of GMSB model parameter space, the analysis presented here is sensitive to any process producing τ leptons in association with jets and missing transverse momentum.This Letter presents a search for supersymmetry in final states with at least one hadronically decaying τ lepton, missing transverse momentum and jets with the ATLAS detector at the LHC. The results of the search are interpreted within the GMSB model. Previous experiments at LEP [32–34] have placed constraints on τ˜ and e˜ masses and on more generic GMSB signatures. Among these the limits from the OPAL experiment [32] were the most stringent, excluding τ˜ NLSPs with masses below 87.4 GeV. The D0 Collaboration performed a search for squark production in events with hadronically decaying τ leptons, jets, and missing transverse momentum [35], and the CMS Collaboration performed searches for new physics in same-sign ditau events [36] and multi-lepton events [37] including τ pairs, but the GMSB model was not specifically considered in any of these results. A search for supersymmetry in final states containing at least two hadronically decaying τ leptons, missing transverse momentum, and jets with the ATLAS detector is presented in another Letter [38].2

ATLAS detector

The ATLAS detector [39] is a multipurpose particle physics apparatus with a forward–backward symmetric cylindrical geometry and nearly 4π coverage in solid angle.11

ATLAS uses a right-handed coordinate system with its origin at the nominal interaction point in the center of the detector and the z-axis coinciding with the axis of the beam pipe. The x-axis points from the interaction point to the center of the LHC ring, and the y-axis points upward. Cylindrical coordinates (r,ϕ) are used in the transverse plane, ϕ being the azimuthal angle around the beam pipe. The pseudorapidity is defined in terms of the polar angle θ as η=−lntan(θ/2).

The inner tracking detector consists of a silicon pixel detector, a silicon microstrip detector, and a transition radiation tracker. The inner detector is surrounded by a thin superconducting solenoid providing a 2 T axial magnetic field and by high-granularity liquid-argon sampling calorimeters. An iron-scintillator tile calorimeter provides hadronic coverage in the central rapidity range. A muon spectrometer consisting of large superconducting toroids and a system of precision tracking chambers surrounds the calorimeters.3

Data and simulated samples

The analysis is based on data collected by the ATLAS detector in proton–proton collisions at a center-of-mass energy of 7 TeV between March and August 2011. Application of beam, detector, and data-quality requirements resulted in an integrated luminosity of 2.05±0.08 fb−1[40,41]. The data were collected using triggers based on one jet with transverse momentum pT>75 GeV, measured at the raw electromagnetic scale, and missing transverse momentum above 45 GeV.In GMSB models, the breaking of SUSY is mediated through flavor-blind SM gauge interactions of messenger fields with mass scale Mmess which is small compared to the Planck mass. In addition to Mmess, the free parameters in GMSB models are the scale of the SUSY breaking, Λ, the number of messenger fields, N5, the sign of the Higgsino mixing parameter, sign(μ), the scale factor for the gravitino mass, Cgrav, and the ratio of the vacuum expectation values of the two Higgs doublets, tanβ. In this analysis, GMSB models are studied in the Λ–tanβ plane for fixed Mmess=250 TeV, N5=3, sign(μ)=+1 and Cgrav=1. The chosen set of parameter values restricts the analysis to specific final states relevant for the search with τ leptons and to promptly decaying NLSPs. For N5⩾2 and large tanβ the lightest τ˜ slepton, τ˜1, is the NLSP.Samples of simulated GMSB events are generated with the Herwig++[42] generator for ten values of Λ in the range 10⩽Λ⩽85 TeV and ten values of tanβ in the range 2⩽tanβ⩽45, with the SUSY mass spectra generated using ISAJET 7.80[43]. The MRST2007 LO*[44] parton distribution functions (PDFs) are used. The production cross sections are calculated with PROSPINO[45–48] to next-to-leading order in the QCD coupling using the next-to-leading-order CTEQ6.6[49] PDF set. The two samples with Λ=30(40) TeV and tanβ=20(30), which have cross sections of 1.95(0.41) pb, are used as representative points for the optimization of the event selection.The dominant background processes in this search are production of W and Z bosons in association with jets (W+jets and Z+jets), top quark pair (tt¯) and single top quark production. The W+jets and Z+jets production processes are simulated with the ALPGEN[50] generator, using the CTEQ6L1[51] PDF set, and are normalized to a cross section of 31.4nb and 9.02nb[52–54], respectively. The tt¯, single-top and diboson production processes are generated with MC@NLO[55] and the CTEQ6.6[49] PDF set, and are normalized using a cross section of 0.165nb, 0.085nb[56–58] and 0.071nb[59,60], respectively. Parton showers and hadronization are simulated with HERWIG and the underlying event is modeled with JIMMY[61]. The programs TAUOLA[62,63] and PHOTOS[64] are used to model the decays of τ leptons and the radiation of photons, respectively. The production of multijet events is simulated with PYTHIA[65], though the multijet background yield in this analysis is estimated using data. All simulated samples are processed through a full simulation of the ATLAS detector [66] based on Geant4 [67]. To match the pile-up (overlap of several interactions in the same bunch crossing) observed in the data, the generated signal and background events are overlaid with minimum-bias events [68,69] and the resulting events are reweighted so that the distribution of the number of interactions per bunch crossing agrees with the data.4

Object reconstruction

Jet candidates are reconstructed with the anti-kt clustering algorithm [70] with radius parameter R=0.4. The inputs to this algorithm are clusters of calorimeter cells seeded by cells with energy significantly above the measured noise. Jets are constructed by performing a four-vector sum over these clusters, treating each cluster as a four-vector with zero mass. Jets are corrected for calorimeter non-compensation, upstream material, and other effects using pT- and η-dependent correction factors obtained from Monte Carlo simulation and validated with extensive test-beam and collision-data studies [71]. Only jet candidates with pT>30 GeV, |η|<2.8 and a distance ΔR>0.2 with respect to the nearest identified electron are considered as real hadronic jets, where the distance is defined as ΔR=(Δη)2+(Δϕ)2.The electron and muon identification criteria are identical to those in Ref. [72]. Electrons and muons are only considered if they satisfy pT>20 GeV and ΔR>0.4 with respect to the nearest identified jet.The magnitude of the missing transverse momentum, ETmiss, is computed from the vector sum of the transverse momenta of all identified electrons and muons, all jets, and remaining clusters of calorimeter cells with |η|<4.5[73].Hadronically decaying τ leptons are reconstructed from jet candidates with pT>10 GeV and are distinguished from quark- or gluon-initiated jets using a boosted decision tree (BDT) based on eleven discriminating shower-shape and tracking variables [74]. Electrons are further rejected using transition radiation and calorimetric information. An energy calibration factor for hadronically decaying τ leptons is applied as function of pT and η. Candidates are required to satisfy pTτ>20 GeV and |η|<2.5 and to have one or three associated reconstructed tracks (prongs) with total charge ±1. The τ candidates are required to satisfy a pT-dependent BDT output criterion [74] chosen to give ∼30% (∼50%) signal efficiency for one-prong (three-prong) τ candidates as estimated in Z(→ττ)+jets events. The BDT selection has a corresponding background acceptance of ∼0.5% (∼3%), estimated in dijet events, and the different selection criteria reflect different abundances of one- and three-prong jets in background samples.During a part of the data-taking period, an electronics failure in the liquid-argon calorimeter created a dead region in the second and third layer of the calorimeter, corresponding to approximately 1.4×0.2rad in Δη×Δϕ. A correction is made to the jet energy using energy depositions in cells neighboring the dead region; events having at least one jet, including the leading τ candidate, in this region for which the corrected energy is above 30 GeV are discarded, resulting in a loss of ∼6% of the data sample.5

Event selection

Events are required to have a reconstructed primary vertex with at least five associated tracks with pT>500 MeV. Events are rejected if they contain identified electrons or muons or if any jet or τ candidate is consistent with arising from detector noise or non-collision background [71]. Events are required to contain one or more identified τ candidates, at least two jets, one with pT>30 GeV and another with pT>130 GeV, and missing transverse momentum ETmiss>130 GeV. The latter two requirements ensure that the trigger efficiency is above 98% in both data and simulation.The two jets leading in pT are required to be separated in azimuth from the direction of the missing transverse momentum by more than 0.3 rad. This requirement reduces multijet events, which typically have instrumental missing transverse momentum aligned with the leading jets. Multijet events are further suppressed by requiring ETmiss/meff>0.25, where the effective mass, meff, is defined as the scalar sum of ETmiss, the pT of the two leading jets, and the pTτ of the leading τ candidate.Events are required to have a transverse mass, mT, above 110 GeV. The transverse mass is defined asmT=mτ2+2pTτETmiss(1−cosΔϕ(pTτ,ETmiss)), where Δϕ(pTτ,ETmiss) is the azimuthal angle between the τ and the direction of the missing transverse momentum. This requirement suppresses backgrounds due to W+jets and top-quark production. The remaining SM backgrounds are further suppressed by requiring meff>600 GeV. This is the final selection defining the signal region for the analysis. The mT and meff requirements as well as the criteria used for the suppression of multijet events are chosen to maximize the signal significance computed with the Asimov approximation [75].6

Background estimation

Background processes are divided into three classes which are estimated separately: events with true τ leptons from t→bτν decays (both top-quark-pair and single top quark production) and W(→τν)+jets events; events with misidentified (‘fake’) τ candidates in top, W+jets, and Z+jets events; and events with fake τ candidates in multijet events. The two fake-τ classes are treated separately to account for differences in τ misidentification probabilities due to different event topologies and jet composition.Events with true τ leptons are estimated in a control region defined by replacing the requirement on the transverse mass in the final selection with the requirement mT<70 GeV. For events with a correctly reconstructed τ lepton and with ETmiss entirely due to a single neutrino, mT is kinematically bounded from above by the W mass, within the detector resolution; by requiring mT<70 GeV, more than 90% of the events in the resulting control region are expected to contain true τ leptons from top-quark and W decays. The composition of the event sample in this control region is given in Table 1

. Within this control region, the background due to Z decays is estimated from simulation and the remaining small background due to multijet events is estimated using a procedure similar to that used to estimate the multijet background in the signal region, described below.

Within the mT<70 GeV control region, top-quark and W+jets yields are estimated individually with a maximum-likelihood fit to the output distribution of a BDT built from four variables: the number of b-quark jets, the total jet multiplicity, the transverse momentum of the second-leading jet, and the transverse thrust T of the event, defined as T=maxnˆ{∑inˆ⋅p→T,i/|∑ip→T,i|}, where i runs over the missing transverse momentum and all jets, excluding the tau candidates, with transverse momentum vectors p→T,i, and the transverse thrust axis is given by the unit vector nˆ for which the maximum is attained. Top-quark events have more reconstructed b-quark jets, a higher jet multiplicity, higher jet momenta, and tend to be more spherical than W+jets events. Jets containing b quarks are identified with about 60% efficiency, evaluated with top-quark events, using secondary vertex reconstruction and three-dimensional impact parameters of tracks associated with the jet [76]. The output distribution of this BDT is shown in Fig. 1

along with the results of the fit. The results of the fit are scale factors for W+jets and top quark backgrounds which reflect differences in cross sections and reconstruction efficiencies between data and simulation. The measured scale factors are 1.22±0.13 for top events and 0.71±0.03 for W+jets events. These scale factors are applied to simulated event samples in the signal region to derive the final expected true-τ yields from background processes.

For the estimation of backgrounds due to fake τ candidates in top-quark, W+jets, and Z+jets events, a second control sample is defined by selecting events that fulfill the event selection but with modified criteria on mT and meff: mT>70 GeV and either mT<110 GeV or meff<600 GeV. Since the mT distribution falls off rapidly above the W mass for true-τ events, the intermediate mT region selected here is relatively enhanced in fake-τ events, and the overall composition of this region is expected to be very similar to that of the signal region. Multijet events are expected to make up less than 3% of this sample and are estimated from simulation. The composition of the fake-τ-enhanced sample in this control region is shown in Table 2

. Within this control region, true-τ backgrounds are subtracted using estimates derived from the true-τ-dominated control region. The numbers of events remaining after the true-τ subtraction are used to determine a scale factor, 0.50±0.08, which is then applied to simulated samples of fake-τ events in the signal region to obtain a final background estimate. While this scale factor differs significantly from unity, it is consistent with other ATLAS studies of the performance of τ fake rates in simulation.

Backgrounds due to multijet events are estimated in a third control region in which either ETmiss/meff<0.25 or one of the two leading jets is aligned in azimuth with the missing transverse momentum direction. Within this sample, the probability for jets (which contain very few true τ leptons) to satisfy the τ selection criteria is estimated by applying the selection to randomly chosen jet candidates. This probability is then applied to a complementary sample of multijet events, where the azimuthal separation and ETmiss/meff, as well as all other event selection requirements, match those of the signal region, but where the τ candidate is again randomly chosen from among the jet candidates. This provides an estimate of the multijet background yield in the signal region. It is found that the multijet background makes up only a few percent of the total SM background in the signal region.Possible contamination from SUSY signals has been considered in all three background-estimation control regions and is found to have a negligible effect on the results presented below.7

Systematic uncertainties

Dominant systematic uncertainties on the estimated background yields are due to uncertainties in the jet energy scale (3–8%) [71], jet energy resolution (6–13%) [71], τ energy scale (2–10%) [74], statistical uncertainties in the data control regions (5–15%), and Monte Carlo uncertainties related to the extrapolation from the control regions to the signal region (10–20%). This last term includes statistical uncertainties in the simulation, variations in the in the assumed W+jets/top/Z+jets mixture in the fake-τ control region, and Monte Carlo generator uncertainties (estimated by varying the shower matching, factorization and renormalization scales, αs, and the amount of initial-state and final-state radiation) [77]. Additional uncertainties on W+jets and top-quark backgrounds are estimated by varying the assumed b-quark identification efficiency within measured uncertainties (4–11%) [76]. Uncertainties on the multijet background yield are estimated by studying correlations between meff and the azimuthal separation between the leading two jets and the missing transverse momentum. Additional systematic uncertainties, including those on the pile-up description in the simulation, are considered and found to be negligible.In addition to the sources described above, systematic uncertainties on the SUSY signal cross section are estimated by varying the factorization and renormalization scales in PROSPINO up and down by a factor of two, by considering variations in αs, and by varying the proton PDFs within their uncertainties. These theoretical uncertainties total typically 8–12% across the relevant region of parameter space. Uncertainties are calculated separately for individual SUSY production processes.8

Results

Fig. 2

shows the distributions of ETmiss, pTτ, and meff for data with all selection requirements applied except for that on meff, along with the corresponding estimated backgrounds. The numbers of expected SM background events and the observed number of events after the meff requirement are shown in Table 3

. The data agree with the background expectation.

Based on these results, limits are placed on contributions beyond the SM to the signal region. With 11 events observed and 13.2±4.2 expected, an upper limit of 8.5 on the number of events observed due to non-SM sources is derived at 95% confidence level (C.L.). This limit corresponds to an upper limit on the visible cross section of 4.0fb, where the visible cross section is defined as the product of production cross section, branching fraction to at least one τ lepton, acceptance, and efficiency using the event selection defined in Section 5. For the two benchmark points Λ=30, tanβ=20 and Λ=40, tanβ=30 the product of branching ratio to τ-leptons, the acceptance and the efficiency for this selection amounts to 1.47% and 1.69%, respectively. Fig. 3

shows an interpretation of the result as a 95% C.L. exclusion limit in the Mmess=250 TeV, N5=3, μ>0, Cgrav=1 slice of the GMSB model. Fig. 3 also shows the variation of the expected limit in response to ±1σ fluctuations in the expected SM background and the SUSY cross sections. The excluded regions are calculated using a profile likelihood method with systematic uncertainties modeled as varying Gaussian-distributed nuisance parameters [78,79]. The resulting limit is compared with previous exclusion limits from searches for τ˜ and e˜ production and GMSB topologies at LEP. The region of small Λ and large tanβ is theoretically excluded since it leads to tachyonic states. In this model, the production of supersymmetric particles can be excluded at 95% C.L. up to Λ=30 TeV, independent of tanβ, and up to Λ=43 TeV for large values of tanβ.

Conclusions

In conclusion, this Letter presents a search for supersymmetry in final states containing jets, missing transverse momentum, and at least one τ lepton with the ATLAS experiment in s=7 TeV proton–proton collisions at the LHC. This is the first search in these final states at the LHC that includes events with one τ lepton. No excess of events is seen beyond the expected Standard Model backgrounds in 2.05fb−1 of data. Limits are placed on the visible cross section and in the context of GMSB models. The limits obtained extend the results from previous experiments.

Acknowledgements

We thank CERN for the very successful operation of the LHC, as well as the support staff from our institutions without whom ATLAS could not be operated efficiently.We acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, Chile; CAS, MOST and NSFC, China; COLCIENCIAS, Colombia; MSMT CR, MPO CR and VSC CR, Czech Republic; DNRF, DNSRC and Lundbeck Foundation, Denmark; EPLANET and ERC, European Union; IN2P3-CNRS, CEA-DSM/IRFU, France; GNAS, Georgia; BMBF, DFG, HGF, MPG and AvH Foundation, Germany; GSRT, Gerece; ISF, MINERVA, GIF, DIP and Benoziyo Center, Israel; INFN, Italy; MEXT and JSPS, Japan; CNRST, Morocco; FOM and NWO, Netherlands; RCN, Norway; MNiSW, Poland; GRICES and FCT, Portugal; MERYS (MECTS), Romania; MES of Russia and ROSATOM, Russian Federation; JINR; MSTD, Serbia; MSSR, Slovakia; ARRS and MVZT, Slovenia; DST/NRF, South Africa; MICINN, Spain; SRC and Wallenberg Foundation, Sweden; SER, SNSF and Cantons of Bern and Geneva, Switzerland; NSC, Taiwan; TAEK, Turkey; STFC, the Royal Society and Leverhulme Trust, United Kingdom; DOE and NSF, United States of America.The crucial computing support from all WLCG partners is acknowledged gratefully, in particular from CERN and the ATLAS Tier-1 facilities at TRIUMF (Canada), NDGF (Denmark, Norway, Sweden), CC-IN2P3 (France), KIT/GridKA (Germany), INFN-CNAF (Italy), NL-T1 (Netherlands), PIC (Spain), ASGC (Taiwan), RAL (UK) and BNL (USA) and in the Tier-2 facilities worldwide.

Open access

This article is published Open Access at sciencedirect.com. It is distributed under the terms of the Creative Commons Attribution License 3.0, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are credited.

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