CERN Accelerating science

002036481 001__ 2036481
002036481 003__ SzGeCERN
002036481 005__ 20220121041225.0
002036481 0247_ $$2DOI$$a10.1103/PhysRevD.92.052007
002036481 0248_ $$aoai:cds.cern.ch:2036481$$pcerncds:FULLTEXT$$pcerncds:CERN:FULLTEXT$$pcerncds:CERN
002036481 035__ $$9arXiv$$aoai:arXiv.org:1507.05666
002036481 035__ $$9Inspire$$a1384115
002036481 037__ $$9arXiv$$aarXiv:1507.05666$$chep-ex
002036481 037__ $$aFERMILAB-PUB-15-312-E
002036481 041__ $$aeng
002036481 088__ $$aFERMILAB-PUB-15-312-E
002036481 100__ $$aAbazov, Victor Mukhamedovich$$iINSPIRE-00039200$$uDubna, JINR$$vJoint Institute for Nuclear Research , Dubna, Russia
002036481 245__ $$aSimultaneous measurement of forward-backward asymmetry and top polarization in dilepton final states from $t\bar t$ production at the Tevatron
002036481 246__ $$9arXiv$$aSimultaneous measurement of forward-backward asymmetry and top polarization in dilepton final states from $t\bar t$ production at the Tevatron
002036481 269__ $$c20 Jul 2015
002036481 260__ $$c2015-09-22
002036481 300__ $$a16 p
002036481 500__ $$9arXiv$$a16 pages, 16 figures, published version
002036481 520__ $$aWe present a simultaneous measurement of the forward-backward asymmetry and the top-quark polarization in $t\bar t$ production in dilepton final states using 9.7 fb$^{-1}$ of proton-antiproton collisions at $\sqrt{s}=1.96$ TeV with the D0 detector. To reconstruct the distributions of kinematic observables we employ a matrix element technique that calculates the likelihood of the possible $t\bar t$ kinematic configurations. After accounting for the presence of background events and for calibration effects, we obtain a forward-backward asymmetry of $A^{t\bar t} = (15.0 \pm 6.4 \text{ (stat)} \pm 4.9 \text{ (syst)})\%$ and a top-quark polarization times spin analyzing power in the beam basis of $\kappa P = (7.2 \pm 10.5 \text{ (stat)} \pm 4.2 \text{ (syst)})\%$, with a correlation of $-56\%$ between the measurements. If we constrain the forward-backward asymmetry to its expected standard model value, we obtain a measurement of the top polarization of $\kappa P = (11.3 \pm 9.1 \text{ (stat)} \pm 1.9 \text{ (syst)})\%.$ If we constrain the top polarization to its expected standard model value, we measure a forward-backward asymmetry of $A^{t\bar t} = (17.5 \pm 5.6 \text{ (stat)} \pm 3.1 \text{ (syst)})\%.$ A combination with the D0 $A^{t\bar t}$ measurement in the lepton+jets final state yields an asymmetry of $ A^{t\bar t} = (11.8 \pm 2.5 \text{ (stat)} \pm 1.3 \text{ (syst)})\% . $ Within their respective uncertainties, all these results are consistent with the standard model expectations.
002036481 520__ $$9APS$$aWe present a simultaneous measurement of the forward-backward asymmetry and the top-quark polarization in tt¯ production in dilepton final states using 9.7  fb-1 of proton-antiproton collisions at s=1.96  TeV with the D0 detector. To reconstruct the distributions of kinematic observables we employ a matrix element technique that calculates the likelihood of the possible tt¯ kinematic configurations. After accounting for the presence of background events and for calibration effects, we obtain a forward-backward asymmetry of Att¯=(15.0±6.4(stat)±4.9(syst))% and a top-quark polarization times spin analyzing power in the beam basis of κP=(7.2±10.5(stat)±4.2(syst))%, with a correlation of -56% between the measurements. If we constrain the forward-backward asymmetry to its expected standard model value, we obtain a measurement of the top polarization of κP=(11.3±9.1(stat)±1.9(syst))%. If we constrain the top polarization to its expected standard model value, we measure a forward-backward asymmetry of Att¯=(17.5±5.6(stat)±3.1(syst))%. A combination with the D0 Att¯ measurement in the lepton+jets final state yields an asymmetry of Att¯=(11.8±2.5(stat)±1.3(syst))%. Within their respective uncertainties, all these results are consistent with the standard model expectations.
002036481 520__ $$9arXiv$$aWe present a simultaneous measurement of the forward-backward asymmetry and the top-quark polarization in $t\bar t$ production in dilepton final states using 9.7 fb$^{-1}$ of proton-antiproton collisions at $\sqrt{s}=1.96$ TeV with the D0 detector. To reconstruct the distributions of kinematic observables we employ a matrix element technique that calculates the likelihood of the possible $t\bar t$ kinematic configurations. After accounting for the presence of background events and for calibration effects, we obtain a forward-backward asymmetry of $A^{t\bar t} = (15.0 \pm 6.4 \text{ (stat)} \pm 4.9 \text{ (syst)})\%$ and a top-quark polarization times spin analyzing power in the beam basis of $\kappa P = (7.2 \pm 10.5 \text{ (stat)} \pm 4.2 \text{ (syst)})\%$, with a correlation of $-56\%$ between the measurements. If we constrain the forward-backward asymmetry to its expected standard model value, we obtain a measurement of the top polarization of $\kappa P = (11.3 \pm 9.1 \text{ (stat)} \pm 1.9 \text{ (syst)})\%.$ If we constrain the top polarization to its expected standard model value, we measure a forward-backward asymmetry of $A^{t\bar t} = (17.5 \pm 5.6 \text{ (stat)} \pm 3.1 \text{ (syst)})\%.$ A combination with the D0 $A^{t\bar t}$ measurement in the lepton+jets final state yields an asymmetry of $ A^{t\bar t} = (11.8 \pm 2.5 \text{ (stat)} \pm 1.3 \text{ (syst)})\% . $ Within their respective uncertainties, all these results are consistent with the standard model expectations.
002036481 540__ $$aarXiv nonexclusive-distrib. 1.0$$barXiv$$uhttp://arxiv.org/licenses/nonexclusive-distrib/1.0/
002036481 542__ $$3Publication$$dAmerican Physical Society$$g2015
002036481 595__ $$aLANL EDS
002036481 595__ $$aNot for annual report
002036481 595__ $$aNot CERN
002036481 65017 $$2arXiv$$aParticle Physics - Experiment
002036481 65027 $$2arXiv$$aParticle Physics - Phenomenology
002036481 690C_ $$aARTICLE
002036481 695__ $$9LANL EDS$$ahep-ex
002036481 690C_ $$aCERN
002036481 695__ $$9LANL EDS$$ahep-ph
002036481 700__ $$aAbbott, Braden Keim$$iINSPIRE-00060668$$uOklahoma U.
002036481 700__ $$aAcharya, Bannanje Sripath$$iINSPIRE-00000955$$uTata Inst.
002036481 700__ $$aAdams, Mark Raymond$$iINSPIRE-00300252$$uIllinois U., Chicago
002036481 700__ $$aAdams, Todd$$iINSPIRE-00060942$$uFlorida State U.
002036481 700__ $$aAgnew, James P$$iINSPIRE-00371378$$uManchester U., Comp. Sci. Dept.
002036481 700__ $$aAlexeev, Guennadi D$$iINSPIRE-00061533$$uDubna, JINR
002036481 700__ $$aAlkhazov, Georgiy D$$iINSPIRE-00061628$$uSt. Petersburg, INP
002036481 700__ $$aAlton, Andrew K$$iINSPIRE-00061762$$uAugustana Coll., Sioux Falls$$uMichigan U.
002036481 700__ $$aAskew, Andrew Warren$$iINSPIRE-00053983$$uFlorida State U.
002036481 700__ $$aAtkins, Scott$$iINSPIRE-00002192$$uLouisiana Tech. U.
002036481 700__ $$aAugsten, Kamil$$uPrague, Tech. U.
002036481 700__ $$aAvila, Carlos A$$iINSPIRE-00063395$$uAndes U., Bogota
002036481 700__ $$aBadaud, Frederique$$iINSPIRE-00063691$$uClermont-Ferrand U.
002036481 700__ $$aBagby, Linda F$$iINSPIRE-00063740$$uFermilab
002036481 700__ $$aBaldin, Boris$$iINSPIRE-00003843$$uFermilab
002036481 700__ $$aBandurin, Dmitry V$$iINSPIRE-00039144$$uVirginia U.
002036481 700__ $$aBanerjee, Sunanda$$iINSPIRE-00064259$$uTata Inst.
002036481 700__ $$aBarberis, Emanuela$$iINSPIRE-00064380$$uNortheastern U.
002036481 700__ $$aBaringer, Philip S$$iINSPIRE-00064543$$uKansas U.
002036481 700__ $$aBartlett, JFrederick$$iINSPIRE-00064938$$uFermilab
002036481 700__ $$aBassler, Ursula Rita$$iINSPIRE-00065057$$uDAPNIA, Saclay
002036481 700__ $$aBazterra, Victor$$iINSPIRE-00011503$$uIllinois U., Chicago
002036481 700__ $$aBean, Alice L$$iINSPIRE-00065301$$uKansas U.
002036481 700__ $$aBegalli, Marcia$$iINSPIRE-00065602$$uRio de Janeiro State U.
002036481 700__ $$aBellantoni, Leo$$iINSPIRE-00065789$$uFermilab
002036481 700__ $$aBeri, Suman B$$iINSPIRE-00045688$$uPanjab U.
002036481 700__ $$aBernardi, Gregorio$$iINSPIRE-00066505$$uParis U., VI-VII
002036481 700__ $$aBernhard, Ralf Patrick$$iINSPIRE-00053972$$uFreiburg U.
002036481 700__ $$aBertram, Iain A$$iINSPIRE-00066653$$uLancaster U.
002036481 700__ $$aBesancon, Marc$$iINSPIRE-00066690$$uDAPNIA, Saclay
002036481 700__ $$aBeuselinck, Raymond$$iINSPIRE-00066717$$uImperial Coll., London
002036481 700__ $$aBhat, Pushpalatha C$$iINSPIRE-00066824$$uFermilab
002036481 700__ $$aBhatia, Sudeep$$iINSPIRE-00333490$$uMississippi U.
002036481 700__ $$aBhatnagar, Vipin$$iINSPIRE-00050934$$uPanjab U.
002036481 700__ $$aBlazey, Gerald Charles$$iINSPIRE-00067428$$uNorthern Illinois U.
002036481 700__ $$aBlessing, Susan K$$iINSPIRE-00067450$$uFlorida State U.
002036481 700__ $$aBloom, Kenneth A$$iINSPIRE-00067576$$uNebraska U.
002036481 700__ $$aBoehnlein, Amber S$$iINSPIRE-00067761$$uFermilab
002036481 700__ $$aBoline, Daniel Dooley$$iINSPIRE-00025121$$uSUNY, Stony Brook
002036481 700__ $$aBoos, Edward E$$iINSPIRE-00068140$$uMoscow State U.
002036481 700__ $$aBorissov, Guennadi$$iINSPIRE-00068300$$uLancaster U.
002036481 700__ $$aBorysova, Maryna$$iINSPIRE-00366281$$uKiev, INR$$uTaras Shevchenko U.
002036481 700__ $$aBrandt, Andrew$$iINSPIRE-00300274$$uTexas U., Arlington
002036481 700__ $$aBrandt, Oleg$$iINSPIRE-00184109$$uGottingen U., Zweites Phys. Inst.
002036481 700__ $$aBrock, Raymond L$$iINSPIRE-00069341$$uMichigan State U.
002036481 700__ $$aBross, Alan D$$iINSPIRE-00069476$$uFermilab
002036481 700__ $$aBrown, Duncan Paul$$iINSPIRE-00007195$$uParis U., VI-VII
002036481 700__ $$aBu, Xue-Bing$$iINSPIRE-00036532$$uFermilab
002036481 700__ $$aBuehler, Marc$$iINSPIRE-00049024$$uFermilab
002036481 700__ $$aBuescher, Volker$$iINSPIRE-00070225$$uMainz U., Inst. Phys.
002036481 700__ $$aBunichev, Viacheslav Yevgenyevich$$iINSPIRE-00040479$$uMoscow State U.
002036481 700__ $$aBurdin, Sergey$$iINSPIRE-00022855$$uLiverpool U.$$uLancaster U.
002036481 700__ $$aBuszello, Claus Peter$$iINSPIRE-00044211$$uUppsala U.
002036481 700__ $$aCamacho-Perez, Enrique$$iINSPIRE-00301173$$uCINVESTAV, IPN
002036481 700__ $$aCasey, Brendan Cameron Kieran$$iINSPIRE-00071454$$uFermilab
002036481 700__ $$aCastilla-Valdez, Heriberto$$iINSPIRE-00071581$$uCINVESTAV, IPN
002036481 700__ $$aCaughron, Seth Aaron$$iINSPIRE-00301352$$uMichigan State U.
002036481 700__ $$aChakrabarti, Subhendu$$iINSPIRE-00005693$$uSUNY, Stony Brook
002036481 700__ $$aChan, Kwok Ming Leo$$iINSPIRE-00032189$$uNotre Dame U.
002036481 700__ $$aChandra, Avdhesh$$iINSPIRE-00039123$$uRice U.
002036481 700__ $$aChapon, Emilien$$iINSPIRE-00015039$$uDAPNIA, Saclay
002036481 700__ $$aChen, Guo$$iINSPIRE-00176968$$uKansas U.
002036481 700__ $$aCho, Sung-Woong$$iINSPIRE-00302582$$uKorea U., KODEL
002036481 700__ $$aChoi, Suyong$$iINSPIRE-00050694$$uKorea U., KODEL
002036481 700__ $$aChoudhary, Brajesh C$$iINSPIRE-00073233$$uDelhi U.
002036481 700__ $$aCihangir, Selcuk$$iINSPIRE-00073533$$uFermilab
002036481 700__ $$aClaes, Daniel R$$iINSPIRE-00073648$$uNebraska U.
002036481 700__ $$aClutter, Justace Randall$$iINSPIRE-00046636$$uKansas U.
002036481 700__ $$aCooke, Michael P$$iINSPIRE-00003477$$uAAAS, Washington, D.C.$$uFermilab
002036481 700__ $$aCooper, William Edward$$iINSPIRE-00074406$$uFermilab
002036481 700__ $$aCorcoran, Marjorie D$$iINSPIRE-00074488$$uRice U.
002036481 700__ $$aCouderc, Fabrice$$iINSPIRE-00043207$$uDAPNIA, Saclay
002036481 700__ $$aCousinou, Marie-Claude$$iINSPIRE-00074742$$uMarseille, CPPM
002036481 700__ $$aCuth, Jakub$$iINSPIRE-00384079$$uMainz U., Inst. Phys.
002036481 700__ $$aCutts, David$$iINSPIRE-00075324$$uBrown U.
002036481 700__ $$aDas, Amitabha$$iINSPIRE-00075742$$uSouthern Methodist U.
002036481 700__ $$aDavies, Gavin John$$iINSPIRE-00075967$$uImperial Coll., London
002036481 700__ $$ade Jong, Sijbrand Jan$$iINSPIRE-00093890$$uNijmegen U.$$uNIKHEF, Amsterdam
002036481 700__ $$aDe La Cruz-Burelo, Eduard$$iINSPIRE-00039100$$uCINVESTAV, IPN
002036481 700__ $$aDeliot, Frederic$$iINSPIRE-00076511$$uDAPNIA, Saclay
002036481 700__ $$aDemina, Regina$$iINSPIRE-00076615$$uRochester U.
002036481 700__ $$aDenisov, Dmitri S$$iINSPIRE-00076696$$uFermilab
002036481 700__ $$aDenisov, Sergei P$$iINSPIRE-00076710$$uSerpukhov, IHEP
002036481 700__ $$aDesai, Satish Vijay$$iINSPIRE-00032804$$uFermilab
002036481 700__ $$aDeterre, Cecile$$iINSPIRE-00220614$$uDESY$$uManchester U., Comp. Sci. Dept.
002036481 700__ $$aDeVaughan, Kayle Otis$$iINSPIRE-00008898$$uNebraska U.
002036481 700__ $$aDiehl, HThomas$$iINSPIRE-00077147$$uFermilab
002036481 700__ $$aDiesburg, Michael$$iINSPIRE-00077172$$uFermilab
002036481 700__ $$aDing, Pengfei$$iINSPIRE-00014205$$uManchester U., Comp. Sci. Dept.
002036481 700__ $$aDominguez, DAaron M$$iINSPIRE-00077677$$uNebraska U.
002036481 700__ $$aDubey, Abhinav Kumar$$iINSPIRE-00300331$$uDelhi U.
002036481 700__ $$aDudko, Lev V$$iINSPIRE-00078338$$uMoscow State U.
002036481 700__ $$aDuperrin, Arnaud$$iINSPIRE-00078558$$uMarseille, CPPM
002036481 700__ $$aDutt, Suneel$$iINSPIRE-00018823$$uPanjab U.
002036481 700__ $$aEads, Michael T$$iINSPIRE-00051750$$uNorthern Illinois U.
002036481 700__ $$aEdmunds, Daniel L$$iINSPIRE-00004510$$uMichigan State U.
002036481 700__ $$aEllison, John A$$iINSPIRE-00079386$$uUC, Riverside
002036481 700__ $$aElvira, VDaniel$$iINSPIRE-00079440$$uFermilab
002036481 700__ $$aEnari, Yuji$$iINSPIRE-00079531$$uParis U., VI-VII
002036481 700__ $$aEvans, Harold G$$iINSPIRE-00080060$$uIndiana U.
002036481 700__ $$aEvdokimov, Anatoly V$$iINSPIRE-00021972$$uIllinois U., Chicago
002036481 700__ $$aEvdokimov, Valeri N$$iINSPIRE-00300342$$uSerpukhov, IHEP
002036481 700__ $$aFaure, Alexandre$$iINSPIRE-00288957$$uDAPNIA, Saclay
002036481 700__ $$aFeng, Lei$$iINSPIRE-00301325$$uNorthern Illinois U.
002036481 700__ $$aFerbel, Thomas$$iINSPIRE-00080790$$uRochester U.
002036481 700__ $$aFiedler, Frank$$iINSPIRE-00081065$$uMainz U., Inst. Phys.
002036481 700__ $$aFilthaut, Frank$$iINSPIRE-00081209$$uNijmegen U.$$uNIKHEF, Amsterdam
002036481 700__ $$aFisher, Wade Cameron$$iINSPIRE-00052479$$uMichigan State U.
002036481 700__ $$aFisk, HEugene$$iINSPIRE-00081503$$uFermilab
002036481 700__ $$aFortner, Michael R$$iINSPIRE-00300353$$uNorthern Illinois U.
002036481 700__ $$aFox, Harald$$iINSPIRE-00082068$$uLancaster U.
002036481 700__ $$aFuess, Stuart C$$iINSPIRE-00082800$$uFermilab
002036481 700__ $$aGarbincius, Peter H$$iINSPIRE-00083572$$uFermilab
002036481 700__ $$aGarcia-Bellido, Aran$$iINSPIRE-00058621$$uRochester U.
002036481 700__ $$aGarcia-Gonzalez, Jose Andres$$iINSPIRE-00201259$$uCINVESTAV, IPN
002036481 700__ $$aGavrilov, Vladimir B$$iINSPIRE-00306950$$uMoscow, ITEP
002036481 700__ $$aGeng, Weigang$$iINSPIRE-00017095$$uMichigan State U.$$uMarseille, CPPM
002036481 700__ $$aGerber, Cecilia Elena$$iINSPIRE-00084394$$uIllinois U., Chicago
002036481 700__ $$aGershtein, Yuri S$$iINSPIRE-00058255$$uRutgers U., Piscataway
002036481 700__ $$aGinther, George E$$iINSPIRE-00084917$$uRochester U.$$uFermilab
002036481 700__ $$aGogota, Olga$$iINSPIRE-00184420$$uTaras Shevchenko U.
002036481 700__ $$aGolovanov, Georgy Anatolievich$$iINSPIRE-00018415$$uDubna, JINR
002036481 700__ $$aGrannis, Paul D$$iINSPIRE-00086404$$uSUNY, Stony Brook
002036481 700__ $$aGreder, Sebastien$$iINSPIRE-00300397$$uLouis Pasteur U., Strasbourg I
002036481 700__ $$aGreenlee, Herbert B$$iINSPIRE-00086638$$uFermilab
002036481 700__ $$aGrenier, Gerald Jean$$iINSPIRE-00086736$$uLyon, IPN
002036481 700__ $$aGris, Phillipe Luc$$iINSPIRE-00086824$$uClermont-Ferrand U.
002036481 700__ $$aGrivaz, Jean-Francois$$iINSPIRE-00086861$$uOrsay, LAL
002036481 700__ $$aGrohsjean, Alexander$$iINSPIRE-00018559$$uDESY$$uDAPNIA, Saclay
002036481 700__ $$aGruenendahl, Stefan$$iINSPIRE-00087119$$uFermilab
002036481 700__ $$aGruenewald, Martin Werner$$iINSPIRE-00087140$$uUniversity Coll., Dublin
002036481 700__ $$aGuillemin, Thibault$$iINSPIRE-00180576$$uOrsay, LAL
002036481 700__ $$aGutierrez, Gaston R$$iINSPIRE-00087511$$uFermilab
002036481 700__ $$aGutierrez, Phillip$$iINSPIRE-00087527$$uOklahoma U.
002036481 700__ $$aHaley, Joseph Glenn Biddle$$iINSPIRE-00006781$$uOklahoma State U.
002036481 700__ $$aHan, Liang$$iINSPIRE-00037384$$uHefei, CUST
002036481 700__ $$aHarder, Kristian$$iINSPIRE-00088612$$uManchester U., Comp. Sci. Dept.
002036481 700__ $$aHarel, Amnon$$iINSPIRE-00048598$$uRochester U.
002036481 700__ $$aHauptman, John Michael$$iINSPIRE-00089150$$uIowa State U.
002036481 700__ $$aHays, Jonathan M$$iINSPIRE-00005408$$uImperial Coll., London
002036481 700__ $$aHead, Tim$$iINSPIRE-00002216$$uManchester U., Comp. Sci. Dept.
002036481 700__ $$aHebbeker, Thomas$$iINSPIRE-00089340$$uAachen, Tech. Hochsch.
002036481 700__ $$aHedin, David R$$iINSPIRE-00089387$$uNorthern Illinois U.
002036481 700__ $$aHegab, Hatim$$iINSPIRE-00032151$$uOklahoma State U.
002036481 700__ $$aHeinson, Ann$$iINSPIRE-00089535$$uUC, Riverside
002036481 700__ $$aHeintz, Ulrich$$iINSPIRE-00089547$$uBrown U.
002036481 700__ $$aHensel, Carsten$$iINSPIRE-00046890$$uRio de Janeiro, CBPF
002036481 700__ $$aHeredia-De La Cruz, Ivan$$iINSPIRE-00014576$$uConacyt, Mexico$$uCINVESTAV, IPN
002036481 700__ $$aHerner, Kenneth Richard$$iINSPIRE-00006570$$uFermilab
002036481 700__ $$aHesketh, Gavin G$$iINSPIRE-00054306$$uUniversity Coll. London$$uManchester U., Comp. Sci. Dept.
002036481 700__ $$aHildreth, Michael D$$iINSPIRE-00090190$$uNotre Dame U.
002036481 700__ $$aHirosky, Robert James$$iINSPIRE-00090388$$uVirginia U.
002036481 700__ $$aHoang, Trang$$iINSPIRE-00180370$$uFlorida State U.
002036481 700__ $$aHobbs, John D$$iINSPIRE-00090491$$uSUNY, Stony Brook
002036481 700__ $$aHoeneisen, Bruce$$iINSPIRE-00090561$$uSan Francisco de Quito U.
002036481 700__ $$aHogan, Julie$$iINSPIRE-00201235$$uRice U.
002036481 700__ $$aHohlfeld, Mark$$iINSPIRE-00039005$$uMainz U., Inst. Phys.
002036481 700__ $$aHolzbauer, Jenny Lyn$$iINSPIRE-00215760$$uMississippi U.
002036481 700__ $$aHowley, Ian James$$iINSPIRE-00236401$$uTexas U., Arlington
002036481 700__ $$aHubacek, Zdenek$$iINSPIRE-00032940$$uDAPNIA, Saclay$$uPrague, Tech. U.
002036481 700__ $$aHynek, Vlastislav$$iINSPIRE-00038993$$uPrague, Tech. U.
002036481 700__ $$aIashvili, Ia$$iINSPIRE-00091832$$uSUNY, Buffalo
002036481 700__ $$aIlchenko, Yuriy$$iINSPIRE-00180687$$uSouthern Methodist U.
002036481 700__ $$aIllingworth, Robert A$$iINSPIRE-00052545$$uFermilab
002036481 700__ $$aIto, Albert S$$iINSPIRE-00092514$$uFermilab
002036481 700__ $$aJabeen, Shabnam$$iINSPIRE-00038975$$uMaryland U., College Park$$uFermilab
002036481 700__ $$aJaffre, Michel J$$iINSPIRE-00092923$$uOrsay, LAL
002036481 700__ $$aJayasinghe, Ayesh$$iINSPIRE-00180326$$uOklahoma U.
002036481 700__ $$aJeong, Min-Soo$$iINSPIRE-00205076$$uKorea U., KODEL
002036481 700__ $$aJesik, Richard L$$iINSPIRE-00093383$$uImperial Coll., London
002036481 700__ $$aJiang, Peng$$iINSPIRE-00233577$$uHefei, CUST
002036481 700__ $$aJohns, Kenneth Arthur$$iINSPIRE-00093591$$uArizona U.
002036481 700__ $$aJohnson, Emily$$iINSPIRE-00347646$$uMichigan State U.
002036481 700__ $$aJohnson, Marvin E$$iINSPIRE-00093653$$uFermilab
002036481 700__ $$aJonckheere, Alan M$$iINSPIRE-00093762$$uFermilab
002036481 700__ $$aJonsson, Per Martin$$iINSPIRE-00093909$$uImperial Coll., London
002036481 700__ $$aJoshi, Jyoti$$iINSPIRE-00019290$$uUC, Riverside
002036481 700__ $$aJung, Andreas Werner$$iINSPIRE-00183962$$uFermilab
002036481 700__ $$aJuste, Aurelio$$iINSPIRE-00094149$$uICREA, Barcelona
002036481 700__ $$aKajfasz, Eric$$iINSPIRE-00094346$$uMarseille, CPPM
002036481 700__ $$aKarmanov, Dmitriy Y$$iINSPIRE-00000967$$uMoscow State U.
002036481 700__ $$aKatsanos, Ioannis$$iINSPIRE-00038956$$uNebraska U.
002036481 700__ $$aKaur, Manbir$$iINSPIRE-00357567$$uPanjab U.
002036481 700__ $$aKehoe, Robert Leo Patrick$$iINSPIRE-00095456$$uSouthern Methodist U.
002036481 700__ $$aKermiche, Smain$$iINSPIRE-00050283$$uMarseille, CPPM
002036481 700__ $$aKhalatyan, Norayr$$iINSPIRE-00032939$$uFermilab
002036481 700__ $$aKhanov, Alexander$$iINSPIRE-00053352$$uOklahoma State U.
002036481 700__ $$aKharchilava, Avto$$iINSPIRE-00095916$$uSUNY, Buffalo
002036481 700__ $$aKharzheev, Yuri N$$iINSPIRE-00000177$$uDubna, JINR
002036481 700__ $$aKiselevich, Ivan Lvovich$$iINSPIRE-00301225$$uMoscow, ITEP
002036481 700__ $$aKohli, Jatinder M$$iINSPIRE-00003839$$uPanjab U.
002036481 700__ $$aKozelov, Alexander V$$iINSPIRE-00038927$$uSerpukhov, IHEP
002036481 700__ $$aKraus, James Alexander$$iINSPIRE-00025588$$uMississippi U.
002036481 700__ $$aKumar, Ashish$$iINSPIRE-00026358$$uSUNY, Buffalo
002036481 700__ $$aKupco, Alexander$$iINSPIRE-00099163$$uPrague, Inst. Phys.
002036481 700__ $$aKurca, Tibor$$iINSPIRE-00099209$$uLyon, IPN
002036481 700__ $$aKuzmin, Valentin Alexandrovich$$iINSPIRE-00046985$$uMoscow State U.
002036481 700__ $$aLammers, Sabine Wedam$$iINSPIRE-00051670$$uIndiana U.
002036481 700__ $$aLebrun, Patrice$$iINSPIRE-00100449$$uLyon, IPN
002036481 700__ $$aLee, Hyeon-Seung$$iINSPIRE-00302606$$uKorea U., KODEL
002036481 700__ $$aLee, Seh-Wook$$iINSPIRE-00255287$$uIowa State U.
002036481 700__ $$aLee, William M$$iINSPIRE-00100793$$uFermilab
002036481 700__ $$aLei, Xiaowen$$iINSPIRE-00219018$$uArizona U.
002036481 700__ $$aLellouch, Jeremie$$iINSPIRE-00024906$$uParis U., VI-VII
002036481 700__ $$aLi, Dikai$$iINSPIRE-00271549$$uParis U., VI-VII
002036481 700__ $$aLi, Hengne$$iINSPIRE-00333509$$uVirginia U.
002036481 700__ $$aLi, Liang$$iINSPIRE-00300470$$uUC, Riverside
002036481 700__ $$aLi, Qi-Zhong$$iINSPIRE-00101541$$uFermilab
002036481 700__ $$aLim, Jeong Ku$$iINSPIRE-00011894$$uKorea U., KODEL
002036481 700__ $$aLincoln, Donald W$$iINSPIRE-00101920$$uFermilab
002036481 700__ $$aLinnemann, James Thomas$$iINSPIRE-00300481$$uMichigan State U.
002036481 700__ $$aLipaev, Vladimir V$$iINSPIRE-00038891$$uSerpukhov, IHEP
002036481 700__ $$aLipton, Ronald J$$iINSPIRE-00102104$$uFermilab
002036481 700__ $$aLiu, Huanzhao$$iINSPIRE-00348078$$uSouthern Methodist U.
002036481 700__ $$aLiu, Yanwen$$iINSPIRE-00034400$$uHefei, CUST
002036481 700__ $$aLobodenko, Alexandre$$iINSPIRE-00038878$$uSt. Petersburg, INP
002036481 700__ $$aLokajicek, Milos$$iINSPIRE-00278790$$uPrague, Inst. Phys.
002036481 700__ $$aLopes de Sa, Rafael$$iINSPIRE-00184069$$uFermilab
002036481 700__ $$aLuna-Garcia, Rene$$iINSPIRE-00017790$$uCIC, IPN$$uCINVESTAV, IPN
002036481 700__ $$aLyon, Adam Leonard$$iINSPIRE-00103329$$uFermilab
002036481 700__ $$aMaciel, Arthur KA$$iINSPIRE-00103569$$uRio de Janeiro, CBPF
002036481 700__ $$aMadar, Romain$$iINSPIRE-00301124$$uFreiburg U.
002036481 700__ $$aMagana-Villalba, Ricardo$$iINSPIRE-00014618$$uCINVESTAV, IPN
002036481 700__ $$aMalik, Sudhir$$iINSPIRE-00005081$$uNebraska U.
002036481 700__ $$aMalyshev, Vladimir L$$iINSPIRE-00300560$$uDubna, JINR
002036481 700__ $$aMansour, Jason$$iINSPIRE-00281038$$uGottingen U., Zweites Phys. Inst.
002036481 700__ $$aMartinez-Ortega, Jorge$$iINSPIRE-00014832$$uCINVESTAV, IPN
002036481 700__ $$aMcCarthy, Robert L$$iINSPIRE-00106112$$uSUNY, Stony Brook
002036481 700__ $$aMcgivern, Carrie Lynne$$iINSPIRE-00012446$$uManchester U., Comp. Sci. Dept.
002036481 700__ $$aMeijer, Melvin M$$iINSPIRE-00300571$$uNijmegen U.$$uNIKHEF, Amsterdam
002036481 700__ $$aMelnitchouk, Alexander S$$iINSPIRE-00054552$$uFermilab
002036481 700__ $$aMenezes, Diego D$$iINSPIRE-00011310$$uNorthern Illinois U.
002036481 700__ $$aMercadante, Pedro Galli$$iINSPIRE-00106948$$uABC Federal U.
002036481 700__ $$aMerkin, Mikhail M$$iINSPIRE-00055966$$uMoscow State U.
002036481 700__ $$aMeyer, Arnd$$iINSPIRE-00300593$$uAachen, Tech. Hochsch.
002036481 700__ $$aMeyer, Jorg Manfred$$iINSPIRE-00107296$$uKIT, Karlsruhe, SCC$$uGottingen U., Zweites Phys. Inst.
002036481 700__ $$aMiconi, Florian$$iINSPIRE-00180384$$uLouis Pasteur U., Strasbourg I
002036481 700__ $$aMondal, Naba K$$iINSPIRE-00300508$$uTata Inst.
002036481 700__ $$aMulhearn, Michael James$$iINSPIRE-00052395$$uVirginia U.
002036481 700__ $$aNagy, Elemer$$iINSPIRE-00110088$$uMarseille, CPPM
002036481 700__ $$aNarain, Meenakshi$$iINSPIRE-00110455$$uBrown U.
002036481 700__ $$aNayyar, Ruchika$$iINSPIRE-00301151$$uArizona U.
002036481 700__ $$aNeal, Homer A$$iINSPIRE-00300519$$uMichigan U.
002036481 700__ $$aNegret, Juan Pablo$$iINSPIRE-00110764$$uAndes U., Bogota
002036481 700__ $$aNeustroev, Petr V$$iINSPIRE-00021941$$uSt. Petersburg, INP
002036481 700__ $$aNguyen, Huong Thi$$iINSPIRE-00265368$$uVirginia U.
002036481 700__ $$aNunnemann, Thomas P$$iINSPIRE-00046334$$uMunich U.
002036481 700__ $$aHernandez Orduna, Jose de Jesus$$iINSPIRE-00010914$$uRice U.
002036481 700__ $$aOsman, Nicolas Ahmed$$iINSPIRE-00011554$$uMarseille, CPPM
002036481 700__ $$aOsta, Jyotsna$$iINSPIRE-00047228$$uNotre Dame U.
002036481 700__ $$aPal, Arnab$$iINSPIRE-00271611$$uTexas U., Arlington
002036481 700__ $$aParashar, Neeti$$iINSPIRE-00038772$$uPurdue U., Calumet
002036481 700__ $$aParihar, Vivek$$iINSPIRE-00011106$$uBrown U.
002036481 700__ $$aPark, Sung Keun$$iINSPIRE-00114681$$uKorea U., KODEL
002036481 700__ $$aPartridge, Richard A$$iINSPIRE-00114805$$uSLAC$$uBrown U.
002036481 700__ $$aParua, Nirmalya$$iINSPIRE-00114817$$uIndiana U.
002036481 700__ $$aPatwa, Abid$$iINSPIRE-00115127$$uDept. of Energy, Wash., D.C.$$uBrookhaven
002036481 700__ $$aPenning, Bjoern$$iINSPIRE-00007584$$uImperial Coll., London
002036481 700__ $$aPerfilov, Maxim Anatolyevich$$iINSPIRE-00036598$$uMoscow State U.
002036481 700__ $$aPeters, Reinhild Yvonne Fatima$$iINSPIRE-00008252$$uManchester U., Comp. Sci. Dept.
002036481 700__ $$aPetridis, Konstantinos$$iINSPIRE-00311357$$uManchester U., Comp. Sci. Dept.
002036481 700__ $$aPetrillo, Gianluca$$iINSPIRE-00019289$$uRochester U.
002036481 700__ $$aPetroff, Pierre$$iINSPIRE-00116049$$uOrsay, LAL
002036481 700__ $$aPleier, Marc-Andre$$iINSPIRE-00046720$$uBrookhaven
002036481 700__ $$aPodstavkov, Vladimir M$$iINSPIRE-00116960$$uFermilab
002036481 700__ $$aPopov, Alexey V$$iINSPIRE-00038751$$uSerpukhov, IHEP
002036481 700__ $$aPrewitt, Michelle$$iINSPIRE-00019110$$uRice U.
002036481 700__ $$aPrice, Darren$$iINSPIRE-00027472$$uManchester U., Comp. Sci. Dept.
002036481 700__ $$aProkopenko, Nikolay N$$iINSPIRE-00036409$$uSerpukhov, IHEP
002036481 700__ $$aQian, Jianming$$iINSPIRE-00118167$$uMichigan U.
002036481 700__ $$aQuadt, Arnulf$$iINSPIRE-00118216$$uGottingen U., Zweites Phys. Inst.
002036481 700__ $$aQuinn, Gene Breese$$iINSPIRE-00118291$$uMississippi U.
002036481 700__ $$aRatoff, Peter N$$iINSPIRE-00119089$$uLancaster U.
002036481 700__ $$aRazumov, Ivan A$$iINSPIRE-00012786$$uSerpukhov, IHEP
002036481 700__ $$aRipp-Baudot, Isabelle$$iINSPIRE-00038728$$uLouis Pasteur U., Strasbourg I
002036481 700__ $$aRizatdinova, Flera$$iINSPIRE-00048668$$uOklahoma State U.
002036481 700__ $$aRominsky, Mandy Kathleen$$iINSPIRE-00007250$$uFermilab
002036481 700__ $$aRoss, Anthony$$iINSPIRE-00301307$$uLancaster U.
002036481 700__ $$aRoyon, Christophe$$iINSPIRE-00121542$$uDAPNIA, Saclay
002036481 700__ $$aRubinov, Paul Michael$$iINSPIRE-00121638$$uFermilab
002036481 700__ $$aRuchti, Randal C$$iINSPIRE-00121660$$uNotre Dame U.
002036481 700__ $$aSajot, Gerard$$iINSPIRE-00122471$$uLPSC, Grenoble
002036481 700__ $$aSanchez-Hernandez, Alberto$$iINSPIRE-00122966$$uCINVESTAV, IPN
002036481 700__ $$aSanders, Michiel P$$iINSPIRE-00038712$$uMunich U.
002036481 700__ $$aSantos, Angelo Souza$$uSao Paulo, IFT$$uRio de Janeiro, CBPF
002036481 700__ $$aSavage, David G$$iINSPIRE-00002100$$uFermilab
002036481 700__ $$aSavitskyi, Mykola$$iINSPIRE-00366854$$uTaras Shevchenko U.
002036481 700__ $$aSawyer, HLee$$iINSPIRE-00123608$$uLouisiana Tech. U.
002036481 700__ $$aScanlon, Timothy P$$iINSPIRE-00038709$$uImperial Coll., London
002036481 700__ $$aSchamberger, RDean$$iINSPIRE-00123848$$uSUNY, Stony Brook
002036481 700__ $$aScheglov, Yury A$$iINSPIRE-00005552$$uSt. Petersburg, INP
002036481 700__ $$aSchellman, Heidi M$$iINSPIRE-00123914$$uNorthwestern U.
002036481 700__ $$aSchott, Matthias$$iINSPIRE-00223276$$uMainz U., Inst. Phys.
002036481 700__ $$aSchwanenberger, Christian$$iINSPIRE-00124643$$uManchester U., Comp. Sci. Dept.
002036481 700__ $$aSchwienhorst, Reinhard H$$iINSPIRE-00050408$$uMichigan State U.
002036481 700__ $$aSekaric, Jadranka$$iINSPIRE-00045058$$uKansas U.
002036481 700__ $$aSeverini, Horst$$iINSPIRE-00125370$$uOklahoma U.
002036481 700__ $$aShabalina, Elizaveta K$$iINSPIRE-00038690$$uGottingen U., Zweites Phys. Inst.
002036481 700__ $$aShary, Viacheslav V$$iINSPIRE-00006382$$uDAPNIA, Saclay
002036481 700__ $$aShaw, Savanna$$iINSPIRE-00347635$$uManchester U., Comp. Sci. Dept.
002036481 700__ $$aShchukin, Andrey A$$iINSPIRE-00038677$$uSerpukhov, IHEP
002036481 700__ $$aSimak, Vladislav J$$iINSPIRE-00126496$$uPrague, Tech. U.
002036481 700__ $$aSkubic, Patrick Louis$$iINSPIRE-00127003$$uOklahoma U.
002036481 700__ $$aSlattery, Paul F$$iINSPIRE-00127058$$uRochester U.
002036481 700__ $$aSmirnov, Dmitri V$$iINSPIRE-00034498$$uNotre Dame U.
002036481 700__ $$aSnow, Gregory R$$iINSPIRE-00127409$$uNebraska U.
002036481 700__ $$aSnow, Joel Mark$$iINSPIRE-00127419$$uLangston U.
002036481 700__ $$aSnyder, Scott Stuart$$iINSPIRE-00300553$$uBrookhaven
002036481 700__ $$aSoldner-Rembold, Stefan$$iINSPIRE-00127655$$uManchester U., Comp. Sci. Dept.
002036481 700__ $$aSonnenschein, Lars$$iINSPIRE-00045957$$uAachen, Tech. Hochsch.
002036481 700__ $$aSoustruznik, Karel$$iINSPIRE-00127970$$uCharles U.
002036481 700__ $$aStark, Jan$$iINSPIRE-00050567$$uLPSC, Grenoble
002036481 700__ $$aStoyanova, Dina A$$iINSPIRE-00038651$$uSerpukhov, IHEP
002036481 700__ $$aStrauss, Michael G$$iINSPIRE-00129297$$uOklahoma U.
002036481 700__ $$aSuter, Louise$$iINSPIRE-00301314$$uManchester U., Comp. Sci. Dept.
002036481 700__ $$aSvoisky, Peter V$$iINSPIRE-00018439$$uOklahoma U.
002036481 700__ $$aTitov, Maxim$$iINSPIRE-00047058$$uDAPNIA, Saclay
002036481 700__ $$aTokmenin, Valeriy V$$iINSPIRE-00038628$$uDubna, JINR
002036481 700__ $$aTsai, Yun-Tse$$iINSPIRE-00301371$$uRochester U.
002036481 700__ $$aTsybychev, Dmitri$$iINSPIRE-00132531$$uSUNY, Stony Brook
002036481 700__ $$aTuchming, Boris$$iINSPIRE-00038604$$uDAPNIA, Saclay
002036481 700__ $$aTully, Christopher George T$$iINSPIRE-00132570$$uPrinceton U.
002036481 700__ $$aUvarov, Lev$$iINSPIRE-00021932$$uSt. Petersburg, INP
002036481 700__ $$aUvarov, Sergey L$$iINSPIRE-00003810$$uSt. Petersburg, INP
002036481 700__ $$aUzunyan, Sergey A$$iINSPIRE-00025458$$uNorthern Illinois U.
002036481 700__ $$aVan Kooten, Richard J$$iINSPIRE-00133340$$uIndiana U.
002036481 700__ $$avan Leeuwen, Willem M$$iINSPIRE-00003808$$uNIKHEF, Amsterdam
002036481 700__ $$aVarelas, Nikos$$iINSPIRE-00133485$$uIllinois U., Chicago
002036481 700__ $$aVarnes, Erich W$$iINSPIRE-00133542$$uArizona U.
002036481 700__ $$aVasilyev, Igor A$$iINSPIRE-00038583$$uSerpukhov, IHEP
002036481 700__ $$aVerkheev, Alexander Yurievich$$iINSPIRE-00019172$$uDubna, JINR
002036481 700__ $$aVertogradov, Leonid S$$iINSPIRE-00038575$$uDubna, JINR
002036481 700__ $$aVerzocchi, Marco$$iINSPIRE-00133842$$uFermilab
002036481 700__ $$aVesterinen, Mika$$iINSPIRE-00014030$$uManchester U., Comp. Sci. Dept.
002036481 700__ $$aVilanova, Didier$$iINSPIRE-00133931$$uDAPNIA, Saclay
002036481 700__ $$aVokac, Petr$$iINSPIRE-00007099$$uPrague, Tech. U.
002036481 700__ $$aWahl, Horst D$$iINSPIRE-00134554$$uFlorida State U.
002036481 700__ $$aWang, Michael HLS$$iINSPIRE-00134871$$uFermilab
002036481 700__ $$aWarchol, Jadwiga$$iINSPIRE-00134960$$uNotre Dame U.
002036481 700__ $$aWatts, Gordon Thomas$$iINSPIRE-00135120$$uWashington U., Seattle
002036481 700__ $$aWayne, Mitchell R$$iINSPIRE-00135150$$uNotre Dame U.
002036481 700__ $$aWeichert, Jonas$$iINSPIRE-00328486$$uMainz U., Inst. Phys.
002036481 700__ $$aWelty-Rieger, Leah Christine$$iINSPIRE-00018450$$uNorthwestern U.
002036481 700__ $$aWilliams, Mark Richard James$$iINSPIRE-00136085$$uCERN$$uIndiana U.
002036481 700__ $$aWilson, Graham Wallace$$iINSPIRE-00136140$$uKansas U.
002036481 700__ $$aWobisch, Markus$$iINSPIRE-00136413$$uLouisiana Tech. U.
002036481 700__ $$aWood, Darien Robert$$iINSPIRE-00300234$$uNortheastern U.
002036481 700__ $$aWyatt, Terence R$$iINSPIRE-00136898$$uManchester U., Comp. Sci. Dept.
002036481 700__ $$aXie, Yunhe$$iINSPIRE-00007769$$uFermilab
002036481 700__ $$aYamada, Ryuji$$iINSPIRE-00137070$$uFermilab
002036481 700__ $$aYang, Siqi$$iINSPIRE-00187470$$uHefei, CUST
002036481 700__ $$aYasuda, Takahiro$$iINSPIRE-00137352$$uFermilab
002036481 700__ $$aYatsunenko, Yuriy A$$iINSPIRE-00137372$$uDubna, JINR
002036481 700__ $$aYe, Wanyu$$iINSPIRE-00336448$$uSUNY, Stony Brook
002036481 700__ $$aYe, Zhenyu$$iINSPIRE-00054712$$uFermilab
002036481 700__ $$aYin, Hang$$iINSPIRE-00038031$$uFermilab
002036481 700__ $$aYip, Kin$$iINSPIRE-00137490$$uBrookhaven
002036481 700__ $$aYoun, Sungwoo$$iINSPIRE-00038548$$uFermilab
002036481 700__ $$aYu, Jiaming$$iINSPIRE-00285170$$uMichigan U.
002036481 700__ $$aZennamo, Joseph$$iINSPIRE-00192060$$uSUNY, Buffalo
002036481 700__ $$aZhao, Tianqi Gilbert$$iINSPIRE-00219365$$uManchester U., Comp. Sci. Dept.
002036481 700__ $$aZhou, Bing$$iINSPIRE-00138410$$uMichigan U.
002036481 700__ $$aZhu, Junjie$$iINSPIRE-00053364$$uMichigan U.
002036481 700__ $$aZielinski, Marek$$iINSPIRE-00138535$$uRochester U.
002036481 700__ $$aZieminska, Daria$$iINSPIRE-00138550$$uIndiana U.
002036481 700__ $$aZivkovic, Lidija$$iINSPIRE-00057284$$uParis U., VI-VII
002036481 710__ $$gD0 Collaboration
002036481 773__ $$c052007$$oPhys. Rev. D 92, 052007 (2015)$$pPhys. Rev. D$$v92$$y2015
002036481 8564_ $$uhttp://lss.fnal.gov/archive/2015/pub/fermilab-pub-15-312-e.pdf$$yFermilab Accepted Manuscript
002036481 8564_ $$82215806$$s388228$$uhttp://cds.cern.ch/record/2036481/files/arXiv:1507.05666.pdf
002036481 8564_ $$82215797$$s26860$$uhttp://cds.cern.ch/record/2036481/files/h_6.png$$y00002 [color online] Comparison of distributions between data and MC simulations at the final selection for (a) the transverse momentum of the leading lepton, (b) the transverse momentum of the secondary lepton, (c) the pseudorapidity of the leading lepton, (d) the pseudorapidity of the secondary lepton, (e) the transverse momentum of the leading jet, (f) the transverse momentum of the secondary jet, (g) the $H_T$, and (h) the difference between the two lepton pseudorapidities. The overflow bin content has been added to the last bin.
002036481 8564_ $$82215798$$s26978$$uhttp://cds.cern.ch/record/2036481/files/h_7.png$$y00003 [color online] Comparison of distributions between data and MC simulations at the final selection for (a) the transverse momentum of the leading lepton, (b) the transverse momentum of the secondary lepton, (c) the pseudorapidity of the leading lepton, (d) the pseudorapidity of the secondary lepton, (e) the transverse momentum of the leading jet, (f) the transverse momentum of the secondary jet, (g) the $H_T$, and (h) the difference between the two lepton pseudorapidities. The overflow bin content has been added to the last bin.
002036481 8564_ $$82215799$$s29624$$uhttp://cds.cern.ch/record/2036481/files/h_4.png$$y00004 [color online] Comparison of distributions between data and MC simulations at the final selection for (a) the transverse momentum of the leading lepton, (b) the transverse momentum of the secondary lepton, (c) the pseudorapidity of the leading lepton, (d) the pseudorapidity of the secondary lepton, (e) the transverse momentum of the leading jet, (f) the transverse momentum of the secondary jet, (g) the $H_T$, and (h) the difference between the two lepton pseudorapidities. The overflow bin content has been added to the last bin.
002036481 8564_ $$82215800$$s29625$$uhttp://cds.cern.ch/record/2036481/files/h_5.png$$y00005 [color online] Comparison of distributions between data and MC simulations at the final selection for (a) the transverse momentum of the leading lepton, (b) the transverse momentum of the secondary lepton, (c) the pseudorapidity of the leading lepton, (d) the pseudorapidity of the secondary lepton, (e) the transverse momentum of the leading jet, (f) the transverse momentum of the secondary jet, (g) the $H_T$, and (h) the difference between the two lepton pseudorapidities. The overflow bin content has been added to the last bin.
002036481 8564_ $$82215801$$s28940$$uhttp://cds.cern.ch/record/2036481/files/h_2.png$$y00000 [color online] Comparison of distributions between data and MC simulations at the final selection for (a) the transverse momentum of the leading lepton, (b) the transverse momentum of the secondary lepton, (c) the pseudorapidity of the leading lepton, (d) the pseudorapidity of the secondary lepton, (e) the transverse momentum of the leading jet, (f) the transverse momentum of the secondary jet, (g) the $H_T$, and (h) the difference between the two lepton pseudorapidities. The overflow bin content has been added to the last bin.
002036481 8564_ $$82215802$$s25621$$uhttp://cds.cern.ch/record/2036481/files/h_3.png$$y00001 [color online] Comparison of distributions between data and MC simulations at the final selection for (a) the transverse momentum of the leading lepton, (b) the transverse momentum of the secondary lepton, (c) the pseudorapidity of the leading lepton, (d) the pseudorapidity of the secondary lepton, (e) the transverse momentum of the leading jet, (f) the transverse momentum of the secondary jet, (g) the $H_T$, and (h) the difference between the two lepton pseudorapidities. The overflow bin content has been added to the last bin.
002036481 8564_ $$82215803$$s29316$$uhttp://cds.cern.ch/record/2036481/files/h_1.png$$y00006 [color online] Comparison of distributions between data and MC simulations at the final selection for (a) the transverse momentum of the leading lepton, (b) the transverse momentum of the secondary lepton, (c) the pseudorapidity of the leading lepton, (d) the pseudorapidity of the secondary lepton, (e) the transverse momentum of the leading jet, (f) the transverse momentum of the secondary jet, (g) the $H_T$, and (h) the difference between the two lepton pseudorapidities. The overflow bin content has been added to the last bin.
002036481 8564_ $$82215804$$s22800$$uhttp://cds.cern.ch/record/2036481/files/hsub_h_rec_costheta2_beam.png$$y00013 [color online] Estimated distribution of the (a) \dyttbar, (b) $\cos\theta^+$, and (c) $\cos\theta^-$ observables in dilepton events after subtracting the expected background contribution. Deviations beweeen the background-subtracted data and MC can be attributed to statistical fluctuations. The background-subtracted data asymmetries and the MC asymmetries extracted from these distributions are also reported. These raw asymmetries need to be corrected for calibration effects to retrieve the parton-level asymmetries.
002036481 8564_ $$82215805$$s47374$$uhttp://cds.cern.ch/record/2036481/files/DY_tanh+cubic_asym.png$$y00014 [color online] Differential asymmetry ${\cal A}(\dyttbar)$ at parton level for different MC samples. See Ref.~\cite{Carmona:2014gra} for the details on axigluon models. The observed $ {\cal A}(\dyttbar)$ is fitted with the functional form of Eq.~(\ref{eq:tanh+cubic}).
002036481 8564_ $$82215807$$s24083$$uhttp://cds.cern.ch/record/2036481/files/costheta1.png$$y00009 [color online] Accumulation of likelihood functions ($\sum_{\text{events}} L_{z_i}(K)$, with $K$ along the vertical axis) versus the corresponding true parton level quantity ($K_{\mathrm{true}}$ along the horizontal axis) in \ttbar\ MC events after applying the selection criteria for (a) $K=\dyttbar$, (b) $K=\cos\theta^+$, and (c) $K=\cos\theta^-$. Each single MC event $i$ contributes in these plots with a complete distribution, $L_{z_i}(X)$, along the vertical axis for a given value on the horizontal axis, $K_{\mathrm{true}}$. The shades of color indicate the bin contents in arbitrary units.
002036481 8564_ $$82215808$$s24247$$uhttp://cds.cern.ch/record/2036481/files/costheta2.png$$y00010 [color online] Accumulation of likelihood functions ($\sum_{\text{events}} L_{z_i}(K)$, with $K$ along the vertical axis) versus the corresponding true parton level quantity ($K_{\mathrm{true}}$ along the horizontal axis) in \ttbar\ MC events after applying the selection criteria for (a) $K=\dyttbar$, (b) $K=\cos\theta^+$, and (c) $K=\cos\theta^-$. Each single MC event $i$ contributes in these plots with a complete distribution, $L_{z_i}(X)$, along the vertical axis for a given value on the horizontal axis, $K_{\mathrm{true}}$. The shades of color indicate the bin contents in arbitrary units.
002036481 8564_ $$82215809$$s32896$$uhttp://cds.cern.ch/record/2036481/files/dy.png$$y00008 [color online] Accumulation of likelihood functions ($\sum_{\text{events}} L_{z_i}(K)$, with $K$ along the vertical axis) versus the corresponding true parton level quantity ($K_{\mathrm{true}}$ along the horizontal axis) in \ttbar\ MC events after applying the selection criteria for (a) $K=\dyttbar$, (b) $K=\cos\theta^+$, and (c) $K=\cos\theta^-$. Each single MC event $i$ contributes in these plots with a complete distribution, $L_{z_i}(X)$, along the vertical axis for a given value on the horizontal axis, $K_{\mathrm{true}}$. The shades of color indicate the bin contents in arbitrary units.
002036481 8564_ $$82215810$$s21378$$uhttp://cds.cern.ch/record/2036481/files/hsub_h_recdy.png$$y00011 [color online] Estimated distribution of the (a) \dyttbar, (b) $\cos\theta^+$, and (c) $\cos\theta^-$ observables in dilepton events after subtracting the expected background contribution. Deviations beweeen the background-subtracted data and MC can be attributed to statistical fluctuations. The background-subtracted data asymmetries and the MC asymmetries extracted from these distributions are also reported. These raw asymmetries need to be corrected for calibration effects to retrieve the parton-level asymmetries.
002036481 8564_ $$82215811$$s23152$$uhttp://cds.cern.ch/record/2036481/files/hsub_h_rec_costheta1_beam.png$$y00012 [color online] Estimated distribution of the (a) \dyttbar, (b) $\cos\theta^+$, and (c) $\cos\theta^-$ observables in dilepton events after subtracting the expected background contribution. Deviations beweeen the background-subtracted data and MC can be attributed to statistical fluctuations. The background-subtracted data asymmetries and the MC asymmetries extracted from these distributions are also reported. These raw asymmetries need to be corrected for calibration effects to retrieve the parton-level asymmetries.
002036481 8564_ $$82215812$$s27242$$uhttp://cds.cern.ch/record/2036481/files/h_15.png$$y00007 [color online] Comparison of distributions between data and MC simulations at the final selection for (a) the transverse momentum of the leading lepton, (b) the transverse momentum of the secondary lepton, (c) the pseudorapidity of the leading lepton, (d) the pseudorapidity of the secondary lepton, (e) the transverse momentum of the leading jet, (f) the transverse momentum of the secondary jet, (g) the $H_T$, and (h) the difference between the two lepton pseudorapidities. The overflow bin content has been added to the last bin.
002036481 8564_ $$82215813$$s38573$$uhttp://cds.cern.ch/record/2036481/files/afb_polar_measurement_statsyst_bsm.png$$y00015 [color online] Two dimensional visualization of the \Att\ and \Ptt\ measurements and comparison with benchmark axigluon models~\cite{Carmona:2014gra}.
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