000060232 001__ 60232
000060232 005__ 20140130012425.0
000060232 035__ $$9arXiv$$aoai:arXiv.org:1301.2233$$zoai:arXiv.org:1301.2233
000060232 035__ $$9SPIRESTeX$$z:2013wz
000060232 037__ $$9arXiv$$aarXiv:1301.2233$$chep-ex
000060232 037__ $$aFERMILAB-PUB-13-011-E
000060232 100__ $$aAbazov, Victor Mukhamedovich$$iINSPIRE-00039200$$uDubna, JINR
000060232 245__ $$aMeasurement of the ratio of differential cross sections ${\sigma}(p\bar{p} \to Z + b jet)/{\sigma}(p\bar{p} \to Z + jet)$ in $p\bar{p}$ collisions at $\sqrt(s)=1.96$ TeV
000060232 246__ $$9arXiv$$aMeasurement of the ratio of differential cross sections {\sigma}(ppbar -> Z + b jet)/{\sigma}(ppbar -> Z + jet) in ppbar collisions at sqrt(s)=1.96 TeV
000060232 269__ $$c2013-01
000060232 500__ $$9arXiv$$asubmitted to Phys. Rev. D Rapid Communications
000060232 520__ $$9arXiv$$aWe measure the ratio of cross sections, {\sigma}(ppbar -> Z + b jet)/{\sigma}(ppbar -> Z + jet), for associated production of a Z boson with at least one jet. The ratio is also measured as a function of the jet transverse momentum, jet pseudorapidity, Z boson transverse momentum, and the azimuthal angle between the Z boson and the closest jet for events with at least one b jet. These measurements use data collected by the D0 experiment in Run II of Fermilab's Tevatron ppbar Collider at a center-of-mass energy of 1.96 TeV, and correspond to an integrated luminosity of 9.7 fb$^{-1}$. The results are compared to predictions from next-to-leading order calculations and various Monte Carlo event generators.
000060232 540__ $$ahttp://arxiv.org/licenses/nonexclusive-distrib/1.0/$$barXiv
000060232 65017 $$2INSPIRE$$aExperiment-HEP
000060232 6507_ $$2PACS$$a12.38.Qk
000060232 6507_ $$2PACS$$a13.85.Qk
000060232 6507_ $$2PACS$$a14.65.Fy
000060232 6507_ $$2PACS$$a14.70.Hp
000060232 693__ $$eFNAL-E-0823
000060232 693__ $$eFNAL-TEV-D0
000060232 695__ $$2INSPIRE$$a* Automatic Keywords *
000060232 695__ $$2INSPIRE$$ajet: bottom
000060232 695__ $$2INSPIRE$$ajet: transverse momentum
000060232 695__ $$2INSPIRE$$ajet: rapidity
000060232 695__ $$2INSPIRE$$adifferential cross section: ratio
000060232 695__ $$2INSPIRE$$aZ0: associated production
000060232 695__ $$2INSPIRE$$aZ0: transverse momentum
000060232 695__ $$2INSPIRE$$across section: ratio
000060232 695__ $$2INSPIRE$$ahigher-order: 1
000060232 695__ $$2INSPIRE$$ameasure: ratio
000060232 695__ $$2INSPIRE$$aMonte Carlo
000060232 695__ $$2INSPIRE$$aBatavia TEVATRON Coll
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000060232 700__ $$aBuszello, Claus Peter$$iINSPIRE-00044211$$uUppsala U.
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000060232 700__ $$aChapon, Emilien$$iINSPIRE-00015039$$uDAPNIA, Saclay
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000060232 700__ $$aCho, Sung-Woong$$iINSPIRE-00302582$$uKorea U., KODEL
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000060232 700__ $$aChoudhary, Brajesh C$$iINSPIRE-00073233$$uDelhi U.
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000060232 700__ $$aDubey, Abhinav Kumar$$iINSPIRE-00300331$$uDelhi U.
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000060232 700__ $$aEdmunds, Daniel L$$iINSPIRE-00004510$$uMichigan State U.
000060232 700__ $$aEllison, John A$$iINSPIRE-00079386$$uUC, Riverside
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000060232 700__ $$aEvdokimov, Valeri N$$iINSPIRE-00300342$$uSerpukhov, IHEP
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000060232 700__ $$aGarcia-Gonzalez, Jose Andres$$iINSPIRE-00201259$$uCINVESTAV, IPN
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000060232 700__ $$aHan, Liang$$iINSPIRE-00037384$$uHefei, CUST
000060232 700__ $$aHarder, Kristian$$iINSPIRE-00088612$$uManchester U., Comp. Sci. Dept.
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000060232 700__ $$aHeintz, Ulrich$$iINSPIRE-00089547$$uBrown U.
000060232 700__ $$aHensel, Carsten$$iINSPIRE-00046890$$uGottingen U., Zweites Phys. Inst.
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000060232 700__ $$aHoeneisen, Bruce$$iINSPIRE-00090561$$uSan Francisco de Quito U.
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000060232 700__ $$aJiang, Peng$$iINSPIRE-00233577$$uHefei, CUST
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000060232 700__ $$aJohnson, Emily$$iINSPIRE-00347646$$uMichigan State U.
000060232 700__ $$aJohnson, Marvin E$$iINSPIRE-00093653$$uFermilab
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000060232 700__ $$aKharzheev, Yuri N$$iINSPIRE-00000177$$uDubna, JINR
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000060232 700__ $$aKuzmin, Valentin Alexandrovich$$iINSPIRE-00046985$$uMoscow State U.
000060232 700__ $$aLammers, Sabine Wedam$$iINSPIRE-00051670$$uIndiana U.
000060232 700__ $$aLandsberg, Greg L$$iINSPIRE-00099870$$uBrown U.
000060232 700__ $$aLebrun, Patrice$$iINSPIRE-00100449$$uLyon, IPN, France
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000060232 700__ $$aLee, William M$$iINSPIRE-00100793$$uFlorida State U.
000060232 700__ $$aLei, Xiaowen$$iINSPIRE-00219018$$uArizona U.
000060232 700__ $$aLellouch, Jeremie$$iINSPIRE-00024906$$uParis U., VI-VII
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000060232 700__ $$aLi, Liang$$iINSPIRE-00300470$$uUC, Riverside
000060232 700__ $$aLi, Qi-Zhong$$iINSPIRE-00101541$$uFermilab
000060232 700__ $$aLim, Jeong Ku$$iINSPIRE-00011894$$uKorea U., KODEL
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000060232 700__ $$aLinnemann, James Thomas$$iINSPIRE-00300481$$uMichigan State U.
000060232 700__ $$aLipaev, Vladimir V$$iINSPIRE-00038891$$uSerpukhov, IHEP
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000060232 700__ $$aLiu, Huanzhao$$iINSPIRE-00348078$$uSouthern Methodist U.
000060232 700__ $$aLiu, Yanwen$$iINSPIRE-00034400$$uHefei, CUST
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000060232 700__ $$aMelnitchouk, Alexander S$$iINSPIRE-00054552$$uFermilab
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000060232 700__ $$aMercadante, Pedro Galli$$iINSPIRE-00106948$$uABC Federal U.
000060232 700__ $$aMerkin, Mikhail M$$iINSPIRE-00055966$$uMoscow State U.
000060232 700__ $$aMeyer, Arnd$$iINSPIRE-00300593$$uAachen, Tech. Hochsch.
000060232 700__ $$aMeyer, Jorg Manfred$$iINSPIRE-00107296$$uGottingen U., Zweites Phys. Inst.
000060232 700__ $$aMiconi, Florian$$iINSPIRE-00180384$$uLouis Pasteur U., Strasbourg I
000060232 700__ $$aMondal, Naba K$$iINSPIRE-00300508$$uTata Inst.
000060232 700__ $$aMulhearn, Michael James$$iINSPIRE-00052395$$uVirginia U.
000060232 700__ $$aNagy, Elemer$$iINSPIRE-00110088$$uMarseille, CPPM
000060232 700__ $$aNaimuddin, Md (Nayeem)$$iINSPIRE-00038820$$uDelhi U.
000060232 700__ $$aNarain, Meenakshi$$iINSPIRE-00110455$$uBrown U.
000060232 700__ $$aNayyar, Ruchika$$iINSPIRE-00301151$$uArizona U.
000060232 700__ $$aNeal, Homer A$$iINSPIRE-00300519$$uMichigan U.
000060232 700__ $$aNegret, Juan Pablo$$iINSPIRE-00110764$$uAndes U., Bogota
000060232 700__ $$aNeustroev, Petr V$$iINSPIRE-00021941$$uSt. Petersburg, INP
000060232 700__ $$aNguyen, Huong Thi$$iINSPIRE-00265368$$uVirginia U.
000060232 700__ $$aNunnemann, Thomas P$$iINSPIRE-00046334$$uMunich U.
000060232 700__ $$aOrduna, Jose de Jesus Hernandez$$iINSPIRE-00010914$$uRice U.
000060232 700__ $$aOsman, Nicolas Ahmed$$iINSPIRE-00011554$$uMarseille, CPPM
000060232 700__ $$aOsta, Jyotsna$$iINSPIRE-00047228$$uNotre Dame U.
000060232 700__ $$aPadilla, Mark Anthony$$iINSPIRE-00010519$$uUC, Riverside
000060232 700__ $$aPal, Arnab$$iINSPIRE-00271611$$uTexas U., Arlington
000060232 700__ $$aParashar, Neeti$$iINSPIRE-00038772$$uPurdue U., Calumet
000060232 700__ $$aParihar, Vivek$$iINSPIRE-00011106$$uBrown U.
000060232 700__ $$aPark, Sung Keun$$iINSPIRE-00114681$$uKorea U., KODEL
000060232 700__ $$aPartridge, Richard A$$iINSPIRE-00114805$$uSLAC$$uBrown U.
000060232 700__ $$aParua, Nirmalya$$iINSPIRE-00114817$$uIndiana U.
000060232 700__ $$aPatwa, Abid$$iINSPIRE-00115127$$uBrookhaven
000060232 700__ $$aPenning, Bjoern$$iINSPIRE-00007584$$uFermilab
000060232 700__ $$aPerfilov, Maxim Anatolyevich$$iINSPIRE-00036598$$uMoscow State U.
000060232 700__ $$aPeters, Reinhild Yvonne Fatima$$iINSPIRE-00008252$$uGottingen U., Zweites Phys. Inst.
000060232 700__ $$aPetridis, Konstantinos$$iINSPIRE-00311357$$uManchester U., Comp. Sci. Dept.
000060232 700__ $$aPetrillo, Gianluca$$iINSPIRE-00019289$$uRochester U.
000060232 700__ $$aPetroff, Pierre$$iINSPIRE-00116049$$uOrsay, LAL
000060232 700__ $$aPleier, Marc-Andre$$iINSPIRE-00046720$$uBrookhaven
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000060232 700__ $$aPopov, Alexey V$$iINSPIRE-00038751$$uSerpukhov, IHEP
000060232 700__ $$aPrewitt, Michelle$$iINSPIRE-00019110$$uRice U.
000060232 700__ $$aPrice, Darren$$iINSPIRE-00027472$$uIndiana U.
000060232 700__ $$aProkopenko, Nikolay N$$iINSPIRE-00036409$$uSerpukhov, IHEP
000060232 700__ $$aQian, Jianming$$iINSPIRE-00118167$$uMichigan U.
000060232 700__ $$aQuadt, Arnulf$$iINSPIRE-00118216$$uGottingen U., Zweites Phys. Inst.
000060232 700__ $$aQuinn, Brian P$$iINSPIRE-00118288$$uMississippi U.
000060232 700__ $$aRangel, Murilo Santana$$iINSPIRE-00024740$$uRio de Janeiro, CBPF
000060232 700__ $$aRanjan, Kirti$$iINSPIRE-00038731$$uDelhi U.
000060232 700__ $$aRatoff, Peter N$$iINSPIRE-00119089$$uLancaster U.
000060232 700__ $$aRazumov, Ivan A$$iINSPIRE-00012786$$uSerpukhov, IHEP
000060232 700__ $$aRenkel, Peter$$iINSPIRE-00008215$$uSouthern Methodist U.
000060232 700__ $$aRipp-Baudot, Isabelle$$iINSPIRE-00038728$$uLouis Pasteur U., Strasbourg I
000060232 700__ $$aRizatdinova, Flera$$iINSPIRE-00048668$$uOklahoma State U.
000060232 700__ $$aRominsky, Mandy Kathleen$$iINSPIRE-00007250$$uFermilab
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000060232 700__ $$aRoyon, Christophe$$iINSPIRE-00121542$$uDAPNIA, Saclay
000060232 700__ $$aRubinov, Paul Michael$$iINSPIRE-00121638$$uFermilab
000060232 700__ $$aRuchti, Randal C$$iINSPIRE-00121660$$uNotre Dame U.
000060232 700__ $$aSajot, Gerard$$iINSPIRE-00122471$$uLPSC, Grenoble
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000060232 700__ $$aSanchez-Hernandez, Alberto$$iINSPIRE-00122966$$uCINVESTAV, IPN
000060232 700__ $$aSanders, Michiel P$$iINSPIRE-00038712$$uMunich U.
000060232 700__ $$aSantos, Angelo Souza$$iINSPIRE-00301078$$uSao Paulo, IFT$$uRio de Janeiro, CBPF
000060232 700__ $$aSavage, David G$$iINSPIRE-00002100$$uFermilab
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000060232 700__ $$aScheglov, Yury A$$iINSPIRE-00005552$$uSt. Petersburg, INP
000060232 700__ $$aSchellman, Heidi M$$iINSPIRE-00123914$$uNorthwestern U.
000060232 700__ $$aSchwanenberger, Christian$$iINSPIRE-00124643$$uManchester U., Comp. Sci. Dept.
000060232 700__ $$aSchwienhorst, Reinhard H$$iINSPIRE-00050408$$uMichigan State U.
000060232 700__ $$aSekaric, Jadranka$$iINSPIRE-00045058$$uKansas U.
000060232 700__ $$aSeverini, Horst$$iINSPIRE-00125370$$uOklahoma U.
000060232 700__ $$aShabalina, Elizaveta K$$iINSPIRE-00038690$$uGottingen U., Zweites Phys. Inst.
000060232 700__ $$aShary, Viacheslav V$$iINSPIRE-00006382$$uDAPNIA, Saclay
000060232 700__ $$aShaw, Savanna$$iINSPIRE-00347635$$uMichigan State U.
000060232 700__ $$aShchukin, Andrey A$$iINSPIRE-00038677$$uSerpukhov, IHEP
000060232 700__ $$aShivpuri, Ram K$$iINSPIRE-00126040$$uDelhi U.
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000060232 700__ $$aSoldner-Rembold, Stefan$$iINSPIRE-00127655$$uManchester U., Comp. Sci. Dept.
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000060232 700__ $$aVarelas, Nikos$$iINSPIRE-00133485$$uIllinois U., Chicago
000060232 700__ $$aVarnes, Erich W$$iINSPIRE-00133542$$uArizona U.
000060232 700__ $$aVasilyev, Igor A$$iINSPIRE-00038583$$uSerpukhov, IHEP
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000060232 700__ $$aWatts, Gordon Thomas$$iINSPIRE-00135120$$uWashington U., Seattle
000060232 700__ $$aWayne, Mitchell R$$iINSPIRE-00135150$$uNotre Dame U.
000060232 700__ $$aWeichert, Jonas$$iINSPIRE-00328486$$uMainz U., Inst. Phys.
000060232 700__ $$aWelty-Rieger, Leah Christine$$iINSPIRE-00018450$$uNorthwestern U.
000060232 700__ $$aWhite, Andrew P$$iINSPIRE-00013505$$uTexas U., Arlington
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000060232 700__ $$aWyatt, Terence R$$iINSPIRE-00136898$$uManchester U., Comp. Sci. Dept.
000060232 700__ $$aXie, Yunhe$$iINSPIRE-00007769$$uFermilab
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000060232 700__ $$aYe, Zhenyu$$iINSPIRE-00054712$$uFermilab
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000060232 700__ $$aZennamo, Joseph$$iINSPIRE-00192060$$uSUNY, Buffalo
000060232 700__ $$aZhao, Tianqi Gilbert$$iINSPIRE-00219365$$uManchester U., Comp. Sci. Dept.
000060232 700__ $$aZhou, Bing$$iINSPIRE-00138410$$uMichigan U.
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000060232 700__ $$aZieminska, Daria$$iINSPIRE-00138550$$uIndiana U.
000060232 700__ $$aZivkovic, Lidija$$iINSPIRE-00057284$$uParis U., VI-VII
000060232 710__ $$gD0 Collaboration
000060232 8564_ $$uhttp://www.fnal.gov/pub/today/archive_2013/today13-01-17.html$$warchive_2013/today13-01-17.html$$yFERMILABTODAY
000060232 8564_ $$uhttp://inspirehep.net/record/1210034/files/arXiv:1301.2233.pdf
000060232 8564_ $$uhttp://inspirehep.net/record/1210034/files/Fig1a.png$$y00000 (color online) The leading jet $p_{T}$ in the (a) $Z\rightarrow ee$ and (b) $Z\rightarrow \mu\mu$ channels for data and background in events with a $Z$ boson candidate and at least one jet before $b$ tagging is applied.
000060232 8564_ $$uhttp://inspirehep.net/record/1210034/files/Fig1b.png$$y00001 (color online) The leading jet $p_{T}$ in the (a) $Z\rightarrow ee$ and (b) $Z\rightarrow \mu\mu$ channels for data and background in events with a $Z$ boson candidate and at least one jet before $b$ tagging is applied.
000060232 8564_ $$uhttp://inspirehep.net/record/1210034/files/Fig2a.png$$y00002 (color online) (a) The probability densities of the \mjl discriminant for $b$, $c$, and light jets passing the $b$ tagging requirements, normalized to unity. These templates are taken from MC simulations. Also shown is the distribution for the negatively tagged (NT) jets in data. (b) The \mjl discriminant distribution of events in the combined sample. The distributions of the $b$, $c$, and light jets are normalized by the fractions found from the fit.
000060232 8564_ $$uhttp://inspirehep.net/record/1210034/files/Fig2b.png$$y00003 (color online) (a) The probability densities of the \mjl discriminant for $b$, $c$, and light jets passing the $b$ tagging requirements, normalized to unity. These templates are taken from MC simulations. Also shown is the distribution for the negatively tagged (NT) jets in data. (b) The \mjl discriminant distribution of events in the combined sample. The distributions of the $b$, $c$, and light jets are normalized by the fractions found from the fit.
000060232 8564_ $$uhttp://inspirehep.net/record/1210034/files/Fig3a.png$$y00005 (color online) Ratios of the differential cross sections. The uncertainties on the data include statistical (inner error bar) and full uncertainties (entire error bar). The data are compared to the prediction from {\sc alpgen}, \sherpae, and the \mcfm NLO calculation, where the band represents the variation of the renormalization and factorization scales up and down by a factor of two. Bin centers are chosen using the prescription found in Ref.~\cite{Terry}.
000060232 8564_ $$uhttp://inspirehep.net/record/1210034/files/Fig3b.png$$y00006 (color online) Ratios of the differential cross sections. The uncertainties on the data include statistical (inner error bar) and full uncertainties (entire error bar). The data are compared to the prediction from {\sc alpgen}, \sherpae, and the \mcfm NLO calculation, where the band represents the variation of the renormalization and factorization scales up and down by a factor of two. Bin centers are chosen using the prescription found in Ref.~\cite{Terry}.
000060232 8564_ $$uhttp://inspirehep.net/record/1210034/files/Fig3c.png$$y00007 (color online) Ratios of the differential cross sections. The uncertainties on the data include statistical (inner error bar) and full uncertainties (entire error bar). The data are compared to the prediction from {\sc alpgen}, \sherpae, and the \mcfm NLO calculation, where the band represents the variation of the renormalization and factorization scales up and down by a factor of two. Bin centers are chosen using the prescription found in Ref.~\cite{Terry}.
000060232 8564_ $$uhttp://inspirehep.net/record/1210034/files/Fig3d.png$$y00008 (color online) Ratios of the differential cross sections. The uncertainties on the data include statistical (inner error bar) and full uncertainties (entire error bar). The data are compared to the prediction from {\sc alpgen}, \sherpae, and the \mcfm NLO calculation, where the band represents the variation of the renormalization and factorization scales up and down by a factor of two. Bin centers are chosen using the prescription found in Ref.~\cite{Terry}.
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000060232 961__ $$x2013-01-10
000060232 961__ $$c2013-01-17
000060232 970__ $$aSPIRES-9912240
000060232 980__ $$aarXiv
000060232 980__ $$aCiteable
000060232 980__ $$aCORE
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