CERN Accelerating science

001624473 001__ 1624473
001624473 003__ SzGeCERN
001624473 005__ 20211118050721.0
001624473 0247_ $$2DOI$$a10.1103/PhysRevD.89.072003
001624473 0248_ $$aoai:cds.cern.ch:1624473$$pcerncds:FULLTEXT$$pcerncds:CERN:FULLTEXT$$pcerncds:CERN
001624473 035__ $$9arXiv$$aoai:arXiv.org:1311.0894
001624473 035__ $$9Inspire$$a1263361
001624473 037__ $$9arXiv$$aarXiv:1311.0894$$chep-ex
001624473 037__ $$aFERMILAB-PUB-13-515-E
001624473 041__ $$aeng
001624473 084__ $$2PACS$$a12.15.Ji
001624473 084__ $$2PACS$$a13.38.Be
001624473 084__ $$2PACS$$a13.85.Qk
001624473 084__ $$2PACS$$a14.70.Fm
001624473 100__ $$aAaltonen, Timo Antero$$iINSPIRE-00010138$$uHelsinki U.$$uHelsinki Inst. of Phys.
001624473 245__ $$aA precise measurement of the $W$-boson mass with the Collider Detector at Fermilab
001624473 260__ $$c2014-04-03
001624473 269__ $$c04 Nov 2013
001624473 300__ $$a40 p
001624473 500__ $$aComments: Submitted to Phys. Rev. D
001624473 500__ $$9arXiv$$aSubmitted to Phys. Rev. D
001624473 520__ $$aWe present a measurement of the $W$-boson mass, $M_W$, using data corresponding to 2.2/fb of integrated luminosity collected in ppbar collisions at $\sqrt{s}$ = 1.96 TeV with the CDF II detector at the Fermilab Tevatron. The selected sample of 470126 $W\to e\nu$ candidates and 624708 $W\to\mu\nu$ candidates yields the measurement $M_W = 80387\pm 12$ (stat) $\pm 15$ (syst)$ = 80387 \pm 19$ MeV$/c^2$ . This is the most precise single measurement of the $W$-boson mass to date.
001624473 520__ $$9APS$$a<p>We present a measurement of the <inline-formula><mml:math display="inline"><mml:mi>W</mml:mi></mml:math></inline-formula>-boson mass, <inline-formula><mml:math display="inline"><mml:msub><mml:mi>M</mml:mi><mml:mi>W</mml:mi></mml:msub></mml:math></inline-formula>, using data corresponding to <inline-formula><mml:math display="inline"><mml:mrow><mml:mn>2.2</mml:mn><mml:mtext> </mml:mtext><mml:mtext> </mml:mtext><mml:msup><mml:mrow><mml:mi>fb</mml:mi></mml:mrow><mml:mrow><mml:mo>−</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> of integrated luminosity collected in <inline-formula><mml:math display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mover accent="true"><mml:mrow><mml:mi>p</mml:mi></mml:mrow><mml:mrow><mml:mo accent="true" stretchy="false">¯</mml:mo></mml:mrow></mml:mover></mml:mrow></mml:math></inline-formula> collisions at <inline-formula><mml:math display="inline"><mml:mrow><mml:msqrt><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msqrt><mml:mo>=</mml:mo><mml:mn>1.96</mml:mn><mml:mtext> </mml:mtext><mml:mtext> </mml:mtext><mml:mi>TeV</mml:mi></mml:mrow></mml:math></inline-formula> with the CDF II detector at the Fermilab Tevatron. The selected sample of 470 126 <inline-formula><mml:math display="inline"><mml:mi>W</mml:mi><mml:mo stretchy="false">→</mml:mo><mml:mi>e</mml:mi><mml:mi>ν</mml:mi></mml:math></inline-formula> candidates and 624 708 <inline-formula><mml:math display="inline"><mml:mi>W</mml:mi><mml:mo stretchy="false">→</mml:mo><mml:mi>μ</mml:mi><mml:mi>ν</mml:mi></mml:math></inline-formula> candidates yields the measurement <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi>M</mml:mi></mml:mrow><mml:mrow><mml:mi>W</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mn>80</mml:mn><mml:mn>387</mml:mn><mml:mo>±</mml:mo><mml:mn>12</mml:mn><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mtext>stat</mml:mtext><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mo>±</mml:mo><mml:mn>15</mml:mn><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mtext>syst</mml:mtext><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:mn>80</mml:mn><mml:mn>387</mml:mn><mml:mo>±</mml:mo><mml:mn>19</mml:mn><mml:mtext> </mml:mtext><mml:mtext> </mml:mtext><mml:mi>MeV</mml:mi><mml:mo>/</mml:mo><mml:msup><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. This is the most precise single measurement of the <inline-formula><mml:math display="inline"><mml:mi>W</mml:mi></mml:math></inline-formula>-boson mass to date.</p>
001624473 520__ $$9arXiv$$aWe present a measurement of the $W$-boson mass, $M_W$, using data corresponding to 2.2/fb of integrated luminosity collected in ppbar collisions at $\sqrt{s}$ = 1.96 TeV with the CDF II detector at the Fermilab Tevatron. The selected sample of 470126 $W\to e\nu$ candidates and 624708 $W\to\mu\nu$ candidates yields the measurement $M_W = 80387\pm 12$ (stat) $\pm 15$ (syst)$ = 80387 \pm 19$ MeV$/c^2$ . This is the most precise single measurement of the $W$-boson mass to date.
001624473 540__ $$aarXiv nonexclusive-distrib. 1.0$$barXiv$$uhttp://arxiv.org/licenses/nonexclusive-distrib/1.0/
001624473 542__ $$3Publication$$dAmerican Physical Society$$g2014
001624473 595__ $$aINSPIRE-PUBL-2014
001624473 65017 $$2arXiv$$aParticle Physics - Experiment
001624473 690C_ $$aARTICLE
001624473 690C_ $$aCERN
001624473 695__ $$9LANL EDS$$ahep-ex
001624473 700__ $$aAmerio, Silvia$$iINSPIRE-00041447$$uPadua U.$$uINFN, Padua
001624473 700__ $$aAmidei, Dante E$$iINSPIRE-00061910$$uMichigan U.
001624473 700__ $$aAnastassov, Anton Iankov$$iINSPIRE-00062009$$uNorthwestern U.$$uFermilab
001624473 700__ $$aAnnovi, Alberto$$iINSPIRE-00041435$$uFrascati
001624473 700__ $$aAntos, Jaroslav$$iINSPIRE-00062457$$uKosice, IEF$$uComenius U.
001624473 700__ $$aApollinari, Giorgio$$iINSPIRE-00062568$$uFermilab
001624473 700__ $$aAppel, Jeffrey A$$iINSPIRE-00062597$$uFermilab
001624473 700__ $$aArisawa, Tetsuo$$iINSPIRE-00062831$$uWaseda U.
001624473 700__ $$aArtikov, Akram Muzafarovich$$iINSPIRE-00005411$$uDubna, JINR
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001624473 700__ $$aBarbaro-Galtieri, Angela$$iINSPIRE-00064338$$uLBL, Berkeley
001624473 700__ $$aBarnes, Virgil E$$iINSPIRE-00064657$$uPurdue U.
001624473 700__ $$aBarnett, Bruce Arnold$$iINSPIRE-00064664$$uJohns Hopkins U.
001624473 700__ $$aBarreiro Guimaraes da Costa, Joao$$iINSPIRE-00087323$$uHarvard U.
001624473 700__ $$aBarria, Patrizia$$iINSPIRE-00014503$$uINFN, Pisa$$uSiena U.
001624473 700__ $$aBartos, Pavol$$iINSPIRE-00304670$$uKosice, IEF$$uComenius U.
001624473 700__ $$aBauce, Matteo$$iINSPIRE-00243631$$uINFN, Padua$$uPadua U.
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001624473 700__ $$aBoveia, Antonio$$iINSPIRE-00041392$$uChicago U., EFI
001624473 700__ $$aBrigliadori, Luca$$iINSPIRE-00069240$$uINFN, Bologna$$uBologna U.
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001624473 700__ $$aBrucken, Erik$$iINSPIRE-00019412$$uHelsinki Inst. of Phys.$$uHelsinki U.
001624473 700__ $$aBudagov, Ioulian A$$iINSPIRE-00211819$$uDubna, JINR
001624473 700__ $$aBudd, Howard Scott$$iINSPIRE-00069880$$uRochester U.
001624473 700__ $$aBurkett, Kevin Alan$$iINSPIRE-00070158$$uFermilab
001624473 700__ $$aBusetto, Giovanni$$iINSPIRE-00070232$$uINFN, Padua$$uPadua U.
001624473 700__ $$aBussey, Peter John$$iINSPIRE-00070265$$uGlasgow U.
001624473 700__ $$aButti, Pierfrancesco$$iINSPIRE-00358725$$uINFN, Pisa$$uPisa U.
001624473 700__ $$aBuzatu, Adrian$$iINSPIRE-00025104$$uGlasgow U.
001624473 700__ $$aCalamba, Aristotle$$iINSPIRE-00218130$$uCarnegie Mellon U.
001624473 700__ $$aCamarda, Stefano$$iINSPIRE-00012655$$uBarcelona, IFAE
001624473 700__ $$aCampanelli, Mario$$iINSPIRE-00070797$$uUniversity Coll. London
001624473 700__ $$aCanelli, Florencia$$iINSPIRE-00070860$$uChicago U., EFI$$uZurich U.
001624473 700__ $$aCarls, Benjamin$$iINSPIRE-00010558$$uIllinois U., Urbana
001624473 700__ $$aCarlsmith, Duncan L$$iINSPIRE-00071156$$uWisconsin U., Madison
001624473 700__ $$aCarosi, Roberto$$iINSPIRE-00071241$$uINFN, Pisa
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001624473 700__ $$aCasal Larana, Bruno$$iINSPIRE-00047672$$uCantabria Inst. of Phys.$$uZurich, ETH
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001624473 700__ $$aCatastini, Pierluigi$$iINSPIRE-00041380$$uHarvard U.
001624473 700__ $$aCauz, Diego$$iINSPIRE-00071702$$uUdine U.$$uINFN, Udine$$uINFN, Trieste
001624473 700__ $$aCavaliere, Viviana$$iINSPIRE-00010976$$uIllinois U., Urbana
001624473 700__ $$aCavalli-Sforza, Matteo$$iINSPIRE-00071735$$uBarcelona, IFAE
001624473 700__ $$aCerri, Alessandro$$iINSPIRE-00050967$$uLBL, Berkeley$$uCERN
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001624473 700__ $$aChen, Yen-Chu$$iINSPIRE-00004797$$uTaiwan, Inst. Phys.
001624473 700__ $$aChertok, Maxwell Benjamin$$iINSPIRE-00072789$$uUC, Davis
001624473 700__ $$aChiarelli, Giorgio$$iINSPIRE-00072892$$uINFN, Pisa
001624473 700__ $$aChlachidze, Gouram$$iINSPIRE-00073077$$uFermilab
001624473 700__ $$aCho, Kihyeon$$iINSPIRE-00073118$$uEwha Women's U., Seoul$$uChonbuk Natl. U.$$uChonnam Natl. U.$$uKISTI, Daejeon$$uSungkyunkwan U.$$uSeoul Natl. U.$$uKyungpook Natl. U.
001624473 700__ $$aChokheli, Davit$$iINSPIRE-00041379$$uDubna, JINR
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001624473 700__ $$aConvery, Mary Elizabeth$$iINSPIRE-00074310$$uFermilab
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001624473 700__ $$aCorbo, Matteo$$iINSPIRE-00307043$$uFermilab$$uParis U., VI-VII
001624473 700__ $$aCordelli, Marco$$iINSPIRE-00300023$$uFrascati
001624473 700__ $$aCox, Charles Alexander$$iINSPIRE-00011805$$uUC, Davis
001624473 700__ $$aCox, David Jeremy$$iINSPIRE-00010140$$uUC, Davis
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001624473 700__ $$aCruz Alonso, Daniel$$iINSPIRE-00265472$$uTexas A-M
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001624473 700__ $$aCulbertson, Raymond Lloyd$$iINSPIRE-00075235$$uFermilab
001624473 700__ $$aD'Ascenzo, Nicola$$iINSPIRE-00327173$$uFermilab$$uMoscow Phys. Eng. Inst.
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001624473 700__ $$aDi Ruzza, Benedetto$$iINSPIRE-00030649$$uFermilab$$uBrookhaven
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001624473 700__ $$aGerchtein, Elena A$$iINSPIRE-00243680$$uFermilab
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001624473 700__ $$aGold, Michael S$$iINSPIRE-00085380$$uNew Mexico U.
001624473 700__ $$aGoldin, Daniel$$iINSPIRE-00243695$$uTexas A-M
001624473 700__ $$aGolossanov, Alexander$$iINSPIRE-00085656$$uFermilab
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001624473 700__ $$aGomez-Ceballos, Guillelmo$$iINSPIRE-00041199$$uMIT
001624473 700__ $$aGoncharov, Maxim T$$iINSPIRE-00085771$$uMIT
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001624473 700__ $$aGrosso-Pilcher, Carla$$iINSPIRE-00087060$$uChicago U., EFI
001624473 700__ $$aGroup, Robert Craig$$iINSPIRE-00041175$$uFermilab$$uVirginia U.
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001624473 700__ $$aIvanov, Andrew Gennadievich$$iINSPIRE-00052500$$uUC, Davis$$uKansas State U.
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001624473 700__ $$aJayatilaka, Bodhitha Anjalike$$iINSPIRE-00052919$$uFermilab
001624473 700__ $$aJeon, Eun-Ju$$iINSPIRE-00041097$$uEwha Women's U., Seoul$$uChonbuk Natl. U.$$uChonnam Natl. U.$$uKISTI, Daejeon$$uSungkyunkwan U.$$uSeoul Natl. U.$$uKyungpook Natl. U.
001624473 700__ $$aJindariani, Sergo Robert$$iINSPIRE-00041085$$uFermilab
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001624473 700__ $$aJoo, Kyung Kwang$$iINSPIRE-00041073$$uEwha Women's U., Seoul$$uChonbuk Natl. U.$$uChonnam Natl. U.$$uKISTI, Daejeon$$uSungkyunkwan U.$$uSeoul Natl. U.$$uKyungpook Natl. U.
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001624473 700__ $$aJunk, Thomas R$$iINSPIRE-00094115$$uFermilab
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001624473 700__ $$aKamon, Teruki$$iINSPIRE-00094564$$uTexas A-M$$uEwha Women's U., Seoul$$uChonbuk Natl. U.$$uChonnam Natl. U.$$uKISTI, Daejeon$$uSungkyunkwan U.$$uSeoul Natl. U.$$uKyungpook Natl. U.
001624473 700__ $$aKarchin, Paul Edmund$$iINSPIRE-00094965$$uWayne State U.
001624473 700__ $$aKasmi, Azeddine$$iINSPIRE-00180696$$uBaylor U.
001624473 700__ $$aKato, Yukihiro$$iINSPIRE-00095181$$uOsaka City U.$$uKinki U., Osaka
001624473 700__ $$aKetchum, Wesley Robert$$iINSPIRE-00300120$$uChicago U., EFI$$uLos Alamos
001624473 700__ $$aKeung, Justin Kien$$iINSPIRE-00021191$$uPennsylvania U.
001624473 700__ $$aKilminster, Benjamin John$$iINSPIRE-00096201$$uFermilab$$uZurich U.
001624473 700__ $$aKim, DongHee$$iINSPIRE-00096223$$uEwha Women's U., Seoul$$uChonbuk Natl. U.$$uChonnam Natl. U.$$uKISTI, Daejeon$$uSungkyunkwan U.$$uSeoul Natl. U.$$uKyungpook Natl. U.
001624473 700__ $$aKim, Hyunsoo$$iINSPIRE-00096259$$uEwha Women's U., Seoul$$uChonbuk Natl. U.$$uChonnam Natl. U.$$uKISTI, Daejeon$$uSungkyunkwan U.$$uSeoul Natl. U.$$uKyungpook Natl. U.
001624473 700__ $$aKim, Jieun$$iINSPIRE-00000135$$uEwha Women's U., Seoul$$uChonbuk Natl. U.$$uChonnam Natl. U.$$uKISTI, Daejeon$$uSungkyunkwan U.$$uSeoul Natl. U.$$uKyungpook Natl. U.
001624473 700__ $$aKim, Min Jeong$$iINSPIRE-00096309$$uFrascati
001624473 700__ $$aKim, Shin-Hong$$iINSPIRE-00019770$$uTsukuba U.
001624473 700__ $$aKim, Soo Bong$$iINSPIRE-00096336$$uEwha Women's U., Seoul$$uChonbuk Natl. U.$$uChonnam Natl. U.$$uKISTI, Daejeon$$uSungkyunkwan U.$$uSeoul Natl. U.$$uKyungpook Natl. U.
001624473 700__ $$aKim, Young-Jin$$iINSPIRE-00265051$$uEwha Women's U., Seoul$$uChonbuk Natl. U.$$uChonnam Natl. U.$$uKISTI, Daejeon$$uSungkyunkwan U.$$uSeoul Natl. U.$$uKyungpook Natl. U.
001624473 700__ $$aKim, Young-Kee$$iINSPIRE-00096350$$uChicago U., EFI
001624473 700__ $$aKimura, Naoki$$iINSPIRE-00008600$$uWaseda U.
001624473 700__ $$aKirby, Michael H$$iINSPIRE-00059470$$uFermilab
001624473 700__ $$aKnoepfel, Kyle James$$iINSPIRE-00003680$$uFermilab
001624473 700__ $$aKondo, Kunitaka$$iINSPIRE-00097557$$uWaseda U.
001624473 700__ $$aKong, Dae Jung$$iINSPIRE-00041051$$uEwha Women's U., Seoul$$uChonbuk Natl. U.$$uChonnam Natl. U.$$uKISTI, Daejeon$$uSungkyunkwan U.$$uSeoul Natl. U.$$uKyungpook Natl. U.
001624473 700__ $$aKonigsberg, Jacobo$$iINSPIRE-00097609$$uFlorida U.
001624473 700__ $$aKotwal, Ashutosh Vijay$$iINSPIRE-00097984$$uDuke U.
001624473 700__ $$aKreps, Michal$$iINSPIRE-00041048$$uKIT, Karlsruhe, EKP
001624473 700__ $$aKroll, IJoseph$$iINSPIRE-00098670$$uPennsylvania U.
001624473 700__ $$aKruse, Mark Charles$$iINSPIRE-00098798$$uDuke U.
001624473 700__ $$aKuhr, Thomas$$iINSPIRE-00030450$$uKIT, Karlsruhe, EKP
001624473 700__ $$aKurata, Masakazu$$iINSPIRE-00012191$$uTsukuba U.
001624473 700__ $$aLaasanen, Alvin Toivo$$iINSPIRE-00099492$$uPurdue U.
001624473 700__ $$aLammel, Stephan$$iINSPIRE-00099781$$uFermilab
001624473 700__ $$aLancaster, Mark$$iINSPIRE-00099803$$uUniversity Coll. London
001624473 700__ $$aLannon, Kevin Patrick$$iINSPIRE-00054488$$uOhio State U.$$uNotre Dame U.
001624473 700__ $$aLatino, Giuseppe$$iINSPIRE-00100151$$uINFN, Pisa$$uSiena U.
001624473 700__ $$aLee, Hyun Su$$iINSPIRE-00300150$$uEwha Women's U., Seoul$$uChonbuk Natl. U.$$uChonnam Natl. U.$$uKISTI, Daejeon$$uSungkyunkwan U.$$uSeoul Natl. U.$$uKyungpook Natl. U.
001624473 700__ $$aLee, Jaison$$iINSPIRE-00307082$$uEwha Women's U., Seoul$$uChonbuk Natl. U.$$uChonnam Natl. U.$$uKISTI, Daejeon$$uSungkyunkwan U.$$uSeoul Natl. U.$$uKyungpook Natl. U.
001624473 700__ $$aLeo, Sabato$$iINSPIRE-00201038$$uINFN, Pisa
001624473 700__ $$aLeone, Sandra$$iINSPIRE-00101163$$uINFN, Pisa
001624473 700__ $$aLewis, Jonathan D$$iINSPIRE-00101520$$uFermilab
001624473 700__ $$aLimosani, Antonio$$iINSPIRE-00219183$$uDuke U.$$uMelbourne U.
001624473 700__ $$aLipeles, Elliot David$$iINSPIRE-00102076$$uPennsylvania U.
001624473 700__ $$aLister, Alison$$iINSPIRE-00149260$$uGeneva U.$$uBritish Columbia U.
001624473 700__ $$aLiu, Hao$$iINSPIRE-00265154$$uVirginia U.
001624473 700__ $$aLiu, Qiuguang$$iINSPIRE-00243703$$uPurdue U.
001624473 700__ $$aLiu, Tiehui Ted$$iINSPIRE-00102265$$uFermilab
001624473 700__ $$aLockwitz, Sarah E$$iINSPIRE-00047280$$uYale U.
001624473 700__ $$aLoginov, Andrey Borisovich$$iINSPIRE-00025442$$uYale U.
001624473 700__ $$aLucchesi, Donatella$$iINSPIRE-00102927$$uINFN, Padua$$uPadua U.
001624473 700__ $$aLucà, Alessandra$$iINSPIRE-00265733$$uFrascati
001624473 700__ $$aLueck, Jan$$iINSPIRE-00048772$$uKIT, Karlsruhe, EKP
001624473 700__ $$aLujan, Paul Joseph$$iINSPIRE-00018533$$uLBL, Berkeley
001624473 700__ $$aLukens, Patrick Thomas$$iINSPIRE-00103032$$uFermilab
001624473 700__ $$aLungu, Gheorghe$$iINSPIRE-00041007$$uRockefeller U.
001624473 700__ $$aLys, Jeremy E$$iINSPIRE-00103363$$uLBL, Berkeley
001624473 700__ $$aLysak, Roman$$iINSPIRE-00040995$$uKosice, IEF$$uComenius U.$$uPrague, Inst. Phys.
001624473 700__ $$aMadrak, Robyn Leigh$$iINSPIRE-00103653$$uFermilab
001624473 700__ $$aMaestro, Paolo$$iINSPIRE-00264893$$uINFN, Pisa$$uSiena U.
001624473 700__ $$aMalik, Sarah Alam$$iINSPIRE-00008612$$uRockefeller U.
001624473 700__ $$aManca, Giulia$$iINSPIRE-00057054$$uLiverpool U.$$uINFN, Cagliari
001624473 700__ $$aManousakis-Katsikakis, Arkadios$$iINSPIRE-00003884$$uAthens U.
001624473 700__ $$aMarchese, Luigi$$iINSPIRE-00377884$$uNaples U.$$uINFN, Bologna
001624473 700__ $$aMargaroli, Fabrizio$$iINSPIRE-00040958$$uINFN, Rome
001624473 700__ $$aMarino, Christopher Phillip$$iINSPIRE-00030781$$uINFN, Pisa$$uPisa, Scuola Normale Superiore
001624473 700__ $$aMartínez-Perez, Mario$$iINSPIRE-00105204$$uBarcelona, IFAE
001624473 700__ $$aMatera, Keith$$iINSPIRE-00264905$$uIllinois U., Urbana
001624473 700__ $$aMattson, Mark Edward$$iINSPIRE-00105871$$uWayne State U.
001624473 700__ $$aMazzacane, Anna$$iINSPIRE-00011173$$uFermilab
001624473 700__ $$aMazzanti, Paolo$$iINSPIRE-00106040$$uINFN, Bologna
001624473 700__ $$aMcNulty, Ronan$$iINSPIRE-00106463$$uLiverpool U.$$uUniversity Coll., Dublin
001624473 700__ $$aMehta, Andrew$$iINSPIRE-00300183$$uLiverpool U.
001624473 700__ $$aMehtala, Petteri$$iINSPIRE-00030434$$uHelsinki Inst. of Phys.$$uHelsinki U.
001624473 700__ $$aMesropian, Christina$$iINSPIRE-00107098$$uRockefeller U.
001624473 700__ $$aMiao, Ting$$iINSPIRE-00107355$$uFermilab
001624473 700__ $$aMietlicki, David John$$iINSPIRE-00012298$$uMichigan U.
001624473 700__ $$aMitra, Ankush$$iINSPIRE-00008077$$uTaiwan, Inst. Phys.
001624473 700__ $$aMiyake, Hideki$$iINSPIRE-00108140$$uTsukuba U.
001624473 700__ $$aMoed, Shulamit$$iINSPIRE-00030422$$uFermilab
001624473 700__ $$aMoggi, Niccolo$$iINSPIRE-00050739$$uINFN, Bologna
001624473 700__ $$aMoon, Chang-Seong$$iINSPIRE-00024851$$uFermilab$$uParis U., VI-VII
001624473 700__ $$aMoore, Ronald Scott$$iINSPIRE-00108704$$uFermilab$$uHarvard Medical School$$uMassachusetts General Hospital
001624473 700__ $$aMorello, Michael Joseph$$iINSPIRE-00016418$$uINFN, Pisa$$uPisa, Scuola Normale Superiore
001624473 700__ $$aMukherjee, Aseet$$iINSPIRE-00109540$$uFermilab
001624473 700__ $$aMuller, Thomas$$iINSPIRE-00109666$$uKIT, Karlsruhe, EKP
001624473 700__ $$aMurat, Pavel A$$iINSPIRE-00002098$$uFermilab
001624473 700__ $$aMussini, Manuel$$iINSPIRE-00024830$$uINFN, Bologna$$uBologna U.
001624473 700__ $$aNachtman, Jane Marie$$iINSPIRE-00109954$$uFermilab$$uIowa U.
001624473 700__ $$aNagai, Yoshikazu$$iINSPIRE-00012203$$uTsukuba U.
001624473 700__ $$aNaganoma, Junji$$iINSPIRE-00040935$$uWaseda U.
001624473 700__ $$aNakano, Itsuo$$iINSPIRE-00040923$$uOkayama U.
001624473 700__ $$aNapier, Austin$$iINSPIRE-00110388$$uTufts U.
001624473 700__ $$aNett, Jason Michael$$iINSPIRE-00011870$$uTexas A-M
001624473 700__ $$aNeu, Christopher Carl$$iINSPIRE-00110970$$uVirginia U.
001624473 700__ $$aNigmanov, Turgun S$$iINSPIRE-00040900$$uPittsburgh U.
001624473 700__ $$aNodulman, Lawrence J$$iINSPIRE-00111767$$uArgonne
001624473 700__ $$aNoh, Seoyoung$$iINSPIRE-00264911$$uEwha Women's U., Seoul$$uChonbuk Natl. U.$$uChonnam Natl. U.$$uKISTI, Daejeon$$uSungkyunkwan U.$$uSeoul Natl. U.$$uKyungpook Natl. U.
001624473 700__ $$aNorniella Francisco, Olga$$iINSPIRE-00046648$$uIllinois U., Urbana
001624473 700__ $$aNurse, Emily L$$iINSPIRE-00052439$$uUniversity Coll. London
001624473 700__ $$aOakes, Louise Beth$$iINSPIRE-00018963$$uOxford U.
001624473 700__ $$aOh, Seog Hwan$$iINSPIRE-00112667$$uDuke U.
001624473 700__ $$aOh, Young-do$$iINSPIRE-00003877$$uEwha Women's U., Seoul$$uChonbuk Natl. U.$$uChonnam Natl. U.$$uKISTI, Daejeon$$uSungkyunkwan U.$$uSeoul Natl. U.$$uKyungpook Natl. U.
001624473 700__ $$aOksuzian, Iuri Artur$$iINSPIRE-00006667$$uVirginia U.
001624473 700__ $$aOkusawa, Toru$$iINSPIRE-00112892$$uOsaka City U.
001624473 700__ $$aOrava, Risto Olavi$$iINSPIRE-00113286$$uHelsinki Inst. of Phys.$$uHelsinki U.
001624473 700__ $$aOrtolan, Lorenzo$$iINSPIRE-00179465$$uBarcelona, IFAE
001624473 700__ $$aPagliarone, Carmine Elvezio$$iINSPIRE-00304689$$uINFN, Trieste
001624473 700__ $$aPalencia, Jose Enrique$$iINSPIRE-00207239$$uCantabria Inst. of Phys.$$uCERN
001624473 700__ $$aPalni, Prabhakar$$iINSPIRE-00265540$$uNew Mexico U.
001624473 700__ $$aPapadimitriou, Vaia$$iINSPIRE-00114423$$uFermilab
001624473 700__ $$aParker, William Chesluk$$iINSPIRE-00206947$$uWisconsin U., Madison
001624473 700__ $$aPauletta, Giovanni$$iINSPIRE-00115172$$uINFN, Udine$$uINFN, Trieste$$uUdine U.
001624473 700__ $$aPaulini, Manfred$$iINSPIRE-00115182$$uCarnegie Mellon U.
001624473 700__ $$aPaus, Christoph Maria Ernst$$iINSPIRE-00115190$$uMIT
001624473 700__ $$aPhillips, Thomas J$$iINSPIRE-00116206$$uDuke U.
001624473 700__ $$aPiacentino, Giovanni M$$iINSPIRE-00004814$$uINFN, Pisa
001624473 700__ $$aPianori, Elisabetta$$iINSPIRE-00009958$$uPennsylvania U.
001624473 700__ $$aPilot, Justin Robert$$iINSPIRE-00243713$$uUC, Davis
001624473 700__ $$aPitts, Kevin T$$iINSPIRE-00116753$$uIllinois U., Urbana
001624473 700__ $$aPlager, Charles$$iINSPIRE-00116811$$uUCLA
001624473 700__ $$aPondrom, Lee G$$iINSPIRE-00117205$$uWisconsin U., Madison
001624473 700__ $$aPoprocki, Stephen$$iINSPIRE-00264625$$uFermilab$$uCornell U.
001624473 700__ $$aPotamianos, Karolos Jozef$$iINSPIRE-00019188$$uLBL, Berkeley
001624473 700__ $$aPranko, Aliaksandr Pavlovich$$iINSPIRE-00049000$$uLBL, Berkeley
001624473 700__ $$aProkoshin, Fedor$$iINSPIRE-00030407$$uDubna, JINR$$uSanta Maria U., Valparaiso
001624473 700__ $$aPtohos, Fotios K$$iINSPIRE-00117980$$uFrascati$$uCyprus U.
001624473 700__ $$aPunzi, Giovanni$$iINSPIRE-00118078$$uINFN, Pisa$$uPisa U.
001624473 700__ $$aRanjan, Niharika$$iINSPIRE-00030395$$uPurdue U.
001624473 700__ $$aRedondo Fernández, Ignacio$$iINSPIRE-00300251$$uMadrid, CIEMAT
001624473 700__ $$aRenton, Peter B$$iINSPIRE-00119660$$uOxford U.
001624473 700__ $$aRescigno, Marco$$iINSPIRE-00119727$$uINFN, Rome
001624473 700__ $$aRiddick, Thomas C$$iINSPIRE-00014594$$uUniversity Coll. London
001624473 700__ $$aRimondi, Franco$$iINSPIRE-00120236$$uINFN, Bologna
001624473 700__ $$aRistori, Luciano$$iINSPIRE-00040831$$uFermilab$$uINFN, Pisa
001624473 700__ $$aRobson, Aidan$$iINSPIRE-00052951$$uGlasgow U.
001624473 700__ $$aRodriguez, Tatiana Isabel$$iINSPIRE-00046914$$uPennsylvania U.
001624473 700__ $$aRolli, Simona$$iINSPIRE-00120949$$uTufts U.$$uDept. of Energy, Wash., D.C.
001624473 700__ $$aRonzani, Manfredi$$iINSPIRE-00265551$$uINFN, Pisa$$uPisa U.
001624473 700__ $$aRoser, Robert Martin$$iINSPIRE-00121249$$uFermilab
001624473 700__ $$aRosner, Jonathan L$$iINSPIRE-00121273$$uChicago U., EFI
001624473 700__ $$aRuffini, Fabrizio$$iINSPIRE-00243727$$uINFN, Pisa$$uSiena U.
001624473 700__ $$aRuiz Jimeno, Alberto$$iINSPIRE-00121790$$uCantabria Inst. of Phys.
001624473 700__ $$aRuss, James S$$iINSPIRE-00121950$$uCarnegie Mellon U.
001624473 700__ $$aRusu, Vadim Liviu$$iINSPIRE-00054817$$uFermilab
001624473 700__ $$aSakumoto, Willis Kazuo$$iINSPIRE-00122656$$uRochester U.
001624473 700__ $$aSakurai, Yuki$$iINSPIRE-00263552$$uWaseda U.
001624473 700__ $$aSanti, Lorenzo$$iINSPIRE-00123140$$uUdine U.$$uINFN, Udine$$uINFN, Trieste
001624473 700__ $$aSato, Koji$$iINSPIRE-00048967$$uTsukuba U.
001624473 700__ $$aSaveliev, Valeri$$iINSPIRE-00123518$$uFermilab$$uMoscow Phys. Eng. Inst.
001624473 700__ $$aSavoy-Navarro, Aurore$$iINSPIRE-00050058$$uFermilab$$uParis U., VI-VII
001624473 700__ $$aSchlabach, Philip$$iINSPIRE-00124075$$uFermilab
001624473 700__ $$aSchmidt, Eugene E$$iINSPIRE-00124202$$uFermilab
001624473 700__ $$aSchwarz, Thomas A$$iINSPIRE-00025352$$uMichigan U.
001624473 700__ $$aScodellaro, Luca$$iINSPIRE-00050941$$uCantabria Inst. of Phys.
001624473 700__ $$aScuri, Fabrizio$$iINSPIRE-00124895$$uINFN, Pisa
001624473 700__ $$aSeidel, Sally C$$iINSPIRE-00125002$$uNew Mexico U.
001624473 700__ $$aSeiya, Yoshihiro$$iINSPIRE-00125059$$uOsaka City U.
001624473 700__ $$aSemenov, Alexei$$iINSPIRE-00300240$$uDubna, JINR
001624473 700__ $$aSforza, Federico$$iINSPIRE-00011580$$uINFN, Pisa$$uPisa U.
001624473 700__ $$aShalhout, Shalhout Zaki$$iINSPIRE-00024697$$uUC, Davis
001624473 700__ $$aShears, Tara G$$iINSPIRE-00125751$$uLiverpool U.
001624473 700__ $$aShekhar, Ravi$$iINSPIRE-00010168$$uDuke U.
001624473 700__ $$aShepard, Paul F$$iINSPIRE-00125822$$uPittsburgh U.
001624473 700__ $$aShimojima, Makoto$$iINSPIRE-00050740$$uTsukuba U.$$uNagasaki Inst. Appl. Sci.
001624473 700__ $$aShochet, Melvyn J$$iINSPIRE-00126064$$uChicago U., EFI
001624473 700__ $$aSimonenko, Alexander V$$iINSPIRE-00304697$$uDubna, JINR
001624473 700__ $$aSliwa, Krzysztof Jan$$iINSPIRE-00127092$$uTufts U.
001624473 700__ $$aSmith, John Rodgers$$iINSPIRE-00127290$$uUC, Davis
001624473 700__ $$aSnider, Frederick Douglas$$iINSPIRE-00127382$$uFermilab
001624473 700__ $$aSong, Hao$$iINSPIRE-00264923$$uPittsburgh U.
001624473 700__ $$aSorin, Maria Veronica$$iINSPIRE-00049169$$uBarcelona, IFAE
001624473 700__ $$aSt Denis, Richard Dante$$iINSPIRE-00128281$$uGlasgow U.
001624473 700__ $$aStancari, Michelle Dawn$$iINSPIRE-00158339$$uFermilab
001624473 700__ $$aStelzer-Chilton, Oliver$$iINSPIRE-00040726$$uTRIUMF$$uToronto U.$$uSimon Fraser U.$$uMcGill U.
001624473 700__ $$aStentz, Dale James$$iINSPIRE-00005352$$uFermilab$$uNorthwestern U.
001624473 700__ $$aStrologas, John$$iINSPIRE-00129384$$uNew Mexico U.
001624473 700__ $$aSudo, Yuji$$iINSPIRE-00012960$$uTsukuba U.
001624473 700__ $$aSukhanov, Alexander I$$iINSPIRE-00129629$$uFermilab
001624473 700__ $$aSun, Siyuan$$iINSPIRE-00375257$$uDuke U.
001624473 700__ $$aSuslov, Igor M$$iINSPIRE-00129846$$uDubna, JINR
001624473 700__ $$aTakemasa, Ken-ichi$$iINSPIRE-00012837$$uTsukuba U.
001624473 700__ $$aTakeuchi, Yuji$$iINSPIRE-00130468$$uTsukuba U.
001624473 700__ $$aTang, Jian$$iINSPIRE-00307095$$uChicago U., EFI
001624473 700__ $$aTecchio, Monica$$iINSPIRE-00130929$$uMichigan U.
001624473 700__ $$aTecker-Shreyber, Irina$$iINSPIRE-00040779$$uMoscow, ITEP
001624473 700__ $$aTeng, Ping-Kun$$iINSPIRE-00040709$$uTaiwan, Inst. Phys.
001624473 700__ $$aThom, Julia$$iINSPIRE-00131258$$uFermilab$$uCornell U.
001624473 700__ $$aThomson, Evelyn Jean$$iINSPIRE-00300284$$uPennsylvania U.
001624473 700__ $$aThukral, Vaikunth$$iINSPIRE-00265563$$uTexas A-M
001624473 700__ $$aToback, David A$$iINSPIRE-00131642$$uTexas A-M
001624473 700__ $$aTokar, Stanislav$$iINSPIRE-00131686$$uKosice, IEF$$uComenius U.
001624473 700__ $$aTollefson, Kirsten Anne$$iINSPIRE-00131715$$uMichigan State U.
001624473 700__ $$aTomura, Tomonobu$$iINSPIRE-00047184$$uTsukuba U.
001624473 700__ $$aTonelli, Diego$$iINSPIRE-00053184$$uFermilab$$uCERN
001624473 700__ $$aTorre, Stefano$$iINSPIRE-00300295$$uFrascati
001624473 700__ $$aTorretta, Donatella$$iINSPIRE-00300206$$uFermilab
001624473 700__ $$aTotaro, Pierluigi$$iINSPIRE-00018931$$uINFN, Padua
001624473 700__ $$aTrovato, Marco$$iINSPIRE-00010990$$uINFN, Pisa$$uPisa, Scuola Normale Superiore
001624473 700__ $$aUkegawa, Fumihiko$$iINSPIRE-00132910$$uTsukuba U.
001624473 700__ $$aUozumi, Satoru$$iINSPIRE-00040667$$uEwha Women's U., Seoul$$uChonbuk Natl. U.$$uChonnam Natl. U.$$uKISTI, Daejeon$$uSungkyunkwan U.$$uSeoul Natl. U.$$uKyungpook Natl. U.
001624473 700__ $$aVázquez-Valencia, Elsa Fabiola$$iINSPIRE-00020395$$uFlorida U.$$uIberoamericana U.
001624473 700__ $$aVelev, Gueorgui$$iINSPIRE-00133716$$uFermilab
001624473 700__ $$aVellidis, Konstantinos$$iINSPIRE-00022018$$uFermilab
001624473 700__ $$aVernieri, Caterina$$iINSPIRE-00342428$$uINFN, Pisa$$uPisa, Scuola Normale Superiore
001624473 700__ $$aVidal Marono, Miguel$$iINSPIRE-00015995$$uPurdue U.
001624473 700__ $$aVilar Cortabitarte, Rocio$$iINSPIRE-00317752$$uCantabria Inst. of Phys.
001624473 700__ $$aVizán Garcia, Jesus Manuel$$iINSPIRE-00309097$$uCantabria Inst. of Phys.$$uLouvain U.
001624473 700__ $$aVogel, Marcelo$$iINSPIRE-00009675$$uNew Mexico U.
001624473 700__ $$aVolpi, Guido$$iINSPIRE-00040623$$uFrascati
001624473 700__ $$aWagner, Peter$$iINSPIRE-00052760$$uPennsylvania U.
001624473 700__ $$aWallny, Rainer S$$iINSPIRE-00040611$$uZurich, ETH$$uFermilab
001624473 700__ $$aWang, Song-Ming$$iINSPIRE-00134900$$uTaiwan, Inst. Phys.
001624473 700__ $$aWaters, David S$$iINSPIRE-00135080$$uUniversity Coll. London
001624473 700__ $$aWester, William Carl$$iINSPIRE-00135583$$uFermilab
001624473 700__ $$aWhiteson, Daniel O$$iINSPIRE-00054720$$uPennsylvania U.$$uUC, Irvine
001624473 700__ $$aWicklund, Arthur Barry$$iINSPIRE-00135838$$uArgonne
001624473 700__ $$aWilbur, Scott$$iINSPIRE-00013324$$uUC, Davis
001624473 700__ $$aWilliams, Hugh H$$iINSPIRE-00136066$$uPennsylvania U.
001624473 700__ $$aWilson, Jonathan Samuel$$iINSPIRE-00007602$$uMichigan U.
001624473 700__ $$aWilson, Peter James$$iINSPIRE-00136160$$uFermilab
001624473 700__ $$aWiner, Brian L$$iINSPIRE-00136218$$uOhio State U.
001624473 700__ $$aWittich, Peter$$iINSPIRE-00136393$$uFermilab$$uCornell U.
001624473 700__ $$aWolbers, Stephen A$$iINSPIRE-00136433$$uFermilab
001624473 700__ $$aWolfe, Homer$$iINSPIRE-00307103$$uOhio State U.
001624473 700__ $$aWright, Thomas Roland$$iINSPIRE-00050660$$uMichigan U.
001624473 700__ $$aWu, Xin$$iINSPIRE-00306899$$uGeneva U.
001624473 700__ $$aWu, Zhenbin$$iINSPIRE-00243730$$uBaylor U.
001624473 700__ $$aYamamoto, Kazuhiro$$iINSPIRE-00137027$$uOsaka City U.
001624473 700__ $$aYamato, Daisuke$$iINSPIRE-00264935$$uOsaka City U.
001624473 700__ $$aYang, Tingjun$$iINSPIRE-00029184$$uFermilab
001624473 700__ $$aYang, Un-Ki$$iINSPIRE-00137286$$uEwha Women's U., Seoul$$uChonbuk Natl. U.$$uChonnam Natl. U.$$uKISTI, Daejeon$$uSungkyunkwan U.$$uSeoul Natl. U.$$uKyungpook Natl. U.
001624473 700__ $$aYang, Yu Chul$$iINSPIRE-00046512$$uEwha Women's U., Seoul$$uChonbuk Natl. U.$$uChonnam Natl. U.$$uKISTI, Daejeon$$uSungkyunkwan U.$$uSeoul Natl. U.$$uKyungpook Natl. U.
001624473 700__ $$aYao, Wei-Ming$$iINSPIRE-00137324$$uLBL, Berkeley
001624473 700__ $$aYeh, Gong Ping$$iINSPIRE-00137427$$uFermilab
001624473 700__ $$aYi, Kai$$iINSPIRE-00137481$$uFermilab$$uIowa U.
001624473 700__ $$aYoh, John$$iINSPIRE-00137542$$uFermilab
001624473 700__ $$aYorita, Kohei$$iINSPIRE-00048979$$uWaseda U.
001624473 700__ $$aYoshida, Takuo$$iINSPIRE-00137621$$uOsaka City U.$$uFukui U.
001624473 700__ $$aYu, Geum Bong$$iINSPIRE-00047046$$uDuke U.
001624473 700__ $$aYu, Intae$$iINSPIRE-00137737$$uEwha Women's U., Seoul$$uChonbuk Natl. U.$$uChonnam Natl. U.$$uKISTI, Daejeon$$uSungkyunkwan U.$$uSeoul Natl. U.$$uKyungpook Natl. U.
001624473 700__ $$aZanetti, Anna Maria$$iINSPIRE-00138097$$uINFN, Trieste
001624473 700__ $$aZeng, Yu$$iINSPIRE-00307111$$uDuke U.
001624473 700__ $$aZhou, Chen$$iINSPIRE-00264959$$uDuke U.
001624473 700__ $$aZucchelli, Stefano$$iINSPIRE-00040570$$uINFN, Bologna$$uBologna U.
001624473 710__ $$gR. C. Group
001624473 773__ $$c072003$$n7$$pPhys. Rev. D$$v89$$y2014
001624473 8564_ $$uhttp://lss.fnal.gov/archive/2013/pub/fermilab-pub-13-515-e.pdf$$yFermilab Library Server (fulltext available)
001624473 8564_ $$uhttp://www.fnal.gov/pub/today/archive/archive_2014/today14-01-16.html$$yFermilab Today Result of the Week
001624473 8564_ $$82206786$$s1097739$$uhttp://cds.cern.ch/record/1624473/files/arXiv:1311.0894.pdf
001624473 8564_ $$81334986$$s1766781$$uhttp://cds.cern.ch/record/1624473/files/fermilab-pub-13-515-e.pdf$$yFulltext
001624473 8564_ $$82206751$$s9715$$uhttp://cds.cern.ch/record/1624473/files/zee_eop_fit_et.png$$y00027 Measured energy scale as a function of electron $E_T$ for $W \to e\nu$ (top) and $Z \to ee$ (bottom) data. The simulation is corrected with the best-fit value of $\xi = (5.25 \pm 0.70) \times 10^{-3}$.
001624473 8564_ $$82206752$$s23752$$uhttp://cds.cern.ch/record/1624473/files/zee_eop_fit.png$$y00029 Distribution of $E/p$ for $W\to e\nu$ (top) and $Z\to ee$ (bottom) data (circles) after the full energy-scale calibration; the best-fit templates (histograms) are overlaid. The fit region is enclosed by arrows.
001624473 8564_ $$82206753$$s22389$$uhttp://cds.cern.ch/record/1624473/files/zmm_mass_fit.png$$y00022 Distribution of $m_{\mu\mu}$ for the best-fit template (histogram) and data (circles) in the $Z\rightarrow\mu\mu$ candidate sample. The filled histogram shows the $\gamma^*\to\mu\mu$ contribution. The fit region is enclosed by the arrows.
001624473 8564_ $$82206754$$s7080$$uhttp://cds.cern.ch/record/1624473/files/recoilw.png$$y00001 Typical vectors associated to quantities reconstructed in a $W$-boson event, with the recoil hadron momentum ($\vec{u}_T$) separated into axes parallel ($u_{||}$) and perpendicular ($u_{\perp}$) to the charged lepton.
001624473 8564_ $$82206755$$s11933$$uhttp://cds.cern.ch/record/1624473/files/chi_we_pt_fit.png$$y00073 Differences between the data and simulation, divided by the expected statistical uncertainty, for the $p_T$ distributions in the muon (top) and electron (bottom) channels.
001624473 8564_ $$82206756$$s25658$$uhttp://cds.cern.ch/record/1624473/files/wm_mt_fit.png$$y00064 Distributions of $m_T$ for $W$ boson decays to $\mu\nu$ (top) and $e\nu$ (bottom) final states in simulated (histogram) and experimental (points) data. The simulation corresponds to the maximum-likelihood value of $M_W$ and includes backgrounds (shaded). The likelihood is computed using events between the two arrows.
001624473 8564_ $$82206757$$s11417$$uhttp://cds.cern.ch/record/1624473/files/chi_wm_mt_fit.png$$y00070 Differences between the data and simulation, divided by the expected statistical uncertainty, for the $m_T$ distributions in the muon (top) and electron (bottom) channels.
001624473 8564_ $$82206758$$s12020$$uhttp://cds.cern.ch/record/1624473/files/chi_wm_met_fit.png$$y00074 Differences between the data and simulation, divided by the expected statistical uncertainty, for the $p_T^\nu$ distributions in the muon (top) and electron (bottom) channels.
001624473 8564_ $$82206759$$s9254$$uhttp://cds.cern.ch/record/1624473/files/alignment.png$$y00009 Definitions of the tilt ($\Delta \tau$) and shift ($R\Delta\phi$) corrections derived for each twelve-wire COT cell using cosmic-ray data.
001624473 8564_ $$82206760$$s13383$$uhttp://cds.cern.ch/record/1624473/files/wmupar_dataMC.png$$y00058 Distributions of $u_{||}$ from simulation (histogram) and data (circles) for $W$ boson decays to $\mu\nu$ (top) and $e\nu$ (bottom) final states. The simulation uses parameters fit from $Z$ boson data, and the uncertainty on the simulation is due to the statistical uncertainty on these parameters. The data mean ($\mu$) and rms spread ($\sigma$) are well-modeled by the simulation.
001624473 8564_ $$82206761$$s10139$$uhttp://cds.cern.ch/record/1624473/files/mass_vs_lowend_el_mt.png$$y00076 Variations of the $M_W$ value determined from the transverse-mass fit as a function of the choice of the (top) lower and (bottom) upper edge of the fit range, for the electron (left) and muon (right) channels. Uncertainty bars indicate expected variationwith respect to the default fit window, as computed using pseudoexperiments. The dashed lines indicate the statistical uncertainty from the default mass fit.
001624473 8564_ $$82206762$$s22401$$uhttp://cds.cern.ch/record/1624473/files/zee_trackmass_hieop_fit.png$$y00033 Best-fit $M_Z$ templates (histogram) compared to data (circles) in $Z\to ee$ decays using only reconstructed track information in events with two nonradiative electrons (top), one radiative electron (middle), or two radiative electrons (bottom). The nonradiative fit region is enclosed by arrows; the other fit regions are to the left of the arrows.
001624473 8564_ $$82206763$$s11285$$uhttp://cds.cern.ch/record/1624473/files/effvsupareleprd.png$$y00008 Electron identification efficiency as a function of the recoil component in the direction of the electron ($u_{||}$).
001624473 8564_ $$82206764$$s24733$$uhttp://cds.cern.ch/record/1624473/files/we_mt_fit.png$$y00065 Distributions of $m_T$ for $W$ boson decays to $\mu\nu$ (top) and $e\nu$ (bottom) final states in simulated (histogram) and experimental (points) data. The simulation corresponds to the maximum-likelihood value of $M_W$ and includes backgrounds (shaded). The likelihood is computed using events between the two arrows.
001624473 8564_ $$82206765$$s11380$$uhttp://cds.cern.ch/record/1624473/files/ups_pt_compare.png$$y00017 Distributions of $p_T^{\mu\mu}$ (top), $p_T^{\mu}$ (middle), and $p_z^{\mu}$ (bottom) in the data (circles) and the tuned simulation of $\Upsilon$ decays (histogram). The data distributions correspond to the mass range $9.30-9.56$ GeV and are background-subtracted using events in the mass ranges $9.17-9.3$ GeV and $9.56-9.69$ GeV.
001624473 8564_ $$82206766$$s9919$$uhttp://cds.cern.ch/record/1624473/files/zmSigmaBalancevsPt1_dataMC.png$$y00051 Resolution on $0.65 p^{\ell\ell}_{\eta} + u_{\eta}$ (left) and $0.65 p^{\ell\ell}_{\xi} + u_{\xi}$ (right) in simulated (lines) and data (circles) $Z$-boson decays to muons (top) and electrons (bottom). The sum of the $\chi^2$ values in the $\xi$ or $\eta$ direction is minimized in the fit for the jet angular resolution parameters or the recoil resolution parameters ($N_{W,Z}$ and $s_\mathrm{had}$), respectively.
001624473 8564_ $$82206767$$s10276$$uhttp://cds.cern.ch/record/1624473/files/mass_vs_lowend_mu_met.png$$y00085 Variations of the $M_W$ value determined from the neutrino-transverse-momentum fit as a function of the choice of the (top) lower and (bottom) upper edge of the fit range, for the electron (left) and muon (right) channels. Uncertainty bars indicate expected variation with respect to the default fit window, as computed using pseudoexperiments. The dashed lines indicate the statistical uncertainty from the default mass fit.
001624473 8564_ $$82206768$$s16757$$uhttp://cds.cern.ch/record/1624473/files/zept_dataMC.png$$y00005 Distributions of $p_T^Z$ from simulation (histogram) and data (circles) for $Z$-boson decays to $\mu\mu$ (top), and to $ee$ (bottom). The distributions are used to fit for the nonperturbative parameter $g_2$ and for $\alpha_s$.
001624473 8564_ $$82206769$$s9619$$uhttp://cds.cern.ch/record/1624473/files/mugridhadetotprd.png$$y00038 Average measured energy (in MeV) in the electromagnetic (top) and hadronic (bottom) calorimeters in the vicinity of the muon in $W$-boson decays. The differences $\Delta \phi$ and $\Delta \eta$ are signed such that positive differences correspond to towers closest to the muon position at the CES detector. The three towers inside the box are removed from the recoil measurement.
001624473 8564_ $$82206770$$s16979$$uhttp://cds.cern.ch/record/1624473/files/eopvcotdiffprd.png$$y00010 Difference in $\langle E/p \rangle$ between positrons and electrons as a function of $\cot\theta$ (left) and $\phi$ (right). The closed triangles correspond to measurements after the cosmic-ray alignment, and the open circles correspond to measurements after curvature corrections based on the $\langle E/p \rangle$ difference.
001624473 8564_ $$82206771$$s10829$$uhttp://cds.cern.ch/record/1624473/files/threetoweretvseta_dataMC.png$$y00043 Variation of underlying event $E_T$ in the three-tower region rotated by $90^\circ$ in $\phi$ from the muon as a function of $u_{||}$ (top), $|u_{\perp}|$ (middle), and $\eta$ (bottom) for $W\to \mu\nu$ data (circles) and simulation (points).
001624473 8564_ $$82206772$$s7019$$uhttp://cds.cern.ch/record/1624473/files/pscale_bfield.png$$y00014 Measured $\Delta p/p$ as a function of the mean $\cot\theta$ of the muon pair from $J/\psi$ decay, after requiring $|\Delta\cot\theta|&lt;0.1$ and including corrections.
001624473 8564_ $$82206773$$s12136$$uhttp://cds.cern.ch/record/1624473/files/chi_we_met_fit.png$$y00075 Differences between the data and simulation, divided by the expected statistical uncertainty, for the $p_T^\nu$ distributions in the muon (top) and electron (bottom) channels.
001624473 8564_ $$82206774$$s9303$$uhttp://cds.cern.ch/record/1624473/files/psi_sumcurv_compare_coths.png$$y00013 Distributions of $p_T^{\mu\mu}$ (top) and $\sum q/p_T^\mu$ (bottom) in the data (circles) and the tuned simulation of $J/\psi$ decays (histogram). The data distributions are background-subtracted using events in the mass range 3.17--3.31 GeV.
001624473 8564_ $$82206775$$s13834$$uhttp://cds.cern.ch/record/1624473/files/weut_dataMC.png$$y00063 Distributions of $u_T$ from simulation (histogram) and data (circles) for $W$ boson decays to $\mu\nu$ (top) and $e\nu$ (bottom) final states. The simulation uses parameters fit from $Z$ boson data, and the uncertainty on the simulation is due to the statistical uncertainty on these parameters. The data mean ($\mu$) and rms spread ($\sigma$) are well-modeled by the simulation.
001624473 8564_ $$82206776$$s12093$$uhttp://cds.cern.ch/record/1624473/files/zmRecoilResponse_dataMC.png$$y00048 Mean value of $R_{\textrm{rec}} \equiv -\vec{u}_T\hat{p}_T^{~\mu\mu}/p_T^{\mu\mu}$, which approximates the recoil response $R$, as a function of dimuon $p_T$. The distribution motivates the logarithmic parametrization of the response. The simulation (lines) models the data (circles) accurately.
001624473 8564_ $$82206777$$s10166$$uhttp://cds.cern.ch/record/1624473/files/mass_vs_highend_el_met.png$$y00086 Variations of the $M_W$ value determined from the neutrino-transverse-momentum fit as a function of the choice of the (top) lower and (bottom) upper edge of the fit range, for the electron (left) and muon (right) channels. Uncertainty bars indicate expected variation with respect to the default fit window, as computed using pseudoexperiments. The dashed lines indicate the statistical uncertainty from the default mass fit.
001624473 8564_ $$82206778$$s9506$$uhttp://cds.cern.ch/record/1624473/files/zmBalancevsPt1_dataMC.png$$y00049 Distribution of $0.65 p^{\ell\ell}_{\eta} + u_{\eta}$ for $Z$-boson decays to muons (top) and electrons (bottom) as a function of $Z$-boson $p_T$ in simulated (lines) and experimental (circles) data. The detector response parameters are obtained by minimizing the combined $\chi^2$ of these distributions.
001624473 8564_ $$82206779$$s13594$$uhttp://cds.cern.ch/record/1624473/files/zee_eopmat_fit.png$$y00025 Distributions of $E/p$ in data (circles) and simulation with the best-fit value of $S^{W,Z}_{\rm mat}$ (histograms) in $W\rightarrow e\nu$ (top) and $Z\to ee$ (bottom) events.
001624473 8564_ $$82206780$$s10958$$uhttp://cds.cern.ch/record/1624473/files/effvsuparmuprd.png$$y00006 Muon identification efficiency as a function of the recoil component in the direction of the muon ($u_{||}$).
001624473 8564_ $$82206781$$s11567$$uhttp://cds.cern.ch/record/1624473/files/chi_we_mt_fit.png$$y00071 Differences between the data and simulation, divided by the expected statistical uncertainty, for the $m_T$ distributions in the muon (top) and electron (bottom) channels.
001624473 8564_ $$82206782$$s10285$$uhttp://cds.cern.ch/record/1624473/files/mass_vs_lowend_el_met.png$$y00084 Variations of the $M_W$ value determined from the neutrino-transverse-momentum fit as a function of the choice of the (top) lower and (bottom) upper edge of the fit range, for the electron (left) and muon (right) channels. Uncertainty bars indicate expected variation with respect to the default fit window, as computed using pseudoexperiments. The dashed lines indicate the statistical uncertainty from the default mass fit.
001624473 8564_ $$82206783$$s8525$$uhttp://cds.cern.ch/record/1624473/files/pscale_curv_PRD.png$$y00015 Top: Fractional momentum correction $\Delta p/p$ as a function of the mean inverse transverse momentum of the muons from $J/\psi$ decay. Bottom: Representative $m_{\mu\mu}$ fit (histogram) to data (circles), here in the range $\langle 1/p_T^\mu\rangle = (0.2,0.225)$~GeV$^{-1}$. The fit region is indicated by arrows.
001624473 8564_ $$82206784$$s10281$$uhttp://cds.cern.ch/record/1624473/files/mass_vs_highend_mu_mt.png$$y00079 Variations of the $M_W$ value determined from the transverse-mass fit as a function of the choice of the (top) lower and (bottom) upper edge of the fit range, for the electron (left) and muon (right) channels. Uncertainty bars indicate expected variationwith respect to the default fit window, as computed using pseudoexperiments. The dashed lines indicate the statistical uncertainty from the default mass fit.
001624473 8564_ $$82206785$$s9000$$uhttp://cds.cern.ch/record/1624473/files/we_eop_fit_eta.png$$y00023 Measured calorimeter energy scale in bins of electron tower in $W\to e\nu$ data after corrections are applied. The towers are numbered in order of increasing $|\eta|$ and each tower subtends $\Delta \eta \approx 0.11$.
001624473 8564_ $$82206787$$s12793$$uhttp://cds.cern.ch/record/1624473/files/wmuper_dataMC.png$$y00060 Distributions of $u_{\perp}$ from simulation (histogram) and data (circles) for $W$ boson decays to $\mu\nu$ (top) and $e\nu$ (bottom) final states. The simulation uses parameters fit from $Z$ boson data, and the uncertainty on the simulation is due to the statistical uncertainty on these parameters. The data mean ($\mu$) and rms spread ($\sigma$) are well-modeled by the simulation.
001624473 8564_ $$82206788$$s11503$$uhttp://cds.cern.ch/record/1624473/files/seventoweretvsuperp90_dataMC.png$$y00045 Variation of underlying event $E_T$ in the seven-tower region rotated by $90^\circ$ in $\phi$ from the electron as a function of $u_{||}$ (top), $|u_{\perp}|$ (middle), and $\eta$ (bottom) for $W\to e\nu$ data (circles) and simulation (points).
001624473 8564_ $$82206789$$s13675$$uhttp://cds.cern.ch/record/1624473/files/etatrigprd.png$$y00007 Trigger efficiency as a function of track $\eta$ for electrons identified in the calorimeter.
001624473 8564_ $$82206790$$s11778$$uhttp://cds.cern.ch/record/1624473/files/wzprod.png$$y00000 Quark-antiquark annihilation producing a $W$ or $Z$ boson in $p\bar{p}$ collisions. Higher-order processes such as initial-state gluon radiation and final-state photon radiation are also illustrated.
001624473 8564_ $$82206791$$s24623$$uhttp://cds.cern.ch/record/1624473/files/zee_trackmass_lohieop_fit.png$$y00032 Best-fit $M_Z$ templates (histogram) compared to data (circles) in $Z\to ee$ decays using only reconstructed track information in events with two nonradiative electrons (top), one radiative electron (middle), or two radiative electrons (bottom). The nonradiative fit region is enclosed by arrows; the other fit regions are to the left of the arrows.
001624473 8564_ $$82206792$$s25405$$uhttp://cds.cern.ch/record/1624473/files/wm_met_fit.png$$y00068 Distributions of $p_T^\nu$ for $W$ boson decays to $\mu\nu$ (top) and $e\nu$ (bottom) final states in simulated (histogram) and experimental (points) data. The simulation corresponds to the maximum-likelihood value of $M_W$ and includes backgrounds (shaded). The likelihood is computed using events between the two arrows.
001624473 8564_ $$82206793$$s11910$$uhttp://cds.cern.ch/record/1624473/files/chi_wm_pt_fit.png$$y00072 Differences between the data and simulation, divided by the expected statistical uncertainty, for the $p_T$ distributions in the muon (top) and electron (bottom) channels.
001624473 8564_ $$82206794$$s13155$$uhttp://cds.cern.ch/record/1624473/files/zeudphipt8_dataMC.png$$y00056 Distributions of the angular separation between the reconstructed recoil vector $\vec{u}_T$ and the dilepton $-\vec{p}_T^{\ell \ell}$ vector in $Z \rightarrow ee$ decays, for simulation (lines) and data (circles) respectively. The distributions are shown for the ranges $p_T^{\ell \ell} &lt; 8$~GeV (top), $8 &lt; p_T^{\ell \ell} &lt; 15$~GeV (middle), and $p_T^{\ell \ell} > 15$~GeV (bottom).
001624473 8564_ $$82206795$$s11350$$uhttp://cds.cern.ch/record/1624473/files/threetoweretvsuperp90_dataMC.png$$y00042 Variation of underlying event $E_T$ in the three-tower region rotated by $90^\circ$ in $\phi$ from the muon as a function of $u_{||}$ (top), $|u_{\perp}|$ (middle), and $\eta$ (bottom) for $W\to \mu\nu$ data (circles) and simulation (points).
001624473 8564_ $$82206796$$s11981$$uhttp://cds.cern.ch/record/1624473/files/seventoweretvsupar_dataMC.png$$y00044 Variation of underlying event $E_T$ in the seven-tower region rotated by $90^\circ$ in $\phi$ from the electron as a function of $u_{||}$ (top), $|u_{\perp}|$ (middle), and $\eta$ (bottom) for $W\to e\nu$ data (circles) and simulation (points).
001624473 8564_ $$82206797$$s9214$$uhttp://cds.cern.ch/record/1624473/files/ups_pzmu_compare.png$$y00019 Distributions of $p_T^{\mu\mu}$ (top), $p_T^{\mu}$ (middle), and $p_z^{\mu}$ (bottom) in the data (circles) and the tuned simulation of $\Upsilon$ decays (histogram). The data distributions correspond to the mass range $9.30-9.56$ GeV and are background-subtracted using events in the mass ranges $9.17-9.3$ GeV and $9.56-9.69$ GeV.
001624473 8564_ $$82206798$$s15166$$uhttp://cds.cern.ch/record/1624473/files/NBCupsilon_mass_fit.png$$y00021 Distribution of $m_{\mu\mu}$ for the best-fit templates (histograms) and the data (circles) in the $\Upsilon\to\mu\mu$ sample used to calibrate the muon momentum scale. The muon tracks are reconstructed with (top) or without (bottom) a constraint to the beam position in the transverse plane. The arrows enclose the fit region.
001624473 8564_ $$82206799$$s12355$$uhttp://cds.cern.ch/record/1624473/files/weuper_dataMC.png$$y00061 Distributions of $u_{\perp}$ from simulation (histogram) and data (circles) for $W$ boson decays to $\mu\nu$ (top) and $e\nu$ (bottom) final states. The simulation uses parameters fit from $Z$ boson data, and the uncertainty on the simulation is due to the statistical uncertainty on these parameters. The data mean ($\mu$) and rms spread ($\sigma$) are well-modeled by the simulation.
001624473 8564_ $$82206800$$s9995$$uhttp://cds.cern.ch/record/1624473/files/mass_vs_lowend_mu_mt.png$$y00077 Variations of the $M_W$ value determined from the transverse-mass fit as a function of the choice of the (top) lower and (bottom) upper edge of the fit range, for the electron (left) and muon (right) channels. Uncertainty bars indicate expected variationwith respect to the default fit window, as computed using pseudoexperiments. The dashed lines indicate the statistical uncertainty from the default mass fit.
001624473 8564_ $$82206801$$s11258$$uhttp://cds.cern.ch/record/1624473/files/seventoweretvseta_dataMC.png$$y00046 Variation of underlying event $E_T$ in the seven-tower region rotated by $90^\circ$ in $\phi$ from the electron as a function of $u_{||}$ (top), $|u_{\perp}|$ (middle), and $\eta$ (bottom) for $W\to e\nu$ data (circles) and simulation (points).
001624473 8564_ $$82206802$$s10174$$uhttp://cds.cern.ch/record/1624473/files/mass_vs_highend_mu_pt.png$$y00083 Variations of the $M_W$ value determined from the charged-lepton transverse-momentum fit as a function of the choice of the (top) lower and (bottom) upper edge of the fit range, for the electron (left) and muon (right) channels. Uncertainty bars indicate expected variation with respect to the default fit window, as computed using pseudoexperiments. The dashed lines indicate the statistical uncertainty from the default mass fit.
001624473 8564_ $$82206803$$s24348$$uhttp://cds.cern.ch/record/1624473/files/zee_trackmass_loeop_fit.png$$y00031 Best-fit $M_Z$ templates (histogram) compared to data (circles) in $Z\to ee$ decays using only reconstructed track information in events with two nonradiative electrons (top), one radiative electron (middle), or two radiative electrons (bottom). The nonradiative fit region is enclosed by arrows; the other fit regions are to the left of the arrows.
001624473 8564_ $$82206804$$s24411$$uhttp://cds.cern.ch/record/1624473/files/zee_mass_loeop_fit.png$$y00034 Best-fit $M_Z$ templates (histogram) compared to data (circles) in $Z\to ee$ decays in events with two nonradiative electrons (top), one radiative electron (middle), and two radiative electrons (bottom). Fit regions are enclosed by arrows.
001624473 8564_ $$82206805$$s10233$$uhttp://cds.cern.ch/record/1624473/files/mass_vs_highend_el_pt.png$$y00082 Variations of the $M_W$ value determined from the charged-lepton transverse-momentum fit as a function of the choice of the (top) lower and (bottom) upper edge of the fit range, for the electron (left) and muon (right) channels. Uncertainty bars indicate expected variation with respect to the default fit window, as computed using pseudoexperiments. The dashed lines indicate the statistical uncertainty from the default mass fit.
001624473 8564_ $$82206806$$s8937$$uhttp://cds.cern.ch/record/1624473/files/gridhadeprd.png$$y00040 Average measured energy (in MeV) in the electromagnetic (top) and hadronic (bottom) calorimeters in the vicinity of the electron shower in $W$-boson decays. The differences $\Delta \phi$ and $\Delta \eta$ are signed such that positive differences correspond to towers closest to the electron shower position at the CES detector. The seven towers inside the box are removed from the recoil measurement.
001624473 8564_ $$82206807$$s10263$$uhttp://cds.cern.ch/record/1624473/files/zeSigmaBalancevsPt1_dataMC.png$$y00053 Resolution on $0.65 p^{\ell\ell}_{\eta} + u_{\eta}$ (left) and $0.65 p^{\ell\ell}_{\xi} + u_{\xi}$ (right) in simulated (lines) and data (circles) $Z$-boson decays to muons (top) and electrons (bottom). The sum of the $\chi^2$ values in the $\xi$ or $\eta$ direction is minimized in the fit for the jet angular resolution parameters or the recoil resolution parameters ($N_{W,Z}$ and $s_\mathrm{had}$), respectively.
001624473 8564_ $$82206808$$s15679$$uhttp://cds.cern.ch/record/1624473/files/we_eopmat_fit.png$$y00024 Distributions of $E/p$ in data (circles) and simulation with the best-fit value of $S^{W,Z}_{\rm mat}$ (histograms) in $W\rightarrow e\nu$ (top) and $Z\to ee$ (bottom) events.
001624473 8564_ $$82206809$$s7187$$uhttp://cds.cern.ch/record/1624473/files/recoilaxespt.png$$y00047 Illustration of the $\eta$ and $\xi$ axes in $Z$ boson events.
001624473 8564_ $$82206810$$s10302$$uhttp://cds.cern.ch/record/1624473/files/mass_vs_highend_mu_met.png$$y00087 Variations of the $M_W$ value determined from the neutrino-transverse-momentum fit as a function of the choice of the (top) lower and (bottom) upper edge of the fit range, for the electron (left) and muon (right) channels. Uncertainty bars indicate expected variation with respect to the default fit window, as computed using pseudoexperiments. The dashed lines indicate the statistical uncertainty from the default mass fit.
001624473 8564_ $$82206811$$s23605$$uhttp://cds.cern.ch/record/1624473/files/zee_mass_lohieop_fit.png$$y00035 Best-fit $M_Z$ templates (histogram) compared to data (circles) in $Z\to ee$ decays in events with two nonradiative electrons (top), one radiative electron (middle), and two radiative electrons (bottom). Fit regions are enclosed by arrows.
001624473 8564_ $$82206812$$s10261$$uhttp://cds.cern.ch/record/1624473/files/mass_vs_lowend_mu_pt.png$$y00081 Variations of the $M_W$ value determined from the charged-lepton transverse-momentum fit as a function of the choice of the (top) lower and (bottom) upper edge of the fit range, for the electron (left) and muon (right) channels. Uncertainty bars indicate expected variation with respect to the default fit window, as computed using pseudoexperiments. The dashed lines indicate the statistical uncertainty from the default mass fit.
001624473 8564_ $$82206813$$s10287$$uhttp://cds.cern.ch/record/1624473/files/gridemeprd.png$$y00039 Average measured energy (in MeV) in the electromagnetic (top) and hadronic (bottom) calorimeters in the vicinity of the electron shower in $W$-boson decays. The differences $\Delta \phi$ and $\Delta \eta$ are signed such that positive differences correspond to towers closest to the electron shower position at the CES detector. The seven towers inside the box are removed from the recoil measurement.
001624473 8564_ $$82206814$$s12122$$uhttp://cds.cern.ch/record/1624473/files/weupar_dataMC.png$$y00059 Distributions of $u_{||}$ from simulation (histogram) and data (circles) for $W$ boson decays to $\mu\nu$ (top) and $e\nu$ (bottom) final states. The simulation uses parameters fit from $Z$ boson data, and the uncertainty on the simulation is due to the statistical uncertainty on these parameters. The data mean ($\mu$) and rms spread ($\sigma$) are well-modeled by the simulation.
001624473 8564_ $$82206815$$s25941$$uhttp://cds.cern.ch/record/1624473/files/wm_pt_fit.png$$y00066 Distributions of $p_T^\ell$ for $W$ boson decays to $\mu\nu$ (top) and $e\nu$ (bottom) final states in simulated (histogram) and experimental (points) data.  The simulation corresponds to the maximum-likelihood value of $M_W$ and includes backgrounds (shaded). The likelihood is computed using events between the two arrows.
001624473 8564_ $$82206816$$s13337$$uhttp://cds.cern.ch/record/1624473/files/eopvphidiffprd.png$$y00011 Difference in $\langle E/p \rangle$ between positrons and electrons as a function of $\cot\theta$ (left) and $\phi$ (right). The closed triangles correspond to measurements after the cosmic-ray alignment, and the open circles correspond to measurements after curvature corrections based on the $\langle E/p \rangle$ difference.
001624473 8564_ $$82206817$$s9731$$uhttp://cds.cern.ch/record/1624473/files/zeBalancevsPt1_dataMC.png$$y00050 Distribution of $0.65 p^{\ell\ell}_{\eta} + u_{\eta}$ for $Z$-boson decays to muons (top) and electrons (bottom) as a function of $Z$-boson $p_T$ in simulated (lines) and experimental (circles) data. The detector response parameters are obtained by minimizing the combined $\chi^2$ of these distributions.
001624473 8564_ $$82206818$$s13307$$uhttp://cds.cern.ch/record/1624473/files/zeudphipt0_dataMC.png$$y00055 Distributions of the angular separation between the reconstructed recoil vector $\vec{u}_T$ and the dilepton $-\vec{p}_T^{\ell \ell}$ vector in $Z \rightarrow ee$ decays, for simulation (lines) and data (circles) respectively. The distributions are shown for the ranges $p_T^{\ell \ell} &lt; 8$~GeV (top), $8 &lt; p_T^{\ell \ell} &lt; 15$~GeV (middle), and $p_T^{\ell \ell} > 15$~GeV (bottom).
001624473 8564_ $$82206819$$s14770$$uhttp://cds.cern.ch/record/1624473/files/wmut_dataMC.png$$y00062 Distributions of $u_T$ from simulation (histogram) and data (circles) for $W$ boson decays to $\mu\nu$ (top) and $e\nu$ (bottom) final states. The simulation uses parameters fit from $Z$ boson data, and the uncertainty on the simulation is due to the statistical uncertainty on these parameters. The data mean ($\mu$) and rms spread ($\sigma$) are well-modeled by the simulation.
001624473 8564_ $$82206820$$s16049$$uhttp://cds.cern.ch/record/1624473/files/zmpt_dataMC.png$$y00004 Distributions of $p_T^Z$ from simulation (histogram) and data (circles) for $Z$-boson decays to $\mu\mu$ (top), and to $ee$ (bottom). The distributions are used to fit for the nonperturbative parameter $g_2$ and for $\alpha_s$.
001624473 8564_ $$82206821$$s13401$$uhttp://cds.cern.ch/record/1624473/files/psimass_curv_bin5.png$$y00016 Top: Fractional momentum correction $\Delta p/p$ as a function of the mean inverse transverse momentum of the muons from $J/\psi$ decay. Bottom: Representative $m_{\mu\mu}$ fit (histogram) to data (circles), here in the range $\langle 1/p_T^\mu\rangle = (0.2,0.225)$~GeV$^{-1}$. The fit region is indicated by arrows.
001624473 8564_ $$82206822$$s65683$$uhttp://cds.cern.ch/record/1624473/files/detector.png$$y00002 Cut-away view of a section of the CDF II detector (the time-of-flight detector is not shown). The slice is in half the $y-z$ plane at $x = 0$.
001624473 8564_ $$82206823$$s104042$$uhttp://cds.cern.ch/record/1624473/files/COTquad.png$$y00003 End view of a section of a COT endplate~\cite{COT}. The endplates contain precision-machined slots where each cell's sense wires and field sheets are held under tension. The radius at the center of each superlayer is shown in centimeters.
001624473 8564_ $$82206824$$s12268$$uhttp://cds.cern.ch/record/1624473/files/threetoweretvsupar_dataMC.png$$y00041 Variation of underlying event $E_T$ in the three-tower region rotated by $90^\circ$ in $\phi$ from the muon as a function of $u_{||}$ (top), $|u_{\perp}|$ (middle), and $\eta$ (bottom) for $W\to \mu\nu$ data (circles) and simulation (points).
001624473 8564_ $$82206825$$s9927$$uhttp://cds.cern.ch/record/1624473/files/zmSigmaXiBalancevsPt1_dataMC.png$$y00052 Resolution on $0.65 p^{\ell\ell}_{\eta} + u_{\eta}$ (left) and $0.65 p^{\ell\ell}_{\xi} + u_{\xi}$ (right) in simulated (lines) and data (circles) $Z$-boson decays to muons (top) and electrons (bottom). The sum of the $\chi^2$ values in the $\xi$ or $\eta$ direction is minimized in the fit for the jet angular resolution parameters or the recoil resolution parameters ($N_{W,Z}$ and $s_\mathrm{had}$), respectively.
001624473 8564_ $$82206826$$s23667$$uhttp://cds.cern.ch/record/1624473/files/zee_mass_hieop_fit.png$$y00036 Best-fit $M_Z$ templates (histogram) compared to data (circles) in $Z\to ee$ decays in events with two nonradiative electrons (top), one radiative electron (middle), and two radiative electrons (bottom). Fit regions are enclosed by arrows.
001624473 8564_ $$82206827$$s11273$$uhttp://cds.cern.ch/record/1624473/files/psi_pt_compare_coths.png$$y00012 Distributions of $p_T^{\mu\mu}$ (top) and $\sum q/p_T^\mu$ (bottom) in the data (circles) and the tuned simulation of $J/\psi$ decays (histogram). The data distributions are background-subtracted using events in the mass range 3.17--3.31 GeV.
001624473 8564_ $$82206828$$s11177$$uhttp://cds.cern.ch/record/1624473/files/mugridemetotprd.png$$y00037 Average measured energy (in MeV) in the electromagnetic (top) and hadronic (bottom) calorimeters in the vicinity of the muon in $W$-boson decays. The differences $\Delta \phi$ and $\Delta \eta$ are signed such that positive differences correspond to towers closest to the muon position at the CES detector. The three towers inside the box are removed from the recoil measurement.
001624473 8564_ $$82206829$$s9409$$uhttp://cds.cern.ch/record/1624473/files/ups_ptmu_compare.png$$y00018 Distributions of $p_T^{\mu\mu}$ (top), $p_T^{\mu}$ (middle), and $p_z^{\mu}$ (bottom) in the data (circles) and the tuned simulation of $\Upsilon$ decays (histogram). The data distributions correspond to the mass range $9.30-9.56$ GeV and are background-subtracted using events in the mass ranges $9.17-9.3$ GeV and $9.56-9.69$ GeV.
001624473 8564_ $$82206830$$s21302$$uhttp://cds.cern.ch/record/1624473/files/we_eop_fit.png$$y00028 Distribution of $E/p$ for $W\to e\nu$ (top) and $Z\to ee$ (bottom) data (circles) after the full energy-scale calibration; the best-fit templates (histograms) are overlaid. The fit region is enclosed by arrows.
001624473 8564_ $$82206831$$s10231$$uhttp://cds.cern.ch/record/1624473/files/mass_vs_highend_el_mt.png$$y00078 Variations of the $M_W$ value determined from the transverse-mass fit as a function of the choice of the (top) lower and (bottom) upper edge of the fit range, for the electron (left) and muon (right) channels. Uncertainty bars indicate expected variationwith respect to the default fit window, as computed using pseudoexperiments. The dashed lines indicate the statistical uncertainty from the default mass fit.
001624473 8564_ $$82206832$$s25056$$uhttp://cds.cern.ch/record/1624473/files/we_pt_fit.png$$y00067 Distributions of $p_T^\ell$ for $W$ boson decays to $\mu\nu$ (top) and $e\nu$ (bottom) final states in simulated (histogram) and experimental (points) data.  The simulation corresponds to the maximum-likelihood value of $M_W$ and includes backgrounds (shaded). The likelihood is computed using events between the two arrows.
001624473 8564_ $$82206833$$s23763$$uhttp://cds.cern.ch/record/1624473/files/zee_mass_fit.png$$y00030 Best-fit $M_Z$ template (histogram) compared to data (circles) in $Z\to ee$ decays. The fit region is enclosed by arrows.
001624473 8564_ $$82206834$$s14841$$uhttp://cds.cern.ch/record/1624473/files/BCupsilon_mass_fit.png$$y00020 Distribution of $m_{\mu\mu}$ for the best-fit templates (histograms) and the data (circles) in the $\Upsilon\to\mu\mu$ sample used to calibrate the muon momentum scale. The muon tracks are reconstructed with (top) or without (bottom) a constraint to the beam position in the transverse plane. The arrows enclose the fit region.
001624473 8564_ $$82206835$$s13651$$uhttp://cds.cern.ch/record/1624473/files/zeudphipt15_dataMC.png$$y00057 Distributions of the angular separation between the reconstructed recoil vector $\vec{u}_T$ and the dilepton $-\vec{p}_T^{\ell \ell}$ vector in $Z \rightarrow ee$ decays, for simulation (lines) and data (circles) respectively. The distributions are shown for the ranges $p_T^{\ell \ell} &lt; 8$~GeV (top), $8 &lt; p_T^{\ell \ell} &lt; 15$~GeV (middle), and $p_T^{\ell \ell} > 15$~GeV (bottom).
001624473 8564_ $$82206836$$s10177$$uhttp://cds.cern.ch/record/1624473/files/mass_vs_lowend_el_pt.png$$y00080 Variations of the $M_W$ value determined from the charged-lepton transverse-momentum fit as a function of the choice of the (top) lower and (bottom) upper edge of the fit range, for the electron (left) and muon (right) channels. Uncertainty bars indicate expected variation with respect to the default fit window, as computed using pseudoexperiments. The dashed lines indicate the statistical uncertainty from the default mass fit.
001624473 8564_ $$82206837$$s10109$$uhttp://cds.cern.ch/record/1624473/files/we_eop_fit_et.png$$y00026 Measured energy scale as a function of electron $E_T$ for $W \to e\nu$ (top) and $Z \to ee$ (bottom) data. The simulation is corrected with the best-fit value of $\xi = (5.25 \pm 0.70) \times 10^{-3}$.
001624473 8564_ $$82206838$$s24985$$uhttp://cds.cern.ch/record/1624473/files/we_met_fit.png$$y00069 Distributions of $p_T^\nu$ for $W$ boson decays to $\mu\nu$ (top) and $e\nu$ (bottom) final states in simulated (histogram) and experimental (points) data. The simulation corresponds to the maximum-likelihood value of $M_W$ and includes backgrounds (shaded). The likelihood is computed using events between the two arrows.
001624473 8564_ $$82206839$$s10138$$uhttp://cds.cern.ch/record/1624473/files/zeSigmaXiBalancevsPt1_dataMC.png$$y00054 Resolution on $0.65 p^{\ell\ell}_{\eta} + u_{\eta}$ (left) and $0.65 p^{\ell\ell}_{\xi} + u_{\xi}$ (right) in simulated (lines) and data (circles) $Z$-boson decays to muons (top) and electrons (bottom). The sum of the $\chi^2$ values in the $\xi$ or $\eta$ direction is minimized in the fit for the jet angular resolution parameters or the recoil resolution parameters ($N_{W,Z}$ and $s_\mathrm{had}$), respectively.
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