Measurement of the top-quark mass in the all-hadronic channel using the full CDF data set
The top-quark mass M sub(top) is measured using top quark-antiquark pairs produced in proton-antiproton collisions at a center-of-mass energy of 1.96 TeV and that decay into a fully hadronic final state. The full data set collected with the CDF II detector at the Fermilab Tevatron Collider, correspo...
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| Veröffentlicht in: | Physical review. D, Particles, fields, gravitation, and cosmology Particles, fields, gravitation, and cosmology, 2014-11, Vol.90 (9), Article 091101 |
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| creator | Aaltonen, T. Amerio, S. Amidei, D. Anastassov, A. Annovi, A. Antos, J. Apollinari, G. Appel, J. A. Arisawa, T. Artikov, A. Asaadi, J. Ashmanskas, W. Auerbach, B. Aurisano, A. Azfar, F. Badgett, W. Bae, T. Barbaro-Galtieri, A. Barnes, V. E. Barnett, B. A. Barria, P. Bartos, P. Bauce, M. Bedeschi, F. Behari, S. Bellettini, G. Bellinger, J. Benjamin, D. Beretvas, A. Bhatti, A. Bland, K. R. Blumenfeld, B. Bocci, A. Bodek, A. Bortoletto, D. Boudreau, J. Boveia, A. Brigliadori, L. Bromberg, C. Brucken, E. Budagov, J. Budd, H. S. Burkett, K. Busetto, G. Bussey, P. Butti, P. Buzatu, A. Calamba, A. Camarda, S. Campanelli, M. Canelli, F. Carls, B. Carlsmith, D. Carosi, R. Carrillo, S. Casal, B. Casarsa, M. Castro, A. Catastini, P. Cauz, D. Cavaliere, V. Cerri, A. Cerrito, L. Chen, Y. C. Chertok, M. Chiarelli, G. Chlachidze, G. Cho, K. Chokheli, D. Clark, A. Clarke, C. Convery, M. E. Conway, J. Corbo, M. Cordelli, M. Cox, C. A. Cox, D. J. Cremonesi, M. Cruz, D. Cuevas, J. Culbertson, R. d’Ascenzo, N. Datta, M. de Barbaro, P. Demortier, L. Deninno, M. D’Errico, M. Devoto, F. Di Canto, A. Di Ruzza, B. Dittmann, J. R. Donati, S. D’Onofrio, M. Dorigo, M. Driutti, A. Ebina, K. Edgar, R. Elagin, A. Erbacher, R. Errede, S. |
| description | The top-quark mass M sub(top) is measured using top quark-antiquark pairs produced in proton-antiproton collisions at a center-of-mass energy of 1.96 TeV and that decay into a fully hadronic final state. The full data set collected with the CDF II detector at the Fermilab Tevatron Collider, corresponding to an integrated luminosity of 9.3 fb super(-1), is used. Events are selected that have six to eight jets, at least one of which is identified as having originated from a b quark. In addition, a multivariate algorithm, containing multiple kinematic variables as inputs, is used to discriminate signal events from background events due to QCD multijet production. Templates for the reconstructed top-quark mass are combined in a likelihood fit to measure M sub(top) with a simultaneous calibration of the jet energy scale. A value of M sub(top) = 175.07 + or - 1.19(stat) (ProQuest: Formulae and/or non-USASCII text omitted)(syst) GeV /c super(2) is obtained for the top-quark mass. |
| doi_str_mv | 10.1103/PhysRevD.90.091101 |
| format | Article |
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A. ; Arisawa, T. ; Artikov, A. ; Asaadi, J. ; Ashmanskas, W. ; Auerbach, B. ; Aurisano, A. ; Azfar, F. ; Badgett, W. ; Bae, T. ; Barbaro-Galtieri, A. ; Barnes, V. E. ; Barnett, B. A. ; Barria, P. ; Bartos, P. ; Bauce, M. ; Bedeschi, F. ; Behari, S. ; Bellettini, G. ; Bellinger, J. ; Benjamin, D. ; Beretvas, A. ; Bhatti, A. ; Bland, K. R. ; Blumenfeld, B. ; Bocci, A. ; Bodek, A. ; Bortoletto, D. ; Boudreau, J. ; Boveia, A. ; Brigliadori, L. ; Bromberg, C. ; Brucken, E. ; Budagov, J. ; Budd, H. S. ; Burkett, K. ; Busetto, G. ; Bussey, P. ; Butti, P. ; Buzatu, A. ; Calamba, A. ; Camarda, S. ; Campanelli, M. ; Canelli, F. ; Carls, B. ; Carlsmith, D. ; Carosi, R. ; Carrillo, S. ; Casal, B. ; Casarsa, M. ; Castro, A. ; Catastini, P. ; Cauz, D. ; Cavaliere, V. ; Cerri, A. ; Cerrito, L. ; Chen, Y. C. ; Chertok, M. ; Chiarelli, G. ; Chlachidze, G. ; Cho, K. ; Chokheli, D. ; Clark, A. ; Clarke, C. ; Convery, M. E. ; Conway, J. ; Corbo, M. ; Cordelli, M. ; Cox, C. A. ; Cox, D. J. ; Cremonesi, M. ; Cruz, D. ; Cuevas, J. ; Culbertson, R. ; d’Ascenzo, N. ; Datta, M. ; de Barbaro, P. ; Demortier, L. ; Deninno, M. ; D’Errico, M. ; Devoto, F. ; Di Canto, A. ; Di Ruzza, B. ; Dittmann, J. R. ; Donati, S. ; D’Onofrio, M. ; Dorigo, M. ; Driutti, A. ; Ebina, K. ; Edgar, R. ; Elagin, A. ; Erbacher, R. ; Errede, S.</creator><creatorcontrib>Aaltonen, T. ; Amerio, S. ; Amidei, D. ; Anastassov, A. ; Annovi, A. ; Antos, J. ; Apollinari, G. ; Appel, J. A. ; Arisawa, T. ; Artikov, A. ; Asaadi, J. ; Ashmanskas, W. ; Auerbach, B. ; Aurisano, A. ; Azfar, F. ; Badgett, W. ; Bae, T. ; Barbaro-Galtieri, A. ; Barnes, V. E. ; Barnett, B. A. ; Barria, P. ; Bartos, P. ; Bauce, M. ; Bedeschi, F. ; Behari, S. ; Bellettini, G. ; Bellinger, J. ; Benjamin, D. ; Beretvas, A. ; Bhatti, A. ; Bland, K. R. ; Blumenfeld, B. ; Bocci, A. ; Bodek, A. ; Bortoletto, D. ; Boudreau, J. ; Boveia, A. ; Brigliadori, L. ; Bromberg, C. ; Brucken, E. ; Budagov, J. ; Budd, H. S. ; Burkett, K. ; Busetto, G. ; Bussey, P. ; Butti, P. ; Buzatu, A. ; Calamba, A. ; Camarda, S. ; Campanelli, M. ; Canelli, F. ; Carls, B. ; Carlsmith, D. ; Carosi, R. ; Carrillo, S. ; Casal, B. ; Casarsa, M. ; Castro, A. ; Catastini, P. ; Cauz, D. ; Cavaliere, V. ; Cerri, A. ; Cerrito, L. ; Chen, Y. C. ; Chertok, M. ; Chiarelli, G. ; Chlachidze, G. ; Cho, K. ; Chokheli, D. ; Clark, A. ; Clarke, C. ; Convery, M. E. ; Conway, J. ; Corbo, M. ; Cordelli, M. ; Cox, C. A. ; Cox, D. J. ; Cremonesi, M. ; Cruz, D. ; Cuevas, J. ; Culbertson, R. ; d’Ascenzo, N. ; Datta, M. ; de Barbaro, P. ; Demortier, L. ; Deninno, M. ; D’Errico, M. ; Devoto, F. ; Di Canto, A. ; Di Ruzza, B. ; Dittmann, J. R. ; Donati, S. ; D’Onofrio, M. ; Dorigo, M. ; Driutti, A. ; Ebina, K. ; Edgar, R. ; Elagin, A. ; Erbacher, R. ; Errede, S. ; CDF Collaboration</creatorcontrib><description>The top-quark mass M sub(top) is measured using top quark-antiquark pairs produced in proton-antiproton collisions at a center-of-mass energy of 1.96 TeV and that decay into a fully hadronic final state. The full data set collected with the CDF II detector at the Fermilab Tevatron Collider, corresponding to an integrated luminosity of 9.3 fb super(-1), is used. Events are selected that have six to eight jets, at least one of which is identified as having originated from a b quark. In addition, a multivariate algorithm, containing multiple kinematic variables as inputs, is used to discriminate signal events from background events due to QCD multijet production. Templates for the reconstructed top-quark mass are combined in a likelihood fit to measure M sub(top) with a simultaneous calibration of the jet energy scale. A value of M sub(top) = 175.07 + or - 1.19(stat) (ProQuest: Formulae and/or non-USASCII text omitted)(syst) GeV /c super(2) is obtained for the top-quark mass.</description><identifier>ISSN: 1550-7998</identifier><identifier>EISSN: 1550-2368</identifier><identifier>DOI: 10.1103/PhysRevD.90.091101</identifier><language>eng</language><publisher>United States: American Physical Society</publisher><subject>Calibration ; Channels ; Cosmology ; Decay ; Energy measurement ; Gravitation ; Jets ; Texts</subject><ispartof>Physical review. 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R.</creatorcontrib><creatorcontrib>Donati, S.</creatorcontrib><creatorcontrib>D’Onofrio, M.</creatorcontrib><creatorcontrib>Dorigo, M.</creatorcontrib><creatorcontrib>Driutti, A.</creatorcontrib><creatorcontrib>Ebina, K.</creatorcontrib><creatorcontrib>Edgar, R.</creatorcontrib><creatorcontrib>Elagin, A.</creatorcontrib><creatorcontrib>Erbacher, R.</creatorcontrib><creatorcontrib>Errede, S.</creatorcontrib><creatorcontrib>CDF Collaboration</creatorcontrib><title>Measurement of the top-quark mass in the all-hadronic channel using the full CDF data set</title><title>Physical review. D, Particles, fields, gravitation, and cosmology</title><description>The top-quark mass M sub(top) is measured using top quark-antiquark pairs produced in proton-antiproton collisions at a center-of-mass energy of 1.96 TeV and that decay into a fully hadronic final state. The full data set collected with the CDF II detector at the Fermilab Tevatron Collider, corresponding to an integrated luminosity of 9.3 fb super(-1), is used. Events are selected that have six to eight jets, at least one of which is identified as having originated from a b quark. In addition, a multivariate algorithm, containing multiple kinematic variables as inputs, is used to discriminate signal events from background events due to QCD multijet production. Templates for the reconstructed top-quark mass are combined in a likelihood fit to measure M sub(top) with a simultaneous calibration of the jet energy scale. A value of M sub(top) = 175.07 + or - 1.19(stat) (ProQuest: Formulae and/or non-USASCII text omitted)(syst) GeV /c super(2) is obtained for the top-quark mass.</description><subject>Calibration</subject><subject>Channels</subject><subject>Cosmology</subject><subject>Decay</subject><subject>Energy measurement</subject><subject>Gravitation</subject><subject>Jets</subject><subject>Texts</subject><issn>1550-7998</issn><issn>1550-2368</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2014</creationdate><recordtype>article</recordtype><recordid>eNo1kLFOwzAQhi0EEqXwAkwWE0uKnYtje0QtBaQiEIKByXIdmwTcpLUdpL49bQPTnf779Ov0IXRJyYRSAjcv9Ta-2p_ZRJIJkbuIHqERZYxkOZTi-G_nUopTdBbjFyGQl5yP0MeT1bEPdmXbhDuHU21x6tbZptfhG690jLhpD6n2Pqt1Fbq2MdjUum2tx31s2s_D2fXe4-lsjiudNI42naMTp320F39zjN7nd2_Th2zxfP84vV1kpmCQslyyJScOCm5BVpAvtSmXhlDJQDjJORRlVQEtJSdcABVgnS6IcEJUzLGKwRhdDb1dTI2KpknW1KbbvWeSolTQvaAxuh6gdeg2vY1JrZporPe6tV0fFeVUSOBQ7tF8QE3oYgzWqXVoVjpsFSVq36X-ZStJ1CAbfgEcdnJo</recordid><startdate>20141118</startdate><enddate>20141118</enddate><creator>Aaltonen, T.</creator><creator>Amerio, S.</creator><creator>Amidei, D.</creator><creator>Anastassov, A.</creator><creator>Annovi, A.</creator><creator>Antos, J.</creator><creator>Apollinari, G.</creator><creator>Appel, J. 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A. ; Barria, P. ; Bartos, P. ; Bauce, M. ; Bedeschi, F. ; Behari, S. ; Bellettini, G. ; Bellinger, J. ; Benjamin, D. ; Beretvas, A. ; Bhatti, A. ; Bland, K. R. ; Blumenfeld, B. ; Bocci, A. ; Bodek, A. ; Bortoletto, D. ; Boudreau, J. ; Boveia, A. ; Brigliadori, L. ; Bromberg, C. ; Brucken, E. ; Budagov, J. ; Budd, H. S. ; Burkett, K. ; Busetto, G. ; Bussey, P. ; Butti, P. ; Buzatu, A. ; Calamba, A. ; Camarda, S. ; Campanelli, M. ; Canelli, F. ; Carls, B. ; Carlsmith, D. ; Carosi, R. ; Carrillo, S. ; Casal, B. ; Casarsa, M. ; Castro, A. ; Catastini, P. ; Cauz, D. ; Cavaliere, V. ; Cerri, A. ; Cerrito, L. ; Chen, Y. C. ; Chertok, M. ; Chiarelli, G. ; Chlachidze, G. ; Cho, K. ; Chokheli, D. ; Clark, A. ; Clarke, C. ; Convery, M. E. ; Conway, J. ; Corbo, M. ; Cordelli, M. ; Cox, C. A. ; Cox, D. J. ; Cremonesi, M. ; Cruz, D. ; Cuevas, J. ; Culbertson, R. ; d’Ascenzo, N. ; Datta, M. ; de Barbaro, P. ; Demortier, L. ; Deninno, M. ; D’Errico, M. ; Devoto, F. ; Di Canto, A. ; Di Ruzza, B. ; Dittmann, J. R. ; Donati, S. ; D’Onofrio, M. ; Dorigo, M. ; Driutti, A. ; Ebina, K. ; Edgar, R. ; Elagin, A. ; Erbacher, R. ; Errede, S.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c453t-295b70f347e39d32bac6bc019538f977346dd316970783183efa408f88d5f5d53</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2014</creationdate><topic>Calibration</topic><topic>Channels</topic><topic>Cosmology</topic><topic>Decay</topic><topic>Energy measurement</topic><topic>Gravitation</topic><topic>Jets</topic><topic>Texts</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Aaltonen, T.</creatorcontrib><creatorcontrib>Amerio, S.</creatorcontrib><creatorcontrib>Amidei, D.</creatorcontrib><creatorcontrib>Anastassov, A.</creatorcontrib><creatorcontrib>Annovi, A.</creatorcontrib><creatorcontrib>Antos, J.</creatorcontrib><creatorcontrib>Apollinari, G.</creatorcontrib><creatorcontrib>Appel, J. 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D, Particles, fields, gravitation, and cosmology</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Aaltonen, T.</au><au>Amerio, S.</au><au>Amidei, D.</au><au>Anastassov, A.</au><au>Annovi, A.</au><au>Antos, J.</au><au>Apollinari, G.</au><au>Appel, J. A.</au><au>Arisawa, T.</au><au>Artikov, A.</au><au>Asaadi, J.</au><au>Ashmanskas, W.</au><au>Auerbach, B.</au><au>Aurisano, A.</au><au>Azfar, F.</au><au>Badgett, W.</au><au>Bae, T.</au><au>Barbaro-Galtieri, A.</au><au>Barnes, V. E.</au><au>Barnett, B. A.</au><au>Barria, P.</au><au>Bartos, P.</au><au>Bauce, M.</au><au>Bedeschi, F.</au><au>Behari, S.</au><au>Bellettini, G.</au><au>Bellinger, J.</au><au>Benjamin, D.</au><au>Beretvas, A.</au><au>Bhatti, A.</au><au>Bland, K. R.</au><au>Blumenfeld, B.</au><au>Bocci, A.</au><au>Bodek, A.</au><au>Bortoletto, D.</au><au>Boudreau, J.</au><au>Boveia, A.</au><au>Brigliadori, L.</au><au>Bromberg, C.</au><au>Brucken, E.</au><au>Budagov, J.</au><au>Budd, H. S.</au><au>Burkett, K.</au><au>Busetto, G.</au><au>Bussey, P.</au><au>Butti, P.</au><au>Buzatu, A.</au><au>Calamba, A.</au><au>Camarda, S.</au><au>Campanelli, M.</au><au>Canelli, F.</au><au>Carls, B.</au><au>Carlsmith, D.</au><au>Carosi, R.</au><au>Carrillo, S.</au><au>Casal, B.</au><au>Casarsa, M.</au><au>Castro, A.</au><au>Catastini, P.</au><au>Cauz, D.</au><au>Cavaliere, V.</au><au>Cerri, A.</au><au>Cerrito, L.</au><au>Chen, Y. C.</au><au>Chertok, M.</au><au>Chiarelli, G.</au><au>Chlachidze, G.</au><au>Cho, K.</au><au>Chokheli, D.</au><au>Clark, A.</au><au>Clarke, C.</au><au>Convery, M. E.</au><au>Conway, J.</au><au>Corbo, M.</au><au>Cordelli, M.</au><au>Cox, C. A.</au><au>Cox, D. J.</au><au>Cremonesi, M.</au><au>Cruz, D.</au><au>Cuevas, J.</au><au>Culbertson, R.</au><au>d’Ascenzo, N.</au><au>Datta, M.</au><au>de Barbaro, P.</au><au>Demortier, L.</au><au>Deninno, M.</au><au>D’Errico, M.</au><au>Devoto, F.</au><au>Di Canto, A.</au><au>Di Ruzza, B.</au><au>Dittmann, J. R.</au><au>Donati, S.</au><au>D’Onofrio, M.</au><au>Dorigo, M.</au><au>Driutti, A.</au><au>Ebina, K.</au><au>Edgar, R.</au><au>Elagin, A.</au><au>Erbacher, R.</au><au>Errede, S.</au><aucorp>CDF Collaboration</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Measurement of the top-quark mass in the all-hadronic channel using the full CDF data set</atitle><jtitle>Physical review. D, Particles, fields, gravitation, and cosmology</jtitle><date>2014-11-18</date><risdate>2014</risdate><volume>90</volume><issue>9</issue><artnum>091101</artnum><issn>1550-7998</issn><eissn>1550-2368</eissn><abstract>The top-quark mass M sub(top) is measured using top quark-antiquark pairs produced in proton-antiproton collisions at a center-of-mass energy of 1.96 TeV and that decay into a fully hadronic final state. The full data set collected with the CDF II detector at the Fermilab Tevatron Collider, corresponding to an integrated luminosity of 9.3 fb super(-1), is used. Events are selected that have six to eight jets, at least one of which is identified as having originated from a b quark. In addition, a multivariate algorithm, containing multiple kinematic variables as inputs, is used to discriminate signal events from background events due to QCD multijet production. Templates for the reconstructed top-quark mass are combined in a likelihood fit to measure M sub(top) with a simultaneous calibration of the jet energy scale. A value of M sub(top) = 175.07 + or - 1.19(stat) (ProQuest: Formulae and/or non-USASCII text omitted)(syst) GeV /c super(2) is obtained for the top-quark mass.</abstract><cop>United States</cop><pub>American Physical Society</pub><doi>10.1103/PhysRevD.90.091101</doi><oa>free_for_read</oa></addata></record> |
| fulltext | fulltext |
| identifier | ISSN: 1550-7998 |
| ispartof | Physical review. D, Particles, fields, gravitation, and cosmology, 2014-11, Vol.90 (9), Article 091101 |
| issn | 1550-7998 1550-2368 |
| language | eng |
| recordid | cdi_osti_scitechconnect_1181110 |
| source | American Physical Society Journals |
| subjects | Calibration Channels Cosmology Decay Energy measurement Gravitation Jets Texts |
| title | Measurement of the top-quark mass in the all-hadronic channel using the full CDF data set |
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