Measurement of the top quark mass in the all-hadronic mode at CDF
A measurement of the top quark mass (M top) in the all-hadronic decay channel is presented. It uses 5.8 fb -1 of pp data collected with the CDF II detector at the Fermilab Tevatron Collider. Events with six to eight jets are selected by a neural network algorithm and by the requirement that at least...
Hoofdauteurs: | , , , , , , , , , , , , , , , , , , , , , , , , |
---|---|
Formaat: | Journal article |
Taal: | English |
Gepubliceerd in: |
2012
|
_version_ | 1826286653672521728 |
---|---|
author | Aaltonen, T Álvarez González, B Amerio, S Amidei, D Anastassov, A Annovi, A Antos, J Apollinari, G Appel, J Arisawa, T Artikov, A Asaadi, J Ashmanskas, W Auerbach, B Aurisano, A Azfar, F Badgett, W Bae, T Barbaro-Galtieri, A Barnes, V Barnett, B Barria, P Bartos, P Bauce, M Bedeschi, F |
author_facet | Aaltonen, T Álvarez González, B Amerio, S Amidei, D Anastassov, A Annovi, A Antos, J Apollinari, G Appel, J Arisawa, T Artikov, A Asaadi, J Ashmanskas, W Auerbach, B Aurisano, A Azfar, F Badgett, W Bae, T Barbaro-Galtieri, A Barnes, V Barnett, B Barria, P Bartos, P Bauce, M Bedeschi, F |
author_sort | Aaltonen, T |
collection | OXFORD |
description | A measurement of the top quark mass (M top) in the all-hadronic decay channel is presented. It uses 5.8 fb -1 of pp data collected with the CDF II detector at the Fermilab Tevatron Collider. Events with six to eight jets are selected by a neural network algorithm and by the requirement that at least one of the jets is tagged as a b-quark jet. The measurement is performed with a likelihood fit technique, which simultaneously determines M top and the jet energy scale (JES) calibration. The fit yields a value of M top=172.5±1.4(stat)±1.0(JES)±1.1(syst) GeV/c 2. © 2012 Elsevier B.V. |
first_indexed | 2024-03-07T01:46:56Z |
format | Journal article |
id | oxford-uuid:98baa842-a155-44db-a62f-cece486d5034 |
institution | University of Oxford |
language | English |
last_indexed | 2024-03-07T01:46:56Z |
publishDate | 2012 |
record_format | dspace |
spelling | oxford-uuid:98baa842-a155-44db-a62f-cece486d50342022-03-27T00:09:10ZMeasurement of the top quark mass in the all-hadronic mode at CDFJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:98baa842-a155-44db-a62f-cece486d5034EnglishSymplectic Elements at Oxford2012Aaltonen, TÁlvarez González, BAmerio, SAmidei, DAnastassov, AAnnovi, AAntos, JApollinari, GAppel, JArisawa, TArtikov, AAsaadi, JAshmanskas, WAuerbach, BAurisano, AAzfar, FBadgett, WBae, TBarbaro-Galtieri, ABarnes, VBarnett, BBarria, PBartos, PBauce, MBedeschi, FA measurement of the top quark mass (M top) in the all-hadronic decay channel is presented. It uses 5.8 fb -1 of pp data collected with the CDF II detector at the Fermilab Tevatron Collider. Events with six to eight jets are selected by a neural network algorithm and by the requirement that at least one of the jets is tagged as a b-quark jet. The measurement is performed with a likelihood fit technique, which simultaneously determines M top and the jet energy scale (JES) calibration. The fit yields a value of M top=172.5±1.4(stat)±1.0(JES)±1.1(syst) GeV/c 2. © 2012 Elsevier B.V. |
spellingShingle | Aaltonen, T Álvarez González, B Amerio, S Amidei, D Anastassov, A Annovi, A Antos, J Apollinari, G Appel, J Arisawa, T Artikov, A Asaadi, J Ashmanskas, W Auerbach, B Aurisano, A Azfar, F Badgett, W Bae, T Barbaro-Galtieri, A Barnes, V Barnett, B Barria, P Bartos, P Bauce, M Bedeschi, F Measurement of the top quark mass in the all-hadronic mode at CDF |
title | Measurement of the top quark mass in the all-hadronic mode at CDF |
title_full | Measurement of the top quark mass in the all-hadronic mode at CDF |
title_fullStr | Measurement of the top quark mass in the all-hadronic mode at CDF |
title_full_unstemmed | Measurement of the top quark mass in the all-hadronic mode at CDF |
title_short | Measurement of the top quark mass in the all-hadronic mode at CDF |
title_sort | measurement of the top quark mass in the all hadronic mode at cdf |
work_keys_str_mv | AT aaltonent measurementofthetopquarkmassintheallhadronicmodeatcdf AT alvarezgonzalezb measurementofthetopquarkmassintheallhadronicmodeatcdf AT amerios measurementofthetopquarkmassintheallhadronicmodeatcdf AT amideid measurementofthetopquarkmassintheallhadronicmodeatcdf AT anastassova measurementofthetopquarkmassintheallhadronicmodeatcdf AT annovia measurementofthetopquarkmassintheallhadronicmodeatcdf AT antosj measurementofthetopquarkmassintheallhadronicmodeatcdf AT apollinarig measurementofthetopquarkmassintheallhadronicmodeatcdf AT appelj measurementofthetopquarkmassintheallhadronicmodeatcdf AT arisawat measurementofthetopquarkmassintheallhadronicmodeatcdf AT artikova measurementofthetopquarkmassintheallhadronicmodeatcdf AT asaadij measurementofthetopquarkmassintheallhadronicmodeatcdf AT ashmanskasw measurementofthetopquarkmassintheallhadronicmodeatcdf AT auerbachb measurementofthetopquarkmassintheallhadronicmodeatcdf AT aurisanoa measurementofthetopquarkmassintheallhadronicmodeatcdf AT azfarf measurementofthetopquarkmassintheallhadronicmodeatcdf AT badgettw measurementofthetopquarkmassintheallhadronicmodeatcdf AT baet measurementofthetopquarkmassintheallhadronicmodeatcdf AT barbarogaltieria measurementofthetopquarkmassintheallhadronicmodeatcdf AT barnesv measurementofthetopquarkmassintheallhadronicmodeatcdf AT barnettb measurementofthetopquarkmassintheallhadronicmodeatcdf AT barriap measurementofthetopquarkmassintheallhadronicmodeatcdf AT bartosp measurementofthetopquarkmassintheallhadronicmodeatcdf AT baucem measurementofthetopquarkmassintheallhadronicmodeatcdf AT bedeschif measurementofthetopquarkmassintheallhadronicmodeatcdf |