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[PDF] Top 20 Observation of $\mathrm{t\overline{t}}$H production

Has 10000 "Observation of $\mathrm{t\overline{t}}$H production" found on our website. Below are the top 20 most common "Observation of $\mathrm{t\overline{t}}$H production".

Observation of $\mathrm{t\overline{t}}$H production

Observation of $\mathrm{t\overline{t}}$H production

... S. Kyriacou, 174 A. Lath, 174 R. Montalvo, 174 K. Nash, 174 M. Osherson, 174 H. Saka, 174 S. Salur, 174 S. Schnetzer, 174 D. Sheffield, 174 S. Somalwar, 174 R. Stone, 174 S. Thomas, 174 P. Thomassen, 174 M. ... See full document

17

Combination of inclusive and differential $ \mathrm{t}\overline{\mathrm{t}} $ charge asymmetry measurements using ATLAS and CMS data at $ \sqrt{s}=7 $ and 8 TeV

Combination of inclusive and differential $ \mathrm{t}\overline{\mathrm{t}} $ charge asymmetry measurements using ATLAS and CMS data at $ \sqrt{s}=7 $ and 8 TeV

... D. Abbaneo, B. Akgun, E. Auffray, P. Baillon, A.H. Ball, D. Barney, J. Bendavid, M. Bianco, P. Bloch, A. Bocci, C. Botta, T. Camporesi, R. Castello, M. Cepeda, G. Cerminara, E. Chapon, Y. Chen, D. d’Enterria, A. ... See full document

65

Measurement of $\mathrm {t}\overline{\mathrm {t}}$ production with additional jet activity, including $\mathrm {b}$ quark jets, in the dilepton decay channel using pp collisions at $\sqrt{s} =$ 8 TeV

Measurement of $\mathrm {t}\overline{\mathrm {t}}$ production with additional jet activity, including $\mathrm {b}$ quark jets, in the dilepton decay channel using pp collisions at $\sqrt{s} =$ 8 TeV

... D. Abbaneo, E. Auffray, G. Auzinger, M. Bachtis, P. Baillon, A.H. Ball, D. Barney, A. Benaglia, J. Bendavid, L. Benhabib, J.F. Benitez, G.M. Berruti, P. Bloch, A. Bocci, A. Bonato, C. Botta, H. Breuker, T. ... See full document

78

Measurement of the $ t\overline{t}W $ and $ t\overline{t}Z $ production cross sections in pp collisions at $ \sqrt{s}=8 $ TeV with the ATLAS detector

Measurement of the $ t\overline{t}W $ and $ t\overline{t}Z $ production cross sections in pp collisions at $ \sqrt{s}=8 $ TeV with the ATLAS detector

... S. Jakobsen 30 , T. Jakoubek 127 , J. Jakubek 128 , D.O. Jamin 114 , D.K. Jana 79 , E. Jansen 78 , R. Jansky 62 , J. Janssen 21 , M. Janus 54 , G. Jarlskog 81 , N. Javadov 65,b , T. Jav˚urek 48 , L. Jeanty ... See full document

47

Measurement of normalized differential $ \mathrm{t}\overline{\mathrm{t}} $ cross sections in the dilepton channel from pp collisions at $ \sqrt{s}=13 $ TeV

Measurement of normalized differential $ \mathrm{t}\overline{\mathrm{t}} $ cross sections in the dilepton channel from pp collisions at $ \sqrt{s}=13 $ TeV

... S. Abdullin, M. Albrow, G. Apollinari, A. Apresyan, A. Apyan, S. Banerjee, L.A.T. Bauerdick, A. Beretvas, J. Berryhill, P.C. Bhat, G. Bolla, K. Burkett, J.N. Butler, A. Canepa, H.W.K. Cheung, F. Chlebana, M. Cremonesi, ... See full document

46

Measurement of the $ t\overline{t} $ production cross-section as a function of jet multiplicity and jet transverse momentum in 7 TeV proton-proton collisions with the ATLAS detector

Measurement of the $ t\overline{t} $ production cross-section as a function of jet multiplicity and jet transverse momentum in 7 TeV proton-proton collisions with the ATLAS detector

... O. Bessidskaia 147a,147b , M.F. Bessner 42 , N. Besson 137 , C. Betancourt 48 , S. Bethke 100 , W. Bhimji 46 , R.M. Bianchi 124 , L. Bianchini 23 , M. Bianco 30 , O. Biebel 99 , S.P. Bieniek 77 , K. Bierwagen 54 , J. ... See full document

75

Measurement of the jet mass in highly boosted ${\mathrm{t}}\overline{\mathrm{t}}$ events from pp collisions at $\sqrt{s}=8$ $\,\text {TeV}$

Measurement of the jet mass in highly boosted ${\mathrm{t}}\overline{\mathrm{t}}$ events from pp collisions at $\sqrt{s}=8$ $\,\text {TeV}$

... D. Abbaneo, E. Auffray, G. Auzinger, P. Baillon, A.H. Ball, D. Barney, P. Bloch, A. Bocci, C. Botta, T. Camporesi, R. Castello, M. Cepeda, G. Cerminara, Y. Chen, D. d’Enterria, A. Dabrowski, V. Daponte, A. David, ... See full document

44

Measurements of the $\mathrm{t}\overline{\mathrm{t}}$ production cross section in lepton+jets final states in pp collisions at 8 $\,\text {TeV}$ and ratio of 8 to 7  $\,\text {TeV}$ cross sections

Measurements of the $\mathrm{t}\overline{\mathrm{t}}$ production cross section in lepton+jets final states in pp collisions at 8 $\,\text {TeV}$ and ratio of 8 to 7  $\,\text {TeV}$ cross sections

... consist of semileptonic heavy-flavour decays and, in the elec- tron channel, events in which pions in jets are misidentified as ...shape of the accepted multijet background is extracted from a sideband data ... See full document

40

Search for MSSM H$^+$ bosons decaying into $H^+ \to \tau^+ \nu_{\tau}$ and $H^+ \to t\overline{b}$ with l+$\tau( \to had)$ and dilepton final states

Search for MSSM H$^+$ bosons decaying into $H^+ \to \tau^+ \nu_{\tau}$ and $H^+ \to t\overline{b}$ with l+$\tau( \to had)$ and dilepton final states

... extension of the SM (MSSM) [3], the Higgs sector contains five particles: three neutral (the CP-even h 0 and H 0 , the CP-odd A 0 ) and two charged (H ± ) Higgs ...detection of a ... See full document

12

Measurement of the inclusive $ \mathrm{t}\overline{\mathrm{t}} $ cross section in pp collisions at $ \sqrt{s}=5.02 $ TeV using final states with at least one charged lepton

Measurement of the inclusive $ \mathrm{t}\overline{\mathrm{t}} $ cross section in pp collisions at $ \sqrt{s}=5.02 $ TeV using final states with at least one charged lepton

... means of a ...behavior of the light jets produced from the W boson hadronic decay in a tt ...during production, they are also expected to be closer in phase space when compared to pairs of ... See full document

42

Search for $ \mathrm{t}\overline{\mathrm{t}} $ resonances in highly boosted lepton+jets and fully hadronic final states in proton-proton collisions at $ \sqrt{s}=13 $ TeV

Search for $ \mathrm{t}\overline{\mathrm{t}} $ resonances in highly boosted lepton+jets and fully hadronic final states in proton-proton collisions at $ \sqrt{s}=13 $ TeV

... resonant production cross sections, are shown in ...combination of the lepton+jets and fully hadronic channels significantly improves the exclusion limits relative to previous results for all models, except ... See full document

44

Measurement of the $\mathrm{t}\overline{{\mathrm{t}}}$ production cross section in the all-jets final state in pp collisions at $\sqrt{s}=8$ $\,\text {TeV}$

Measurement of the $\mathrm{t}\overline{{\mathrm{t}}}$ production cross section in the all-jets final state in pp collisions at $\sqrt{s}=8$ $\,\text {TeV}$

... simulation of up to three additional partons. The value of the top quark mass is set to m t = ...matching of matrix element jets to those from parton ...counting of the radiative ... See full document

36

Measurement of jet multiplicity distributions in $\mathrm {t}\overline{\mathrm {t}}$ production in pp collisions at $\sqrt{s} = 7\,\text {TeV} $

Measurement of jet multiplicity distributions in $\mathrm {t}\overline{\mathrm {t}}$ production in pp collisions at $\sqrt{s} = 7\,\text {TeV} $

... tt production cross section as a function of the jet multiplicity is measured from the number of signal events after background subtraction and correction for the detector efficiencies and ...number ... See full document

41

Measurement of the $ t\overline{t}\gamma $ production cross section in proton-proton collisions at $ \sqrt{s}=8 $ TeV with the ATLAS detector

Measurement of the $ t\overline{t}\gamma $ production cross section in proton-proton collisions at $ \sqrt{s}=8 $ TeV with the ATLAS detector

... T. Klapdor-Kleingrothaus 51 , M.H. Klein 38 , M. Klein 77 , U. Klein 77 , K. Kleinknecht 86 , P. Klimek 110 , A. Klimentov 27 , R. Klingenberg 46 , T. Klingl 23 , T. Klioutchnikova 32 , E.-E. Kluge ... See full document

42

Angular distributions in $t \overline{t}H(H → b \overline{b})$ reconstructed events at the LHC

Angular distributions in $t \overline{t}H(H → b \overline{b})$ reconstructed events at the LHC

... discovery of a scalar particle at CERN’s Large Hadron Collider ...mass of about 125 GeV was later identified as the Higgs boson, responsible for the generation of all particle masses through the ... See full document

12

Search for $\mathrm{t}\overline{\mathrm{t}}$H production in the all-jet final state in proton-proton collisions at $\sqrt{s}=$ 13 TeV

Search for $\mathrm{t}\overline{\mathrm{t}}$H production in the all-jet final state in proton-proton collisions at $\sqrt{s}=$ 13 TeV

... number of simulated background and signal events leads to statistical fluctuations in the nom- inal ...bin of each sample that can be changed by its uncertainty as described in ...sources of ... See full document

44

Measurement of the semileptonic $ \mathrm{t}\overline{\mathrm{t}} $ + γ production cross section in pp collisions at $ \sqrt{s}=8 $ TeV

Measurement of the semileptonic $ \mathrm{t}\overline{\mathrm{t}} $ + γ production cross section in pp collisions at $ \sqrt{s}=8 $ TeV

... mance of the LHC and thank the technical and administrative staffs at CERN and at other CMS institutes for their contributions to the success of the CMS ...personnel of the Worldwide LHC Computing ... See full document

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Identidade como Territorialidade em t r a b a l h o s d e a r t e c o n t e m p o r â n e a

Identidade como Territorialidade em t r a b a l h o s d e a r t e c o n t e m p o r â n e a

... Apesar das tentativas dos artistas em driblar o problema mercadológico, ou seja, escapar do enlace entre obra de arte e mercadoria para consumo, tem havido uma estranha reversão no pro[r] ... See full document

102

C H A R A C T E R I Z A T I O N OF PESTICIDE CONSUMPTION IN T H E C O U N T Y OF S A N T A R É M , PARÁ, B R A Z I L

C H A R A C T E R I Z A T I O N OF PESTICIDE CONSUMPTION IN T H E C O U N T Y OF S A N T A R É M , PARÁ, B R A Z I L

... Information compiled in this study was collected by survey. The qualita­ tive part of the study was conducted between January and March 1997 and between August and October 1998. Oral[r] ... See full document

14

Measurements of b-jet tagging efficiency with the ATLAS detector using $ t\overline{t} $ events at $ \sqrt{s}=13 $ TeV

Measurements of b-jet tagging efficiency with the ATLAS detector using $ t\overline{t} $ events at $ \sqrt{s}=13 $ TeV

... E. Valdes Santurio 43a,43b , M. Valente 52 , S. Valentinetti 23b,23a , A. Valero 171 , L. Valéry 44 , R.A. Vallance 21 , A. Vallier 5 , J.A. Valls Ferrer 171 , T.R. Van Daalen 14 , W. Van Den Wollenberg 118 , H. ... See full document

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