Measurement of the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>W</mml:mi></mml:math>Boson Mass with the D0 Detector

Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M. R.; Adams, T.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Alverson, G.; Aoki, M.; Askew, A.; Sman, B.; Atkins, S.; Atramentov, O.; Augsten, K.; Ávila, C.; Badaud, F.; Bagby, L.; Baldin, B.; Bandurin, D. V.; Banerjee, S.; Barberis, E.; Baringer, P.; Barreto, J.; Bartlett, J. F.; Bassler, U.; Bazterra, V. E.; Bean, A.; Begalli, M.; Bélanger-Champagne, C.; Bellantoni, L.; Beri, S. B.; Bernardi, G.; Bernhard, R.; Bertram, I.; Besançon, M.; Beuselinck, R.; Bezzubov, V. A.; Bhat, P. C.; Bhatia, S.; Bhatnagar, V.; Blazey, G.; Blessing, S.; Bloom, K.; Boehnlein, A.; Boline, D.; Boos, E.; Borissov, G.; Bose, T.; Brandt, A.; Brandt, O.; Brock, R.; Brooijmans, G.; Bross, A.; Brown, D.; Brown, J.; Bu, X. B.; Buehler, M.; Buescher, V.; Bunichev, V.; Burdin, S.; Buszello, C. P.; Camacho-Pérez, E.; Casey, B. C.K.; Castilla‐Valdez, H.; Caughron, S.; Chakrabarti, S.; Chakraborty, D.; Chan, K. M.; Chandra, A.; Chapon, É.; Chen, G.; Chevalier-Théry, S.; Cho, D. K.; Cho, S. W.; Choi, S.; Choudhary, B. C.; Cihangir, S.; Claes, D. R.; Clutter, J.; Cooke, M.; Cooper, W. E.; Corcoran, M.; Couderc, F.; Cousinou, M. C.; Croc, A.; Ćutts, D.; Das, A.; Davies, G.; Jong, S. J. De; Cruz-Burelo, E. De La; Déliot, F.; Démina, R.; Denisov, D.; Denisov, S. P.; Desai, S.; Deterre, C.; Devaughan, K.; Diehl, H. T.; Diesburg, M.; Ding, P. F.; Dominguez, A.; Dorland, T.; Dubey, A.; Dudko, L.; Duggan, D.; Duperrin, A.; Dutt, S.; Dyshkant, A.; Eads, M.; Edmunds, D.; Ellison, J.; Elvira, V. D.; Enari, Y.; Evans, H.; Evdokimov, A.; Евдокимов, В. Н.; Facini, G.; Liu, Feng; Ferbel, T.; Fiedler, F.; Filthaut, F.; Fisher, W. C.; Fisk, H. E.; Fortner, M.; Fox, H.; Fuess, S.; García-Bellido, A.; García-Guerra, G. A.; Gavrilov, V.; Geng, W.; Gerbaudo, D.; Gerber, C. E.; Gershtein, Y.; Ginther, G.; Golovanov, G.; Goussiou, A. G.; Grannis, P. 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T.; Tschann-Grimm, K.; Tsybychev, D.; Tuchming, B.; Tully, C.; Uvarov, L.; Uvarov, S.; Uzunyan, S.; Kooten, R. Van; Leeuwen, W. M. Van; Varelas, N.; Varnes, E. W.; Vasilyev, I. A.; Verdier, P.; Verkheev, A. Y.; Vertogradov, L. S.; Verzocchi, M.; Vesterinen, M.; Vilanova, D.; Vokáč, P.; Wahl, H. D.; Wang, Michael; Warchol, J.; Watts, G.; Wayne, M.; Weichert, J.; Welty-Rieger, L.; White, A.; Wicke, D.; Williams, Mark Richard James; Wilson, G. W.; Wobisch, M.; Wood, D.; Wyatt, T. R.; Xie, Y.; Yacoob, S.; Yamada, R.; Yang, W. C.; Yasuda, T.; Yatsunenko, Y. A.; Ye, W.; Ye, Z.; Yin, H.; Yip, K.; Youn, S. W.; Zhao, T.; Zhou, B.; Zhu, J.; Zieliński, M.; Ziemińska, D.; Živković, L.

doi:10.1103/physrevlett.108.151804

Cited by 485 publications

(774 citation statements)

References 32 publications

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“…Recent measurements performed with the CDF [16] and D0 [17] experiments have improved the combined world measurement to M W ¼ 80385 AE 15 MeV=c 2 [18]. The CDF measurement, M W ¼ 80387 AE 19 MeV=c 2 [16], is described in this paper and is the most precise single measurement of the W-boson mass to date.…”

Section: 8mentioning

confidence: 94%

Precise measurement of theW-boson mass with the Collider Detector at Fermilab

Aaltonen¹,

Amerio²,

Amidei³

et al. 2014

Phys. Rev. D

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Section: 8mentioning

confidence: 94%

Precise measurement of theW-boson mass with the Collider Detector at Fermilab

Aaltonen¹,

Amerio²,

Amidei³

et al. 2014

Phys. Rev. D

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“…16 The status of electroweak precision observables did not change since then, except for the mass of the W boson. The latter was recently updated based on Tevatron results [99,100], and the new world average is now [101] m W = 80.385 ± 0.015 GeV. (C.…”

Section: Jhep10(2012)004mentioning

confidence: 99%

Higgs low-energy theorem (and its corrections) in composite models

Gillioz

Gröber

Grojean

et al. 2012

J. High Energ. Phys.

120

124

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The Higgs low-energy theorem gives a simple and elegant way to estimate the couplings of the Higgs boson to massless gluons and photons induced by loops of heavy particles. We extend this theorem to take into account possible nonlinear Higgs interactions as well as new states resulting from a strong dynamics at the origin of the breaking of the electroweak symmetry. We show that, while it approximates with an accuracy of order a few percents single Higgs production, it receives corrections of order 50% for double Higgs production. A full one-loop computation of the gg → hh cross section is explicitly performed in MCHM5, the minimal composite Higgs model based on the SO(5)/SO(4) coset with the Standard Model fermions embedded into the fundamental representation of SO(5). In particular we take into account the contributions of all fermionic resonances, which give sizeable (negative) corrections to the result obtained considering only the Higgs nonlinearities. Constraints from electroweak precision and flavor data on the top partners are analyzed in detail, as well as direct searches at the LHC for these new fermions called to play a crucial role in the electroweak symmetry breaking dynamics.

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“…Fermions acquire their masses via their interactions with the scalar field. Precision electroweak data, including the latest W boson and top-quark mass measurements at the CDF and D0 experiments at the Fermilab Tevatron Collider [5][6][7], constrain the mass of a SM Higgs boson to M H < 152 GeV [8] at 95% confidence level (C.L.). Direct searches at the ALEPH, DELPHI, L3, and OPAL experiments at the CERN e þ e À Collider (LEP) [9], the CDF and D0 experiments [10,11], and the ATLAS [12] and CMS [13] experiments at the CERN Large Hadron Collider (LHC) limit the SM Higgs boson mass to 122 GeV < M H < 127 GeV at 95% C.L.…”

Section: Introductionmentioning

confidence: 99%

Combined search for the Higgs boson with the D0 experiment

et al. 2013

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We perform a combination of searches for standard model Higgs boson production in p p collisions recorded by the D0 detector at the Fermilab Tevatron Collider at a center of mass energy of ffiffi ffi s p ¼ 1:96 TeV. The different production and decay channels have been analyzed separately, with integrated luminosities of up to 9:7 fb À1 and for Higgs boson masses 90 M H 200 GeV. We combine these final states to achieve optimal sensitivity to the production of the Higgs boson. We also interpret the combination in terms of models with a fourth generation of fermions, and models with suppressed Higgs boson couplings to fermions. The result excludes a standard model Higgs boson at 95% C.L. in the ranges 90 < M H < 101 GeV and 157 < M H < 178 GeV, with an expected exclusion of 155 < M H < 175 GeV. In the range 120 < M H < 145 GeV, the data exhibit an excess over the expected background of up to 2 standard deviations, consistent with the presence of a standard model Higgs boson of mass 125 GeV.

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Measurement of theWBoson Mass with the D0 Detector

Cited by 485 publications

References 32 publications

Precise measurement of theW-boson mass with the Collider Detector at Fermilab

Precise measurement of theW-boson mass with the Collider Detector at Fermilab

Higgs low-energy theorem (and its corrections) in composite models

Combined search for the Higgs boson with the D0 experiment

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