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Abulencia, A.; Adelman, J.; Affolder, A. A.; Akimoto, T.; Albrow, M.; Ambrose, D.; Amerio, S.; Amidei, D.; Anastassov, A.; Anikeev, K.; Annovi, A.; Antos̆, J.; Aoki, M.; Apollinari, G.; Arguin, J-F.; Arisawa, T.; Artikov, A.; Ashmanskas, W.; Attal, A.; Azfar, F.; Azzi-Bacchetta, P.; Azzurri, P.; Bacchetta, N.; Badgett, W.; Barbaro‐Galtieri, A.; Barnes, V. E.; Barnett, B. A.; Baroiant, S.; Bartsch, V.; Bauer, G.; Bedeschi, F.; Behari, S.; Belforte, S.; Bellettini, G.; Bellinger, J.; Belloni, A.; Benjamin, D.; Beretvas, A.; Beringer, J.; Berry, T.; Bhatti, A.; Binkley, M.; Bisello, D.; Blair, R. E.; Blocker, C.; Blumenfeld, B.; Bocci, A.; Bodek, A.; Boisvert, V.; Bolla, G.; Bolshov, A.; Bortoletto, D.; Boudreau, J.; Boveia, A.; Brau, B.; Brigliadori, L.; Bromberg, C.; Brubaker, E.; Budagov, J.; Budd, H. S.; Budd, S.; Budroni, S.; Burkett, K.; Busetto, G.; Bussey, P.; Byrum, K. 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Van; Varganov, A.; Vataga, E.; Vázquez, F.; Velev, G.; Veramendi, G.; Veszprémi, V.; Vidal, R.; Vila, I.; Vilar, R.; Vine, T.; Vollrath, I.; Volobouev, I.; Volpi, G.; Würthwein, F.; Wagner, P.; Wagner, R. G.; Wagner, R. L.; Wagner, J.; Wagner, W.; Wallny, R.; Wang, S. M.; Warburton, A.; Waschke, S.; Waters, D.; Weinberger, M.; Wester, W. C.; Whitehouse, B.; Whiteson, D.; Wicklund, A. B.; Wicklund, E.; Williams, G.; Williams, H. H.; Wilson, P.; Winer, B. L.; Wittich, P.; Wolbers, S.; Wolfe, C.; Wright, T.; Wu, X.; Wynne, S. M.; Yagil, A.; Yamamoto, K.; Yamaoka, J.; Yamashita, T.; Yang, C.; Yang, U. K.; Yang, Y. C.; Yao, W-M.; Yeh, G. P.; Yoh, J.; Yorita, K.; Yoshida, T.; Yu, G. B.; Yu, I.; Yu, S. S.; Yun, J. C.; Zanello, L.; Zanetti, A.; Zaw, I.; Zhang, X.; Zhou, J.; Zucchelli, S.

doi:10.1103/physrevd.75.032003

Cited by 9 publications

(3 citation statements)

References 50 publications

Supporting

Mentioning

Contrasting

Order By: Relevance

“…1 by means of the χ 2 -profiles obtained in the variants of the ABM11 fit with α s c The twist-6 terms were also checked in the fit and found comparable to zero within errors applying the cut of Q 2 > 2.5 GeV 2 used in the present analysis. [4] in comparison to the ones obtained by JR [12], CTEQ [13], MSTW [14], and NNPDF [15] from the analysis of the DIS data (squares) and from the combination of the DIS and jet Tevatron data [16,17] (circles).…”

Section: Strong Coupling Constantmentioning

confidence: 99%

DETERMINATION OF α_s AND m_c IN DEEP-INELASTIC SCATTERING

2013

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We describe the determination of the strong coupling constant αs(M 2 Z ) and of the charm-quark mass mc(mc) in the MS-scheme, based on the QCD analysis of the unpolarized World deep-inelastic scattering data. At NNLO the values of αs(M 2 Z ) = 0.1134 ± 0.0011(exp) and mc(mc) = 1.24 ± 0.03(exp) +0.03 −0.02 (scale) +0.00 −0.07 (th) are obtained and are compared with other determinations, also clarifying discrepancies.

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Section: Strong Coupling Constantmentioning

confidence: 99%

DETERMINATION OF α_s AND m_c IN DEEP-INELASTIC SCATTERING

2013

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“…The fourth technique, the Decay Length Method" [233,234] relies solely on tracking, and thus avoids the jet-energy scale uncertainty. This methods exploits the fact that, in the rest frame of the top quark, the boost given to the bottom quark has a Lorentz factor γ b ≈ 0.4 m t /m b .…”

Section: Lepton+jets Channelmentioning

confidence: 99%

“…Measurements that involve particles beyond the SM or the Higgs boson are covered in Section 9. The decay angle cos θ * has been used by both experiments in several analyses with increasing luminosity [278,279,280,281]. This observable requires the reconstruction of the full top pair decay kinematics to find the rest frame of the W boson that is needed to calculate cos θ * .…”

Section: Top-quark Production and Decay Propertiesmentioning

confidence: 99%

Status and prospects of top-quark physics

Incandela

Quadt

Wagner

et al. 2009

Progress in Particle and Nuclear Physics

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The top quark is the heaviest elementary particle observed to date. Its large mass of about 173 GeV/c 2 makes the top quark act differently than other elementary fermions, as it decays before it hadronises, passing its spin information on to its decay products. In addition, the top quark plays an important role in higher-order loop corrections to standard model processes, which makes the top quark mass a crucial parameter for precision tests of the electroweak theory. The top quark is also a powerful probe for new phenomena beyond the standard model. During the time of discovery at the Tevatron in 1995 only a few properties of the top quark could be measured. In recent years, since the start of Tevatron Run II, the field of top-quark physics has changed and entered a precision era. This report summarises the latest measurements and studies of top-quark properties and gives prospects for future measurements at the Large Hadron Collider (LHC).

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