The 2019 High Energy and Particle Physics Prize of the EPS for an outstanding
contribution to High Energy Physics is awarded to the CDF and D0 Collaborations
for the discovery of the top quark and the detailed measurement of its properties.
The top quark is the heaviest elementary particle known to date and the only quark
whose mass of about 173 GeV resides at the electroweak symmetry breaking scale.
Its phenomenology is unique: being heavier than a W boson, it immediately decays
into a real W boson and a bottom quark after its creation and therefore does nothadronise into mesons or baryons. In addition, it is the only quark whose Yukawa
coupling to the Higgs boson is of the order of unity. For these reasons, an accurate
knowledge of its properties (mass, width, electroweak couplings, production crosssections, decay branching ratios) brings unique information on the fundamental
interactions at the electroweak breaking scale and beyond.
The existence of a third generation was proposed by Kobayashi and Maskawa in 1973
to allow for CP violation in the quark sector. The discovery of the bottom quark in 1977
then triggered the search for the top quark whose existence was required by theinternal consistency of the Standard Model of the weak and strong interactions. The
search for the top quark lasted for almost two decades, first at electron-positron
colliders, and then at higher energy hadron colliders. Lower limits on its mass fromdirect searches and precision electroweak measurements increased progressively
over the years.
In 1986 the Tevatron at the Fermilab National Accelerator Laboratory started colliding
protons and anti-protons at a centre-of-mass energy of 1.8 TeV. Evidence for a top
quark at a mass of 170-180 GeV was first reported [1] in 1994 by the CDF
collaboration. The announcement of the observation was given simultaneously by theCDF and D0 collaborations a year later, in 1995 [2,3]. A key aspect of the discovery
was the possibility of detecting two different final states, single-lepton and di-lepton,
and discriminating the signal from backgrounds using b-tagging and kinematicvariables.
With about 10 fb-1 of data per experiment collected during Run II at 1.96 TeV in 20012011, the CDF and D0 collaborations have determined the top quark key properties(e.g., its mass to better than 1%), measured the top quark pair production crosssection at the 10% level [4,5], and finally provided the first observation of the weak
production of a single top quark [6,7] in 2009.
CDF and D0 are worldwide collaborations which consist of about 400 scientists andtechnicians each, see https://www-cdf.fnal.gov/ and https://www-d0.fnal.gov/ .
[1] F. Abe et al. [CDF collaboration], Evidence for top quark production in protonantiproton collisions at √s = 1.8 TeV, Phys. Rev. Lett. 73 (1994) 225-231.
[2] F. Abe et al. [CDF collaboration], Observation of top quark production in protonantiproton collisions at √s = 1.8 TeV, Phys. Rev. Lett. 74 (1995) 2626-2631.

[3] S. Abachi et al. [D0 collaboration], Observation of the top quark, Phys. Rev. Lett.
74 (1995) 2632-2637.
[4] T. Aaltonen et al. [CDF collaboration], Measurement of the top-quark pair
production cross-section in events with two leptons and bottom-quark jets using thefull CDF data set, Phys. Rev. D88 (2013) 091103.
[5] V.M. Abazov et al. [D0 collaboration], Measurement of the inclusive top-antitop
production cross section in proton-antiproton collisions at √s=1.96 TeV anddetermination of the top quark pole mass, Phys. Rev. D94 (2016) 092004.
[6] T. Aaltonen et al. [CDF collaboration], First observation of electroweak single top
quark production, Phys. Rev. Lett. 103 (2009) 092002.
[7] V.M. Abazov et al. [D0 collaboration], Observation single top quark production,
Phys. Rev. Lett. 103 (2009) 092001.