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Related papers: Bs Physics at CDF and D0

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With the start of Run II at the Fermilab Tevatron a host of new physics opportunities are opened. In this paper we will review the prospects for physics at the CDF and \Dzero experiments. Topics ranging from QCD, to electro-weak precision…

High Energy Physics - Experiment · Physics 2014-11-17 Harold G. Evans

In Run II at the Tevatron, the major goal of the upgraded CDF and \dzero detectors is a Higgs search in the mass range of 110-200 GeV. They will also contribute significantly to B physics. Among many possibilities they will be able to…

High Energy Physics - Experiment · Physics 2007-05-23 Valentin E. Kuznetsov

We present the B physics results from the CDF and D{\O} experiments at the Tevatron Run II at Fermilab and their future prospect. This includes various B mass and lifetime measurements, B mixing, the confirmation of the discovery of the X…

High Energy Physics - Experiment · Physics 2007-05-23 Kin Yip

Both experiments CDF and D0 at the Tevatron collider have now the first samples of B_s particles where preliminary measurements are performed. The mass and lifetime measurements are presented and the yield for the hadronic B_s decays, the…

High Energy Physics - Experiment · Physics 2019-08-14 Donatella Lucchesi

The Tevatron Run-II program has been in progress since 2001, and the CDF and D0 experiments have been operational with upgraded detectors. Coupled with recent improvements in the Tevatron accelerator performance, the experiments have…

High Energy Physics - Experiment · Physics 2019-08-14 Fumihiko Ukegawa

After a five year upgrade period, the Fermilab experiments CDF and DO are taking high quality data in Run II of the Tevatron Collider. We report on the start-up of both detectors and present a selection of first B physics results from the…

High Energy Physics - Experiment · Physics 2019-08-14 Manfred Paulini

The B physics program planned for the D0 Upgrade Detector for Run 2 of the Tevatron is described. Current performance of the detector pertinent to B physics is presented and compared to expectations. Detection of b hadrons through…

High Energy Physics - Experiment · Physics 2019-08-14 R. Van Kooten

The Tevatron experiments, CDF and D0, have produced a wealth of new B-physics results since the start of Run II in 2001. We've observed new B-hadrons, seen new effects, and increased many-fold the precision with which we know the properties…

High Energy Physics - Experiment · Physics 2019-08-14 Harold G Evans

After a five year upgrade period, the CDF detector located at the Fermilab Tevatron Collider is back in operation taking high quality data with all subsystems functional. We report on the status of the CDF experiment in Run II and discuss…

High Energy Physics - Experiment · Physics 2010-04-22 M. Paulini

While B0 and B+ mesons are well studied at B-factories, large samples of B0s mesons are only available at the Tevatron so far. Since the B0s meson consists of quarks of the second and third generation it provides a complementary probe for…

High Energy Physics - Experiment · Physics 2019-08-14 Thomas Kuhr

The Tevatron Run II program is in progress since 2001. The CDF experiment have accumulated roughly five times more data than in Run I, with much improved detectors. Preliminary results from the CDF experiment are presented. We focus on the…

High Energy Physics - Experiment · Physics 2007-05-23 Soushi Tsuno

With the advent of the Tevatron Run 2, the collider experiments, CDF and D0, have reestablished the top quark and the W and Z signals and have begun programs of precision measurements of top quark and electroweak properties. We will survey…

High Energy Physics - Experiment · Physics 2014-11-17 Mark C. Kruse

Measuring the oscillation frequency in the $B_s^0$-meson system was one of the main goals in b-physics for the two experiments CDF and D{\O} at the Tevatron-Collider since the start of RunII in the year 2001. The D{\O} collaboration was the…

High Energy Physics - Experiment · Physics 2019-08-14 Gernot A. Weber

This report provides a comprehensive overview of the prospects for B physics at the Tevatron. The work was carried out during a series of workshops starting in September 1999. There were four working groups: 1) CP Violation, 2) Rare and…

As the integrated luminosity of the Run II Tevatron increases, the sensitivity to new physics is approaching and in some cases surpassing that previously attained in Run I. Presented below are a selection of new results from searches for…

High Energy Physics - Experiment · Physics 2019-08-14 Jonathan Hays

The Run II physics programme of the Tevatron is proceeding with more than 300 pb-1 of analysis quality data, collected at a centre-of-mass energy of 1.96 TeV. Searches for supersymmetric particles are starting to set new limits, improving…

High Energy Physics - Experiment · Physics 2007-05-23 Giulia Manca

The phenomenology of b-production and some of the previous Run I measurements of CDF and D0 are briefly reviewed. A new analysis by CDF of Run I b-bbar angular correlations and a new measurement by D0 of Run II b-jet cross-section, are…

High Energy Physics - Experiment · Physics 2007-05-23 Eric Kajfasz

In order to fully exploit the physics potential of the Tevatron Run 2, the D0 detector has been upgraded. Having nearly completed the commissioning phase, the D0 detector is starting to produce its first physics results. An overview of the…

High Energy Physics - Experiment · Physics 2007-05-23 Aurelio Juste

The Fermilab Tevatron (p pbar), operating at sqrt(s)=1.96 TeV, is a rich source of B hadrons. The large acceptance in terms of rapidity and transverse momentum of the charged particle tracking system and the muon system make the upgraded…

High Energy Physics - Experiment · Physics 2019-08-14 Jan Stark

Run II at the Tevatron Collider started at the beginning of March 2001. With extensive upgrades on both detectors and electronics the CDF II began to collect data. This paper reviews early Run II physics results obtained by analyzing data…

High Energy Physics - Experiment · Physics 2007-05-23 C. Pagliarone
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