Run II at the Tevatron started on March 1, 2001 with a design instantaneous luminosity of 2 x 10{sup 32} cm{sup -2} s{sup -1}. The upgraded D0 detector is expected to collect 2 fb{sup -1} of data at {radical}s = 2.0 TeV in approximately 2 years. The D0 collaboration is planning to make measurements in a number of important areas of B physics, including sin(2{beta}), B{sub s} mixing, the {Lambda}{sub b} lifetime and rare B decays. In this note we describe the upgraded D0 detector and highlights of the B physics program in D0
The integrated luminosity at Run 2 of the Tevatron is approaching the Run 1 total, and data analysis...
Both experiments CDF and D0 at the Tevatron collider have now the first samples of B{sub s} where pr...
The Tevatron experiments, CDF and D0, have produced a wealth of new B-physics results since the star...
Run II at the Tevatron will begin in the spring of 2001. With p{bar p} collisions at {radical}s = 2....
The B physics program planned for the D0 Upgrade Detector for Run 2 of the Tevatron is described. Cu...
The Fermilab Tevatron (p{bar p}), operating at {radical}s = 1.96 TeV, is a rich source of B hadrons....
A vibrant B physics program is being pursued at the Tevatron for Run II using the upgraded accelerat...
Between 1992 and 1996, the CDF and D0 experiments have collected data samples of 110 pb{sup -1} each...
Precision B-physics results from the CDF and D0 Collaborations based on data collected during the Te...
The current status of Run II at the Tevatron is covered. Upgrades of both the CDF and D0 detectors a...
Between 1992 to 1996, the CDF and D0 detectors each collected data samples exceeding 100 pb{sup {min...
In order to fully exploit the physics potential of the Tevatron Run 2, the D0 detector has been upgr...
The D0 detector as collected over 3.7 fb{sup -1} of high quality data. With this large data set, D0 ...
In order to fully exploit the physics potential of the Tevatron Run 2, the D0 detector has been upgr...
After a five year upgrade period, the Fermilab experiments CDF and D0 are taking high quality data i...
The integrated luminosity at Run 2 of the Tevatron is approaching the Run 1 total, and data analysis...
Both experiments CDF and D0 at the Tevatron collider have now the first samples of B{sub s} where pr...
The Tevatron experiments, CDF and D0, have produced a wealth of new B-physics results since the star...
Run II at the Tevatron will begin in the spring of 2001. With p{bar p} collisions at {radical}s = 2....
The B physics program planned for the D0 Upgrade Detector for Run 2 of the Tevatron is described. Cu...
The Fermilab Tevatron (p{bar p}), operating at {radical}s = 1.96 TeV, is a rich source of B hadrons....
A vibrant B physics program is being pursued at the Tevatron for Run II using the upgraded accelerat...
Between 1992 and 1996, the CDF and D0 experiments have collected data samples of 110 pb{sup -1} each...
Precision B-physics results from the CDF and D0 Collaborations based on data collected during the Te...
The current status of Run II at the Tevatron is covered. Upgrades of both the CDF and D0 detectors a...
Between 1992 to 1996, the CDF and D0 detectors each collected data samples exceeding 100 pb{sup {min...
In order to fully exploit the physics potential of the Tevatron Run 2, the D0 detector has been upgr...
The D0 detector as collected over 3.7 fb{sup -1} of high quality data. With this large data set, D0 ...
In order to fully exploit the physics potential of the Tevatron Run 2, the D0 detector has been upgr...
After a five year upgrade period, the Fermilab experiments CDF and D0 are taking high quality data i...
The integrated luminosity at Run 2 of the Tevatron is approaching the Run 1 total, and data analysis...
Both experiments CDF and D0 at the Tevatron collider have now the first samples of B{sub s} where pr...
The Tevatron experiments, CDF and D0, have produced a wealth of new B-physics results since the star...