Add to ORKGThe 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 semileptonic decay and lifetime information is shown and some examples of prospects for the future given
After a five year upgrade period, the Fermilab experiments CDF and D0 are taking high quality data i...
The \d0 (DZERO) Detector at Fermilab is currently collecting data since March 1, 2001, called Run 2....
The integrated luminosity at Run 2 of the Tevatron is approaching the Run 1 total, and data analysis...
Run II at the Tevatron started on March 1, 2001 with a design instantaneous luminosity of 2 x 10{sup...
Run II at the Tevatron will begin in the spring of 2001. With p{bar p} collisions at {radical}s = 2....
The Fermilab Tevatron (p pbar), operating at sqrt(s)=1.96 TeV, is a rich source of B hadrons. The la...
In order to fully exploit the physics potential of the Tevatron Run 2, the D0 detector has been upgr...
In order to fully exploit the physics potential of the Tevatron Run 2, the D0 detector has been upgr...
A vibrant B physics program is being pursued at the Tevatron for Run II using the upgraded accelerat...
The D0 detector as collected over 3.7 fb{sup -1} of high quality data. With this large data set, D0 ...
The current status of Run II at the Tevatron is covered. Upgrades of both the CDF and D0 detectors a...
The latest results in B physics from the CDF and D0 experiments at the Tevatron are presented, inclu...
The D0 (DZERO) Detector at Fermilab has been collecting data since March 1, 2001. The detector has u...
Between 1992 and 1996, the CDF and D0 experiments have collected data samples of 110 pb{sup -1} each...
The latest results in B physics from the CDF and D0 experiments at the Tevatron are presented, inclu...
After a five year upgrade period, the Fermilab experiments CDF and D0 are taking high quality data i...
The \d0 (DZERO) Detector at Fermilab is currently collecting data since March 1, 2001, called Run 2....
The integrated luminosity at Run 2 of the Tevatron is approaching the Run 1 total, and data analysis...
Run II at the Tevatron started on March 1, 2001 with a design instantaneous luminosity of 2 x 10{sup...
Run II at the Tevatron will begin in the spring of 2001. With p{bar p} collisions at {radical}s = 2....
The Fermilab Tevatron (p pbar), operating at sqrt(s)=1.96 TeV, is a rich source of B hadrons. The la...
In order to fully exploit the physics potential of the Tevatron Run 2, the D0 detector has been upgr...
In order to fully exploit the physics potential of the Tevatron Run 2, the D0 detector has been upgr...
A vibrant B physics program is being pursued at the Tevatron for Run II using the upgraded accelerat...
The D0 detector as collected over 3.7 fb{sup -1} of high quality data. With this large data set, D0 ...
The current status of Run II at the Tevatron is covered. Upgrades of both the CDF and D0 detectors a...
The latest results in B physics from the CDF and D0 experiments at the Tevatron are presented, inclu...
The D0 (DZERO) Detector at Fermilab has been collecting data since March 1, 2001. The detector has u...
Between 1992 and 1996, the CDF and D0 experiments have collected data samples of 110 pb{sup -1} each...
The latest results in B physics from the CDF and D0 experiments at the Tevatron are presented, inclu...
After a five year upgrade period, the Fermilab experiments CDF and D0 are taking high quality data i...
The \d0 (DZERO) Detector at Fermilab is currently collecting data since March 1, 2001, called Run 2....
The integrated luminosity at Run 2 of the Tevatron is approaching the Run 1 total, and data analysis...