CDF Experiment
Detector Simulation
at Fermilab
Carnegie Mellon
Physics Department

Hadron Collider Physics with CDF

Particle Physics at the Highest Available Energies

Our group is working with the Collider Detector at Fermilab (CDF) which is operating at the Tevatron Collider at the Fermi National Accelerator Laboratory (Fermilab). The Tevatron collider is a proton-antiproton storage ring with a centre-of-mass energy of 1.8 TeV which is currently the highest available energy until the start of the Large Hadron Collider (LHC) at CERN. A public tour of the Tevatron Collider can be found here. General information about the CDF experiment is available here.

The CDF Group at CMU


Projects

   
CDF Layer 00 CDF Run IIb Detector CDF Hadron Calorimeter
CDF Layer 00 CDF Run IIb Silicon CDF Hadron Calorimeter

Besides the projects above, we are also involved in the CDF Detector Simulation Project.


Physics

Our group is interested in heavy flavour physics, in particular in the physics of B mesons. The principal interest in studying B hadrons in the context of the Standard Model arises from the fact that B hadron decays provide valuable information on the weak mixing matrix, the Cabibbo-Kobayashi-Maskawa (CKM) matrix. Eigenstates of the weak interaction Hamiltonian are not the same as the quark mass eigenstates. The matrix used to transform between these bases is called the CKM matrix. In fact, measurements of B hadron decay rates, as well as observation of BB= mixing, allow the determination of five of the nine CKM matrix elements.

Traditionally, B physics has been the domain of e+ e- machines, but already the UA1 collaboration at CERN has shown that B physics is feasible at a hadron collider. However, the combination of a better mass resolution and vertex detection with the Silicon Vertex Detector (see this example with explanation) enabled the CDF experiment during the 1992-1995 data taking period (Run I) to perform a broad B physics program.

After a successful detector upgrade period, the CDF experiment will start taking data in March 2001 for a five year data taking period (Run II). The anticipated amount of high quality data promises a wealth of important physics results. The future interest in B physics lies in the study of CP violation in the system of neutral B mesons. Besides CP violation, we are also interested in observing flavour oscillations in the BS meson system as well as the spectroscopy of BC mesons. You can view CDF's plans to measure CP violation as outlined in the CDF Technical Design Report for Run II. Please visit also the Workshop on B Physics at the Tevatron for an overview of B physics prospects during Run II at the Tevatron.


MP