Evidence for the Heavy Baryon Resonance State [Lambda] b*0 Observed with the CDF II Detector, and Studies of New Particle Tracking Technologies Using the LANSCE Proton Beam

To discover and probe the properties of new particles, we need to collide highly energetic particles. The Tevatron at Fermilab has collided protons and anti-protons at very high energies. These collisions produce short lived and stable particles, some known and some previously unknown. The CDF detector is used to study the products of such collisions and discover new elementary particles. To study the interaction between high energy charged particles and the detector materials often requires development of new instruments. Thus this dissertation involves a measurement at a contemporary experiment and development of technologies for related future experiments that will build on the contemporary one.;Using data from proton-antiproton collisions at sqrt(s) = 1.96TeV recorded by the CDF II detector at the Fermilab Tevatron, evidence for the excited resonance state Lambda_b.;*0 is presented in its Lambda_b.;0 pi.;+ pi.;- decay,followed by the Lambda_b.;0 -> Lambda_c.;+ pi.;- and Lambda_c.;+ -> p K.;- pi.;+decays. The analysis is based on a data sample corresponding to an integrated luminosity of 9.6 fb.;-1 collected by an online event selection process basedon charged particle tracks displaced from the proton-antiproton interaction point. The significance of the observed signal is 3.5sigma The mass of the observed state is found to be 5919.22 +/- 0.76 MeV/c 2 in agreement with similar findings in proton-proton collision experiments.;To predict the radiation damage to the components of new particle tracking detectors, prototype devices are irradiated at test beam facilities that reproduce the radiation conditions expected. The profile of the test beam and the fluence applied per unit time must be known. We have developed a technique to monitor in real time the beam profile and fluence using an array of pin semiconductor diodes whose forward voltage is linear with fluence over the fluence regime relevant to, for example, silicon tracking detectors in the LHC upgrade era. We have demonstrated this technique in the 800 MeV proton beam at the LANSCE facility of Los Alamos National Laboratory.