Challenges in the design of the detector solenoid for the Mu2e experiment
Abstract Not Provided
Engineering topics
Publications and source records attributed to Coleman, R.
Abstract Not Provided
RadBall{trademark} is a novel technology that can locate and quantify unknown radioactive hazards within contaminated areas, hot cells, and gloveboxes. The device consists of a colander-like outer tungsten collimator that houses a radiation-sensitive polymer semi-sphere. The collimator has a number of small holes with tungsten inserts; as a result, specific areas of the polymer are exposed to radiation becoming increasingly more opaque in proportion to the absorbed dose. The polymer semi-sphere is imaged in an optical computed tomography scanner that produces a high resolution 3D map of optical attenuation coefficients. A subsequent analysis of the optical attenuation data using a reverse ray tracing or backprojection technique provides information on the spatial distribution of gamma-ray sources in a given area forming a 3D characterization of the area of interest. RadBall{trademark} was originally designed for dry deployments and several tests, completed at Savannah River National Laboratory and Oak Ridge National Laboratory, substantiate its modeled capabilities. This study involves the investigation of the RadBall{trademark} technology during four submerged deployments in two water filled cells at the DOE Hanford Site's Waste Encapsulation Storage Facility.
This Technical Memorandum (TM) summarizes the Fermilab accelerator and accelerator experiment operations for FY 2010. It is one of a series of annual publications intended to gather information in one place. In this case, the information concerns the FY 2010 Run II at the Tevatron Collider, the MINOS and MINER?A experiments using the Main Injector Neutrino Beam (NuMI), the MiniBooNE experiment running in the Booster Neutrino Beam (BNB), and the Meson Test Beam (MTest) activities in the 120 GeV external Switchyard beam (SY120). Each section was prepared by the relevant authors, and was somewhat edited for inclusion in this summary.
The authors present precise tests of CP and CPT symmetry based on the full dataset of K {yields} {pi}{pi} decays collected by the KTeV experiment at Fermi National Accelerator Laboratory during 1996, 1997, and 1999. this dataset contains 16 million K {yields} {pi}{sup 0}{pi}{sup 0} and 69 million K {yields} {pi}{sup +}{pi}{sup -} decays. They measure the direct CP violation parameter Re({epsilon}{prime}/{epsilon}) = (19.2 {+-} 2.1) x 10{sup -4}. They find the K{sub L}-K{sub S} mass difference {Delta}m = (5270 {+-} 12) x 10{sup 6} {h_bar}s{sup -1} and the K{sub S} lifetime {tau}{sub S} = (89.62 {+-} 0.05) x 10{sup -12} s. They also measure several parameters that test CPT invariance. They find the difference between the phase of the indirect CP violation parameter, {epsilon}, and the superweak phase, {phi}{sub {epsilon}} - {phi}{sub SW} = (0.40 {+-} 0.56){sup o}. They measure the difference of the relative phases between the CP violating and CP conserving decay amplitudes for K {yields} {pi}{sup +}{pi}{sup -} ({phi}{sub +-}) and for K {yields} {pi}{sup 0}{pi}{sup 0} ({phi}{sub 00}), {Delta}{phi} = (0.30 {+-} 0.35){sup o}. From these phase measurements, they place a limit on the mass difference between K{sup 0} and {bar K}{sup 0}, {Delta}M < 4.8 x 10{sup -19} GeV/c{sup 2} at 95% C.L. These results are consistent with those of other experiments, their own earlier measurements, and CPT symmetry.