PPT-Sensors for high radiation calorimetry

Roger Rusack The University of Minnesota Upgrades to the CMS detector Outline This talk is the context of preparation for Snowmass I want to motivate some technical developments for detectors at the high intensities that we will see at the energy frontier. A high frequency alternating current is fed through a coil embedded in a sensor housing The electromagnetic field from the coil induces eddy currents in the conductive target As a consequence the alternating current resistance of the coil changes Th Measured values show the thermophysical properties of the examined system or sample There are two bas ic types of calorimeters isothermal and adiabatic Constant temperature is sustained in t he isothermal calorimeter t means that the calorimeter is 97 No 1 pp 6973 2001 Nuclear Technology Publishing BIOMARKERS SPECIFIC TO DENSELYIONISING HIGH LET RADIATIONS D J Brenner N Okladnikova P Hande L Burak C R Geard and T Azizova Center for Radiological Research Columbia University 6 Datasheet 2 What makes our sensors better? Precise measurement: The industry’s smallest Total Error Band, fast response time, and high accuracy provide precise measurement and high performance i R&D I: Electromagnetic Radiation Damage Studies. BeamCal. instrument expected to receive up to 100 . Mrad. per year of electromagnetically-induced radiation. SLAC Experiment T506 uses End Station Test Beam directed on 7 X. Sensors . Based on Novel Microwave Gratings . . Student: Ken Smith, Electrical and Computer Engineering . Faculty . Advisor: . Dr. . Hai. Xiao, Electrical Engineering. Project Objectives. Related Work . Fall, 2010 Indirect Calorimetry 1 Indirect Calorimetry Indirect Calorimetry CALORIMETRY The science that quantifies the heat release from metabolism is termed calorimetry . Figure 4.5 CALORIMETRY D Sensor Requirements. Sensor requirements (consistent with IPHC development direction). ~2 cm x 2 cm (1 reticle) size.. Pixel size < 30 µm.. Integration time of ≤ 200 µs for L = 8 x 10. 27. cm. BeamCal. instrument expected to receive up to 100 . Mrad. per year of electromagnetically-induced radiation. SLAC Experiment T506 uses End Station Test Beam directed on 7 X. 0. of Tungsten radiator to generate EM showers. SiD. ?. Adam Para. ALCPG meeting, December 20, 2007. Other Possible Titles. Homogeneous Dual Readout Calorimeter. A List of Miracles and Why You would Like Them to Happen. Prospects for Crystal-based Hadron Calorimetry. ATOC . SkyWatch. - 29 Jan to 5 Feb 2019. John Cassano. ATOC 4500. Objectives. Compare temperature observed by Hobo weather stations and Kestrel Drop sensors from a 1 week deployment at ATOC . SkyWatch. FCC week Washington. 23. -27 March . 2015. W. . Riegler. D. . Denisov. , H. . ten. Kate, L. . Lienssen. , F. . Lanni. , M. . Abbrescia. , R. Richter, Y. . Onel. , W. Smith, S. . C. hekanov. Exploration + Higgs as a tool for . What is radiation?. Radiation is the giving off of high amounts of energy in the form of particles and/or waves.. The Electroscope. The Geiger Counter. Disposal of Radioactive Wastes. Radiation in Household Products. longwave is calculated by combining the output of two longwave sensors. Net shortwave is calculated separately by combining the output of two shortwave sensors. This model includes two shortwave and