164x Filetype PPTX File size 1.31 MB Source: fdjpkc.fudan.edu.cn
1.Accelerators • History-Why • Particle Sources • Acceleration stage • Space charge • Diagnostics • Application 2. Detectors Gas-Filled Radiation Detectors ionization chambers proportional counters Geiger-Muller counters Scintillation Detectors Photomultiplier tube Semiconductor Detectors Personal Dosimeters photographic films photographic emulsion plates Others Cloud and Bubble Chambers Particle identification E-ΔE, TOF Measurement theory Detection Equipment Ionization Chambers Key Components in a Simple Ionization Chamber Ionizing Battery the voltage must be radiation + sufficiently high for effective collection of –+–+– Load electrons. +–+–+ resister – Detector Ampere- chamber meter The average energy required to Current (A) is proportional to charges collected ionize a gas atom 30 eV/ion. If particles entering an air-filled on electrode in ionization chambers. detector deposit an average of -1 The current registered in the ionization chamber is 1 GeV S in the gas, the proportional to the number of ion pairs generated by average current flowing through radioactivity the chamber How can the sensitivities of ionization chambers be improved? What happens when the voltage is increased? Proportional Counters Gas Multiplication Key Components in a Simple Ionization Chamber Ionizing Battery X00 V radiation + –+ –+–+– Load +–+–+ resister – –+–+–+ Detector Ampere- chamber meter –+–+–+–+–+–+–+–+–+ Proportional counters –+–+–+–+–+–+–+–+–+–+–+– Gas multiplication due to +–+–+–+–+–+–+–+–+–+–+–+– secondary ion pairs when the +–+–+–+–+–+–+–+–+–+–+–+– ionization chambers operate at + higher voltage. not only collect but also accelerate electrons 5 It should be noted, however, that the small mass and high energy of electrons make them drift 100,000 times faster than ions. Thus, the current is mainly due to the drifting electrons with only a small fraction due to the drift of ions. Despite the multiplication due to secondary ion pairs, the ampere-meters register currents proportional to the numbers of primary electrons caused by radiation entering the detectors. Thus, currents of proportional chambers correspond to amounts of ionization radiation entering the proportional chamber.
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