In this configuration, the semiconductor detector is placed opposite to the surface of the sample being analyzed, and an energy spectrum of charged particles emitted by the neutron-induced reaction is acquired.
12.
All semiconductor detectors function rather inefficiently in crystal receivers, because the low voltage input to the detector is too low to result in much difference between forward better conduction direction, and the reverse weaker conduction.
13.
A "'semiconductor detector "'in ionising radiation detection physics is a device that uses a semiconductor ( usually silicon or germanium ) to measure the effect of incident charged particles or photons.
14.
Semiconductor detectors, also called solid-state detectors, are fundamentally different from scintillation detectors : They rely on detection of the charge carriers ( electrons and holes ) generated in semiconductors by energy deposited by gamma ray photons.
15.
"' Semiconductor detectors "'can be used in theory, and their applications are increasing as their technology improves, but historically their use for WDX has been restricted by their slow response ( see EDX ).
16.
Examples of detectors common in spectroscopy include heterodyne receivers in the microwave, bolometers in the millimeter-wave and infrared, mercury cadmium telluride and other cooled semiconductor detectors in the infrared, and photodiodes and photomultiplier tubes in the visible and ultraviolet.
17.
It has also been applied to materials used for particle detectors or semiconductor detectors used in nuclear research, for example, high-resistivity silicon, cadmium telluride ( CdTe ), etc . TSC has also been applied to various organic insulators.
18.
He designed and built about 15 electronic instruments, including a counting-rate meter with industrial applications, a closed-circuit television system used at the cyclotron, a charge-sensitive low-noise amplifier and a precision pulse generator for a semiconductor detector spectrometer and a switching circuit for photomultiplier tubes.
19.
You get a very pure sample of 14 ( any 12 C will contribute to the mass, but not beta decay, which throws off the measurement ), completely cover it with semiconductor detectors ( any solid angle not covered allows beta particles to escape uncounted ), and then let it sit for a long, long time.
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