Proportional Counter
a gas-filled discharge device for the detection of ionizing particles and quanta. The counter produces a signal with an amplitude proportional to the energy of the particle being detected. On passing through the gas inside the counter, a charged particle produces in its path ion-electron pairs, the number of pairs depending on the energy lost by the particle in the gas.
When the particle is brought to a full stop in a proportional counter, the impulse is proportional to the particle’s energy. As in the ionization chamber, an electric field sends the electrons toward the anode and the ions toward the cathode. In contrast to the ionization chamber, the field near the anode of the proportional counter is so strong that the electrons acquire energy sufficient for secondary ionization. As a result, instead of a single primary electron, an avalanche of electrons arrives at the anode, and the total number of electrons thus collected far exceeds the number of primary electrons. The ratio of the total number of collected electrons to the number of primary electrons is called the gas amplification factor (ions also take part in the formation of the impulse).
A cylinder usually serves as the cathode in a proportional counter, and a fine (10–100 μ) metal wire, stretched along the axis of the cylinder, serves as the anode (see Figure 1). Gas amplification occurs near the anode at a distance comparable to the wire’s diameter; beyond this region, the electrons drift under the action of the electric field without “multiplication.” Proportional counters are filled with an inert gas (the gas must not absorb drifting electrons) with the addition of a small amount of a polyatomic gas, which absorbs the photons formed in the avalanches.
Proportional counters usually have a gas amplification factor of ~103-104 (which may reach 106 or more) and and an impulse amplitude of ~10-2 V when the capacitance of the proportional counter is about 20 picofarads. An avalanche develops in ~10-9–10-8 sec, but the instant at which a signal appears at the output of the proportional counter depends on the path of the ionizing particle, that is, on the time required for the electrons to drift to the wire. At a radius of approximately 1 cm and a pressure of approximately 1 atmosphere, the delay time of the signal with respect to the particle’s passage is ~106 sec. The sensitivity of the proportional counter surpasses that of the scintillation counter but is less than that of the semiconductor detector. However, proportional counters allow work in the energy range below 1 kiloelectron volt, where semiconductor detectors cannot be used.
Proportional counters are used to detect all types of ionizing radiation. There are counters designed to detect, for example, alpha particles, electrons, nuclear fission fragments, neutrons, gamma quanta, and X-ray quanta. In the case of proportional counters that detect neutrons, gamma, and X-ray quanta, interactions with the gas filling the counter are employed to produce secondary charged particles that lend themselves to detection. The proportional counter, together with the ionization chamber, played an important role in nuclear physics in the 1920’s and 1930’s as virtually the only spectrometric detector.
In the late 1960’s, the physics of high-energy particles found a new use for the proportional counter in the form of a proportional chamber, which consists of a large number (102–103) of proportional counters arranged in coplanar fashion in a gas-filled enclosure. Such a device makes it possible not only to measure the ionization of a particle in each individual counter but also to locate the track of the particle. Typical parameters of proportional chambers are a distance between adjacent anode wires of ~ 1–2 mm, a distance between anode and cathode planes of approximately 1 cm, and a resolution time of ~ 10-7sec. The development of microelectronics and the introduction of electronic computers in experimental techniques have made possible the development of systems consisting of tens of thousands of individual wires connected directly to a computer, which stores and processes all information from the proportional chamber. Such systems thus function simultaneously as both high-speed spectrometers and track registration detectors.
The drift chamber, which uses the drift of electrons preceding the formation of an avalanche to measure the track of a particle, appeared in the 1970’s. By alternating the anodes and cathodes of the individual proportional counters in one plane and measuring the drift time of electrons, it is possible to measure the track of a particle through the chamber with a high degree of precision (~0.1 mm) with only one-tenth as many wires as in a proportional chamber.
Proportional counters are used not only in nuclear physics but also in such fields as the physics of cosmic rays, astrophysics, engineering, medicine, geology, and archaeology. For example, an X-ray fluorescence analysis of the lunar soil was carried out by means of a proportional counter mounted on Lunokhod 1.
REFERENCES
Veksler, V., L. Groshev, and B. Isaev. lonizatsionnye metody issledovaniia izluchenii. Moscow-Leningrad, 1949.Printsipy i melody registratsii elementarnykh chastits. Moscow, 1963. (Translated from English.)
Kalashnikova, V. I., and M. S. Kozodaev. Detektory elementarnykh chastits. (Eksperimental’nye metody iadernoi fiziki, part 1.) Moscow, 1966.
V. S. KAFTANOV and A. V. STRELKOV
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