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Subatomic Physics

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64 Detectors<br />

Figure 4.13: Neutrino interaction in a hydrogen bubble chamber. A neutrino enters from the right<br />

and interacts with the proton of a hydrogen atom to yield a muon (the long track that extends<br />

to the top left), a positive pion (the short top track), and a proton (the short bottom track).<br />

[Courtesy Argonne National Laboratory.]<br />

3.6 m (12 ft) hydrogen bubble chamber of the Argonne National Laboratory which<br />

contained about 20,000 liters of hydrogen. A superconducting magnet produced a<br />

field of about 18 kG in the chamber volume of 25 m 3 .<br />

Because of their slow response, bubble chambers are seldomly used in present<br />

days for experiments with high counting rates. However, they are still being used for<br />

applications with low counting rates in combination with CCD cameras. (5) Some<br />

versions can be triggered using the spike in pressure when a pulse develops. In the<br />

next section we explain in more detail what triggering means.<br />

4.5 Spark Chambers<br />

Whereas spark chambers are no longer state-of-the-art, they illustrate the basic<br />

principles of a triggerable detector clearly. Spark chambers are based on a simple<br />

fact. If the voltage across two metal plates, spaced by a distance of the order<br />

of cm, is increased beyond a certain value, a breakdown occurs. If an ionizing<br />

particle passes through the volume between the plates, it produces ion pairs, and<br />

the breakdown takes the form of a spark that follows the track of the particle. Since<br />

the ions remain between the plates for a few µs, the voltage can be applied after<br />

passage of the particle: A spark chamber is a triggerable detector.<br />

The elements of a spark chamber system are shown in Fig. 4.14. The problem<br />

to be studied in this simplified arrangement is the reaction of an incoming charged<br />

particle with a nucleus in the chamber, giving rise to at least two charged products.<br />

Thus the signature of the desired events is “one charged in, two charged out.”<br />

Three scintillation counters, A, B, and C, detect the three charged particles. If the<br />

particles pass through the three counters, the LOGIC circuit activates the high-<br />

5 See, for example, W.J. Bolte et al., Journal of <strong>Physics</strong>: Conference Series 39, 126 (2006);<br />

http://collargroup.uchicago.edu/<br />

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