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4.8. Time Projection Chambers 67<br />

Figure 4.16: Drift chambers can be used to track charged particles. In this picture a scientist checks<br />

part of the TWIST apparatus, (8) which used 44 drift chamber planes to do precision measurements<br />

of muon decay. The drift chambers are circular planes whose edges can be seen in the photograph.<br />

[Courtesy Bob Tribble.]<br />

Drift chambers are still very popular because they are reliable and not expensive.<br />

Figure 4.16 shows a picture of the TWIST apparatus which used drift chambers to<br />

track electrons from muon decay. (8)<br />

A drift chamber can be planar or cylindrical. In the latter form it can be made<br />

into a time projection chamber.<br />

4.8 Time Projection Chambers<br />

Wire chambers have one major disadvantage: they only yield information about one<br />

spatial direction. To determine both coordinates, a second wire chamber must be<br />

used. This requirement makes the experimental arrangement complicated and reduces<br />

the solid angle subtended by the detector. Time projection chambers (TPCs),<br />

invented in 1974 by David Nygren, avoid this limitation and are nearly ideal detectors:<br />

TPCs have large solid angles, give excellent spatial resolution in three dimensions,<br />

yield charge and mass information, and allow good pattern recognition. (9,10)<br />

TPCs can be as small as a grapefruit or weigh as much as 10 tons. The main<br />

features are illustrated in Fig. 4.17. The drift chamber is filled with a gas, usually a<br />

mixture of Ar and CH4 because it is inexpensive and allows high electron mobility.<br />

Uniform electric (E) and magnetic (B) fields are applied parallel to the axis (beam<br />

pipe). A charged particle passing through the chamber produces ion pairs along its<br />

8 TWIST Collaboration, Phys. Rev. Lett. 94, 101805 (2005).<br />

9 R. J. Madaras and P. J. Oddone, Phys. Today 37, 38 (August 1984).<br />

10 “The Time Projection Chamber”, ed. J.A. MacDonald, AIP Conference Proceedings No. 108,<br />

American Institute of <strong>Physics</strong>, New York, 1984.

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