The barometer coefficient and the mu-meson production spectrum.

In the following account, we are interested in what happens to the mu-meson component of cosmic radiation in the atmosphere. Two main effects are to be distinguished. The first is the gradual absorption of the momentum of a meson, by collision with charged particles in the air, as the meson descends...

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Bibliographic Details
Main Author: Wilson, Roderic. L.
Other Authors: Morris, T. (Supervisor)
Format: Others
Language:en
Published: McGill University 1955
Subjects:
Online Access:http://digitool.Library.McGill.CA:80/R/?func=dbin-jump-full&object_id=109884
Description
Summary:In the following account, we are interested in what happens to the mu-meson component of cosmic radiation in the atmosphere. Two main effects are to be distinguished. The first is the gradual absorption of the momentum of a meson, by collision with charged particles in the air, as the meson descends. This is called the “mass absorption” of momentum. The second effect is the spontaneous disintegration of a mu-meson, while in flight. The disintegration en masse of mu-mesons is called the “decay” effect.