Mathematical Treatment of Random Processes with Dead Time
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概要
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Random events measured with a constant dead time give a counting rate smaller than the event rate. The latter has been obtained after dead time correction. A current method of dead time correction as expressed in Eq. (1) is provd to be justified only if the event rate is constant in time. In general the average event rate is obtained, as shown in Eq. (27), by dividing the average number of counts by the average length of live time, the measuring time minus dead time. The probability distribution and variance are explicitly given in Eqs. (20) and (35), respectively. An example we met in a rocket observation of fast electrons is described for illustration.
- 宇宙航空研究開発機構の論文
著者
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Nagase F
Inst. Space And Astronautical Science Kanagawa
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Hayakawa S
Hiroshima Univ. Higashi‐hiroshima Jpn
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MAKINO Fumiyoshi
Institute of Space and Astronautical Science
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NAGASE Fumiaki
The Institute of Space and Astronautical Science
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Hayakawa Satio
Department Of Astrophysics Faculty Of Science Nagoya University
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Makino Fumiyoshi
Iss Science Project Office Institute Of Space And Astronautical Science Japan Aerospace Exploration
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Makino Fumiyoshi
Institute Of Space And Astronautical Science Nagoya University
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Makino Fumiyoshi
Department Of Physics Nagoya University
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Nagase Fumiaki
Department Of Astrophysics Faculty Of Science Nagoya University
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Nagase F
The Institute Of Space And Astronautical Science
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