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By Eugenio Nappi
Content material:
Chapter 1 advent (pages 1–20):
Chapter 2 simple tactics in Gaseous Detectors (pages 21–51):
Chapter three conventional Position?Sensitive Gaseous Detectors and Their historic improvement: From the Geiger Counter to the Multi?wire Proportional Chamber (1905 until eventually 1968) (pages 53–83):
Chapter four The Multi cord Proportional Chamber period (pages 85–90):
Chapter five extra extensive approximately Gaseous Detectors (pages 91–144):
Chapter 6 New rules on Gaseous Detectors Conceived through the Early Years of the “Multi twine Proportional Chambers” period (1968–1977) (pages 145–159):
Chapter 7 advancements in MWPCs, PPACs, and RPCs after 1977 (pages 161–213):
Chapter eight Micropattern Gaseous Detectors (pages 215–249):
Chapter nine purposes of Imaging Gaseous Detectors (pages 251–311):
Chapter 10 Conclusions (pages 313–317):
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Additional resources for Imaging Gaseous Detectors and Their Applications
Example text
11]). 10) For Nph photons of the same energy Ev traversing a gas volume of thickness l, the resulting number of primary photoelectrons n0 is given by: n0 = Nph (1 − exp{−σi (Ev )nl}) where σi (Ev ) is the gas ionization cross section. 6 Mass absorption coefficient of various gases as a function of the photon energy Eν . Carbon is also included to allow the calculation of the absorption of hydrocarbon-based gases (from Ref. [4]). 14, for some intervals of photon energies, in which Ev > Ei the absorption occurs mostly via the photoionization (or photoelectric effect), it turns out that σi ∼ σa .
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