By J.B.A. England
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Additional resources for Techniques in Nuclear Structure Physics: Part 1
The factor F is now known as the 'Fano factor'. 4(a) which has a dielectric gas between the parallel electrode plates. 4 (a) Schematic representation of a parallel-plate geometry gas-filled ion chamber; (b) schematic representation of a cylindrical geometry gas-filled ion chamber Detectors and Methods of Detection 23 total charge Nq in the gas, where q is the number of charges produced per ion pair. Usually q = 2e where e is the electron charge. S(a) shows the variation of the collected charge, f~ Ii dt where /i is the instantaneous current drawn from the device, as a function of the applied voltage V.
Corresponds to 4·00 MeV and channel 1024 corresponds to 6·00 MeV, the typical value for 8McA would be 2 keV. The expected value for the final FWHM spread from these figures would be 34 keV, quite close to the best value of 35 keV obtained in practice. 5. Finally, consider the operation of a detector of cylindrical geometry operating in the Geiger mode in region IV. In this region the output charge pulses from the detector are independent of the amount of ionisation produced by the incident particle.
111 The anode resistance of their detector Ro was typically 40 kil mm -t. Thus the total resistance of the anode of the detector was many megohms for a long detector. This raises problems with recovery time and with resistive noise contributions. The alternative system used, for example, by Williams et a/. 113 and Westphal et al. 9(b ). One end of the anode is grounded and the position signal Qrx/L is received at the other end, where x is the position along the anode as measured from the grounded end and L is the length of the anode.
Techniques in Nuclear Structure Physics: Part 1 by J.B.A. England