Download PDF by Prange G.: Die Hamilton-Jacobische Theorie fuer Doppelintegrale

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Additional info for Die Hamilton-Jacobische Theorie fuer Doppelintegrale

Example text

D. 6. 00 1180 Cl

E of the incident radiation, two pulse amplitudes are formed, one with a maximum at V and one with a maximum at V', where V' is proportional to (E- EArKa). This second pulse amplitude is called the escape peak. As shown in the upper part of Fig. 7 the escape peak (at about 100 mV) is roughly 10% the intensity of the photo-peak (400 mV). The counting rate is proportional to the area under the distribution. As the counter voltage is increased all pulses are enlarged, but at low voltage levels are insufficiently large to pass the threshold level.

The escape peak is, however, still too small to pass the threshold. This situation remains up to a voltalge of about 1550 V, line C, and so there is a plateau between B and C. Further increase in voltage brings the escape peak amplitude also over the threshold level with a further increase in count rate (the count rate scale on the ordinate of the lower curve is not linear) proportional to the area below the escape peak curve. Further increase in voltage beyond about 1600 V, line D, gives no further increase in count rate since no further pulses are brought above the threshold and the count rate registered is always proportional to the number of pulses above the threshold level.

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Die Hamilton-Jacobische Theorie fuer Doppelintegrale by Prange G.

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