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At a characteristic voltage, an avalanche of electrons are formed all over the anode, called “Townsend Avalanche”.
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At this point the pulse height is constant irrespective of the energy of the radiation that triggers the count.
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If we define a term called amplification (A) that represents the ratio of the total ion-electron pairs collected to the number primarily formed by the radiation, its value in GM region reaches ~ 106.
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The value of A in the Ionisation chamber plateau is one.
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It gradually increases in the proportional region.
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The reason for the pulse height being independent of the initial number of ion-electron pair is that the amplification is so high that it saturates the detector, cripples the electric field and prevents further multiplication.
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This plateau is called the GM Plateau.
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It has been argued that as the voltage is increased, the avalanche spreads radially and increases the count rate or the pulse height, though the increase is small.
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Thus, the plateau has a slight positive slope.
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As the voltage is increased, at a characteristic voltage, the gas breaks down and goes into a continuous discharge region.
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The detector will fail if taken to continuous discharge region.
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The slope of the GM Plateau is defined as a percentage increase in count rate per 100 V.
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It is given as

.