Changes

The speed of the amplifier response is one of the chief challenges. The transistors themselves, at a bandwidth of ~4 GHz, cover the expected signal spectrum well enough. However, points in the amplifier circuit where currents are injected present integrators with the RC time set by the effective AC coupling capacitance and input impedance of the following stage. Since reduction of effective capacitance at the SiPM circuit stage is not an option (the effective charge deposited per SiPM pixel discharge decreases) the input impedance was minimized. This is accomplished both in the amplifier and summing circuit input stages with injection on the transistor emitter (as opposed to base). The effective resistance is thus on the order of 20 Ω (generally quiescent current-dependent value) as opposed to βR_E as would be seen looking into the base.

The speed of the amplifier response is one of the chief challenges. The transistors themselves, at a bandwidth of ~4 GHz, cover the expected signal spectrum well enough. However, points in the amplifier circuit where currents are injected present integrators with the RC time set by the effective AC coupling capacitance and input impedance of the following stage. Since reduction of effective capacitance at the SiPM circuit stage is not an option (the effective charge deposited per SiPM pixel discharge decreases) the input impedance was minimized. This is accomplished both in the amplifier and summing circuit input stages with injection on the transistor emitter (as opposed to base). The effective resistance is thus on the order of 20 Ω (generally quiescent current-dependent value) as opposed to βR_E as would be seen looking into the base.

The spectral response of the modeled amplifier in its low and high gain setting s(see [[SiPM Amplifier Optimization]]) is shown here. Note the beginning of the roll-off in the response (due to the integration described above) within the spectral envelope of the input signal. The stretching seen in the time-domain plot is due to this attenuation of high frequency components. However, given the ADC's sampling rate of 250 MSPs shortening the pulse further (flattening the frequency response across the entire signal spectrum) is not necessary.

The spectral response of the modeled amplifier in its low and high gain setting (see [[SiPM Amplifier Optimization]]) is shown here. Note the beginning of the roll-off in the response (due to the integration described above) within the spectral envelope of the input signal. The stretching seen in the time-domain plot is due to this attenuation of high frequency components. However, given the ADC's sampling rate of 250 MSPs shortening the pulse further (flattening the frequency response across the entire signal spectrum) is not necessary.