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By Arthur Pehr Robert Wadlund

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The same principle applies to pixels   Electronics Part I The weighting field FQ is calculated by applying unit potential to the signal electrode and zero to all others. Note that for charge movement this field is irrelevant. It is not an electric field with the unit V/cm, but a field that is not derived from a physical quantity, so its unit is simply /cm. For a more detailed discussion, see Spieler ( pp –). In a simple parallel-electrode detector the weighting field is uniform, so for a constant charge velocity the signal current is constant.

Signal Fluctuations . . . . . . . . . . . . . . . . . .   Signal Formation . . . . . . . . . . . . . . . . . . .  Electronic Noise . . . . . . . . . Electronic Noise Levels . . . . . . . Noise in Amplifiers . . . . . . . . Noise Versus Dynamic Range . . . . . . . . . ............... ............... . . . . . . . .  Signal Charge Measurements . . . . . Charge-Sensitive Amplifiers . . . . .

C. Grupen, I. /----_, © Springer-Verlag Berlin Heidelberg    Electronics Part I Abstract: Detectors come in many different forms and apply a wide range of technologies, but their principles can be understood by applying basic physics. In analyzing the signal acquisition, relatively simple models provide sufficient information to assess the effect of different readout schemes. This chapter discusses signal formation in various types of detectors and fluctuations in signal magnitude.

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