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William Angerer - Department of Physics and Astronomy - University ...

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191<br />

PMT<br />

to photon counter<br />

snubber<br />

Figure 7.7: Snubber schematic to reduce current pulse ringing. A signal is reflected<br />

from the short coaxial cable <strong>and</strong> reshapes the current pulse from the P:\IT. The<br />

length <strong>of</strong> the cable determines the delay <strong>of</strong> the reflected pulse <strong>and</strong> the resistance <strong>of</strong><br />

the variable resistor determines the magnitude <strong>of</strong> the reflected signal. We adjusted<br />

the variable resistor while observing the current pulse on an oscilloscope to minimize<br />

pulse ringing. This figure was adapted from reference [lllJ.<br />

a main pulse followed by several smaller pulses. If the height <strong>of</strong> these secondary<br />

oscillations had been above the discriminator level, the pulse was counted twice. By<br />

placing a variable resistor at a distance <strong>of</strong> 6 inches from the PMT <strong>and</strong> in parallel with<br />

the signal cable to the photon counter [lllJ, we introduced electrical feedback into<br />

the signal (see Fig. 7.7). This feedback reshaped the pulse <strong>and</strong> damped the pulse<br />

ringing. Hence, we ensured each signal pulse was counted only once.<br />

7.2.3 Registering <strong>and</strong> Positioning Samples<br />

In contrast to second-harmonic generation from a Si wafer, which is homogeneous.<br />

many applications <strong>of</strong> second-harmonic microscopy require accurate <strong>and</strong> reproducible<br />

control <strong>of</strong> the sample position. Reproducibility <strong>and</strong> accuracy <strong>of</strong> the sample position<br />

Reproduced with permission <strong>of</strong> the copyright owner. Further reproduction prohibited without permission.

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