Difference between revisions of "CDC 23 01 2008"

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m (News on the preAmp - Gerard's visit)
m (News on the preAmp - Gerard's visit)
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== News on the preAmp - Gerard's visit ==
 
== News on the preAmp - Gerard's visit ==
Today Gerard started to look at the the CDC setup in order to get the new preAmp working. Here are some things he found:
+
Today Gerard has started to look at the the CDC setup in order to get the new preAmp working. Here are some things he found:
  
 
*) Our self made differential probe causes the oscillations... they disappear when Gerard uses his own differential probe.
 
*) Our self made differential probe causes the oscillations... they disappear when Gerard uses his own differential probe.

Revision as of 16:45, 21 January 2008

News on the preAmp - Gerard's visit

Today Gerard has started to look at the the CDC setup in order to get the new preAmp working. Here are some things he found:

  • ) Our self made differential probe causes the oscillations... they disappear when Gerard uses his own differential probe.
  • ) In order to reduce the noise a different LV power supply was used - the ground connections between HVDB (HV Distribution Board) and the CDC where beefed. The LEMO-BNC adaptors where removed. Apparently the type we use at CMU has a known problem (bad grounding) which I did not know of.

In figure 1,2,3, and 4 one can see output signals from the cable (CDC + HVDB + new preAMp + cable) with the CDC at 1950, 2050, 2050, and 1850 V respectively, some signals that saturate can be observed. We used a Ru-106 source.

figure 1: New preAmp output signal with the CDC at 1950V.
figure 2: New preAmp output signal with the CDC at 2050V.
figure 3: New preAmp output signal with the CDC at 2050V.
figure 4: New preAmp output signal with the CDC at 1850V.

To be continued...

Understanding the drift time spectrum

As mentioned on the Collaboration meeting the drift time spectrum shown in figure 5 is not understood. One expects a drop-off around 1100 ns = 900 + 200 ns, with 200 ns the maximum drift time in the straw.

figure 5: two typical drift time spectra.

First test was to look at the drift time spectra containing only hits from tracks. These spectra had the same shape. The second test was to look if the fADC was really running at 200 MHz. Therefore it was ran at 100 MHz and a signal with high amplitude was compared with the 200MHz ran fADC. In figure 6, the signal taken with the fADC ran at 100 MHz is shown in figure 7 the same but now with the fADC ran at 200 MHz. One can see clearly the difference between the two signals.

figure 6: Signal vs time (100 MHz).
figure 7: Signal vs time (200 MHz).