On Wed, Mar 24, 2010 at 5:19 PM, Brad Sawatzky <<a href="mailto:brads@jlab.org">brads@jlab.org</a>> wrote:<br><div class="gmail_quote"><blockquote class="gmail_quote">
It is the 2ns RF clock that drives the RF in the accelerator. The JLab<br>
"CW" beam is really pulsed with a 2ns period.<br></blockquote><div><br>Thanks --<br><br>A plot of (either) of these variables for p = 0.60 GeV is a problem. The crate mapping is wrong in the DB -- similar to my Scintillator TDCs and ADCs a while back.<br>
<br>I found the proper mapping for = 1.70 GeV -- so I can send this update out in addition to the S1,S2m stuff once it's all done.<br><br>Speaking of -- now that I have the RF time -- I remember Chiranjib discussing his use of this for the scintillator calibrations... I'm not quite sure of why this makes sense to look at this? <br>
</div></div><br clear="all"><br><br>-----------------------------------------------------------<br>David Flay<br>Physics Department<br>Temple University<br>Philadelphia, PA 19122 <br><br>office: Barton Hall, BA319<br>phone: (215) 204-1331<br>
<br>e-mail: <a href="mailto:flay@jlab.org">flay@jlab.org</a> <br> <a href="mailto:flay@temple.edu">flay@temple.edu</a><br><br>website: <a href="http://www.jlab.org/~flay">http://www.jlab.org/~flay</a><br> <a href="http://quarks.temple.edu">http://quarks.temple.edu</a><br>
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