Hi Elke, That's a good idea to start thinking about requests for any sort of electronics people will need over the next few months, especially in light of CD-3. We currently have 4 10-bit fADC-250 under tests/debugging and I don't expect these will be released until early 2008. We have been discussing the possibility of an engineering run, 5-10 boards, in the fADC group for use by users and for testing the trigger system. Please be aware that it make take up to 8 weeks before we get any new boards (ordering components, PCB fabrication, assembly, test). I will be away on Wednesday, 11/21/07 for the Thanksgiving holiday. Best regards, Fernando Elke-Caroline Aschenauer wrote: On Fri, 16 Nov 2007, Matthew Shepherd wrote: Fernando and Matt, i think we all agree test are needed we can do what was suggested in the report. Currently we have 5 250MHz FADCs. I suggest that on Wednesday in the weekly Hall D meeting we find out how many FADCs pleople might need for test stands and than see we have to produce more. bye elkeDate: Fri, 16 Nov 2007 16:46:11 -0500 From: Matthew Shepherd <mashephe@indiana.edu> To: Fernando J. Barbosa <barbosa@jlab.org> Cc: halld-cal@jlab.org Subject: Re: Flash ADC Timing Hi Fernando, I understand the claims in the document are rather optimistic; however, the fact of the matter is that we probably just need timing resolution roughly on the scale of sampling rate to suppress beam- related out of time noise. If you have a real fADC that is ready for use we're happy to take it and get it setup and running here. This would serve many purposes -- probably most important at this point is that we could use the real PMT, light guide, base, and fADC that we plan for the actual experiment to readout just one bar and probe the low energy threshold of the calorimeter using cosmic rays (and guidance from simulation). -Matt On Nov 16, 2007, at 3:01 PM, Fernando J. Barbosa wrote:Hi Matt, I am familiar with those documents and I recall that at the time we started developing the fADC (~2 years?), I suggested that someone needed to take some real data with Paul's single-channel prototype and try doing the prescribed fittings, etc. To the best of my knowledge, no one in the collaboration has done that. Referring to the document, the algorithm relies on finding the exact pulse peak and getting the two preceding samples to determine the 50% time, for instance. The exact peak was determined from sampling at 2.5 GHz (400 ps intervals) and fitting the data with a 9th degree polynomial. The data was then "degraded" to provide the equivalent of 8 or 10-bit, 250 MHz (4 ns intervals) sampling. Note that the exact peak is critical for the algorithm to provide the quoted resolution, although these details are missing from the document. The real fADC, and sampling at 250 MHz, will not provide a sample of the true pulse peak. I believe that such "fluctuation" will degrade the effective resolution considerably. So, I suggest that this needs to be checked with a real fADC, perform the algorithm on real raw fADC data (offline) and determined the effective resolution that can be achieved by this method. Obtaining 400 ps resolution from 4 ns data points and from 10 ns pulse rise times seems difficult to me. We actually may have to shape (i.e. slow) the pulse to get more samples on the leading edge of the pulse. Once the algorithm is well understood, it will need to be implemented in a relatively simple/compact manner to fit within the resources of the FPGAs or board memory. Eventually, any data that is passed up the chain must be balanced with the backplane bandwidth. Let me suggest you set up a test with the real PMTs/bases/ scintillator/fiber/laser and get data with a real fADC, a TDC and CFD. We could lend you one fADC-250 to get the raw data. Let me know what you decide and how I can help. Best regards, Fernando Matthew Shepherd wrote:Hi all, The study I was referring to has been linked to the FCAL page here: http://www.jlab.org/Hall-D/software/wiki/index.php/FCAL This work was done about 3 years ago and claims a resolution of about ~160 ps can be achieved. This is far better than is actually needed to push down backgrounds. I think Scott had in mind another application: using the FCAL to determine the event start time. The algorithm does a transformation of the leading edge of the pulse to determine the start time and depends on having the two samples before the peak on the leading edge. I believe Paul had planned to implement this in a simple lookup table which would require about 65K of memory on the chip. Perhaps that could be optimized even more. It was never investigated in detail mainly because it seemed like something relatively easy to implement. All of these buffers will need some processing -- the drift chambers will also depend on the timing algorithms that are built into the flash ADCs. -Matt <barbosa.vcf>( `,_' )+=-+=-+=-+=-+=-+=-+=-+=-+=-+=-+=-+=-+=-+=-+=-+=-+= ) `\ - / '. | + | `, Elke-Caroline Aschenauer = \,_ `-/ - ,&&&&&V Jefferson Lab + ,&&&&&&&&: HALL-D 12C / F381 121-A Atlantic Avenue = ,&&&&&&&&&&; Mailstop: 12H5 Hampton, VA 23664 - | |&&&&&&&;\ 12000 Jefferson Ave + | | :_) _ Newport News, VA 23606 Tel.: 001-757-224-1216 = | | ;--' | Mail: elke@jlab.org Mobil: 001-757-256-5224 - '--' `-.--. | + \_ | |---' Tel.: 001-757-269-5352 = `-._\__/ Fax.: 001-757-269-6248 - +=-+=-+=-+=-+=-+=-+=-+=-+=-+=-+=-+=-+=-+=-+=-+=-+=-+=-+=-+=-+ |
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