Re: Optical Algorithm for RHIC PID

From: Michael Murray (murray@cyclotronmail.tamu.edu)
Date: Mon Sep 17 2001 - 09:42:27 EDT

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      Dear Borge,
              Julia's algorithm does not require a 
    fixed radius. Rather one would adapt the radius
    based on the knowledge of the momentum. For 
    each track of momentum P their will be 3 possible
    ring with the pion one being largest, then the
    kaons and finally the smallest for the proton 
    if it is above threshold.
               Yours Michael
    
    Quoting Borge Svane Nielsen <borge@alf.nbi.dk>:
    
    > Hi all,
    > 
    > Concerning ring finding algoritms, I think one should be careful
    > assuming
    > fixed radius in our case. We have pions, kaons and protons, many of
    > them
    > close to the Cherenkov threshold, i.e. not saturated rings. 
    > 
    > To use Julia's method would mean first to determine the momentum and
    > then
    > assume in sequence that the particle is a pion/kaon/proton, do the ring
    > finding and fitting to a circle and then at the end produce
    > probabilities
    > for each of the hypotheses. This is indeed a viable method, but did
    > does
    > introduce systematic effects. Adding knowledge about the centre of the
    > circle is just one more parameter in the game. This kind of method is
    > reported as one option in the paper I quoted.
    > 
    > The other type of method relies a little more on knowing the centre,
    > but
    > is probably less biased when it comes to pre-knowledge about the
    > radius. It is basically Claus' concept: start with a centre, histogram
    > radii from the centre and determine a best radius - possibly followed by
    > a
    > refitting of the hits in the found ring to a (slightly) shifted centre
    > and
    > radius.
    > 
    > In either case, the worst problem is to suppress background hits not
    > belonging to the ring. It pays to have a good understanding of the
    > background sources: white noise, other reconstructable tracks, not
    > reconstructable tracks, etc. The background is typically not flat,
    > because
    > the geometry in the RICH is limited, i.e. you are always close to the
    > edge
    > of the detector.
    > 
    > Another thing relating to Claus' mail. Gain matching is of limited
    > value. All you really need to know is if the signal is above threshold
    > to
    > be counted as a photon. Trying to count photons in a given channel from
    > the measured pulse height is difficult to impossible due to the signal
    > spread of a single photon. I am not sure, Claus, if your dR signals
    > were
    > weighted with ADC count. I think they shouldn't be.
    > 
    > Cheers,
    > Borge
    > 
    > +------------------------------------------------------------------------+
    > | Børge Svane Nielsen                 E-mail:  borge@nbi.dk             
    > |
    > | Technical Coordinator               http://www.nbi.dk/TECHI           
    > |
    > | Niels Bohr Institute                Phone:   (+45) 3532 5433          
    > |
    > | University of Copenhagen            Fax:     (+45) 3532 5465          
    > |
    > | Blegdamsvej 17,  DK-2100 Copenhagen O,  Denmark                       
    > |
    > +------------------------------------------------------------------------+
    > 
    > 
    
    
    
    Michael Murray, Cyclotron TAMU, 979 845 1411 x 273, Fax 1899
    



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