June 11, 2002, updated June 25
 
 
2nd method (Dan) to get centrality at 20 GeV 
          
 See 
a)  
all_raw.gif  
b)  
all_norm.gif  
c) 
au130+au200.gif  
d)  
au20+au200.gif  
 
 The abcisa factors in the figures for au130 and au200 are shown.
One observes good consistency in the scaling from au200 and au130.
The results shown in the above figures seem consistent with the method 
used earlier at 20 GeV suggested by Zhangbu. Updated results of this 
method, including 20, 130 and 200 GeV are presented 
here  
 
This 
Fig.   
shows the good agreement observed at 20, 130 and 200 GeV. The 
points at 0% cross section were obtained using Zhangbu's method. All the 
points above 0% for 130 and 200 GeV were determined previously at STAR. 
The points above 0% cross section for 20 GeV were obtained using the 2nd 
method discussed here.
 
 Here are details of what was done on the 2nd method suggested by 
Dan Cebra:
0) Files : 
au20: 
/auto/stardata/starspec3/flow_pDST_production/reco/minBias22GeVZDC/ReversedHalfField/P02ge/2001/
au130: /auto/stardata/starspec/schweda/pDST/P01hi/minbias/global/
au200: 
/auto/stardata/starspec2/flow_pDST_production/reco/MinBiasVertex/ReversedFullField/P01gk/2001/
 
1) It was verified independently that mUncorrNegMult and mUncorrPosMult 
indeed correspond do the number of tracks as defined in Masashi's code 
that produces pDst. See Masashi's e-mail to Roppon: 
------------------------------------------------------------------
mUncorrNegMult and mUncorrPosMult are copied from StEventUtilities
function uncorrectedNumberOfNegativePrimaries(const StEvent&) and
uncorrectedNumberOfPositivePrimaries(cont StEvent&).
It is number of tracks that are:
  number of Fit points >=10
  |eta|<=0.5
  DCA < 3.0 cm
For detail, please look at $STAR/StRoot/StEventUtilities/StuRefMult.hh.
mMultEta seems to be defined as number of tracks of which |eta|<0.75.
It is counted by a variable goodTracksEta in StFlowMaker.cxx in SL02e.
I used SL02e to produced 20GeV Au+Au flow pico DSTs, because it is
P02ge production. 
                                                           Best regards, 
                                                           Masashi Kaneta 
------------------------------------------------------------------------
2) Histograms were made for Nch= mUncorrNegMult+mUncorrPosMult, as defined 
in the code. x-bin= 800. Printed out the x and y values.
3) In a spread sheet program (Kaleid) the x-axis for au130 
was multiplied by a factor x130 such that the spectra  along the x-axis 
matches (by eye) the one for au20. Also the y-axis of the au130 
spectra was scaled to match (by eye) the spectra at au20. 
  Similarly, the x-axis for au200 was multiplied by a factor x200 such 
that the spectra  along the x-axis 
matches (by eye) the one for au20. Also the y-axis of the au200
spectra was scaled to match (by eye) the spectra at au20. 
 
The present  factors x130 and x200 extracted are listed
in the figures and here: 
au130: x130=0.652 
au200: x200=0.562 
 
4) Finally, the centrality values for au20 derived from those 
determined for au130, as quoted by Manuel, are listed next. The last 
column was
 obtained by multiplying the au130 values 
by x130 = 0.652, as determined above.
 
cent au130 au20 
------------------- 
05% 431.00 281 
10% 364.00 237 
20% 260.00 170 
30% 179.00 117 
40% 118.00 76 
50% 74.000 48 
60% 43.000 28 
70% 22.000 14 
80% 10.000 7