Plots 1: (Click here)
  Since in the experiments, efficiency and purity of detector plays a big role in results, so we simulate effect of efficiency and purity on final results in our analysis. we asume efficeincy & purity varies as gaussian with a mean and sigma. These mean and sigma differs for postive and negative particles.
Now we have taken following case shown in table and calculate values of D's. Plot values of  D's Vs N_sub.
Set
 Mean of Strangeness (MeanS)
 Mean for Baryon (MeanB). Sigma for both Strangeness & Baryon
Pure HIJING


First 0.13
 0.10
 0.1
Second
 0.13
 0.10
 0.05
Third
 0.13
 0.10
 0.02


black line = Pure HIJING
red line = First set
green line = Second set
pink line = Third Set


example:
       effS= gRandom->Gaus(MeanS, Sigma);
       effB= gRandom->Gaus(MeanB, Sigma);
       puritySpos= gRandom->Gaus(MeanS ,Sigma);
       puritySneg= gRandom->Gaus(MeanS, Sigma);
       purityBpos= gRandom->Gaus(MeanB, Sigma);
       purityBneg= gRandom->Gaus(MeanB, Sigma);
      TOT_Baryon = tot_baryon*effB + (tot_impurityPos*purityBpos-tot_impurityNeg*purityBneg);
       Float_t TOT_Strange = tot_strange*effS + (tot_impurityPos*puritySpos-tot_impurityNeg*puritySneg);
    
where
tot_impurityPos = all postive pions  & tot_impurityNeg = all negative pions,  which we  consider as impuirty

Plots 2 (Click here)
Plots show's how the values of Baryon, Strange and Hypercharge

Black line is for pure HIJING
Red line is for  first set
Green line is for  second set
Purple line is for third set


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