C+C pions rapidity fits with temperature formula 
y = C * T^3 * ( (m0/T)^2 + 2*m0/(T*cosh(y*y_cm)) + 2/(cosh(y*y_cm)**2) ) *exp(-m0*cosh(y*y_cm)/T) 
where y = (y_lab-y_cm)/y_cm 
with 2 parameters C and T. 
Constants: m0=139.57,   y_cm=0.677 for 1 GeV and 0.907 for 2 GeV 
(e.g. S Sadovski PhD page 78 eq 7.17) 
First check of the formula on the "ideal" PLUTO distribution for 1 GeV with T=58 MeV and A_2=0 (and blast=0):
 
-  PLUTO right: fit within measured range, left: fit in full range - both work well, see parameter p1 == T 
    
 
 
Now fit of PLUTO distribution for 1 GeV with T=58 MeV and anisotropy A_2=0.34:
 
-  PLUTO right: fit within measured range, left: fit in full range: in full range the fitted slope changed by 16 MeV, chi^2 high. In measured range the
 
 
T slope cannot be recovered.
    
Now exp. data fit (together with fit of UrQMD data within measured range and full range) for CC at 1 GeV and 2 GeV. Results are summarized below in the table:
 
-  C+C 1 AGeV: 
    
 
 
 
-  C+C 2 AGeV: 
    
 
 
C+C 1 AGeV 
	
		
			|     | 
			 exp.  | 
			    | 
			 UrQMD  | 
			    | 
			 UrQMD  | 
			    | 
		
		
			|     | 
			    | 
			    | 
			 exp. range  | 
			    | 
			 full range fit  | 
			    | 
		
		
			|     | 
			 T  | 
			 chi2/NDF  | 
			 T  | 
			 chi2/NDF  | 
			 T  | 
			 chi2/NDF  | 
		
		
			|  pi+  | 
			 119+-24  | 
			 2.7/20  | 
			 1530+-2040  | 
			 4256/20  | 
			 172.4+-0.5  | 
			 16600/39  | 
		
		
			|  pi-  | 
			 114+-22  | 
			 4.6/20  | 
			 1634+-2057  | 
			 6072/20  | 
			 184.0+-0.6  | 
			 23400/39  | 
		
	
C+C 2 AGeV 
	
		
			|     | 
			 exp.  | 
			    | 
			 UrQMD  | 
			    | 
			 UrQMD  | 
			    | 
		
		
			|     | 
			    | 
			    | 
			 exp. range  | 
			    | 
			 full range fit  | 
			    | 
		
		
			|     | 
			 T  | 
			 chi2/NDF  | 
			 T  | 
			 chi2/NDF  | 
			 T  | 
			 chi2/NDF  | 
		
		
			|  pi+  | 
			 2900+-111  | 
			 31/13  | 
			 2600+-2050  | 
			 7280/13  | 
			 315.4+-1.4  | 
			 49200/39  | 
		
		
			|  pi-  | 
			 2677+-53  | 
			 26/13  | 
			 2393+-5  | 
			 6449/13  | 
			 310.0+-1.3  | 
			 48300/39  | 
		
	
-- 
PavelTlusty - 28 May 2008