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are usually located at µ$_{B}$ < 200 MeV whereas chiral CEP have much larger µ$_{B}$ . So there is a good chance for observing CEP at RHIC by using energy scan [47]. We also find that CEP obtained in our models almost overlaps with the points on the freezeout curve. The freezeout point occurs close to RHIC energy and hence the fluctuations in multiplicity etc. can experimentally provide a clear signal for CEP. 

Before we conclude we would like to discuss the recent lattice data obtained by de For- crand and Philipsen [12, 13] who used 2+1 and 3 flavors staggered fermions and a taylor expansion in µ$_{q}$/T to study the curvature of the critical surface at very light quark masses 

