occur simultaneously which infers the absence of the possible elastic scattering after chemical freeze-out [@Prorok:2004wi; @Prorok:2006ve].

The paper is organized as follows: in section-II, we give the formulation of the SHGM with an excluded volume correction and the method of inclusion of collective flow. In section-III, we show the results and in section-IV, we discuss the relation of $E_{T}/N_{ch}$ with various freeze-out criteria. In section V, we give the summary with outlook and open problems.

Formulation of The Model
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The formula for the number density of the i-th baryon in the Maxwell-Boltzmann’s statistics can be written as [@Mishra:2008tc] : $$n_i^{ex} = (1-R)I_i\lambda_i-I_i\lambda_i^2\frac{\partial{R}}{\partial{\lambda_i}},$$ where $\displaystyle R=\sum_in_i^{ex}V_i^0$ is the fractional occupied volume by the baryons [@Tiwari:2013wga]. $\displaystyle V_i^0= (4\pi\;r'^3)/3$ is the eigen-volume of each baryon having a hard-core radius $r'$ and $\lambda_i$ is the fugacity of the i-th baryon. Here we take $r'$ = 0.8$fm$, which is the only free parameter in the discussed model. $I_i$ is the momentum integral for baryons in the Boltzmann’s statistics. Eq. (1) can be reduced in the following form [@Tiwari:2013pva; @Tiwari:2013] :

&=&.

Here $y$ is the rapidity variable and $m_T=\sqrt{{m}^2+{p_T}^2}$ is the transverse mass. $E_i$ is the energy of the i-th baryon, V is 