the rate of dephasing, the time at which the maximum entanglement can be detected increases with the phase fluctuation.

Aiming at the prospect of increasing the degree of entanglement, $V_{s}$ is plotted against $time$ for $\theta=0.25$, $\gamma=0.75\Gamma$ and different values of the linear gain coefficient. As clearly shown in Fig. \[fig4\], the degree of entanglement increases with the linear gain coefficient in the early stages of the lasing process. Quite remarkably, in light of the oscillation, there is a window of time where the entanglement can decrease with the linear gain coefficient. Once again, at larger time scale the dependence of the entanglement on the linear gain coefficient tends to be much lesser when compared to the earlier times. Fitting things together may indicate that the nonclassical features and intensity of the cavity radiation take maximum values before they start damping oscillation that dies at longer time scale where the steady state properties begins to take effect.

In stronger driving regime
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The entanglement generated from coherently pumped correlated emission laser when $\eta=0$, $\gamma=\Gamma$ and $\theta=0$ was studied earlier using the criteria of DGCZ. It is generally noted that $\Delta u^{2}+\Delta v^{2}$ is very close to one at steady state 