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Abstract

The density distribution of supersonic isothermal turbulence plays a critical role in many astrophysical systems. It is commonly approximated by a lognormal distribution with a variance of $\sigma_{s,V}^2 \approx \ln(1 + b^2 M_{\rm V}^2),$ where $s \equiv \ln \rho/\rho_0,$ $M_{\rm V}$ is the rms volume-weighted Mach number, and $b$ is a parameter that depends on the driving mechanism, which can be solenoidal (divergence-free), compressive (curl-free), or a mix of the two. However, this neglects the correlation time of driving ($\tau_{\rm a}$), which plays a key role whenever compressive driving is significant. Here we conduct turbulence simulations spanning a wide range of Mach numbers, $1\lesssim M_{\rm V}\lesssim 10$, driving mechanisms, and $\tau_{\rm a}$ values. In the compressive case, we find that $\sigma_{s,V}^2$ scales approximately linearly with $M_{\rm V},$ and its dependence on $\tau_{\rm a}$ is $\sigma_{s,V}^2 \approx M_{\rm V} [1 + \frac{2}{3}(\lambda_{\rm a} + 1)\Theta(\lambda_{\rm a} + 1)]$, where $\lambda_{\rm a} \equiv \ln(\tau_{\rm a}/\tau_{\rm e})$, $\tau_{\rm e}$ is the eddy turnover time, and $\Theta$ is the Heaviside step function. Mixed-driven turbulence shows a weaker dependence on $\tau_{\rm a},$ and for solenoidally-driven turbulence, $\sigma_{s,V}^2 \approx \frac{1}{3}M_{\rm V}$, independent of $\tau_{\rm a}$ and consistent with the standard expression when $M_V \lesssim 10.$ The volume-weighted mean and skewness also show systematic trends with $M_{\rm V}$ and $\tau_{\rm a}$, deviating from lognormal expectations. For the mass-weighted density distribution, we observe significant broadening and skewness in compressively driven cases, especially at large $\tau_{\rm a}/\tau_{\rm e}$. These results provide a refined framework for modeling astrophysical turbulence.