Step 1: The Dulong-Petit law states that the molar specific heat of a solid approaches the constant value \(C_V = 3R\), independent of temperature.
Step 2: Both the Einstein and Debye models reduce to \(3R\) in the high-temperature limit. For the Einstein model, when \(kT \gg h\nu\) the factor \(\left(\dfrac{h\nu}{kT}\right)^2 \dfrac{e^{h\nu/kT}}{(e^{h\nu/kT}-1)^2} \to 1\), giving \(C_V \to 3R\).
Step 3: For the Debye model, when \(T \gg \theta_D\) the Debye integral gives \(C_V \to 3R\) as well.
Step 4: Therefore both laws merge with Dulong-Petit at high temperature.
\[\boxed{\text{High } T}\]