Yes, it seems related to the Oberth effect. Starting from the solar orbit, we need $\Delta v$ to enter an orbit to Mars. By energy conservation the velocity of the spaceship at launch from Earth has to be $$v_0 = \sqrt{v_{\text{esc}}^2+\Delta v^2} \ ,$$ where $v_{\text{esc}}$ is the escape velocity. For $v_{\text{esc}} \gg \Delta v$, we find that the $\Delta v^{\prime}$ on top of the escape velocity is $$\Delta v^{\prime} \simeq \frac{1}{2}\frac{\Delta v^2}{v_{\text{esc}}} \ .$$ This formula relates your Delta-v's in your question. We observe that $\Delta v^{\prime}$ becomes smaller the bigger the escape velocity from Earth. Bigger escape velocity means that you're deeper in the gravitational well. By the Oberth effect, a small Delta-v deep in the gravitational well has a bigger effect outside of the well.
In fact, irrespectively of the above approximation, we always have $$\Delta v^{\prime} = \sqrt{v_{\text{esc}}^2+\Delta v^2}-v_{\text{esc}} \leqslant \Delta v \ .$$