This is very late, but maybe it's worth it anyway...
The time-scale plane is not the same as the time-frequency plane, although it might be useful as well. Signals at different places in the time scale plane are related by $x(t) \rightarrow x(\Delta s(t-\Delta t))$, where $\Delta s$ moves you up (or down) in scale and $\Delta t$ shifts you in time. The same transformation in the time-frequency plane is $x(t) \rightarrow x(t-\Delta t) e^{i \Delta \omega t}$, where $\Delta \omega$ is a shift in frequency. If your signal $x(t)$ is a sine wave, the two transformations are the same.
The DWT, or discrete wavelet transform, computes only discrete scales, just as the FFT computes only discrete frequencies. And the comment that @Spacey made above that the DWT is not translation-invariant is correct. This occurs because at every stage of the DWT, the signal is decimated by two. This makes the DWT faster than the FFT, $O(N)$, but also destroys the translation-invariance.
So using the DWT to examine the time-scale plane isn't going to get you very far. This is especially true because the scales "visited" by the DWT are separated by factors of two, and are much less dense than the coverage you can get in the time-frequency plane with the FFT. You need to use a wavelet transform that is translation-invariant, sometimes called the undecimated wavelet transform, among many other names. Even then, you still have the sparsity of the computed scale samples to contend with.
Furthermore, it's often desirable to think of locations in the time-scale plane as having an energy density. This approach is facilitated by using an analytic wavelet, such as the complex Morlet wavelet mentioned earlier. One method that balances translation-invariance and analyticity against computation time is the complex dual-tree wavelet transform. Doing the same thing in the time-frequency plane is perhaps simpler: do an approximate Hilbert transform on your signal first by doing an FFT, zeroing out all the negative frequencies, followed by an IFFT.
If the intuition that correlation looks for similarity in time and coherence looks for similarity in frequency is correct, then you might be better off sticking to the time-frequency plane. It's certainly simpler to compute, and it's easy to refine the sampling along the frequency axis. None of the approaches mentioned above address sampling the scale axis more densely. To do that, you pretty much have to go to the continuous wavelet transform, although there might be something else out there that I'm not aware of. If you have Matlab, follow the link above and have at it.