The term "Euclidean harmonic analysis" means the studying of the classical Fourier transform for functions on $\mathbb{R}^n$ or $\mathbb{T}^n$. This include the basic properties of the Fourier transform such as Plancherel's theorem for $L^2$ functions as well as other more sophisticated techniques and results, for example, the Fourier transform for $L^p$ functions, Hardy-Littlewood maximal function, Littlewood-Paley functionals, etc.
My question is if there is any application for these theories to geometry? What I know about applications of the Fourier transform to geometry is that it can be used to define Sobolev spaces for $L^2$ functions on manifolds and then pseudodifferential operators. Combining these with the topological $K$-theory, one can prove the Atiyah-Singer index theorem which gives a lot of interesting results for compact manifolds. A standard reference for this is Lawson's book, Spin Geometry.
But to do this we don't need anything that is essentially more delicate then the Plancherel's theorem or formulae such as $\widehat{\partial_x^\alpha u}(\xi)=\xi^\alpha \widehat{u}(\xi)$. So do all those $L^p$ results or Hardy-Littlewood maximal functions, etc. help us understand more about geometry? If so, does anyone has some reference for this kind of results?