The invariantly
harmonic functions in the unit ball ${\Bbb B}^n$ in ${\Bbb C}^n$ are those annihilated by the
Bergman Laplacian $\Delta$. The Poisson-Szeg\"o kernel $P(z,\zeta)$ solves the Dirichlet problem for
$\Delta$: if $f\in C(S^n)$, the Poisson-Szeg\"o transform of $f$, $P[f](z)=\int_{S^n}P(z,\zeta)
f(\zeta)\,d\sigma(\zeta),$ where $d\sigma$ is the normalized Lebesgue measure on $S^n$, is the unique
invariantly harmonic function $u$ in ${\Bbb B}^n$, continuous up to the boundary, such that $u=f$ on
$S^n$. The Poisson-Szeg\"o transform establishes, loosely speaking, a one-to-one correspondence
between function theory in $S^n$ and invariantly harmonic function theory in ${\Bbb B}^n$. When
$n\geq 2$, it is natural to consider on $S^n$ function spaces related to its natural non-isotropic
metric, for these are the spaces arising from complex analysis. In the paper, different
characterizations of such spaces of smooth functions are given in terms of their invariantly harmonic
extensions, using maximal functions and area integrals, as in the corresponding Euclidean theory.
Particular attention is given to characterization in terms of purely radial or purely tangential
derivatives. The smoothness is measured in two different scales: that of Sobolev spaces and that of
Lipschitz spaces, including BMO and Besov spaces.
1991 Mathematics Subject Classification:
32A35, 32A37, 32M15, 42B25.