I want to study the behavior of this singular distribution $T \in \mathcal{D}'(\mathbb{R}^n)$, defined by
\begin{equation} T(\phi)(x) = \int_{\mathbb{R}^n} \frac{\phi(y)}{|x-y|^n} \mathrm{d}y, \tag{1} \end{equation}
with $\phi(x) \geq 0$, $\phi \in L^1(\mathbb{R}^n)$. I want to know if $T$ has a name, classified under what type of distributions, and its properties.
There are similar distributions. Namely if the denominator of the kernel was $(x-y)^n$ instead of $|x-y|^n$, then $T$ was just Riesz transform (Hilbert transform if $n=1$), and the integral can have a finite principal value.
In more general setting, if the kernel of the distribution $T(\phi)(x) = \int K_{\Omega}(x,y) \phi(y) \mathrm{d}y$ is of the form
\begin{equation} K_{\Omega}(x) = \frac{\Omega(x/|x|)}{|x|^n} \end{equation}
with the condition that $\Omega$ is zero mean value on unit sphere $\mathbb{S}^{n-1}$, then this is Calderon-Zygmund kernel, and I can relate the Calderon-Zygmund decomposition (Grafakos, section 5.2.1).
But the distribution of (1) is non of the above forms. becasue, its kernel $K_{\Omega}(x) = 1/|x|^n$ and $\Omega(x/|x|) =1 $ is not zero mean. I am wondering what are the name of such distributions, can they be studied by Calderon-Zygmund, or so they have their own properties? For instance, unless $\phi(0) = 0$, $T$ is always unbounded.
I am also looking for some reference suggestions. Thank you!
It is not a distribution on $\Bbb{R}^n$ because $$ \lim_{r \to 0}\int_{\mathbb{R}^n} \phi(x)\frac{1_{|x|> r}}{|x|^n} d^n x $$ diverges whenever $\phi(0) \ne 0$. What is a (tempered) distribution is $$<T,\phi>= \int_{\mathbb{R}^n} (\phi(x)-\phi(0) 1_{|x|<1})\frac{1}{|x|^n} d^n x $$ And $$T \ast \phi(y)= \int_{\mathbb{R}^n} (\phi(y-x)-\phi(y) 1_{|x|<1})\frac{1}{|x|^n} d^n x $$ The choice of $1_{|x|<1}$ is non-canonical but you can call it $$T=fp(\frac1{|x|^n})$$ (finite part) everyone will understand that you meant $$<fp(\frac1{|x|^n}),\phi>= \int_{\mathbb{R}^n} (\phi(x)-\phi(0) \psi(x))\frac{1}{|x|^n} d^n x=<T+c\delta ,\phi>$$ for some $\psi(0) = 1$