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Let $F$ be a tempered distribution on $\mathbb{R}^2$ and $n \in \mathbb{N}$ be a fixed natural number. I wonder what exactly it means by

$\lvert F(x,y) \rvert \leq \lvert x-y \rvert^{-n}$ where $x,y \in \mathbb{R}$.

I run into such notations when dealing with a sequence of tempered distributions and their integral representation.

By definition, $F$ is a continuous linear functional on the Schwartz space $\mathcal{S}(\mathbb{R}^2)$. So, I guess the above bound should be expressed in terms of Schwartz functions.

Could anyone please clarify for me?

Add : A reference context is this paper, with p.211 Eqn (6) in particular.

Add 2 : For those who down-voted it, could you please tell me what you don't like about this problem, for the sake of being constructive?

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    $\begingroup$ It is implicit in the hypotheses of Thm.5.1 there, which contains Eq.(6), that the $\mathfrak{S}(x_1,\ldots,x_n)$ (or your $F(x,y)$) are just ordinary functions away from the diagonals, not arbitrary distributions. This is very tersely explained in the text just preceding the theorem, but (again implicitly) the authors assume that the reader is already familiar with what Wightman/Schwinger functions are. So your original interpretation, which led to the confusion, is not correct. $\endgroup$ Commented Mar 8 at 14:28
  • $\begingroup$ @IgorKhavkine What do you mean by ordinary functions? The text clearly says they are tempered distributions so that they are integrated against test functions....I believe that you totally misunderstood the text.. $\endgroup$
    – Isaac
    Commented Mar 8 at 14:59
  • $\begingroup$ In fact the whole paper is about distributions.. $\endgroup$
    – Isaac
    Commented Mar 8 at 15:00
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    $\begingroup$ For the record, I did not vote on this question. The last and only productive thing that I can add is that your question can be fully resolved by a careful rereading of Thm.5.1 and the paragraph before it. $\endgroup$ Commented Mar 8 at 16:47
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    $\begingroup$ For distributions $T$ and $T_1$ on $\Omega$ and open $U\subseteq\Omega$ one can define $|\,T\,|\le T_1$ on $U$ to mean that $|\,T\,\varphi\,|\le T_1\varphi$ hold for nonnegative test functions $\varphi$ with support included in $U$. One can define $T$ to be "real" by requiring that it maps real test functions to real numbers, and one can define "positivity" of $T$ on $U$ by requiring that $0\le T\,\varphi$ hold for any nonnegative test function $\varphi$ with support included in $U$. For real $T$ then $|\,T\,|\le T_1$ on $U$ reduces to $T_1$ and $T_1-T$ and $T_1+T$ being positive on $U$. $\endgroup$
    – TaQ
    Commented Mar 11 at 5:40

3 Answers 3

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I'll try to explain what Igor meant in his comments in a different way, maybe it helps.

  1. Of course, any tempered distribution is a distribution in the broader sense - more precisely, any compactly supported test function is tempered, and the seminorms defining the topology of $\mathscr{S}(\mathbb{R}^n)$ are majorized by seminorms defining the topology of $\mathscr{C}^\infty(K)$ for all $K\subset\mathbb{R}^n$ compact with nonvoid interior.

  2. Any distribution $u$ in $\mathbb{R}^n$ (tempered or not, by 1.) may be restricted to a nonvoid open subset $U$ thereof by restricting to test functions supported in $U$. The result is, of course, a distribution $u|_U$ in $U$ (which is no longer tempered because temperedness only has meaning if $U=\mathbb{R}^n$), for the needed seminorm bounds guaranteeing the continuity of $u|_U$ are clearly inherited from those of $u$.

  3. A basic theorem in distribution theory tells us that if two continuous functions $f,g$ on $U$ as in 2. are such that $$ \int_U f\phi\,dx=\int_U g\phi\,dx$$ for all test functions $\phi$ compactly supported in $U$, then $f=g$. This means that if $f$ is a continuous function on $U$ such that $$u|_U(\phi)=u(\phi)=\int_U f\phi\,dx$$ for all such test functions, then $f$ is the only continuous function on $U$ with such a property, and therefore we may identify $u|_U$ with (the smearing of compactly supported test functions on $U$ with) $f$. More generally, this can be done with $f$ any locally integrable function on $U$, but then the identification is only up to a zero-measure subset of $U$ because of the integral in the rhs. This freedom disappears if $f$ is required to be continuous. In the case of $n$-point Schwinger functions on $\mathbb{R}^d$, $$U=\mathbb{R}^{nd}\smallsetminus\{(x_1,\cdots,x_n)\in\mathbb{R}^{nd}\ |\ x_i\in\mathbb{R}^d\ ,i=1,\ldots,n\ ,\,x_j=x_k\text{ for some }j\neq k\}$$ and $f$ is a real analytic (hence continuous) function, so $f$ is the unique such function.

1.-3. together explain what your inequality means - to wit, it implicitly states that the restriction $F|_U$ of $F$ to the open subset $U=\mathbb{R}^2\smallsetminus\{(x,x)\ |\ x\in\mathbb{R}\}$ is identified with (the smearing of compactly supported test functions on $U$ with) a(n at least locally integrable) function $f$ on $U$ which then satisfies the given inequality, since the latter's rhs is clearly only defined in $U$. In the context of the paper, $f$ is real analytic and therefore continuous as in the end of 3., so $f$ is unique and thus the given inequality has a clear, unambiguous meaning.

Hope it helped somehow to understand Igor's comments. Sorry if my answer sounds pedantic at places, but I wanted to be sure not to leave any stone unturned.

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    $\begingroup$ In due time: as Abdelmalek said at the end of its answer, strictly speaking it may not always be the case that if one starts with an analytic function $f$ on $U$ as in the end of 3. above, the boundary values of $f$ on the big diagonal exist in the tempered distribution sense. One needs polynomial bounds such as the one in the OP to ensure that, otherwise one generally only obtains that way what is called a "hyperfunction", which is even more singular than a distribution. $\endgroup$ Commented Mar 8 at 19:15
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    $\begingroup$ The first paper by Osterwalder and Schrader on the reconstruction of the Wightman $n$-point functions from the corresponding Schwinger $n$-point functions overlooked that point, and a proper discussion of this matter in the context of hyperfunction theory was provided in their second paper (as well as in an independent paper by Glaser). $\endgroup$ Commented Mar 8 at 19:17
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    $\begingroup$ I should also qualify my 1st comment: "boundary values of $f$" are really meant in the sense of holomorphic functions viewed as distributions. The imaginary part of their argument is seen as parameters sent to zero in the distribution sense while keeping the real part at the complement of $U$ - depending on the direction one approaches zero, one may get a different boundary value. $\endgroup$ Commented Mar 8 at 20:43
  • $\begingroup$ Generally there are many ways to continuously extend a distribution $u$ from $\mathscr{D}(U)$ to $\mathscr{D}(\mathbb{R}^n)$, taking boundary values of $u$ identified with a real analytic function $f$ on $U$, which then admits a unique extension to a holomorphic function on an open domain in $\mathbb{C}^n$ containing $U$, is a particular case. These extensions are collectively called renormalizations, and their existence is ensured by the Hahn-Banach theorem. $\endgroup$ Commented Mar 8 at 20:47
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    $\begingroup$ @Isaac we may continue this discussion by email, no problem, also because we're kind of departing from the strict matter of the OP. $\endgroup$ Commented Mar 8 at 21:10
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Distributions and ordinary functions are two different things, however, there are bridges between them, going both ways, modulo some technical hypotheses. If $f$ is an ordinary function one can associate to it a distribution that sends a smooth test function g to $\int fg$, i.e., by "integrating against $f$" as mentioned in the article. For this to make sense, i.e., for the integral to converge and the resulting linear form to be continuous, the needed technical hypothesis is that $f$ is locally $L^1$. Conversely, given a distribution $T$ on $\Omega$, it has a singular support $K$, which allows one to produce a smooth function $f$ by "restriction" to $\Omega\backslash K$. Namely, that means that if $g$ is a test function with support in $\Omega\backslash K$, then $T(g)=\int_{\Omega\backslash K} fg$.

Traditionally, Schwinger functions are defined as ordinary functions with domain given by the complement of the big diagonal, i.e., for non-coinciding points. Then, one can ask if one can associate a distribution to that. This is a bit tricky because this does not use the standard spaces of distributions say PDE folks work with.

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This is just a comment (but I am not entitled) to put on record that there is a simple and natural way to answer the question in the title (the meaning of the claim $|F(x,y)|\leq |x-y|^{-n}$ for any (tempered) distribution $F$ of two variables). First note that any bounded, measurable function defines a unique distribution (true even for a locally integrable function). Secondly, one can always multiply a distribution by a smooth function. Hence it is natural to say that an (arbitrary) distribution $F$ satisfies the inequality whenever the distribution $F(x,y)(x-y)^n$ corresponds to a function in the ball of $L^\infty$ in the above sense.

I would emphasise that this is a reply to the question of how to ascribe meaning to the statement in the title, independent of any explicit context.

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