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I am reading A. Zee, QFT in a nutshell, and in appendix 1 he has:

Meanwhile the principal value integral is defined by: $$\int dx\,{\cal P}{1\over x}f(x)~=~ \lim_{\epsilon \rightarrow 0} \int dx\, {x\over x^2+\epsilon^2}f(x)$$

Please can someone explain to me why this is the case? As I understood it the principal value integral is rather defined as $$\int_a^b dx\,{\cal P}{1\over x}f(x)~=~ \lim_{\epsilon \rightarrow 0^+} \int_a^{-\epsilon} dx\, {1\over x}f(x)+\lim_{\epsilon \rightarrow 0^+} \int_{\epsilon}^b dx\, {1\over x}f(x),$$ where $a<0<b$. But as far as I can see these two definitions are not equivalent.

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3 Answers

up vote 7 down vote accepted

The short answer is that the two principal value definitions agree on sufficiently well-behaved functions, but may disagree on sufficiently singular functions. For instance, on one hand $$\lim_{\epsilon\searrow 0} \int_{\mathbb{R}\backslash[-\epsilon,\epsilon]} \frac{\mathrm{d}x}{x^3}~=~0$$

is zero, while on the other hand

$$\lim_{\epsilon\searrow 0} \int_{\mathbb{R}} \frac{\mathrm{d}x}{x(x^2+\epsilon^2)}$$

is not well-defined, since the integrand is not integrable at $x=0$.

I) Here we would like to investigate further the definition of principal value $P\int\! \mathrm{d} x$.

Definition. Let $\chi=(\chi_{\epsilon})_{\epsilon>0}$ be a family of functions $\chi_{\epsilon}:\mathbb{R}\to [0,1]\subseteq \mathbb{R}$ that are:

  1. even functions $\chi_{\epsilon}(x)~=~\chi_{\epsilon}(-x),$

  2. Lebesgue measurable functions,

  3. $\chi_{\epsilon}(x)\nearrow 1$ pointwise almost everywhere for $\epsilon \searrow 0$.

Let us refer to such a function $\chi_{\epsilon}$ as a kernel function.

Examples of kernel functions $\chi_{\epsilon}$ are for instance:

  1. the characteristic function $$\chi_{\epsilon}(x) ~=~\chi^{\rm std}_{\epsilon}(x) ~:=~ 1_{\mathbb{R}\backslash[-\epsilon,\epsilon]}(x)$$ for the set $\mathbb{R}\backslash[-\epsilon,\epsilon]$. (This choice $\chi^{\rm std}$ will lead to the standard definition of principal value.)

  2. the continuous function $$\chi_{\epsilon}(x) ~=~ \chi^{a,b}_{\epsilon}(x) ~:=~ \frac{|x|^a}{|x|^a+ \epsilon^b},$$ where $a,b>0$ are two positive constants. (The choice $\chi^{2,2}$ will lead to the other definition of principal value mentioned by OP.)

  3. the constant unit function $\chi_{\epsilon}(x) ~=~ 1$. (Unsurprisingly, this latter choice will turn out to be not so useful.)


Definition. Define the set $V(\chi)$ of $\chi$-admissible functions as $$V(\chi)~:=~\left\{ f: \mathbb{R} \to \mathbb{C} ~\left|~ \begin{array}{c} f~\text{is Lebesgue measurable},\cr \forall \epsilon>0~:~~ \chi_{\epsilon} f~\in~ {\cal L}^1(\mathbb{R}), \cr \text{and} \cr \left(\int\! \mathrm{d}x~ \chi_{\epsilon}(x) f(x)\right)_{\epsilon>0} \text{is convergent for}~ \epsilon\searrow 0 \end{array}\right.\right\}. $$

Definition. If a function $f\in V(\chi)$ is $\chi$-admissible, we define the $\chi$-based principal value as $$P(\chi)\int\! \mathrm{d} x f(x)~:=~\lim_{\epsilon\searrow 0} \int\! \mathrm{d}x~ \chi_{\epsilon}(x) f(x).$$

Here ${\cal L}^1(\mathbb{R})$ denotes the set of functions that are Lebesgue integrable, i.e. functions that are Lebesgue measurable and whose absolute value has a finite integral. ${\cal L}^1(\mathbb{R})$ is an example of an ${\cal L}^p$ space.

III) It is not hard to see that:

  1. If $f\in{\cal L}^1(\mathbb{R})$ is Lebesgue integrable, then it is $\chi$-admissible $f\in V(\chi)$, and the principal value $$P(\chi)\int\! \mathrm{d} x ~f(x)~=~ \int\! \mathrm{d} x ~f(x)$$ is just the ordinary Lebesgue integral because of the Lebesgue dominated convergence theorem.

  2. The set $V(\chi)$ of $\chi$-admissible functions is a $\mathbb{C}$-vector space.

  3. If a function $f\in V(\chi)$ is $\chi$-admissible, so is the mirrored function $(x\mapsto f(-x))\in V(\chi)$, with same principal value.

  4. If an $\chi$-admissible function $f\in V(\chi)$ is odd, then $P(\chi)\int\! \mathrm{d} x~f(x) ~=~ 0$.

Thus it is enough to investigate even and odd functions.

Finally, let us investigate power functions $x\mapsto x^p$, $p\in\mathbb{R}$, which play an important role in practice as building blocks.

IV) Even functions. Let

$$g_{p,K}(x) ~:=~ 1_{[-K,K]}(x) |x|^p~=~g_{p,K}(-x)$$

be a truncated power function, where $p\in\mathbb{R}$ is a real power, and where $K>0$ is a positive truncation constant.

It is not hard to show that in the case of Example 1, 2, or 3,

$$g_{p,K}\in V(\chi) \qquad \Leftrightarrow \qquad p>-1\qquad \Leftrightarrow \qquad g_{p,K}\in {\cal L}^1(\mathbb{R}).$$

In the affirmative case $p>-1$, the principal value definitions based on the three Examples 1, 2, and 3 agree:

$$P(\chi)\int\! \mathrm{d} x ~g_{p,K}~=~\int\! \mathrm{d} x ~g_{p,K}~=~ \frac{2K^{p+1}}{p+1}.$$

V) Odd functions. Let

$$h_{p,K}(x) ~:=~ {\rm sgn}(x) 1_{[-K,K]}(x) |x|^p~=~-h_{p,K}(-x)$$

be a truncated power function, where $p\in\mathbb{R}$ is a real power, and where $K>0$ is a positive truncation constant. In the three Examples 1, 2, and 3, we get

  1. $h_{p,K}\in V(\chi^{\rm std})$ always,
  2. $h_{p,K}\in V(\chi^{a,b}) \qquad \Leftrightarrow \qquad p+a>-1$,
  3. $h_{p,K}\in V(1) \qquad \Leftrightarrow \qquad p>-1\qquad \Leftrightarrow \qquad h_{p,K}\in {\cal L}^1(\mathbb{R}).$
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Note that the right spelling is "principal value".

The formulae aren't identical but the results are the same whenever both definitions yield a well-defined expression. What matters is that we remove the leading logarithmic divergence on both sides from $x=0$ and we do so in a symmetric way with respect to $x\to -x$.

If you denote the second definition-based integral $Cut(\epsilon)$, $$ Cut(\epsilon) = \left(\int_{a}^{-\epsilon}+\int_{\epsilon}^b\right) \frac{dx}x f(x)$$ then I claim that there exists a weighting function $g(y)$ such that $$\int_0^{\infty} g(y) Cut(y) dy = \int dx\,\frac{x}{x^2+\epsilon^2}f(x) $$ so it reduces to the first definition-based integral. The function $g(y)$ is supported for $y$ of the same order as $\epsilon$ so the limit has the same effect on both expressions.

You may also see the equivalence of both expressions if you just Taylor-expand $f(x)$ near zero. Assuming that $f(x)$ is finite and well-behaved near $x=0$, it's easy to prove that both definitions yield the same result. The real purpose of the "principal value" terminology deals with branches of functions of complex variables. So you may also imagine that $f(x)$ is a meromorphic or holomorphic function of a complex $x$. The indefinite integral $\int f(x)/x$ has a logarithmic singularity around $x=0$ and one needs to define on which branch we are at. The principal value takes the average of the results one would get on the $+i\pi$ and $-i\pi$ branches for the logarithm of the negative numbers.

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Thanks for your help. I will correct the spelling. I think the $f(x) x/(x^2+\epsilon^2)$ in the question and answer should have integration limits from a to b. In that case I can see from examples that the two expressions are equivalent. I tried doing the Taylor series expansion to prove it but couldn't quite get the result. If anyone can point me to a reference where this is proved I would appreciate it. –  physicsphile Jul 3 '12 at 18:02
Dear physicsphile, please, this is really trivial. You won't find textbooks written about this stuff. Write $f(x)=a_0+a_1x+a_2 x^2+a_3 x^3+\dots$. Then integrate $f(x)/x$ from $a$ to $b$. Obviously, almost all the terms behave in the same way whether you omit the $(-\epsilon,+\epsilon)$ interval or not, whether you add the extra factor $x^2/(x^2+\epsilon^2)$, or not. The only exception is the absolute term $a_0$, i.e. integral of $a_0/x$, and both rules give you $a_0\ln|b/a|$ as the result of the integral in the limit $\epsilon\to 0$. Just try it. –  Luboš Motl Jul 4 '12 at 4:36
I see Weinberg in "The Quantum Theory of Fields I" describes its similarly to you on pg 113: "The function ${\cal P}/x\equiv x/(x^2+\epsilon^2)$ is just $1/x$ for $|x|\gg\epsilon$, and vanishes for $x\rightarrow 0$, so for $\epsilon\rightarrow 0$ it behaves just like the `principal value function' ${\cal P}/x$, which allows us to give meaning to integrals of $1/x$ times any smooth function of $x$, by excluding an infinitesimal interval around $x=0$." –  physicsphile Jul 5 '12 at 6:31
Good (but not really necessary) to see a confirmation by a famous Gentleman. –  Luboš Motl Jul 5 '12 at 6:46
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There are two issues here which recur frequently on this forum--- which functions can be regarded as distributions and what is the nature of convergence in the sense of distributions? Perhaps a mathematician's take might be of interest. It is standard that locally integrable functions can be regarded as distributions in a natural way, less so that the same applies to meromorphic functions (in the OP $\frac 1x$). The method is the same in both cases but is particularly simple in the one in hand. The function $\ln |x|$ is locally integrable and so a distribution. It has a distributional derivative and it is natural to define the distribution $\frac 1x$ to be this derivative. One can show quite easily that it then has all of the properties that one expects (including those of the approach using principal parts).

As to convergence, I will forego the precise definition. For almost all practical purposes, it suffices to know 2 facts. Firstly, if a sequence of functions converges locally in the $L^1$-norm, then it converges in the sense of distributions and, secondly, we can always differentiate such a convergent family and convergence is retained (the dream theorem of every calculus student).

After this preparation, the question in hand has a one line proof. The family $\frac 12 \ln (x^2+\epsilon^2)$ converges to $\ln|x|$ in the above sense and differentiating provides the required formula.

All the facts about distributions used here can be found in the monograph of L. Schwartz but I can recommend the elementary approach of J. Sebastiao e Silva which is expounded in "An Introduction to the Theory of Distributions" by Campos Ferreira. This uses only the tools of elementary one-dimensional calculus.

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Sounds interesting, but to be honest I am not quite sure of the connection to my question. Could you add in a bit more about how this applies to my question? Sorry if I am being a bit slow. –  physicsphile Jun 23 '13 at 2:06
Sorry, I must have misunderstood your question. I thought you were asking for a proof that the two ways of regarding $\frac 1 x$ as a distribition (via the principal value or the explicit limit) coincide. I also formulated it in a manner which suggests that these methods can be used in a number of related situations. Am quite prepared to delete (if I can) if you think that it is not relevant. –  mathuser5891 Jun 23 '13 at 4:43
I think you are answering it but maybe your answer is just not explicit enough for me to completely follow. But in general I understand that as Lubos Motl explained they are equivalent because if one concentrates around the crucial $x=0$ area and so takes $f(x)=A+Bx$ where $A$ and $B$ are constants then everything can be done analytically and the two methods clearly give the same answer. –  physicsphile Jun 23 '13 at 7:59
I suppose that my quarrel with the above answers is that theyare much too elaborate for something which is really very simple. In particular, the introduction of the complex plane is just muddying the water. The claim that one won't find textbooks written about this stuff is mildly surprising. Also the fact that these anwers manage without a clear definition of what it means for a family of functions to converge to a distribution. My main point is, I suppose, that a mathematically rigorous proof (as I provided) is often much simpler than a non-rigorous one. –  mathuser5891 Jun 23 '13 at 8:28
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