Dirac writes down the following formula on page 61 of his "Principles of quantum mechanics": $\frac{d}{dx}\log x = \frac{1}{x} i\pi\delta(x)$, see http://adsabs.harvard.edu/abs/1947pqm..book.....D for the exact reference (but no text). What is the best way of formalizing this to a mathematician's satisfaction?

16$\begingroup$ I'm sure Dirac was thinking that ln(x)=lnx+i H(x)π, where H(x) is the Heavside step function. $\endgroup$– Tom CopelandApr 15, 2013 at 10:27

5$\begingroup$ @Tom, in the text surrounding that formula, Dirac states precisely that (though less explicitly). $\endgroup$– Igor KhavkineApr 15, 2013 at 11:21

9$\begingroup$ Your information seems to be out of date. We mathematicians have been satisfied with $H$ and its derivatives for over 60 years. Also, the last equation in your comment has a spurious absolute value sign. $\endgroup$– S. Carnahan ♦Apr 15, 2013 at 12:40

2$\begingroup$ @katz: Scott is right, you probably just missed this detail. If $x<0$, the argument of $log(x)$ is still negative. You want to write $log(x) = log(x) + \pi i H(x)$. $\endgroup$– Ryan BudneyApr 15, 2013 at 19:07

13$\begingroup$ I would write Dirac's formula as $\log(x+i0^+)= p.v.\frac{1}{x}−i\pi \delta(x)$, and this is now a perfectly rigorous equation in the space of distributions (using whatever branch of the logarithm one wishes which does not cut ${\bf R}+i0^+$), indeed it is just the Plemelj formula given in the answers below, written in distributional form. $\endgroup$– Terry TaoApr 15, 2013 at 21:50
6 Answers
In integral form, this amounts to the SokhotskiPlemelj theorem:
$\lim_{\epsilon\rightarrow 0^{+}}\int_{\infty}^{\infty}dx f(x) \frac{d}{dx}\log (x+i\epsilon)=i\pi f(0)+{\cal P}\int_{\infty}^{\infty}dx f(x)\frac{1}{x}$.
The symbol ${\cal P}$ indicates that the Cauchy principal value of the integral is to be taken. Formalization then amounts to stating the conditions on $f$ so that the principal value integral exists.
The logarithm for $x<0$ is defined as $\log x= \log(x) + i\pi$. You can avoid the delta function by including the absolute value signs in the logarithm:
$\int_{\infty}^{\infty}dx f(x) \frac{d}{dx}\logx={\cal P}\int_{\infty}^{\infty}dx f(x)\frac{1}{x}$.

$\begingroup$ Thanks, but somehow that looks less elegant than Dirac's formula. $\endgroup$ Apr 15, 2013 at 9:07

8$\begingroup$ less elegant, perhaps, but you do need to specify that the principal value is to be taken, otherwise the formula is not correct (or not complete). $\endgroup$ Apr 15, 2013 at 9:16

$\begingroup$ Thanks for the reference. I think it should be "Plemelj". One can specify a branch of log and still hope for a more direct formalisation with functions having local values. $\endgroup$ Apr 15, 2013 at 12:54


12$\begingroup$ You may cirticize this as "less elegant" but others can criticize the original Dirac formula as "less rigorous". $\endgroup$ Apr 15, 2013 at 20:47
Questions about distributions, usually involving the $\delta$ distribution ("function"), are of frequent occurrence on this and related sites. Since they are often treated in a rather cavalier fashion, I would like to attempt to answer this query in some detail. The basic problem lies in the interpretation of the functions $\frac 1 x$ and $\log x$ (notabene not $\log x $) as distributions. As a preliminary remark, it is not surprising that theoretical physicists are guided by their physical intuition and not by mathematical rigour in dealing with such questions and it is perfectly acceptable for mathematicians to proceed in the same way in formulating such conjectures. However, since this is a mathematical forum, one does have the right to expect that the final formulation of the solution conforms to the usual standards of mathematical rigour (as is implied in the OP). In fact it is rather disquieting that this is often not the case, since this task can be achieved by elementary methods which have been on record in the primary and secondary literature for at least 50 years.
For the example in question (and, indeed, for most of the examples in such forums), one need only be cognisant of the following simple facts about distributions.
$1$. Every continuous function on the reals, better, every locally integrable function, determines in a natural way a distribution.
$2$. There is a notion of convergence for distributions. For our purposes, it suffices to know that if a sequence of continuous functions converges uniformly on compacts, then it converges in the sense of distributions. In fact, local $L^1$ convergence suffices.
$3$. The dream theorem of every freshman calculus student holdsif a sequence of distributions converges, then the sequence obtained by differentiating term by term also converges.
We can now turn to the above query. Note that the problem lies in the fact that while the function $\log x$, being locally integrable, determines a distribution, the same is not true a priori for $\frac 1 x$ and $\log x $. In these two cases, we have to proceed in a more delicate manner.
Firstly, note that the function $\log x$ is locally integrable and so is a distribution. More importantly the same is true for its derivative in the distributional sense. It is then rather natural to define this derivative to be the distribution $\frac 1 x$.
The case of the distribution $\log x$ is rather more subtle. In this case we resort to the complex logarithm. y thus we define, for nonzero $\epsilon $, the distribution $\log(x+i\epsilon)$ to be $\logx+i \arctan \frac \epsilon x$ (i.e., we are using the principal branch of the complex logarithm). We now define the distribution $\log x $ to be the limit of this distribution as $\epsilon$ tends to zero. At this point, we see that we get different values, depending on whether we consider the limit $\epsilon \to 0_+$ or $\epsilon \to 0_$. If we now differentiate this equation we obtain the required formula.
To conclude, a few remarks.
The above approach is due to the portuguese mathematician J. Sebastião e Silva who developed it in the context of his axiomatic approach to the theory of distributions.
Sadly, the definitive monograph on his approach that he was preparing 40 years ago was never completed, due to his premature passing.
However, the elementary part has been presented in the book "An introduction to the theory of distributions" by Campos Ferreira which is based on lectures at the University of Lisbon (ca. 1970) and this contains the material described here.
The above is a special case of the family of distributions $x^\lambda$ for general $\lambda$ (even complex) which is developed in detail in the above reference. They are also described in the standard four volume text of Gelfand and Silov.
The distribution $\frac 1 x$ is also treated by Laurent Schwartz who used the Hadamard principal value (the latter was his great uncle by marriage). The connection with the above approach can easily be established by considering the truncated function $\log_\epsilon$ (which is set equal to zero on the interval $]\epsilon,\epsilon[$), letting $\epsilon$ tend to zero and differentiating.
The ambiguity in the definition of the distribution $\log x$ is no more disconcerting than that in the definition of the logarithm function for complex arguments. In a more sophisticated approach this distribution would not be defined on the real line but on the natural domain of definition of the latter, i.e., on the unversal covering of the punctured plane.

1$\begingroup$ Really, weren't the results for the limiting case of the derivative of the log worked out fairly rigorously by Cauchy and Poisson in their work on potential theory long before 20'th century mathematicians put a formal dress on them? $\endgroup$ Apr 15, 2013 at 23:49

$\begingroup$ See, e.g., the OP's paper "A Cauchy–Dirac delta function" by Mikhail G. Katz and David Tall arxiv.org/abs/1206.0119 See Zemanian "Distribution theory and transform analysis" for precise discussions of different nascent delta functions. $\endgroup$ Nov 3, 2019 at 14:04
Here is another context where something like this shows up, though I don't know how or if it's related to your question. Consider the simple left $\mathscr{D}$ module on $\mathbf{A}^1$ generated by $\text{log}x$, and similarly for $1/x$ and $\delta(x)$ $$\mathscr{D}\cdot\text{log}x\ =\ \mathscr{D}/\mathscr{D}\partial x\partial \ = \ k[x]\log x +k[x,x^{1}],$$ $$\mathscr{D}\cdot 1/x\ =\ \mathscr{D}/\mathscr{D}\partial x \ = \ k[x,x^{1}],$$ $$\mathscr{D}\cdot\delta(x)\ =\ \mathscr{D}/\mathscr{D}x \ = \ k[\partial]\delta(x)$$ where the global sections of $\mathscr{D}$ is the algebra $k[x,\partial]$ with $[x,\partial]=1$. There is an exact sequence of $\mathscr{D}$ modules $$0 \ \longrightarrow \ \mathscr{D}\cdot 1/x \ \longrightarrow \ \mathscr{D}\cdot\log x\ \longrightarrow \ \mathscr{D}\cdot \delta(x)\ \longrightarrow \ 0$$ which in plain language just means that the subspace $k[x,x^{1}]$ is preserved by $x$ and $\partial$.
Note that to get this $``\log=1/x+\delta"$ principle to work you really have to work with the whole $\mathscr{D}$ modules, not just consider elements of them. Indeed, the element $\log x\in\mathscr{D}\cdot\log x$ just satisfies $\partial \log x=1/x$.
$$ \lim_{\epsilon \rightarrow0} \int_{\epsilon}^{+\epsilon}\frac{d\ln x}{dx} dx = \lim_{\epsilon \rightarrow0}[\ln \epsilon\ln(\epsilon)] \\ \ln(\epsilon)= \ln\epsilon+ i\Theta \\ $$ choose the principle value for the angle$$ \Theta=\theta= \pi \\ \lim_{\epsilon \rightarrow0} \int_{\epsilon}^{+\epsilon}d\ln x = \lim_{\epsilon \rightarrow0}[\ln \epsilon\ln(\epsilon)] =\lim_{\epsilon \rightarrow0}[\ln \epsilon\ln(\epsilon)i\pi]=i\pi $$
$$\lim_{\epsilon \rightarrow0} \int_{\epsilon}^{+\epsilon}\frac{1}{x}dx =0$$ Because 1/x is a odd function, thus its integral vanished.
The left hand side equals to $i\pi$, thus we need add $i\pi$ to the right hand side.
Above all, we can obtain
$$ \lim_{\epsilon \rightarrow0} \int_{\epsilon}^{+\epsilon}\frac{d\ln x}{dx} dx = \lim_{\epsilon \rightarrow0} \int_{\epsilon}^{+\epsilon}\frac{1}{x}dx i\pi= \lim_{\epsilon \rightarrow0} \int_{\epsilon}^{+\epsilon}\frac{1}{x} i\pi\delta(x)\ dx$$
According to the inside parts of integrals, we finally got $$ \frac{d\ln x}{dx} =\frac{1}{x} i\pi\delta(x) $$
Belatedly fleshing out some of my initial comments, the following analysis suggests how naturally Dirac would have concluded that the derivative of $\ln(x)=\ln(x)+ i\pi H(x) $ has a delta function from his exposure to potential theory developed in the 19th century.
Note first
$$\frac{d}{dz}\ln(z)= \frac{1}{z} = \frac{xiy}{x^2+y^2},$$
regardless of how the branch cut for the logarithm is chosen. The notion of a Dirac delta function follows naturally from a limiting Cauchy contour integration over a rectangular contour centered symmetrically about the origin whose length is $2L$ and height $2\epsilon.$ Let $f(z)$ be analytic within this contour. Then starting the contour at the lower left corner of the rectangle,
$$\frac{1}{2 \pi i} \oint_{rect} \frac{f(z)}{z}dz = f(0)$$
$$= \frac{1}{2 \pi i} [ \int_{Li\epsilon}^{Li\epsilon} + \int_{Li\epsilon}^{L+i\epsilon} + \int_{L+i\epsilon}^{L+i\epsilon} + \int_{L+i\epsilon}^{Li\epsilon} ] \frac{f(z)}{z}dz.$$
Since we will let $\epsilon$ tend to zero, the two integrals over the vertical edges of the rectangle vanish in the limit, so consider just the two horizontal edges.
$$I(L,\epsilon) = \frac{1}{2 \pi i} [ \int_{Li\epsilon}^{Li\epsilon} + \int_{L+i\epsilon}^{L+i\epsilon}] \frac{f(z)}{z}dx.$$
$$=\frac{1}{2 \pi i} \int_{L}^{L} [ \frac{f(xi\epsilon)}{xi\epsilon} \frac{f(x+i\epsilon)}{x+i\epsilon} ]dx.$$
Assuming the region of convergence is sufficient for our contour, Taylor series give
$$f(x\pm i\epsilon) = f(0) + f^{'}(0)(x\pm i\epsilon)+ ... .$$
Then our integral reduces to
$$I(L,\epsilon) = \frac{1}{2 \pi i} \int_{L}^{L} [ \frac{f(0))}{xi\epsilon} \frac{f(0)}{x+i\epsilon} ]dx$$
since the first derivative terms will cancel out and the subtraction of other terms in
$$\sum_{n=2}^{\infty} \frac{f^{n}(0)}{n!}[(xi\epsilon)^{n1}(x+i\epsilon)^{n1}]$$
leave summands of degree one or more in $\epsilon$ and will vanish as epsilon vanishes, so we need consider in the limit only
$$I(L,\epsilon)=f(0)\frac{1}{2 \pi i} \int_{L}^{L} [ \frac{1}{xi\epsilon} \frac{1}{x+i\epsilon} ]dx$$
$$=f(0)\frac{1}{\pi} \int_{L}^{L} \frac{\epsilon}{x^2+\epsilon^2} dx$$
$$=f(0)\frac{2}{ \pi} \arctan(L/\epsilon)=f(0)R(L,\epsilon),$$
and as $\epsilon$ tends to zero,
$$ \lim_{\epsilon \rightarrow 0^{+}} \frac{2}{\pi}\arctan(L/\epsilon)=1.$$
Note, of course, if the function is entire and diminishes sufficiently fast at positive and negative infinity, then the contour integrals on the horizontal edges will vanish as $L$ tends to infinity even for finite $\epsilon$ and $R(L,\epsilon)$ will tend to one in this case as well.
We can conclude that the integrand
$$\delta_\epsilon(x) = \frac{1}{\pi} \frac{\epsilon}{x^2+\epsilon^2} $$
is a nascent Dirac delta function, having, in addition to the sifting property in the limit, the requisite properties $\delta_\epsilon(x)= \delta_\epsilon(x)$ and
$$\lim_{\epsilon \rightarrow 0^{+}} \int_{L}^{L} f(x) \delta_\epsilon(ax) dx = \lim_{\epsilon \rightarrow 0} \int_{L}^{L} f(x) \frac{\delta_\epsilon(x)}{a} dx = f(0)/a.$$
The integrand
$$\delta_y(x) = \frac{1}{\pi} \frac{y}{x^2+y^2} $$
is called the Poisson kernel associated to the Poisson integral
$$u(x,y) = \int_{\infty}^{\infty} f(t)\delta_y(xt)dt,$$
giving the harmonic function $u(x,y)$, i.e., $\nabla^2 u(x,y) = 0$, in the upper halfplane that has the boundary value $f(x)$ on the real axis.
Aside from the origin,
$$\frac{1}{\pi z}= \delta_x(y)i\delta_y(x),$$
is analytic, so its real and imaginary components, $\delta_x(y)$ and $\delta_y(x)$, are a harmonic pair. They are proportional to the components of the electric field in any plane intersected orthogonally at the origin by an infinite line of uniform charge density. (Careful, the indices $x,y$ do not represent differentiation here, but rather analytic continuation of the Dirac delta function obtained as $x$ or $y$ tend to zero, within an integral.)
With degrees in electrical engineering, math, and physics from British universities, Dirac was certainly familiar with the Poisson and Dirichlet Laplacian equations and the Poisson and, more generally, Green function integrals in electrostatics as well as Heaviside's contributions to telegraphy and vector analysis.
Note that the electrostatic interpretation with the force on an electron directed away from the wire determines the choice of $\ln(x) = \lnx+i \pi H(x)$ rather than $\ln(x) = \ln(x) i \pi H(x)$, eliminating the ambiguity of an otherwise arbitrary mathematical choice, and equivalently, the choice of direction (CW or CCW) of the contour of integration and final eval as $f(0)$ rather than $f(0)$. The purely formal mathematical interpretations don't eliminate this ambiguity.
Some related history:
"The CauchyDirac Delta Function" by Katz and Tall
"7 Green’s Functions and Nonhomogeneous Problems" Chapter 7 of the book Introduction to Partial Differential Equations by Herman. Cf. pages 225 and 262.
"An Essay on the Application of mathematical Analysis to the theories of Electricity and Magnetism" by Green
"Masters of Theory: Cambridge and the Rise of Mathematical Physics" by Andrew Warwick. See p. 508 for a note on Heaviside's influence on Dirac.
Added 1/29/22:
There is also the closely related hyperfunction approach
$$H(x) = \frac{1}{2\pi i} (\ln(xi0)  \ln(x+i0)).$$
Grothendieck, Feynman, and no doubt earlier researchers used essentially this approach (see the comment on the “iε” cabbala below).
Added 9/22/22: Historical note on the HeavisideDirac delta function
In Section 526 of Electromagnetic Theory Vol. 3, The Solution of Definite Integrals by Differential Transformation, Heaviside reviews his introduction of the delta function/operator in his earlier work.
He defines $t_1 = \frac{\partial}{\partial t}$ and $x_1 = \frac{\partial}{\partial x}$. Then with 1$=H(x) =(1+sign(x))/2$ or $=H(t)$ depending on the context, the Heaviside step function, he calls $t_11$ a unit impulse at $t=0$ and $x_11$ a unit impulse at $x=0$, which, in modern notation, become
$t_11=\partial_tH(t) = \delta(t)$ and $x_11=\partial_xH(x) = \delta(x)$.
Then. for $x,t > 0$, his eqn. (8) for the sifting property of the delta function
$$f(t) = \int_0^\infty \; f(x) \; (e^{x_1t}x_1)dx$$
may be reexpressed, for any real $x$ and $t$ with $H(0)=1/2$, as
$$H(t)f(t) = \int_{\infty}^\infty \;H(x) f(x) \; (e^{t\partial_x}\partial_xH(x))dx = \int_{\infty}^\infty \;H(x) f(x) \; e^{t\partial_x}\delta(x)dx$$
$$ = \int_{\infty}^\infty \;H(x) f(x) \; \delta(xt))dx. $$
Heaviside and Dirac, following Heaviside, had the temerity to relate their delta fcts/operators to the derivative of a discontinuous functiona touch of wizardry and the inspiration for a rigorous foundation to generalized functions/distribution theory.

$\begingroup$ Dirac was keenly interested in projective geometry and once stated it influenced his development of quantum field theory. Certainly he was aware as Ahflors said, “Riemann virtually puts equality signs between twodimensional potential theory and complex function theory.” (From "Physics in Riemann's mathematical papers" by Papadopoulos.) $\endgroup$ Jul 2, 2020 at 4:40

$\begingroup$ More on Riemann and potential theory in "Bernhard Riemann, a(rche)typical mathematicalphysicist?" by Emilio Elizalde. $\endgroup$ Jul 2, 2020 at 4:42

$\begingroup$ For more on Dirac's interest in projective geometry (and a great book on the development of QM), see Darrigol, Olivier. From cNumbers to qNumbers: The Classical Analogy in the History of Quantum Theory. Berkeley: University of California Press, 1992. ark.cdlib.org/ark:/13030/ft4t1nb2gv $\endgroup$ Aug 26, 2020 at 0:03

$\begingroup$ Also Ooguri, "Lecture 9: Riemann surfaces, elliptic functions" ocw.utokyo.ac.jp/lecture_files/sci_03/9/notes/en/ooguri09.pdf $\endgroup$ Sep 9, 2020 at 16:31

$\begingroup$ See p.160 of Mathematics for Physics, A Guided Tour for Graduate Students by Stone and Goldbart: "... the Plemelj equations are commonly encoded in physics papers via the “iε” cabbala ... ." $\endgroup$ Oct 27, 2020 at 15:13
The question is not meaningful since $\ln x$ is not defined for $x\le 0$. You may define, with derivatives in the distribution sense $$ f(x)=\ln\vert x\vert\text{ (even)},\quad f'(x)=pv\frac1{x} \text{ (odd, homogeneous degree 1)} $$ $$ g(x)=\ln(x+i0)=\lim_{\epsilon\rightarrow 0_+}\ln(x+i\epsilon),\quad g'(x)=\frac{1}{x+i0}= pv\frac1{x}i\pi \delta, \text{(homogeneous degree 1)} $$ where the latter formula follows from $$ \ln(z)=\oint_{[1,z]}\frac{d\xi}{\xi},\quad z\in \mathbb C\backslash \mathbb R_. $$ By analytic continuation we have (for $z\in \mathbb C\backslash \mathbb R_$) $e^{\ln z}=z$ and with $H=\mathbf 1_{\mathbb R_+}$ $$ \ln(x+i0)=\ln\vert x\vert +i\pi H(x)\Longrightarrow g'(x)=\frac{1}{x+i0}= pv\frac1{x}i\pi \delta. $$ Taking the complex conjugate of $g$ gives you the definition of $\frac{1}{xi0}$.