Proof of an infinite product formula

AI Thread Summary
The discussion centers on proving the infinite product formula \(\prod_{n=1}^{\infty} \left(1-\frac{q^2}{n^2} \right) = \frac{\sin(\pi q)}{\pi q}\). Participants mention that both sides are entire functions of \(q\) and share the same zeros at integer values. A reference to the Weierstrass factorization theorem is made as a potential proof method, alongside contour integration techniques, though these require knowledge of complex analysis. One contributor notes that a textbook on the Riemann Zeta Function contains simpler proofs as exercises, which can be worked through without advanced complex analysis. The conversation concludes with a mention of related identities inspired by the original formula, linking them to the multi zeta function.
Omri
Messages
34
Reaction score
0
Hi,

I am looking for a proof of the following formula:

\prod_{n=1}^{\infty} \left(1-\frac{q^2}{n^2} \right) = \frac{\sin(\pi q)}{\pi q}

Does anyone know where to find such a proof?

Thanks :smile:
 
Mathematics news on Phys.org
In any good textbook on Complex Analysis. Observe that both the left and the right hand side of your equation is an entire function of q (considered as a complex variable) and that the zeroes of both side coincide, more precisely the zeros are exactly the integers.

The theorem is called http://en.wikipedia.org/wiki/Weierstrass_factorization_theorem"
 
Last edited by a moderator:
First I must confess that I have never heard of the term "entire function" or about the factorization theorem. This is probably because I don't know everything about complex analysis, and have never taken a real university course in the subject (hence I wouldn't have a good textbook...). I only know about it from my tutor, who taught me the basics, and now he asked me to find a proof of the product above.

It is indeed easily seen that the zeros of both sides coincide, and that they are indeed the cases where q is an integer. But is that enough? And also, that factor (pi*q)^-1 on the right-hand side has now effect on the zeros, so in general I could have replaced it with any other numeric factor. Why should it be this specific one?

Thanks a lot for you help.
 
This can be proved as a special case of the http://en.wikipedia.org/wiki/Weierstrass_factorization_theorem" , or more directly by contour integration. However, that requires complex analysis.

A book I have (An introduction to the theory of the Riemann Zeta-Function by S.J. Patterson) contains a couple of simple proofs, given as exercises. They in fact prove
<br /> \pi\cot\pi z=z^{-1}+\sum_{n&gt;0}2z/(z^2-n^2)<br />
which is just the http://en.wikipedia.org/wiki/Logarithmic_derivative" of the identity you state.


The first proof only requires knowing that the only bounded entire functions (i.e. differentiable functions on the complex plane) are the constant functions, whereas the second doesn't require any complex analysis). I'll write it out as it appears in the book and let you work through the details of the proofs yourself.

1.12 Show that
<br /> f(z)=z^{-1}+\sum_{n&gt;0}2z/(z^2-n^2)<br />
can be expressed as
<br /> f(z)=\lim_{N\rightarrow\infty}\sum_{n=-N}^N(z-n)^{-1}.<br />
Deduce that
<br /> f(z+1)=f(z).<br />
Show also that if |Im(z)|>4 then |f(z)|<5. Conclude that
<br /> f(z)-\pi\cot\pi z<br />
is a constant. Finally show that this constant is zero.

And, the second proof.

1.13 Show that with f as in Exercise 1.12
<br /> \begin{align*}<br /> f(z)^2=&amp;z^{-2}+\sum_{n&gt;0}\left\{4z^2(z^2-n^2)^{-2}+4(z^2-n^2)^{-1}\right\}\\<br /> &amp; +4z^2\sum_{\substack{m,n&gt;0\\ m\not=n}}(z^2-n^2)^{-1}(z^2-m^2)^{-1}\\<br /> =&amp; z^{-2}+\sum_{n&gt;0}\left\{4z^2(z^2-n^2)^{-2}+4(z^2-n^2)^{-1}\right\}\\<br /> &amp; - 8z^2\sum_{n&gt;0}(z^2-n^2)^{-1}\sum_{\substack{m&gt;0\\ m\not=n}}(m^2-n^2)^{-1}.<br /> \end{align*}<br />
Show that
<br /> \sum_{\substack{m&gt;0\\ m\not=n}}(m^2-n^2)^{-1}=3/4n^2<br />
and deduce that
<br /> f^\prime(z)=-f(z)^2-6\sum_{n\ge 1}n^{-2}.<br />
Finally prove that
<br /> f(z)=\pi\cot\pi z<br />
and
<br /> \sum_{n&gt;0}n^{-2}=\pi^2/6.<br />
(This argument, which avoids the techniques of complex analysis and Fourier theory, is due to Eisenstein).
 
Last edited by a moderator:
Omri said:
Hi,

I am looking for a proof of the following formula:

\prod_{n=1}^{\infty} \left(1-\frac{q^2}{n^2} \right) = \frac{\sin(\pi q)}{\pi q}

Does anyone know where to find such a proof?

Thanks :smile:


I found this thread and I just wanted to say that this identity inspired me to find these identities:
  • - \frac{\pi ^2}{3!} = \displaystyle \sum_{j_1=1}^{\infty} -j_1^{-2}
  • \frac{\pi ^4}{5!} = \displaystyle \sum_{j_1,j_2=1 \atop j_1 \neq j_2}^{\infty} (j_1j_2)^{-2}
  • - \frac{\pi ^6}{7!} = \displaystyle \sum_{j_1,j_2,j_3=1 \atop j_i \neq j_k} - (j_1j_2j_3)^{-2}
  • \vdots
  • \frac{\pi ^{2n}}{(2n+1)!} = \displaystyle \sum_{j_1,...j_n=1 \atop j_i \neq j_k}^{\infty} (j_1j_2...j_n)^{-2}
  • \vdots

I explain how at my math blog http://www.futurebird.com/?p=156

It turns out these sums are something called the multi zeta function... Neat, no?
 
Suppose ,instead of the usual x,y coordinate system with an I basis vector along the x -axis and a corresponding j basis vector along the y-axis we instead have a different pair of basis vectors ,call them e and f along their respective axes. I have seen that this is an important subject in maths My question is what physical applications does such a model apply to? I am asking here because I have devoted quite a lot of time in the past to understanding convectors and the dual...
Insights auto threads is broken atm, so I'm manually creating these for new Insight articles. In Dirac’s Principles of Quantum Mechanics published in 1930 he introduced a “convenient notation” he referred to as a “delta function” which he treated as a continuum analog to the discrete Kronecker delta. The Kronecker delta is simply the indexed components of the identity operator in matrix algebra Source: https://www.physicsforums.com/insights/what-exactly-is-diracs-delta-function/ by...
Back
Top