<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Solved Problems on Nam Le</title><link>https://blog.namln.org/en/tags/solved-problems/</link><description>Recent content in Solved Problems on Nam Le</description><generator>Hugo</generator><language>en-US</language><lastBuildDate>Thu, 28 May 2026 00:00:00 +0000</lastBuildDate><atom:link href="https://blog.namln.org/en/tags/solved-problems/index.xml" rel="self" type="application/rss+xml"/><item><title>Inequality for Square-Summable Complex Series</title><link>https://blog.namln.org/en/posts/inequality-square-summable-complex-series/</link><pubDate>Thu, 28 May 2026 00:00:00 +0000</pubDate><guid>https://blog.namln.org/en/posts/inequality-square-summable-complex-series/</guid><description>&lt;p&gt;Some inequalities look formidable until the right decomposition makes them
transparent. The conjecture below, posed by Zoltan Retkes on the
&lt;a href="http://www.openproblemgarden.org/op/inequality_for_square_summable_complex_series"&gt;Open Problem Garden&lt;/a&gt;
in 2012 with a £10 prize attached, is one such case: once the dyadic structure of
the positive integers is made explicit, the proof reduces to two classical facts.&lt;/p&gt;
&lt;div style="padding:10px 14px; border:2px solid dodgerblue; border-radius:6px; margin:16px 0;"&gt;
&lt;span style="color:dodgerblue; font-weight:bold;"&gt;Conjecture (Retkes, 2012), now proved&lt;/span&gt;
&lt;p&gt;For all $\alpha = (\alpha_1, \alpha_2, \ldots) \in \ell^2(\mathbb{C})$,
$$\sum_{n \geq 1} |\alpha_n|^2 \geq \frac{6}{\pi^2} \sum_{k \geq 0}
\left|, \sum_{l \geq 0} \frac{\alpha_{2^k(2l+1)}}{l+1} ,\right|^2.$$&lt;/p&gt;
&lt;/div&gt;
&lt;p&gt;The conjecture was confirmed by an anonymous comment on the problem page in November
2013. A self-contained proof and an extension to $\ell^p$ were subsequently published
by Ibragimov and Salimova in &lt;em&gt;Elemente der Mathematik&lt;/em&gt; &lt;strong&gt;70&lt;/strong&gt; (2015), 79–81.&lt;/p&gt;
&lt;hr&gt;
&lt;h2 class="heading" id="the-dyadic-decomposition"&gt;
 The Dyadic Decomposition&lt;span class="heading__anchor"&gt; &lt;a href="#the-dyadic-decomposition"&gt;#&lt;/a&gt;&lt;/span&gt;
&lt;/h2&gt;&lt;p&gt;The index $2^k(2l+1)$ running over $k \geq 0$ and $l \geq 0$ is not arbitrary:
it encodes a canonical partition of the positive integers. Every $n \in \mathbb{N}^+$
factors uniquely as
$$n = 2^k \cdot r, \qquad k \geq 0,\quad r \text{ odd positive},$$
where $k = v_2(n)$ is the 2-adic valuation of $n$ and $r = n/2^k$ is its odd part.
Writing $r = 2l+1$ gives the bijection $\mathbb{N}_0 \times \mathbb{N}_0 \to \mathbb{N}^+$,
$(k, l) \mapsto 2^k(2l+1)$. In particular the sets
$$A_k = {2^k(2l+1) : l \geq 0} = {2^k, 3 \cdot 2^k, 5 \cdot 2^k, \ldots}$$
form a &lt;strong&gt;partition&lt;/strong&gt; of $\mathbb{N}^+$. Explicitly: $A_0 = {1, 3, 5, 7, \ldots}$
(odd numbers), $A_1 = {2, 6, 10, 14, \ldots}$ (twice an odd number), and so on.
This partition is the key structural fact behind the proof.&lt;/p&gt;
&lt;hr&gt;
&lt;h2 class="heading" id="proof"&gt;
 Proof&lt;span class="heading__anchor"&gt; &lt;a href="#proof"&gt;#&lt;/a&gt;&lt;/span&gt;
&lt;/h2&gt;&lt;p&gt;The argument has two ingredients: the &lt;strong&gt;Basel sum&lt;/strong&gt; $\sum_{l \geq 0}(l+1)^{-2} = \pi^2/6$,
and the &lt;strong&gt;Cauchy–Schwarz inequality&lt;/strong&gt; in $\ell^2(\mathbb{C})$.&lt;/p&gt;
&lt;p&gt;Define two sequences in $\ell^2(\mathbb{C})$:
$$x = \left(1,, \tfrac{1}{2},, \tfrac{1}{3},, \ldots\right), \qquad
y_k = \left(\alpha_{2^k},, \alpha_{3 \cdot 2^k},, \alpha_{5 \cdot 2^k},, \ldots\right)
\quad (k \geq 0).$$&lt;/p&gt;
&lt;p&gt;The inner sum in the conjecture is exactly the $\ell^2$ inner product $\langle x, y_k \rangle$:
$$\sum_{l \geq 0} \frac{\alpha_{2^k(2l+1)}}{l+1} = \langle x, y_k \rangle.$$&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Step 1: Apply Cauchy–Schwarz.&lt;/strong&gt; For each $k$,&lt;/p&gt;
&lt;p&gt;$$|\langle x, y_k \rangle|^2 \leq |x|_2^2 \cdot |y_k|_2^2.$$&lt;/p&gt;
&lt;p&gt;Summing over $k \geq 0$,&lt;/p&gt;
&lt;p&gt;$$\sum _{k \geq 0} |\langle x, y _k \rangle|^2 \leq |x| _2^2 \sum _{k \geq 0} |y _k| _2^2.$$&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Step 2: Evaluate using the Basel problem and the partition.&lt;/strong&gt; The Basel problem gives
$$|x| _2^2 = \sum _{l \geq 0} \frac{1}{(l+1)^2} = \frac{\pi^2}{6}.$$&lt;/p&gt;
&lt;p&gt;Since the sets $A_k$ partition $\mathbb{N}^+$,
$$\sum _{k \geq 0} |y_k|_2^2 = \sum _{k \geq 0} \sum _{l \geq 0} |\alpha _{2^k(2l+1)}|^2
= \sum _{n \geq 1} |\alpha_n|^2.$$&lt;/p&gt;
&lt;p&gt;Combining both steps,
$$\sum_{k \geq 0} \left|\sum_{l \geq 0} \frac{\alpha_{2^k(2l+1)}}{l+1}\right|^2
\leq \frac{\pi^2}{6} \sum_{n \geq 1} |\alpha_n|^2,$$
which is the inequality with the $\frac{6}{\pi^2}$ factor moved to the other side.&lt;/p&gt;
&lt;hr&gt;
&lt;h2 class="heading" id="sharpness-of-the-constant"&gt;
 Sharpness of the Constant&lt;span class="heading__anchor"&gt; &lt;a href="#sharpness-of-the-constant"&gt;#&lt;/a&gt;&lt;/span&gt;
&lt;/h2&gt;&lt;p&gt;The constant $6/\pi^2$ is the best possible. To see this, consider the truncated
sequence $\alpha^{(N)}$ defined by $\alpha^{(N)}_{2l+1} = 1/(l+1)$ for
$l = 0, 1, \ldots, N-1$ and $\alpha^{(N)}_n = 0$ otherwise. Then:&lt;/p&gt;
&lt;ul&gt;
&lt;li&gt;The left-hand side equals $\displaystyle\sum_{l=0}^{N-1} \frac{1}{(l+1)^2} \to \frac{\pi^2}{6}$.&lt;/li&gt;
&lt;li&gt;The only non-zero contribution to the right-hand side comes from $k = 0$
(since all non-zero indices are odd, i.e. in $A_0$), giving
$\displaystyle\frac{6}{\pi^2}\left(\sum_{l=0}^{N-1} \frac{1}{(l+1)^2}\right)^2 \to \frac{6}{\pi^2} \cdot \frac{\pi^4}{36} = \frac{\pi^2}{6}$.&lt;/li&gt;
&lt;/ul&gt;
&lt;p&gt;The ratio of the right-hand side to the left-hand side therefore tends to $1$ as
$N \to \infty$, so no larger constant than $6/\pi^2$ can hold universally. Equality
is never achieved for $\alpha \in \ell^2(\mathbb{C})\setminus{0}$ with finite norm
since the limiting sequence does not belong to $\ell^2(\mathbb{C})$.&lt;/p&gt;
&lt;hr&gt;
&lt;h2 class="heading" id="extension-to-ellp"&gt;
 Extension to $\ell^p$&lt;span class="heading__anchor"&gt; &lt;a href="#extension-to-ellp"&gt;#&lt;/a&gt;&lt;/span&gt;
&lt;/h2&gt;&lt;p&gt;The Cauchy–Schwarz inequality used above is a special case of Hölder&amp;rsquo;s inequality,
and the proof generalises immediately.&lt;/p&gt;
&lt;div style="padding:10px 14px; border:2px solid #27ae60; border-radius:6px; margin:16px 0;"&gt;
&lt;span style="color:#27ae60; font-weight:bold;"&gt;Theorem (Ibragimov–Salimova, 2015)&lt;/span&gt;
&lt;p&gt;Let $p, q \in (1,\infty)$ with $\tfrac{1}{p} + \tfrac{1}{q} = 1$. For all
$\alpha = (\alpha_1, \alpha_2, \ldots) \in \ell^p(\mathbb{C})$ and
$x = (x_0, x_1, \ldots) \in \ell^q(\mathbb{C})$,
$$\sum_{n \geq 1} |\alpha_n|^p \geq \left(\sum_{l \geq 0} |x_l|^q\right)^{-p/q}
\sum_{k \geq 0} \left|\sum_{l \geq 0} x_l, \alpha_{2^k(2l+1)}\right|^p.$$&lt;/p&gt;
&lt;/div&gt;
&lt;p&gt;Retkes&amp;rsquo;s original inequality is the case $p = q = 2$ and $x_l = 1/(l+1)$, where
$(\sum_{l\geq 0}|x_l|^2)^{-1} = 6/\pi^2$ by the Basel problem.&lt;/p&gt;
&lt;hr&gt;
&lt;h2 class="heading" id="remarks-on-structure"&gt;
 Remarks on Structure&lt;span class="heading__anchor"&gt; &lt;a href="#remarks-on-structure"&gt;#&lt;/a&gt;&lt;/span&gt;
&lt;/h2&gt;&lt;p&gt;&lt;strong&gt;The role of the dyadic partition.&lt;/strong&gt; The sets $A_k$ are the &lt;em&gt;dyadic layers&lt;/em&gt; of
$\mathbb{N}^+$: each integer sits in exactly one layer determined by its 2-adic
valuation. This structure also appears in the theory of Hardy spaces, where the
dyadic martingale decomposition underpins the $H^1$–BMO duality, and in wavelets,
where the dyadic scaling of the real line organises the multiresolution analysis.
The inequality can be read as a norm comparison between the $\ell^2$ norm and a
weighted sum over dyadic layers.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Relation to the Basel problem.&lt;/strong&gt; The constant $6/\pi^2$, the reciprocal of
$\zeta(2)$, appears here because the weight sequence $1/(l+1)$ used in the inner
sum is precisely the harmonic sequence, whose $\ell^2$ norm squared is $\zeta(2)$.
Any other weight sequence $x \in \ell^2(\mathbb{C})$ would produce the analogous
inequality with $|x|_2^{-2}$ in place of $6/\pi^2$.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;The inequality as a rearrangement estimate.&lt;/strong&gt; The right-hand side reorganises the
entries of $\alpha$ by their dyadic layer and applies a weighted average within each
layer. The inequality says the total $\ell^2$ energy cannot be less than $6/\pi^2$
times the energy of this rearranged, averaged version of the sequence, a
quantitative statement about how averaging destroys energy.&lt;/p&gt;
&lt;hr&gt;
&lt;h2 class="heading" id="further-questions"&gt;
 Further Questions&lt;span class="heading__anchor"&gt; &lt;a href="#further-questions"&gt;#&lt;/a&gt;&lt;/span&gt;
&lt;/h2&gt;&lt;p&gt;While the original conjecture is settled, several natural variants remain.&lt;/p&gt;
&lt;div style="padding:10px 14px; border:2px solid #8e44ad; border-radius:6px; margin:16px 0;"&gt;
&lt;span style="color:#8e44ad; font-weight:bold;"&gt;Question 1&lt;/span&gt;
&lt;p&gt;What is the sharp constant in the inequality if the dyadic partition is replaced by
the partition induced by a prime $p \neq 2$, i.e. by the sets
$A_k^{(p)} = {p^k m : \gcd(m, p) = 1}$? The same argument applies with
$x_l = w_l$ for any weight sequence $w \in \ell^2(\mathbb{C})$, but the resulting
constant depends on $|w|_2$ and the choice of weight, not on $\pi$.&lt;/p&gt;
&lt;/div&gt;
&lt;div style="padding:10px 14px; border:2px solid #8e44ad; border-radius:6px; margin:16px 0;"&gt;
&lt;span style="color:#8e44ad; font-weight:bold;"&gt;Question 2&lt;/span&gt;
&lt;p&gt;The inner sum $\sum_{l \geq 0} \alpha_{2^k(2l+1)}/(l+1)$ averages the entries in
layer $A_k$ with the harmonic weights. What happens if the harmonic weight $1/(l+1)$
is replaced by a weight $w(l)$ depending on the position $l$ within the layer in a
more general way, for instance $w(l) = l^{-s}$ for $s &amp;gt; 1/2$? The sharp constant
would then involve $\zeta(2s)$ instead of $\zeta(2) = \pi^2/6$.&lt;/p&gt;
&lt;/div&gt;
&lt;div style="padding:10px 14px; border:2px solid #8e44ad; border-radius:6px; margin:16px 0;"&gt;
&lt;span style="color:#8e44ad; font-weight:bold;"&gt;Question 3&lt;/span&gt;
&lt;p&gt;For $p = 1$ the Ibragimov–Salimova theorem requires $q = \infty$, and the Hölder
inequality takes a different form. Does an analogue of Retkes&amp;rsquo;s inequality hold for
$\alpha \in \ell^1(\mathbb{C})$, and if so, what is the sharp constant?&lt;/p&gt;
&lt;/div&gt;
&lt;hr&gt;
&lt;h2 class="heading" id="references"&gt;
 References&lt;span class="heading__anchor"&gt; &lt;a href="#references"&gt;#&lt;/a&gt;&lt;/span&gt;
&lt;/h2&gt;&lt;ol&gt;
&lt;li&gt;Ibragimov, Z. O. &amp;amp; Salimova, D. F. (2015). On an inequality in $\ell_p(\mathbb{C})$ involving Basel problem. &lt;em&gt;Elemente der Mathematik&lt;/em&gt;, &lt;strong&gt;70&lt;/strong&gt;(2), 79–81. &lt;a href="https://ems.press/content/serial-article-files/45532"&gt;https://ems.press/content/serial-article-files/45532&lt;/a&gt;&lt;/li&gt;
&lt;li&gt;Retkes, Z. (2012). Inequality for square summable complex series. &lt;em&gt;Open Problem Garden&lt;/em&gt;. &lt;a href="http://www.openproblemgarden.org/op/inequality_for_square_summable_complex_series"&gt;http://www.openproblemgarden.org/op/inequality_for_square_summable_complex_series&lt;/a&gt;&lt;/li&gt;
&lt;li&gt;Benko, D. &amp;amp; Molokach, J. (2013). The Basel problem as a rearrangement of series. &lt;em&gt;College Mathematics Journal&lt;/em&gt;, &lt;strong&gt;44&lt;/strong&gt;(3), 171–176.&lt;/li&gt;
&lt;li&gt;Ritelli, D. (2013). Another proof of $\zeta(2) = \pi^2/6$ using double integrals. &lt;em&gt;American Mathematical Monthly&lt;/em&gt;, &lt;strong&gt;120&lt;/strong&gt;(7), 642–645.&lt;/li&gt;
&lt;/ol&gt;</description></item></channel></rss>