Math
Maximum Norm of random vectors
Step-by-step mathematics solution: Maximum Norm of random vectors
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Problem statement (re‑phrased)
Let
[ X_{1},\dots ,X_{N}\in\mathbb R^{n} ]
be independent copies of a random vector (X=(X_{1},\dots ,X_{n})) whose coordinates
- are independent,
- have mean (0) and variance (1) (so (X) is isotropic), and
- satisfy a sub‑gaussian bound
[ |X_{ij}|{\psi{2}}\le K\qquad (1\le i\le N,\;1\le j\le n) ]
for some absolute constant (K\ge 1).
Show that the expected largest Euclidean norm among the (N) vectors is bounded by
[ \boxed{\; \mathbb E\Bigl[\max_{1\le i\le N}|X_i|_{2}\Bigr] \;\le\; C K^{2}\Bigl(\sqrt n+\sqrt{\log N}\Bigr) \;} ]
where (C>0) is an absolute constant (independent of (n,N,K)).
In particular, if the coordinates are standard sub‑gaussian ((K=1)),
[ \mathbb E\Bigl[\max_{i\le N}|X_i|_{2}\Bigr]\le C\bigl(\sqrt n+\sqrt{\log N}\bigr). ]
Full solution, step by step
We proceed in three stages:
- Concentration of the Euclidean norm of a single vector.
- Sub‑gaussian control of the deviation (|X_i|_{2}-\sqrt n).
- Bounding the maximum over (i=1,\dots ,N).
1. Concentration of (|X|_{2}) for an isotropic sub‑gaussian vector
Because the coordinates are independent, centred, unit‑variance and sub‑gaussian, the vector (X) is isotropic: [ \mathbb E X X^{\top}=I_{n}. ]
A standard result (Corollary 3.12 in Vershynin) states that for every (t\ge 0)
[ \boxed{\; \mathbb P!\Bigl(\bigl||X|_{2}-\sqrt n\bigr|\ge t\Bigr) \le 2\exp!\Bigl(-c\,\frac{t^{2}}{K^{4}}\Bigr) \;} \tag{1} ]
where (c>0) is an absolute constant.
The proof uses the Hanson–Wright inequality applied to (|X|{2}^{2}=\sum{j=1}^{n}X_{j}^{2}).
2. Sub‑gaussian norm of the deviation
Recall the definition of the sub‑gaussian (Orlicz) norm:
[ |Y|{\psi{2}}:=\inf{s>0:\;\mathbb E\exp(Y^{2}/s^{2})\le 2}. ]
A random variable (Y) satisfies a tail bound
[ \mathbb P(|Y|\ge t)\le 2\exp(-t^{2}/\sigma^{2})\quad\forall t\ge0 ]
iff (|Y|{\psi{2}}\le C\sigma) for some absolute constant (C).
Comparing (1) with this form gives
[ \boxed{\; \bigl|\; |X|{2}-\sqrt n\;\bigr|{\psi_{2}}\le C_{1}K^{2} \;} \tag{2} ]
for another absolute constant (C_{1}).
Thus each deviation (Y_{i}:=|X_{i}|{2}-\sqrt n) is a centred sub‑gaussian random variable with (|Y{i}|{\psi{2}}\le C_{1}K^{2}).
3. From a single vector to the maximum of (N) vectors
3.1 A generic maximal‑sub‑gaussian inequality
If (Y_{1},\dots ,Y_{N}) are (not necessarily independent) sub‑gaussian with the same (\psi_{2})‑norm (\sigma), then (Lemma 2.2.2 in the book)
[ \mathbb E\Bigl[\max_{1\le i\le N}|Y_{i}|\Bigr]\le C_{2}\,\sigma\sqrt{\log N}, \tag{3} ]
where (C_{2}>0) is absolute.
The proof integrates the tail bound (union bound + (1)).
3.2 Apply (3) to the deviations
Take (Y_{i}= |X_{i}|{2}-\sqrt n).
From (2) we have (\sigma = C{1}K^{2}). Plugging into (3),
[ \mathbb E\Bigl[\max_{i\le N}\bigl||X_{i}|{2}-\sqrt n\bigr|\Bigr] \le C{2}\,C_{1}K^{2}\sqrt{\log N} = C_{3}K^{2}\sqrt{\log N}. \tag{4} ]
3.3 Add back the deterministic part (\sqrt n)
For any numbers (a_{i}),
[ \max_{i}a_{i}\le \sqrt n + \max_{i}|a_{i}-\sqrt n|. ]
Apply expectation and (4):
[
\begin{aligned}
\mathbb E\Bigl[\max_{i\le N}|X_{i}|{2}\Bigr]
&\le \sqrt n +
\mathbb E\Bigl[\max{i\le N}\bigl||X_{i}|{2}-\sqrt n\bigr|\Bigr]
&\le \sqrt n + C{3}K^{2}\sqrt{\log N}.
\end{aligned}
]
Finally absorb the constant in front of (\sqrt n) (the term (\sqrt n) itself is deterministic, so we may multiply it by a harmless absolute constant) and write
[ \boxed{\; \mathbb E\Bigl[\max_{i\le N}|X_{i}|_{2}\Bigr] \;\le\; C K^{2}\bigl(\sqrt n+\sqrt{\log N}\bigr) \;} ]
with a universal constant (C>0).
When (K=1) (standard sub‑gaussian entries) the bound simplifies to
[ \mathbb E\max_{i\le N}|X_{i}|_{2}\le C\bigl(\sqrt n+\sqrt{\log N}\bigr). ]
Final answer
[ \boxed{\displaystyle \mathbb{E}\Bigl[\max_{1\le i\le N}|X_i|_{2}\Bigr] \le C K^{2}\bigl(\sqrt{n}+\sqrt{\log N}\bigr) } ]
where (K=\max_{i,j}|X_{ij}|{\psi{2}}) and (C>0) is an absolute constant.
Common mistakes to avoid
| Mistake | Why it is wrong | How to fix it | ||
|---|---|---|---|---|
| Forgetting the isotropic assumption. | Without (\mathbb E XX^{\top}=I_{n}) the mean of (|X|_{2}) is not (\sqrt n); the concentration inequality (1) no longer holds. | Verify that the coordinates have variance 1, which guarantees isotropy. | ||
| Bounding (|X_i|_{2}) directly instead of its deviation. | (|X_i|{2}) is not sub‑gaussian (its tail is only sub‑exponential). The sub‑gaussian property holds for the *centered* quantity (|X_i|{2}-\sqrt n). | First prove (1) for the deviation, then apply the maximal inequality to ( | |X_i|_{2}-\sqrt n | ). |
| Using the (\psi_{2})–norm of the coordinates instead of that of the deviation. | The bound (|X_{ij}|{\psi{2}}\le K) does not directly give (||X_i|{2}|{\psi_{2}}\le K). | Use Corollary 3.12 (or Hanson–Wright) to translate coordinate sub‑gaussianity into (2). The resulting (\psi_{2})–norm scales like (K^{2}). | ||
| Dropping the constant (K^{2}). | The concentration (1) has a denominator (K^{4}), so the (\psi_{2}) norm of the deviation is proportional to (K^{2}). Ignoring it yields a bound that is false for large (K). | Keep the factor (K^{2}) throughout; it appears in the final constant. | ||
| Applying the union bound after taking expectations. | The bound (\mathbb E\max_i Y_i\le \max_i \mathbb E Y_i) is false; expectation does not commute with max. | Use the tail‑integration method (Lemma 2.2.2) that gives (3) directly from the sub‑gaussian tail. |
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