Coverings of random ellipsoids, and invertibility of matrices with i.i.d. heavy-tailed entries

Elizaveta Rebrova, Konstantin Tikhomirov

Introduction

In this paper, we consider random matrices AA satisfying

We are concerned with the following question: how many translates of a Euclidean ball nB2n\sqrt{n}B_{2}^{n} (or its constant multiple) are needed to cover the random ellipsoid A(B2n)A(B_{2}^{n})? Being geometrically natural, this problem, as we will see later, has an application to studying invertibility properties of the matrix AA.

In particular, the above theorem implies the following more elegant

For any δ∈(0,1/4]\delta\in(0,1/4] and n≥14δn\geq\frac{1}{4\delta} there exists a non-random subset N⊂B2n{\mathcal{N}}\subset B_{2}^{n} of cardinality at most exp⁡(13nδln⁡2eδ)\exp(13n\delta\ln\frac{2e}{\delta}) such that for any n×nn\times n matrix AA satisfying (* ‣ 1), we have

for some universal constant C′>0C^{\prime}>0.

Both results have geometric interpretation in terms of covering numbers. Recall that for two subsets SS and KK of a vector space the covering number N(S,K){\bf N}(S,K) is defined as the smallest number of parallel translates of KK sufficient to cover SS. By Theorem A, {\bf N}(A(B_{2}^{n}),\frac{C\sqrt{n}}{\delta}B_{2}^{n})\leq\exp\bigl{(}13\delta n\ln\frac{2e}{\delta}\bigr{)} with probability at least 1−4exp⁡(−δn/8)1-4\exp(-\delta n/8).

A crucial feature of these results is that the set C\mathcal{C} in the theorem is non-random. Moreover, C\mathcal{C} (as well as the set N{\mathcal{N}} from Corollary A) provides a “universal” covering which is independent of the distribution of the entries of AA.

Finally, compared to Corollary A, the statement of Theorem A is more flexible as it enables us to choose the “anchor” points within the parallelepipeds when constructing corresponding ε\varepsilon-net (this matter is covered in detail at the beginning of Section 5).

Let us briefly describe the main idea of the proof. The collection C\mathcal{C} of parallelepipeds is constructed using a special subset D{\mathcal{D}} of diagonal operators with diagonal elements in the interval (0,1](0,1]. Namely, we define D{\mathcal{D}} as the set of all diagonal operators with diagonal entries in {1}∪{2−2k}k=0∞\{1\}\cup\{2^{-2^{k}}\}_{k=0}^{\infty} and with determinants bounded from below by exp⁡(−δn)\exp(-\delta n). Then, for every operator DD from D{\mathcal{D}}, we take a covering of the ball B2nB_{2}^{n} by appropriate translates of parallelepiped D(L′′n−1/2B∞n)D(L^{\prime\prime}n^{-1/2}B_{\infty}^{n}) (for some L′′=L′′(δ)L^{\prime\prime}=L^{\prime\prime}(\delta)), and let C\mathcal{C} be the union of such coverings over D{\mathcal{D}}. It turns out that Theorem A follows almost immediately from the following relation:

In Section 3, we show that (1) holds true under condition (* ‣ 1); see Theorem 3.1. Geometrically, this property means that it is possible to construct a random parallelepiped P⊂nP\subset^{n} with sides parallel to the standard coordinate axes, such that Vol(P)≥exp⁡(−δn){\rm Vol}(P)\geq\exp(-\delta n) and AA maps PP inside the Euclidean ball CnδB2n\frac{Cn}{\sqrt{\delta}}B_{2}^{n} with probability at least 1−4exp⁡(−δn/8)1-4\exp(-\delta n/8). Note that parallelepiped PP will be “narrow” along directions w∈Sn−1w\in S^{n-1} for which ∥Aw∥\|Aw\| is large.

As we already mentioned above, Theorem A has a direct application to the problem of obtaining quantitative (non-asymptotic) estimates for the smallest singular value of AA. Recall that, given an m×nm\times n (m≥nm\geq n) matrix MM, its smallest singular value can be defined as sn(M)=inf⁡y∈Sn−1∥My∥s_{n}(M)=\inf\limits_{y\in S^{n-1}}\|My\|. An argument based on Theorem A and results of Rudelson and Vershynin from , yields:

Let us put Theorem B in the context of known results.

Convergence of (appropriately normalized) smallest singular values for a sequence of random rectangular matrices with i.i.d. entries and growing dimensions was established by Bai and Yin (see also , where the result is proved under optimal moment assumptions). For non-asymptotic results in this direction, we refer the reader to papers for the case of i.i.d. entries (see also where no moment conditions are assumed); for log-concave distributions of rows and for more general isotropic distributions. We refer to surveys (see also ) for more information.

where L>0L>0 and u∈(0,1)u\in(0,1) depend only on the subgaussian moment of aija_{ij}’s. Note that Theorem B gives an estimate of exactly the same form, but for the matrices with heavy-tailed entries.

The idea of the proof of Theorem B can be described as follows. Denote by A′A^{\prime} the transpose of the first n−1n-1 columns of AA. A principal component of the proof of is an analysis of the arithmetic structure of null vectors of A′A^{\prime}, which is described with the help of the notion of the least common denominator (LCD). To show that null vectors of A′A^{\prime} typically have an exponentially large LCD, the authors of consider subsets SS of the unit sphere corresponding to vectors with small LCD, and show that inf⁡x∈S∥A′x∥>0\inf\limits_{x\in S}\|A^{\prime}x\|>0 with a large probability. For this, they use the standard ε\varepsilon-net argument, when the infimum is estimated by taking a Euclidean ε\varepsilon-net N{\mathcal{N}} on SS and applying relation inf⁡x∈S∥A′x∥≥inf⁡y∈N∥A′y∥−ε∥A′∥2→2\inf\limits_{x\in S}\|A^{\prime}x\|\geq\inf\limits_{y\in{\mathcal{N}}}\|A^{\prime}y\|-\varepsilon\|A^{\prime}\|_{2\to 2} together with the estimate ∥A′∥2→2≤Cn\|A^{\prime}\|_{2\to 2}\leq C\sqrt{n} which holds with probability very close to one under the subgaussian moment assumptions on the entries. In our setting, the principal difficulty consists in the fact that the condition (* ‣ 1) does not guarantee a good upper bound for the operator norm ∥A′∥2→2\|A^{\prime}\|_{2\to 2}. To deal with this fundamental issue, we “refine” the nets constructed in by applying Theorem A. Indeed, it can be shown that Theorem A implies that, given an ε\varepsilon-net N{\mathcal{N}} on SS, it is possible to construct a subset N~⊂S\widetilde{\mathcal{N}}\subset S of cardinality at most \exp\bigl{(}13\delta n\ln\frac{2e}{\delta}\bigr{)}|{\mathcal{N}}| which is an L′εnL^{\prime}\varepsilon\sqrt{n}-net on SS (for some L′=L′(δ)L^{\prime}=L^{\prime}(\delta)) with respect to the pseudometric d(x,y)=∥A′(x−y)∥d(x,y)=\|A^{\prime}(x-y)\| with probability at least 1−4exp⁡(−δn/8)1-4\exp(-\delta n/8). Then, inf⁡x∈S∥A′x∥≥inf⁡y∈N~∥A′y∥−L′εn\inf\limits_{x\in S}\|A^{\prime}x\|\geq\inf\limits_{y\in\widetilde{\mathcal{N}}}\|A^{\prime}y\|-L^{\prime}\varepsilon\sqrt{n}, so the argument does not depend any more on the value of ∥A′∥2→2\|A^{\prime}\|_{2\to 2}.

The paper is organized as follows: Sections 2 and 3 are devoted to proving the main novel element of the paper — Theorem A. Then, in Section 4, we collect some results from , and, in Section 5, prove Theorem B.

Throughout the paper, by Dn\mathcal{D}_{n} we denote the set of all n×nn\times n diagonal matrices with diagonal elements belonging to the interval (0,1](0,1] (we will sometimes refer to such matrices as positive diagonal contractions). Further, denote by Dn2{\mathcal{D}}^{2}_{n} the set of all n×nn\times n positive diagonal contractions whose diagonal entries belong to the set {1}∪{2−2k}k=0∞\{1\}\cup\{2^{-2^{k}}\}_{k=0}^{\infty}. The set Dn2{\mathcal{D}}^{2}_{n} can be regarded as a discretization of Dn\mathcal{D}_{n}.

Proposition 2.1 is a foundation block of our paper. In Section 3, we will amplify this result (the case p=2p=2) by proving its “matrix version” (Theorem 3.1). The case p≠2p\neq 2 in this section is considered just for completeness.

Note that a trivial definition of the diagonal operator D=(dij)D=(d_{ij}) by setting

We will need the following standard fact:

Y~\widetilde{Y} and Z~\widetilde{Z} are equidistributed with YY and ZZ, respectively;

Fix for a moment i≤ni\leq n and consider the distributions of yiy_{i} and ziz_{i}. Take any t>0t>0. If τk(yi)≤t\tau_{k}(y_{i})\leq t for all k≥0k\geq 0 then, obviously,

Otherwise, let k(t):=max⁡{k≥0: τk(yi)≤t}k(t):=\max\{k\geq 0:\,\tau_{k}(y_{i})\leq t\}. Then

The next lemma provides an actual construction of the required diagonal operator.

For any α∈(0,1)\alpha\in(0,1) there is L=L(α)>0L=L(\alpha)>0 with the following property. Let (τk)k=1∞(\tau_{k})_{k=1}^{\infty} be an increasing non-negative sequence satisfying ∑k=1∞τk2−k<∞\sum_{k=1}^{\infty}\tau_{k}2^{-k}<\infty, and let

Let L≥2eL\geq 2e be a number which we will determine later. Now, for each k≥0k\geq 0, define random variables

As building blocks of the contraction D~\widetilde{D}, let us consider random diagonal matrices D(k)D^{(k)} with

In particular, for all kk such that L2−kn/δ≥1L2^{-k}n/\delta\geq 1, using the relation L≥2eL\geq 2e, we obtain

and for all kk satisfying L2−kn/δ<1L2^{-k}n/\delta<1, we get

Now, let us choose L=L(α)L=L(\alpha) sufficiently large so that both

(we set Wi=0W_{i}=0 for zi=−∞z_{i}=-\infty). Further, for every zz we let

The above statement can be “tensorized”. In what follows, we are interested only in the case p=2p=2 and α=1/2\alpha=1/2.

There is a universal constant C>0C>0 with the following property. Let A=(aij)A=(a_{ij}) be an n×nn\times n random matrix satisfying (* ‣ 1), and let δ∈(0,1]\delta\in(0,1]. Then there is a random positive contraction DD taking values in Dn\mathcal{D}_{n} such that the Euclidean norms of the rows of ADAD are uniformly bounded by Cδn\frac{C}{\sqrt{\delta}}\sqrt{n} everywhere on the probability space, and

Indeed, for any i=1,2,…,ni=1,2,\dots,n, let DiD_{i} be the positive contraction defined with respect to the ii-th row of AA using Proposition 2.1 (with parameters α=1/2\alpha=1/2, p=2p=2), so that D1,D2,…,DnD_{1},D_{2},\dots,D_{n} are jointly independent. Then the product of these contractions D:=∏i=1nDiD:=\prod_{i=1}^{n}D_{i} satisfies the required conditions. ∎

Coverings of random ellipsoids

Let δ∈(0,1]\delta\in(0,1] and let A=(aij)A=(a_{ij}) be an n×nn\times n random matrix satisfying (* ‣ 1). Then

where C\refparallelepiped norm estimate>0C_{\text{\tiny\ref{parallelepiped norm estimate}}}>0 is a universal constant.

The above theorem can be seen as a way to “regularize” the random matrix AA by reducing its norm while preserving its “structure”. In this connection, let us mention work where a very general problem of regularizing random matrices was discussed (see [10, Section 5.4]).

As we have mentioned in the introduction, Theorem A follows almost immediately from the above statement; we give the proof of Theorem A at the very end of the section. The section is organized as follows. First, we use D~\widetilde{D} constructed in Remark 2.8 to verify Theorem 3.1 under an additional assumption that the entries of AA are symmetrically distributed (see Proposition 3.6). Then, we will apply a symmetrization procedure to prove Theorem 3.1 in full generality.

A random variable ξ\xi is subgaussian if there exists a number K>0K>0 such that

To put an emphasis on the value of KK, we will sometimes call ξ\xi KK-subgaussian. We note that the smallest value of KK satisfying (3) is equivalent to the subgaussian norm of ξ\xi (see, for example, [29, Lemma 5.5]); however, the latter notion is less convenient for us and will not be used in this paper.

The next lemma is equivalent to a standard Khintchine–type inequality (see, for example, ).

Let r1,r2,…,rnr_{1},r_{2},\dots,r_{n} be independent Rademacher random variables. Then for any vector y∈Sn−1y\in S^{n-1} the random variable ∑i=1nyiri\sum_{i=1}^{n}y_{i}r_{i} is C\refKhintchineC_{\text{\tiny\ref{Khintchine}}}-subgaussian, where C\refKhintchine>0C_{\text{\tiny\ref{Khintchine}}}>0 is a universal constant.

The sum of squares of subgaussian variables has good concentration properties; the bound below follows from a standard “Laplace transform” argument (see, for example, [29, Corollary 5.17]):

For any T>0T>0 there is L\refsum of subgaussians>0L_{\text{\tiny\ref{sum of subgaussians}}}>0 depending on TT with the following property: Let ξ1,ξ2,…,ξn\xi_{1},\xi_{2},\dots,\xi_{n} be independent centered 11-subgaussian random variables. Then

The next proposition implies that for a random matrix AA satisfying (* ‣ 1) with symmetrically distributed entries and the operator D~\widetilde{D} from Remark 2.8, the norm ∥AD~∥∞→2\|A\widetilde{D}\|_{\infty\to 2} can be efficiently bounded from above as long as D~\widetilde{D} is a Borel function of ∣A∣|A| (here and further in the text, given a matrix B=(bij)B=(b_{ij}), by ∣B∣|B| we shall denote the matrix (∣bij∣)(|b_{ij}|)).

Let K>0K>0 and let AA be an n×nn\times n random matrix satisfying (* ‣ 1), with symmetrically distributed entries. Further, let F⊂Dn{\mathcal{F}}\subset\mathcal{D}_{n} be any countable subset. Denote by E{\mathcal{E}} the event

Next, as the unit cube n^{n} is the convex hull of its vertices V={−1,1}nV=\{-1,1\}^{n}, we have

Note that, given event ED{\mathcal{E}}_{D}, the entries of Af(∣A∣)=ADAf(|A|)=AD are symmetrically distributed, so the distribution of ADvADv given ED{\mathcal{E}}_{D} is the same for any vertex v∈Vv\in V. Fix a vertex vv.

Then the variables ⟨B~Dv,ei⟩\langle\widetilde{B}Dv,e_{i}\rangle, i=1,2,…,ni=1,2,\dots,n, are jointly independent and, in view of Lemma 3.3 and the choice of BB, each variable K−1n−1/2⟨B~Dv,ei⟩K^{-1}n^{-1/2}\langle\widetilde{B}Dv,e_{i}\rangle is C\refKhintchineC_{\text{\tiny\ref{Khintchine}}}-subgaussian. By Lemma 3.4, there is a universal constant C>0C>0 such that

Then, taking a union bound over 2n2^{n} vertices of the unit cube and using (5) and (4), we get an estimate

Let δ∈(0,1]\delta\in(0,1] and let A=(aij)A=(a_{ij}) be an n×nn\times n random matrix satisfying (* ‣ 1), with symmetrically distributed entries. Then

In view of the conditions on DD and Markov’s inequality, we have

Hence, by Proposition 3.5, taking F{\mathcal{F}} to be the set of all contractions from Dn2{\mathcal{D}}^{2}_{n} having determinant at least exp⁡(−δn)\exp(-\delta n), we obtain

for a universal constant C\refparallelepiped norm estimate sym>0C_{\text{\tiny\ref{parallelepiped norm estimate sym}}}>0. ∎

SkS_{k} is a refinement of Sk−1S_{k-1} for all k=1,2,…,nk=1,2,\dots,n;

For each k∈{1,2,…,n}k\in\{1,2,\dots,n\} and any Q,Q′∈SkQ,Q^{\prime}\in S_{k} such that Q∪Q′Q\cup Q^{\prime} is a subset of an element of Sk−1S_{k-1}, there is a one-to-one mapping ϕ:Q→Q′\phi:Q\to Q^{\prime} such that d(s,ϕ(s))≤bkd(s,\phi(s))\leq b_{k} for all s∈Qs\in Q.

In particular, the above conditions on SkS_{k} imply that all elements of SkS_{k} have the same cardinality.

In , the above theorem is formulated for metric spaces. It is easy to see that passing to pseudometrics does not change the picture.

Denote by Πn\Pi_{n} the set of permutations of [n]:={1,2,…,n}[n]:=\{1,2,\dots,n\}.

Without loss of generality, we can assume that ∣yj∣≥∣yj+1∣|y_{j}|\geq|y_{j+1}| (j=1,2,…,n−1j=1,2,\dots,n-1). Define a pseudometric dd on Πn\Pi_{n}: for any p,q∈Πnp,q\in\Pi_{n} let

Further, we define a sequence of partitions (Πn,k)k=0n(\Pi_{n,k})_{k=0}^{n} of Πn\Pi_{n}: let Πn,0:={Πn}\Pi_{n,0}:=\{\Pi_{n}\} and for each k=1,2,…,nk=1,2,\dots,n, let Πn,k\Pi_{n,k} consist of all subsets of Πn\Pi_{n} of the form

for all {i1,i2,…,ik}⊂[n]\{i_{1},i_{2},\dots,i_{k}\}\subset[n].

Now, let k∈{1,2,…,n}k\in\{1,2,\dots,n\} and let Q,Q′∈Πn,kQ,Q^{\prime}\in\Pi_{n,k} be such that Q∪Q′Q\cup Q^{\prime} is a subset of an element of Πn,k−1\Pi_{n,k-1}. Note that there are numbers i1,i2,…,iki_{1},i_{2},\dots,i_{k}, ik′i_{k}^{\prime} such that p(j)=ijp(j)=i_{j} for all j<kj<k and p∈Q∪Q′p\in Q\cup Q^{\prime}; p(k)=ikp(k)=i_{k} for all p∈Qp\in Q and p(k)=ik′p(k)=i_{k}^{\prime} for all p∈Q′p\in Q^{\prime}. Define a one-to-one mapping ϕ:Q→Q′\phi:Q\to Q^{\prime} by

with the last inequality due to the fact that p−1(ik′)≥kp^{-1}(i_{k}^{\prime})\geq k. Thus, the space (Πn,d)(\Pi_{n},d) is of length at most 4∥y∥4\|y\|. Applying Theorem 3.7, we get the result. ∎

The next statement shall be used in a symmetrization argument within the proof of Theorem 3.1; we think it may be of interest in itself.

Let B=(bij)B=(b_{ij}) be a non-random n×nn\times n matrix such that the Euclidean norm of every row is at most n\sqrt{n} and such that

Further, let πi\pi_{i} (i=1,2,…,ni=1,2,\dots,n) be independent random permutations uniformly distributed on Πn\Pi_{n}, and denote by B~=(b~ij)\widetilde{B}=(\widetilde{b}_{ij}) the random n×nn\times n matrix with entries defined by

for a universal constant C\refpermutation model>0C_{\text{\tiny\ref{permutation model}}}>0.

We will show that for any v∈{−1,1}nv\in\{-1,1\}^{n} we have

for a sufficiently large universal constant C\refpermutation modelC_{\text{\tiny\ref{permutation model}}} and then take the union bound over the vertices of the cube.

Fix any v=(v1,v2,…,vn)∈{−1,1}nv=(v_{1},v_{2},\dots,v_{n})\in\{-1,1\}^{n} and let mm be the number of ones in (v1,…,vn)(v_{1},\dots,v_{n}). Clearly, the random variables ⟨B~v,ei⟩\langle\widetilde{B}v,e_{i}\rangle (i=1,2,…,ni=1,2,\dots,n) are independent. Next, for a fixed ii, the distribution of ⟨B~v,ei⟩\langle\widetilde{B}v,e_{i}\rangle coincides with that of the variable ξi:=∑j=1nvπi(j)bij\xi_{i}:=\sum_{j=1}^{n}v_{\pi_{i}(j)}b_{ij}. By Lemma 3.9 and in view of the condition on the rows of BB, we have

for some constant C~>0\widetilde{C}>0. Finally, observe that

Let A~\widetilde{A} be an independent copy of AA. Obviously

for every i=1,2,…,ni=1,2,\dots,n. Then, in view of Markov’s inequality, each row of A~\widetilde{A} satisfies

with probability at least 1−δ/16>exp⁡(−δ/8)1-\delta/16>\exp(-\delta/8). Denote by E~\widetilde{\mathcal{E}} the event

But B~\widetilde{B} is equidistributed with A~\widetilde{A} given E~\widetilde{\mathcal{E}}, so that

Clearly, ∥A~D∥∞→2≤∥A~∥∞→2\|\widetilde{A}D\|_{\infty\to 2}\leq\|\widetilde{A}\|_{\infty\to 2} for any contraction D∈DnD\in\mathcal{D}_{n} (deterministically), so we obtain for the event {\mathcal{E}}_{1}:=\big{\{}\|\widetilde{A}D\|_{\infty\to 2}\leq C_{\text{\tiny\ref{permutation model}}}\sqrt{32/\delta}\,n\;\;\mbox{for all }D\in\mathcal{D}_{n}\big{\}}:

Next, the matrix 2−1/2(A−A~)2^{-1/2}(A-\widetilde{A}) has symmetrically distributed entries, and satisfies conditions of Proposition 3.6. Hence,

Conditioning on E1{\mathcal{E}}_{1}, we get

Note that, given E1{\mathcal{E}}_{1}, we have ∥AD∥∞→2≤∥(A−A~)D∥∞→2+C\refpermutation model32/δ n\|AD\|_{\infty\to 2}\leq\|(A-\widetilde{A})D\|_{\infty\to 2}+C_{\text{\tiny\ref{permutation model}}}\sqrt{32/\delta}\,n for all contractions D∈DnD\in\mathcal{D}_{n}. Combining this with the last formula, we obtain

Finally, since AA is independent from E1{\mathcal{E}}_{1}, the conditioning in the last estimate can be dropped, and we obtain the statement. ∎

To complete the proof of Theorem A, we will need two more technical lemmas:

Denote {\mathcal{S}}:=\{D\in{\mathcal{D}}^{2}_{n}:\,\det D\geq\exp(-\delta n)\bigr{\}}. Note that for any matrix D∈SD\in{\mathcal{S}} and for any k≥0k\geq 0, the number of diagonal elements of DD equal to 2−2k2^{-2^{k}} is less than 2−k+1δn2^{-k+1}\delta n. Hence, the cardinality of S{\mathcal{S}} can be estimated as

First, note that for any y∈B2ny\in B_{2}^{n} we have

Let δ∈(0,1/4]\delta\in(0,1/4] and n≥14δn\geq\frac{1}{4\delta}. First, applying Lemma 3.12 with K=1/δK=1/\sqrt{\delta}, we see that B2nB^{n}_{2} can be covered by (2e/δ)8nδ(2e/\delta)^{8n\delta} translates of the dilated cube 1nδB∞n\frac{1}{\sqrt{n\delta}}B^{n}_{\infty}. Let

Then, in view of Lemma 3.11, we get that B∞nB_{\infty}^{n} can be covered by at most (2e/δ)4δnexp⁡(δn)(2e/\delta)^{4\delta n}\exp(\delta n) parallelepipeds in such a way that for any y∈B∞ny\in B_{\infty}^{n} and D∈QD\in{\mathcal{Q}}, yy is covered by a translate of D(B∞n)D(B_{\infty}^{n}). Combining the two coverings, we get a collection C\mathcal{C} of parallelepipeds covering B2nB_{2}^{n} such that

and for any y∈B2ny\in B_{2}^{n} and D∈QD\in{\mathcal{Q}}, the set C\mathcal{C} contains a translate of D(1nδB∞n)D(\frac{1}{\sqrt{n\delta}}B_{\infty}^{n}) covering yy. Finally, applying Theorem 3.1, we get that with probability at least 1−4exp⁡(−δn/8)1-4\exp(-\delta n/8) for some D∈QD\in{\mathcal{Q}} we have AD(B∞n)⊂C\refparallelepiped norm estimatenδB2nAD(B^{n}_{\infty})\subset\frac{C_{\text{\tiny\ref{parallelepiped norm estimate}}}n}{\sqrt{\delta}}B^{n}_{2}, implying

(the multiple “22” in the last formula appears because the translation −Ax+A(P)-Ax+A(P) is not origin-symmetric in general). ∎

Fix nn and δ\delta, and let C\mathcal{C} be the collection of parallelepipeds defined in Theorem A. For each P∈CP\in\mathcal{C}, choose a point yp∈P∩B2ny_{p}\in P\cap B_{2}^{n}, and let N:={yP: P∈C}{\mathcal{N}}:=\{y_{P}:\,P\in\mathcal{C}\}. Then, clearly,

and with probability at least 1−4exp⁡(−δn/8)1-4\exp(-\delta n/8) for every x∈B2nx\in B_{2}^{n} there is y=y(x)∈Ny=y(x)\in{\mathcal{N}} with −Ax+Ay∈CnδB2n-Ax+Ay\in\frac{C\sqrt{n}}{\delta}B_{2}^{n}. In short,

The smallest singular value — Preliminaries

As we already mentioned in the introduction, the proof of Theorem B heavily relies on results obtained by Rudelson and Vershynin in papers and . In this section, we will state several intermediate results from those papers that we will need in Section 5 to complete our proof.

A crucial step in the proof of [20, Theorem 1.2] is a decomposition of the unit sphere into sets of “compressible” and “incompressible” vectors.

A similar decomposition of the unit sphere was already introduced in an earlier paper for the purpose of bounding the smallest singular value of rectangular matrices.

Obviously, for any ε>0\varepsilon>0 we have

Treatment of the compressible vectors is simpler due to the fact the the set Comp⁡\operatorname{Comp} is “small”; we will deal with this set in the first part of Section 5. Let us remark that, unlike in the subgaussian result of , where an estimate for compressible vectors follows almost directly from an analogue of Lemma 4.9 (see below) together with a standard covering argument, in our case we will still need to use additional results (proved in Section 3) as the norm ∥A∥2→2\|A\|_{2\to 2} may be “too large”. We will need the following simple lemma:

For any θ,ρ∈(0,1]\theta,\rho\in(0,1] the set Comp⁡=Comp⁡n(θ,ρ)\operatorname{Comp}=\operatorname{Comp}_{n}(\theta,\rho) admits a Euclidean 3ρ3\rho-net N⊂Comp⁡{\mathcal{N}}\subset\operatorname{Comp} of cardinality |{\mathcal{N}}|\leq(e/\theta)^{\theta n}\bigl{(}\frac{5}{\rho}\bigr{)}^{\theta n}.

Note that the definition of Comp⁡\operatorname{Comp} implies that for any y∈Comp⁡y\in\operatorname{Comp} there is y′∈Sn−1y^{\prime}\in S^{n-1} such that ∣supp(y′)∣≤θn|{\rm supp}(y^{\prime})|\leq\theta n and ∥y−y′∥≤2ρ\|y-y^{\prime}\|\leq 2\rho. Hence, it is enough to show that one can find a Euclidean ρ\rho-net N{\mathcal{N}} on the set of θn\theta n-sparse unit vectors, with the required estimate on ∣N∣|{\mathcal{N}}|. This follows from a standard estimate on the cardinality of an optimal ρ\rho-net on S⌊θn⌋−1S^{\lfloor\theta n\rfloor-1}, together with a bound for the binomial coefficient (n⌊θ⌋){n\choose\lfloor\theta\rfloor}. ∎

Incompressible vectors have the important property that a significant portion of their coordinates are of order n−1/2n^{-1/2}. In paper , this property was referred to as “incompressible vectors are spread”. For reader’s convenience, we provide a proof of this fact below (let us note once again that analogous concepts were already considered in ).

For any θ,ρ∈(0,1)\theta,\rho\in(0,1) and for any vector x∈Incomp⁡n(θ,ρ)x\in\operatorname{Incomp}_{n}(\theta,\rho) there is a subset of indices σ(x)⊂{1,2,…,n}\sigma(x)\subset\{1,2,\dots,n\} of cardinality at least 12ρ2θn\frac{1}{2}\rho^{2}\theta n such that for all i∈σ(x)i\in\sigma(x) we have

For every subset I⊂{1,2,…,n}I\subset\{1,2,\dots,n\}, let PIP_{I} be the coordinate projection onto the span of {ei: i∈I}\{e_{i}:\,i\in I\}. Let σ=σ(x):=σ1∩σ2\sigma=\sigma(x):=\sigma_{1}\cap\sigma_{2}, where

Since ∥x∥=1\|x\|=1, we have ∣σ1c∣≤θn|\sigma_{1}^{c}|\leq\theta n, and Pσ1c(x)P_{\sigma_{1}^{c}}(x) is a θn\theta n-sparse vector. Then the condition that xx is incompressible implies ∥Pσ1(x)∥=∥x−Pσ1c(x)∥>ρ\|P_{\sigma_{1}}(x)\|=\|x-P_{\sigma_{1}^{c}}(x)\|>\rho. Hence,

On the other hand, in view of the inclusion σ(x)⊂σ1\sigma(x)\subset\sigma_{1}, we get

Together (7) and (8) imply that ∣σ∣≥12ρ2θn|\sigma|\geq\frac{1}{2}\rho^{2}\theta n. ∎

For incompressible vectors we will need the following basic estimate from .

Let MM be a random n×nn\times n matrix with column vectors X1X^{1}, X2,…,XnX^{2},\dots,X^{n}, and let HjH_{j} (j=1,2,…,nj=1,2,\dots,n) be the span of all column vectors except the jj-th. Then for every ε>0\varepsilon>0 we have

In view of independence and equi-measurability of the columns of AA in our model, the above proposition yields for any ε>0\varepsilon>0:

where X∗=(X1∗,X2∗,…,Xn∗)X^{*}=(X_{1}^{*},X_{2}^{*},\dots,X_{n}^{*}) denotes a random normal unit vector to the span of the first n−1n-1 columns of AA. Obtaining small ball probability estimates for \Bigl{|}\sum\limits_{i=1}^{n}X_{i}^{*}a_{in}\Bigr{|} was a crucial ingredient of .

Given a real-valued random variable ξ\xi, define its Levy concentration function is

First, let us look at some well known estimates of L(ξ,v){\mathcal{L}}(\xi,v) and then state a stronger bound from .

where C\reft:Rogozin>0C_{\ref{t: Rogozin}}>0 is a universal constant.

Obviously, if ξ\xi is essentially non-constant, there are v>0v>0 and u∈(0,1)u\in(0,1) such that L(ξ,v)≤u{\mathcal{L}}(\xi,v)\leq u. The following lemma is an elementary consequence of Theorem 4.6 (see [11, Lemma 3.6] and [20, Lemma 2.6] for similar statements proved under additional moment assumptions on the variable).

Let ξ\xi be a random variable with L(ξ,v~)≤u~{\mathcal{L}}(\xi,\widetilde{v})\leq\widetilde{u} for some v~>0\widetilde{v}>0 and u~∈(0,1)\widetilde{u}\in(0,1). Then there are v′>0v^{\prime}>0 and u′∈(0,1)u^{\prime}\in(0,1) depending only on u~,v~\widetilde{u},\widetilde{v} with the following property: Let ξ1,ξ2,…,ξn\xi_{1},\xi_{2},\dots,\xi_{n} be independent copies of ξ\xi. Then for any vector y∈Sn−1y\in S^{n-1} we have

By Theorem 4.6, for any y∈Sn−1y\in S^{n-1} and any h≥max⁡j∣yj∣v~h\geq\max\limits_{j}|y_{j}|\widetilde{v}, we have

Define v′:=v~1−u~2C\reft:Rogozinv^{\prime}:=\frac{\widetilde{v}\sqrt{1-\widetilde{u}}}{2C_{\ref{t: Rogozin}}} and consider two cases.

1) For every j=1,…,nj=1,\ldots,n we have ∣yj∣≤1−u~2C\reft:Rogozin|y_{j}|\leq\frac{\sqrt{1-\widetilde{u}}}{2C_{\ref{t: Rogozin}}}. Then v′≥max⁡j∣yj∣v~v^{\prime}\geq\max\limits_{j}|y_{j}|\widetilde{v}, and we obtain from the above relation

2) There is j0j_{0} such that ∣yj0∣>1−u~2C\reft:Rogozin|y_{j_{0}}|>\frac{\sqrt{1-\widetilde{u}}}{2C_{\ref{t: Rogozin}}}. Then we get

Thus, we can take u′:=max⁡(1/2,u~)u^{\prime}:=\max(1/2,\widetilde{u}). ∎

Let α1,α2,…,αn\alpha_{1},\alpha_{2},\dots,\alpha_{n} be i.i.d. random variables, and let ε0>0\varepsilon_{0}>0.

Assume that L(α1,v′)≤u′{\mathcal{L}}(\alpha_{1},v^{\prime})\leq u^{\prime} for some v′>0v^{\prime}>0 and u′∈(0,1)u^{\prime}\in(0,1). Then there are v>0v>0 and u∈(0,1)u\in(0,1) depending only on u′,v′u^{\prime},v^{\prime} such that

As a consequence of Lemmas 4.7 and 4.8, we get

Let α\alpha be a random variable with L(α,v~)≤u~{\mathcal{L}}(\alpha,\widetilde{v})\leq\widetilde{u} for some v~>0\widetilde{v}>0 and u~∈(0,1)\widetilde{u}\in(0,1). Then there are v>0v>0 and u∈(0,1)u\in(0,1) depending only on u~,v~\widetilde{u},\widetilde{v} with the following property: Let AA be an n×nn\times n random matrix with i.i.d. entries equidistributed with α\alpha. Then for any y∈Sn−1y\in S^{n-1} we have

Lemma 4.9 can be compared with [11, Proposition 3.4] and [20, Corollary 2.7]; however, those statements were proved with additional assumptions on the entries of AA.

To get a stronger estimate than the one obtained in Lemma 4.7, the following notion was developed in and (see also preceding work by Tao and Vu).

We note that later we shall choose rr sufficiently small and hh to be a small multiple of n\sqrt{n}. Thus, most of the coordinates of LCD⁡h,r(x)⋅x\operatorname{LCD}_{h,r}(x)\cdot x are within a small distance to integers. For a detailed discussion of the above notion, we refer to .

Let ξ1,ξ2,…,ξn\xi_{1},\xi_{2},\dots,\xi_{n} be independent copies of a centered random variable such that L(ξi,v)≤u{\mathcal{L}}(\xi_{i},v)\leq u for some v>0v>0 and u∈(0,1)u\in(0,1). Further, let x=(x1,x2,…,xn)∈Sn−1x=(x_{1},x_{2},\dots,x_{n})\in S^{n-1} be a fixed vector. Then for every h>0h>0, r∈(0,1)r\in(0,1) and for every

where C\refsmall ball probabilityC_{\text{\tiny\ref{small ball probability}}} is a universal constant.

Thus, in order to get a satisfactory small ball probability estimate for the infimum over incompressible vectors, it is sufficient to show that the random normal X∗X^{*} has exponentially large LCD⁡\operatorname{LCD} with probability close to one. This will be done in the second part of Section 5. As for the set Comp⁡\operatorname{Comp}, our treatment of the random normal will be based on results of Section 3.

The smallest singular value — proof of Theorem B

In this section we give a proof of Theorem B stated in the introduction. Let us start with a version of Theorem A more convenient for us:

Let δ∈(0,1/4]\delta\in(0,1/4], n≥14δn\geq\frac{1}{4\delta}, ε∈(0,1/2]\varepsilon\in(0,1/2], S⊂Sn−1S\subset S^{n-1}, and let N⊂S{\mathcal{N}}\subset S be a Euclidean ε\varepsilon-net on SS. Then there exists a (deterministic) subset N~⊂S\widetilde{\mathcal{N}}\subset S with |\widetilde{\mathcal{N}}|~{}\leq~{}\exp\bigl{(}13\delta n\ln\frac{2e}{\delta}\bigr{)}|{\mathcal{N}}| such that for any n×nn\times n random matrix AA satisfying (* ‣ 1), with probability at least 1−4exp⁡(−δn/8)1-4\exp(-\delta n/8) the set N~\widetilde{\mathcal{N}} is a (εC⋆δn)(\frac{\varepsilon C_{\star}}{\delta}\sqrt{n})–net on SS with respect to the pseudometric d(x,y):=∥A(x−y)∥d(x,y):=\|A(x-y)\| (x,y∈Sn−1x,y\in S^{n-1}), where C⋆>0C_{\star}>0 is a universal constant.

Fix parameters nn and δ\delta, and let C\mathcal{C} be the collection of parallelepipeds from Theorem A covering B2nB_{2}^{n}. Define a set \widetilde{\mathcal{C}}:=\big{\{}\varepsilon P+y:\,P\in\mathcal{C},\;y\in{\mathcal{N}},\;S\cap(\varepsilon P+y)\neq\emptyset\big{\}} and for every P~∈C\widetilde{P}\in\mathcal{C} let yP~y_{\widetilde{P}} be a point in the intersection S∩P~S\cap\widetilde{P}. Finally, set N~:={yP~: P~∈C~}\widetilde{\mathcal{N}}:=\{y_{\widetilde{P}}:\,\widetilde{P}\in\widetilde{\mathcal{C}}\}. Informally speaking, C~\widetilde{\mathcal{C}} is a “product” of the rescaled collection ε⋅C\varepsilon\cdot\mathcal{C} and the net N{\mathcal{N}}. For each parallelepiped in C~\widetilde{\mathcal{C}} having a non-empty intersection with SS, we take one (arbitrary) point from this intersection to construct the refined net N~\widetilde{\mathcal{N}}. What remains is to check that with high probability N~\widetilde{\mathcal{N}} is indeed a (εCδn)(\frac{\varepsilon C}{\delta}\sqrt{n})–net on SS with respect to the pseudometric d(x,y):=∥A(x−y)∥d(x,y):=\|A(x-y)\|.

Next, let AA be an n×nn\times n random matrix satisfying (* ‣ 1), and define event E{\mathcal{E}} as

Fix any point x∈Sx\in S. By the definition of N{\mathcal{N}}, there is a vector y∈Ny\in{\mathcal{N}} such that ε−1(x−y)∈B2n\varepsilon^{-1}(x-y)\in B_{2}^{n}. Hence, for any point ω∈E\omega\in{\mathcal{E}} on the probability space, there is a parallelepiped P=P(ω)∈CP=P(\omega)\in\mathcal{C} such that ε−1(x−y)∈P\varepsilon^{-1}(x-y)\in P and

Note that S∩(εP+y)⊃{x}≠∅S\cap(\varepsilon P+y)\supset\{x\}\neq\emptyset, whence P~:=εP+y∈C~\widetilde{P}:=\varepsilon P+y\in\widetilde{\mathcal{C}}, and, from the above relation,

where yP~∈N~y_{\widetilde{P}}\in\widetilde{\mathcal{N}}. We have shown that

Let us note that a weaker version of Theorem A⋆A^{\star}, with condition N~⊂S\widetilde{\mathcal{N}}\subset S dropped, can be proved by applying Corollary A instead of Theorem A.

At this point, a significant part of our argument follows the same scheme as in . In the first part of this section, we are dealing with compressible vectors.

Without loss of generality, we can assume that nn is large. First, note that by Lemma 4.9 we have a strong probability estimate for any fixed unit vector: there are v>0v>0 and u∈(0,1)u\in(0,1) depending on v~,u~\widetilde{v},\widetilde{u} such that for any y∈Sn−1y\in S^{n-1} we get

In order to obtain a uniform estimate over a set S=Comp⁡n(θ,θ)S=\operatorname{Comp}_{n}(\theta,\theta) for some small parameter θ\theta, we will take a net N⊂S{\mathcal{N}}\subset S constructed in Lemma 4.3 and refine it with the help of Theorem A⋆A^{\star} to get a net N~\widetilde{\mathcal{N}} with respect to pseudometric ∥A(x−y)∥\|A(x-y)\|. We will apply Theorem A⋆A^{\star} with parameter δ\delta defined as the largest number in (0,1/4](0,1/4] so that \exp\bigl{(}13\delta n\ln\frac{2e}{\delta}\bigr{)}\leq u^{-n/3}. Let us describe the procedure in more detail.

First, define parameter θ∈(0,1/6]\theta\in(0,1/6] as the largest number satisfying the inequalities

Let SS be as above. By Lemma 4.3, there is a 3θ3\theta-net N⊂S{\mathcal{N}}\subset S on SS (with respect to the usual Euclidean metric) of cardinality ∣N∣≤(5eθ2)θn|{\mathcal{N}}|\leq(\frac{5e}{\theta^{2}})^{\theta n}. Now, by Theorem A⋆A^{\star}, there is a deterministic subset N~⊂S\widetilde{\mathcal{N}}\subset S having the following properties:

|\widetilde{\mathcal{N}}|\leq\exp\bigl{(}13\delta n\ln\frac{2e}{\delta}\bigr{)}\cdot|{\mathcal{N}}|\leq u^{-n/3}\cdot\big{(}\frac{5e}{\theta^{2}}\big{)}^{\theta n}\leq u^{-2n/3};

With probability at least 1−4exp⁡(−δn/8)1-4\exp(-\delta n/8) for every y∈Sy\in S there exists x(y)∈N~x(y)\in\widetilde{\mathcal{N}} such that

Applying the union bound over N~\widetilde{\mathcal{N}} to relation (9), we get

On the other hand, the second property of N~\widetilde{\mathcal{N}} implies that

and the result follows with u\refcompressible prop:=max⁡{u1/3,exp⁡(−δ/8)}u_{\text{\tiny\ref{compressible prop}}}:=\max\{u^{1/3},\exp(-\delta/8)\}. ∎

It is not difficult to see that Proposition 5.2 can be stated and proved in the same way for AA which is not square, but instead is an n−1×nn-1\times n matrix with i.i.d. entries equidistributed with α\alpha. Indeed, for nn large enough we can assume that γ⋅n<(n−1)<n\gamma\cdot n<(n-1)<n for γ\gamma as close to one as we want (the values of θ\refcompressible prop\theta_{\text{\tiny\ref{compressible prop}}}, u\refcompressible propu_{\text{\tiny\ref{compressible prop}}} and v\refcompressible propv_{\text{\tiny{\ref{compressible prop}}}} may differ in that case). This will be important for us later.

Proposition 5.2 could be proved by a completely different argument based on [27, Proposition 13] and not using results of Section 3 at all. However, we prefer to have a “uniform” treatment of both compressible and incompressible vectors.

Let us turn to estimating the infimum over incompressible vectors. As we already discussed in Section 4, it suffices to show that the random unit normal vector to the span of the first n−1n-1 columns of AA has exponentially large LCD⁡\operatorname{LCD} with probability very close to one. This property is verified in Theorem 5.9 below. We start with some auxiliary statements. First, note that Theorem 4.12 together with Lemma 4.8 imply that anti-concentration probability for a single vector can be estimated in terms of the LCD of the vector. Namely, the bigger LCD⁡(x)\operatorname{LCD}(x) is, the less is the probability that the image AxAx concentrates in a small ball:

Let h>0h>0, r∈(0,1)r\in(0,1) and let α\alpha be a random variable satisfying L(α,v~)≤u~{\mathcal{L}}(\alpha,\widetilde{v})\leq\widetilde{u} for some v~>0\widetilde{v}>0 and u~∈(0,1)\widetilde{u}\in(0,1). Then there is L\refsmall ball single vector≥1L_{\text{\tiny\ref{small ball single vector}}}\geq 1 depending only on v~,u~\widetilde{v},\widetilde{u} with the following property: Let A′A^{\prime} be an n−1×nn-1\times n random matrix with i.i.d. elements equidistributed with α\alpha. Then for any vector x∈Sn−1x\in S^{n-1} and any

Fix any vector x∈Sn−1x\in S^{n-1} and denote Y=(Y1,Y2,…,Yn−1):=A′xY=(Y_{1},Y_{2},\dots,Y_{n-1}):=A^{\prime}x. Note that, in view of Theorem 4.12, we have

for any ε\varepsilon satisfying conditions of the lemma. Hence, by Lemma 4.8,

The above statement is useful for incompressible vectors: the following Lemma 5.6 shows that incompressible vectors have LCD⁡\operatorname{LCD} at least of order n\sqrt{n}. The lemma is taken from papers , and its proof is included for completeness.

For every θ,ρ∈(0,1)\theta,\rho\in(0,1) there are q\refincompressible lcd=q\refincompressible lcd(θ,ρ)>0q_{\text{\tiny\ref{incompressible lcd}}}=q_{\text{\tiny\ref{incompressible lcd}}}(\theta,\rho)>0 and r\refincompressible lcd=r\refincompressible lcd(θ,ρ)>0r_{\text{\tiny\ref{incompressible lcd}}}=r_{\text{\tiny\ref{incompressible lcd}}}(\theta,\rho)>0 such that for every h>0h>0 any vector x∈Incomp⁡n(θ,ρ)x\in\operatorname{Incomp}_{n}(\theta,\rho) satisfies

Set a:=12ρ2θa:=\frac{1}{2}\rho^{2}\theta and b:=ρ/2b:=\rho/\sqrt{2}. We choose r=r\refincompressible lcd:=ba2=12ρ2θr=r_{\text{\tiny\ref{incompressible lcd}}}:=b\sqrt{\frac{a}{2}}=\frac{1}{2}\rho^{2}\sqrt{\theta} and q=q_{\text{\tiny\ref{incompressible lcd}}}:=\big{(}1/\sqrt{\theta}+\frac{2r}{a}\big{)}^{-1}=\sqrt{\theta}/3.

It is easy to check that for a vector with such norm the set

has a cardinality at least (1−a24)n(1-\frac{a^{2}}{4})n. Further, by Lemma 4.4, the set of “spread” coordinates σ(x)\sigma(x) has cardinality at least anan. Hence, the set I(x):=σ(x)∩σ~(x)I(x):=\sigma(x)\cap\widetilde{\sigma}(x) is non-empty, and ∣I(x)∣>a2n|I(x)|>\frac{a}{2}n. For any i∈I(x)i\in I(x) we have

Finally, due to the definition of I(x)I(x) and our choice of rr, denoting by PJP_{J} the coordinate projection on a span {i∈J:ei}\{i\in J:e_{i}\}, we obtain

which contradicts (10) and, hence, the assumption that LCD⁡h,r(x)<qn\operatorname{LCD}_{h,r}(x)<q\sqrt{n}. ∎

In the proof of the theorem below we will partition Incomp⁡n(θ,ρ)\operatorname{Incomp}_{n}(\theta,\rho) into subsets of vectors having LCD⁡\operatorname{LCD}’s of the same order:

where, using Lemma 5.6, we introduce the lower bound i0:=log⁡2(q\refincompressible lcdn/2)i_{0}:=\log_{2}(q_{\text{\tiny\ref{incompressible lcd}}}\sqrt{n}/2) (we have Sk=∅S_{k}=\emptyset for all k<q\refincompressible lcdn/2k<q_{\text{\tiny\ref{incompressible lcd}}}\sqrt{n}/2). Following , we are going to combine estimates for individual sets SkS_{k}.

A principal observation made in and is that the sets SkS_{k} admit Euclidean ε\varepsilon-nets of relatively small cardinality. We give both the formal statement and its proof from below for the sake of completeness:

For any θ,ρ∈(0,1)\theta,\rho\in(0,1) there is L=L(θ,ρ)>0L=L(\theta,\rho)>0 such that for every h≥1h\geq 1 and k>0k>0 the set SkS_{k} admits a Euclidean (4h/k)(4h/k)-net of cardinality at most \bigl{(}kL/\sqrt{n}\bigr{)}^{n}.

In view of Lemma 5.6, we can assume that k≥q\refincompressible lcdn/2k\geq q_{\text{\tiny\ref{incompressible lcd}}}\sqrt{n}/2. Further, without loss of generality 4hk<2\frac{4h}{k}<2; otherwise a one-point net works.

It is a simple planimetric observation that if we normalize the vector p/LCD⁡h,r\refincompressible lcd(x)p/\operatorname{LCD}_{h,r_{\text{\tiny\ref{incompressible lcd}}}}(x), the distance to the unit vector xx cannot increase more than twice:

for an appropriate number L=L(θ,ρ)>0L=L(\theta,\rho)>0. The net Nint{\mathcal{N}}_{int} does not have to be contained in SkS_{k}. But, by a standard argument, we can “replace” Nint{\mathcal{N}}_{int} with a 4h/k4h/k-net of the same cardinality, and with elements from the set SkS_{k}. ∎

Together with Theorem A⋆A^{\star}, the above lemma gives

For any θ,ρ∈(0,1)\theta,\rho\in(0,1) there is L\refnet on level sets=L\refnet on level sets(θ,ρ)≥1L_{\text{\tiny\ref{net on level sets}}}=L_{\text{\tiny\ref{net on level sets}}}(\theta,\rho)\geq 1 such that for every h≥1h\geq 1 and k>0k>0 there is a finite subset N⊂Sk{\mathcal{N}}\subset S_{k} of cardinality at most \bigl{(}kL_{\text{\tiny\ref{net on level sets}}}/\sqrt{n}\bigr{)}^{n} with the following property. The event

has probability at least 1−4exp⁡(−n/32)1-4\exp(-n/32).

Let α\alpha be a centered random variable of unit variance such that L(α,v~)≤u~{\mathcal{L}}(\alpha,\widetilde{v})\leq\widetilde{u} for some v~>0\widetilde{v}>0 and u~∈(0,1)\widetilde{u}\in(0,1). Then there exist q,s,w,r>0q,s,w,r>0 depending only on v~,u~\widetilde{v},\widetilde{u} with the following property: let X1,X2…,Xn−1X^{1},X^{2}\dots,X^{n-1} be random nn-dimensional vectors whose coordinates are jointly independent copies of α\alpha. Consider any random unit vector X∗X^{*} orthogonal to {X1,X2,…,Xn−1}\{X^{1},X^{2},\dots,X^{n-1}\}. Then

Without loss of generality, we can assume that nn is a large number and that v~≤1\widetilde{v}\leq 1. Denote by A′A^{\prime} the n−1×nn-1\times n matrix with rows X1,X2,…,Xn−1X^{1},X^{2},\dots,X^{n-1}. Then, by the definition of X∗X^{*}, we have A′X∗=0A^{\prime}X^{*}=0 almost surely. Let θ\refcompressible prop\theta_{\text{\tiny\ref{compressible prop}}} and u\refcompressible propu_{\text{\tiny\ref{compressible prop}}} be defined as in Remark 5.3 (with A′A^{\prime} replacing AA). Then, by Proposition 5.2 and Remark 5.3, we have

for w>0w>0 such that, say, exp⁡(−2w)>u\refcompressible prop\exp(-2w)>u_{\text{\tiny\ref{compressible prop}}}, and provided that nn is large. Thus, it is enough to prove that

for small enough r,w,s,qr,w,s,q depending only on v~,u~\widetilde{v},\widetilde{u}. We start by defining r:=r\refincompressible lcd(θ\refcompressible prop,θ\refcompressible prop)r:=r_{\text{\tiny\ref{incompressible lcd}}}(\theta_{\text{\tiny\ref{compressible prop}}},\theta_{\text{\tiny\ref{compressible prop}}}). Note that, by Lemma 5.6, we have

for any s>0s>0, and, in particular for ss defined by s:=v~r4L\refnet on level sets2L\refsmall ball single vectors:=\frac{\widetilde{v}r}{4L^{2}_{\text{\tiny\ref{net on level sets}}}L_{\text{\tiny\ref{small ball single vector}}}}, where L\refnet on level sets=L\refnet on level sets(θ\refcompressible prop,θ\refcompressible prop)L_{\text{\tiny\ref{net on level sets}}}=L_{\text{\tiny\ref{net on level sets}}}(\theta_{\text{\tiny\ref{compressible prop}}},\theta_{\text{\tiny\ref{compressible prop}}}) and L\refsmall ball single vectorL_{\text{\tiny\ref{small ball single vector}}} are taken from Lemmas 5.8 and 5.5, respectively, and q\refincompressible lcd=q\refincompressible lcd(θ\refcompressible prop,θ\refcompressible prop)q_{\text{\tiny\ref{incompressible lcd}}}=q_{\text{\tiny\ref{incompressible lcd}}}(\theta_{\text{\tiny\ref{compressible prop}}},\theta_{\text{\tiny\ref{compressible prop}}}). Let us emphasize that no vicious cycle is created here in regard to interdependence between ss and rr. Finally, we let q:=2s2(1−u~)q:=2s^{2}(1-\widetilde{u}) (ww will be defined at the very end of the proof).

We will make use of representation (11) of the set Incomp⁡n(θ\refcompressible prop,θ\refcompressible prop)\operatorname{Incomp}_{n}(\theta_{\text{\tiny\ref{compressible prop}}},\theta_{\text{\tiny\ref{compressible prop}}}). Denote

Indeed, since ∣K∣<qn|{\mathcal{K}}|<qn, the union bound over K{\mathcal{K}} will conclude the theorem.

In turn, (12) will follow as long as we show that

Fix for a moment any k∈Kk\in{\mathcal{K}} and let Nk{\mathcal{N}}_{k} be the subset of SkS_{k} of cardinality at most (kL\refnet on level sets/n)n(kL_{\text{\tiny\ref{net on level sets}}}/\sqrt{n})^{n}, constructed in Lemma 5.8 (with h:=snh:=s\sqrt{n}). Further, take ε:=v~rn2kL\refnet on level setsL\refsmall ball single vector\varepsilon:=\frac{\widetilde{v}r\sqrt{n}}{2kL_{\text{\tiny\ref{net on level sets}}}L_{\text{\tiny\ref{small ball single vector}}}}. Note that, in view of the definition of qq and K{\mathcal{K}}, we have k≤exp⁡(2s2(1−u~)n)k\leq\exp(2s^{2}(1-\widetilde{u})n). Hence, for nn large enough, ε\varepsilon satisfies the condition of Lemma 5.5:

where the last relation follows by the assumption v~≤1\widetilde{v}\leq 1. Finally, note that, since s≤1/4s\leq 1/4, the last quantity is bounded from below by 1−2−n/21-2^{-n/2}. Applying the definition of Nk{\mathcal{N}}_{k} in Lemma 5.8 and noticing that hL\refnet on level setsn/k≤εn/2hL_{\text{\tiny\ref{net on level sets}}}\sqrt{n}/k\leq\varepsilon\sqrt{n}/2, we get

This proves (12) and implies the result. ∎

Without loss of generality, the dimension nn is large. Let A=(aij)A=(a_{ij}) be an n×nn\times n random matrix with i.i.d. centered entries with unit variance such that for some v~>0\widetilde{v}>0 and u~∈(0,1)\widetilde{u}\in(0,1) we have L(aij,v~)≤u~{\mathcal{L}}(a_{ij},\widetilde{v})\leq\widetilde{u}. We define θ:=θ\refcompressible prop(v~,u~)\theta:=\theta_{\text{\tiny\ref{compressible prop}}}(\widetilde{v},\widetilde{u}) and v:=v\refcompressible prop(v~,u~)v:=v_{\text{\tiny\ref{compressible prop}}}(\widetilde{v},\widetilde{u}), where θ\refcompressible prop,v\refcompressible prop\theta_{\text{\tiny\ref{compressible prop}}},v_{\text{\tiny\ref{compressible prop}}} are taken from Proposition 5.2, and let q,s,w,rq,s,w,r be as in Theorem 5.9 (with respect to v~,u~\widetilde{v},\widetilde{u}). We will prove a small ball probability bound for sn(A)s_{n}(A).

It is sufficient to consider the parameter domain \varepsilon\in\big{(}\theta\widetilde{v}\exp(-qn),1\big{]}. We have

where we have applied Proposition 5.2. Further, by Proposition 4.5, we have

where X∗X^{*} denotes a random unit normal vector to the span of the first n−1n-1 columns of AA. In view of Theorem 4.12, this last relation implies

Finally, noticing that θv~ε−1≤exp⁡(qn)\theta\widetilde{v}\varepsilon^{-1}\leq\exp(qn) and applying Theorem 5.9, we get

Together with an estimate for the compressible vectors, this implies the result. ∎

Acknowledgements

We would like to thank N. Tomczak-Jaegermann and R. Vershynin for valuable suggestions that helped improve the presentation of the work. The second named author is grateful to A. Litvak for inspiring discussions. Both authors are indebted to the referee for very useful remarks and suggestions.

References