A second moment bound for critical points of planar Gaussian fields in shrinking height windows
Stephen Muirhead

TL;DR
This paper improves the second moment bounds for the number of critical points of planar Gaussian fields within shrinking height windows, extending previous results to more delicate regimes.
Contribution
It provides an enhanced second moment bound for critical points in shrinking height windows, advancing the understanding of Gaussian field critical point statistics.
Findings
Established an improved second moment bound for critical points in shrinking height windows.
Extended previous bounds to more delicate regimes where the height window shrinks with domain size.
Confirmed the optimality of bounds in non-shrinking cases.
Abstract
We consider the number of critical points of a stationary planar Gaussian field, restricted to a large domain, whose heights lie in a certain interval. Asymptotics for the mean of this quantity are simple to establish via the Kac-Rice formula, and recently Estrade and Fournier proved a second moment bound that is optimal in the case that the height interval does not depend on the size of the domain. We establish an improved bound in the more delicate case of height windows that are shrinking with the size of the domain.
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A second moment bound for
critical points of planar Gaussian fields
in shrinking height windows
Stephen Muirhead
School of Mathematical Sciences, Queen Mary University of London
Abstract.
We consider the number of critical points of a stationary planar Gaussian field, restricted to a large domain, whose heights lie in a certain interval. Asymptotics for the mean of this quantity are simple to establish via the Kac-Rice formula, and recently Estrade and Fournier proved a second moment bound that is optimal in the case that the height interval does not depend on the size of the domain. We establish an improved bound in the more delicate case of height windows that are shrinking with the size of the domain.
Key words and phrases:
Gaussian fields, critical points, second moment bound
2010 Mathematics Subject Classification:
60G60 (primary); 60F99 (secondary)
We would like to thank Dmitry Beliaev and Michael McAuley for helpful discussions, especially with respect to the application to the number of level and excursion sets [4] that motivated this work, and Igor Wigman for assisting with references. We would also like to thank an anonymous referee for helpful corrections and for pointing out reference [1].
1. Introduction
Let be a -smooth stationary planar Gaussian field, and denote by its covariance kernel. For each and , let denote the ball of radius centred at the origin, and let denote the number of critical points of inside whose heights (i.e. ‘critical values’) lie in the interval , i.e.,
[TABLE]
where denotes cardinality of a set . A simple application of the Kac-Rice formula shows that, under mild conditions on , the mean of is of order , and it is not difficult to compute asymptotics for explicitly (see, e.g., [7, 9] for special cases). On the other hand, the second moment of is a more difficult quantity to control, and indeed its finiteness was only established recently [11] (see also [1, 10, 12]), with the finiteness of higher moments remaining an important open question.
Out of the proof of [11] one can show that there exists a such that, for each and , . This bound is of the correct order when the height window is fixed (see also [8, 15], in which asymptotics for are computed for fixed) but is far from optimal if as . Our aim in this note is to derive bounds on that remain optimal in the more delicate regime in which as (‘shrinking height windows’). Such bounds have applications in analysing the variance of geometric functionals of planar Gaussian fields, such as the number of level or excursion sets contained in a large domain [4].
To state our main result we suppose that the following smoothness, non-degeneracy and decay conditions hold:
Condition 1.1**.**
- •
The covariance kernel is of class .
- •
For each , the Gaussian vector is non-degenerate.
- •
As , .
The first condition implies that is almost surely -smooth, and for all multi-indices and such that , is Gaussian with covariance .
We also need an extra condition on the support of the spectral measure , defined to satisfy .
Condition 1.2**.**
The support of is not contained in the union of two lines.
Conditions 1.1 and 1.2 are extremely mild, and will be satisfied in most applications. Notably, while these conditions imply that and are non-degenerate, we do not insist that be jointly non-degenerate, and so they hold in particular for the ‘random plane wave’ (the case , where is the zeroth Bessel function; see, e.g., [3, 6, 16]).
Our main result on the number of critical points of is the following:
Theorem 1.3**.**
Suppose satisfies Conditions 1.1 and 1.2. Then there exists a such that, for all and ,
[TABLE]
Remark 1.4*.*
The bound exhibits crossover behaviour if , which is the regime in which , and hence also .
Remark 1.5*.*
As in [1, 11], we could probably replace the condition that is with the weaker condition that is and satisfies a Geman condition [13, 14], i.e. there exists a such that
[TABLE]
Since optimum conditions for Theorem 1.3 are not our primary interest, we work with the simpler condition here.
Remark 1.6*.*
It is likely that our analysis could extend to higher dimensional fields (as in [11]), but this would increase the computational complexity of our proof (especially of Lemma 2.4). On the other hand, our analysis goes through unchanged in the (easier) one-dimensional case; we discuss this in the appendix.
Naturally, the constant in Theorem 1.3 depends on the Gaussian field . Our second result gives a bound that is uniform over a collection of Gaussian fields, which is useful in applications [4].
Theorem 1.7**.**
Let be a collection of continuous (not necessarily stationary) Gaussian fields, each defined on a compact domain , with a -smooth covariance kernel. Let be the number of critical points of in whose heights lie in . Suppose that:
- (1)
The fields are normalised so that, for each and ,
[TABLE]
and is non-degenerate for all distinct ; 2. (2)
There exists a constant such that ; 3. (3)
There exists a constant such that
[TABLE]
where denotes the derivative with respect to coordinate axes in the direction; 4. (4)
For each , there exists a constant such that
[TABLE]
where and denote respectively the covariance matrices of
[TABLE]
Then there exists a such that, for all and ,
[TABLE]
2. Proof of the second moment bound
We shall prove Theorem 1.3 as a corollary of Theorem 1.7. Let be a continuous Gaussian field on a compact domain with a -smooth covariance kernel. Suppose that is normalised so that
[TABLE]
and the vector is non-degenerate for all distinct .
We begin by introducing a parameter , and splitting
[TABLE]
into three terms
[TABLE]
so that . A simple application of the Kac-Rice formula yields the following upper bounds on the expectation of each term:
Proposition 2.1**.**
There exists an absolute constant such that, for each and ,
[TABLE]
and
[TABLE]
where , and denote the intensity functions
[TABLE]
and where , and denote, respectively, the densities of the (non-degenerate) Gaussian vectors
[TABLE]
Moreover, , and are continuous on , and respectively.
Proof.
This is a direct application of the Kac-Rice formula [2, Theorem 6.3] after bounding the relevant integrands by their suprema; the Kac-Rice formula is valid in our setting since is almost surely and the vector is non-degenerate for . ∎
In the case of large height window (), we bound more simply as follows:
Proposition 2.2**.**
There exists an absolute constant such that, for each ,
[TABLE]
where and denote the intensity functions
[TABLE]
and where and denote, respectively, the densities of the (non-degenerate) Gaussian vectors
[TABLE]
Moreover, and are continuous on and respectively.
Proof.
This is again an application of the Kac-Rice formula [2, Theorem 6.3]. ∎
The technical heart of the proof is to establish the following bounds on the intensity functions:
Lemma 2.3** (Off-diagonal part).**
Let be given. Suppose that there exist such that
[TABLE]
where and denote respectively the covariance matrices of the vectors
[TABLE]
Then there exists a , depending only on and , such that .
Lemma 2.4** (Near-diagonal part).**
Suppose that there exist such that
[TABLE]
and
[TABLE]
Then there exist , depending only on and , such that .
Lemma 2.5** (On-diagonal part).**
Suppose that there exist such that
[TABLE]
Then there exists a , depending only on , such that .
Lemma 2.6** (No height window).**
Suppose that there exist such that
[TABLE]
[TABLE]
Then there exist , depending only on and , such that and . Moreover, let be given and suppose there exists such that
[TABLE]
where is as in (2.3). Then there exists , depending only on and , such that .
The proofs of Lemmas 2.3–2.6 reduce to some Gaussian computations which we carry out in the next section. Let us conclude this section by showing how they imply Theorems 1.3 and 1.7.
Proof of Theorem 1.7.
Under the assumptions of Theorem 1.7, the constant appearing in Lemmas 2.4 and 2.6 can be chosen uniformly for all . Fix such a . Then, again under the assumptions of Theorem 1.7, the conditions in Lemmas 2.3–2.6 hold uniformly for all . The proof then follows by combining Propositions 2.1 and 2.2, and Lemmas 2.3–2.6. ∎
Proof of Theorem 1.3.
By stationarity and since is non-degenerate, via a linear rescaling of and the domain we may assume the normalisation
[TABLE]
This normalisation changes by a multiplicative constant that does not depend on and , and so does not affect the conclusion of Theorem 1.3.
It suffices to show that, under Conditions 1.1 and 1.2, the assumptions in Theorem 1.7 are satisfied for , , and .
(1)–(2). Immediate from (2.8) and the fact that is .
(3). Fix and align the coordinate axis with . By stationarity and the Cauchy-Schwarz inequality applied in Fourier space,
[TABLE]
with equality if and only if the spectral measure is supported on a pair of parallel lines , . Similarly,
[TABLE]
with equality if and only if the spectral measure is supported on the lines . Since Condition 1.2 rules out the cases of equality, and since is compact, we validate the assumption.
(4). Let and be the covariance matrices defined in (2.3), and observe that these are strictly positive-definite under Condition 1.1. By Gaussian regression ([2, Proposition 1.2])
[TABLE]
where
[TABLE]
are also strictly positive-definite. Since both determinants and inverses are continuous with respect to the entry-wise sup-norm on the set of strictly positive-definite matrices, this implies that and are strictly positive and continuous in . Since, under Condition 1.1, , it follows that
[TABLE]
the so the assumption is validated by the continuity of (and the stationarity of ). ∎
3. Gaussian computations
To assist in proving Lemmas 2.3–2.6, we rely on the following auxiliary lemma:
Lemma 3.1**.**
Fix and . Let be a random matrix, let and be random vectors, and suppose that is jointly Gaussian and centred, with non-degenerate. Let and denote respectively the density and covariance matrix of , and let denote the covariance matrix of (which does not depend on by Gaussian regression). Then there exists a constant , depending only on , such that
[TABLE]
is bounded above by
[TABLE]
where denotes the product of the largest two entries of a positive matrix. In turn, (3.1) is bounded above by
[TABLE]
Remark 3.2*.*
Lemma 3.1 can be compared to [5, Lemma A.4], in which a similar bound was established.
Proof.
Let denote a positive constant, depending only on , that may change from line to line. Throughout the proof we repeatedly use the fact that conditioning on part of a Gaussian vector reduces the variance of all coordinates. If is a matrix, then by expanding the determinant it is immediate that
[TABLE]
Hence, applying Hölder’s inequality,
[TABLE]
Since a normally distributed random variable satisfies , we have that is bounded above by
[TABLE]
Recalling that
[TABLE]
and since \mathbb{E}\big{[}X^{2}_{i,j}\,|\,Y=0,Z=0\big{]}\leq\mathbb{E}\big{[}X^{2}_{i,j}\,|\,Z=0\big{]}, to establish (3.1) it remains to show that
[TABLE]
For this, write , where is a orthogonal matrix and is the diagonal matrix of (strictly positive) eigenvalues of . Abbreviating and replacing by , by Gaussian regression we have that
[TABLE]
Differentiating in and computing explicitly, the maximum of the expression on the right-hand side is attained, in the case , at
[TABLE]
and, in the case , at
[TABLE]
In both cases, this yields a maximum value of
[TABLE]
Since the eigenvalues of a positive-definite real-symmetric matrix are bounded by a constant times the maximum diagonal entry,
[TABLE]
Moreover, since has entries bounded above in absolute value by (being orthogonal), and by the Cauchy-Schwarz inequality,
[TABLE]
Since \mathbb{E}\big{[}Y_{k}^{2}\,|\,Z=0\big{]}\leq\mathbb{E}\big{[}Y_{k}^{2}\big{]}, combining the above establishes (3.3) and hence (3.1). Finally, (3.2) follows from (3.1) since \mathbb{E}\big{[}X_{i,j}^{2}\,|\,Z=0\big{]}\leq\mathbb{E}\big{[}X_{i,j}^{2}\big{]}. ∎
We now proceed to the proofs of Lemmas 2.3–2.6. For this we recall that is centred, which implies that and are also centred Gaussian random vectors.
Proof of Lemma 2.3.
By the Cauchy-Schwarz inequality, is bounded above by
[TABLE]
Applying Lemma 3.1 (more precisely (3.2)) with the setting , this is bounded by
[TABLE]
where is an absolute constant, and denotes the covariance matrix of the vector
[TABLE]
Since, by Gaussian regression, , the result follows from (2.1) and (2.2). ∎
Proof of Lemma 2.4.
Arguing as in the proof of Lemma 2.3, and this time applying (3.1) of Lemma 3.1 with the setting and , there exists a such that
[TABLE]
where
[TABLE]
and and denote respectively the covariance matrix of the vectors
[TABLE]
Given (2.1), it remains to examine the asymptotics, as , of the quantities , and . In particular it is sufficient to prove that, as ,
- (1)
; 2. (2)
There exists a such that ; 3. (3)
There exists a such that ;
where and the constants implicit in depend only the constants and defined in (2.4) and (2.5).
Let us finish the proof by validating the claimed asymptotics. For this, we rely on the following matrix computation (whose proof is simple to verify):
Lemma 3.3**.**
For parameters , define the matrices
[TABLE]
and
[TABLE]
Then
[TABLE]
Moreover, assuming that , the diagonal elements of are equal to \Big{(}\frac{b_{1}^{2}}{2a_{2}-a_{2}^{2}},\frac{b_{2}^{2}}{2a_{3}-a_{3}^{2}},\frac{b_{2}^{2}}{2a_{2}-a_{2}^{2}}\Big{)}.
Fix and define . Under the normalisation (2.1), and since is , we may write (implicitly evaluating derivatives of at ),
[TABLE]
where the constant implicit in depends only on (defined in (2.4)). Let us suppose, without loss of generality, that , for . Recall defined in (2.3), and denote by the covariance matrix between
[TABLE]
and by the covariance matrix of , considered as the vector
[TABLE]
Computing the entries explicitly, observe that , and have the structure of the matrices and respectively in Lemma 3.3, with parameter settings
[TABLE]
[TABLE]
Applying Lemma 3.3,
[TABLE]
Since and , the claimed asymptotics for follow from (2.5). Again applying Lemma 3.3, the diagonal elements of are equal, respectively, to
[TABLE]
[TABLE]
and
[TABLE]
On the other hand, by explicit computation the diagonal elements of are equal to \big{(}\partial^{(4,0)}K_{x},\,\partial^{(2,2)}K_{x},\,\partial^{(0,4)}K_{x}\big{)}, and so the diagonal elements of are equal to . Since by Gaussian regression these diagonal elements are
[TABLE]
for respectively, we deduce that as claimed. Finally, by Gaussian regression,
[TABLE]
and since, by Lemma 3.3,
[TABLE]
we have that
[TABLE]
as claimed. ∎
Proof of Lemma 2.5.
Arguing as in the proof of Lemma 2.3, and this time applying Lemma 3.1 (more precisely (3.2)) with the setting and , there exists a constant such that
[TABLE]
where denotes the covariance matrix of , and denotes the variance of . Under the normalisation (2.1), , and the result follows from (2.6). ∎
Proof of Lemma 2.6.
Arguing as in the proof of Lemma 2.3, and applying Hölder’s inequality as in the proof of Lemma 3.1, there exists a such that
[TABLE]
where is defined in (3.5). Moreover, by Gaussian regression and the normalisation (2.1),
[TABLE]
and similarly
[TABLE]
where and are defined in (2.3), (3.4) and (3.6). Hence
[TABLE]
and the uniform bound on follows as in the proofs of Lemmas 2.3 and 2.4. Similarly
[TABLE]
which is uniformly bounded by (2.1) and (2.7). ∎
4. Appendix: The one-dimensional case
Analogous bounds also hold in the one-dimensional case. Let be a -smooth stationary Gaussian process, with its covariance kernel. The analogue of Condition 1.1 is the following:
Condition 4.1**.**
- •
The covariance kernel is of class .
- •
For each , the Gaussian vector is non-degenerate.
- •
As , .
For each and , let denote the number of critical points of in the interval whose heights (i.e. ‘critical values’) lie in the interval , i.e.,
[TABLE]
Then we have the following bound on the second moment of :
Theorem 4.2**.**
Suppose satisfies Condition 4.1. Then there exists a such that, for all and ,
[TABLE]
Remark 4.3*.*
In the one-dimensional case we can omit the extra condition, analogous to Condition 1.2, that the spectral measure of is not supported on two points, since this is already implied by Condition 4.1.
We can also state a uniform bound analogous to Theorem 1.7.
Theorem 4.4**.**
Let be a collection of continuous (not necessarily stationary) Gaussian processes, each defined on a compact interval , with a -smooth covariance kernel. Let be the number of critical points of on whose heights lie in . Suppose that:
- (1)
The processes are normalised so that, for each and ,
[TABLE]
and is non-degenerate for all distinct ; 2. (2)
There exists a constant such that ; 3. (3)
There exists a constant such that ; 4. (4)
For each , there exists a constant such that
[TABLE]
where and denote the covariance matrices of and .
Then there exists a such that, for all and ,
[TABLE]
The proof of Theorems 4.2 and 4.4 are identical to the proofs of Theorems 1.3 and 1.7, save for the obvious changes in notation. Indeed, in this case we only require simplified versions of the auxiliary Lemmas 3.1 and 3.3.
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