5.2 Proofs for Section 4.4 “The Bifrequency Cross-Periodogram”

In this section, proofs of lemmas and theorems presented in Section 4.4 on bias and covariance of the bifrequency cross-periodogram are reported.

The following Lemma 5.2.1 allows, in the proofs of the subsequent lemmas and theorems, the free interchange of the order of limit and sum operations.

Lemma 5.2.1 (Napolitano 2003, Lemma A.1).

a. Under Assumption 4.4.3a (series regularity), the function series img is uniformly convergent. Moreover, for any function sequence img of uniformly bounded functions img the function series img is uniformly convergent.
b. Under Assumption 4.4.3b (series regularity), the function series

img

is uniformly convergent. Moreover, for any function sequence img of uniformly bounded functions, the function series

img

is uniformly convergent.

Proof: The uniform convergence of the function series img is an immediate consequence of (4.97) and the Weierstrass criterium (Smirnov 1964). Moreover, since the functions img are uniformly bounded, accounting for (4.97), it results in img and hence, for the Weierstrass criterium the function series img turns out to be uniformly convergent. Part b) of the Lemma can be proved analogously. equation

5.2.1 Proof of Lemma 4.4.6 Expected Value of the Bifrequency Cross-Periodogram

By substituting into (4.93) the STFTs img and img expressed according to (4.94b), and taking the expected value, one has

equation

(5.6) equation

where, in the third equality, (4.95) with z1 = y and z2 = x(*) is used.

In the derivation of (5.6), the order of integral and expectation operators can be interchanged due to the Fubini and Tonelli theorem (Champeney 1990, Chapter 3). In fact, defined

(5.7) equation

and accounting for Assumptions 4.4.3a and 4.4.5, for the integrand function in the right-hand side of (5.6) we have

(5.8) equation

The interchange of sum and integral operations to obtain (4.106) from (5.6) is justified even if the set img is not finite by using the dominated convergence theorem (Champeney 1990, Chapter 4). Specifically, by denoting with img an increasing sequence of finite subsets of img, i.e., such that img for h < k and img, we have

(5.9) equation

In fact, it results that

(5.10) equation

with the right-hand side bounded by the right-hand side of (5.8). That is, the integrand function in the second term of equality (5.9) is bounded by a summable function of ν1 not depending on k. equation

5.2.2 Proof of Lemma 4.4.7 Covariance of the Bifrequency Cross-Periodogram

For zero mean stochastic processes x(t) and y(t), also the STFTs img and img are zero mean. By specializing to N = 4 and zero-mean processes the expression of Nth-order cumulant in terms of Nth-and lower-order moments (4.39), the result is that

(5.11) equation

Thus, accounting for the STFT expression (4.94b), from (5.11) it follows that

(5.12) equation

Finally, by substituting (4.95) and (4.96) into (5.12), and using the sampling property of the Dirac delta, (4.108) follows.

The interchange of expectation, sum, and integral operations can be justified as in the proof of Lemma 4.4.6.

Lemma 5.2.2 (Napolitano 2003, Lemma A.2). Let Ψ(n)(f1) be a function satisfying Assumption 4.4.4 (support-curve regularity (I)). For any function V(ν) continuous a.e. and infinitesimal at ±∞, one has

(5.13) equation

for any λ1 such that img is a continuity point of V.

Proof. If f2 ≠ Ψ(n)(f1), then f2 ≠ Ψ(n)(f1) definitively in a neighborhood of f1 since Ψ(n) is derivable and, hence, continuous. Thus, one has

(5.14) equation

from which it follows that

(5.15) equation

since V(ν) is continuous a.e. and infinitesimal at ±∞. Furthermore, if f2 = Ψ(n)(f1) then, from the assumption of derivability of Ψ(n)(f1), one has

(5.16) equation

Thus, (5.13) follows from the a.e. continuity of V. equation

Lemma 5.2.3 (Napolitano 2003, Lemma A.3). Let img and img be second-order harmonizable jointly SC stochastic processes with bifrequency cross-spectrum (4.15), and define the function

(5.17) equation

Under Assumptions 4.4.3a (series regularity), 4.4.4 (support-curve regularity (I)), and 4.4.5 (data-tapering window regularity), one obtains

(5.18) equation

with E(n)(f1) defined in (4.113).

Proof. By making into (5.17) the variable change λ1 = (f1ν1)/Δf and accounting for (4.103) and (4.107) one has

(5.19) equation

Denoted by GΔf(λ1) the integrand function in (5.19) and accounting for (4.97) and Assumption 4.4.5, the result is that

(5.20) equation

with the right-hand side independent of Δf. Thus, the dominated convergence theorem (Champeney 1990) can be applied:

(5.21) equation

where, in obtaining (5.21), the limit (as Δf → 0) and the sum (over n) operations can be interchanged since WB is bounded (Assumption 4.4.5) and hence, by Lemma 5.2.1a, the integrand function series in (5.19) is uniformly convergent. Moreover, the sum and the integral operations can be interchanged due to the same arguments used in the proof of Lemma 4.4.6. Furthermore, since img and is regular at ±∞, then is infinitesimal at ±∞. Thus, by substituting (5.13) (Lemma 5.2.2) with V = WB into (5.21) for all img except, possibly, the λ1s belonging to a set with zero Lebesgue maesure, (5.18) immediately follows. equation

Observe that, strictly speaking, to prove Lemmas 4.4.6, 5.2.1, and 5.2.3, Assumptions 4.4.3a and 4.4.4 need to hold only for z1 = y and z2 = x(*).

5.2.3 Proof of Theorem 4.4.8 Asymptotic Expected Value of the Bifrequency Cross-Periodogram

It immediately follows from Lemma 5.2.3 for t1 = t2 = t.

5.2.4 Proof of Theorem 4.4.9 Asymptotic Covariance of the Bifrequency Cross-Periodogram

The asymptotic covariance expression (4.115) is obtained from (4.108) as Δf → 0. In fact, the convergence, as Δf → 0, of the terms img and img (see (4.109) and (4.110)) to img and img (see (4.116) and (4.117)), respectively, can be easily proved by using Lemma 5.2.3. Moreover, the term img (see (4.111)) approaches zero as Δf → 0. In fact, by making into (4.111) the variable changes λy1 = (fy1νy1)/Δf, λx1 = (fx1νx1)/Δf, λy2 = (fy2νy2)/Δf and accounting for (4.103) and (4.107), one has

(5.22) equation

where f − λΔf img [fy1λy1Δf, fx1λx1Δf, fy2λy2Δf].

Denoted by HΔf(λy1, λx1, λy2) the integrand function in (5.22) and accounting for (4.98) and Assumption 4.4.5 the result is that

(5.23) equation

with the right-hand side independent of Δf. Thus,

(5.24) equation

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