3.10 Proofs for Section 2.6.2 “Asymptotic Results as N→ ∞”

Lemma 3.10.1 Let img be given by (2.184) with a(t) as in Assumption 2.4.5. It results that

(3.155) equation

Proof: Since a(t) has finite support [− 1/2, 1/2), to prove (3.155) is equivalent to prove that

(3.156) equation

Let us consider first the case img.

Since a(t) is Riemann integrable (Assumption 2.4.5), we have

(3.157) equation

Let us consider now the case img, ν > 0.

For every img the function img is Riemann integrable and we have

(3.158) equation

that is, ∀img1 > 0 img such that for img

(3.159) equation

(not necessarily uniformly with respect to img).

Since img, the Riemann-Lebesgue theorem (Champeney 1990, Chapter 3) can be applied. Thus,

(3.160) equation

that is, ∀img2 > 0 img such that for img

(3.161) equation

Let us consider, now, the following inequality:

(3.162) equation

Since ν > 0, take img2 arbitrarily small in (3.158), and define img such that img. Fix img in (3.158) and take img1 arbitrarily small and img in (3.159). Let img and img. It results in img in (3.161) and img in (3.159). Thus, the right-hand side of (3.162) is bounded by img1 + img2 with img1 and img2 arbitrarily small, which proves (3.156) for ν > 0. Finally, note that the result holds for every non-integer ν since the function img is periodic in ν with period 1.

As a final remark, note that Lemma 3.10.1 can also be obtained as corollary of the following Lemma 3.10.2 with b(t) = rect(t), m = 0. To prove Lemma 3.10.1, however, the assumption img bounded is not used.

img

Lemma 3.10.2 Let a(t) be bounded and continuous in (− 1/2, 1/2) except, possibly, at t = ± 1/2, derivable almost-everywhere with bounded derivative, and let img. Let both a(t) and b(t) be with finite support [− 1/2, 1/2], and such that for every τ img [− 1, 1] the function a(t + τ)b*(t) is Riemann integrable in [− 1/2, 1/2]. We have

(3.163) equation

Proof: The function b(t) has finite support [− 1/2, 1/2]. Thus the sum in (3.163) can be extended from −N to N.

img. The following inequality holds

(3.164) equation

As regards the first term in the right-hand side of (3.164), observe that the first-order derivative img exists a.e. and is bounded (Assumption 2.4.5). Therefore, for almost all t1 and t2 there exists img such that img and, hence, img. Consequently,

(3.165) equation

As regards the second term in the right-hand side of (3.164), observe that the function a(t + τ)b*(t) is Riemann integrable in [− 1/2, 1/2] so that, for τ = 0,

(3.166) equation

That is, ∀img > 0 ∃ Nimg such that for N > Nimg one has

(3.167) equation

Therefore, the right-hand side of (3.164) is bounded by

equation

which can be made arbitrarily small, provided that N is sufficiently large.

This proves (3.163) for img.

img. For every img, img, the function img is Riemann integrable in [− 1/2, 1/2]. Thus

(3.168) equation

that is, ∀img1 > 0 img such that for img

(3.169) equation

not necessarily uniformly with respect to img and τ. Since img and img, it results in img. Thus, the Riemann-Lebesgue theorem (Champeney 1990, Section 3.7 can be applied:

(3.170) equation

that is, ∀img2 > 0 img such that for img

(3.171) equation

not necessarily uniformly with respect to τ.

For arbitrarily small img2, fix img so that (3.171) holds. Once img is fixed, for arbitrarily small img1 fix img such that (3.169) holds. Thus, by setting img, in (3.169) and (3.171), we have the following inequality

(3.172) equation

Let img such that img. For img, the right-hand side of (3.172) is bounded by img1 + img2 with img1 and img2 arbitrarily small. Thus, for ν ≠ 0 (and hence for ν non-integer due to the periodicity in ν) we have

(3.173) equation

Accounting for (3.165) and (3.172) (with τ = 0), we have the following inequality.

(3.174) equation

The rhs of (3.174) can be made arbitrarily small. This proves (3.163) for img.

This proof is simplified when a slightly modified version of this Lemma is used in Section 3.11 for the proof of the asymptotic covariance of the hybrid cyclic cross-correlogram. Specifically, we have the following.

(3.175) equation

img

3.10.1 Proof of Theorem 2.6.4 Asymptotic Expected Value of the Discrete-Time Cyclic Cross-Correlogram

From (2.183) it follows

(3.176) equation

where, in the third equality, Lemma 3.10.1 is used.

In the second equality, the interchange of the limit and sum operations is justified by the Weierstrass criterium (Johnsonbaugh and Pfaffenberger 2002, Theorem 62.6; Smirnov 1964) since the series of functions of N

equation

is uniformly convergent. In fact, by using (3.145) and Assumptions 2.4.3a and 2.4.5, we have

(3.177) equation

with the right-hand side bounded and independent of N.

3.10.2 Proof of Theorem 2.6.5 Asymptotic Covariance of the Discrete-Time Cyclic Cross-Correlogram

Let us consider the covariance expression (2.186). As regards the term img defined in (2.187), let

equation

It results that

(3.179) equation

where img is defined in (2.196) and Lemma 3.10.2 (with ab) has been accounted for.

The interchange of the order of limit and sum operations in (3.179) is allowed since the three-index series over (k′, k′′, img) of functions of N is uniformly convergent for the Weierstrass criterium (Johnsonbaugh and Pfaffenberger 2002, Theorem 62.6), (Smirnov 1964). In fact,

(3.180) equation

with the right-hand side independent of N, where the inequality

(3.181) equation

is used. The inequality in (3.181) follows from the fact that the sum over n is at most on 2N + 1 nonzero terms. The right-hand side of (3.180) is bounded due to Assumptions 2.4.3a and 2.4.8a. In particular, from Assumption 2.4.8a it follows that

(3.182) equation

In fact, img is the Riemann sum for the integral img, with the function img assumed to be Riemann integrable.

Analogously, it can be shown that

(3.183) equation

where img is defined in (2.197).

As regards the term img defined in (2.189), let

(3.184) equation

It results that

(3.185) equation

where img is defined in (2.198) and Lemma 3.10.2 (with ab) has been accounted for.

The interchange of the order of limit and sum operations in (3.185) is allowed since the double-index series over k and img of functions of N is uniformly convergent for the Weierstrass criterium (Johnsonbaugh and Pfaffenberger 2002, Theorem 62.6), (Smirnov 1964). In fact,

(3.186) equation

with the right-hand side independent of N, where the inequality (3.181) is used. The right-hand side of (3.186) is bounded due to Assumption 2.4.8b from which it follows that

(3.187) equation

under the assumption that the function img is Riemann integrable with respect to s.

As a final remark, observe that the sum over img in (3.180) is finite. In fact, a(t) has finite support [− 1/2, 1/2] and, hence, img only for −2Nm ≤ 2N. Consequently, in (3.180), −2Nimgn01 + n02 ≤ 2N. This fact, however, is not sufficient to make the right-hand side of (3.180) independent of N. Therefore, Assumption 2.4.8a needs to be exploited.

Lemma 3.10.3 Let img img [− 1/2, 1/2], img ≠ 0, and γ > 1. Thus

(3.188) equation

where img.

Proof: For img img [− 1/2, 1/2], img ≠ 0 one has

(3.189) equation

Thus,

(3.190) equation

img

3.10.3 Proof of Theorem 2.6.7 Rate of Convergence of the Bias of the Discrete-Time Cyclic Cross-Correlogram

From (2.179b) and (2.200) it follows

(3.191) equation

and from (2.183) we have

equation

Therefore,

(3.192) equation

Let us consider the first term in the rhs of (3.192). Accounting for (2.184) we have

(3.193) equation

where A(f) is the Fourier transform of a(t) and A(0) = 1 (see (3.64)). According to Assumption 2.4.5, we have |A(f)| ≤ K/|f|γ for |f| sufficiently large, say, |f| > f*. Thus, for N sufficiently large such that 2N + 1 > f* (and for | img|img 1), we have

(3.194) equation

where the sum in the third line is convergent when γ > 1. Note that in the special case of a rectangular data-tapering window a(t) = rect(t) ⇒ A(f) = sinc(f). Even if γ = 1, the result is that A(img (2N + 1)) = 0 for img ≠ 0, N integer. Thus, img.

Let us now consider the second term in the rhs of (3.192).

From (2.184) we have

(3.195) equation

with img never equal to zero since img integer when img. Moreover, under Assumption 2.6.6,

(3.196) equation

Let N be sufficiently large such that img. Thus, for all img and for all img it results in img and, hence,

(3.197) equation

By taking img in Lemma 3.10.3 (imgk img [− 1/2, 1/2), imgk ≠ 0 for img), for every fixed img, m, Ts, and k one obtains

(3.198) equation

Thus, by using (3.194)(3.198) into (3.192), we have

(3.199) equation

where, in the last inequality, Assumption 2.6.6 (img) is used. Thus, (2.202) immediately follows.

For a rectangular lag-product-tapering window, img, Kγ = 0 can be taken in (3.194), and (3.199) (with γ = 1) must be accordingly modified.

For a rectangular signal-tapering window, the corresponding lag-product-tapering window img has Fourier transform img such that (Fact 3.5.3)

(3.200) equation

Thus, (3.200) and (3.199) (with γ = 1) lead to

(3.201) equation

3.10.4 Proof of Lemma 2.6.9 Rate of Convergence to Zero of Cumulants of Discrete-Time Cyclic Cross-Correlograms

By using (2.181), (2.182), and the multilinearity property of cumulants we have

(3.202) equation

where, in the third equality, the variable changes nk = n and ni = n + ri, i = 1, ..., k − 1 are made, r img [r1, ..., rk−1], and all the sums are finite since the function a(·) has finite support (Assumption 2.4.5). Note that the order of finite sums can be freely interchanged. From (3.202) it follows that

(3.203) equation

where Assumption 2.6.8 is used and all the sums converge. In fact, ∑rϕ(r1Ts, ..., rk−1Ts)Ts is the Riemann sum for img and ∑n|a((nn0k)/(2N + 1))|/(2N + 1) is the Riemann sum for img. Thus, (2.206) immediately follows.

This lemma is the discrete-time counterpart of Lemma 2.4.17 on the rate of convergence to zero of the cumulant of continuous-time cyclic cross-correlograms. Note that in the discrete-time case Assumption 2.4.16 is not used. In fact, such assumption is used in the continuous-time case in Lemma 2.4.17 to interchange the order of integrals. In the discrete-time case, as a consequence of the finite support of a(·), all the sums are finite and their order can be freely interchanged.

img

3.10.5 Proof of Theorem 2.6.10 Asymptotic Joint Normality of the Discrete-Time Cyclic Cross-Correlograms

From Theorem 2.6.7 holding for γ > 1 (or γ = 1 if a(t) = rect(t)) we have

(3.204) equation

From Theorem 2.6.5 it follows that the asymptotic covariance

(3.205) equation

is finite. From Theorem 3.13.2 it follows that the asymptotic conjugate covariance is finite. Moreover, from Lemma 2.6.9 with img and k img 3 we have

(3.206) equation

where the second equality holds since the value of the cumulant does not change by adding a constant to each of the random variables (Brillinger 1981, Theorem 2.3.1).

Thus, according to the results of Section 1.4.2, for every fixed img the random variables img, i = 1, ..., k, are asymptotically (N→ ∞) zero-mean jointly complex Normal (Picinbono 1996; van den Bos 1995).

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