/ / Article

Research Article | Open Access

Volume 2011 |Article ID 272801 | https://doi.org/10.1155/2011/272801

Fei Li, Jianwei Yang, "Shift Unitary Transform for Constructing Two-Dimensional Wavelet Filters", Journal of Applied Mathematics, vol. 2011, Article ID 272801, 19 pages, 2011. https://doi.org/10.1155/2011/272801

# Shift Unitary Transform for Constructing Two-Dimensional Wavelet Filters

Academic Editor: F. Marcellรกn
Received13 Mar 2011
Revised27 May 2011
Accepted08 Jun 2011
Published14 Sep 2011

#### Abstract

Due to the difficulty for constructing two-dimensional wavelet filters, the commonly used wavelet filters are tensor-product of one-dimensional wavelet filters. In some applications, more perfect reconstruction filters should be provided. In this paper, we introduce a transformation which is referred to as Shift Unitary Transform (SUT) of Conjugate Quadrature Filter (CQF). In terms of this transformation, we propose a parametrization method for constructing two-dimensional orthogonal wavelet filters. It is proved that tensor-product wavelet filters are only special cases of this parametrization method. To show this, we introduce the SUT of one-dimensional CQF and present a complete parametrization of one-dimensional wavelet system. As a result, more ways are provided to randomly generate two-dimensional perfect reconstruction filters.

#### 1. Introduction

In her celebrated paper [1], Daubechies constructed a family of compactly supported orthonormal scaling functions and their corresponding orthonormal wavelets. Since then, wavelets with compact support have been found to be very useful in applications (see [2] and references therein). By now, the theory for the construction of one-dimensional wavelets is well developed [1, 3โ9]. But, there still exists many open problems for the construction of multidimensional wavelets ([10โ13], etc.).

To apply wavelet methods to digital image processing, two-dimensional wavelets have to be constructed. The most common wavelets used for image processing are tensor-product of one-dimensional wavelets (separable wavelets). Nevertheless, separable wavelets have a number of drawbacks [11]. Nonseparable wavelets offer the hope of more isotropic analysis ([14โ16], etc.). Many efforts have been made on constructing nonseparable wavelets. However, up to now, only a few constructions have been published. Cohen and Daubechies [14] used the univariate construction [1] to produce nonseparable scaling function with higher accuracy. Continuous nonseparable scaling functions were constructed by He and Lai [12] and Kovaeviฤ [15]. Arbitrarily smooth nonseparable orthogonal wavelets were constructed by Ayache [10] and Belogay and wang [11]. Recently, Lai [13] proposed a constructive method to find compactly supported orthonormal wavelets for any given compactly supported scaling function in the multivariate setting.

In some applications of wavelets, such as wavelet-based watermarking [17, 18], parametrization of two-dimensional wavelet filters is preferred. To make some wavelet-based watermarking schemes more robust, we need to create as many ways as possible to randomly generate perfect reconstruction filters [17]. The ample choices of wavelet filters will increase the difficulty for counterfeiters to gain the exact knowledge of the filters (see [17โ20]). But in methods available, to derive two-dimensional wavelet filters, one has to solve transcendental constraints for the parameters. Hence, wavelet filters used in wavelet-based watermarking schemes, such as [17โ20], are only tensor-product of one-dimensional wavelets.

In this paper, a transformation that we refer to as Shift Unitary Transform (SUT) of Conjugate Quadrature Filter (CQF) is proposed. In terms of this transformation, we present a parametrization method for constructing two-dimensional orthogonal wavelet filters. The choosing of the parameters is not restricted by any implicit condition. It is proved that tensor-product wavelet filters are only special cases of this parametrization method. Therefore, more ways are provided to randomly generate perfect reconstruction filters. The ample choices of wavelet filters will increase the difficulty for counterfeiters to gain the exact knowledge of the filters and make watermarking schemes based on wavelet filters more robust [17โ20].

First of all, it should be pointed out that all the filters along the paper are FIR (finite impulse response). For a matrix , we denote its transpose by in this paper.

To show that tensor-product wavelet filters are only special cases of our construction, we introduce the SUT of one-dimensional CQF and present a complete parametrization of one-dimensional wavelet system in Section 2. In Section 3, we show that tensor-product orthogonal wavelet filters can be constructed by SUT of CQF. Then, based on SUT of two-dimensional CQF, a parameterized method is presented for constructing real-valued two-dimensional orthogonal wavelet filters. Finally, nonseparable wavelet filters are derived. Conclusion remarks are given in Section 4.

#### 2. Parametrization of One-Dimensional Wavelet Filters

To construct one-dimensional orthogonal scaling function we need construct sequences such that (see [4, 21] and many others) where denotes the Kronecker delta The sequence which satisfies (2.4) is called a one-dimensional CQF, and the sequence , which satisfies (2.2), (2.3), (2.4) simultaneously, is called one-dimensional orthogonal low-pass wavelet filter.

Definition 2.1. Let be a one-dimensional CQF and an arbitrary orthogonal matrix. is called the shift unitary transform (SUT) of by if satisfies and is called the inverse shift unitary transform (ISUT) of by if satisfies where for any ,

The SUT and the ISUT of by are, respectively, denoted by By directly calculating, we have the following results.

Lemma 2.2. If is a one-dimensional CQF, then and are one-dimensional CQFs.

Lemma 2.3. If , then .

Therefore, for a one-dimensional CQF, different one-dimensional CQFs can be derived when we choose different orthogonal matrices . For a sequence , letting , we call the support of . If is a one-dimensional CQF and the support of it is in , we call a simple one-dimensional CQF.

Theorem 2.4. If is a one-dimensional CQF, it can be constructed from a simple one-dimensional CQF by a series of SUT.

Proof. It only needs to prove that by a series of ISUT of , we can get a simple one-dimensional CQF.
Without loss of generality, we assume that the support of is in , and . We will prove this theorem by induction.
We see that the theorem is true for . Assume it is true for the case . We now prove it is true for the case . Suppose that is a one-dimensional CQF and . We denote that where . Recall that is a one-dimensional CQF, that is, , which implies that . Therefore, It follows that the support of is in . Suppose that , then . It follows that there exists , such that . Furthermore, if , then . By the hypothesis, the theorem is proved.

Theorem 2.4 shows that any one-dimensional orthogonal low-pass wavelet filter can be constructed by a series of SUT. Suppose that an orthogonal scaling function satisfies (2.1). Then the sequence is a one-dimensional CQF. By Theorem 2.4, we know that can be constructed by a simple one-dimensional CQF and a series of orthogonal matrices. For a real number , we denote as the orthogonal matrix: Let be a simple one-dimensional CQF such that For an arbitrary positive integer , choosing , we define as follows: In general, the support of is in . In other words, is a length- filter. From the proof of Theorem 2.4, we know that the length- filter can be constructed by at most times SUT of one-dimensional CQF.

We can prove inductively the following theorems.

Theorem 2.5. Let , then

Theorem 2.6. Let then the sequence given in (2.14) is a one-dimensional low-pass wavelet filter.

Theorem 2.6 provides a condition for choosing such that the one-dimensional CQF given in (2.14) is a one-dimensional orthogonal low-pass wavelet filter.

In addition, if the low-pass wavelet filter satisfies the Cohen's condition (see [4]), then the corresponding to in (2.2) is an orthogonal scaling function.

By Theorem 2.6, we know that a length- one-dimensional low-pass wavelet filter can be constructed by choosing such that condition (2.16) is satisfied. Therefore, any length- one-dimensional low-pass wavelet filter can be parameterized into a -parameter family of wavelet system. In fact, we can give an explicit parametrization of any length- filter: where .

Applications of one-dimensional parameterized wavelets to compression are, for example, discussed in [22, 23]. Parameterizing all possible filter coefficients that correspond to compactly supported one-dimensional orthonormal wavelets has been studied by several authors [6, 9, 24โ26]. We provide explicit parametrization of any length- filters which satisfy the necessary conditions for orthogonality in terms of SUT.

#### 3. Construction of Two-Dimensional Wavelet Filters

##### 3.1. SUT of Two-Dimensional CQF

To construct two-dimensional orthogonal scaling function and its associated wavelets we need construct sequences and such that (see [10, 12, 13], etc.) where and .

The sequence , which satisfies (3.4), is called a two-dimensional CQF. If satisfies (3.3), (3.4), and (3.5) simultaneously, we call it a two-dimensional low-pass wavelet filter. The sequences , which satisfy (3.6) and (3.7), are called two-dimensional high-pass wavelet filters.

For an arbitrary real-valued sequence , we define and is called the support set of . If is finite, we call finite supported sequence. As aforementioned, the sequences we consider are real-valued and finite supported (FIR).

We note that any sequence can be split into 4 disjoint subsets

Definition 3.1. Let be an arbitrary orthogonal matrix, and let be an FIR. For and for all , we set Then , which is defined as follows: is called the two-dimensional SUT of .

Lemma 3.2. If is a two-dimensional CQF and is given by (3.11), then is also a two-dimensional CQF.

Proof. By directly calculating, we can prove that satisfies the following equation: This completes the proof.

If the new two-dimensional CQF is a low-pass wavelet filter, then it is worthwhile to construct the associated high-pass wavelet filters. Now we provide a result of it.

Lemma 3.3. Suppose that is a two-dimensional CQF, satisfy (3.6) and (3.7), is a two-dimensional CQF obtained by SUT of , then , which are derived by SUT of , satisfy (3.6) and (3.7) simultaneously.

It can be proved by direct calculation, so we omit the proof.

Definition 3.4. (i) is called the SUT0 of if one chooses in (3.11). This transform is denoted by .
(ii) is called the SUTT1 of if one chooses in (3.11). This transform is denoted by . is called the SUTT2 of if one chooses This transform is denoted by .
(iii) is called the SUT1 of if one chooses in (3.11). This transform is denoted by . is called the SUT2 of if we choose This transform is denoted by .

For a two-dimensional CQF, when we choose different orthogonal matrices, many new two-dimensional CQFs can be obtained. It is obvious that, after SUT0, the support of the new two-dimensional CQF does not change. But it is different for SUTT1, SUTT2, SUT1, and SUT2. For example, the support of the two-dimensional CQF is , and the support of the filter is , where and In general, for integers , if the support of is in , after SUT1 (or SUT2) the support of the new filter is in (or in ). If the support of is , we call a simple two-dimensional filter.

We will adopt the following notations in the rest of this paper. For arbitrary , let be the FIR defined as follows: Furthermore, let be the filters as follows and let be orthogonal matrices such that respectively. Then is a simple two-dimensional CQF, and satisfy (3.6) and (3.7).

From the special two-dimensional CQF , by SUTT1, SUTT2, SUT1, SUT2, and the matrices , we can construct some new two-dimensional CQFs.

##### 3.2. Tensor-Product Wavelet Filters

In this subsection, we will show that all tensor-product wavelet filters can be constructed by SUTT1 and SUTT2.

A two-dimensional low-pass wavelet filters is called tensor-product wavelet filter if it satisfies the following equations: where , are one-dimensional orthogonal low-pass wavelet filters.

Theorem 3.5. If is a tensor-product low-pass wavelet filter, then, it can be constructed by SUTT1 and SUTT2 from .

Proof. , it follows from (3.24) that Suppose that is a length- one-dimensional filter. Then there exist such that , and We denote Let be two-dimensional filter such that It follows that Hence, can be constructed by SUTT1 of .
It can be proved inductively that can be constructed by a series of SUTT1 from , and can be constructed by a series of SUTT2 from , where denotes the filter Therefore, any tensor-product two-dimensional low-pass wavelet filters can be constructed by SUTT1 and SUTT2 from .

##### 3.3. Two-Dimensional Wavelet Filters in Terms of SUT1 and SUT2

From now on, we give a method of construction of two-dimensional orthogonal wavelet filters from a simple two-dimensional CQF by SUT1 and SUT2.

For arbitrary positive integers and , choosing ,, is defined as where and Then is a two-dimensional CQF, and its support is in . We are now in a position to draw some conditions on choosing , such that is a two-dimensional low-pass wavelet filter.

Theorem 3.6. Let Then

Proof. It can be proved inductively. For the case , it is obviously true. Assume that it is true for the case ; now we prove that it is true for the case .
Let be the integer such that and . Suppose that It follows that and . Let it follows that Let . Since , then Therefore, For , let It follows from that Therefore, where Namely, it is true for the case .
Similarly for the case . This completes the proof.

Now we provide the condition on choosing , such that is a two-dimensional low-pass wavelet filter.

Theorem 3.7. If there exists integers and , such that then the sequence constructed in (3.31) is a two-dimensional low-pass wavelet filter.

Proof. It follows from Theorem 3.6 that Therefore, satisfies conditions (3.3) and (3.5), then it is a two-dimensional low-pass wavelet filter.

Corollary 3.8. If as given in (3.31) is a low-pass wavelet filter, then are the high-pass filters associated with , where .

Remark 3.9. We can choose other orthogonal matrices than and such as where ; but conditions in Theorem 3.7 should be changed.

Example 3.10. We choose in (3.31). For , define as follows:

By choosing such that , we can get many two-dimensional low-pass wavelet filters and their corresponding high-pass wavelet filters. For instance, set , , , . By (3.31) and (3.47), we can get a nonseparable orthogonal low-pass wavelet filter (see Table 1) and its associated high-pass wavelet filters (Tables 2, 3, and 4). Figure 1 shows that the high frequency sub-bands by the derived filter can reveal more features than that by the commonly used tensor-product wavelet filter.

 ๐ ( ๐ , ๐ ) ๐ = 0 ๐ = 1 ๐ = 2 ๐ = 3 ๐ = 0 โ0.020275 โ0.054787 0.243250 0.657306 ๐ = 1 0.024899 0.067282 0.198076 0.535237 ๐ = 2 โ0.025190 0.009322 0.302214 โ0.111841 ๐ = 3 0.030935 โ0.011448 0.246090 โ0.091071
 ๐ 1 ( ๐ , ๐ ) ๐ = 0 ๐ = 1 ๐ = 2 ๐ = 3 ๐ = 0 0.009322 0.025190 โ0.111841 โ0.302214 ๐ = 1 โ0.011448 โ0.030935 โ0.091071 โ0.246090 ๐ = 2 โ0.054787 0.020275 0.657306 โ0.243250 ๐ = 3 0.067282 โ0.024899 0.535237 โ0.198076
 ๐ 2 ( ๐ , ๐ ) ๐ = 0 ๐ = 1 ๐ = 2 ๐ = 3 ๐ = 0 0.198076 0.535237 0.024899 0.067282 ๐ = 1 โ0.243250 โ0.657306 0.020275 0.054787 ๐ = 2 0.246090 โ0.091071 0.030935 โ0.011448 ๐ = 3 โ0.302214 0.111841 0.025190 โ0.009322
 ๐ 3 ( ๐ , ๐ ) ๐ = 0 ๐ = 1 ๐ = 2 ๐ = 3 ๐ = 0 โ0.091071 โ0.246090 โ0.011448 โ0.030935 ๐ = 1 0.111841 0.302214 โ0.009322 โ0.025190 ๐ = 2 0.535237 โ0.198076 0.067282 โ0.024899 ๐ = 3 โ0.657306 0.243250 0.054787 โ0.020275

Remark 3.11. By Section 3.2, we know that any two-dimensional tensor-product orthogonal wavelet filters can be constructed by SUTT1 and SUTT2. By Example 3.10, we know that, by SUT1 and SUT2, nonseparable wavelet filters can be achieved. Therefore, the construction of two-dimensional wavelet filters in terms of SUT of two-dimensional CQF is a generalization of the construction of separable orthogonal wavelet filters. Furthermore, from (3.31) and (3.47), we can see that our construction is a parametrization method.

#### 4. Conclusion

SUT of CQF is introduced in this paper. In terms of SUT of one-dimensional CQF, any one-dimensional orthogonal wavelet filters with dilation factor 2 can be given in explicit expression. The SUT of two-dimensional CQF is applied to the construction of two-dimensional orthogonal wavelet filters, and a parametrization method is presented. The selection of the parameters is not restricted by any implicit condition. Tensor-product wavelet filters are only special case of this method. It provides more ways to randomly generate perfect reconstruction filters.

Our method provides many possible choices for the parameters. But what is a good choice of the parameters? Should any restriction on the choice of the parameters imply certain properties? Characteristics of SUT should be deeply studied.

#### Acknowledgments

The authors would like to thank the anonymous reviewers and the associate editor for their valuable comments and suggestions to improve the presentation of this paper. This work was supported in part by the National Science Foundation of China under Grant 60973157. This work was also supported in part by the National Science Foundation of Jiangsu Province Education Department under Grant no. 08KJB520004, and in part by Philosophy and Social Sciences Planning Project of Beijing Municipal Commission of Education under Grant no. SM201010011002.

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Copyright © 2011 Fei Li and Jianwei Yang. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

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