The signature vector-based spectral measures described in Section 16.2 calculate the spectral similarity value between a pair of two signature vectors using only the spectral information provided by L bands within these two signature vectors. So, if a material signature vector is mixed by other substances, the spectral characteristics of the signature vector to be processed do not necessarily characterize the spectral properties of the material signature vector it represents. This often occurs in real applications when a material signature vector is either mixed with other signature vectors such as background signatures or embedded in a single signature vector as a subsample target. In both cases, using a signature vector-based spectral measure to measure material similarity is generally not effective. In order to resolve this dilemma, signature vector-based hyeprspectral measures are extended to correlation-weighted hyperspectral measures that can be categorized into two classes. One comprises of hyperspectral measures that introduce a priori sample spectral correlation into signature vector-based spectral measure so as to improve discrimination performance in spectral similarity. The other is made up of hyperspectral measures weighted by a posteriori sample spectral correlation to do what a priori sample spectral correlation does.
A hyperspectral measure weighted by a priori correlation assumes that there is known correlation available prior to material discrimination and identification. A good example of best utilization of such prior correlation is the OSP approach recently developed by Harsanyi and Chang (1994) that separates desired target signature vectors from undesired target signature vectors to achieve better hyperspectral image classification. This OSP concept can be used to design new hyperspectral measures as follows.
Assume that there are p target signature vectors which are known a priori and si is a signature vector of interest. We can define a matrix, U to be a matrix formed by all a priori known target signature vectors except si. By taking advantage of the following orthogonal projector defined by Harsanyi and Chang (1994) or (2.86) in Chapter 2:
we can de-correlate the signature vector si via orthogonal projection from all other known target signatures in U by projecting si to the space orthogonal to the space linearly spanned by undesired target signature vectors in U, and derive a family of several OSP-based hyperspectral measures. Depending on how to use , these OSP-based hyperspectral measures can be either used for discrimination or identification.
Two separate problems, discrimination, and identification are considered. When discrimination is performed, it only needs to discriminate one signature vector from another. When identification is performed, we generally assume that there is a database, available for signature identification.
Two OSP-based hyperspectral measures can be designed for discrimination between two signature vectors si and sj. One includes as a weighting matrix into ED in (16.2), called EDOSP, defined by
where U is an undesired signature matrix formed by all known signatures excluding si and sj.
The other is derived from the concept of OPD in (16.3), called OSP-based divergence, DOSP, defined by
with the same U defined in (16.10).
If in (16.10) is assumed to be the identity matrix, then (16.10) is reduced to ED in (16.1). On the other hand, (16.11) is an extension of the OPD by including to eliminate the interference caused by undesired target signature vectors. However, it should be noted that unlike the EDOSP, which is a nonnegative measure, the in (16.11) can take positive or negative values depending upon whether or not si and sj point to the same direction. To avoid this problem, the absolute value is used in (16.11).
In the previous subsection, the signature vectors si and sj are assumed to be signature vectors in real data and (16.10) and (16.11) are used for signature discrimination. In this subsection, we assume that there is a database or spectral library available to be used to identify a signature vector in real data si. In this case, DOSP can be modified to perform signature identification in two different ways depending on how to use the matched signature either from the database Δ, denoted by IDOSP,Δ or itself, denoted by IDOSP as follows:
where Uk is a matrix formed by all signature vectors in Δ excluding signature vector dk.
Using (16.12) and (16.13) a signature vector si can be identified via a database Δ by the one in Δ that yields the IDOSP,Δ or IDOSP.
In many applications, obtaining a priori correlation information is very difficult, if not impossible. Therefore, it is highly desirable if we can generate necessary information directly from the image data without relying on prior knowledge. It has been demonstrated in Chapter 12 that the a priori correlation provided by can be approximated by the inverse of the sample spectral correlation matrix, R−1, which can be used to account for a posteriori correlation. In light of this interpretation, the sample spectral correlation/covariance is used to derive new a posteriori correlation-weighted hyperspectral measures.
As noted in Section 12.5, the RX detector (RXD) defined by (12.76) was developed by Reed and Yu (1990) for anomaly detection. If the r and μ in (12.76) are replaced with si and sj, respectively, then the RX anomaly detector becomes
Since (16.14) is a Mahalanobis distance (MD)-like measure, we can define a new hyperspectral MD-like measure via (16.14), called MDRX as follows:
Two comments on (16.15) are noteworthy.
As also noted in Section 12.4.1.2, replacing the used in the OSP in (12.22) with the inverse of spectral correlation matrix, R−1 yields the constrained energy minimization (CEM) in (12.52). Using the same token we can also define a new hyperspectral measure weighted by a posteriori correlation from the EDOSP, called MDCEM defined by
Interestingly, comparing (16.18) to (16.15) MDRX and MDCEM have the same identical structure except the a posteriori correlation in (16.15) provided by K−1 as opposed to R−1 used to account for a posteriori correlation in (16.18).
As special cases where the sample spectral covariance matrix K and the sample spectral correlation matrix R are whitened, that is, and , both (16.15) and (16.18) are reduced to ED
(16.19)
According to RXD specified by (12.76), we can also derive a new hyperspectral measure, denoted by MFDRX by replacing the both r's in (12.76) with sj and si, respectively, as follows:
where μ is the sample mean of the data to be processed. Since sj and si are not the same signature vectors, the values produced by in (16.20) are not necessarily non-negative. In this case, the absolute value is used in (16.20).
As an alternative, we can also take advantage of CEM in another way to account for a posteriori correlation by designing a new hyperspectral measure, called CEM-matched filter distance, MFDCEM defined by
Comparing (16.21) with (16.20), (16.20) can be also obtained by replacing si, R−1 and sj with si − μ, K−1 and sj − μ, respectively.
In analogy with (16.17), if K and R are whitened, that is, and , and μ = 0, (16.20) and (16.21) are reduced to SAM
where SAM(si,sj) is defined by (16.2). Interestingly, the four proposed a posteriori correlation-based hyperspectral measures, MDRX, MDCEM, MFDRX, and MFDCEM turn out to be the same four target discrimination measures developed in Chang and Chiang (2002).
Recently, an adaptive coherence estimator (ACE) developed by Kraut et al. (1999) and
where d is the target signal to be detected and r is a data sample vector to be processed. By virtue of (16.23) we can further define a new discrimination measure, denoted by MFDACE by replacing d with si and r with sj as
If we further use K−1/2 as a whitening matrix as discussed in Section 6.3.1 of Chapter 6 (i.e., making K an identity matrix I by K=I) and define , , and , then (16.23) and (16.24) can be re-expressed respectively as follows
(16.25)
which is a square of an inner product of two unit vectors, and , and
which also becomes the SAM measure of two unit signature vectors and similar to (16.22) with signature vector lengths being unit length.
In addition to discrimination specified by (16.15) and (16.18) and (16.21), (16.22), (16.24) and (16.26) these equations can be also used to perform identification in the same way that (16.12) and (16.13) do by comparing a real signature vector against a database Δ. However, such identification is rather straightforward because the used a posteriori correlation is provided by either sample covariance matrix K or sample correlation matrix R compared to the a priori correlation which must be determined by the undesired signature matrix U used for annihilation.
Since all the spectral measures defined by (16.10) and (16.11), (16.15) and (16.18), and (16.20), (16.21), (16.24) involve the calculation of correlation either provided by or the inverse of the sample spectral correlation matrix, R−1 or the inverse of the sample covariance matrix K−1, they can be referred to as second-order hyperspectral measures. On the other hand, the sample spectral correlation is not included in any pure signature vector-based spectral similarity measure. So, SAM and SID can be considered as the first-order spectral measures. Figure 16.1 summarizes relationships among various first-order and second-order hyperspectral measures.
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