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principles and applications of microearthquake networks

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120 5. Iwersioti arid Optirnizntiori<br />

(5.58) x = A-b<br />

is always unique. If matrix A is <strong>of</strong> full rank (i.e., Y = n), then R = I, <strong>and</strong> D<br />

= I,. Thus, fr: corresponds to the usual least squares solution. If matrix A<br />

is rank deficient (i.e., r < n), then there is no unique solution to the least<br />

squares problem. In this case, we must choose a solution by some criteria.<br />

A simple criterion is that the solution k has the least vector length, <strong>and</strong> Eq.<br />

(5.58) satisfies this requirement. Finally, we introduce the unscaled<br />

covariance matrix C (Lawson <strong>and</strong> Hanson, 1974, pp. 67-68)<br />

(5.59) c = V( ST)2VT<br />

The Moore-Penrose generalized inverse is one <strong>of</strong> many generalized<br />

inverses (Ben-Israel <strong>and</strong> Greville, 1974). In other words, there are other<br />

choices for the matrix H, which can serve as an inverse, <strong>and</strong> thus one can<br />

obtain different approximate solutions to the problem Ax = b. For example,<br />

in the method <strong>of</strong> damped least squares (or ridge regression), the<br />

matrix H is chosen to be<br />

(5.60a)<br />

H = VFSTUT<br />

In this equation, F is an n X n diagonal filter matrix whose components are<br />

(5.60b)<br />

F- 22 = u:/(uf + 02) for i = I, 2, . . . , n<br />

where 8 is an adjustable parameter usually much less than the largest<br />

singular value ul.<br />

The effect <strong>of</strong> this H as the inverse is to produce an estimate Er whose<br />

components along the singular vectors corresponding to small singular<br />

values are damped in comparison with their values obtained from the<br />

Moore-Penrose generalized inverse solution. This Er can be shown (Lawson<br />

<strong>and</strong> Hanson, 1974) to solve the problem<br />

(5.60~) minimize {IIAx - bI(2 + O z ~ ~ ~ ~ z }<br />

<strong>and</strong> thus represents a compromise between fitting the data <strong>and</strong> limiting the<br />

size <strong>of</strong> the solution. Such an idea is also used in the context <strong>of</strong> nonlinear<br />

least squares where it is known as the Levenberg-Marquardt method (see<br />

Section 5.4.3).<br />

Unlike the ordinary inverse, the Moore-Penrose generalized inverse<br />

always exists, even when the matrix is singular. In constructing this generalized<br />

inverse, we are careful to h<strong>and</strong>le the zero singular values. In Eq.<br />

(539, we define u: = l/at only for ui > 0, <strong>and</strong> ui = 0, for ui = 0. This<br />

avoids the problem <strong>of</strong> the ordinary inverse, where (T;' = l/ui. Furthermore,<br />

singular values give insight to the rank <strong>and</strong> condition <strong>of</strong> a matrix.<br />

The usual definition <strong>of</strong> rank <strong>of</strong> a matrix is the maximum number <strong>of</strong>

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