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There is no need therefore to discuss this system any further. Let us turn our attention then to the more interesting case of a double zero root. It will be convenient to take the system as n + 2 dimensional. If A,,... denotes the usual quantities A,... 1) then by a suitable choice of coordinates A, = diag(02, A ) where A is an n x n stable matrix and O2 has one of two forms J 02=(0 J. 0 0 0 0 or 02=( If O2 is of the first form the system reduces to lil = -B ld4 t 2 = - B2Cp(a) f = Ax - bq(a) a = 7151 + Y 2 t 2 + c’x It is clear though that there exist nonzero constants that the above system has the solution t1 = gl, t2 = 52 r2,5, xand 0,E2a such0.

Dt Since by hypothesis o(t) + + 00 with t, and since Ily(t)II remains finite we may choose T so large that for t 2 T we have o(t) - C'A - ' y ( t ) > 0. Upon integrating then from T t o t we obtain [o(t) - C'A - 'Y(t)]'T < 0. As a consequence, since Ily(t)II is bounded, so is the proof of the theorem. o(t). This completes $3. Lurie's Method and a Variant By taking a more restricted type of matrix C and assuming that the characteristic roots of the matrix A are all distinct, Lurie obtained a narrower sufficiency condition for absolute stability than the inequality (Fi).

A more complete result is the following proposition due to LaSalle [l]. 2) Theorem of LaSalle. Let A be stable and C (hence B ) > 0. Then d C - ' d > c'A-'b. 3) 28 52. 1 1) is still valid without imposing on q(a) property I11 of I , $1 (divergence o f t h e integral @(a) as a -, f 00). 3a) Corollary. 1) in the strongerform p > c'A-'b. REMARK. 3) was obtained earlier by Yacubovich. 3). This is the crux of the matter and the more difficult part of the argument: we first show that if x , y are two n vectors then (Bx - y)'C- ' ( B x - y ) 2 2y'A- ' x .

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