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Extension Theorems of Hahn-Banach Type for Nonlinear Disjointly ...

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308 MARCUS AND MIZEI.<br />

PROPOSITION 3.4. Let ~2’ be a rich subspace <strong>of</strong> L”(m). Then. there e.rists a<br />

vector measure p: 7 + I1 such that<br />

I. TV has bounded total variation (which we denote by j p I);<br />

II. TV is absolutely continuous with respect to m;<br />

III. p is a I.yapunov measure;<br />

IIT. &? =: {f ELm(m) : Snf dW = O}.<br />

Conversely, if TV: 7 ---+ l1 is a Lyapunov measure satisfying conditions I and II<br />

and if AS? is de$ned by IV, then Jd is a rich subspace.<br />

A measure p satisfying the conditions <strong>of</strong> Proposition 3.4 will bc called a<br />

Lyapunov measure associated with JY.<br />

Given a Lyapunov measure, one can construct related measures which arc<br />

also <strong>of</strong> Lyapunov type. The f o 11 owing proposition describes two such<br />

constructions.<br />

PROPOSITION 3.5. Let TV: 7 - l X be a Lyapunov measure which is absolutely<br />

continuous with respect to m.<br />

(a) If gl ,..., g,. are in Ll(m) and p: 7 + Rk :< S is the measure given bzl<br />

then j.2 is a Lyapunov measure.<br />

F(E) .-z (lEgl dm ,... , .kg, dnz, p(E)), VE E 7, (3.1)<br />

(b) If u is a p-integrable function and af 1/U is the indefinite integral <strong>of</strong> u z&h<br />

respect to p, then vl, is a Lyapunov measure.<br />

For the pro<strong>of</strong> <strong>of</strong> part (a) see [9; Sect. 21 and <strong>for</strong> the pro<strong>of</strong> <strong>of</strong> part (1~) see<br />

[4; Chap. V, Sect. 21.<br />

We now prove the following statement which was mentioned in Section 2.<br />

LEMMA 3.6. (a) If J&’ is a closed linear subspace <strong>of</strong> LY(m), 1 ; p < z,<br />

such that A? is <strong>of</strong> $nite codimension, then At is a rich subspace.<br />

(b) If .Ad is a w*-closed linear subspace <strong>of</strong> Lx(m) <strong>of</strong> Ji ni t e codimension then A<br />

is a rich subspace.<br />

Pro<strong>of</strong>. Under the above assumptions the annihilator <strong>of</strong> JZZ’ in L”(M), (1 /p) +<br />

(l/q) :: I, is finite dimensional. i2s be<strong>for</strong>e, denote the annihilator by k’ .<br />

Clearly, by assumption (a) or (b), the annihilator <strong>of</strong> .~&‘l in Ln(m) is precisely JZ.<br />

Let (ql ,..., pk) be a basis <strong>for</strong> J&‘~ and set

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