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Theorem 15.35.29016C2906071

Theorem 15.35.2.9016C2906071 Fix $\lambda >0$, and suppose that (15.35.1) has an exponential subsolution $s\in \mathrm{PSH}(X,h)$. For $k\geq 1$, let $u_ k$ be the continuous solution of

\[ \mathrm{MA}_ h(u_ k)=\mathrm{e}^{\lambda u_ k}f_ k\, \mathrm{d}V, \qquad f_ k=\min (f,k), \]

given by theorem 14.19.3. Then $u_ k$ decreases to a solution $u_\lambda $ of (15.35.1), and $\mathrm{MA}^{\mathrm{ext}}_ h(u_\lambda )$ has finite mass. Moreover, $u_\lambda $ is the greatest exponential subsolution: every exponential subsolution $v$ at exponent $\lambda $ satisfies $v\leq u_\lambda $. In particular, $u_\lambda $ is the greatest solution of (15.35.1).

Proof. Since $f_ k\leq f_{k+1}$, lemma 14.19.28 gives $u_{k+1}\leq u_ k$.

We first show that every exponential subsolution $v$ lies below each $u_ k$. Let $t>0$. On the set $\{ u_ k<v-t\} $,

\[ \mathrm{MA}_ h(u_ k)=\mathrm{e}^{\lambda u_ k}f_ k\, \mathrm{d}V \leq \mathrm{e}^{-\lambda t}\mathrm{e}^{\lambda v}f\, \mathrm{d}V \leq \mathrm{e}^{-\lambda t}\mathrm{MA}^{\mathrm{ext}}_ h(v-t). \]

Since $u_ k$ is bounded, $P_{h/2}(u_ k)\geq \inf _ Xu_ k$ is not identically $-\infty $, and $v-t\preceq u_ k$. Strict domination, theorem 15.2.2, therefore gives $u_ k\geq v-t$. Letting $t\downarrow 0$ gives $u_ k\geq v$.

In particular $s\leq u_ k\leq u_1$ for every $k$, so the decreasing limit $u_\lambda \geq s$ is not identically $-\infty $ and belongs to $\mathrm{PSH}(X,h)$. By lemma 5.29.19, $u_ k\to u_\lambda $ in capacity. Choose a constant $A\geq \sup _ Xu_1$. The nonpositive functions $u_ k-A$ satisfy

\[ \mathrm{MA}^{\mathrm{ext}}_ h(u_ k-A)=\mathrm{e}^{\lambda (u_ k-A)}\, \mathrm{e}^{\lambda A}f_ k\, \mathrm{d}V, \]

and $\mathrm{e}^{\lambda A}f_ k\to \mathrm{e}^{\lambda A}f$ in $L^1(\mathrm{d}V)$. Theorem 15.34.2, applied with $\mu =\mathrm{d}V$ and constant exponents, shows that $\mathrm{MA}^{\mathrm{ext}}_ h(u_\lambda )$ is finite and that $u_\lambda $ solves (15.35.1). Finally, every exponential subsolution lies below all $u_ k$, hence below $u_\lambda $, which is itself a subsolution. $\square$

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