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Is this statement true. A bounded half-superharmonic function in $\mathbb R$ is a constant. That is $(-\Delta)^{1/2} u\geq 0$ implies $u\equiv 0.$

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This claim true, but the details depend on your favourite definition of $(-\Delta)^{1/2} u$ and regularity assumptions on $u$.

One argument could be as follows: Suppose that $u \geqslant 0$ and $(-\Delta)^{1/2} u \geqslant 0$. Denote by $P_r(x,z)$ the Poisson kernel for $(-\Delta)^{1/2}$ in $(-r,r)$ and by $G_r(x,y)$ the Green function for $(-\Delta)^{1/2}$ in $(-r,r)$. Then $$ u(x) = \int_{(-r,r)} G_r(x,y) (-\Delta)^{1/2} u(y) dy + \int_{\mathbb{R} \setminus (-r,r)} P_r(x,z) u(z) dz . $$ In particular, $$ u(x) \geqslant \int_{(-r,r)} G_r(x,y) (-\Delta)^{1/2} u(y) dy . $$ Passing to the limit as $r \to \infty$ and using the monotone convergence theorem, we find that $$ u(x) \geqslant \int_{\mathbb{R}} \infty \times (-\Delta)^{1/2} u(y) dy .$$ It follows that $(-\Delta)^{1/2} u(y) = 0$, and, consequently, $u$ is harmonic for $(-\Delta)^{1/2}$. By Liouville's theorem, $u$ is constant.

You can find more details in Landkoff's book [1], I suppose. Liouville's theorem in full generality is due to Fall [2].

References:

[1] N. S. Landkof, Foundations of Modern Potential Theory, Springer, New York–Heidelberg, 1972

[2] M. M. Fall, Entire $s$-harmonic functions are affine, Proc. Am. Math. Soc., 144(6) (2016), 2587–2592

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  • $\begingroup$ Thank you for the explicit proof. At this moment, I consider $u$ is smooth and bounded. $\endgroup$
    – Spal
    Commented Oct 29, 2019 at 7:08
  • $\begingroup$ @Spal: OK, then you are good to go. The expression for $u(x)$ in terms of $G_r$ and $P_r$ is a relatively simple consequence of Dynkin's formula, which works for functions in the Feller domain; this includes $C_0^2(\mathbb{R})$, and your function can be approximated appropriately by $C_0^2(\mathbb{R})$ functions. $\endgroup$ Commented Oct 29, 2019 at 8:26

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