  We study horocycle eigenfunctions at Lobachevsky plane. These are functions
$u\colon \mathbb H=\mathbb C^+=\{z\in\mathbb C\colon \Im z>0\}\to\mathbb C$
such that $\left(-y^2\left(\frac{\partial^2}{\partial
x^2}+\frac{\partial^2}{\partial y^2}\right)+ 2i\tau y\frac{\partial}{\partial
x}\right)u(x+iy)=s^2 u(x+iy)$, $x+iy\in\mathbb C^+$, with $\tau,s\in\mathbb R$,
$\tau$ large and $s/\tau$ small. In other words, we study eigenfunctions of
\emph{magnetic} quantum Hamiltonian on hyperbolic plane. By semiclassical
correspondence principle, asymptotic behavior of such functions is related to
horocycle flow on $T\mathbb H$. If a sequence of horocycle functions possesses
microlocal quantum unique ergodicity at the admissible energy level (with
$\hbar=1/\tau$) then we may find asymptotic distribution of divisor of $u$
analytically continued to the complexified Lobachevsky plane $\mathbb H^\mathbb
C$. This is done by establishing the asymptotic estimates on $|u|$ in $\mathbb
H^\mathbb C$. The growth of functions $u$ as $\tau\to\infty$ turns to be
governed by the growth of complexified \emph{gauge factor} occurring in
$\tau$-automorphic kernels for functions on $\mathbb H$.
