Let and be both continuous functions on
with for and let , $G\left( x\right) =\mathcal{L
}\left( g\right) fgx>0t^{\ast }\in \left( 0,\infty
\right) f/g\left( 0,t^{\ast }\right)
\left( t^{\ast },\infty \right) F/G\left( 0,\infty \right) $ if and only if
\begin{equation*} H_{F,G}\left( 0^{+}\right) =\lim_{x\rightarrow 0^{+}}\left(
\frac{F^{\prime }\left( x\right) }{G^{\prime }\left( x\right) }G\left( x\right)
-F\left( x\right) \right) \geq 0, \end{equation*} with \begin{equation*}
\lim_{x\rightarrow 0^{+}}\frac{F\left( x\right) }{G\left( x\right) }
=\lim_{t\rightarrow \infty }\frac{f\left( t\right) }{g\left( t\right) }\text{
and \ }\lim_{x\rightarrow \infty }\frac{F\left( x\right) }{G\left( x\right)
}=\lim_{t\rightarrow 0^{+}}\frac{f\left( t\right) }{g\left( t\right) }
\end{equation*} provide the indicated limits exist. While $H_{F,G}\left(
0^{+}\right) <0x^{\ast }>0F/G$ is
increasing on and decreasing on $\left( x^{\ast
},\infty \right) $. As applications of this monotonicity rule, a unified
treatment for certain bounds of psi function is presented, and some properties
of the modified Bessel functions of the second are established. These show that
the monotonicity rules in this paper may contribute to study for certain
special functions because many special functions can be expressed as
corresponding Laplace transforms.

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