  A new x-ray amplification mechanism is considered in an interaction between a
x-ray and an intense visible-light laser in a plasma. In normal circumstances,
the x-ray amplification from this type of the physical processes is implausible
because its phase, which is the \textbf{non-resonant} perturbation, is not
suitable for transferring the energy from the visible light laser to the x-ray.
As proposed in this paper, this undesirable phase can be manipulated into the
desirable one. Two situations are considered. The first case is in the presence
of the strong plasma density gradient. A lasting amplification is possible when
a strong Langmuir wave, whose phase velocity matches with the x-ray group
velocity, provides the density gradient along the way of the x-ray propagation.
  The second case is in the presence of a pre-excited Langmuir wave. The author
considers two lasers, with their frequency differing by the Langmuir wave,
counter-propagating and exciting a rather strong Langmuir wave. In the presence
of the mentioned Langmuir wave, it is demonstrated that the ponderomotive
interaction between the x-ray and one of the lasers excites the plasma density
perturbation with a desired phase, resulting to amplify (decay) the x-ray
(visible light laser). The condition for achieving the mentioned favorable
phase and the amplification strength, when the condition is met, is estimated.
The amplification strength is quite high, where the gain per length could reach
1000 per cm in both cases.
