Ablation of organic polymers is described on the basis of photothermal bond
breaking within the bulk material. Here, we assume a first order chemical
reaction, which can be described by an Arrhenius law, Ablation starts when
the density of broken bonds at the surface reaches a certain critical value
. In order to understand the ablation behavior near the threshold fluence,
phi(th), non-stationary regimes are considered. The present treatment revea
ls several qualitative differences with respect to models which treat ablat
ion as a surface process: (i) Ablation starts sharply with a front velocity
that has its maximum value just after the onset. (ii) The transition to qu
asi-stationary ablation is much faster. (iii) Near threshold, the ablated d
epth has a square-root dependence on laser fluence, phi - phi(th). (iv) Wit
h phi approximate to phi(th), ablation starts well after the laser pulse. (
v) The depletion of species is responsible for the Arrhenius tail with flue
nces phi less than or equal to phi(th). (C) 1999 Elsevier Science B.V. All
rights reserved.