The role of incidence angle in the laser ablation of planar ICF targets

TL;DR

This paper investigates how the laser incidence angle affects ablation dynamics in planar ICF targets, revealing that ablation rate and pressure depend on the cosine of the angle, with implications for optimizing polar direct drive configurations.

Contribution

It extends the textbook laser ablation model to include incidence angle effects, providing analytical scaling laws and insights for PDD target design.

Findings

Ablation rate scales with cosine^(4/3) of incidence angle.

Ablation pressure scales with cosine^(2/3) of incidence angle.

Conduction zone width increases with incidence angle, reducing laser imprint.

Abstract

The effect of the laser ray incidence angle on the mass ablation rate and ablation pressure of planar inertial confinement fusion (ICF) targets is explored using an idealized model. Polar direct drive (PDD) on the National Ignition Facility (NIF) requires the repointing of its 192 beams clustered within 50 degrees of the poles to minimize the imparted polar varying payload kinetic energy of the target. Due to this repointing, non-normal incidence angles of the beam centerlines are encountered in any PDD design. The formulation of a PDD scheme that minimizes non-uniformity is a significant challenge that requires an understanding of the induced differences in ablation including those of incidence angle. In this work, a modified version of the textbook model of laser ablation [Manheimer et al. Phys. Fluids 25, 1644 (1982)] is used to demonstrate that the mass ablation rate and ablation pressure scale with the 4/3 and 2/3 power of the cosine of the laser ray incidence angle for the planar case during the beginning portion of the laser ablation. This result is considered with an idealized 1-D two segment planar model using rays at different incidence angles for each segment. Within the model, the segments cannot have equal mass and velocity simultaneously without tailoring the ray's time-dependent intensity for each segment. However, with the correct segment-to-segment time-independent ray intensities, equal velocity and dynamic pressure can be achieved approximately without tailoring. Additionally, an analytic prediction for the conduction zone width as a function of incidence angle is provided. It is predicted that this width increases with incidence angle, resulting in a decrease in laser imprint, an effect which has been previously observed in experiments. These results, when generalized to spherical geometry, may provide insight into the implosion dynamics encountered in PDD.