The growth due to the Rayleigh-Taylor (RT) instability of single-wavel
ength surface perturbations on planar foils of brominated CH [CH(Br)]
and fluorosilicone (FS) was measured. The foils were accelerated by x-
ray ablation with temporally shaped drive pulses. A range of initial a
mplitudes (a0) and wavelengths (lambda) have been used. This paper foc
uses upon foils with small a0/lambda, which exhibit substantial growth
in the linear regime, and are most sensitive to the calculated growth
rate. The CH(Br) foils exhibit slower RT perturbation growth because
opacity differences result in a larger ablation velocity and a longer
density scale length than for FS. Tabulated opacities from detailed at
omic models, OPAL [Astrophys. J. 397, 717 (1992)] and super transition
array (STA) [Phys. Rev. A 40, 3183 (1989)] were employed. Unlike prev
ious simulations which employed the average atom (XSN) opacity treatme
nt, parameter adjustments to fit experimental data no longer appear ne
cessary. Nonlocal thermodynamic equilibrium (NLTE) effects do not appe
ar to be important. Other variables which may affect the modeling, suc
h as changes of the equation of state and radiation drive spectrum, we
re also examined. The current calculational model, which incorporates
physically justified choices for these calculational ingredients, agre
es with the Nova single wavelength RT perturbation growth data.