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Copyright: American Scientific Publishers
RESEARCH ARTICLE
Copyright © 2008 American Scientific Publishers
All rights reserved
Printed in the United States of America
Journal of
Nanoscience and Nanotechnology
Vol. 8, 6075–6081, 2008
Multi-Time Step Modeling of Plume Dynamics in
Nanosecond-Scale Carbon Ablation
Kedar Pathak and Alex Povitsky
*
Department of Mechanical Engineering, The University of Akron, Akron, OH 44325-3903, USA
The time span of plume dynamics in laser ablation of carbon ranges from nanoseconds to millisec-
onds. Multi-time step approach is developed to study the plume dynamics over this entire range with
minimum requirements of numerical computational resources. This approach is applied to study
one of the important aspects of nanosecond-scale laser ablation, namely the shielding of incident
laser beam with previously ejected plumes. Capturing the shielding effect requires smaller than
nanosecond-scale time step because of large velocity and pressure gradients in plume. Use of this
time step over the entire domain needs enormous amount of computer time to cover the whole
time span of plume dynamics. Multi-time step modeling for such an application is therefore useful.
In general, for nanosecond-scale laser ablation this shielding is caused by ionized particles and
by gas molecules. It is shown for carbon plume resulting from the nanosecond-scale lasers that
the degree of ionization is small. Ionization of ablated carbon is estimated by Saha equation for
the given initial plume conditions. The shielding of incident laser beam is therefore calculated by
normal molecular absorption. The laser-light intensity that reaches the target for subsequent pulses
is evaluated.
Keywords: Multi-Time Step, Plume Dynamics, Shielding Effect, Carbon Ablation.
1. INTRODUCTION
Plume dynamics in laser ablation in presence of back-
ground gas has been studied experimentally
1–8
and theore-
tically.
9–18
Nevertheless, the laser ablation in the process
of production and synthesis of nanoparticles is still an
open research field that is bursting with numerous impor-
tant phenomena, which are still to be understood by
researchers.
19–21
The entire process of laser ablation invol-
ves numerous phenomena such as molecular bond break-
ing, non-equilibrium electronic excitations, multi-photon
or saturation processes, gas dynamics of plume, condensa-
tion of metallic catalysts, nucleation of nanotubes etc. In
general, the time scales that spans in laser ablation range
from femtosecond-scale to millisecond-scale.
In carbon nanotubes synthesis, it is of crucial impor-
tance to know the dynamic behavior of the plume of
ablated material in the laser ablation furnace. When a pow-
erful laser illuminates the target, it sublimes the target
surface and creates the high-pressure plume. The result-
ing gas explosion produces a plume of rapidly expanding
gaseous carbon with embedded catalyst particles. Lit-
tle experimental information has been available for the
*
Author to whom correspondence should be addressed.
initial conditions at the surface of the carbon target.
18
For complete description of gas dynamic and thermody-
namic state of plume one needs to know the mass ablation
rate, temperature, pressure, and the injection velocity with
which the ablated plume emerges. Out of these parame-
ters the only known experimental parameter is the mass
ablation rate.
18
The estimations based on the ideal gas and
the Clausius-Claperyon equations resulted in the initial gas
pressure in the ablated plume of the order of 100 atm.
2 18
This pressure produces shock waves in the ambient fur-
nace gas. The propagation of incident and reflected shock
waves in a confined space of laser furnace affect the plume
behind the incident shock wave. These effects of furnace
geometry on plume evolution have been studied.
17
In the
study,
22
the authors have obtained the temperature of the
catalyst particles in plume, which is crucial for model-
ing of growth of nanotubes. They show the influence of
chamber pressure, injection velocity, and multiple ejec-
tions of the plume on the temperature of particles, and
discuss physical reasons for non-monotonic temperature
behavior of catalyst particles. Their study included multi-
ple plumes; however, they did not consider shielding effect
and assumed the same mass ablation rate and injection
velocity for all plumes.
J. Nanosci. Nanotechnol. 2008, Vol. 8, No. 11 1533-4880/2008/8/6075/007 doi:10.1166/jnn.2008.SW20 6075