Mario M. Jakas
J.
Phys. D: Appl. Phys. 38, 1-5 (2005)
E.R.Custidiano and Mario M. Jakas.
Physical Review A 72, 022708- (2005).
Mario
M. Jakas
Phil.
Trans. R. Soc. London
A, 139-156 (2004)
M. M. Jakas, F.J.Pérez de
Physical Review A 68,
032903-032909 (2003).
Mario
M. Jakas
Nuclear Instruments and Methods in Physics Research B 193, 727-733
(2002).
Mario M. Jakas, E. M. Bringa and R.E. Johnson.
Physical Review B 65, 165425-
(2002).
E.R. Custidiano, F.J.Pérez de
Physical Review A 66, 052902
(2002).
F.J.Pérez de
Radiation Effects
and Defects in Solids 157, 289-302 (2002).
Jakas-M.M., E.M. Bringa
and R.E. Johnson.
Physical Review B 62, 824-830 (2000). Abstract
Bringa-E.M., Jakas-M.M. and Johnson
R.E.
Nuclear-Instruments-&-Methods-in-Physics-Research,-Section-B. vol 164-165, April 2000, pages 762-771.
Abstract
Mario M. Jakas
Radiation Effects and Defects in Solids. Vol 152, 157-163 (2000). Abstract
E.M. Bringa,
R.E. Johnson and Jakas-M.M.
Physical Review B60, 15107-15116(1999). Abstract
R.A. Baragiola, C.L. Atteberry, D.A. Bahr and Jakas-M.M.
Nuclear Instruments and Methods B157, 233-238 (1999). Abstract
M.I. Pascuet, C.J. Aquino, N.E. Capuj, and Jakas-M.M.
Radiation Effects and Defects in Solids 145,179-190 (1998). Abstract
Mario M. Jakas.
Nuclear-Instruments-&-Methods-in-Physics-Research,-Section-B. vol.115, no.1-4;
July 1996; p.255-60. Abstract
Mario M. Jakas
Radiation-Effects-and-Defects-in-Solids. vol.141, no.1-4;
1997; p.23-36. Abstract
Capuj-NE and Jakas-MM.
Nuclear Instrum.and
Methods in Physics research, Section B 115 , 146
(1996). Abstract
Mario M. Jakas
Physical-Review-A-. vol.52, no.1; July 1995; p.866-9. Abstract
Jakas-MM; Capuj-NE. Physical-Review-A-.
vol.52, no.1; July 1995; p.439-44. Abstract
Jakas-MM and Capuj-NE.
Physical-Review-A-. vol.54, no.6; Dec. 1996; p.5031-6. Abstract
Jakas-MM and Capuj-NE.
Journal-of-Physics:-Condensed-Matter. vol.7, no.24; 12 June 1995; p.4593-601. Abstract
Jakas-MM; Hernandez-Cabrera-AJ and Aceituno-P.
Modern-Physics-Letters-B. vol.9, no.5; 28 Feb. 1995;
p.299-305 Abstract
Jakas-MM and Capuj-NE.
Physica-A. vol.215, no.1-2;
15 April 1995; p.51-60. Abstract
Jakas-M.M. and Capuj-NE.
Physical-Review-A-. vol.51, no.3; March 1995; p.2277-80. Abstract
Jakas-MM and Capuj-NE.
Nuclear-Instruments-&-Methods-in-Physics-Research,-Section-B. vol.B93, no.1;
July 1994; p.14-20. Abstract
Mario M. Jakas
Nuclear-Instruments-&-Methods-in-Physics-Research,-Section-B. vol.B93, no.1; July
1994; p.11-13. Abstract
Mario M. Jakas
Vacuum. vol.44, no.3-4; March-April 1993; p.337-9.
Abstract
Mario M. Jakas
Nuclear-Instruments-&-Methods-in-Physics-Research,-Section-B.
vol.B69, no.1; June 1992; p.142-5. Abstract
J. Calera-Rubio, A. Gras-Martí, N.R. Arista, Mario M. Jakas, S. Sroubek and G. Falcone.
Radiation Effects
and Defects in Solids, 117, 173- (1991).
Calera-Rubio-J; Gras-Marti-A; Arista-NR; Jakas-MM; Sroubek-Z; Falcone-G.
Surface-Science. vol.251-252;
July 1991; p.136-9. Abstract
Forcada-ML; Jakas-MM
and Gras-Marti-A.
Journal-of-Chemical-Physics. vol.95,
no.1; 1 July 1991; p.706-8. Abstract
N.R. Capuj, and Mario M. Jakas.
Ion-Solid Interactions, Eds. Gras-Martí, F.Flores, N.R.Arista, Plenum (1990).
Jakas-MM and Capuj-NE.
Physical-Review-A-. vol.40, no.12; 15 Dec. 1989; p.7369-72. Abstract
Jakas-MM and Capuj-NE.
Nuclear-Instruments-&-Methods-in-Physics-Research, Section-B.
vol.B36, no.4; April 1989; p.491-3. Abstract
Capuj-NE; Eckardt-JC; Lantschner-GH; Arista-NR and Jakas-MM.
Physical-Review-A. vol.39, no.3; 1 Feb.
1989; p.1049-52. Abstract
N.E. Capuj, J.C. Eckardt, G.H. Lantschner, N.R. Arista and Mario
M. Jakas.
Proc.
Plasma-Surface Interaction and Processing of Materials,
N.E. Capuj and Mario M. Jakas.
Proc.
Plasma-Surface Interaction and Processing of Materials,
Lantschner-GH; Eckardt-JC; Jakas-MM; Capuj-NE
and Ascolani-H.
Physical-Review-A. vol.36, no.10; 15
Nov. 1987; p.4667-71. Abstract
Oliva-Florio-A; Baragiola-RA; Jakas-MM; Alonso-EV and Ferron-J.
Physical-Review-B-. vol.35, no.5; 15
Feb. 1987; p.2198-204. Abstract
Arista-NR; Jakas-MM;
Lantschner-GH and Eckardt-JC.
Physical-Review-A-. vol.34, no.6;
Dec. 1986; p.5112-4. Abstract
Harrison-DE-Jr;
Jakas-MM.
Radiation-Effects.
vol.99, no.1-4; 1986; p.153-69. Abstract
Harrison-DE-Jr and Jakas-MM.
Nuclear-Instruments-&-Methods-in-Physics-Research, Section B . vol.B15, no.1-6; April 1986; p.25-8. Abstract
Webb-RP; Harrison-DE-Jr; and Jakas-MM.
Nuclear-Instruments-&-Methods-in-Physics-Research,-Section-B. vol.B15, no.1-6;
April 1986; p.1-7. Abstract
Jakas-MM and Harrison-DE-Jr.
Nuclear-Instruments-&-Methods-in-Physics-Research, Section B . vol.B14, no.4-6; April 1986; p.535-41. Abstract
Jakas-MM and Harrison-DE-Jr.
Physical-Review-Letters. vol.55, no.17; 21 Oct. 1985; p.1782-5. Abstract
Jakas-MM and Harrison-DE-Jr.
Physical-Review-B-. vol.32, no.5; 1 Sept. 1985; p.2752-60. Abstract
Jakas-MM and Harrison-DE-Jr.
Surface-Science. vol.149, no.2-3;
Jan. 1985; p.500-16. Abstract
Jakas-MM and Harrison-DE-Jr.
Physical-Review-B-. vol.30, no.6; 15 Sept. 1984; p.3573-4. Abstract
Eckardt-JC; Lantschner-GH; Jakas-MM andPonce-VH.
Nuclear-Instruments-&-Methods-in-Physics-Research,
Section B . vol.230, no.1-3; March
1984; p.168-72. Abstract
Jakas-MM and Ponce-VH.
Journal-of-Physics-D-(Applied-Physics). vol.17, no.6; 14
June 1984; p.1301-14. Abstract
Jakas-MM; Lantschner-GH; Eckardt-JC and Ponce-VH.
Physical-Review-A-. vol.29, no.4;
April 1984; p.1838-43. Abstract
Jakas-MM and Biersack-JP.
Zeitschrift-fur-Physik-A-(Atoms-and-Nuclei). vol.315, no.1; 1984;
p.29-33. Abstract
Jakas-MM; Lantschner-GH; Eckardt-JC and Ponce-VH.
Physica-status-solidi-B. vol.117, no.2; 1 June 1983; p.K131-4.
Abstract
Mario M. Jakas
Physical-Review-A-. vol.25, no.3;
March 1982; p.1782-5. Abstract
E.V. Alonso, R.A. Baragiola, J. Ferrón, M.M. Jakas and A.R. Oliva-Florio.
Physical Review. B 22, 80 (1981).
Jakas-MM and Williams-MMR.
Journal-of-Physics-D-(Applied-Physics). vol.13, no.7; 14 July 1980; p.1169-80 Abstract
Jakas-MM and Baragiola-RA.
Physical-Review-Letters. vol.44, no.6; 11 Feb. 1980; p.424-6 Abstract
Oliva-Florio-AR;
Alonso-EV; Baragiola-RA; Ferron-J
and Jakas-MM.
Radiation-Effects-Letters. vol.50, no.1; 1979; p.3-7 Abstract
Mario
M. Jakas
Physics-Letters-A. vol.72A, no.6; 6
Aug. 1979; p.423-6. Abstract
Bringa-E.M., Jakas-M.M. and Johnson R.E.
Nuclear-Instruments-&-Methods-in-Physics-Research,-Section-B vol. 164-165,
April 2000, pages 762-771.
Abstract
Jakas-M.M. and E.M. Bringa.
Submitted to Physical Review B.
Abstract
A Note on thermal spikes and
sputtering yields.
Jakas-M.M.
Radiation Effects and Defects in Solids. Vol 152, 157-163 (2000).
Abstract
Molecular Dynamics simulations of
electronic sputtering. E.M. Bringa, R.E.
Johnson and
Jakas-M.M. Physical Review B60, 15107-15116(1999).
Abstract
Solid-state Ozone synthesis by energetic
ions.
R.A.
Baragiola, C.L. Atteberry,
D.A. Bahr and Jakas-M.M. Nuclear Instriments and Methods B157, 233-238 (1999).
Abstract
The angular dependence of the energy
loss for high energy H+-ions transmitted through thin Al films.
M.I.
Pascuet, C.J. Aquino, N.E. Capuj, Jakas-M.M..
Radiation Effects and Defects in Solids 145,179-190 (1998).
Abstract
The production of high-energy
electrons during low energy atomic collisions in solids.
Jakas-MM.
Nuclear-Instruments-&-Methods-in-Physics-Research,
Section-B . vol.115, no.1-4; July
1996; p.255-60.
Abstract
The acceleration of electrons during low-energy atomic collisions in solids is
studied. It is shown that a classical, high energy electron can be
"trapped" in a sequence of head-on collisions with the ion and the
target atom. Then, due to the Fermi acceleration mechanism the trapped electron
may absorb energy from the center-of-mass motion up to a maximum value, above
which such a sequence becomes unstable. A quantum study of the same process
indicates that virtual states appear higher in the continuum of the
quasi-molecule formed by the nuclei in the colliding pair, which can be used by
the electron to increase its energy during the
incoming part of the collision.
The influence of multiple scattering
and Coulomb repulsion on the transmission of H2+ through solid targets.
Capuj-NE; Jakas-MM.
Nuclear-Instruments-&-Methods-in-Physics-Research,
Section-B . vol.115, no.1-4; July 1996; p.146-51
Abstract
The transmission yield of H2+ ions through solid targets decreases rapidly with
dwell time in the foil. This is basically due to the occurrence of three
mechanisms: screened Coulomb repulsion, multiple scattering and the wake
forces. Using
Increasing efficiency of ion-solid
Jakas-MM.
Radiation-Effects-and-Defects-in-Solids. vol.141, no.1-4; 1997; p.23-36
Astract
A procedure that increases the efficiency in
Trapping of a classical electron
between two heavy scattering centers.
Jakas-MM.
Physical-Review-A-. vol.52, no.1;
July 1995; p.866-9.
Abstract
This paper shows that a classical electron may get trapped within the field of
two atomic nuclei even though it is free, i.e., the total energy of the
electron is greater than that at large distances from the attractive centers.
The consequences of this phenomenon for the emission of high-energy electrons
during slow-atom bombardment of solids are discussed.
Jakas-MM; Capuj-NE.
Physical-Review-A-. vol.52, no.1; July 1995; p.439-44
Abstract
We calculate the mean energy loss of H2+ molecular ions transmitted through
carbon and aluminum foils as a function of the bombarding energy. Our results
are in good agreement with available experimental data. Furthermore, inhomogeneities containing the foil are found to be
essential in the energy-loss measurement of transmitted molecular ions.
Wake effects on the energy loss as a function of the scattering
angle for thin-film-transmitted H2+ ions
Jakas-MM; Capuj-NE
Physical-Review-A-. vol.54, no.6; Dec. 1996; p.5031-6
Abstract
We calculated the mean energy loss as a function of the exit angle for 100 and
400 keV/amu H2+ ions transmitted through thin carbon
foils. The results showed that at 100 keV the energy
loss exhibited a maximum in the forward direction as opposed to that of
protons, which had a minimum at zero degree ejection angle.
Our studies demonstrate that such a difference stems from the wake or
polarization forces acting upon the trailing ion in the cluster.
Jakas-MM; Capuj-NE.
Journal-of-Physics:-Condensed-Matter.
vol.7, no.24; 12 June 1995; p.4593-601.
Abstract
We report calculations of the energy-loss spectra for 25-300 keV/amu H2+ ions transmitted through carbon and aluminium foils. At 25 keV/amu the mean energy-loss of transmitted H2+ ions
is approximately 15% smaller than that of two protons at the same velocity,
whereas at 300 keV/amu it becomes 10% greater. When
compared to those of two uncorrelated protons, the width of the energy-loss
distribution appears to increase with a decrease of the bombarding energy,
becoming 3-5 times larger at 25 keV/amu
for molecules transmitted through aluminium and
carbon foils, respectively.
Orbiting of free, classical electrons
in the field of two slowly approaching charges.
Jakas-MM; Hernandez-Cabrera-AJ; Aceituno-P.
Modern-Physics-Letters-B. vol.9, no.5; 28 Feb. 1995;
p.299-305
Abstract
The motion of a free, classical, spinless electron in
the field of two nuclei during low velocity atomic collisions is investigated.
It is found that if one neglects the bremmstrahlung
and interactions with other electrons, a free electron can orbit around the two
nuclei with a surprisingly high stability. A maximum energy, however, appears
above which such an orbiting becomes unstable. The connection between these
findings and the acceleration of electrons by means of the Fermi shuttle effect
is also discussed.
Increasing efficiency in
Jakas-MM; Capuj-NE.
Physica-A. vol.215, no.1-2;
15 April 1995; p.51-60.
Abstract
We have derived a procedure which increases the efficiency of
Wake forces and the transmission yield of H2+ through
thin carbon foils.
Jakas-MM; Capuj-NE.
Physical-Review-A-. vol.51, no.3;
March 1995; p.2277-80.
Abstract
The transmission of 0.05-1.0 MeV/amu H2+ molecular
ions has been calculated as a function of dwell time
in carbon foils. The results indicate that wake forces may have a manifest
influence upon the transmission yields. Experimental results, however, are
lacking within the range of dwell time and bombarding energy where wake effects
are expected to become noticeable.
Calculation of energetic
H2+-transmission yield using an efficient
Jakas-MM; Capuj-NE.
Nuclear-Instruments-&-Methods-in-Physics-Research,-Section-B-(Beam-Interactions-with-Materials-and-Atoms). vol.B93, no.1;
July 1994; p.14-20.
Abstract
The transmission yield of 0.1-1.0 MeV/amu H2+
molecular ions as a function of dwell-time ( tau ) in thin carbon foils have been calculated by
Monte Carlo (MC) simulations. As transmission yields drop rapidly with
increasing dwell-time, the simulations are speeded up by using a technique known
as killing-and-splitting (KS). This technique enables us to simulate, for the
first time, the transmission of molecules over the entire range of dwell-time
where experimental results are available, i.e., 0< tau
<30 fs. A detailed description of the KS-method
and comparisons of calculations with previous experiments are offered.
Wake effects on the transmission of fast H2+-ions
through thin carbon foils.
Jakas-MM
Nuclear-Instruments-&-Methods-in-Physics-Research,-Section-B-(Beam-Interactions-with-Materials-and-Atoms). vol.B93, no.1;
July 1994; p.11-13.
Abstract
According to
Computer simulation of growth during
molecular-beam epitaxy of metal-on-metal surfaces.
Jakas-MM.
Vacuum. vol.44, no.3-4; March-April
1993; p.337-9.
Abstract
By using
Wake effects on the center of mass of dissociated
molecules traversing thin solid films.
Jakas-MM.
Nuclear-Instruments-&-Methods-in-Physics-Research,-Section-B-(Beam-Interactions-with-Materials-and-Atoms). vol.B69, no.1;
June 1992; p.142-5.
Abstract
Calculations are presented showing that wake forces can be observed on the
angular distribution of the center of mass (COM) of dissociated fragments in
Coulomb explosion experiments. The author's results indicate that wake forces
produce a broadening in the angular distribution of the COM which may be
comparable to that of multiple scattering. Results contained in this paper aim
at new applications of Coulomb explosion techniques, especially for experiments
equipped with x-z position-sensitive detectors.
Electron excitations by slow ions in
metals.
Calera-Rubio-J; Gras-Marti-A; Arista-NR; Jakas-MM; Sroubek-Z; Falcone-G.
Surface-Science. vol.251-252; July
1991; p.136-9.
Abstract
The energy and angular distribution of electrons excited by slow charged
particles penetrating an electron gas, is analyzed using a representation of
the particle by a general self-consistent potential. The number of excited
electrons per unit path-length is also calculated. Oscillations with the
nuclear charge of the ion, Z, are obtained for the spectra of electron
excitations and the total excitation rate. These Z oscillations have the same
origin as those found, both theoretically and experimentally, for the stopping
power of low-velocity ions. The connection of electron excitation spectra with
ion
slowing down and with experiments on secondary electron emission is discussed.
On liquid-film thickness measurements
with the atomic-force microscope.
Forcada-ML; Jakas-MM; Gras-Marti-A
Journal-of-Chemical-Physics. vol.95, no.1; 1
July 1991; p.706-8.
Abstract
The authors provide a theoretical description of some measurements were the
thicknesses of solid-supported thin lubricant films are measured using the
atomic-force microscope (Mate et al., J. Chem. Phys. 90, 7550 (1989)). In their
model, the differences observed between the thicknesses measured with the force
microscope and ellipsometric thicknesses are
explained by the appearance of an instability in the
liquid film. Their calculations also predict the dependence of these
differences on the thickness of the film.
Corrections to vicinage-effect data for molecular ions
due to foil inhomogeneities
Jakas-MM; Capuj-NE.
Physical-Review-A-. vol.40, no.12; 15
Dec. 1989; p.7369-72.
Abstract
Calculations are presented showing the influence of foil inhomogeneities
upon the mean energy loss of molecular ions transmitted through thin films.
They indicate that, due to the strong dependence of the transmission of
molecular ions on thickness, previous measurements of the stopping of such ions
at low bombarding energies can be affected by thickness variations of the foil.
Scaling for the angular variation of
the energy loss of ions induced by foil inhomogeneities.
Jakas-MM; Capuj-NE.
Nuclear-Instruments-&-Methods-in-Physics-Research,
Section-B . vol.B36, no.4; April
1989; p.491-3.
Abstract
Analytical calculations have been made in order to assess the influence of foil
inhomogeneity upon the angular variation of the mean
energy loss of atomic projectiles, and to calculate the path-length as a
function of the exit angle of ions transmitted through thin, inhomogeneous
foils. By introducing reduced values of angle and thickness and assuming that
the degree of inhomogeneity amounts to a small
perturbation, a scaling law was obtained which allows one to obtain a general
solution independent of particle and target species, energy, and inhomogeneity.
Thin-film inhomogeneities
studied by energy-loss measurements using ion beams.
Capuj-NE; Eckardt-JC; Lantschner-GH; Arista-NR; Jakas-MM.
Physical-Review-A-. vol.39, no.3; 1
Feb. 1989; p.1049-52.
Abstract
A method to evaluate thin-film thickness inhomogeneities
is presented. It is based on the measurements of the first two moments of the
energy-loss distributions of swift ions traversing thin foils at two different
beam incidence angles. The authors apply the method to a set of thin ( approximately 200-AA) aluminum foils, resolving thickness
fluctuations of the order of 10%.
Variation of peak energy for energy
loss with angle of observation.
Lantschner-GH; Eckardt-JC; Jakas-MM; Capuj-NE;
Ascolani-H.
Physical-Review-A-. vol.36, no.10; 15
Nov. 1987; p.4667-71.
Abstract
The energy loss for protons on Al, Cu, and Ag thin foils around the maximum of
the stopping have been measured at two different exit angles. The bombardment
energy E/sub max/ where such a maximum occurs is found to depend on the angle
of observation, E/sub max/ being greater when the detector is positioned off
beam than when measured downstream in the beam direction. These results are
discussed in terms of a varying participation of different electrons in the
target. The effect of foil inhomogeneities on E/sub
max/ is also evaluated.
Noble-gas ion sputtering yield of gold and copper:
dependence on the energy and angle of incidence of the projectiles.
Oliva-Florio-A; Baragiola-RA; Jakas-MM; Alonso-EV; Ferron-J.
Physical-Review-B-. vol.35, no.5; 15
Feb. 1987; p.2198-204.
Abstract
The authors have measured the sputtering yield of Au and Cu targets as a
function of energy and the angle of incidence of noble-gas projectiles in the
energy range 2-50 keV. The experimental results were
compared with the analytical theory of sputtering and with computer
simulations. Their study indicates that the linear-cascade model is applicable
only asymptotically for low nuclear stopping powers.
Analysis of secondary-electron emission in beam-foil
experiments with molecular ions.
Arista-NR; Jakas-MM;
Lantschner-GH; Eckardt-JC.
Physical-Review-A-. vol.34, no.6;
Dec. 1986; p.5112-4.
Abstract
The authors analyze the possibility of large oscillatory wake effects in
secondary-electron emission induced by molecular ions, which were proposed in
previous interpretations of results derived from beam-foil experiments. They
show that theoretical expectations are in disagreement with the description of
such oscillatory effects in terms of wake phenomena. Their analysis of various
experimental evidences suggests a different origin for the effect. They propose
a simple explanation for the molecular effect in secondary-electron emission,
which is based on previous knowledge of electron emission from solid targets,
and of molecular effects in the energy loss of ion clusters in solid foils.
Simulation of the atomic collision cascade
Harrison-DE-Jr; Jakas-MM
Radiation-Effects. vol.99, no.1-4; 1986; p.153-69
Abstract
Molecular dynamics computer simulations can be used to evaluate pre-existing theoretical
concepts, or used directly as a research tool, simulations can directly
investigate natural phenomena. The TRIM program, a binary-collision simulation
of atomic collision cascades, is a well-known example of the first usage. The
authors compare and contrast TRIM results with computations from a
multiple-interaction cascade simulation program, QDYN. QDYN is described in
detail; then some issues of potential function development for simulation use
are introduced, followed by some examples of QDYN based research. Two current
simulation based research topics are presented in greater detail. One is a
study of very low energy cascades, where directed bonds and chemical effects
are important. The other is the influence of electronic processes on cascade
development. Characteristics of atoms ejected from the surface are emphasised. Both topics have potential applications in the si! mulation
of atomic collision cascades in insulators. These investigations emphasise the possibility that direct comparisons between
simulations of collision cascades in metals, semiconductors, and insulators can
help to solve outstanding research problems in both fields.
Inelastic energy losses in cascades and atom ejection
Harrison-DE-Jr; Jakas-MM
Nuclear-Instruments-&-Methods-in-Physics-Research,
Section B . vol.B15, no.1-6; April 1986; p.25-8
Abstract
Recent molecular dynamics simulation studies demonstrated the important role
that electronic stopping plays in the sputtering of metals when the loss rate
is proportional to the velocity. Inelastic energy losses by the ions and
energetic recoil atoms have relatively little effect, but losses by low energy
atoms, late in the cascade, significantly reduce the ejected atom yield. The
simulation results are consistent with recently obtained analytic results. Here
ejected atom yield ratios and energy and ejection time distributions are
compared, with and without inelastic losses, for two simulation programs:
TRIM.SP, a binary collision model and QDYN, a multiple interaction model. The
results differ little within a given model, and the differences between models
are well understood.
The computer simulation of ion induced atomic collision
cascades
Webb-RP; Harrison-DE-Jr;
Jakas-MM.
Nuclear-Instruments-&-Methods-in-Physics-Research,-Section-B-(Beam-Interactions-with-Materials-and-Atoms). vol.B15, no.1-6; April 1986; p.1-7
Abstract
The use of computer simulation to understand the physics of atomic collision
phenomenon has escalated in recent years. Even with this proliferation of
simulation codes the majority of programs fall into two categories-the event
store and the time step models. These models are discussed, and a hybrid formed
from the two is described. The best uses of each model is indicated and some
examples given. The event store simulations give an accurate method of
evaluating range data and the time step models conveniently give information on
cascade propagation and nonlinear behaviour.
A comparison between multiple
interaction computer simulations and the linear theory of sputtering.
Jakas-MM; Harrison-DE-Jr.
Nuclear-Instruments-&-Methods-in-Physics-Research,
Section B . vol.B14, no.4-6; April
1986; p.535-41.
Abstract
A multiple interaction simulation and a binary collision simulation modified to
mimic the analytic linear theory of sputtering, have been used to study the
sputtering of metal targets by ions with keV
energies. Detailed comparisons between the two models disclose fundamental
differences in the behaviour of collision cascades at
energies below 1.0 keV. The binary collision models'
failure to include multiple interactions, i.e. many-body collision effects, is
a significant shortcoming, which can lead to serious misunderstandings and
misinterpretations of the basic physical processes which are commonly
identified as 'nonlinear' sputtering.
Many-body effects in atomic-collision cascades.
Jakas-MM; Harrison-DE-Jr.
Physical-Review-Letters. vol.55, no.17; 21 Oct. 1985;
p.1782-5
Abstract
Molecular-dynamics simulations have been used to identify two cooperative
atom-ejection mechanisms which increase sputtering yield. Their effects are
analogous to the 'thermal spike', 'shock wave', and 'reduced binding energy'
sputtering mechanisms. They are examples of nonlinear, many-body effects in
cascades which go beyond collisions between randomly moving particles.
Dependence of atom ejection on electronic energy loss
Jakas-MM;
Harrison-DE-Jr
Physical-Review-B-. vol.32, no.5; 1 Sept. 1985;
p.2752-60
Abstract
The authors extend previous theoretical models to emphasize the influence of
electronic energy losses upon the ejection of atoms by bombarding ions. This
sensitivity of the sputtering yield to inelastic energy losses was first
observed in computer simulations of sputtering. The theoretical analysis
supports the simulation-derived conclusion that the total yield is much more
sensitive to electronic energy losses by the atoms than to electronic energy
losses of the bombarding ions, even when the ion is much lighter than the
target atoms.
Computer studies of the reflection of 30 keV N/sub 2//sup +/ ions from a (010)Cu
surface
Jakas-MM;
Harrison-DE-Jr
Surface-Science. vol.149, no.2-3; Jan. 1985; p.500-16
Abstract
The reflection of 30 keV N/sub 2//sup +/ molecular
ions from a Cu(010) surface has been studied using
molecular dynamics multiple interaction simulations. The model is used to
investigate the trajectories leading to the reflection of undissociated
N/sub 2//sup +/ ions. A theoretical analysis of the reflection of diatomic
molecules is also given, which provides proper insight into the process as well
as a useful guide to the simulations. In contrast to previous theories,
correlations in the motion of molecule's nuclei were found to play an important
role on the reflection of bound clusters.
Influence of electronic energy losses on atom ejection
processes
Jakas-MM;
Harrison-DE-Jr
Physical-Review-B-. vol.30, no.6; 15 Sept. 1984;
p.3573-4
Abstract
Two independent computer simulations models establish that when ions bombard
solid targets, electronic energy losses by atoms within the collision cascade
have greater influence on the ejected atom yield than the ion's electronic
losses. This conclusion is independent of the ion's mass or energy, or the mass
ratio.
The correlation between inelastic energy loss and
scattering angle in transmission experiments
Eckardt-JC; Lantschner-GH; Jakas-MM;
Ponce-VH
Nuclear-Instruments-&-Methods-in-Physics-Research,
Section B . vol.230, no.1-3; March 1984; p.168-72
Abstract
The authors measure the energy loss as a function of the emergence angle, and
the angular spread as a function of the energy loss for 50-200 keV H/sup +/ and He/sup +/ on 410 AA C and 170 AA Al foils.
A strong dependence of the angular spread on the energy loss has been observed,
as well as an angular dependence of the energy loss far beyond that predicted
by path length enlargement and nuclear stopping power. Theoretical expressions
for the previous magnitudes were obtained on the basis of a multiple scattering
formalism and a single collision energy loss-scattering angle function Q( theta ). In addition, a procedure is presented to
retrieve this Q-function from the experimental data.
Anomalous enhanced backscattering of fast light ions
from amorphous solid targets
Jakas-MM;
Ponce-VH
Journal-of-Physics-D-(Applied-Physics). vol.17, no.6; 14 June 1984;
p.1301-14
Abstract
The anomalous enhanced backscattering of fast light ions from heavy amorphous
solid targets is studied within the formalism of transport theory. The angle
distribution of emerging ions is obtained by a variational
procedure, where the correlation in the collisions on the incoming and outgoing
paths is treated as a perturbation. When using a power potential for the
ion-target interaction this distribution can be expressed in terms of reduced
variables for the emerging angle and backscattering depth, and the dependence
on the collision energy and atom species appears only on the scale factors. The
observation of the enhancement in the distribution of backscattered ions will
depend on the value of these scale factors as compared with the experimental
resolutions.
Study on the angular dependence of the average energy
loss for ions in solids
Jakas-MM; Lantschner-GH; Eckardt-JC;
Ponce-VH
Physical-Review-A-. vol.29, no.4; April 1984; p.1838-43
Abstract
By using the transport theory, the authors have derived a general expression
which connects Delta E( theta ), the average energy
loss measured at different theta emergence angles, and Q( theta ), the average
elastic and inelastic energy loss in a single scattering as a function of the
scattering angle theta , for ions transmitted through thin films. In this way,
the effect of multiple scattering of the angular dependence of the energy loss
is properly taken into account. By means of this procedure the average
energy-loss function Q is retrieved from experimental Delta E( theta ) data, as
the authors show for the cases of 50-200-keV H/sup +/ on C and Al foils.
Variational calculation of the
angular width of the multiple scattering distribution
in foil transmission
Jakas-MM; Biersack-JP
Zeitschrift-fur-Physik-A-(Atoms-and-Nuclei). vol.315, no.1;
1984; p.29-33.
Abstract
A simple formula is derived for calculating the angular width of multiple
scattering distributions for atomic particles traversing thin foils. The
universal result is obtained by applying the variational
method on standard multiple scattering theory. This
procedure can be carried through in a straight-forward way, thus saving lengthy
series expansions and Fourier transforms. In the case of power cross sections
exact analytical expressions can be obtained. A remarkably good agreement is
found between this calculation and previous theories, as well as with results
from computer simulations.
Angular dependence of stopping power
Jakas-MM; Lantschner-GH; Eckardt-JC; Ponce-VH
Physica-Status-Solidi-B. vol.117, no.2; 1 June 1983;
p.K131-4
Abstract
In a recent publication, Iferov and Zhukova (1982) reported measurements of the stopping power
as a function of the observation angle for 100 to 400 keV
protons transmitted through gold films. According to them, Q( theta ), the
average inelastic energy loss in a single scattering having a scattering angle
theta , is related with Delta E( theta ), the stopping power measured within
the angle theta according to the expression Q( theta )= Delta E( theta )- Delta
E(0)- Delta E/sub n/( theta )-( theta /sup 2//4) Delta E, where Delta E/sub n/(
theta ) is the nuclear energy loss corresponding to the scattering angle theta
and the last term in the expression represents the increase of the observed
energy loss when going from theta =0 to theta not=0 due to enlargement in the
ion path length, and Delta E is the average energy loss for such a beam-foil
experiment. The authors aim to show that the expression is an
oversimplification and therefore not correct.
Energy loss for electronically elastic atom-molecule
collisions in the keV energy range
Jakas-MM
Physical-Review-A-. vol.25, no.3; March 1982; p.1782-5
Abstract
An analytical expression is obtained for the average energy loss of atomic
projectiles scattered by homonuclear diatomic
molecules in the absence of electronic excitations.
Z/sub 1/ dependence of ion-induced electron emission
from aluminum
Alonso-EV; Baragiola-RA; Ferron-J; Jakas-MM; Oliva-Florio-A
Physical-Review-B-. vol.22, no.1; 1 July 1980; p.80-7
Abstract
The authors have measured the electron emission yields gamma of clean aluminum
under bombardment with H+, H2+, D+, D2+, He+, B+, C+, N+, N2+, O+, O2+, F+, Ne+, S+, Cl+, Ar+,
Kr+, and Xe+ in the energy range 1.2-50 keV. The clean surfaces were prepared by in situ
evaporation of high-purity Al under ultra-high-vacuum conditions. It is found
that kinetic electron emission yields gamma /sub k/, obtained after subtracting
from the measured gamma a contribution due to potential emission, are roughly
proportional to the electronic stopping powers, for projectiles lighter than
Al. For heavier projectiles there is a sizable contribution to electron
emission from collisions involving rapidly recoiling target atoms, which
increases with the mass of the projectile, and which dominates the threshold
and near-threshold behavior of kinetic emiss! ion. The results, together with recently reported data on
Auger electron emission from ion-bombarded Al show that the mechanism proposed
by Parilis and Kishinevskii
of inner-shell excitation and subsequent Auger decay is negligible for light
ions and probably small for heavy ions on Al and in the authors' energy range.
The authors thus conclude that kinetic electron emission under bombardment by
low-energy ions results mainly from the escape of excited valence electrons.
Energy reflection by back-scattering and sputtering:
total yields and angular distribution
Jakas-MM;
Williams-MMR
Journal-of-Physics-D-(Applied-Physics). vol.13, no.7; 14 July 1980;
p.1169-80
Abstract
The energy reflection coefficient-total yields and angular distributions-have
been calculated by solving the transport equation for the average kinetic
energy flux. The energy flux transported by projectiles and by recoils were
evaluated separately, thus the back-scattering and sputtering contributions to
the reflected energy were obtained. The authors considered an infinite medium
of stopping material and neglected the electronic energy loss as well as
crystalline effects. The introduction of a power scattering law leads to the
reduction of the integral equation for the energy flux to an algebraic system
of equations for the spatial moments. An analytical treatment to evaluate the
energy flux carried by the projectiles is also included. Good agreement was
found between the authors theory and experiment, in
particular with recently reported angular distributions of the reflected
energy. A special aspect of this work lies in the use of a synthetic kernel to
rep! resent the anisotropy of scattering in the
laboratory system of co-ordinates.
Explanation for the 180 degrees
Jakas-MM; Baragiola-RA
Physical-Review-Letters. vol.44, no.6; 11 Feb. 1980; p.424-6
Abstract
An explanation is given for the unusual enhancement in the
Energy dependence of the molecular effect in sputtering
Oliva-Florio-AR; Alonso-EV; Baragiola-RA; Ferron-J; Jakas-MM
Radiation-Effects-Letters. vol.50, no.1; 1979; p.3-7
Abstract
Reports measurements of sputtering yields of Au for Xe/sup
+/ and Xe/sub 2//sup +/ impact in the energy range
1-50 keV. It was found that non-linear effects exist
well outside the range predicted in a recent thermal spike model (Sigmund,
1974).
Fluctuation in the spatial
distribution of energy deposited by atomic particles.
Jakas-MM.
Physics-Letters-A. vol.72A, no.6; 6
Aug. 1979; p.423-6.
Abstract
The standard deviation distribution corresponding to the spatial distribution
of energy deposited in the slowing down of atomic particles in solids is
calculated. Large fluctuations are found that agree well with