- Quantum-Trajectory calculations of
proton-hydrogen model collisions M.
Acuña, J. Fiol Nucl. Instrum. Methods
B En prensa2008
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Abstract
We investigate a
proton-hydrogen model collision using a method based on the de
Broglie-Bohm formulation of Quantum Dynamics. By studying the
quantum trajectories of the particles we obtain approximate
ionization and capture cross sections that are in good agreement
with the exact values. In particular, the implementation of this
high-order approximation method allows us to solve each
\emphtrajectory independently. The method has a relatively low
computational cost and can be straightforwardly parallelized for
many bodies systems.
- Dynamics of collisions with
positrons J. Fiol, R. O. Barrachina,
P. Macri Nucl. Instrum. Methods
B En prensa2008
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Abstract
The measurement of ionization
by positron impact reveals that the maximum of the electron capture
to the continuum cusp is shifted from its theoretical position. In
this work the hypothesis that the observed effect is the result of
an anisotropic momentum distribution in the projectile-electron
reference system is considered. By elaborating on the ansatz that
the cusp asymmetry is qualitatively similar for positron impact
than the for for ion-atom collisions, we obtain fully differential
cross sections that show the same features than those
experimentally observed. The present estimation for the position of
the maximum agrees well with cross section measurements performed
in coincident electron-positron detection experiments.
- Threshold effects in the ionization of
atoms by positron impact R. O.
Barrachina, J. Fiol, P. Macri Nuclear
Instruments and Methods in Physics Research B 266 402-4062008
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Abstract
We employ different
theoretical models, both classical and quantum-mechanical, to
explore the recoil-ion momentum distribution in positron-atom
collisions. We pay special attention to the vicinity of the
kinematical threshold between ionization and positronium formation.
We demonstrate that it is intertwined by dynamical constraints to
the formation of highly excited and low-lying continuum
electron-positron states. Finally we discuss how the study of
recoil-ion momentum distribution, which is characteristic of a
reaction microscopy technique, might represent an alternative
approach to the standard spectroscopy of electrons and
positrons.
- Momentum-transfer dependence of ionization
cross sections for C6++He collisions J. Fiol, S. Otranto, R. E. Olson Journal of Physics: Conference Series 58 161-1642007
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Abstract
In this work we study the
dependence of the fully differential cross sections (FDCS) for
single ionization of He by 100 MeV/amu C6+ on the
momentum transferred by the projectile to the target. Three
dimensional plots of the FDCS are used to illustrate how the
different configurations contribute when the theoretical results
are convoluted over the experimental uncertainties. This
convolution is shown to be essential in order to properly reproduce
the measured data.
- Fully differential ionization cross
sections in fast ion-atom collisions J. Fiol, S. Otranto, R. E. Olson Journal of Physics: Conference Series 88 012014 (8pp)2007
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Abstract
Fully differential cross
sections for helium ionization by fast ion collisions are analyzed.
The emitted-electron angular distributions for fixed momentum
transfer and electron energies are described theoretically and
compared to the experiment. The effect of uncertainties in the
determination of the momentum is considered within the theoretical
model. The cross sections are found to be extremely sensitive to
the inclusion of the uncertainties. Important quantitative and
qualitative modifications of the calculated cross sections are
obtained by including small uncertainties in the determination of
the momentum transferred by the projectile to the target.
- Critical comparison between theory and
experiment for C6+He fully differential ionization cross
sections J. Fiol, S. Otranto, R. E.
Olson J. Phys. B: At. Mol.
Phys. 39 L285-L2902006
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Abstract
Fully-differential cross
sections for single ionization of helium induced by impact of
100 \mathrmMeV\mathrmu-1 \mathrmC6+ ions
are examined within a quantum-mechanical distorted wave model. The
experimental uncertainties are included in the theoretical
calculations, leading to a quantitative description of the
experimental cross sections. In particular, the ionization cross
section for the electron emitted in the plane perpendicular to the
scattering plane is reproduced for the first time by a full
quantum-mechanical model. The role of the internuclear interaction
in this perturbative-regime collision is discussed and found to be
unimportant for the present kinematical conditions.
- Angular distributions and Dalitz plots for
C6+ ionization of He S.
Otranto, R. E. Olson, J. Fiol J. Phys.
B: At. Mol. Phys. 39
7 L175-L1832006
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Abstract
Single ionization fully
differential cross sections for 2 MeV/amu C6+ + He
collisions are obtained and analysed using the classical trajectory
Monte Carlo and continuum distorted wave models. The present
theoretical results are compared with the recent experimental data
of Fischer et al . The published experimental conditions are
considered in both theoretical models. The inclusion of the
momentum distribution of the target atom leads to an improved
description of the forward electron emission. Dalitz plots for
single ionization fully differential cross sections in ion–atom
collisions are presented and are used to help elucidate the
collision dynamics.
- Theory of ionization processes in
positron-atom collisions R. Della
Picca, J. Fiol, R. O. Barrachina, V. D. Rodríguez
Nucl. Instrum. Methods B 247 52-572006
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Abstract
We review past and present
theoretical developments in the description of ionization processes
in positron-atom collisions. Starting from an analysis that
incorporates all the interactions in the final state on an equal
footing and keeps an exact account of the few-body kinematics, we
perform a critical comparison of different approximations, and how
they affect the evaluation of the ionization cross section.
Finally, we describe the appearance of fingerprints of capture to
the continuum, saddle-point and other kinematical mechanisms.
- Investigation of saddle point electrons in
positron-atom ionization collisions R.
Della Picca, J. Fiol, R. O. Barrachina Nuclear Instruments and Methods in Physics Research
B 233 270-2752005
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Abstract
We investigate the
appearance of fingerprints of saddle-point electrons in the
ionization of atoms and molecules by positron impact. We calculate
the quintuple differential cross section by means of a continuum
distorted wave approxi- mation that employs the correct kinematics.
We find a clear structure located at precisely the energy and
emission angle where a saddle-point electron is supposed to appear.
Unmistakable signatures of this structure can also been pinpointed
in the projectile dispersion and the recoiling of the target
ion.
- Extreme Sensitivity of Differential
Momentum Transfer Cross Sections to Target Atom Initial
Conditions R. E. Olson, J. Fiol
Phys. Rev. Lett. 95 26
2632032005
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Abstract
Heavy-particle cross sections
differential in the momentum transferred to the target are
investigated using the classical trajectory Monte Carlo method.
With the 3.6 MeV/u Au53++He system as a test case, it is
shown that these cross sections are extremely sensitive to the
initial target temperature. In particular, when thermal motion is
varied for one of the target's initial momentum components between
0 and 25 K the absolute cross sections vary by orders of magnitude
and, in addition, their relative shapes undergo major changes. We
find that by setting one of the target's transverse momenta to a
temperature of 16 K, previously reported major discrepancies
between theory and experiment are removed.
- Dynamics of collisions revealed by
classical methods R. E. Olson, J.
Fiol, J. Perez, P. Beiersdorfer Nuclear Instruments and Methods in Physics Research
B 233 12-182005
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Abstract
Single ionization of helium
by impact of 3.6 MeV/u Au53+ ions is investigated by means of
quantum and classical methods. Calculation of fully differential
cross sections are compared to recently published data for
ionization of low-energy electrons as a function of the momentum
transferred by the projectile to the target system. The results
show that inclusion of the resolution and uncertainties present in
the experiment has a major influence on both the shape and
magnitude of the calculated cross sections. The effect of using a
two-electron model for the He target along with including
electron-electron correlation are also investigated. However, after
incorporating all the experimental conditions within the
calculations, the one- and two-electron results present similar
behavior.
- Three-body dynamics in fast heavy ion-atom
ionization collisions J. Fiol, R. E.
Olson J. Phys. B: At. Mol.
Phys. 37 3947-39602004
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Abstract
Single ionization of helium by
impact of 3.6 MeV u-1 Au53+ ions is
investigated by means of quantum mechanical and classical methods.
Calculations of fully-differential cross sections are compared with
recently published data for ionization of low-energy electrons as a
function of the momentum transferred by the projectile to the
target system. A description of initial and final states of the He
atom in terms of a Hartree-Fock potential provides an improvement
over previous hydrogen-like models. The present results show that
inclusion of the resolution and uncertainties present in the
experiment has a major influence on both the shape and magnitude of
the cross sections. The effect of four-bodies and electron-electron
correlation are also investigated. However, after including the
experimental conditions into the calculations, the three- and
four-body results present similar behavior.
- Dynamical electron-electron correlation in
C2++He simultaneous target-projectile collisional
ionization J. Fiol, R. E. Olson, R.
Moshammer, J. Ullrich J. Phys. B: At.
Mol. Phys. 36
L99-L1052003
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Abstract
Simultaneous target and
projectile single ionization in 3.6 MeV u-1
C2+ + He collisions is considered, within a six-body
classical trajectory Monte Carlo model. Analysis of the relative
azimuthal angle between the two emitted electrons allows one to
discriminate the ionization contribution produced by the two-centre
dynamical electron-electron interaction from that due to
nucleus-electron interactions. The present calculations agree well
with cross section measurements recently performed in kinematically
complete experiments.
- Dynamics underlying fully differential
cross sections for fast C6++He collisions
R. E. Olson, J. Fiol J. Phys. B: At. Mol. Phys. 36 20
L365-L3732003
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Abstract
Single ionization of helium
by impact of 100 MeV u-1 C6+
ions is investigated using the three-body classical trajectory
Monte Carlo method. Fully differential cross section calculations
are compared to recently published data for ionized electrons
emitted both in the scattering plane, and in the plane
perpendicular to it that contains the initial velocity. The present
calculations show good agreement with the experimental data, and
improve upon continuum-distorted-wave results. The collision
mechanisms that lead to the different structures observed in the
fully differential cross sections are investigated and include
those of the binary and recoil peaks for in-plane collisions as
well as the maxima observed in the out-of-plane scattering.
- Correlation in fast collisions of highly
charged ions with atoms J. Fiol, R. E.
Olson Nucl. Instrum. Methods B
205 474-4782003
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Abstract
Atomic hydrogen and helium
ionization by impact of 3.6 MeV/u Au53+ is
investigated within Classical Trajectory Monte Carlo and
quantum-mechanical CDW-B1 and CDW-EIS models. For helium
ionization, a description of initial and final electron states in
terms of Hartree-Fock potentials is compared with hydrogenic
models. Different ionization mechanisms are characterized. A strong
correlation of the electron, projectile and target nucleus is
observed. Good agreement is obtained between calculations performed
with the different models.
- Characteristic low-energy electrons emitted
in proton-atom collisions at intermediate impact velocities
J. Fiol, S. Suárez, D. Fregenal, A. D.
González, P. D. Fainstein Phys. Rev.
A 67 050702(R)2003
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Abstract
We report experimental and
theoretical electron spectra within the very low-electron-energy
range below 30 eV. Doubly differential cross sections for
ionization of different noble gases (He, Ne, Ar, Kr, Xe) by impact
of 100-keV and 225-keV protons are reported. A pronounced structure
in the low-energy region of emittedelectron spectra is observed
with different intensities for the different targets. We compare
our experimental findings with two theoretical models: the
first-order Born approximation and the “continuum-distorted-wave–
eikonal-initial-state” model using different optimized central
potentials to calculate the bound and continuum states of the
target. We attribute our experimental observation to a signature of
the predicted low-energy binary peak.
- Dynamics of secondary ion emission: Novel
energy and angular spectrometry T.
Jalowy, R. Neugebauer, M. Hattass, J. Fiol, F. Afaneh, J. A. M.
Pereira, V. Collado, E. F. da Silveira, H. Schmidt-Böcking, K. O.
Groeneveld Nucl. Instrum. Methods
B 193 762-7672002
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Abstract
A new spectrometer has been
developed based on the combination of standard time-of-flight
technique and position sensitive delay line detectors. The basic
features of the spectrometer, particularly of the multi-hit capable
detector, are described. To demonstrate the performance of this new
system, the dynamic emission characteristics, i.e. the three-
dimensional velocity distribution, of desorbed Hþ from Al target by
Ar0 impact (570 keV) is presented. It is found that the desorption
yield is maximum for radial and axial emission velocities at 1.2
and 12 km/s respectively, corresponding to 1.5 eV ions emitted at
57\circ to normal (following the projectile radial
direction). The initial energy distribution spreads out over 16
eV.
- Three-body dynamics in hydrogen ionization
by fast highly charged particles J.
Fiol, R. E. Olson J. Phys. B: At. Mol.
Phys. 35 7 1759-17732002
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Abstract
Electron double and triple
differential cross sections are calculated as a function of
projectile momentum transfer for ionization of ground and excited
state hydrogen by 3.6 MeV u -1 C.
6+ and Au 53+ ions. These three-body Coulomb
systems are investigated using the classical-trajectory Monte Carlo
and continuum distorted wave methods that incorporate all
interactions including the nuclear-nuclear potential. The
calculations allow one to distinguish cross section features
associated with three collision mechanisms. The first is due to
distance collisions that lead primarily to a binary interaction
between the projectile and electron. The second is a strong
three-body interaction by the projectile with both the electron and
the target ion when the projectile passes between the electron and
its parent nucleus. These two mechanisms result in binary peak
electrons located near the momentum transfer vector Q. with active
participation by the recoil ion along - Q. in order to determine
the overall momentum transfer magnitude. The third mechanism, which
is present only for fast highly charged ion impact, yields electron
spectra that here-to-fore have not been observed. Rather than the
electrons being scattered near the angle θ associated with the
momentum transfer vector Q. , they are found at an angle of
360^\circ-\theta . Such electrons are due to a close collision of
the projectile with the target nucleus with the electron being
forced to swing by its parent. These electrons are not so-called
recoil electrons associated with the angle 180^\circ+ \theta .
Moreover, in this case neither the recoil ion nor the electron
spectra peak near Q. . Calculations are also presented for
collisions with excited hydrogen in order to assess the collision
dynamics as a function of the radial dimensions of the target
atom.
- Cusp formation in the single-particle
momentum distributions of three-body continuum states
J. Fiol, R. O. Barrachina, V. D.
Rodríguez J. Phys. B: At. Mol.
Phys. 35 1 149-1642002
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Abstract
We investigate the appearance
of cusp structures in single-particle momentum distributions for
processes leading to three-body continuum states. We discuss under
which circumstances these structures are produced, and identify
some of their properties by means of a final-state interaction
theory. Finally, we show how they change with the relative mass
ratios of the three particles in the final state.
- Nuclear-electron versus nuclear-nuclear
interactions in ionization of atoms by highly charged ions
impact J. Fiol, R. E. Olson
Application of Accelerators in Research and
Industry Int. Conf. 680
138-1422002
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- Three-body dynamics in the ionization of
hydrogen by positron impact J. Fiol,
R. E. Olson J. Phys. B: At. Mol.
Phys. 35 5 1173-11842002
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Abstract
Three-body dynamics are
investigated for single ionization of hydrogen by 50
and 100 eV positron impact. The momentum distributions of
the electron, the projectile and the recoiling target nucleus are
investigated. The present results show that, despite the large mass
of the target nucleus, it actively participates in the dynamics of
the ionizing collisions. In particular, a strong correlation
between the positron and the recoil-ion momenta is found, which is
especially important at the lower collision energy of this
study.
- Mapping of the Bethe surface in
single-ionization ion-atom collisions R. E. Olson, J. Fiol J.
Phys. B: At. Mol. Phys. 34
19 L625-L6312001
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Abstract
The three-body Coulomb
problem is explored using classical-trajectory Monte Carlo and
continuum distorted-wave methods that include all interactions,
including the nuclear-nuclear term. Calculations for low-energy
electron emission as a function of projectile deflection, the Bethe
surface, are compared with experiment for single ionization of He
by 100 MeV u -1 C6+ and
3.6 MeV u -1 Au 53+ . Good
agreement is realized for the C6+ system. For Au
53+ poor agreement with experiment is obtained,
indicating that the proposed lack of the nuclear-nuclear
interaction is not the source of the discrepancy. The calculations
further show that significant cross sections at large projectile
deflections are only realized for double ionization, not single
ionization.
- Simultaneous Projectile and Target
Ionization in He+ + Ne Collisions J. Fiol, R. E. Olson, A. C. F. Santos, G. M. Sigaud, E.
C. Montenegro J. Phys. B: At. Mol.
Phys. 34 16 L503-L5092001
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Abstract
Cross sections for single and
multiple ionization of the target atom with simultaneous ionization
of the projectile have been measured for 1-4 MeV collisions of
He + with Ne. The observations are interpreted using the
n -body classical trajectory Monte Carlo method. The 11-body
calculations include the L-shell electrons of the Ne and the
K-shell electron on the He + . In this model, each
electron interacts with both nuclei and with all the electrons
belonging to the other centre. For single ionization from both
centres, it is found that the dynamical
electron-electron (e-e) interaction produces a clear signature
in the relative azimuthal angle distribution between the ionized
electrons. For low values of momentum transfer q , this interaction
is reflected in a pronounced enhancement near 180^\circ in the
azimuthal angle between electrons. Integral values of the azimuthal
angle events, summed over all q values, indicate that it is
possible to determine the relative importance of the e-e versus the
nuclear-electron (N-e) interactions.
- Electron capture to the continuum by proton
and positron impact J. Fiol, V. D.
Rodríguez, R. O. Barrachina J. Phys.
B: At. Mol. Phys. 34
5 933-9442001
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Abstract
We describe recent
experimental triple-differential cross sections of ionization by
the impact of both protons and positrons by means of a single,
kinematically exact theory. This model incorporates all the
interactions in the final state on an equal footing and keeps an
exact account of the three-body kinematics. We show that these
provisions make it possible to evaluate any multiple-differential
cross section for any given mass configuration, and analyse how it
changes with the relative masses of the three particles in the
final state. We analyse the differences in the electron cusp
formation by both heavy and light projectile impact at the
double-differential cross section level.
- Zero-energy resonances efects in break-up
collisions J. Fiol, C. Courbin, V. D.
Rodríguez, R. O. Barrachina Few-Body
Systems 13 46-552001
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Abstract
We show that the analysis of
cusp and threshold structures in breakup collisions of nuclei,
atoms and molecules represents an alternative approach for the
study of elastic two-particles collisions at extremely
low-energies. We illustrate these general ideas by showing that the
“electron capture to the continuum” cusp in the ionization of atoms
by neutral projectiles can be understood in terms of a resonance
mechanism. This approach allows for the extraction of the s-wave
scattering length for the electron-projectile interaction.
- Recent Experiments on the Roles of
Projectile Electrons in Ion-Atom Collisions D. Fregenal, J. Fiol, S. Suárez, G. Bernardi, P. Focke,
A. D. González Application of
Accelerators in Research and Industry - Sixteenth Int. Conf.
576 164-1672001
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- Minimum in the distribution of electrons
emitted from solids in the backward direction C. D. Denton, T. Jalowy, H. Luna, J. Fiol, D. Fregenal,
S. Suárez, G. Bernardi, A. González, N. R. Arista, K. O.
Groeneveld Nucl. Instrum. Methods
B 164 927-9322000
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Abstract
We have investigated the
electron emission from carbon and aluminum foils in the backward
direction induced by proton impact with energies in the range
50-250 keV. Doubly differential angular emission spectra were
obtained for several electron energies covering the angular range
extended from 160 degrees to 200 degrees, A minimum in the electron
angular distribution centred at 180 degrees was observed for slow
electrons and it disappears with increasing electron energies. We
have interpreted these results as a combination of three effects:
the excitation of single conduction electrons in the target, the
transmission of the excited electrons across the surface barrier
and the effect of the image force acting on the emitted electrons
when they are in the vacuum.
- Classical description of threshold effects
in ion-atom ionization collisions J.
Fiol, C. Courbin, V. D. Rodríguez, R. O. Barrachina
J. Phys. B: At. Mol. Phys.
33 23
5343-53552000
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Abstract
We employ a three-body
classical trajectory Monte Carlo (CTMC) method to calculate
the recoil-ion momentum distribution at its kinematic threshold in
ion-atom ionization collisions. We analyse how this threshold is
intertwined by dynamical constraints to the electron capture to the
continuum cusp in the electron double differential cross section.
We compare these calculations with those from a full
quantum-mechanical description and explore how these structures
depend on the interactions among the three particles in the final
state.
- Cusp formation and threshold effects in
break-up collisions R. O. Barrachina,
J. Fiol, V. D. Rodríguez, P. Macri The
Physics of Electronic and Atomic Collisions
510-5192000
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Abstract
We show how the
singe-particle double differential cross sections (DDCS) in breakup
collisions are intertwined by dynamical constraints. In particular,
we study the corresponding relations among threshold and cusp
structures and identify some of their properties by means of a
final-state interaction theory. We provide general expressions for
the cusp and threshold structures that any theoretical description
of the collision process has to fulfill. Finally, we show how these
structures change with the relative mass ratios of the tree
particles in the final state.
- A classical interpretation of the off-shell
Coulomb transition matrix J. Fiol, R.
O. Barrachina J. Phys. B: At. Mol.
Phys. 33 15 2847-28572000
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Abstract
We analyse the transition
matrix for the two-body Coulomb scattering problem out of the
energy shell. This quantity appears in high-order perturbation
treatments of multichannel processes and plays a central role in
the generalization of the scattering theory to include long-range
interactions. In particular, its branch-point singularities on the
initial and final half of the energy shell are known to produce
sizeable effects in multiple-scattering amplitudes for
rearrangement and ionization collisions. In this paper we present a
classical description of the off-shell collision process which
helps to clarify its essential concepts.
- Double capture with simultaneous ionization
in ion-atom collisions D. Fregenal, J.
Fiol, G. Bernardi, S. Suárez, P. Focke, A. D. González, A. Muthig,
T. Jalowy, H. Luna Phys. Rev. A
62 127032000
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Abstract
We have investigated double
electron capture with simultaneous target ionization in collisions
of 25-keV/amu 3He(2+) projectiles on argon.
Doubly differential cross sections for electrons emitted in angles
0 degrees, 20 degrees, 45 degrees, 90 degrees, 128 degrees, 175
degrees, in coincidence with the neutralized projectiles were
obtained. To establish the relative importance of the double
capture channel in the electron emission at the present
intermediate impact velocity, differential cross sections for total
electron emission were also measured. A narrow symmetric
cusp-shaped structure for electrons with velocity close to the ion
velocity, associated with the neutral emerging projectile, is
observed. Binary encounter electrons, masked by other processes in
total emission, are clearly observed for the double capture plus
ionization channel.
- Emisión electrónica en el continuo de un
átomo neutro utilizando proyectiles de H0 and
H+ on He and Ar M. Galassi,
J. Revelli, J. Fiol, G. Bernardi Anales de la Asociación Física Argentina
581998
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- An Alternative Classical Approach to the
quantum-mechanical definition of the Scattering Cross
Section J. Fiol, R. G. Pregliasco, I.
Samengo, R. O. Barrachina Am. J.
Phys. 65 433-4361997
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Abstract
We discuss an alternative
classical description of the nonrelativistic scattering process
that is completely analogous to the time-independent formalism
employed in quantum-mechanics textbooks, This approach provides an
elementary introduction to the standard stationary scattering
theory, embodying many of its essential concepts.
- Regularización del problema de dispersión
en presencia de potenciales de largo alcance J. Fiol, R. O. Barrachina Anales de la Asociación Física Argentina
4281997
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Abstract
Almost every process in atomic
collisions involves coulomb interactions either in the asymptotic
evolution of the system or in intermediate states in charge
exchange processes. However, this type of long range interactions
does not fit into the usual formal scattering theory, which
requires a free asymptotic evolution of the colliding fragments.
Many different methods have been proposed in order to circumvent
these difficulties and include long range interactions. One of them
consists in evaluating the on-energy-shell limit in a regularized
version of the off-energy-shell transition matrix. Using a
classical description, we show the close relation between this
method and another one suggested by Dettmann in 1971 which consists
in postponing the infinite time limit in a time-dependent
wave-packet formalism.
- Una perspectiva clásica de la función de
onda coulombiana del continuo I.
Samengo, R. G. Pregliasco, J. Fiol, R. O. Barrachina
Anales de la Asociación Física
Argentina 4221997
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Abstract
In this work we develop a
method to calculate the classical density of particles scattered by
a central force. using this technique we find an analytical
expression for the classical density in the scattering from a
Coulomb potential. We compare it with the quantum-mechanical
result. We conclude that both distributions have the same global
behavior. We show that, not only in the asymptotic region but in
every point of the space, the classical distributions can be
separated in incoming and outgoing components. Furthermore, the
densities for the attractive and repulsive case can be mapped into
each other. These results lead to an interpretation of the
different features of the quantum-mechanical densities in terms of
classical concepts.