Michael Haftel - Academia.edu (original) (raw)
Papers by Michael Haftel
Few Body Dynamics, 1976
Publisher Summary This chapter reviews the N–P Final State Interaction (FSI) angular distribution... more Publisher Summary This chapter reviews the N–P Final State Interaction (FSI) angular distribution in deuteron breakup at 45 MeV. An experiment described in the chapter was performed to provide an FSI angular distribution at energy higher than previously available. The experiment was performed with the NRL Sector Focusing Cyclotron using standard coincidence electronics for kinematically complete experiments. The chapter presents a comparison of the data with the results of calculations using several S-wave separable potentials tailored to test for sensitivity to off-shell and on-shell effects. These potentials have been described previously. The potentials have two different form factors A and B: A has off-shell behavior similar to that of the Reid soft core potential while B has off-shell behavior resembling the softer Yamaguchi. The potentials fit two different sets of phase shifts: set 1 corresponds nearly to experimental p–p 90° cross sections and set 2 corresponds to cross sections less than the p–p experimental values at energies above 10 MeV. The results, when put in the context of previous experiments and calculations, emphasize that there are still some basic factors not being considered in deuteron breakup calculations.
Experimental and theoretical cross sections are presented for the â¶Li(³He,³He³He)³H and â¶... more Experimental and theoretical cross sections are presented for the â¶Li(³He,³He³He)³H and â¶Li(³He,t³He)³He reactions for the symmetric angle pairs 20°â»Â²Â°sup 0/, 28.3°-28.3°, and 35°â»Â³âµsup 0/. The theoretical cross sections are calculated in a three-body model where the trions (i.e., mass-3 nuclei) are treated as elementary particles with â¶Li being a ³He-³H bound state. The trion-trion interaction is represented by S wave
Lecture Notes in Physics
Without Abstract
Physical Review Letters, 1975
Physical Review C, 1972
The pp cross sections relevant to a factorized-impulse-approximation treatment of (p, 2p) reactio... more The pp cross sections relevant to a factorized-impulse-approximation treatment of (p, 2p) reactions from 150to 350 MeV are calculated. Several on-shell prescriptions are used and compared with the half-off-shell prescription suggestedby the Faddeev-Watson multiplescattering series. Four phenomenological potentials, Hamada-Johnston, Bryan-Scott III, Reid hard core, and Reid soft core, are investigated as well as three potentials which are phase-shift equivalent to the Reid soft-core potential. We find significant differences ...
Physical Review C, 1977
Experimental and theoretical cross sections are presented for the 6Li(3He, 3He3He)3H and 6Li(3He,... more Experimental and theoretical cross sections are presented for the 6Li(3He, 3He3He)3H and 6Li(3He,t3He)3He reactions for the symmetric angle pairs 20°-20°, 28.3°-28.3°, and 35°-35°. The theoretical cross sections are calculated in a three-body model where the trions (i.e., mass-3 nuclei) are treated as elementary particles with 6Li being a 3He-3H bound state. The trion-trion interaction is represented by S wave separable
Nuclear Physics A, 1972
We calculate the binding energy of 16O for a set of phase-shift-equivalent potentials previously ... more We calculate the binding energy of 16O for a set of phase-shift-equivalent potentials previously studied in nuclear matter. Off-shell variations of up to 2.8 MeV per particle occur compared with about a 10 MeV per particle variation in nuclear matter. As in nuclear matter calculations a nearly linear relation exists between the variations in the binding-energy results and the wound integral k. We compare the 16O results with a nuclear matter calculation at the ``equivalent'' nuclear matter density of kF = 1.13 fm-1. This ``equivalent'' density reflects the fact that 16O has a surface and hence a lower average density than nuclear matter. The 16O and nuclear matter off-shell variations are comparable once one takes into account the lower average density of 16O and the suppression of the relative D-wave interaction - also a surface effect. We present a method of computing the correlated wave functions of finite nuclear systems and display such wave functions for 16O. The correlated wave functions of 16O and of nuclear matter are strikingly similar for all of the potentials studied. Supported in part by the Atomic Energy Commission under Contract AT(30-1) 2098.
Nuclear Physics A, 1976
This paper presents and analyses the data for the 2H(p, pp)n reaction at Einc = 44.9 MeV. Kinemat... more This paper presents and analyses the data for the 2H(p, pp)n reaction at Einc = 44.9 MeV. Kinematic conditions including the quasi-free scattering region and the regions far from quasi-two-body processes are considered. The experimental results are compared with the predictions of several separable S-wave models of the N-N interaction. Potential models that differ only off-shell, as well as models
The Journal of Chemical Physics, 1982
Elastic and dissociative scattering of He on He2 are studied for an incident laboratory energy of... more Elastic and dissociative scattering of He on He2 are studied for an incident laboratory energy of 1 K. We apply Faddeev-AGS multiple-scattering theory in momentum space to the analysis. We show that this leads to a simple justification for the importance of the ‘‘complex-formation mechanism’’ in termolecular recombination, the time reverse of collision-induced dissociation. Our work, in which separable expansions of two phenomenological He–He potentials are used, predicts significant magnitude differences in the cross sections derived from the interactions and also verifies the validity of the ‘‘peaking approximation’’ for hyperthermal-energy elastic collisions.
The Journal of Chemical Physics, 1986
This paper examines the role of vibrational (and rotational) excitations in collision-induced dis... more This paper examines the role of vibrational (and rotational) excitations in collision-induced dissociation in atom–diatom reactions. We treat a model system of identical, bosonic hydrogen atoms and investigate the total H+H2→H+H+H cross section as functions of total center-of-mass (c.m.) energy and vibrational–rotational quantum numbers v, j. The investigations are based on Faddeev–AGS theory and both three-dimensional (3D) and collinear (one-dimensional, 1D) geometries are considered. We derive both low- and high-energy relations between the total dissociation cross section, c.m. energy, and the vibrational–rotational wave functions, employing the single-scattering approximation of Faddeev theory. We apply these relations to the spectrum of the Kolos–Wolniewicz potential, both in three dimensions and one dimension. For collisions with a fixed total c.m. energy, our investigations predict considerable vibrational enhancement of the total cross section in the low-energy limit, with t...
Chemical Physics Letters, 1981
ABSTRACT Exact Faddeev theory and microscopic reversibility are applied to the description of ter... more ABSTRACT Exact Faddeev theory and microscopic reversibility are applied to the description of termolecular recombination in a model system of three helium-like atoms. Our results indicate that experimentally determined values of k3(T) can be reproduced.
Chemical Physics Letters, 1982
Please see Document Availability for additional information on obtaining the full-text document. ... more Please see Document Availability for additional information on obtaining the full-text document. Library patrons may search WorldCat to identify libraries that may hold this item. Keep in mind that many technical reports are not cataloged in WorldCat. ... Select a citation type above to copy/paste or download the reference. ... Some links on this page may take you to non-federal websites. Their policies may differ from this site.
Physical Review C, 1980
Electron-deuteron scattering observables, including the tensor polarizations T,o, T,+"T,+"are cal... more Electron-deuteron scattering observables, including the tensor polarizations T,o, T,+"T,+"are calculated for a variety of S-N potential models. The main goal is to determine how the tensor polarization experiments can help distinguish competing potential models with respect to off-shell behavior and tensor force strength. The pair meson-exchange-current correction of Gari and Hyuga is included in the analysis as well as a correction suggested by Friar for energy-dependent potentials. It is found that whereas electrondeuteron elastic scattering cross sections do not readily distinguish different potentials, the tensor polarizations do. The tensor polarization T,o mainly distinguishes potentials with different deuteron s-wave momentum distributions, but does not distinguish potentials with different d-state probabilities (PD). The tensor polarization T,+"since it factors essentially into a product of the magnetic and quadrupole form factors, allows for the extraction of the quadrupole form factor which is closely related to the tensor force strength and PD. The tensor polarization T, +, is completely determined by the elastic scattering cross sections and magnetic form factor, and yields no additional information on the N-lV force unobtainable from elastic scattering measurements. The tensor polarizations T,o and T» have maximum values of order unity in the region q = 2 to 5 fm '; The calculations indicate that measurements of T,o for 2&q & 5 fm and T, +, for 3&q &5 fm ' could yield important information on the off-shell behavior and tensor force strength. The meson-exchange-current and energy-dependence corrections are important and must be taken into account to extract potential properties from such experiments. NUCLEAR STHUCTURK H: form factors, tensor polarization calculated: dependence on of'f-shell behavior and &z, seven potential models; pair currents included.
An efficient method of solving the three-body Schroedinger equation is presented. The wave functi... more An efficient method of solving the three-body Schroedinger equation is presented. The wave function is decomposed into the product of a correlation factor describing the singularity and clustering structure, and a smooth factor expanded in hyperspherical harmonics. The application to the Helium atom yields a ground state energy of 2.9037244 (2.9033052) au for infinite (finite) nuclear mass. The convergence pattern shows that the accuracy of these values is better than a few parts in 14/1
Few Body Dynamics, 1976
Publisher Summary This chapter reviews the N–P Final State Interaction (FSI) angular distribution... more Publisher Summary This chapter reviews the N–P Final State Interaction (FSI) angular distribution in deuteron breakup at 45 MeV. An experiment described in the chapter was performed to provide an FSI angular distribution at energy higher than previously available. The experiment was performed with the NRL Sector Focusing Cyclotron using standard coincidence electronics for kinematically complete experiments. The chapter presents a comparison of the data with the results of calculations using several S-wave separable potentials tailored to test for sensitivity to off-shell and on-shell effects. These potentials have been described previously. The potentials have two different form factors A and B: A has off-shell behavior similar to that of the Reid soft core potential while B has off-shell behavior resembling the softer Yamaguchi. The potentials fit two different sets of phase shifts: set 1 corresponds nearly to experimental p–p 90° cross sections and set 2 corresponds to cross sections less than the p–p experimental values at energies above 10 MeV. The results, when put in the context of previous experiments and calculations, emphasize that there are still some basic factors not being considered in deuteron breakup calculations.
Experimental and theoretical cross sections are presented for the â¶Li(³He,³He³He)³H and â¶... more Experimental and theoretical cross sections are presented for the â¶Li(³He,³He³He)³H and â¶Li(³He,t³He)³He reactions for the symmetric angle pairs 20°â»Â²Â°sup 0/, 28.3°-28.3°, and 35°â»Â³âµsup 0/. The theoretical cross sections are calculated in a three-body model where the trions (i.e., mass-3 nuclei) are treated as elementary particles with â¶Li being a ³He-³H bound state. The trion-trion interaction is represented by S wave
Lecture Notes in Physics
Without Abstract
Physical Review Letters, 1975
Physical Review C, 1972
The pp cross sections relevant to a factorized-impulse-approximation treatment of (p, 2p) reactio... more The pp cross sections relevant to a factorized-impulse-approximation treatment of (p, 2p) reactions from 150to 350 MeV are calculated. Several on-shell prescriptions are used and compared with the half-off-shell prescription suggestedby the Faddeev-Watson multiplescattering series. Four phenomenological potentials, Hamada-Johnston, Bryan-Scott III, Reid hard core, and Reid soft core, are investigated as well as three potentials which are phase-shift equivalent to the Reid soft-core potential. We find significant differences ...
Physical Review C, 1977
Experimental and theoretical cross sections are presented for the 6Li(3He, 3He3He)3H and 6Li(3He,... more Experimental and theoretical cross sections are presented for the 6Li(3He, 3He3He)3H and 6Li(3He,t3He)3He reactions for the symmetric angle pairs 20°-20°, 28.3°-28.3°, and 35°-35°. The theoretical cross sections are calculated in a three-body model where the trions (i.e., mass-3 nuclei) are treated as elementary particles with 6Li being a 3He-3H bound state. The trion-trion interaction is represented by S wave separable
Nuclear Physics A, 1972
We calculate the binding energy of 16O for a set of phase-shift-equivalent potentials previously ... more We calculate the binding energy of 16O for a set of phase-shift-equivalent potentials previously studied in nuclear matter. Off-shell variations of up to 2.8 MeV per particle occur compared with about a 10 MeV per particle variation in nuclear matter. As in nuclear matter calculations a nearly linear relation exists between the variations in the binding-energy results and the wound integral k. We compare the 16O results with a nuclear matter calculation at the ``equivalent'' nuclear matter density of kF = 1.13 fm-1. This ``equivalent'' density reflects the fact that 16O has a surface and hence a lower average density than nuclear matter. The 16O and nuclear matter off-shell variations are comparable once one takes into account the lower average density of 16O and the suppression of the relative D-wave interaction - also a surface effect. We present a method of computing the correlated wave functions of finite nuclear systems and display such wave functions for 16O. The correlated wave functions of 16O and of nuclear matter are strikingly similar for all of the potentials studied. Supported in part by the Atomic Energy Commission under Contract AT(30-1) 2098.
Nuclear Physics A, 1976
This paper presents and analyses the data for the 2H(p, pp)n reaction at Einc = 44.9 MeV. Kinemat... more This paper presents and analyses the data for the 2H(p, pp)n reaction at Einc = 44.9 MeV. Kinematic conditions including the quasi-free scattering region and the regions far from quasi-two-body processes are considered. The experimental results are compared with the predictions of several separable S-wave models of the N-N interaction. Potential models that differ only off-shell, as well as models
The Journal of Chemical Physics, 1982
Elastic and dissociative scattering of He on He2 are studied for an incident laboratory energy of... more Elastic and dissociative scattering of He on He2 are studied for an incident laboratory energy of 1 K. We apply Faddeev-AGS multiple-scattering theory in momentum space to the analysis. We show that this leads to a simple justification for the importance of the ‘‘complex-formation mechanism’’ in termolecular recombination, the time reverse of collision-induced dissociation. Our work, in which separable expansions of two phenomenological He–He potentials are used, predicts significant magnitude differences in the cross sections derived from the interactions and also verifies the validity of the ‘‘peaking approximation’’ for hyperthermal-energy elastic collisions.
The Journal of Chemical Physics, 1986
This paper examines the role of vibrational (and rotational) excitations in collision-induced dis... more This paper examines the role of vibrational (and rotational) excitations in collision-induced dissociation in atom–diatom reactions. We treat a model system of identical, bosonic hydrogen atoms and investigate the total H+H2→H+H+H cross section as functions of total center-of-mass (c.m.) energy and vibrational–rotational quantum numbers v, j. The investigations are based on Faddeev–AGS theory and both three-dimensional (3D) and collinear (one-dimensional, 1D) geometries are considered. We derive both low- and high-energy relations between the total dissociation cross section, c.m. energy, and the vibrational–rotational wave functions, employing the single-scattering approximation of Faddeev theory. We apply these relations to the spectrum of the Kolos–Wolniewicz potential, both in three dimensions and one dimension. For collisions with a fixed total c.m. energy, our investigations predict considerable vibrational enhancement of the total cross section in the low-energy limit, with t...
Chemical Physics Letters, 1981
ABSTRACT Exact Faddeev theory and microscopic reversibility are applied to the description of ter... more ABSTRACT Exact Faddeev theory and microscopic reversibility are applied to the description of termolecular recombination in a model system of three helium-like atoms. Our results indicate that experimentally determined values of k3(T) can be reproduced.
Chemical Physics Letters, 1982
Please see Document Availability for additional information on obtaining the full-text document. ... more Please see Document Availability for additional information on obtaining the full-text document. Library patrons may search WorldCat to identify libraries that may hold this item. Keep in mind that many technical reports are not cataloged in WorldCat. ... Select a citation type above to copy/paste or download the reference. ... Some links on this page may take you to non-federal websites. Their policies may differ from this site.
Physical Review C, 1980
Electron-deuteron scattering observables, including the tensor polarizations T,o, T,+"T,+"are cal... more Electron-deuteron scattering observables, including the tensor polarizations T,o, T,+"T,+"are calculated for a variety of S-N potential models. The main goal is to determine how the tensor polarization experiments can help distinguish competing potential models with respect to off-shell behavior and tensor force strength. The pair meson-exchange-current correction of Gari and Hyuga is included in the analysis as well as a correction suggested by Friar for energy-dependent potentials. It is found that whereas electrondeuteron elastic scattering cross sections do not readily distinguish different potentials, the tensor polarizations do. The tensor polarization T,o mainly distinguishes potentials with different deuteron s-wave momentum distributions, but does not distinguish potentials with different d-state probabilities (PD). The tensor polarization T,+"since it factors essentially into a product of the magnetic and quadrupole form factors, allows for the extraction of the quadrupole form factor which is closely related to the tensor force strength and PD. The tensor polarization T, +, is completely determined by the elastic scattering cross sections and magnetic form factor, and yields no additional information on the N-lV force unobtainable from elastic scattering measurements. The tensor polarizations T,o and T» have maximum values of order unity in the region q = 2 to 5 fm '; The calculations indicate that measurements of T,o for 2&q & 5 fm and T, +, for 3&q &5 fm ' could yield important information on the off-shell behavior and tensor force strength. The meson-exchange-current and energy-dependence corrections are important and must be taken into account to extract potential properties from such experiments. NUCLEAR STHUCTURK H: form factors, tensor polarization calculated: dependence on of'f-shell behavior and &z, seven potential models; pair currents included.
An efficient method of solving the three-body Schroedinger equation is presented. The wave functi... more An efficient method of solving the three-body Schroedinger equation is presented. The wave function is decomposed into the product of a correlation factor describing the singularity and clustering structure, and a smooth factor expanded in hyperspherical harmonics. The application to the Helium atom yields a ground state energy of 2.9037244 (2.9033052) au for infinite (finite) nuclear mass. The convergence pattern shows that the accuracy of these values is better than a few parts in 14/1