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NSR database version of April 11, 2024.

Search: Author = E.Friedman

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2024GA06      Phys.Rev. C 109, 024001 (2024)

D.Gazda, A.Perez-Obiol, E.Friedman, A.Gal

Hypertriton lifetime

doi: 10.1103/PhysRevC.109.024001
Citations: PlumX Metrics


2023FR06      Nucl.Phys. A1039, 122725 (2023)

E.Friedman, A.Gal

Λ hypernuclear potentials beyond linear density dependence

doi: 10.1016/j.nuclphysa.2023.122725
Citations: PlumX Metrics


2022OB01      Phys.Rev. C 106, 065201 (2022)

J.Obertova, E.Friedman, J.Mares

First application of a microscopic K-NN absorption model in calculations of kaonic atoms

ATOMIC PHYSICS 12C, 31P, 32S, 35Cl, 63Cu, 118Sn, 208Pb; calculated shifts, widths for kaonic atoms, primary-interaction branching ratios for mesonic and nonmesonic absorption of K- in 12C+K- system. Calculations were performed using microscopic K-N+K-NN potentials based on scattering amplitudes derived from two chiral coupled-channels meson-baryon interaction models - the Barcelona and Prague models. Comparison to experimental data.

doi: 10.1103/PhysRevC.106.065201
Citations: PlumX Metrics


2021BA02      Nucl.Phys. A1006, 122112 (2021)

N.Barnea, E.Friedman, A.Gal

On the width of the K-D atom ground state

ATOMIC PHYSICS 2H; calculated g.s. widths for K-D atom. Comparison with available data.

doi: 10.1016/j.nuclphysa.2020.122112
Citations: PlumX Metrics


2021FR12      Phys.Lett. B 820, 136555 (2021)

E.Friedman, A.Gal

Constraints on Ξ- nuclear interactions from capture events in emulsion

doi: 10.1016/j.physletb.2021.136555
Citations: PlumX Metrics


2020PE16      Phys.Lett. B 811, 135916 (2020)

A.Perez-Obiol, D.Gazda, E.Friedman, A.Gal

Revisiting the hypertriton lifetime puzzle

RADIOACTIVITY 3H(β-); analyzed available data for conflicting values of the hypertriton lifetime; calculated T1/2, decay rate using three-body wavefunctions generated in a chiral effective field theory approach; deduced impact of ALICE and STAR lifetimes on separation energy.

doi: 10.1016/j.physletb.2020.135916
Citations: PlumX Metrics


2017BA44      Nucl.Phys. A968, 35 (2017)

N.Barnea, E.Friedman, A.Gal

Onset of η-meson binding in the He isotopes

NUCLEAR STRUCTURE 2,3H, 3,4He; calculated η-meson binding energy, Q using few-body stochastic variational method calculations with ηN potentials derived from coupled-channel models of the N*(1535) resonance and different NN central potentials. Compared with results of ηNNN and ηNNNN pionless effective field theory.

doi: 10.1016/j.nuclphysa.2017.07.021
Citations: PlumX Metrics


2017FR01      Nucl.Phys. A959, 66 (2017)

E.Friedman, A.Gal

K-N amplitudes below threshold constrained by multinucleon absorption

doi: 10.1016/j.nuclphysa.2016.12.009
Citations: PlumX Metrics


2017GA27      Acta Phys.Pol. B48, 1781 (2017)

A.Gal, N.Barnea, B.Bazak, E.Friedman

Onset of η-Nuclear Binding

NUCLEAR STRUCTURE 3,4He; calculated η-nuclear binding, Q of η-hypernuclei using energy-dependent η-nucleon potential.

doi: 10.5506/APhysPolB.48.1781
Citations: PlumX Metrics


2016FR05      Nucl.Phys. A954, 114 (2016)

E.Friedman

K+-nucleus potentials from K+-nucleon amplitudes

NUCLEAR REACTIONS 2H, 6Li(K+, x), E at 488, 531, 656, 714 MeV/c; calculated total σ; compared 3 times σ on 2H with σ on 6Li, ratio reaction to total σ, experimental to calculated σ. C, Si, Ca(K+, x), E not given; calculated experimental to calculated σ. C(K+, K+), E at 715 MeV/c; calculated σ(θ). Compared with data. Optical potentials for K+-nucleus interactions constructed from K+-nucleon ones, with and without Pauli correlations.

doi: 10.1016/j.nuclphysa.2016.02.053
Citations: PlumX Metrics


2015FR05      Nucl.Phys. A943, 101 (2015)

E.Friedman, A.Gal, B.Loiseau, S.Wycech

Antinucleon-nucleus interaction near threshold from the Paris N(bar)N potential

NUCLEAR REACTIONS 1H(n-bar, x), (p-bar, x), E at 50-390 MeV/c;Ca(p-bar, x), E at 70-390 MeV/c; calculated annihilation σ using Paris 2009 potential. 40Ca(p-bar, x), E=47.8 MeV; calculated σ(θ) using Paris 2009 and empirical potentials compared with data.

doi: 10.1016/j.nuclphysa.2015.08.010
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2014CI05      Nucl.Phys. A925, 126 (2014)

A.Cieply, E.Friedman, A.Gal, J.Mares

In-medium ηN interactions and η nuclear bound states

NUCLEAR STRUCTURE C, Mg, Ca, Zr, Pb; calculated binding energy, mass excess of η bound nuclear states using meson-baryon coupled channel model with N*(1535) baryon resonance.

doi: 10.1016/j.nuclphysa.2014.02.007
Citations: PlumX Metrics


2014FR04      Nucl.Phys. A928, 128 (2014)

E.Friedman, A.Gal

Testing in-medium πN dynamics on pionic atoms

NUCLEAR STRUCTURE 1n; calculated πN amplitudes in pionic atoms using pion-nucleon in-medium interaction; deduced constraints for the neutron radius parameter.

doi: 10.1016/j.nuclphysa.2014.05.017
Citations: PlumX Metrics


2014FR06      Nucl.Phys. A925, 141 (2014)

E.Friedman

Antineutron and antiproton nuclear interactions at very low energies

NUCLEAR REACTIONS 40Ca(p-bar, p-bar), E=48 MeV; calculated σ(θ). C, Al, Cu, Pb(p-bar, x), (n-bar, x), E at 0-400 MeV/c; calculated total annihilation σ. Compared with available data.

doi: 10.1016/j.nuclphysa.2014.02.010
Citations: PlumX Metrics


2013FR05      Nucl.Phys. A899, 60 (2013)

E.Friedman, A.Gal

Kaonic atoms and in-medium K-N amplitudes II: Interplay between theory and phenomenology

doi: 10.1016/j.nuclphysa.2013.01.016
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2013FR11      Nucl.Phys. A915, 170 (2013)

E.Friedman, S.Okada

Feasibility guidelines for kaonic atom experiments with ultra-high-resolution X-ray spectrometry

ATOMIC PHYSICS Ca, Ti, Cr, Se, Kr, Sr, Zr, Sn, Te, Ce, Yb, Hf, Pb mesic atoms; calculated kaonic atoms strong interaction widths, X-ray energy.

doi: 10.1016/j.nuclphysa.2013.07.005
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2012FR04      Nucl.Phys. A881, 150 (2012)

E.Friedman, A.Gal

Kaonic atoms and in-medium K-N amplitudes

NUCLEAR STRUCTURE Ni, Pb; analyzed published data; calculated K- nuclear potentials using CC chiral models.

doi: 10.1016/j.nuclphysa.2012.01.005
Citations: PlumX Metrics


2012FR08      Nucl.Phys. A896, 46 (2012)

E.Friedman

Neutron skins of 208Pb and 48Ca from pionic probes

NUCLEAR REACTIONS C, Ca, Pb(π+, X), E at 0.7-2.0 GeV/c; calculated, analyzed total σ at relativistic energies varying neutron radial parameters and using simultaneous fit to Allardyce data. 208Pb deduced neutron, proton radii.

ATOMIC PHYSICS 48Ca, 208Pb; calculated, analyzed pionic atom level shifts, level widths by varying neutron radial parameters and using de Laat and Powers data sets; deduced nuclear radii, neutron skin.

doi: 10.1016/j.nuclphysa.2012.09.007
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2011CI06      Phys.Rev. C 84, 045206 (2011)

A.Cieply, E.Friedman, A.Gal, D.Gazda, J.Mares

K- nuclear potentials from in-medium chirally motivated models

doi: 10.1103/PhysRevC.84.045206
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2010GA32      Nucl.Phys. A835, 287c (2010)

D.Gazda, E.Friedman, A.Gal, J.Mares

Kaon condensation and multi-strange matter

NUCLEAR STRUCTURE 16O, 40Ca, 90Zr, 208Pb; calculated hypernuclei mass excess, density distribution.

doi: 10.1016/j.nuclphysa.2010.01.204
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2009GA30      Phys.Rev. C 80, 035205 (2009)

D.Gazda, E.Friedman, A.Gal, J.Mares

Multi-K(bar) hypernuclei

NUCLEAR STRUCTURE 16O, 40Ca, 90Zr, 208Pb; calculated 1s-K(bar) separation energies, density distributions and other parameters for multi-K(bar) hypernuclei using relativistic mean-field (RMF) approach.

doi: 10.1103/PhysRevC.80.035205
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2008GA12      Phys.Rev. C 77, 045206 (2008)

D.Gazda, E.Friedman, A.Gal, J.Mares

Multi-K-bar nuclei and kaon condensation

NUCLEAR REACTIONS 16O, 40Ca, 208Pb(K-, X) E not given; calculated K- separation energy, nuclear density, K- effective mass.

doi: 10.1103/PhysRevC.77.045206
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2007BA07      Phys.Rev. C 75, 022202 (2007)

N.Barnea, E.Friedman

Radial sensitivity of kaonic atoms and strongly bound K-bar states

ATOMIC PHYSICS 12C, Ni; calculated kaon-nucleus potentials for kaonic atoms. Functional derivatives of global fits.

doi: 10.1103/PhysRevC.75.022202
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2007GA53      Phys.Rev. C 76, 055204 (2007); Erratum Phys.Rev. C 77, 019904 (2008)

D.Gazda, E.Friedman, A.Gal, J.Mares

Dynamics of K-bar and multi-K-bar nuclei

NUCLEAR STRUCTURE 12C, 16O, 40Ca, 208Pb; calculated K-meson hypernuclear excitation energies, configurations, level widths, nuclear densities, binding energies using relativistic mean field model.

doi: 10.1103/PhysRevC.76.055204
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2006BR17      Phys.Lett. B 639, 424 (2006)

J.Breitschopf, M.Bauer, H.Clement, M.Croni, H.Denz, E.Friedman, E.F.Gibson, R.Meier, G.J.Wagner

Pionic charge exchange on the proton from 40 to 250 MeV

NUCLEAR REACTIONS 1H(π-, π0), E=39-247 MeV; measured total charge exchange σ. Transmission technique. Comparison with other results and model calculations.

doi: 10.1016/j.physletb.2006.07.009
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0749.


2006GA03      Phys.Rev. C 73, 015208 (2006)

A.Gal, E.Friedman

Room for an S = +1 pentaquark in K+-nucleus phenomenology

NUCLEAR REACTIONS 6Li, 12C, 28Si, 40Ca(K+, X), E at 488, 531, 656, 714 MeV/c; analyzed total, reaction, and elastic σ; deduced role of pentaquark production.

doi: 10.1103/PhysRevC.73.015208
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2006MA20      Nucl.Phys. A770, 84 (2006)

J.Mares, E.Friedman, A.Gal

(K-bar)-nuclear bound states in a dynamical model

NUCLEAR STRUCTURE 6Li, 12C, 16O, 40Ca, 208Pb; calculated deeply bound kaonic states binding energies, widths, densities. 16O; calculated deeply bound kaonic states radius, neutron single-particle energies.

doi: 10.1016/j.nuclphysa.2006.02.010
Citations: PlumX Metrics


2006MA28      Acta Phys.Slovaca 56, 95 (2006)

J.Mares, E.Friedman, A.Gal

Kaonic nuclei

NUCLEAR STRUCTURE 12C, 16O; calculated binding energies and widths for deeply bound kaonic states.


2005FR28      Phys.Rev. C 72, 034609 (2005)

E.Friedman, M.Bauer, J.Breitschopf, H.Clement, H.Denz, E.Doroshkevich, A.Erhardt, G.J.Hofman, S.Kritchman, R.Meier, G.J.Wagner, G.Yaari

Elastic scattering of low energy pions by nuclei and the in-medium isovector πN amplitude

NUCLEAR REACTIONS Si, Ca, Ni, Zr(π+, π+), (π-, π-), E=21.5 MeV; measured σ(θ); deduced optical potential parameters, in-medium isovector amplitude, related features.

doi: 10.1103/PhysRevC.72.034609
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2005FR31      Nucl.Phys. A761, 283 (2005)

E.Friedman, A.Gal, J.Mares

Antiproton-nucleus potentials from global fits to antiprotonic X-rays and radiochemical data

doi: 10.1016/j.nuclphysa.2005.08.001
Citations: PlumX Metrics


2005GA06      Phys.Rev.Lett. 94, 072301 (2005)

A.Gal, E.Friedman

Traces of the Θ+ Pentaquark in K+-Nucleus Dynamics

NUCLEAR REACTIONS 6Li, 12C, 28Si, 40Ca(K+, X), E at 488-714 MeV/c; analyzed reaction σ; deduced absorption σ, possible contribution from pentaquark formation.

doi: 10.1103/PhysRevLett.94.072301
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2005MA02      Phys.Lett. B 606, 295 (2005)

J.Mares, E.Friedman, A.Gal

Widths of (K-bar)-nuclear deeply bound states in a dynamical model

NUCLEAR STRUCTURE 12C, 16O; calculated deeply bound kaonic states binding energies, widths, densities, radii, neutron single-particle energies.

doi: 10.1016/j.physletb.2004.12.086
Citations: PlumX Metrics


2004CI05      Acta Phys.Pol. B35, 1011 (2004)

A.Cieply, E.Friedman, A.Gal, J.Mares

K--Nucleus Potentials Consistent with Kaonic Atoms

NUCLEAR REACTIONS 12C(K-, π-), (K-, π0), E at rest; calculated hypernucleus production rates, kaon-nucleus potential features.


2004FR01      Phys.Lett. B 578, 85 (2004)

E.Friedman, A.Gal

Testing chiral dynamics in pionic atoms

ATOMIC PHYSICS, Mesic-atoms Z=10-92; analyzed pionic atoms data; deduced energy-dependent amplitudes.

doi: 10.1016/j.physletb.2003.10.035
Citations: PlumX Metrics


2004FR03      Nucl.Instrum.Methods Phys.Res. B214, 160 (2004)

E.Friedman, A.Gal

Antiprotonic potentials from global fits to the PS209 data

doi: 10.1016/S0168-583X(03)01763-4
Citations: PlumX Metrics


2004FR18      Acta Phys.Pol. B35, 979 (2004)

E.Friedman

Medium Effects of Low Energy Pions

NUCLEAR STRUCTURE A=12-238; analyzed pionic atom data; deduced medium effects in pion-nucleus potential.


2004FR28      Phys.Rev.Lett. 93, 122302 (2004)

E.Friedman, M.Bauer, J.Breitschopf, H.Clement, H.Denz, E.Doroshkevich, A.Erhardt, G.J.Hofman, R.Meier, G.J.Wagner, G.Yaari

In-Medium Isovector πN Amplitude from Low-Energy Pion Scattering

NUCLEAR REACTIONS Si, Ca, Ni, Zr(π+, π+), (π-, π-), E=21.5 MeV; measured σ(θ); deduced in-medium amplitudes.

doi: 10.1103/PhysRevLett.93.122302
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2004ME07      Phys.Lett. B 588, 155 (2004)

R.Meier, M.Croni, R.Bilger, B.van den Brandt, J.Breitschopf, H.Clement, J.R.Comfort, H.Denz, A.Erhardt, K.Fohl, E.Friedman, J.Grater, P.Hautle, G.J.Hofman, J.A.Konter, S.Mango, J.Patzold, M.M.Pavan, G.J.Wagner, F.von Wrochem

Low energy analyzing powers in pion-proton elastic scattering

NUCLEAR REACTIONS 1H(π+, π+), E=45.2, 51.2, 57.2, 68.5, 77.2, 87.2 MeV; 1H(π-, π-), E=67.3, 87.2 MeV; measured Ay(θ). Polarized target. Comparison with model predictions.

doi: 10.1016/j.physletb.2004.02.071
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2003CI04      Nucl.Phys. A721, 975c (2003)

A.Cieply, E.Friedman, A.Gal, J.Mares

Testing the K--nucleus interaction in (K-stop, π) reactions

NUCLEAR REACTIONS 12C(K-, π-), (K-, π0), E at rest; calculated hypernucleus production rates.

doi: 10.1016/S0375-9474(03)01263-6
Citations: PlumX Metrics


2003FR17      Nucl.Phys. A724, 143 (2003)

E.Friedman, A.Gal

Renormalization of the isovector πN amplitude in pionic atoms

doi: 10.1016/S0375-9474(03)01476-3
Citations: PlumX Metrics


2003FR29      Nucl.Phys. A721, 842c (2003)

E.Friedman, A.Gal

The s-wave repulsion and deeply bound pionic atoms: fact and fancy

doi: 10.1016/S0375-9474(03)01222-3
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2002FR01      Phys.Lett. 524B, 87 (2002)

E.Friedman

Indications of Partial Chiral Symmetry Restoration from Pionic Atoms

NUCLEAR REACTIONS Ca(π+, π+), (π-, π-), E=19.5 MeV; calculated σ(θ). Density-dependent isovector scattering.

ATOMIC PHYSICS Z=8-92; analyzed pionic atom data. Density-dependent isovector scattering.

doi: 10.1016/S0370-2693(01)01326-0
Citations: PlumX Metrics


2002FR15      Nucl.Phys. A710, 117 (2002)

E.Friedman

Density dependence of the s-wave repulsion in pionic atoms

ATOMIC PHYSICS Z=8-92; analyzed pionic atom data; deduced potential parameters.

doi: 10.1016/S0375-9474(02)01126-0
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2001BA55      Nucl.Phys. A689, 721 (2001)

C.J.Batty, E.Friedman, A.Gal

Unified Optical-Model Approach to Low-Energy Antiproton Annihilation on Nuclei and to Antiprotonic Atoms

NUCLEAR REACTIONS 1H(p-bar, X), E at 40-180 MeV/c; Ne(p-bar, X), E at 57, 193 MeV/c; 3,4He(p-bar, X), E at 47, 55, 70 MeV/c; calculated annihilation σ. 4He, 6Li, 9Be, 10B, 12C, 16O, Ne, Ca(p-bar, X), E at rest; analyzed data; deduced s-wave scattering lengths. Folding model, optical potential.

doi: 10.1016/S0375-9474(00)00608-4
Citations: PlumX Metrics


2001CI09      Nucl.Phys. A696, 173 (2001)

A.Cieply, E.Friedman, A.Gal, J.Mares

Study of Chirally Motivated Low-Energy K- Optical Potentials

NUCLEAR REACTIONS 1H(K-, K-), (K-, K0), (K-, π-X), (K-, π0X), (K-, π+X), E at 50-200 MeV/c; calculated σ. 12C(K-, X)12C/12B, E at rest; calculated hypernucleus production σ. 12C, 28Si(π+, K+), (K-, p), E at 1 GeV/c; calculated σ(θ=0°). Comparisons with data.

doi: 10.1016/S0375-9474(01)01145-9
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2000FR08      Nucl.Phys. A663-664, 557c (2000)

E.Friedman, A.Gal

Narrow Deeply Bound K- and (p-bar) Atomic States

ATOMIC PHYSICS, Mesic-atoms Pb; calculated kaonic, antiprotonic atom energy levels. Production mechanisms discussed.

doi: 10.1016/S0375-9474(99)00655-7
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2000GA45      Phys.Lett. 491B, 219 (2000)

A.Gal, E.Friedman, C.J.Batty

Saturation of Low-Energy Antiproton Annihilation on Nuclei

NUCLEAR REACTIONS 4He, Ne(p-bar, X), E at 57 MeV/c; calculated reaction σ; deduced optical potential features, saturation mechanism.

doi: 10.1016/S0370-2693(00)01040-6
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1999BA02      Phys.Rev. C59, 295 (1999)

C.J.Batty, E.Friedman, A.Gal

Experiments with Ξ- Atoms

ATOMIC PHYSICS, Mesic-Atoms N, O, F, Ne, Na, Si, S, Cl, Ca, Ag, Sn, I, Ba, Ta, W, Pb; calculated Ξ- atoms strong interaction shifts, widths. 2H; calculated Ξ- atoms S and P state capture fractions vs Stark mixing parameter. Proposals for future experiments discussed.

doi: 10.1103/PhysRevC.59.295
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1999FR19      Phys.Lett. 459B, 43 (1999)

E.Friedman, A.Gal

Narrow Deeply Bound K- Atomic States

ATOMIC PHYSICS, Mesic-atoms C, Ni, Pb; calculated deeply bound kaonic levels energies, widths. Optical potentials.

doi: 10.1016/S0370-2693(99)00651-6
Citations: PlumX Metrics


1999FR22      Phys.Rev. C60, 024314 (1999)

E.Friedman, A.Gal, J.Mares, A.Cieply

K--Nucleus Relativistic Mean Field Potentials Consistent with Kaonic Atoms

doi: 10.1103/PhysRevC.60.024314
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1999FR36      Nucl.Phys. A658, 345 (1999)

E.Friedman, A.Gal

K- and p(bar) Deeply Bound Atomic States

ATOMIC PHYSICS, Mesic-atoms C, Ni, Zr, Pb; calculated kaonic, antiprotonic atoms energy levels. Production mechanisms discussed.

doi: 10.1016/S0375-9474(99)00360-7
Citations: PlumX Metrics


1999GR01      Eur.Phys.J. A 4, 5 (1999)

J.Grater, P.A.Amaudruz, R.Bilger, P.Camerini, J.Clark, H.Clement, E.Friedman, L.Felawka, S.N.Filippov, E.Friagiacomo, Yu.K.Gavrilov, E.Gibson, N.Grion, G.J.Hofman, B.Jamieson, T.L.Karavicheva, M.Kermani, E.L.Mathie, R.Meier, G.Moloney, D.Ottewell, J.Patzold, O.Patarakin, K.Raywood, R.Rui, M.Schepkin, M.E.Sevior, G.R.Smith, H.Staudenmaier, R.Tacik, G.Tagliente, G.J.Wagner, M.Yeomans

Search for a Bound Trineutron with the 3He(π-π+)nnn Reaction

NUCLEAR REACTIONS 3He(π-, π+), E=65, 75, 120 MeV; measured three-neutron system invariant mass spectra; deduced no trineutron bound state or unbound resonance.

doi: 10.1007/s100500050196
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1998FR10      Phys.Lett. 432B, 235 (1998)

E.Friedman, A.Gal

On the Determination of the Pion Effective Mass in Nuclei from Pionic Atoms

ATOMIC PHYSICS, Mesic-atoms 207Pb; analyzed data; deduced pion-nucleus potential, pion effective mass.

doi: 10.1016/S0370-2693(98)00655-8
Citations: PlumX Metrics


1998FR12      Nucl.Phys. A639, 511c (1998)

E.Friedman

Strange Exotic Atoms

doi: 10.1016/S0375-9474(98)00319-4
Citations: PlumX Metrics


1997BB03      Phys.Rep. 287, 385 (1997)

C.J.Batty, E.Friedman, A.Gal

Strong Interaction Physics from Hadronic Atoms

doi: 10.1016/S0370-1573(97)00011-2
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1997FR02      Phys.Rev. C55, 1304 (1997)

E.Friedman, A.Gal, R.Weiss, J.Aclander, J.Alster, I.Mardor, Y.Mardor, S.May Tal-Beck, E.Piasetzky, A.I.Yavin, S.Bart, R.E.Chrien, P.H.Pile, R.Sawafta, R.J.Sutter, M.Barakat, K.Johnston, R.A.Krauss, H.Seyfarth, R.L.Stearns

K+ Nucleus Reaction and Total Cross Sections: New analysis of transmission experiments

NUCLEAR REACTIONS 6Li, C, Si, Ca(K+, X), E at 488-714 MeV/c; measured attenuation σ, transmission experiments; deduced reaction, total σ.

doi: 10.1103/PhysRevC.55.1304
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1997FR08      Phys.Lett. 396, 21 (1997)

E.Friedman, A.Gal, J.Mares

Medium Effects in K+ Nucleus Interaction from Consistent Analysis of Integral and Differential Cross Sections

NUCLEAR REACTIONS 6Li, C(K+, K+), E at 715 MeV/c; calculated σ(θ). Li, C, Si, Cu(K+, X), E at 714 MeV/c; calculated reaction, total σ. Medium effects, self-consistent approach.

doi: 10.1016/S0370-2693(97)00087-7
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1997FR21      Nucl.Phys. A625, 272 (1997)

E.Friedman, A.Gal, J.Mares

Medium Effects in K+ Nuclear Interactions

NUCLEAR REACTIONS 6Li, C, Si, Ca(K+, X), E at 488-714 MeV/c; calculated total, reaction σ; deduced medium effects.

doi: 10.1016/S0375-9474(97)00484-3
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1997RA12      Phys.Rev. C55, 2492 (1997)

K.J.Raywood, J.B.Lange, G.Jones, M.Pavan, M.E.Sevior, D.A.Hutcheon, A.Olin, D.Ottewell, S.Yen, S.J.Lee, K.S.Sim, A.Altman, E.Friedman, A.Trudel

Search for Deeply Bound Pionic States in 208Pb Via Radiative Atomic Capture of Negative Pions

NUCLEAR REACTIONS 208Pb(π-, X), E=20, 25 MeV; measured radiative capture Eγ, Iγ; deduced atomic capture σ, probability.

ATOMIC PHYSICS, Mesic-Atoms 208Pb(π-, X), E=20, 25 MeV; measured radiative capture Eγ, Iγ; deduced atomic capture σ, probability.

doi: 10.1103/PhysRevC.55.2492
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1996GA21      Nucl.Phys. A606, 283 (1996)

A.Gal, E.Friedman, C.J.Batty

On the Interplay between Coulomb and Nuclear States in Exotic Atoms

ATOMIC PHYSICS 16O(p-bar, X), E not given; calculated strong interaction shifts, widths; deduced Coulomb, nuclear states interplay role.

NUCLEAR REACTIONS 16O(p-bar, X), E not given; calculated strong interaction shifts, widths; deduced Coulomb, nuclear states interplay role.

doi: 10.1016/0375-9474(96)00211-4
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1995BA71      Nucl.Phys. A592, 487 (1995)

C.J.Batty, E.Friedman, A.Gal

Density-Dependent (p-bar)-Nucleus Optical Potentials from Global Fits to (p-bar) Atom Data

NUCLEAR REACTIONS C, N, 16,18O, F, Na, Si, 31P, S, Cl, K, Fe, 89Y, Zr, 92,98Mo, Sn, 127I, Ba, 141Pr(p-bar, X), E not given; analyzed (p-bar)-atom data; deduced (p-bar)-nucleus optical potentials. Density-dependence introduced.

doi: 10.1016/0375-9474(95)00308-N
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1995MA63      Nucl.Phys. A594, 311 (1995)

J.Mares, E.Friedman, A.Gal, B.K.Jennings

Constraints on Σ-Nucleus Dynamics from Dirac Phenomenology of Σ- Atoms

NUCLEAR STRUCTURE Si, Ca, Pb; calculated Σ--nucleus potentials, interaction shifts, widths; deduced isovector meson-hyperon coupling, implication to Σ-hypernuclei. Relativistic mean field approach.

ATOMIC PHYSICS, Mesic-Atoms Si, Ca, Pb; calculated Σ--nucleus potentials, interaction shifts, widths; deduced isovector meson-hyperon coupling, implication to Σ hypernuclei. Relativistic mean field approach.

doi: 10.1016/0375-9474(95)00358-8
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1994BA61      Phys.Lett. 335B, 273 (1994)

C.J.Batty, E.Friedman, A.Gal

Density Dependence of the Σ Nucleus Optical Potential Derived from Σ- Atom Data

doi: 10.1016/0370-2693(94)90349-2
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1994BB13      Prog.Theor.Phys.(Kyoto), Suppl. 117, 227 (1994)

C.J.Batty, E.Friedman, A.Gal

Density Dependence in Σ- Atoms and Implications for Σ Hypernuclei

ATOMIC PHYSICS, Mesic-Atoms C, O, Mg, 27Al, Si, S, Ca, Ti, Ba, W, Pb; analyzed Σ- atomic level strong interaction energy shifts, widths, yields data; deduced Σ-nucleus optical potential parameters. Density-dependent interactions.

doi: 10.1143/PTPS.117.227
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1994FR13      Nucl.Phys. A579, 518 (1994)

E.Friedman, A.Gal, C.J.Batty

Density-Dependent K- Nuclear Optical Potentials from Kaonic Atoms

NUCLEAR STRUCTURE A=4-238; compiled, reviewed, analyzed kaon scattering data. Density-dependent optical potentials.

ATOMIC PHYSICS, Mesic-Atoms A=4-238; compiled, reviewed, analyzed kaon scattering data. Density-dependent optical potentials.

doi: 10.1016/0375-9474(94)90921-0
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1993FR02      Phys.Lett. 302B, 18 (1993)

E.Friedman, M.Paul, M.Schechter, A.Altman, B.K.Jennings, G.J.Wagner, N.Fazel, R.R.Johnson, N.Suen, Z.Fraenkel

Integral Cross Sections for π-p Interaction in the 3, 3 Resonance Region

NUCLEAR REACTIONS 1H(π-, X), E=126-202 MeV; measured total, single charge exchange σ. Model comparison.

doi: 10.1016/0370-2693(93)90629-V
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0749.


1993FR10      Phys.Lett. 308B, 6 (1993)

E.Friedman, A.Gal, C.J.Batty

Density Dependence in Kaonic Atoms

NUCLEAR STRUCTURE Z=3-92; analyzed kaonic atom data; deduced optical potential characteristics.

ATOMIC PHYSICS, Mesic-Atoms Z=3-92; analyzed kaonic atom data; deduced optical potential characteristics.

doi: 10.1016/0370-2693(93)90593-7
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1993FR20      Acta Phys.Pol. B24, 1673 (1993)

E.Friedman

Gross Properties of Pion- and Kaon-Nucleus Interaction

NUCLEAR REACTIONS 48Ca(π+, π+), (π-, π-), E=50 MeV; 40Ca(π, π), E=30-80 MeV; analyzed σ(θ); compiled, reviewed other reactions data; deduced nuclear medium modification of meson-nucleon interaction features.


1992GA09      Phys.Lett. 281B, 11 (1992)

A.Gal, B.K.Jennings, E.Friedman

Does the Relativistic Impulse Approximation Produce Sufficient s-Wave Repulsion for Pionic Atoms ( Questions )

NUCLEAR REACTIONS 40Ca(π, π), E=low; analyzed pionic atom data; deduced pion-nucleus potentials parameters. Relativistic impulse approximation, ambiguities discussed.

doi: 10.1016/0370-2693(92)90265-6
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1991BA44      Nucl.Phys. A535, 548 (1991)

C.J.Batty, E.Friedman, A.Gal, G.Kalbermann

Finite-Range Effects in Hadronic Atoms (II). Kaonic and Antiprotonic Atoms

NUCLEAR STRUCTURE 16O, 32S; calculated kaonic level shift, width. Nonlocal optical model, finite-range effects.

ATOMIC PHYSICS, Mesic-Atoms 16O, 32S; calculated kaonic level shift, width. Nonlocal optical model, finite-range effects.

doi: 10.1016/0375-9474(91)90475-L
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1991FR01      Phys.Lett. 254B, 40 (1991)

E.Friedman, A.Goldring, R.R.Johnson, D.Vetterli, J.Jaki, M.Metzler, B.K.Jennings

Integral Cross Sections for π+p Interaction in the 3, 3 Resonance Region

NUCLEAR REACTIONS 1H(π+, π+), E=125.9-201.7 MeV; measured σ. Transmission method. Phase shift calculations.

doi: 10.1016/0370-2693(91)90392-4
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1991FR04      Phys.Lett. 257B, 17 (1991)

E.Friedman, A.Goldring, R.R.Johnson, O.Meirav, D.Vetterli, P.Weber, A.Altman

Total Reaction Cross Sections for 20-30 MeV Pions and the Anomaly of Pionic Atoms

NUCLEAR REACTIONS C, Ni(π-, X), E=20, 30 MeV; C, Ni(π+, X), E=30 MeV; measured reaction σ. Different potentials in model analyses.

doi: 10.1016/0370-2693(91)90850-P
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1990FR09      Nucl.Phys. A514, 601 (1990)

E.Friedman, A.Goldring, G.J.Wagner, A.Altman, R.R.Johnson, O.Meirav, B.K.Jennings

Integral Cross Sections for π+p Interactions at Low Energies

NUCLEAR REACTIONS 1H(π+, π+), E=45-126 MeV; measured σ. Beam attenuation technique.

doi: 10.1016/0375-9474(90)90012-B
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1989FR11      Phys.Lett. 231B, 39 (1989)

E.Friedman, A.Goldring, G.J.Wagner, A.Altman, R.R.Johnson, O.Meirav, M.Hanna, B.K.Jennings

Integral Cross Sections for π+p Scattering between 52 and 126 MeV

NUCLEAR REACTIONS 1H(π+, π+), E=52-126 MeV; measured σ(E). Model comparison.

doi: 10.1016/0370-2693(89)90109-3
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1989KA37      Nucl.Phys. A503, 632 (1989)

G.Kalbermann, E.Friedman, A.Gal, C.J.Batty

Finite-Range Effects in Pionic Atoms

ATOMIC PHYSICS, Mesic-Atoms 16,18O, 19F, 20Ne, Si, Ca, 44Ca, Fe, Ge, 168Er, 209Bi, U; analyzed pionic atom data; deduced finite-range effects role.

doi: 10.1016/0375-9474(89)90433-8
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1989ME07      Phys.Rev. C40, 843 (1989)

O.Meirav, E.Friedman, R.R.Johnson, R.Olszewski, P.Weber

Low Energy Pion-Nucleus Potentials from Differential and Integral Data

NUCLEAR REACTIONS Si, Ni(π+, X), (π-, X), E=50 MeV; Ni(π-, X), (π+, X), E=65 MeV; C, Ca, Zr, Pb(π+, X), (π-, X), E=80 MeV; measured reaction σ; deduced model parmeters. Analysis of other data.

doi: 10.1103/PhysRevC.40.843
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1988FR02      Phys.Lett. 200B, 251 (1988)

E.Friedman, A.Gal, G.Kalbermann, C.J.Batty

Strong-Interaction Finite-Range Effects in Light Pionic Atoms

ATOMIC PHYSICS, Mesic-Atoms 4He, 16O; calculated pionic atom level shifts, widths. Finite-range interaction model.

doi: 10.1016/0370-2693(88)90765-4
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1988FR10      Phys.Lett. 207B, 381 (1988)

E.Friedman

Scattering of Low Energy Pions by 12C, 40Ca, 58,60,64Ni and the Anomaly in Pionic Atoms

NUCLEAR REACTIONS 40Ca, 12C(π+, π+), (π-, π-), E=19.5 MeV; 58,60,64Ni(π+, π+), (π-, π-), E=30 MeV; analyzed σ(θ); deduced pion-nucleus potential features.

doi: 10.1016/0370-2693(88)90668-5
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1987ME12      Phys.Rev. C36, 1066 (1987)

O.Meirav, E.Friedman, A.Altman, M.Hanna, R.R.Johnson, D.R.Gill

Total Reaction Cross Sections of 50 and 65 MeV Pions on Nuclei

NUCLEAR REACTIONS C, O, 18O, S, Ca, Zr(π+, X), (π-, X), E=50, 65 MeV; measured reaction σ. Ca(π-, π-), E=50 MeV; measured σ(θ); deduced elastic corrections.

doi: 10.1103/PhysRevC.36.1066
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1987ME20      Phys.Lett. 199B, 9 (1987)

O.Meirav, E.Friedman, A.Altman, M.Hanna, R.R.Johnson, D.R.Gill

Pion-Nucleus Potentials in the Energy Range of 0-80 MeV

NUCLEAR REACTIONS 64Ni, 40Ca, 90Zr(π+, π+), (π-, π-), E=65, 80 MeV; 208Pb(π+, π+), (π-, π-), E=30, 80 MeV; calculated σ(θ); deduced potential parameters. Optical model.

doi: 10.1016/0370-2693(87)91453-5
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1986FR10      Nucl.Phys. A455, 573 (1986)

E.Friedman, J.Lichtenstadt

The Information Content of Antiproton-Nucleus Scattering Data

NUCLEAR REACTIONS 12C, 16,18O, 40Ca(p-bar, p-bar), E=180 MeV; 40Ca(p-bar, p-bar), E=40 MeV; analyzed data; deduced folding model parameters.

doi: 10.1016/0375-9474(86)90451-3
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1986FR20      Phys.Rev. C34, 2244 (1986)

E.Friedman, G.Kalbermann, C.J.Batty

Kemmer-Duffin-Petiau Equation for Pionic Atoms and Anomalous Strong Interaction Effects

ATOMIC PHYSICS, Mesic-Atoms Mg, Pb, U, 16O, 168Er; calculated pion atom level shifts, widths.

doi: 10.1103/PhysRevC.34.2244
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1985BA09      Nucl.Phys. A436, 621 (1985)

C.J.Batty, E.Friedman, J.Lichtenstadt

Combined Analysis of Antiprotonic Atoms and Antiproton Elastic Scattering Data

ATOMIC PHYSICS 12C, 16O, S, 89Y; analyzed antiprotonic atom data; deduced transition shifts, widths.

NUCLEAR REACTIONS 12C(p-bar, p-bar), E=47 MeV; analyzed σ(θ); deduced antiprotonic atom potential parameters. Antiprotonic atom data input.

doi: 10.1016/0375-9474(85)90551-2
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1985FR03      J.Phys.(London) G11, L37 (1985)

E.Friedman, G.Soff

Calculations of Deeply Bound Pionic States in Heavy and Superheavy Atoms

ATOMIC PHYSICS, Mesic-Atoms 238U, 120Sn, 296136; calculated pionic level binding energies, widths.

doi: 10.1088/0305-4616/11/3/003
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1985GI02      J.Phys.(London) G11, 85 (1985)

H.J.Gils, E.Friedman

Combined Analysis of Pionic Atoms and Elastic Scattering of Alpha Particles

ATOMIC PHYSICS, Mesic-Atoms 40,42,44,48Ca; analyzed pionic atom strong interaction shifts, widths data. 40,42,44,48Ca deduced neutron density radial moments. Elastic α-scattering data input.

NUCLEAR REACTIONS 40,42,44,48Ca(α, α), E=104 MeV; analyzed σ(θ). 40,42,44,48Ca deduced neutron density radial moments. Pionic atom data input.

doi: 10.1088/0305-4616/11/1/013
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1984BA39      Phys.Lett. 142B, 241 (1984)

C.J.Batty, E.Friedman, J.Lichtenstadt

Optical Potentials for Low Energy Antiproton-Nucleus Interactions

ATOMIC PHYSICS C, O, S, Y; analyzed antiprotonic atom data; deduced model independent potentials. Optical model.

NUCLEAR REACTIONS 12C(p-bar, p-bar), E=47 MeV; analyzed data; deduced model independent potentials. Optical model.

doi: 10.1016/0370-2693(84)91190-0
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1984GI03      Phys.Rev. C29, 1295 (1984)

H.J.Gils, H.Rebel, E.Friedman

Isotopic and Isotonic Differences between α Particle Optical Potentials and Nuclear Densities of 1f7/2 Nuclei

NUCLEAR REACTIONS 40,42,43,44,48Ca, 50Ti, 51V, 52Cr(α, α), E=104 MeV; analyzed σ(θ); deduced isotopic, isotonic differences of optical potentials and nuclear matter densities. Fourier-Bessel potential, folding model analysis.

doi: 10.1103/PhysRevC.29.1295
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1983BA27      Nucl.Phys. A402, 411 (1983)

C.J.Batty, E.Friedman, A.Gal

Saturation Effects in Pionic Atoms and the π--Nucleus Optical Potential

ATOMIC PHYSICS, Mesic-Atoms 16,18O, 19F, 44Ca, Ca, 20Ne, Si, Fe, Ge, Ag, Bi, Na, As, Ta; analyzed pionic atom level shift, width data. Different pion-nucleus optical potentials.

doi: 10.1016/0375-9474(83)90211-7
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1983FR22      Phys.Rev. C28, 1264 (1983)

E.Friedman

Systematics of Pion-Nucleus Optical Potentials from Analysis of Elastic Scattering

NUCLEAR REACTIONS 12C(π-, π-), E=80 MeV; 12C(π+, π+), E=14, 50, 65, 80 MeV; 90Zr(π+, π+), E=30, 50, 80 MeV; 40Ca(π+, π+), (π-, π-), E=65 MeV; analyzed σ(θ); deduced pion-nucleus optical potential characteristics, energy, charge dependence. Complex local potential, Fourier-Bessel series parametrization.

doi: 10.1103/PhysRevC.28.1264
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1983PE10      Z.Phys. A313, 111 (1983)

R.Pesl, H.J.Gils, H.Rebel, E.Friedman, J.Buschmann, H.Klewe-Nebenius, S.Zagromski

Optical Potentials and Isoscalar Transition Rates from 104 MeV Alpha-Particle Scattering by the N = 28 Isotones 48Ca, 50Ti and 52Cr

NUCLEAR REACTIONS 48Ca, 50Ti, 52Cr(α, α), (α, α'), E=104 MeV; measured σ(θ); deduced optical model, deformation parameters. 50Ti, 52Cr deduced rms charge radii, isoscalar transition rates. 48Ca deduced rms charge radii.

doi: 10.1007/BF02115849
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2262.


1982EN05      Phys.Lett. 117B, 279 (1982)

Y.M.Engel, E.Friedman, R.D.Levine

The Maximun Entropy Determination of Nuclear Densities of Calcium Isotopes from Elastic Scattering of Alpha Particles

NUCLEAR STRUCTURE 40,42,44,48Ca; calculated rms radius. Fourier-Bessel analysis, maximum entropy formalism, folding model potential radial moment constraint.

doi: 10.1016/0370-2693(82)90718-3
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1982FI14      Nucl.Phys. A389, 18 (1982)

D.Fink, E.Friedman, M.Paul, A.Moalem

Experimental Determination of the Normalization Constant of the (α, t) Reaction

NUCLEAR REACTIONS 48Ca, 92Mo(α, t), E=26-30 MeV; 48Ca, 92Mo(3He, d), E=16 MeV; measured absolute σ(θ). 49Sc, 93Tc level deduced normalizations. Enriched targets.

doi: 10.1016/0375-9474(82)90287-1
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1982FR06      Phys.Rev. C25, 1551 (1982)

E.Friedman, H.J.Gils, H.Rebel

Comparison between Radial Sensitivity of Different Strongly Interacting Probes

NUCLEAR REACTIONS 48Ca(α, α), E=104 MeV; 48Ca(p, p), E=1 GeV; 48Ca(π+, π+), (π-, π-), E=50, 130 MeV; analyzed σ(θ). 48Ca deduced neutron density radial dependence, rms radii. Optical model, Fourier-Bessel method.

ATOMIC PHYSICS, Mesic-Atoms 48Ca; calculated strong interaction shifts, widths; deduced surface effects. Optical model, Fourier-Bessel method.

doi: 10.1103/PhysRevC.25.1551
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1981AL04      Nucl.Phys. A356, 307 (1981)

Y.Alexander, A.Gal, V.B.Mandelzweig, E.Friedman

Finite-Range Effects in Pionic Atoms

ATOMIC PHYSICS, Mesic-Atoms 16,18O, 40,44Ca, Fe, 28Si, Ag, 209Bi; calculated strong interaction shifts, widths; deduced finite range mass dependence. Modified pion-nucleus optical potential.

doi: 10.1016/0375-9474(81)90191-3
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1981FR10      Nucl.Phys. A363, 137 (1981)

E.Friedman, H.J.Gils, H.Rebel, R.Pesl

The Dependence on Energy and Mass Number of the α-Particle Optical Potential: Support for the folding model approach

NUCLEAR REACTIONS 40,42,44,48Ca, 50Ti, 52Cr, 90Zr(α, α), E=104 MeV; 40Ca, 46,48,50Ti, 58Ni, 90Zr, 208Pb(α, α), E=140 MeV; 58,60,62,64Ni(α, α), E=173 MeV; analyzed σ(θ); deduced mass, energy dependence of rms radius of optical potential components. Fourier-Bessel description.

doi: 10.1016/0375-9474(81)90458-9
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1981FR17      Phys.Lett. 104B, 357 (1981)

E.Friedman

Zero Energy Pion-Nucleus Potential from 1s States in Pionic Atoms

ATOMIC PHYSICS, Mesic-Atoms 10,11B, 16,18O, 19F; analyzed pionic level shifts, widths; deduced local potential isovector component. Optical model.

doi: 10.1016/0370-2693(81)90697-3
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1981RE09      Nucl.Phys. A368, 61 (1981)

H.Rebel, R.Pesl, H.J.Gils, E.Friedman

Method for Analysis of Inelastic α-Particle Scattering

NUCLEAR REACTIONS 50Ti, 52Cr(α, α'), E=104 MeV; calculated σ(θ). Fourier-Bessel method.

doi: 10.1016/0375-9474(81)90730-2
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1980FR09      Nucl.Phys. A345, 457 (1980)

E.Friedman, A.Gal

Investigation of the Pion-Nucleus Optical Potential from Pionic Atoms

ATOMIC PHYSICS, Mesic-Atoms 18O, 44Ca, Fe, 23Na, 181Ta, Re, 209Bi; calculated strong interaction level shifts, widths in pionic atoms. Zero-energy π--nucleus optical potential, Lorentz-Lorenz effect.

doi: 10.1016/0375-9474(80)90350-4
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1980GI02      Phys.Rev. C21, 1239 (1980)

H.J.Gils, E.Friedman, H.Rebel, J.Buschmann, S.Zagromski, H.Klewe-Nebenius, B.Neumann, R.Peel, G.Bechtold

Nuclear Sizes of 40,42,44,48Ca from Elastic Scattering of 104 MeV Alpha Particles. I. Experimental Results and Optical Potentials

NUCLEAR REACTIONS 40,42,44,48Ca(α, α), E=104 MeV; measured σ(θ); deduced real potential isotopic dependence. Optical model analysis, Fourier-Bessel method.

doi: 10.1103/PhysRevC.21.1239
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0332.


1979BA07      Phys.Lett. 81B, 165 (1979)

C.J.Batty, S.F.Biagi, E.Friedman, S.D.Hoath, J.D.Davies, C.J.Pyle, G.T.A.Squier, D.M.Asbury, M.Leon

Pionic X-Rays and the Neutron Radius of 44Ca

ATOMIC PHYSICS, Mesic-Atoms 40,44Ca; measured pionic X-rays for 3d→2p; deduced isotopic dependence of strong interaction shifts, rms neutron radii. Effective pion-nucleus potential.

doi: 10.1016/0370-2693(79)90513-6
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