NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = M.A.Franey Found 43 matches. 2004RI05 Phys.Rev. C 69, 024616 (2004) C.M.Riedel, D.Dehnhard, M.Palarczyk, M.A.Espy, M.A.Franey, J.L.Langenbrunner, L.C.Bland, D.S.Carman, B.Brinkmoller, R.Madey, Y.Wang, J.W.Watson Measurement of 4He(p(pol), n) at 100 and 200 MeV: Analysis with recoil-corrected continuum shell model NUCLEAR REACTIONS 4He(polarized p, n), E=100, 200 MeV; measured σ(E, θ), Ay(θ); deduced core contributions and ground-state correlation effects. Recoil-corrected continuum shell model analysis.
doi: 10.1103/PhysRevC.69.024616
1998PA22 Phys.Rev. C58, 645 (1998) M.Palarczyk, C.M.Riedel, D.Dehnhard, M.A.Espy, M.A.Franey, J.L.Langenbrunner, L.C.Bland, D.S.Carman, B.Brinkmoller, R.Madey, Y.Wang, J.W.Watson, N.S.Chant Cross Sections and Analyzing Powers for the (p(pol), n) Reaction on 3He and 4He at 200 MeV NUCLEAR REACTIONS 3,4He(polarized p, n), E=200 MeV; measured neutron spectra, σ(Ex, θ), A(y)(θ). DWIA analysis.
doi: 10.1103/PhysRevC.58.645
1996ED02 Phys.Lett. 368B, 39 (1996); Erratum Phys.Lett. 380B, 493 (1996) C.M.Edwards, M.Palarczyk, D.Dehnhard, M.A.Espy, M.A.Franey, J.L.Langenbrunner, L.C.Bland, D.S.Carman, B.Brinkmoller, R.Madey, Y.Wang, J.W.Watson, L.Bildsten The 4He(p, n)4Li(*) Reaction at 100 and 200 MeV; Implications for the mass-four system and for astrophysics NUCLEAR REACTIONS 4He(p, nX), E=100, 200 MeV; measured inclusive σ(θ, En). 4Li deduced evidence for narrow states.
doi: 10.1016/0370-2693(95)01499-3
1995MA44 Phys.Rev. C52, 291 (1995) A.M.Mack, N.M.Hintz, D.Cook, M.A.Franey, J.Amann, M.Barlett, G.W.Hoffmann, G.Pauletta, D.Ciskowski, M.Purcell Proton Scattering by 206,207,208Pb at 650 MeV: Phenomenological analysis NUCLEAR REACTIONS 206,207,208Pb(polarized p, p), (polarized p, p'), E=650 MeV; measured σ(θ), analyzing power vs θ; deduced model parameters. 206,208Pb levels deduced B(λ), neutron-proton matrix element ratios. Phenomenological analysis.
doi: 10.1103/PhysRevC.52.291
1994YE06 Phys.Rev. C50, 897 (1994) Y.-F.Yen, B.Brinkmoller, D.Dehnhard, M.A.Franey, S.M.Sterbenz, Y.-J.Yu, B.Berman, G.R.Burleson, K.Cranston, A.Klein, G.S.Kyle, R.Alarcon, T.Averett, J.R.Comfort, J.J.Gorgen, B.G.Ritchie, J.R.Tinsley, M.Barlett, G.W.Hoffmann, K.Johnson, C.F.Moore, M.Purcell, H.Ward, A.Williams, J.A.Faucett, S.J.Greene, J.J.Jarmer, J.A.McGill, C.L.Morris, S.I.Penttila, N.Tanaka, H.T.Fortune, E.Insko, R.Ivie, J.M.O'Donnell, D.Smith, M.A.Khandaker, S.Chakravarti Pion Elastic Scattering from Polarized 13C in the Energy Region of the P33 Resonance NUCLEAR REACTIONS 13C(π+, π+), (π-, π-), E=130-180 MeV; 13C(π+, π+), E=223 MeV; 13C(π-, π-), E=226 MeV; measured analyzing power A(y)(θ), σ(θ); deduced spin-flip transition quadrupole component role. Polarized, unpolarized target. DWIA calculations, optical, Δ-hole models.
doi: 10.1103/PhysRevC.50.897
1990IE01 Phys.Rev. C42, 457 (1990) K.Ieki, J.Iimura, M.Iwase, H.Ohnuma, H.Shimizu, H.Toyokawa, K.Furukawa, H.Kabasawa, T.Nakagawa, T.Tohei, H.Orihara, S.I.Hayakawa, T.Hasegawa, K.Nisimura, M.Yasue, K.Miura, T.Suehiro, M.A.Franey Density Dependent Interaction Applied to Low-Multipole (p, p') and (p, n) Transitions in Light Nuclei NUCLEAR REACTIONS 14C, 14N(polarized p, n); 14N, 12C(polarized p, p'), E=35 MeV; measured σ(θ), A(θ); deduced density dependence of effective interaction. DWBA analysis.
doi: 10.1103/PhysRevC.42.457
1990OH04 Nucl.Phys. A514, 273 (1990) H.Ohnuma, N.Hoshino, K.Ieki, M.Iwase, H.Shimizu, H.Toyokawa, T.Hasegawa, K.Nisimura, M.Yasue, H.Kabasawa, T.Nakagawa, T.Tohei, H.Orihara, S.I.Hayakawa, K.Miura, T.Suehiro, S.K.Nanda, D.Dehnhard, M.A.Franey The 16O(p(pol), p) Reaction at 35 MeV NUCLEAR REACTIONS 16O(polarized p, p'), E=35 MeV; measured σ(θ), A(θ). DWBA analysis, shell model wave functions, electron scattering transition densities, density independent, dependent interactions.
doi: 10.1016/0375-9474(90)90070-3
1988HI01 Phys.Rev. C37, 692 (1988) N.M.Hintz, D.Cook, M.Gazzaly, M.A.Franey, M.L.Barlett, G.W.Hoffmann, R.Fergerson, J.McGill, G.Pauletta, R.L.Boudrie, J.B.McClelland, K.W.Jones Energy Dependence of Neutron-Proton Matrix Element Ratios Derived from 25-800 MeV Energy Proton Scattering NUCLEAR REACTIONS 58Ni, 208Pb(p, p), (p, p'), E=318-800 MeV; measured σ(θ); deduced potential deformation lengths. 40Ca, 58Ni, 208Pb levels deduced neutron, proton matrix element ratio. Other data input.
doi: 10.1103/PhysRevC.37.692
1988SE04 Phys.Rev. C37, 2057 (1988) S.J.Seestrom-Morris, D.Dehnhard, M.A.Franey, D.B.Holtkamp, C.L.Blilie, C.L.Morris, J.D.Zumbro, H.T.Fortune Pion Inelastic Scattering to the Three Lowest 2+ States of 18O NUCLEAR REACTIONS 18O(π+, π+'), (π-, π-'), E=164 MeV; measured σ(θ). 18O levels deduced matrix elements, transition densities. Gas Target. DWIA analysis.
doi: 10.1103/PhysRevC.37.2057
1987CH14 Phys.Rev. C35, 2197 (1987) S.Chakravarti, D.Dehnhard, M.A.Franey, S.J.Seestrom-Morris, D.B.Holtkamp, C.L.Blilie, A.C.Hayes, C.L.Morris, D.J.Millener Distorted-Wave Impulse Approximation and Coupled-Channels Analysis of Inelastic Pion Scattering from 18O NUCLEAR REACTIONS 18O(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=164 MeV; calculated σ(θ). 18O levels deduced transition densities. DWIA, coupled-channels calculations.
doi: 10.1103/PhysRevC.35.2197
1987LO13 Phys.Rev.Lett. 59, 1401 (1987) W.G.Love, K.Nakayama, M.A.Franey Isovector Couplings for Nucleon Charge-Exchange Reactions at Intermediate Energies NUCLEAR REACTIONS 14C(p, n), E=60-450 MeV; calculated σ(θ=0°) vs E; deduced nucleon-nucleon interaction isovector component features.
doi: 10.1103/PhysRevLett.59.1401
1986EL04 Nucl.Phys. A458, 269 (1986) P.J.Ellis, Z.El-Itaoui, M.A.Franey, B.A.Mughrabi Inelastic Excitation and the Nucleon Optical Potential NUCLEAR REACTIONS 40Ca(p, p), (p, p'), (n, n), 208Pb(p, p), (n, n), E=30 MeV; calculated σ(θ). Approximate polarization potentials, optical model, coupled channels calculations.
doi: 10.1016/0375-9474(86)90357-X
1986KL01 Phys.Rev.Lett. 56, 700 (1986) Antinucleon Charge-Exchange Reaction as a Probe of Longitudinal Spin Excitations NUCLEAR REACTIONS 90Zr(p-bar, n-bar), E=175 MeV; calculated σ; deduced longitudinal spin excitation probe selectivity. 90Zr(p-bar, p-bar'), E=175 MeV; calculated longitudinal, isovector transition potentials.
doi: 10.1103/PhysRevLett.56.700
1985BL22 Phys.Rev. C32, 2152 (1985) G.S.Blanpied, B.G.Ritchie, M.L.Barlett, G.W.Hoffmann, J.A.McGill, M.A.Franey, M.Gazzaly Elastic Scattering of 0.8 GeV Protons from the Non-Zero-Spin Nuclei 13C and 14N NUCLEAR REACTIONS 12,13C, 14N(p, p), (polarized p, p), E=0.8 GeV; measured σ(θ), analyzing power vs θ; deduced optical potential parameters.
doi: 10.1103/PhysRevC.32.2152
1984AU10 Phys.Rev. C30, 736 (1984) N.Auerbach, J.D.Bowman, M.A.Franey, W.G.Love Reply to '' Comment on ' (p, n) and (n, p) Reactions as Probes of Isovector Giant Monopole Resonances ' '' NUCLEAR REACTIONS 90Zr(p, n), E=120 MeV; calculated IAS, isovector monopole resonance excitation σ(θ=0°); deduced medium corrections role.
doi: 10.1103/PhysRevC.30.736
1984BL14 Phys.Rev. C30, 1233 (1984) G.S.Blanpied, G.A.Balchin, G.E.Langston, B.G.Ritchie, M.L.Barlett, G.W.Hoffmann, J.A.McGill, M.A.Franey, M.Gazzaly, B.H.Wildenthal Excitation of the Ground State Rotational Band in 20Ne by 0.8 GeV Protons NUCLEAR REACTIONS 20Ne(polarized p, p'), E=0.8 GeV; measured σ(θ), analyzing power vs θ, σ(Ep'); deduced potential parameters. 20Ne levels deduced β, B(λ). Coupled-channels calculation.
doi: 10.1103/PhysRevC.30.1233
1984BL17 Phys.Rev. C30, 1989 (1984) C.L.Blilie, D.Dehnhard, M.A.Franey, D.H.Gay, D.B.Holtkamp, S.J.Seestrom-Morris, P.J.Ellis, C.L.Morris, D.J.Millener Isospin Structure of Transitions in 17O from Inelastic Pion Scattering at 164 MeV NUCLEAR REACTIONS 16,17O(π+, π+'), (π-, π-'), E=164 MeV; measured σ(θ), σ(E(π)). 17O deduced M4, E2 transition strength distribution. Microscopic DWIA calculations.
doi: 10.1103/PhysRevC.30.1989
1984CL05 Phys.Rev. C30, 314 (1984) B.C.Clark, S.Hama, E.Sugarbaker, M.A.Franey, R.L.Mercer, L.Ray, G.W.Hoffmann, B.D.Serot Relativistic Description of (p, n) Reactions to the Isobaric Analog State NUCLEAR REACTIONS 90Zr(polarized p, p), (polarized p, n), E=160, 500 MeV; calculated σ(θ), analyzing power vs θ, spin rotation function vs θ; deduced proton-nucleus optical potential parameters. Lane model, relativistic generalization.
doi: 10.1103/PhysRevC.30.314
1984DE19 Phys.Rev. C30, 242 (1984) D.Dehnhard, D.H.Gay, C.L.Blilie, S.J.Seestrom-Morris, M.A.Franey, C.L.Morris, R.L.Boudrie, T.S.Bhatia, C.F.Moore, L.C.Bland, H.Ohnuma Excitation of the 1+ State in 48Ca(10.2 MeV) by Inelastic Scattering of π- and π+ NUCLEAR REACTIONS 48Ca(π+, π+'), (π-, π-'), E=116-180 MeV; measured σ(E(π)), σ(θ). 48Ca level deduced σ(π-)/σ(π+), isoscalar, isovector rescaling factor dependence. DWIA analysis.
doi: 10.1103/PhysRevC.30.242
1984DO15 Phys.Lett. 143B, 45 (1984) C.B.Dover, M.A.Franey, W.G.Love, M.E.Sainio, G.E.Walker Antinucleon-Nucleus Inelastic Scattering and the Spin Dependence of the N(bar)N Annihilation Potential NUCLEAR REACTIONS 12C(p-bar, p-bar'), E=175 MeV; calculated σ(θ), polarization; deduced nucleon-antinucleon annihilation potential.
doi: 10.1016/0370-2693(84)90801-3
1984HI10 Phys.Rev. C30, 1976 (1984) N.M.Hintz, M.A.Franey, M.M.Gazzaly, D.Cook, G.S.Kyle, D.Dehnhard, S.J.Seestrom-Morris, G.W.Hoffmann, M.Barlett, G.S.Blanpied, J.A.McGill, J.B.McClelland, R.L.Boudrie, F.Irom, G.Pauletta High Spin States in 28Si and 58Ni NUCLEAR REACTIONS 28Si, 58Ni(p, p'), E=333, 498, 800 MeV; measured σ(θ), σ(Ep). 28Si, 58Ni levels deduced transition densities. DWIA, other (p, p'), (e, e') data analysis.
doi: 10.1103/PhysRevC.30.1976
1984LO10 J.Phys.(Paris), Colloq.C4, 231 (1984); See 1984Lo20 Effective Interactions and the Excitation of Giant Resonances
1984LO20 J.Phys.(Paris), Colloq.C-4, 231 (1984) Effective Interactions and the Excitation of Giant Resonances NUCLEAR REACTIONS 12C(p, p'), E=120, 200, 398, 800 MeV; 208Pb(p, p'), E=135, 334, 800 MeV; 90Zr(p, p'), E=201 MeV; 90Zr(p, n), E=120 MeV; calculated σ(θ). Free nucleon-nucleon t-matrix.
1984SE12 Phys.Rev. C30, 270 (1984) S.J.Seestrom-Morris, M.A.Franey, D.Dehnhard, D.B.Holtkamp, R.L.Boudrie, J.F.Amann, G.C.Idzorek, C.A.Goulding 13C(p(pol), p')13C Reaction at T(p) = 547 MeV NUCLEAR REACTIONS 13C(polarized p, p'), E=547 MeV; measured σ(Ep'), σ(θ), analyzing power vs θ. DWIA analysis, shell model transition densities.
doi: 10.1103/PhysRevC.30.270
1983AU05 Phys.Rev. C28, 280 (1983) N.Auerbach, J.D.Bowman, M.A.Franey, W.G.Love (p, n) and (n, p) Reactions as Probes of Isovector Giant Monopole Resonances NUCLEAR REACTIONS 90Zr, 40Ca, 120Sn, 208Pb(p, n), E=120, 800 MeV; calculated σ(θ) for isovector giant monopole resonance excitation. DWIA, RPA based charge exchange transition densities.
doi: 10.1103/PhysRevC.28.280
1983GA09 Phys.Rev. C28, 294 (1983) M.M.Gazzaly, N.M.Hintz, M.A.Franey, J.Dubach, W.C.Haxton Neutron and Proton Transition Matrix Elements for 90Zr from a Microscopic Analysis of 0.8 GeV Proton Inelastic Scattering NUCLEAR REACTIONS 90Zr(p, p'), E=0.8 GeV; measured absolute σ(θ). 90Zr levels deduced core to total deformation parameter ratio, enhancement factors, neutron, proton matrix element ratios. DWIA, shell model transition densities.
doi: 10.1103/PhysRevC.28.294
1983SE15 Phys.Rev. C28, 1301 (1983) S.J.Seestrom-Morris, D.Dehnhard, M.A.Franey, C.L.Morris, R.L.Boudrie, H.A.Thiessen Analysis of Elastic and Inelastic Scattering of 162 MeV Pions from 13C by an Optical Potential and a Collective Model NUCLEAR REACTIONS 13C(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=162 MeV; measured σ(θ). 13C levels deduced neutron, proton B(λ) components. Optical, collective model analyses.
doi: 10.1103/PhysRevC.28.1301
1983SH18 Phys.Rev. C28, 717 (1983) V.Shkolnik, D.Dehnhard, M.A.Franey Elastic Scattering of 16O by 28Si NUCLEAR REACTIONS 28,29,30Si(16O, 16O), E=45-63 MeV; measured σ(θ) vs E; deduced optical model parameters, potential strength ambiguities, L-dependent potential resonances.
doi: 10.1103/PhysRevC.28.717
1982BL01 Phys.Rev. C25, 422 (1982) G.S.Blanpied, N.M.Hintz, G.S.Kyle, M.A.Franey, S.J.Seestrom-Morris, R.K.Owen, J.W.Palm, D.Dehnhard, M.L.Barlett, C.J.Harvey, G.W.Hoffmann, J.A.McGill, R.P.Liljestrand, L.Ray Elastic and Inelastic Scattering of 0.8 GeV Protons from 24Mg and 26Mg NUCLEAR REACTIONS 24,26Mg(p, p), (p, p'), E=0.8 GeV; measured σ(θ). 24,26Mg deduced deformation lengths, multipole moments. Optical model, DWBA, coupled-channels analyses, rotational model.
doi: 10.1103/PhysRevC.25.422
1982HA26 Phys.Rev. C25, 3035 (1982) M.Haji-Saeid, G.Igo, F.Irom, J.B.McClelland, G.Pauletta, C.A.Whitten, Jr., C.Glashausser, W.D.Cornelius, J.M.Moss, H.A.Thiessen, M.A.Franey, M.Gazzaly, W.G.Love Excitation of Low Spin States in the 12C(p, p') Reaction at 800 MeV NUCLEAR REACTIONS 12C(p, p'), E=0.8 GeV; measured σ(θ). DWIA, nucleon-nucleon t-matrix, shell model, electron scattering transition densities.
doi: 10.1103/PhysRevC.25.3035
1982SE04 Phys.Rev. C26, 594 (1982) S.J.Seestrom-Morris, D.Dehnhard, M.A.Franey, G.S.Kyle, C.L.Morris, R.L.Boudrie, J.Piffaretti, H.A.Thiessen Inelastic Pion Scattering from 13C at 162 MeV NUCLEAR REACTIONS 13C(π+, π+'), (π-, π-'), E=162 MeV; measured σ(θ). 13C levels deduced L. Microscopic DWIA analysis, shell model wave functions.
doi: 10.1103/PhysRevC.26.594
1982SE12 Phys.Rev. C26, 2131 (1982) S.J.Seestrom-Morris, J.M.Moss, J.B.McClelland, W.D.Cornelius, T.A.Carey, N.M.Hintz, M.Gazzaly, M.A.Franey, S.Nanda, B.Aas Spin-Flip Probability in 12C(p(pol), p'(pol))12C at 397 MeV NUCLEAR REACTIONS 12C(polarized p, p'), E=397 MeV; measured spin-flip probability. DWBA, effective interaction, Cohen-Kurath wave functions.
doi: 10.1103/PhysRevC.26.2131
1981FR02 Phys.Rev. C23, 787 (1981) Coulomb and Nuclear Inelastic Excitations and the Optical Potential for Heavy Ions NUCLEAR REACTIONS 152Sm(16O, 16O), E=72 MeV; 40Ca(13C, 13C'), E=68 MeV; analyzed σ(θ); deduced optical potential. Coupled-channels analysis.
doi: 10.1103/PhysRevC.23.787
1981LO11 Phys.Rev. C24, 1073 (1981); Erratum Phys.Rev. C27, 438 (1983) Effective Nucleon-Nucleon Interaction for Scattering at Intermediate Energies NUCLEAR REACTIONS 12C(p, p'), E=120, 402, 800 MeV; 90Zr(p, n), E=120 MeV; 58Ni(p, p'), E=800 MeV; calculated σ(θ). On-shell nucleon-nucleon t-matrix, energy-dependent Yukawa representation.
doi: 10.1103/PhysRevC.24.1073
1980BA30 Phys.Rev. C22, 1168 (1980) M.L.Bartlett, J.A.McGill, L.Ray, M.M.Bartlett, G.W.Hoffmann, N.M.Hintz, G.S.Kyle, M.A.Franey, G.Blanpied Proton Scattering from 154Sm and 176Yb at 0.8 GeV NUCLEAR REACTIONS 154Sm, 176Yb(p, p), (p, p'), E=0.8 GeV; measured σ(θ); deduced optical model parameters. 154Sm, 176Yb levels deduced deformation lengths. DWBA, coupled channel analysis, rotational model. Enriched targets.
doi: 10.1103/PhysRevC.22.1168
1980LI11 Nucl.Phys. A342, 165 (1980) J.S.Lilley, M.A.Franey, D.H.Feng Alpha Inelastic Scattering by 208Pb Near the Coulomb Barrier NUCLEAR REACTIONS 208Pb(α, α), (α, α'), E=23.5 MeV; measured σ(θ); deduced nuclear matter surface distribution, transition density, potential parameters. 208Pb level deduced B(E3), β. Deformed potential model, folding model.
doi: 10.1016/0375-9474(80)90512-6
1979DE34 Phys.Rev.Lett. 43, 1091 (1979) D.Dehnhard, S.J.Tripp, M.A.Franey, G.S.Kyle, C.L.Morris, R.L.Boudrie, J.Piffaretti, H.A.Thiessen Pure Neutron and Pure Proton Transitions in Inelastic Scattering of Pions by 13C NUCLEAR REACTIONS 13C(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=162 MeV; measured σ(θ). 13C deduced pure n, p transitions. Shell-model, weak coupling-model configurations.
doi: 10.1103/PhysRevLett.43.1091
1979FR01 Phys.Lett. 81B, 132 (1979) M.A.Franey, V.Shkolnik, D.Dehnhard Elastic Transfer in the Scattering of 16O by 28Si NUCLEAR REACTIONS 28Si(16O, 16O), E=30-60 MeV; measured σ(E, θ); deduced interference of potential scattering, elastic transfer amplitude, Sα.
doi: 10.1016/0370-2693(79)90505-7
1979FR07 Nucl.Phys. A324, 193 (1979) M.A.Franey, J.S.Lilley, W.R.Phillips Sub-Coulomb Transfer Reactions on 208Pb with Carbon and Oxygen Projectiles NUCLEAR REACTIONS 208Pb(13C, 12C), (13C, 14C), E=52.07, 54.07 MeV; 208Pb(12C, 13C), E=54.07 MeV; 208Pb(16O, 17O), E=69.05, 70.95, 72.95 MeV; 208Pb(17O, 16O), (17O, 18O), (18O, 17O), (18O, 19O), E=66.95 MeV; 12C(17O, 16O), E=12.6, 13.1 MeV; measured σ(θ). 208Pb deduced single-particle orbitals, rms radii, n-excess distribution.
doi: 10.1016/0375-9474(79)90088-5
1978DE09 Phys.Rev.Lett. 40, 1549 (1978) D.Dehnhard, V.Shkolnik, M.A.Franey Parity Dependence of the Heavy-Ion Optical Potential NUCLEAR REACTIONS 28Si(16O, 16O), E=30-65 MeV; calculated σ(E, θ).
doi: 10.1103/PhysRevLett.40.1549
1978FR19 Phys.Rev.Lett. 41, 837 (1978) M.A.Franey, B.F.Bayman, J.S.Lilley, W.R.Phillips Two-Neutron-Transfer Reaction Mechanism with Heavy Ions at Sub-Coulomb Energies NUCLEAR REACTIONS 206Pb(18O, 16O), 208Pb(16O, 18O), E=69, 71, 73 MeV; measured σ.
doi: 10.1103/PhysRevLett.41.837
1978SH02 Phys.Lett. 74B, 195 (1978) V.Shkolnik, D.Dehnhard, S.Kubono, M.A.Franey, S.Tripp Potential Description of Elastic Scattering of 28Si + 16O between 45 and 63 MeV NUCLEAR REACTIONS 28Si(16O, 16O), E=45-63 MeV; measured σ(E, θ).
doi: 10.1016/0370-2693(78)90551-8
1976DE25 Phys.Rev.Lett. 37, 481 (1976) R.M.DeVries, J.S.Lilley, M.A.Franey Absolute Reduced α Widths in the Lead Region NUCLEAR REACTIONS 208Pb, 208Bi(α, α), (α, X); analyzed data; deduced α-nucleus potentials. 212,211,210,208Po, 213At deduced reduced α-widths.
doi: 10.1103/PhysRevLett.37.481
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