NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = F.Osterfeld Found 54 matches. 1998MO35 Acta Phys.Pol. B29, 3087 (1998) The ΔN-Interaction in Hadronic Reactions on a Deuteron Target NUCLEAR REACTIONS 2H(π+, p), E=142 MeV; 2H(p, nX), (p, nπ+), E=789 MeV; analyzed σ(θ); deduced Δ excitation role.
1997KO08 Phys.Rev. C55, 1819 (1997) B.Korfgen, P.Oltmanns, F.Osterfeld, T.Udagawa Damping Mechanisms of the Δ Resonance in Nuclei NUCLEAR REACTIONS 12C(π+, π+p), E=245 MeV; analyzed σ(Ep, θp, θ(π)). 12C(π+, 2p), E=165 MeV; analyzed σ(θ(p1), θ(p2)), σ(θ(p1), θ(p2), E1). 12C(3He, tpπ+), (3He, t2p), E=2 GeV; analyzed σ(θ) vs ω; deduced Δ(1232) resonance damping mechanisms related features. Δ-hole model.
doi: 10.1103/PhysRevC.55.1819
1997MO21 Phys.Rev. C56, 2014 (1997) Δ(1232)-Nucleon Interaction in the 2H(p, n) Charge-Exchange Reaction NUCLEAR REACTIONS 2H(p, X), E=790 MeV; analyzed Δ++ production associated σ(En, θ); deduced Δ-N interaction effects. Coupled-channels approach.
doi: 10.1103/PhysRevC.56.2014
1996OS02 Nucl.Phys. A599, 129c (1996) Nucleon Resonances in the Medium NUCLEAR REACTIONS 12C(p, n), E=800 MeV; compiled, reviewed data, analyses. 12C(3He, tπ+), E=2 GeV; 12C(π-, π-), E=120 MeV; 12C(γ, π0), E not given; analyzed σ(θ), other data; deduced medium role on Δ dynamics.
doi: 10.1016/0375-9474(96)00055-3
1996PR03 Phys.Rev.Lett. 76, 4488 (1996) D.L.Prout, S.DeLucia, D.Cooper, B.Luther, E.Sugarbaker, T.N.Taddeucci, L.J.Rybarcyk, J.Rapaport, B.K.Park, C.D.Goodman, G.Edwards, C.Glashausser, T.Sams, T.Udagawa, F.Osterfeld Spin Decomposition of the Δ Resonance Cross Section using the 12C(p(pol), n(pol)) Reaction at E(p) = 795 MeV NUCLEAR REACTIONS 12C(polarized p, n), E=795 MeV; measured polarization observables; deduced spin-longitudinal, spin-transverse, spin-independent partial σ, Δ-production related features.
doi: 10.1103/PhysRevLett.76.4488
1994KO23 Phys.Rev. C50, 1637 (1994) B.Korfgen, F.Osterfeld, T.Udagawa Longitudinal and Transverse Spin Response of 12C in the Δ Resonance Region NUCLEAR REACTIONS 12C(π-, π-), E=120-280 MeV; 12C(γ, π0), E at ≈ 175-450 MeV/c; calculated σ(θ), σ(E). 12C(3He, tπ+), E=2 GeV; calculated σ(θ). Isobar-hole model.
doi: 10.1103/PhysRevC.50.1637
1994OS02 Nucl.Phys. A577, 237c (1994) F.Osterfeld, B.Korfgen, P.Oltmanns, T.Udagawa Δ Excitations in Nuclei and Their Decay Properties NUCLEAR REACTIONS 12C(3He, t), (3He, 2pt), E=2 GeV; analyzed σ(θ) vs energy transfer. 12C(3He, tπ+), E=2 GeV; 12C(π-, π-), E=120 MeV; 12C(γ, π0), E at 235 MeV/c; analyzed σ(θ(π)). Isobar-hole model.
doi: 10.1016/0375-9474(94)90862-1
1994UD01 Phys.Rev. C49, 3162 (1994) T.Udagawa, P.Oltmanns, F.Osterfeld, S.W.Hong Δ Excitations in Nuclei and Their Decay Properties NUCLEAR REACTIONS 1H(p, nX), 12C(p, n), E=0.8 GeV; 1H(3He, tX), 12C(3He, t), E=2 GeV; calculated σ(θ, En), σ(θ, Et). 1H(polarized p, nX), E=0.8 GeV; calculated spin transfer coefficient. Formalism for Δ excitation.
doi: 10.1103/PhysRevC.49.3162
1993OL01 Phys.Lett. 299B, 194 (1993) P.Oltmanns, F.Osterfeld, T.Udagawa Coherent Pion Production in Intermediate Energy Charge-Exchange Reactions NUCLEAR REACTIONS 12C(p, nX), E=800, 822 MeV; calculated inclusive, exclusive, coherent pion production, σ(θ, E); deduced unique signature on nuclear pionic mode.
doi: 10.1016/0370-2693(93)90246-E
1993OL06 Acta Phys.Pol. B24, 1609 (1993) P.Oltmanns, B.Korfgen, F.Osterfeld, T.Udagawa Coherent Pion Production in the Delta Resonance Region NUCLEAR REACTIONS 12C(3He, tX), E=2 GeV; 12C(γ, π0), E=235, 291 MeV; compiled, reviewed data, model analyses; deduced coherent pion production features.
1993OS02 Phys.Scr. 48, 95 (1993) F.Osterfeld, B.Korfgen, P.Oltmanns, T.Udagawa Δ Excitations in Nuclei and the Coherent Pion Decay NUCLEAR REACTIONS 12C(γ, X), (π, X), E=200-400 MeV; calculated total σ(E). 1H(polarized p, X), E=800 MeV; calculated spin transfer coefficients vs energy transfer for neutron. 12C(polarized p, n), E=800, 822 MeV; calculated σ(θ), spin transfer coefficient vs energy transfer. Isobar-hole model.
doi: 10.1088/0031-8949/48/1/016
1993WY01 Nucl.Phys. A553, 599c (1993) P.Wyborny, K.Holinde, F.Osterfeld, J.Speth Meson Exchange K+-N Interaction and K+-Nucleus Cross Sections NUCLEAR REACTIONS 2H, 12C(K+, X), E at ≈ 0.45-0.8 GeV/c; calculated σ(ratio). Meson exchange model, coupled-channel treatment.
doi: 10.1016/0375-9474(93)90666-L
1992OS03 Phys.Rev. C45, 2854 (1992) F.Osterfeld, N.Anantaraman, S.M.Austin, J.A.Carr, J.S.Winfield Heavy-Ion Charge-Exchange Reactions and the Measurement of Gamow-Teller Strength NUCLEAR REACTIONS 26Mg(12C, 12B), E=70 MeV/nucleon; analyzed σ(θ). 26Al deduced Gamow-Teller strength. Strong absorption model, heavy-ion induced charge-exchange reactions.
doi: 10.1103/PhysRevC.45.2854
1991OS02 Nucl.Phys. A527, 405c (1991) F.Osterfeld, S.-W.Hong, T.Udagawa Spin-Isospin Response of Nuclei in the Δ Resonance Region NUCLEAR REACTIONS 12C(p, n), E=800 MeV; 12C(3He, t), E=2 GeV; calculated ejectile spectra, σ(θ, E); deduced isobar peak shift features.
doi: 10.1016/0375-9474(91)90130-X
1990UD01 Phys.Lett. 245B, 1 (1990) T.Udagawa, S.-W.Hong, F.Osterfeld Δ Excitations in Nuclei NUCLEAR REACTIONS 1H, 12C(p, nX), E=0.8 GeV; 1H, 12C(3He, tX), E=2 GeV; calculated σ(θ, E); deduced Δ excitations role. TDA, DWIA.
doi: 10.1016/0370-2693(90)90154-X
1989AU02 Phys.Lett. 219B, 184 (1989) N.Auerbach, F.Osterfeld, T.Udagawa The Spin Isovector Monopole Strength and the (3He, t) Reaction NUCLEAR REACTIONS 90Zr(p, n), E=200 MeV; 90Zr(3He, t), E=600 MeV; calculated σ(θ), energy integrated σ; deduced spin-flip isovector monopole resonance role.
doi: 10.1016/0370-2693(89)90374-2
1989CH02 Phys.Rev. C39, 694 (1989) Theoretical Analysis of 208Pb(p, n) Spectra at 200 MeV NUCLEAR REACTIONS 208Pb(p, n), E=200 MeV; analyzed forward angle neutron spectra. 208Bi deduced Gamow-Teller transition strength. RPA, DWBA analyses.
doi: 10.1103/PhysRevC.39.694
1989MA14 Phys.Rev. C39, 1215 (1989) Angular Momentum Dependence of the Absorptive Optical Potential NUCLEAR REACTIONS 40Ca(p, p), E not given; calculated potential parameters; deduced nonlocality projectile l dependence.
doi: 10.1103/PhysRevC.39.1215
1988UD03 Nucl.Phys. A482, 391c (1988) Delta Excitations in Nuclei NUCLEAR REACTIONS 40Ca, 12C(p, n), E=800 MeV; 40Ca, 12C(3He, t), E=2 GeV; calculated σ(θ, En), σ(θ, Et). Isobar-hole model.
doi: 10.1016/0375-9474(88)90599-4
1987DR09 Phys.Lett. 189B, 271 (1987) S.Drozdz, F.Osterfeld, J.Speth, J.Wambach Damping of the Giant Spin-Flip Dipole and Spin-Flip Quadrupole Charge Exchange Modes in 90Zr NUCLEAR STRUCTURE 90Zr; calculated Gamow-Teller strength distribution function. Second random-phase approximation.
doi: 10.1016/0370-2693(87)91430-4
1987SC04 Phys.Lett. 183B, 243 (1987) A.Schulte, T.Udagawa, F.Osterfeld, D.Cha Theoretical Study of the 90Zr(3He, t) and 90Zr(p, n) Reactions at E = 200 MeV per Nucleon NUCLEAR REACTIONS 90Zr(3He, t), (p, n), E=200 MeV/nucleon; calculated σ(θ), σ(θt, Et), σ(θn, En). 90Nb deduced high L mode excitation mechanism. DWIA, random phase approximation.
doi: 10.1016/0370-2693(87)90956-7
1987UD02 Nucl.Phys. A474, 131 (1987) T.Udagawa, A.Schulte, F.Osterfeld Antisymmetric Distorted Wave Impulse Approximation Calculations for Composite Particle Scattering NUCLEAR REACTIONS 90Zr(3He, t), E=600 MeV; calculated σ(θ); deduced σ(E). Microscopic DWIA.
doi: 10.1016/0375-9474(87)90197-7
1987YA10 Phys.Lett. 192B, 26 (1987) Theoretical Investigation of the 48Ca(n, p)48K and 48Ca(p, n)48Sc Reactions at E = 200 MeV NUCLEAR REACTIONS 48Ca(n, p), (p, n), E=200 MeV; calculated σ(θ), σ(Ep, θp), σ(En, θn). 48Sc, 48K deduced Gamow-Teller transition sum rule validity.
doi: 10.1016/0370-2693(87)91135-X
1986WE04 Z.Phys. A323, 485 (1986) C.Wesselborg, K.Schiffer, K.O.Zell, P.von Brentano, D.Bohle, A.Richter, G.P.A.Berg, B.Brinkmoller, J.G.M.Romer, F.Osterfeld, M.Yabe Search for the New M1 Mode in 156Gd by Inelastic Proton Scattering at Low Incident Energy NUCLEAR REACTIONS 156Gd(p, p'), E=24.7 MeV; measured σ(θ), σ(Ep'). 156Gd deduced 1+ excitation σ upper limit, convection current dependent M1 mode.
1986YA09 Phys.Lett. 178B, 5 (1986) Microscopic Analysis of 90Zr(p(pol), p'(pol))-Spin-Flip Spectra at E = 319 MeV NUCLEAR REACTIONS 90Zr(polarized p, p'), E=319 MeV; calculated σ(θ), spin-flip σ(θp, Ep). DWIA.
doi: 10.1016/0370-2693(86)90460-0
1985LE15 Phys.Rev. C32, 789 (1985) Microscopic Approach to the Alpha-Particle-Nucleus Optical Potential NUCLEAR STRUCTURE 44Ti; calculated levels, rotational bands. Fish-bone model, α+40Ca structure. NUCLEAR REACTIONS 40Ca(α, α), E=26.1, 31, 36.1 MeV; calculated σ(θ). Microscopic α-nucleus potential.
doi: 10.1103/PhysRevC.32.789
1985OS01 Phys.Rev. C31, 372 (1985) Microscopic Analysis of Complete 90Zr(p, n) Spectra Including the Δ Isobar Effect NUCLEAR REACTIONS 90Zr(p, n), E=200 MeV; calculated σ(E, θ); deduced isobar-hole admixture role. 42Sc deduced spin-isospin strength distribution function. Microscopic model.
doi: 10.1103/PhysRevC.31.372
1985OS04 Phys.Rev. C32, 108 (1985) Microscopic Calculation of the Imaginary Lane Isospin Potential W1 NUCLEAR REACTIONS 48Ca(p, n), E=25 MeV; calculated charge-exchange imaginary potential, σ(θ). Microscopic calculation.
doi: 10.1103/PhysRevC.32.108
1984DE03 Phys.Rev. C29, 1075 (1984) H.Dermawan, F.Osterfeld, V.A.Madsen Microscopic Calculation of the Imaginary Optical Potential for 208Pb(p, p) at 14 MeV NUCLEAR REACTIONS 208Pb(p, p), E=14 MeV; calculated σ(θ). Microscopic second-order imaginary potential, RPA transition densities.
doi: 10.1103/PhysRevC.29.1075
1984OS02 Phys.Lett. 138B, 23 (1984) Microscopic Background Calculations for the 90Zr(p, n)-Reaction at E = 200 MeV NUCLEAR REACTIONS 90Zr(p, n), E=200 MeV; calculated σ(θn, En). 90Nb deduced giant resonance, missing Gamow-Teller transition strength distribution.
doi: 10.1016/0370-2693(84)91864-1
1984OS04 J.Phys.(Paris), Colloq.C4, 13 (1984); See 1984Os07 Microscopic Calculations of the Background below Giant Resonances
1984OS07 J.Phys.(Paris), Colloq.C-4, 13 (1984) Microscopic Calculations of the Background below Giant Resonances NUCLEAR REACTIONS 40Ca(p, n), E=160 MeV; 90Zr(p, n), E=200 MeV; calculated σ(En, θn). Doorway model.
1983DE12 Phys.Rev. C27, 1474 (1983) H.Dermawan, F.Osterfeld, V.A.Madsen Cross Section Calculations for Nucleon-40Ca and α-40Ca Elastic Scattering from Microscopic Nonlocal Optical Potentials NUCLEAR REACTIONS 40Ca(p, p), E=17.7, 25 MeV; 40Ca(n, n), E=17.7 MeV; 40Ca(α, α), E=31 MeV; calculated σ(θ), σ(elastic). Microscopic optical model, nonlocal potentials.
doi: 10.1103/PhysRevC.27.1474
1982BE14 Phys.Rev. C25, 2100 (1982) G.P.A.Berg, W.Hurlimann, I.Katayama, S.A.Martin, J.Meissburger, J.Romer, B.Styczen, F.Osterfeld, G.Gaul, R.Santo, G.Sondermann Excitation of the 10.212 MeV 1+ State in 48Ca(p, p') at E(p) = 44.4 MeV NUCLEAR REACTIONS 48Ca(p, p'), E=44.4 MeV; measured σ(θ), proton momentum spectra. High resolution magnetic spectrometer. Microscopic DWBA, RPA wave functions.
doi: 10.1103/PhysRevC.25.2100
1982DE04 Phys.Rev. C25, 180 (1982) H.Dermawan, F.Osterfeld, V.A.Madsen Nuclear Structure Approach to the Calculation of the Imaginary Alpha-Nucleus Optical Potential NUCLEAR REACTIONS 40Ca(α, α), E=31-100 MeV; calculated σ(θ), imaginary α-nucleus potential. RPA.
doi: 10.1103/PhysRevC.25.180
1982OS03 Phys.Rev.Lett. 49, 11 (1982) F.Osterfeld, S.Krewald, J.Speth, T.Suzuki Effect of the Δ(1232) Isobar in 48Ca(p, n) Cross Sections NUCLEAR REACTIONS 48Ca(p, n), E=160 MeV; analyzed σ(θ); deduced isobar effects. 48Sc levels deduced isobar quenching dependence on multipolarity. Microscopic model.
doi: 10.1103/PhysRevLett.49.11
1982OS04 Phys.Rev. C26, 762 (1982) Microscopic Background Calculations for (p, n) Reactions at Intermediate Energies NUCLEAR REACTIONS 40,48Ca(p, n), E=160 MeV; calculated σ(θ, En); deduced Gamow-Teller strength in background. 48Sc deduced strong 3+ resonance excitation. Microscopic model, DWIA approach.
doi: 10.1103/PhysRevC.26.762
1981KE01 Phys.Rev.Lett. 46, 103 (1981) S.Krewald, F.Osterfeld, J.Speth, G.E.Brown Nuclear-Structure Effects Connected with Charge-Exchange Resonances NUCLEAR STRUCTURE 208Pb, 208Bi; calculated GDR, IAR, Gamow-Teller resonance energies. Generalized Landau-Migdal interaction, dynamical RPA, collective effects. NUCLEAR REACTIONS 208Pb(p, n), E=120 MeV; calculated σ(θ). 208Bi deduced nuclear structure effects associated with Gamow-Teller resonance, IAS. Generalized Landau-Migdal interaction, dynamical RPA, collective effects.
doi: 10.1103/PhysRevLett.46.103
1981OS01 Phys.Rev. C23, 179 (1981) F.Osterfeld, J.Wambach, V.A.Madsen Antisymmetrized, Microscopic Calculation for the 40Ca(n, n) Optical Potential NUCLEAR REACTIONS 40Ca(n, n), E=30 MeV; calculated σ(θ); deduced collective, intermediate charge-exchange state effects. Antisymmetrized, microscopic optical potential.
doi: 10.1103/PhysRevC.23.179
1981OS03 Phys.Lett. 99B, 75 (1981) F.Osterfeld, T.Suzuki, J.Speth No Evidence for Precritical Phenomena of Pion Condensation in A=48 Nuclei NUCLEAR REACTIONS 48Ca(e, e'), E=250 MeV; calculated from factors; 48Ca(p, p'), E=160 MeV; 48Ca(p, n), E=160 MeV; calculated σ(θ); 48Ca, 48Sc deduced no pion condensation phenomena for 1+ state excitation. RPA, variable Landau-Migdal force parameter.
doi: 10.1016/0370-2693(81)90953-9
1981OS09 Phys.Lett. 105B, 257 (1981) F.Osterfeld, S.Krewald, H.Dermawan, J.Speth Pionic ΔL = 1 Charge-Exchange Modes in Heavy Mass Nuclei NUCLEAR REACTIONS 208Pb(p, n), E=45, 49, 160 MeV; calculated σ(θ), σ(θ, En). 208Bi deduced charge exchange resonance character. Antisymmetrized DWBA, effective interaction, RPA. NUCLEAR STRUCTURE 208Bi; calculated collective spin-flip, nonspin-flip charge exchange mode energies. RPA.
doi: 10.1016/0370-2693(81)90883-2
1981OS10 Phys.Rev. C24, 2468 (1981) Nuclear Structure Approach to the Coulomb Correction of the Imaginary Nucleon-Nucleus Optical Potential NUCLEAR REACTIONS 40Ca(p, p), (n, n), E=17.7, 25 MeV; calculated imaginary optical potential. RPA transition densities, inelastic, charge-exchange intermediate states.
doi: 10.1103/PhysRevC.24.2468
1981SU04 Phys.Lett. 100B, 443 (1981) T.Suzuki, F.Osterfeld, J.Speth Critical Analysis of a Precritical Phenomenon in Connection with Pion Condensation NUCLEAR REACTIONS 12C(p, p'), E=122, 156 MeV; calculated σ(θ); 12C(e, e'), E=57.7 MeV; calculated form factors, transition densities; deduced precritical phenomenon redundancy. RPA.
doi: 10.1016/0370-2693(81)90601-8
1980KR08 Phys.Lett. 93B, 218 (1980) A Comment on the Isovector Dipole and Gamow-Teller Transitions in 90Zr NUCLEAR REACTIONS 90Zr(3He, t), E=80, 130 MeV; 90Zr(p, n), E not given; analyzed data. 93Nb resonance deduced isospin, dipole character. Shell model.
doi: 10.1016/0370-2693(80)90498-0
1979OS03 Nucl.Phys. A318, 45 (1979) F.Osterfeld, J.Wambach, H.Lenske, J.Speth Investigation of the Hadronic Transition Operator for Inelastic Proton Scattering NUCLEAR REACTIONS 208Pb(p, p'), E=61.5 MeV; calculated σ(θ), B(E3). Local part of hadronic transition operator.
doi: 10.1016/0375-9474(79)90468-8
1979WA09 Nucl.Phys. A324, 77 (1979) J.Wambach, F.Osterfeld, J.Speth, V.A.Madsen Theoretical Investigation of Giant Resonances by Inelastic Proton Scattering NUCLEAR REACTIONS 16O(p, p'), E=45 MeV; 40Ca(p, p'), E=156 MeV; 208Pb(p, p'), E=60, 156 MeV; calculated σ(θ) in giant resonance region. Antisymmetrized microscopic DWBA, RPA wave functions deduced breathing mode character of giant resonance.
doi: 10.1016/0375-9474(79)90079-4
1978BA11 Phys.Rev. C17, 819 (1978) G.Baur, V.A.Madsen, F.Osterfeld Microscopic Theory of the Imaginary Inelastic Transition Form Factor NUCLEAR REACTIONS 40Ca(n, n'), E=30 MeV; calculated form factor.
doi: 10.1103/PhysRevC.17.819
1978HE03 Z.Phys. A284, 413 (1978) E.F.Hefter, H.V.Geramb, F.Osterfeld, T.Udagawa Two-Step Processes in Inelastic Proton Scattering NUCLEAR REACTIONS 16O, 40Ca(p, p'), 16O(p, d), E=25-46 MeV; calculated σ(θ). Reaction mechanism study.
doi: 10.1007/BF01422110
1977OS01 Nucl.Phys. A278, 1 (1977) F.Osterfeld, T.Udagawa, H.H.Wolter Effects of Nonorthogonality Corrections in Two-Step Processes in (τ, t) Reactions NUCLEAR REACTIONS 48Ca(3He, t), E=18, 22, 23, 30.2 MeV; calculated σ(Et, θ).
doi: 10.1016/0375-9474(77)90181-6
1977OS02 Phys.Lett. 68B, 319 (1977) F.Osterfeld, V.Hnizdo, C.Toepffer Is the Difference between 12C-20Ne and 16O-16O Scattering Due to Entrance Channel Effects (Question) NUCLEAR REACTIONS 20Ne(12C, 12C); calculated σ(θ).
doi: 10.1016/0370-2693(77)90484-1
1976CA30 Nucl.Phys. A273, 523 (1976) J.Carter, R.G.Clarkson, V.Hnizdo, R.J.Keddy, D.W.Mingay, F.Osterfeld, J.P.F.Sellschop Elastic and Inelastic Scattering of 16O and 12C by 24Mg Near the Coulomb Barrier NUCLEAR REACTIONS 24Mg(16O, 16O), E=28, 29, 30, 33 MeV; 24Mg(12C, 12C), E=21, 24 MeV; measured σ(θ) for ground state, first 2+ in 24Mg; deduced optical model potentials. DWBA, ICC analysis. Enriched target.
doi: 10.1016/0375-9474(76)90608-4
1976OS02 Phys.Lett. 60B, 253 (1976) Investigation of Direct and Two-Step Mechanism in the 48Ca(6Li, 6He)48Sc Reaction NUCLEAR REACTIONS 48Ca(6Li, 6He), E=34 MeV; calculated σ(E(6He), θ); deduced reaction mechanism.
doi: 10.1016/0370-2693(76)90293-8
1975FA02 Nucl.Phys. A245, 466 (1975) A.Faessler, F.Grummer, F.Krmpotic, F.Osterfeld, A.Plastino Two-Nucleon Transfer Processes in the Lead Region NUCLEAR REACTIONS 206,208Pb(t, p), 208,210Pb(p, t), E=20 MeV; 208Pb, 204Hg(3He, n), E=28 MeV; calculated σ.
doi: 10.1016/0375-9474(75)90622-3
1974GA17 Nucl.Phys. A222, 579 (1974) C.Gaarde, T.Kammuri, F.Osterfeld The (6Li, 6He) Spin-Isospin-Flip Reaction NUCLEAR REACTIONS 48Ca(6Li, 6He), E=34 MeV; measured nothing, calculated σ(E(6He), θ). 48Sc levels deduced wavefunctions.
doi: 10.1016/0375-9474(74)90340-6
Back to query form |