NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = R.R.Borchers Found 29 matches. 1979GR06 Phys.Rev. C19, 2127 (1979) S.M.Grimes, R.C.Haight, K.R.Alvar, H.H.Barschall, R.R.Borchers Charged-Particle Emission in Reactions of 15-MeV Neutrons with Isotopes of Chromium, Iron, Nickel, and Copper NUCLEAR REACTIONS 50,52Cr, Cr, 54,56Fe, Fe, 58,60Ni, Ni, 63,65Cu(n, p), (n, d), (n, α), E=14.8 MeV; measured σ(Ep, θ), σ(Ed, θ), σ(Eα, θ); deduced reaction mechanism. Enriched, natural targets. Hauser-Feshbach analysis.
doi: 10.1103/PhysRevC.19.2127
1974RO40 Nucl.Phys. A236, 165 (1974) W.M.Roney, D.W.Gebbie, R.R.Borchers Gyromagnetic Ratios of Excited States in 123,125Te NUCLEAR REACTIONS 123,125Te(16O, 16O'γ), E=33 MeV; measured 16O'γ(θ, H). 123,125Te levels deduced B(E2), T1/2, g, γ-mixing.
doi: 10.1016/0375-9474(74)90226-7
1973KA17 Nucl.Phys. A206, 558 (1973) R.Kalish, B.Herskind, R.R.Borchers, G.M.Heestand The Gyromagnetic Ratio of the 208 keV 3/2- State of 199Hg NUCLEAR REACTIONS 199Hg(16O, 16O'γ), E=25, 33 MeV; measured 16O, γ(θ, H). 199Hg levels deduced g. IMPAC method.
doi: 10.1016/0375-9474(73)90085-7
1972KU10 Nucl.Phys. A186, 513 (1972) H.W.Kugel, R.R.Borchers, R.Kalish Magnetic Moment Measurements of the First (2+) and Second (4+) States of Even Nd and Sm Nuclei NUCLEAR REACTIONS 144,146,148,150Nd, 148,150,152,154Sm(16O, 16O'γ), E=35 MeV; measured γγ(θ, H) in polarized Fe; deduced hyperfine field. 144,146,148,150Nd, 148,150,152,154Sm levels deduced g. Impact.
doi: 10.1016/0375-9474(72)90981-5
1971KA03 Nucl.Phys. A161, 637 (1971) R.Kalish, R.R.Borchers, H.W.Kugel Revised Level Scheme of 199Hg Following Coulomb Excitation NUCLEAR REACTIONS 199Hg(16O, 16O'γ), E=25, 33 MeV; measured σ(E(16O'), Eγ, θ(γ)), 16O'γγ-coin. 199Hg deduced levels branching ratios B(E2), J, π, , γ-mixing. 201Hg(16O, 16O'γ), E=33 MeV; measured σ(E(16O'), Eγ). Enriched target.
doi: 10.1016/0375-9474(71)90392-7
1971KU09 Nucl.Phys. A167, 193 (1971) H.W.Kugel, R.Kalish, R.R.Borchers Precession Measurements of the 545 keV (6+) Rotational State of 154Sm NUCLEAR REACTIONS 154Sm(16O, 16O'γ), E=52 MeV; measured σ(E(16O'), Eγ, θ(γ)), (16O)γ(θ, H) in Cu, polarized Fe; deduced magnetic hyperfine fields. 154Sm levels deduced g ratios. IMPACT.
doi: 10.1016/0375-9474(71)90592-6
1971RA22 Phys.Rev.Lett. 27, 603 (1971) W.L.Randolph, Jr., R.R.Borchers, R.Michaelsen, D.W.Haag, W.Ribbe Magnetic Moments of the 7/2- Mirror States in 37Ar and 37K NUCLEAR REACTIONS 37Cl(p, nγ), E not given; 40Ca(p, αγ), E=13 MeV; measured pγ(θ, H, t), αγ(θ, H, t). 37Ar, 37K levels deduced T1/2, μ.
doi: 10.1103/PhysRevLett.27.603
1970KA09 Nucl.Phys. A147, 161 (1970); R.R.Borchers - Priv.Comm. (May 1972) R.Kalish, R.R.Borchers, H.W.Kugel Electromagnetic Properties of the First 2+ States of the Even Hg Isotopes NUCLEAR REACTIONS 198,200,202,204Hg(16O, 16O'γ), E = 33-38 MeV; measured σ(E(16O'), Eγ), γγ(θ, H). 198,200,202,204Hg levels deduced B(E2), T1/2, g.
doi: 10.1016/0375-9474(70)90518-X
1970KU19 Phys.Lett. 32B, 463 (1970) H.W.Kugel, T.Polga, R.Kalish, R.R.Borchers Static and Transient Hyperfine Magnetic Fields at Ba Isotopes Recoiled In Iron NUCLEAR REACTIONS 130,132,134,136Ba(16O, 16O'γ); measured γ(θ, H, t); deduced hyperfine fields.
doi: 10.1016/0370-2693(70)90384-9
1969HE11 Nucl.Phys. A133, 310 (1969); R.R.Borchers - Priv.Comm. (May 1972) G.M.Heestand, R.R.Borchers, B.Herskind, L.Grodzins, R.Kalish, D.E.Murnick g-Factors for 2+ States of Doubly Even Nuclei (Ge, Se, Mo, Ru, Pd, Cd and Te) NUCLEAR REACTIONS 70,72,74,76Ge, 76,78,80,82Se, 98,100Mo, 99,100,102,104Ru, 104,106,108,110Pd, 110,112,114,116Cd, 120,122,124,126,128,130Te(16O, 16O'γ); measured γγ(θ, H) from recoil implantation. 70,72,74,76Ge, 76,78,80,82Se, 98,100Mo, 99,100,102,104Ru, 104,106,108,110Pd, 110,112,114,116Cd, 120,122,124,126,128,130Te deduced g for first 2+ state.
doi: 10.1016/0375-9474(69)90633-2
1969KU06 Nucl.Phys. A137, 500 (1969) H.W.Kugel, R.R.Borchers, R.Kalish Magnetic Moment Measurements of the 211.2 keV(3/2-) and 239.8 keV(5/2-) States of 195Pt NUCLEAR REACTIONS 195Pt(16O, 16O'γ), E = 35 MeV; measured (16O)γ-coin, γγ(θ, H). 195Pt levels deduced g.
doi: 10.1016/0375-9474(69)90088-8
1969MU14 Proc.Roy.Soc.(London) 311A, 111 (1969) D.E.Murnick, J.R.MacDonald, R.R.Borchers, G.Heestand, B.Herskind Implantation Perturbed Angular Correlation Experiments in Iron after Inelastic Proton Scattering NUCLEAR REACTIONS 54,56Fe(p, p'), E=6.51, 6.78 MeV; 56Fe(16O, 16O'γ), E=33 MeV; measured p'γ(θ), (16O')(γ)(θ); deduced hyperfine fields.
doi: 10.1098/rspa.1969.0103
1968KA27 Proc.Intern.Conf.Hyperfine Struct.Nucl.Radiations, Asilomar, Pacific Grove, Calif. (1967), E.Matthias, D.A.Shirley, Eds., North-Holland Publ.Co., Amsterdam, p.208 (1968) R.Kalish, L.Grodzins, D.E.Murnick, R.R.Borchers, B.Herskind, J.D.Bronson Magnetic Moments of the First Excited 2+ States in Even Hg Isotopes NUCLEAR REACTIONS 198,200,202,204Hg(16O, 16O'γ), E = 40 MeV; measured γγ(θ, H). 198,200,202,204Hg levels deduced g.
1967CH16 Nucl.Phys. A102, 481 (1967) P.R.Christensen, B.Herskind, R.R.Borchers, L.Westgaard Neutron Single-Particle States in 143Nd and 145Sm NUCLEAR REACTIONS 142Nd, 144Sm(d, d), E=12 MeV; measured σ(θ), 143Nd(d, d'), E=12 MeV; measured σ(Ed', θ). 142Nd, 144Sm(d, p), (d, pγ), E=12 MeV; measured σ(Ep, θ), pγ-coin; deduced Q. 143Nd, 145Sm deduced levels, J, π, L(n), S. Enriched targets.
doi: 10.1016/0375-9474(67)90387-9
1967KA16 Phys.Rev. 161, 1196 (1967); R.R.Borchers - Priv.Comm. (May 1972) R.Kalish, L.Grodzins, R.R.Borchers, J.D.Bronson, B.Herskind Magnetic Moments of the First Excited 2+ States in the Even Pt Isotopes NUCLEAR STRUCTURE 194Pt, 196Pt, 198Pt; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.161.1196
1967MU22 Phys.Rev. 163, 254 (1967); R.R.Borchers - Priv.Comm. (May 1972) D.E.Murnick, L.Grodzins, J.D.Bronson, B.Herskind, R.R.Borchers Effective Magnetic Fields on Samarium-150 in Ferromagnetic Lattices NUCLEAR STRUCTURE 150Sm; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.163.254
1966BO19 Phys.Rev.Letters 17, 1099 (1966) R.R.Borchers, J.D.Bronson, D.E.Murnick, L.Grodzins Magnetic Moments of 2+ States in Even Te Nuclei NUCLEAR STRUCTURE 128Te, 126Te, 122Te, 120Te, 124Te; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.17.1099
1966BO23 Nucl.Phys. 88, 689 (1966) R.R.Borchers, R.M.Wood, C.H.Holbrow Continuous Neutron Spectra from (p, n) Reactions NUCLEAR REACTIONS 89Y, 93Nb, 115In, 139La, 141Pr, 181Ta, 197Au(p, n), E = 8-14 MeV; measured σ(E;En, θ(n)); deduced level densities. Natural targets.
doi: 10.1016/0029-5582(66)90424-X
1966GR20 Nucl.Phys. 88, 474 (1966) L.Grodzins, R.R.Borchers, G.B.Hagemann Coulomb Excitation in the Platinum Isotopes NUCLEAR REACTIONS 190,192,194,195,196,198Pt(16O, 16O'γ), E = 36 MeV; measured Iγ. 190,192,194,196,198Pt deduced B(E2).
doi: 10.1016/0029-5582(66)90604-3
1965OV01 Nucl.Phys. 65, 156 (1965) Neutrons from the B11(p, n)C11 reaction NUCLEAR REACTIONS 11B(p, n), E = 4.0-11.5 MeV; measured σ(E;En, θ), Q-values; 12C; deduced structure, 11C levels, J, π. Natural target.
doi: 10.1016/0029-5582(65)90303-2
1965WO04 Nucl.Phys. 71, 529 (1965) R.M.Wood, R.R.Borchers, H.H.Barschall Neutrons from Protons on Isotopes of Tin NUCLEAR REACTIONS 112,116,117,118,119,120,122,124Sn(p, n), E = 7-14 MeV; measured σ(E;En, θ n). 116,117,118,120Sb deduced levels, level densities. Enriched targets.
doi: 10.1016/0029-5582(65)90763-7
1963BO06 Phys.Rev. 129, 2679 (1963) Neutrons from Proton Bombardment of Lithium NUCLEAR STRUCTURE 7Li; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.129.2679
1963OV01 Bull.Am.Phys.Soc. 8, No.4, 291, A8 (1963) J.C.Overley, R.R.Borchers, A.S.Mahajan, R.G.Kerr Neutrons from the B11(p, n)C11 Reaction NUCLEAR STRUCTURE 11B; measured not abstracted; deduced nuclear properties.
1963PO02 Phys.Rev. 129, 733 (1963) C.H.Poppe, C.H.Holbrow, R.R.Borchers Neutrons from D + T and D + H NUCLEAR STRUCTURE 1H, 3H; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.129.733
1962LE12 Phys.Rev. 128, 1328 (1962) H.W.Lefevre, R.R.Borchers, C.H.Poppe Neutrons from Deuteron Breakup on D, T, and He NUCLEAR STRUCTURE 4He; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.128.1328
1962PO13 Bull.Am.Phys.Soc. 7, 350, WA11 (1962) C.H.Poppe, C.H.Holbrow, R.R.Borchers, B.Hoop Neutrons from D+T and D+H NUCLEAR REACTIONS 1,3H(d, X)1NN, E=5-12 MeV; measured reaction products, En, In, TOF; deduced σ(θ), neutron spectra.
1961BO17 Bull.Am.Phys.Soc. 6, No.5, 429, J3 (1961) R.R.Borchers, C.H.Poppe, C.H.Holbrow Neutrons from Proton Bombardment of Lithium NUCLEAR STRUCTURE 7Li; measured not abstracted; deduced nuclear properties.
1960DA05 Bull.Am.Phys.Soc. 5, No.4, 245, HA4 (1960) P.Dagley, W.Haeberli, J.X.Saladin, R.R.Borchers Neutron Yield from the C13(p, n)N13 Reaction NUCLEAR STRUCTURE 13N; measured not abstracted; deduced nuclear properties.
1960DA22 Proc.Intern.Conf.Nuclear Structure, Kingston, Canada, D.A.Bromley, E.W.Vogt, Editors, University of Toronto Press, p.359 (1960) P.Dagley, W.Haeberli, J.X.Saladin, R.R.Borchers The Neutron Yield from the C13(pn)N13 Reaction NUCLEAR STRUCTURE 13C; measured not abstracted; deduced nuclear properties.
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