NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = J.Nolen Found 92 matches. 2024SO03 Phys.Rev. C 109, 024605 (2024) J.Song, G.Savard, J.Greene, J.A.Nolen Design and validation of a fission-product source for radioactive beams
doi: 10.1103/PhysRevC.109.024605
2020SU23 Phys.Rev. C 102, 064615 (2020) H.Suzuki, K.Yoshida, N.Fukuda, H.Takeda, Y.Shimizu, D.S.Ahn, T.Sumikama, N.Inabe, T.Komatsubara, H.Sato, Z.Korkulu, K.Kusaka, Y.Yanagisawa, M.Ohtake, H.Ueno, T.Kubo, S.Michimasa, N.Kitamura, K.Kawata, N.Imai, O.B.Tarasov, D.Bazin, J.Nolen, W.F.Henning Experimental studies of the two-step scheme with an intense radioactive 132Sn beam for next-generation production of very neutron-rich nuclei NUCLEAR REACTIONS 9Be(132Sn, X)108Nb/109Nb/110Nb/111Nb/112Nb/111Mo/112Mo/113Mo/114Mo/115Mo/116Mo/114Tc/115Tc/116Tc/117Tc/118Tc/119Tc/115Ru/116Ru/117Ru/118Ru/119Ru/120Ru/121Ru/122Ru/123Ru/120Rh/121Rh/122Rh/123Rh/124Rh/125Rh/126Rh/117Pd/118Pd/119Pd/120Pd/121Pd/122Pd/123Pd/124Pd/125Pd/126Pd/127Pd/128Pd/129Pd/130Pd/131Pd/126Ag/127Ag/128Ag/129Ag/130Ag/129Cd/130Cd/131Cd, E=278 MeV/nucleon, [132Sn secondary beam from 9Be(238U, F), E=345 MeV/nucleon primary reaction]; measured neutron-rich reaction products, A/Q particle-identification plots, production σ in two-step mechanism of fission and fragmentation using BigRIPS separator and ZeroDegree spectrometer at RIBF-RIKEN facility. Comparison of production σ for one-step (in-flight fission or fragmentation) and two-step (ISOL followed by in-beam fragmentation) mechanisms. Comparison with experimental production σ data from GSI, and with theoretical calculations using CORFA1.0 and EPAX3.1a codes.
doi: 10.1103/PhysRevC.102.064615
2015DE24 Eur.Phys.J. A 51, 66 (2015) F.Dechery, A.Drouart, H.Savajols, J.Nolen, M.Authier, A.M.Amthor, D.Boutin, O.Delferriere, B.Gall, A.Hue, B.Laune, F.Le Blanc, S.Manikonda, J.Payet, M.-H.Stodel, E.Traykov, D.Uriot, Toward the drip lines and the superheavy island of stability with the Super Separator Spectrometer S3
doi: 10.1140/epja/i2015-15066-3
2012KA36 Phys.Rev. C 86, 054319 (2012) D.Kameda, T.Kubo, T.Ohnishi, K.Kusaka, A.Yoshida, K.Yoshida, M.Ohtake, N.Fukuda, H.Takeda, K.Tanaka, N.Inabe, Y.Yanagisawa, Y.Gono, H.Watanabe, H.Otsu, H.Baba, T.Ichihara, Y.Yamaguchi, M.Takechi, S.Nishimura, H.Ueno, A.Yoshimi, H.Sakurai, T.Motobayashi, T.Nakao, Y.Mizoi, M.Matsushita, K.Ieki, N.Kobayashi, K.Tanaka, Y.Kawada, N.Tanaka, S.Deguchi, Y.Satou, Y.Kondo, T.Nakamura, K.Yoshinaga, C.Ishii, H.Yoshii, Y.Miyashita, N.Uematsu, Y.Shiraki, T.Sumikama, J.Chiba, E.Ideguchi, A.Saito, T.Yamaguchi, I.Hachiuma, T.Suzuki, T.Moriguchi, A.Ozawa, T.Ohtsubo, M.A.Famiano, H.Geissel, A.S.Nettleton, O.B.Tarasov, D.Bazin, B.M.Sherrill, S.L.Manikonda, J.A.Nolen Observation of new microsecond isomers among fission products from in-flight fission of 345 MeV/nucleon 238U NUCLEAR REACTIONS 9Be(238U, F)43S/50K/54Sc/56Sc/59Ti/60V/64Mn/67Fe/76Ni/75Cu/78Zn/82Ga/90As/92Se/93Se/ 92Br/94Br/95Br/96Br/95Kr/96Rb/97Rb/98Rb/97Sr/100Sr/101Y/106Nb/108Nb/109Nb/108Zr/109Mo/112Tc/113Tc/117Ru/119Ru/120Rh/122Rh/121Pd/124Pd/124Ag/125Ag/126Ag/125Cd/127Cd, 128Cd/130Cd/129In/130In/131In/130Sn/131Sn/132Sn/134Sn/136Sb, E=345 MeV/nucleon; measured fission fragment spectra, time of flight, energy loss, magnetic rigidity, Eγ, Iγ, γγ-coin, (fragment)γ-correlations, delayed γ spectra, isomer half-lives by γ(t) using BigRIPS separator and ZeroDegree spectrometer at RIBF, RIKEN accelerator complex. RADIOACTIVITY 43S, 50K, 54,56Sc, 59Ti, 60V, 64Mn, 67Fe, 76Ni, 75Cu, 78Zn, 82Ga, 90As, 92,93Se, 92,94,95,96Br, 95Kr, 96,97,98Rb, 97,100Sr, 101Y, 106,108,109Nb, 108Zr, 109Mo, 112,113Tc, 117,119Ru, 120,122Rh, 121,124Pd, 124,125,126Ag, 125,127,128,130Cd, 129,130,131In, 130,131,132,134Sn, 136Sb(IT)[from 9Be(238U, F), E=345 MeV/nucleon]; measured Eγ, Iγ, γγ-coin, (fragment)γ-correlations, delayed γ spectra, isomer half-lives by γ(t) using BigRIPS separator and ZeroDegree spectrometer at RIBF, RIKEN accelerator complex; deduced levels, J, π, shape isomers, multipolarity, configuration. Comparison with previous studies.
doi: 10.1103/PhysRevC.86.054319
2010DR04 Nucl.Phys. A834, 747c (2010) A.Drouart, A.M.Amthor, D.Boutin, O.Delferriere, M.Duval, S.Manikonda, J.A.Nolen, J.Payet, H.Savajols, M.-H.Stodel, D.Uriot The Super Separator Spectrometer (S3) for SPIRAL2 stable beams
doi: 10.1016/j.nuclphysa.2010.01.135
2010OH02 J.Phys.Soc.Jpn. 79, 073201 (2010) T.Ohnishi, T.Kubo, K.Kusaka, A.Yoshida, K.Yoshida, M.Ohtake, N.Fukuda, H.Takeda, D.Kameda, K.Tanaka, N.Inabe, Y.Yanagisawa, Y.Gono, H.Watanabe, H.Otsu, H.Baba, T.Ichihara, Y.Yamaguchi, M.Takechi, S.Nishimura, H.Ueno, A.Yoshimi, H.Sakurai, T.Motobayashi, T.Nakao, Y.Mizoi, M.Matsushita, K.Ieki, N.Kobayashi, K.Tanaka, Y.Kawada, N.Tanaka, S.Deguchi, Y.Satou, Y.Kondo, T.Nakamura, K.Yoshinaga, C.Ishii, H.Yoshii, Y.Miyashita, N.Uematsu, Y.Shiraki, T.Sumikama, J.Chiba, E.Ideguchi, A.Saito, T.Yamaguchi, I.Hachiuma, T.Suzuki, T.Moriguchi, A.Ozawa, T.Ohtsubo, M.A.Famiano, H.Geissel, A.S.Nettleton, O.B.Tarasov, D.P.Bazin, B.M.Sherrill, S.L.Manikonda, J.A.Nolen Identification of 45 New Neutron-Rich Isotopes Produced by In-Flight Fission of a 238U Beam at 345 MeV/nucleon NUCLEAR REACTIONS Be, Pb(238U, F), E=345 MeV/nucleon; measured yields of fission fragments. Z=20-56, A=52-152; measured yields. 71Mn, 73,74Fe, 76Co, 79Ni, 81,82Cu, 84,85Zn, 87Ga, 90Ge, 95Se, 98Br, 101Kr, 103Rb, 106,107Sr, 108,109Y, 111,112Zr, 114,115Nb, 115,116,117Mo, 119,120Tc, 121,122,123,124Ru, 123,124,125,126Rh, 127,128Pd, 133Cd, 138Sn, 140Sb, 143Te, 145I, 148Xe, 152Ba; measured yields and cross sections, identified new isotopes using RI beam factory at RIKEN, ΔE-TOF-Bρ method.
doi: 10.1143/JPSJ.79.073201
2009DR11 Int.J.Mod.Phys. E18, 2160 (2009) A.Drouart, J.A.Nolen, H.Savajols Super separator spectrometer for the LINAG heavy ion beams
doi: 10.1142/S0218301309014482
2009JI08 Phys.Rev. C 80, 044613 (2009) C.L.Jiang, K.E.Rehm, D.Ackermann, I.Ahmad, J.P.Greene, B.Harss, D.Henderson, W.F.Henning, R.V.F.Janssens, J.Nolen, R.C.Pardo, P.Reiter, J.P.Schiffer, D.Seweryniak, A.Sonzogni, J.Uusitalo, I.Wiedenhover, A.H.Wuosmaa, F.Brumwell, G.McMichael, M.Paul, R.E.Segel Experimental study of the 56Ni(3He, d)57Cu reaction in inverse kinematics NUCLEAR REACTIONS 3He(56Ni, d), E=250 MeV; measured Ed, Id, σ, σ(θ). 57Cu; deduced levels, J, π, spectroscopic factors. DWBA analysis. Discussed implications for 56Ni(p, γ)57Cu reaction of astrophysical interest.
doi: 10.1103/PhysRevC.80.044613
2008OH06 J.Phys.Soc.Jpn. 77, 83201 (2008) T.Ohnishi, T.Kubo, K.Kusaka, A.Yoshida, K.Yoshida, N.Fukuda, M.Ohtake, Y.Yanagisawa, H.Takeda, D.Kameda, Y.Yamaguchi, N.Aoi, K.-I.Yoneda, H.Otsu, S.Takeuchi, T.Sugimoto, Y.Kondo, H.Scheit, Y.Gono, H.Sakurai, T.Motobayashi, H.Suzuki, T.Nakao, H.Kimura, Y.Mizoi, M.Matsushita, K.Ieki, T.Kuboki, T.Yamaguchi, T.Suzuki, A.Ozawa, T.Moriguchi, Y.Yasuda, T.Nakamura, T.Nannichi, T.Shimamura, Y.Nakayama, H.Geissel, H.Weick, J.A.Nolen, O.B.Tarasov, A.S.Nettleton, D.P.Bazin, B.M.Sherrill, D.J.Morrissey, W.Mittig Identification of New Isotopes 125Pd and 126Pd Produced by In-Flight Fission of 345 MeV/nucleon 238U: First Results from the RIKEN RI Beam Factory NUCLEAR REACTIONS Be(238U, X)125Pd/126Pd, E=345 MeV/nucleon; measured fragment energies, ToF, Eγ, Iγ, (fragment)γ-coin, yields.
doi: 10.1143/JPSJ.77.083201
2007NO11 Nucl.Phys. A787, 84c (2007) Plans for an Advanced Exotic Beam facility in the U.S.
doi: 10.1016/j.nuclphysa.2006.12.018
2004GO52 Nucl.Phys. A746, 453c (2004) The use of electron beam in RIA R+D
doi: 10.1016/j.nuclphysa.2004.09.132
2004GR29 Nucl.Phys. A746, 425c (2004) J.P.Greene, A.Levand, J.Nolen, T.Burtseva Uranium carbide fission target R+D for RIA - an update
doi: 10.1016/j.nuclphysa.2004.09.130
2004JI09 Nucl.Phys. A746, 403c (2004) C.L.Jiang, B.B.Back, J.Nolen, K.E.Rehm, G.Savard The influence of secondary reactions in the wedge of a magnetic separator at RIA
doi: 10.1016/j.nuclphysa.2004.09.142
2004MU33 Nucl.Phys. A746, 437c (2004) B.Mustapha, J.A.Nolen, I.C.Gomes Simulation of effusion from targets of tilted foils
doi: 10.1016/j.nuclphysa.2004.09.150
2004NO10 Nucl.Phys. A734, 661 (2004) Overview of the U.S. Rare Isotope Accelerator Proposal
doi: 10.1016/j.nuclphysa.2004.01.120
2004NO17 Nucl.Phys. A746, 9c (2004) Radioactive beam facilities of North America
doi: 10.1016/j.nuclphysa.2004.09.013
2004RE30 Nucl.Phys. A746, 161c (2004) C.B.Reed, J.A.Nolen, J.R.Specht, V.J.Novick, P.Plotkin A 20 kw beam-on-target test of a high-power liquid lithium target for RIA
doi: 10.1016/j.nuclphysa.2004.09.127
2004VI12 Nucl.Phys. A746, 445c (2004) N.Y.Vinogradov, J.A.Nolen, P.N.Ostroumov, K.W.Shepard Development of a low charge-to-mass ratio injector for a RIB linac
doi: 10.1016/j.nuclphysa.2004.09.131
2002HA15 Phys.Rev. C65, 035803 (2002) B.Harss, C.L.Jiang, K.E.Rehm, J.P.Schiffer, J.Caggiano, P.Collon, J.P.Greene, D.Henderson, A.Heinz, R.V.F.Janssens, J.Nolen, R.C.Pardo, T.Pennington, R.H.Siemssen, A.A.Sonzogni, J.Uusitalo, I.Wiedenhover, M.Paul, T.F.Wang, F.Borasi, R.E.Segel, J.C.Blackmon, M.Smith, A.Chen, P.Parker Widths of Astrophysically Important Resonances in 18Ne NUCLEAR REACTIONS 1H(17F, p), (17F, α), E(cm)=3.07-3.94 MeV; measured σ, σ(E, θ). 17F(p, p'), E(cm) ≈ 3.5 MeV; deduced σ(θ). 14O(α, p), E=low; deduced astrophysical reaction rates. 18Ne deduced resonance parameters.
doi: 10.1103/PhysRevC.65.035803
2002JI08 Nucl.Instrum.Methods Phys.Res. A492, 57 (2002) C.L.Jiang, B.B.Back, I.Gomes, A.M.Heinz, J.Nolen, K.E.Rehm, G.Savard, J.P.Schiffer Yield calculations for a facility for short-lived nuclear beams NUCLEAR REACTIONS 7Li(86Kr, X)78Ni, E ≈ 0.1-1 GeV/nucleon; 9Be(40Ar, X)19C, E ≈ 0.1-1 GeV/nucleon; calculated yields vs target thickness. Yields for many other reactions discussed.
doi: 10.1016/S0168-9002(02)01352-9
2002NO02 Eur.Phys.J. A 13, 255 (2002) Prospects for Exotic Beam Facilities in North America
doi: 10.1007/s10050-002-8752-y
2002NO07 Nucl.Phys. A701, 312c (2002) J.A.Nolen, C.B.Reed, A.Hassanein, I.C.Gomes Liquid-Lithium Cooling for 100-kW ISOL and Fragmentation Targets
doi: 10.1016/S0375-9474(01)01604-9
2001CA37 Phys.Rev. C64, 025802 (2001) J.A.Caggiano, D.Bazin, W.Benenson, B.Davids, R.Ibbotson, H.Scheit, B.M.Sherrill, M.Steiner, J.Yurkon, A.F.Zeller, B.Blank, M.Chartier, J.Greene, J.A.Nolen, Jr., A.H.Wuosmaa, M.Bhattacharya, A.Garcia, M.Wiescher Spectroscopy of 23Al and 27P using the (7Li, 8He) Reaction and the Implications for 22Na and 26Al Nucleosynthesis in Explosive Hydrogen Burning NUCLEAR REACTIONS 9Be, 10B, 24Mg, 28Si(7Li, 8He), E=50.1 MeV/nucleon; measured particle spectra. 23Al, 27P deduced level energies. 22Mg, 26Si(p, γ), E=low; deduced stellar reaction rates. ATOMIC MASSES 23Al, 27P; measured ground-state mass excess.
doi: 10.1103/PhysRevC.64.025802
2000RE11 Nucl.Instrum.Methods Phys.Res. A449, 208 (2000) K.E.Rehm, F.Borasi, C.J.Jiang, D.Ackermann, I.Ahmad, F.Brumwell, C.N.Davids, P.Decrock, S.M.Fischer, J.Gorres, J.P.Greene, G.Hackmann, B.Harss, D.Henderson, W.Henning, R.V.F.Janssens, G.McMichael, V.Nanal, D.Nisius, J.Nolen, R.C.Pardo, M.Paul, P.Reiter, J.P.Schiffer, D.Seweryniak, R.E.Segel, I.Wiedenhover, M.Wiescher, A.H.Wuosmaa Experiments with a Radioactive 56Ni Beam NUCLEAR REACTIONS 63,65Cu, 58Ni(p, X), E=50 MeV; measured delayed Eγ, Iγ; deduced evidence for 56Ni, 56,57Co, 52Mn, 65Zn. 2H(28Si, 29Si), E=125 MeV; 2H(56Co, 57Co), E=250 MeV; measured σ(Ep, θ). 57Co levels deduced spectroscopic factors.
doi: 10.1016/S0168-9002(99)01439-4
2000SO01 Phys.Rev.Lett. 84, 1651 (2000) A.A.Sonzogni, K.E.Rehm, I.Ahmad, F.Borasi, D.L.Bowers, F.Brumwell, J.Caggiano, C.N.Davids, J.P.Greene, B.Harss, A.Heinz, D.Henderson, R.V.F.Janssens, C.L.Jiang, G.McMichael, J.Nolen, R.C.Pardo, M.Paul, J.P.Schiffer, R.E.Segel, D.Seweryniak, R.H.Siemssen, J.W.Truran, J.Uusitalo, I.Wiedenhover, B.Zabransky The 44Ti(α, p) Reaction and Its Implication on the 44Ti Yield in Supernovae NUCLEAR REACTIONS 44Ti(α, p), E(cm)=5.7-9 MeV; measured σ, astrophysical reaction rate. Comparison with statistical model calculations. Effects on the production of 44Ti in core-collapsed supernovae discussed.
doi: 10.1103/PhysRevLett.84.1651
1999HA14 Phys.Rev.Lett. 82, 3964 (1999); Comment Phys.Rev.Lett. 84, 1635 (2000) B.Harss, J.P.Greene, D.Henderson, R.V.F.Janssens, C.L.Jiang, J.Nolen, R.C.Pardo, K.E.Rehm, J.P.Schiffer, R.H.Siemssen, A.A.Sonzogni, J.Uusitalo, I.Wiedenhover, M.Paul, T.F.Wang, F.Borasi, R.E.Segel, J.C.Blackmon, M.S.Smith, A.Chen, P.Parker Stellar Reactions with Short-Lived Nuclei: 17F(p, α)14O NUCLEAR REACTIONS 1H(17F, 14O), E(cm)=2.2-3.8 MeV; measured particle energies, (14O)α-coin, σ(E). 18Ne deduced resonance parameters. Implications for astrophysical processes discussed.
doi: 10.1103/PhysRevLett.82.3964
1998RE01 Phys.Rev.Lett. 80, 676 (1998) K.E.Rehm, F.Borasi, C.L.Jiang, D.Ackermann, I.Ahmad, B.A.Brown, F.Brumwell, C.N.Davids, P.Decrock, S.M.Fischer, J.Gorres, J.Greene, G.Hackmann, B.Harss, D.Henderson, W.Henning, R.V.F.Janssens, G.McMichael, V.Nanal, D.Nisius, J.Nolen, R.C.Pardo, M.Paul, P.Reiter, J.P.Schiffer, D.Seweryniak, R.E.Segel, M.Wiescher, A.H.Wuosmaa Study of the 56Ni(d, p)57Ni Reaction and the Astrophysical 56Ni(p, γ)57Cu Reaction Rate NUCLEAR REACTIONS 2H(56Ni, p), E=250 MeV; measured σ(Ep, θ). 57Ni deduced levels, J, π, spectroscopic factors, astrophysical (p, γ) reaction rates.
doi: 10.1103/PhysRevLett.80.676
1998RE18 Phys.Rev.Lett. 81, 3341 (1998) K.E.Rehm, H.Esbensen, C.L.Jiang, B.B.Back, F.Borasi, B.Harss, R.V.F.Janssens, V.Nanal, J.Nolen, R.C.Pardo, M.Paul, P.Reiter, R.E.Segel, A.Sonzogni, J.Uusitalo, A.H.Wuosmaa Fusion Cross Sections for the Proton Drip Line Nucleus 17F at Energies Below the Coulomb Barrier NUCLEAR REACTIONS 208Pb(17F, X), E(cm)=80-92 MeV; 208Pb(19F, X), E(cm)=78-100 MeV; measured fusion-fission σ; deduced no enhancement for lighter projectile. Dynamical model calculations.
doi: 10.1103/PhysRevLett.81.3341
1998RE24 Nucl.Instrum.Methods Phys.Res. A418, 355 (1998) K.E.Rehm, C.L.Jiang, M.Paul, D.Blumenthal, L.A.Daniel, C.N.Davids, P.Decrock, S.M.Fischer, D.Henderson, C.Lister, J.Nickles, J.Nolen, R.C.Pardo, J.P.Schiffer, D.Seweryniak, R.E.Segel Study of Radiative Capture Reactions with Radioactive Ion Beams NUCLEAR REACTIONS 1H(18F, 19Ne), E=13.4 MeV; measured σ upper limit. 18F(p, γ), E(cm)=670 keV; deduced σ upper limit. Radioactive beams, inverse kinematics, fragment mass analyzer.
doi: 10.1016/S0168-9002(98)00885-7
1997RE02 Phys.Rev. C55, R566 (1997) K.E.Rehm, C.L.Jiang, M.Paul, D.Blumenthal, L.A.Daniel, C.N.Davids, P.Decrock, S.M.Fischer, D.Henderson, C.Lister, J.Nickles, J.Nolen, R.C.Pardo, J.P.Schiffer, D.Seweryniak, R.E.Segel Exploring the 18F(p, γ)19Ne Gateway to the Formation of Heavy Elements in Hot Stars NUCLEAR REACTIONS, ICPND 18F(p, γ)19Ne, E=13.4 MeV; measured σ. 18O(p, γ)19F, E=14.4-18 MeV; measured σ; calculated σ(E); deduced 19Ne production, astrophysical reaction rate for 18F(p, γ)19Ne upper limits. 19Ne level deduced upper limit for Γγ.
doi: 10.1103/PhysRevC.55.R566
1997RE05 Nucl.Phys. A616, 115c (1997) K.E.Rehm, M.Paul, A.D.Roberts, C.L.Jiang, D.Blumenthal, C.N.Davids, P.DeCrock, S.M.Fischer, J.Gehring, D.Henderson, C.J.Lister, J.Nickles, J.Nolen, R.C.Pardo, J.P.Schiffer, R.E.Segel Nuclear Reaction Studies with Radioactive 18F Beams at ATLAS NUCLEAR REACTIONS, ICPND 1H(18F, α), E(cm) ≈ 5.75-7 MeV; measured σ(E). 1H(18F, γ), E(cm)=0.67 MeV; measured σ; deduced reaction rates ratio, small contribution from (p, γ) route to 19Ne formation.
doi: 10.1016/S0375-9474(97)00080-8
1997RE17 Nucl.Phys. A621, 191c (1997) K.E.Rehm, M.Paul, A.D.Roberts, C.L.Jiang, D.Blumenthal, C.N.Davids, P.DeCrock, S.M.Fischer, J.Gehring, D.Henderson, C.J.Lister, J.Nickles, J.Nolen, R.C.Pardo, J.P.Schiffer, R.E.Segel, D.Seweryniak The Influence of 18F Induced Reactions in the Hot CNO Cycle NUCLEAR REACTIONS, ICPND 1H(18F, 15O), (18F, 19Ne), E=11.7-15.1 MeV; measured resonance reaction σ vs E; deduced reaction rates features. 19Ne deduced resonance strengths, widths. Astrophysical implications, radioactive beam.
doi: 10.1016/S0375-9474(97)00236-4
1996RE05 Phys.Rev. C53, 1950 (1996) K.E.Rehm, M.Paul, A.D.Roberts, C.L.Jiang, D.J.Blumenthal, S.M.Fischer, J.Gehring, D.Henderson, J.Nickles, J.Nolen, R.C.Pardo, J.P.Schiffer, R.E.Segel Astrophysical Reaction Rate for the 18F(p, α)15O Reaction NUCLEAR REACTIONS, ICPND 18F(p, α), E(cm)=600-800 keV; measured σ(E), resonance yield; calculated reaction rate. 19Ne deduced resonance, J, π, Γp, Γα, Γ.
doi: 10.1103/PhysRevC.53.1950
1996ZI06 Nucl.Instrum.Methods Phys.Res. A382, 132 (1996) G.P.Zinkann, P.Billquist, J.Bogaty, B.Clifft, F.Munson, K.Nakagawa, J.Nolen, R.Pardo, K.W.Shepard, J.Specht, A.Sutherland, B.Tieman, I.Tilbrook Current Status of ATLAS and Proposed Expansion to an Exotic Beam Facility
doi: 10.1016/S0168-9002(96)00624-9
1995RE11 Phys.Rev. C52, R460 (1995) K.E.Rehm, M.Paul, A.D.Roberts, D.J.Blumenthal, J.Gehring, D.Henderson, C.L.Jiang, J.Nickles, J.Nolen, R.C.Pardo, J.P.Schiffer, R.E.Segel Study of the 18F(p, α)15O Reaction at Astrophyical Energies using a 18F Beam NUCLEAR REACTIONS 18F(p, α), E(cm)=580-760 keV; measured σ(θ) vs E; deduced nuclosynthesis, CNO cycle implications. 19Ne deduced resonance, Γp, Γα, s-wave resonance strength. Gas-filled magnet technique.
doi: 10.1103/PhysRevC.52.R460
1995RO40 Nucl.Instrum.Methods Phys.Res. B103, 523 (1995) A.D.Roberts, R.J.Nickles, M.Paul, K.E.Rehm, C.J.Jiang, D.J.Blumenthal, J.Gehring, D.Henderson, J.Nolen, R.C.Pardo, J.P.Schiffer, R.E.Segel Production of a Radioactive 18F Ion Beam for Nuclear Reaction Studies
doi: 10.1016/0168-583X(95)00657-5
1991AN12 Phys.Rev. C44, 398 (1991) N.Anantaraman, J.S.Winfield, S.M.Austin, J.A.Carr, C.Djalali, A.Gillibert, W.Mittig, J.A.Nolen, Jr., Z.E.Long (12C, 12B) and (12C, 12N) Reactions at E/A = 70 MeV as Spin Probes: Calibration and application to 1+ states in 56Mn NUCLEAR REACTIONS 12C, 26Mg, 54Fe, 58Ni, 90Zr(12C, 12B), 12C, 56Fe(12C, 12N), E=840 MeV; measured σ(θ). 56Mn deduced 1+ level Gamow-Teller strengths. DWBA, shell model.
doi: 10.1103/PhysRevC.44.398
1991HA25 Phys.Rev. C44, 2365 (1991) R.Harkewicz, D.J.Morrissey, B.A.Brown, J.A.Nolen, Jr., N.A.Orr, B.M.Sherrill, J.S.Winfield, J.A.Winger β-Decay Branching Ratios of the Neutron-Rich Nucleus 15B RADIOACTIVITY 15B(β-n) [from 9Be(18O, X), E=80 MeV/nucleon]; measured β-decay curve, delayed-neutron spectra, Iβ; deduced log ft. 15C deduced levels, β-decay branching ratios. Shell model, psd model space.
doi: 10.1103/PhysRevC.44.2365
1989ZH04 Phys.Rev. C39, 1985 (1989) Z.Zhao, M.Gai, B.J.Lund, S.L.Rugari, D.Mikolas, B.A.Brown, J.A.Nolen, Jr., M.Samuel Beta Decay of 18N to Alpha Particle Emitting States in 18O and a Proposed Search for Parity Violation in 18O RADIOACTIVITY 18N(β-) [from Ta(22Ne, X), E=35 MeV/nucleon]; measured absolute β-decay branching ratios; deduced log ft, Gamow-Teller matrix elements. 18O(α) [from 18N β-decay]; measured total β-delayed α-yield. 18O deduced possible new levels.
doi: 10.1103/PhysRevC.39.1985
1988MI03 Phys.Rev. C37, 766 (1988) D.Mikolas, B.A.Brown, W.Benenson, L.H.Harwood, E.Kashy, J.A.Nolen, Jr., B.Sherrill, J.Stevenson, J.S.Winfield, Z.Q.Xie, R.Sherr Branching Ratios of 9C to Low Lying States in 9B RADIOACTIVITY 9C(β+) [from Ni(12C, X), E=35 MeV/nucleon]; measured β-delayed Ep, Ip, β-delayed Eα, Iα, βαp-coin; deduced log ft. 9B levels deduced Iβ, Gamow-Teller transition strengths, comparison with other data. NUCLEAR STRUCTURE 9B, 9Be, 9C; calculated levels, Gamow-Teller transition strengths, particle decay spectroscopic factors, particle decay reduced widths. Input from 9Be(p, n) reaction.
doi: 10.1103/PhysRevC.37.766
1988MO18 Phys.Rev. C38, 737 (1988) M.F.Mohar, E.Adamides, W.Benenson, C.Bloch, B.A.Brown, J.Clayton, E.Kashy, M.Lowe, J.A.Nolen, Jr., W.E.Ormand, J.van der Plicht, B.Sherrill, J.Stevenson, J.S.Winfield Mass of 39Sc via the 40Ca(7Li, 8He) Reaction NUCLEAR REACTIONS 40Ca(7Li, 8He), E=27.24 MeV/nucleon; measured σ(E(8He)); deduced Q, mass equation parameters. 39Sc deduced mass excess. Isobaric multiplet mass equation, isospin-nonconserving Hamiltonian.
doi: 10.1103/PhysRevC.38.737
1988SA04 Phys.Rev. C37, 1314 (1988) M.Samuel, B.A.Brown, D.Mikolas, J.Nolen, B.Sherrill, J.Stevenson, J.S.Winfield, Z.Q.Xie Measurement of the Beta Decay Half-Life of 17B RADIOACTIVITY 9Li, 12,13,15,17B, 17C, 19N [from Ta(23Ne, X), E=35 MeV/nucleon]; measured β-decay T1/2.
doi: 10.1103/PhysRevC.37.1314
1988ST06 Phys.Rev. C37, 2220 (1988) J.Stevenson, B.A.Brown, Y.Chen, J.Clayton, E.Kashy, D.Mikolas, J.Nolen, M.Samuel, B.Sherrill, J.S.Winfield, Z.Q.Xie, R.E.Julies, W.A.Richter Search for the Exotic Nucleus 10He NUCLEAR REACTIONS Sn(18O, X), E=30 MeV/nucleon; measured fragment mass spectra; deduced 10He production upper limit. NUCLEAR STRUCTURE 4,5,6,7,8,9,10He; calculated binding energy. Shell model.
doi: 10.1103/PhysRevC.37.2220
1986CU01 Phys.Rev.Lett. 56, 34 (1986) M.S.Curtin, L.H.Harwood, J.A.Nolen, B.Sherrill, Z.Q.Xie, B.A.Brown Lifetime Measurements of Neutron-Rich Light Isotopes 14Be and 17C RADIOACTIVITY 9,11Li, 14,12Be, 12,14,15B, 17C(β-) [from 181Ta(18O, X), E=30 MeV/nucleon]; measured β-decay T1/2.
doi: 10.1103/PhysRevLett.56.34
1985FR13 Phys.Rev. C32, 975 (1985) K.A.Frankel, J.A.Bistirlich, R.Bossingham, H.R.Bowman, K.M.Crowe, C.J.Martoff, D.L.Murphy, J.O.Rasmussen, J.P.Sullivan, E.Yoo, W.A.Zajc, J.P.Miller, O.Hashimoto, M.Koike, J.Peter, W.Benenson, G.M.Crawley, E.Kashy, J.A.Nolen, Jr., J.Quebert Pion Production Near Mid-Rapidity in High-Energy Heavy-Ion Collisions NUCLEAR REACTIONS C, Ca, U(40Ar, X), E=1050 MeV/nucleon; 9Be, 23Na, 19F(20Ne, X), E=655 MeV/nucleon; measured σ(θ(π+), E(π+)), σ(θ(π-), E(π-)); deduced ratio. Coulomb effect calculation comparison.
doi: 10.1103/PhysRevC.32.975
1985SH03 Phys.Rev. C31, 875 (1985) B.Sherrill, K.Beard, W.Benenson, C.Bloch, B.A.Brown, E.Kashy, J.A.Nolen, Jr., A.D.Panagiotou, J.van der Plicht, J.S.Winfield Mass of 57Cu NUCLEAR STRUCTURE A=39-59; calculated Coulomb displacement energies; deduced rp-process rate for 56Ni(p, γ) reaction. Mass excess input. NUCLEAR REACTIONS 58Ni(7Li, 8He), E=173.6 MeV; measured Q, σ(θ). 57Cu deduced levels, mass excess.
doi: 10.1103/PhysRevC.31.875
1983FI10 Nucl.Phys. A407, 163 (1983) J.E.Finck, G.M.Crawley, J.A.Nolen, Jr., R.T.Kouzes A Study of 206Pb by Inelastic Scattering of 35 MeV Protons NUCLEAR REACTIONS 206Pb(p, p'), E=35 MeV; measured σ(Ep'), σ(θ). 206Pb deduced levels, L, deformation β(L). Collective, microscopic models, RPA, TDA wave functions.
doi: 10.1016/0375-9474(83)90313-5
1983ZW02 Phys.Rev. C28, 542 (1983) B.Zwieglinski, G.M.Crawley, J.A.Nolen, Jr., R.M.Ronningen Coupled Channel Effects in 26Mg(p, p') at 40 MeV NUCLEAR REACTIONS 26Mg(p, p'), E=40 MeV; measured σ(Ep), σ(θ); deduced optical model parameters. 26Mg levels deduced interference effects, multipole matrix elements, inelastic transition rates. Coupled-channels method, shell model wave functions. Enriched target.
doi: 10.1103/PhysRevC.28.542
1982FR05 Phys.Rev. C25, 1102 (1982) K.A.Frankel, J.A.Bistirlich, R.Bossingham, H.R.Bowman, K.M.Crowe, C.J.Martoff, D.Murphy, J.O.Rasmussen, J.P.Sullivan, W.A.Zajc, J.P.Miller, O.Hashimoto, M.Koike, J.Peter, W.Benenson, G.M.Crawley, E.Kashy, J.A.Nolen, Jr., J.Quebert Pions Produced near the Center-of-Mass Velocity in Heavy-Ion Collisions NUCLEAR REACTIONS C, Ca, U(40Ar, π+), (40Ar, π-), E=1.05 GeV/nucleon; measured σ(E, θ).
doi: 10.1103/PhysRevC.25.1102
1982SU01 Phys.Rev. C25, 1499 (1982) J.P.Sullivan, J.A.Bistirlich, H.R.Bowman, R.Bossingham, T.Buttke, K.M.Crowe, K.A.Frankel, C.J.Martoff, J.Miller, D.L.Murphy, J.O.Rasmussen, W.A.Zajc, O.Hashimoto, M.Koike, J.Peter, W.Benenson, G.M.Crawley, E.Kashy, J.A.Nolen, Jr. Strong Coulomb Effects on Pions Produced in Heavy Ion Collisions NUCLEAR REACTIONS C, Na, F, Cu, U(20Ne, π+), (20Ne, π-), E=280-480 MeV/nucleon; C, K, Cl(40Ar, π+), (40Ar, π-), E=535 MeV/nucleon; measured σ(Eπ, θπ); deduced Coulomb effects, projectile fragment charges.
doi: 10.1103/PhysRevC.25.1499
1981DE12 Phys.Rev. C23, 1414 (1981) P.T.Deason, C.H.King, R.M.Ronningen, T.L.Khoo, F.M.Bernthal, J.A.Nolen, Jr. 194,196,198Pt(p, p') Reactions at 35 MeV NUCLEAR REACTIONS 194,196,198Pt(p, p'), E=35 MeV; measured σ(Ep, θ); deduced optical model parameters. 194,196,198Pt deduced levels, J, π, quadrupole, hexadecapole moments, β2, β4, B(E4), band structure. Magnetic spectrograph, enriched targets. Interacting boson model, coupled-channels calculation.
doi: 10.1103/PhysRevC.23.1414
1981FI07 Phys.Lett. 107B, 182 (1981) J.E.Finck, G.M.Crawley, J.A.Nolen, Jr., R.Kouzes Systematics of Collective States in Lead Nuclei from Inelastic Proton Scattering NUCLEAR REACTIONS 206Pb(p, p'), E=35 MeV; measured σ(θ). 206Pb deduced levels, transition strengths. Collective DWBA analysis.
doi: 10.1016/0370-2693(81)90808-X
1981RO02 Phys.Rev. C23, 973 (1981) R.G.H.Robertson, J.A.Nolen, Jr., T.Chapuran, R.Vodhanel Mass of 6Li and the Excitation Energy of its 3.56-MeV State NUCLEAR REACTIONS 6Li(γ, γ'), E=7 MeV bremsstrahlung; measured Eγ. 6Li level deduced energy. Ge(Li) detector. 6Li(p, α), E=10.5 MeV; measured Q. 6Li deduced mass excess. Magnetic spectrograph.
doi: 10.1103/PhysRevC.23.973
1981RO09 Phys.Rev.Lett. 47, 635 (1981) R.M.Ronningen, R.C.Melin, J.A.Nolen, Jr., G.M.Crawley, C.E.Bemis, Jr. Higher-Order Deformations of 232Th and 234,236,238U NUCLEAR REACTIONS 232Th, 234,236,238U(p, p), (p, p'), E=35 MeV; measured σ(θ). 232Th, 234,236,238U deduced deformation parameters β2, β4, β6, multipole moments. Coupled-channels calculations, deformed spin-orbit interaction.
doi: 10.1103/PhysRevLett.47.635
1980FU04 Nucl.Phys. A343, 133 (1980) H.Fuchs, J.A.Nolen, G.J.Wagner, H.Lenske, G.Baur Experimental and Theoretical Study of Line Shapes in 13C(α, α') Inelastic Scattering to Resonant States NUCLEAR REACTIONS 13C(α, α'), E=22, 36 MeV; measured σ(Eα, θ). 13C resonance deduced line shape parameter. Enriched target.
doi: 10.1016/0375-9474(80)90645-4
1979BE31 Phys.Rev.Lett. 43, 683 (1979) W.Benenson, G.Bertsch, G.M.Crawley, E.Kashy, J.A.Nolen, Jr., H.Bowman, J.G.Ingersoll, J.O.Rasmussen, J.Sullivan, M.Koike, M.Sasao, J.Peter, T.E.Ward Low-Energy Pion Production at 0° with Heavy Ions from 125 to 400 MeV/Nucleon NUCLEAR REACTIONS Na, F, Cu, U(20Ne, π+), (20Ne, π-), E=125-400 MeV/nucleon; measured σ(0°), σ(π+)/σ(π-); discussed reaction mechanisms.
doi: 10.1103/PhysRevLett.43.683
1979DE25 Phys.Rev. C20, 927 (1979) P.T.Deason, C.H.King, T.L.Khoo, J.A.Nolen, Jr., F.M.Bernthal 194,196,198Pt(p, t) Reactions at 35 MeV NUCLEAR REACTIONS 194,196,198Pt(p, t), E=35 MeV; measured σ(Et, θ). 192,194,196Pt deduced levels, L, J, π, enhancement factor. DWBA analysis. Interacting boson approximation model. Enriched targets.
doi: 10.1103/PhysRevC.20.927
1979KI14 Phys.Rev. C20, 2084 (1979) C.H.King, J.E.Finck, G.M.Crawley, J.A.Nolen, Jr., R.M.Ronningen Multipole Moments of 154Sm, 176Yb, 232Th, and 238U from Proton Inelastic Scattering NUCLEAR REACTIONS 154Sm, 176Yb, 232Th, 238U(p, p'), E=35 MeV; measured σ(Ep', θ); deduced optical model, β2, β4 parameters. Enriched targets, emulsion plates, proportional counter. Coupled channels calculations, rotation model.
doi: 10.1103/PhysRevC.20.2084
1979SU01 Nucl.Phys. A313, 141 (1979) T.Suehiro, J.E.Finck, J.A.Nolen, Jr. A Study of the 54Fe(p, d)53Fe Reaction at 40 MeV NUCLEAR REACTIONS 54Fe(p, d), E=40.16 MeV; measured σ(θ, Ed). 53Fe deduced levels, L, S. 54Fe enriched target.
doi: 10.1016/0375-9474(79)90572-4
1979ZW02 Phys.Rev. C20, 2449 (1979) B.Zwieglinski, G.M.Crawley, J.A.Nolen, Jr. The Two-Step Pickup-Stripping Process in the 24Mg(p, p')24Mg Reaction at 40 MeV to Some Negative Parity States in 24Mg NUCLEAR REACTIONS 24Mg(p, p'), E=40 MeV; measured σ(θ); deduced reaction mechanism. Two-step coupled-channels calculation.
doi: 10.1103/PhysRevC.20.2449
1978BH02 Phys.Lett. 76B, 562 (1978) T.S.Bhatia, H.Hafner, J.A.Nolen, Jr., W.Saathoff, R.Schuhmacher, R.E.Tribble, G.J.Wagner, C.A.Wiedner The Mass of 15B via a Three-Proton Stripping Reaction NUCLEAR REACTIONS 48Ca(18O, 15B), E=102 MeV; measured yields; deduced Q. 15B deduced mass excess.
doi: 10.1016/0370-2693(78)90854-7
1978SM05 Phys.Rev. C18, 2065 (1978) P.A.Smith, J.A.Nolen, Jr., R.G.Markham, M.A.M.Shahabuddin 52Cr(p, α)49V Reaction NUCLEAR REACTIONS 52Cr(p, α), E=35 MeV; measured σ(θ). 49V deduced levels. Studied reaction mechanism.
doi: 10.1103/PhysRevC.18.2065
1978WI06 Phys.Lett. 78B, 26 (1978) C.A.Wiedner, J.A.Nolen, Jr., W.Saathoff, R.E.Tribble, J.Bolger, J.Zichy, K.Stricker, H.McManus, J.A.Carr A Comparison of 180 MeV π+ and π- Scattering from 24Mg NUCLEAR REACTIONS 24Mg(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=180 MeV; measured σ(θ).
doi: 10.1016/0370-2693(78)90339-8
1978ZE04 Phys.Rev. C18, 2122 (1978) Mass and Low-Lying Energy Levels of 69Cu NUCLEAR REACTIONS 64,66,68Zn(d, 3He), E=23.3 MeV; measured σ(θ). 70Zn(d, 3He), E=23.3 MeV; measured σ(θ); deduced Q. 69Cu deduced mass excess, levels, L, C2S. 63,65,67Cu deduced levels, L, C2S.
doi: 10.1103/PhysRevC.18.2122
1978ZW01 Phys.Rev. C17, 872 (1978) B.Zwieglinski, G.M.Crawley, H.Nann, J.A.Nolen, Jr. Inelastic Scattering of 40 MeV Protons from 24Mg. I. Natural Parity Transitions NUCLEAR REACTIONS 24Mg(p, p'), E=40 MeV; measured σ(Ep', θ); deduced optical model parameters. 24Mg levels deduced β, L, J, π.
doi: 10.1103/PhysRevC.17.872
1978ZW02 Phys.Rev. C18, 1228 (1978) B.Zwieglinski, G.M.Crawley, W.Chung, H.Nann, J.A.Nolen, Jr. Inelastic Scattering of 40 MeV Protons from 24Mg. II. Microscopic Calculations for Positive Parity States NUCLEAR REACTIONS 24Mg(p, p'), E=40 MeV; calculated σ(θ) to positive parity states; deduced collective enhancement factors. Microscopic DWBA.
doi: 10.1103/PhysRevC.18.1228
1977NO08 Phys.Lett. 71B, 314(1977) J.A.Nolen, T.S.Bhatia, H.Hafner, P.Doll, C.A.Wiedner, G.J.Wagner The Mass and Low-Lying Level Structure of 17C NUCLEAR REACTIONS 48Ca(18O, 17C), E=102 MeV; measured yields, σ; deduced reaction Q. 17C deduced mass excess.
doi: 10.1016/0370-2693(77)90225-8
1977TO17 Phys.Rev. C16, 1357 (1977) J.F.Tonn, R.E.Segel, J.A.Nolen, W.S.Chien, P.T.Debevec 40Ar(p, d)39Ar Reaction at E = 35 MeV NUCLEAR REACTIONS 40Ar(p, d), E=35 MeV; measured σ(Ed, θ). 39Ar deduced levels, L, S. DWBA analysis, planar gas cell target.
doi: 10.1103/PhysRevC.16.1357
1976NO02 Phys.Rev. C13, 1773 (1976) Measurement of the Excitation Energy of the 7.654 MeV State of 12C and The Rate of the 3α Reaction NUCLEAR REACTIONS 12C, 15N, 16O(p, p'), E=34.75 MeV; measured σ(Ep'); deduced Q for astrophysical 3α burning rate. 12C, 15N deduced resonances.
doi: 10.1103/PhysRevC.13.1773
1976SH17 Nucl.Phys. A263, 293 (1976) D.L.Show, B.H.Wildenthal, J.A.Nolen, Jr., E.Kashy A High Resolution Study of 26Al via the (p, d) Reaction NUCLEAR REACTIONS 27Al(p, d), E=35 MeV; measured σ(Ed, θ). 26Al deduced levels, L, J, π, S. Magnetic spectrograph.
doi: 10.1016/0375-9474(76)90175-5
1975CH17 Phys.Rev. C12, 332 (1975) W.S.Chien, C.H.King, J.A.Nolen, Jr., M.A.M.Shahabuddin Unnatural Parity Transitions in 22Ne(p, t)20Ne NUCLEAR REACTIONS 22Ne(p, t), E=40 MeV; measured σ(Et, θ).
doi: 10.1103/PhysRevC.12.332
1975NO04 Phys.Rev. C11, 1159 (1975) J.A.Nolen, Jr., R.J.Gleitsmann High-Resolution Study of 40Ca via Inelastic Proton Scattering at 35 Mev NUCLEAR REACTIONS 40Ca(p, p'), E=35.2 MeV; measured σ(Ep'). 40Ca deduced levels, T.
doi: 10.1103/PhysRevC.11.1159
1974KA15 Phys.Rev. C9, 2102 (1974) E.Kashy, W.Benenson, J.A.Nolen, Jr. A = 9 Isospin Quartet NUCLEAR REACTIONS 11B(p, t), (p, 3He), E=42 MeV; 10,11B(p, p'), E=35 MeV; measured σ(Et, E(3He), Ep'), Q. 9,10,11B, 9Be deduced levels.
doi: 10.1103/PhysRevC.9.2102
1974NO07 Nucl.Instrum.Methods 115, 189 (1974) J.A.Nolen, Jr., G.Hamilton, E.Kashy, I.D.Proctor Measuring Nuclear Excitation Energies and Q-Values with a Cyclotron-Magnetic Spectrograph System NUCLEAR REACTIONS 24Mg, 12C(p, p'), (p, d); 24Mg(p, t); measured Q. 11,12C, 24Mg deduced levels.
doi: 10.1016/0029-554X(74)90446-7
1971FO01 Phys.Rev. C3, 337 (1971) H.T.Fortune, G.C.Morrison, J.A.Nolen, Jr., P.Kienle Ru103,105 States Observed in the Reactions Ru102,104(d, p) NUCLEAR REACTIONS 102,104Ru(d, p), E=14 MeV; measured σ(Ep, θ). 103,105Ru deduced levels, J, π, L(n), S.
doi: 10.1103/PhysRevC.3.337
1970OH01 Phys.Rev. C1, 496 (1970) H.Ohnuma, J.R.Erskine, J.P.Schiffer, J.A.Nolen, Jr., N.Williams Level Structure of Sc48 from the Ca48(He3, t) Reaction NUCLEAR REACTIONS 48Ca(3He, t), E=15 MeV; measured σ(Et, θ). 48Sc deduced levels, J, π, configurations.
doi: 10.1103/PhysRevC.1.496
1970VO04 Phys.Rev. C1, 2066 (1970) D.von Ehrenstein, G.C.Morrison, J.A.Nolen, Jr., N.Williams Study of the (d, p) Reaction on the Even-A Barium Isotopes 130-138 NUCLEAR REACTIONS 130,132,134,136,138Ba(d, p), E=12 MeV; measured σ(Ep, θ), Q. 131,133,135,137,139Ba deduced levels, L(n), J, π, S.
doi: 10.1103/PhysRevC.1.2066
1970WI18 Phys.Rev. C2, 1539 (1970) N.Williams, G.C.Morrison, J.A.Nolen, Jr., Z.Vager, D.von Ehrenstein Isobaric Analog Resonances from Proton Scattering on the Barium Isotope NUCLEAR REACTIONS 130,132,134,136,138Ba(p, p), E=7-12 MeV; measured σ(E;θ). 131,133,135,137,139La deduced isobaric analog resonances, level-width, S, Coulomb displacement energies.
doi: 10.1103/PhysRevC.2.1539
1969NO03 Phys.Letters 29B, 396 (1969) Coulomb Energies - An Anomaly in Nuclear Matter Radii NUCLEAR STRUCTURE 17O, 29Si, 33S, 41,48Ca, 62Ni, 120Sn, 208Pb; calculated nuclear matter radii.
doi: 10.1016/0370-2693(69)90228-7
1969OH01 Phys.Rev. 177, 1695 (1969) H.Ohnuma, J.R.Erskine, J.A.Nolen, Jr., J.P.Schiffer, P.G.Roos Study of the Ca48(He3, p)Sc50 Reaction NUCLEAR REACTIONS 48Ca(3He, p), E=12 MeV; measured σ(Ep, θ); deduced Q. 50Sc deduced levels, J, π, isobaric analog. Enriched target.
doi: 10.1103/PhysRev.177.1695
1969SC14 Phys.Letters 29B, 399 (1969) J.P.Schiffer, J.A.Nolen, Jr., N.Williams On Coulomb Energies, the Anomalous Isotope Shift of Nuclear Radii, and Core Polarization by the Neutron Excess
doi: 10.1016/0370-2693(69)90229-9
1969VO05 Phys.Rev. To Be Published (1969) D.Von Ehrenstein, J.A.Nolen, Jr., G.C.Morrison, N.Williams
1968NO02 Bull.Am.Phys.Soc. 13, No.4, 584, BF15 (1968) J.A.Nolen, Jr., H.T.Fortune, P.Kienle, G.C.Morrison Energy Levels of 103Ru and 105Ru from the 102,104Ru(d, p) Reaction NUCLEAR STRUCTURE 103Ru, 105Ru; measured not abstracted; deduced nuclear properties.
1968ZE01 Bull.Am.Phys.Soc. 13, No.1, 105, GG12 (1968); Priv.Comm. (April 1968) Zn64,65,68,70(d, He3) Reactions at 23.3 MeV NUCLEAR STRUCTURE 67Cu, 69Cu, 65Cu, 63Cu; measured not abstracted; deduced nuclear properties.
1967MO15 Phys.Rev.Letters 19, 592 (1967) G.C.Morrison, N.Williams, J.A.Nolen, Jr., D.Von Ehrenstein Structure of Particle-Hole States in Ba138 NUCLEAR STRUCTURE 138Ba; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.19.592
1967NO01 Phys.Rev.Letters 18, 1140 (1967) J.A.Nolen, Jr., J.P.Schiffer, N.Williams, D.Von Ehrenstein Coulomb Displacement Energies of Ca-Sc Isobaric Pairs NUCLEAR STRUCTURE 42Sc, 44Sc, 46Sc, 50Sc, 48Sc, 47Sc; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.18.1140
1967OH01 Bull.Am.Phys.Soc. 12, No.1, 110, GF4 (1967) H.Ohnuma, J.R.Erskine, J.A.Nolen, Jr., J.P.Schiffer Investigation of the Ca48(He3, P)Sc50 Reaction NUCLEAR STRUCTURE 50Sc; measured not abstracted; deduced nuclear properties.
1966NO04 Phys.Lett. 21, 705 (1966) J.A.Nolen, Jr., C.M.Glashausser, M.E.Rickey J-Dependence in the (p, α) Reaction NUCLEAR STRUCTURE 63Cu, 65Cu, 89Y; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(66)90134-X
1966NO06 TID-23239, p.18 (1966) Direct (p, α) Reactions on Isotopes of Cu and Zn NUCLEAR STRUCTURE 62Ni; measured not abstracted; deduced nuclear properties.
1965NO01 Bull.Am.Phys.Soc. 10, No.1, 26, BC10 (1965) (p, α) Reactions on Copper and Zinc Isotopes at 17.5 MeV NUCLEAR STRUCTURE 67Cu, 89Y, 60Ni, 65Cu, 62Ni, 63Cu, 61Cu; measured not abstracted; deduced nuclear properties.
1965NO05 Thesis, Princeton Univ. (1965); PUC-937-171A (1965) Direct (p, α) Reactions on Isotopes of Copper and Zinc NUCLEAR STRUCTURE 61Cu, 63Cu, 62Ni, 65Cu, 60Ni, 67Cu; measured not abstracted; deduced nuclear properties.
1964NO02 Bull.Am.Phys.Soc. 9, No.4, 440, FA9 (1964) 27Al(p, α)24Mg and 25Mg(p, d)24Mg Reactions NUCLEAR STRUCTURE 24Mg; measured not abstracted; deduced nuclear properties.
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