NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = J.Cerny Found 153 matches. Showing 1 to 100. [Next]2011LE25 J.Phys.(London) G38, 075201 (2011) D.W.Lee, J.Powell, K.Perajarvi, F.Q.Guo, D.M.Moltz, J.Cerny Study of the 11C(p, γ) reaction via the indirect d(11C, 12N)n transfer reaction NUCLEAR REACTIONS 2H(11C, 12N), E=150 MeV; measured reaction products; deduced σ(θ), S-factors, reaction rates. DWUCK4 code calculations.
doi: 10.1088/0954-3899/38/7/075201
2009CE04 Phys.Rev.Lett. 103, 152502 (2009) J.Cerny, D.M.Moltz, D.W.Lee, K.Perajarvi, B.R.Barquest, L.E.Grossman, W.Jeong, C.C.Jewett Reinvestigation of the Direct Two-Proton Decay of the Long-Lived Isomer 94Agm [0.4 s, 6.7 MeV, (21+)] RADIOACTIVITY 94Ag(p), (2p) [from Ni(40Ca, 3np), E=197 MeV]; measured Ep, Ip, pp-coin.; deduced 94Agm one-proton radioactivity, energy groups, branching ratio, no two-proton radioactivity.
doi: 10.1103/PhysRevLett.103.152502
2007BL24 Nucl.Instrum.Methods Phys.Res. B 261, 974 (2007) D.L.Bleuel, M.A.Mcmahan, L.Ahle, B.R.Barquest, J.Cerny, L.H.Heilbronn, C.C.Jewett Characterization of a tunable quasi-monoenergetic neutron beam from deuteron breakup NUCLEAR REACTIONS Ti(d, np), Ta(d, np), E=20-29 MeV; measured products, Eπ, Iπ; deduced σ(θ, E). Data were imported from EXFOR entry C1595.
doi: 10.1016/j.nimb.2007.04.125
2007LE26 Phys.Rev. C 76, 024314 (2007) D.W.Lee, K.Perajarvi, J.Powell, J.P.O'Neil, D.M.Moltz, V.Z.Goldberg, J.Cerny Low-lying resonant states in 16F using a 15O radioactive ion beam NUCLEAR REACTIONS 1H(15O, p), E=120 MeV; measured excitation function. 16F deduced level widths.
doi: 10.1103/PhysRevC.76.024314
2006PE21 Phys.Rev. C 74, 024306 (2006) K.Perajarvi, C.Fu, G.V.Rogachev, G.Chubarian, V.Z.Goldberg, F.Q.Guo, D.Lee, D.M.Moltz, J.Powell, B.B.Skorodumov, G.Tabacaru, X.D.Tang, R.E.Tribble, B.A.Brown, A.Volya, J.Cerny Structure of 12N using 11C+p resonance scattering NUCLEAR REACTIONS 1H(11C, p), E(cm)=2.2-11.0 MeV; measured recoil proton spectra, σ(θ), excitation functions. 12N deduced levels, J, π, widths. R-matrix analysis.
doi: 10.1103/PhysRevC.74.024306
2005CE02 Nucl.Instrum.Methods Phys.Res. A540, 430 (2005) J.Cerny, Z.Dlouhy, Z.Dolezal, M.P.Ivanov, P.Kubik, E.A.Kuznetsova, Yu.E.Penionzhkevich, E.A.Sokol, J.Svejda, I.Wilhelm Neutron response function for a detector with 3He counters for the 0.39-1.54 MeV neutron energy range NUCLEAR REACTIONS 3H(p, n), E=1.2-2.3 MeV; measured neutron spectra.
doi: 10.1016/j.nima.2004.11.047
2005GU25 Phys.Rev. C 72, 034312 (2005) F.Q.Guo, J.Powell, D.W.Lee, D.Leitner, M.A.McMahan, D.M.Moltz, J.P.O'Neil, K.Perajarvi, L.Phair, C.A.Ramsey, X.J.Xu, J.Cerny Reexamination of the energy levels of 15F by 14O + 1H elastic resonance scattering NUCLEAR REACTIONS 1H(14O, p), E=120 MeV; measured recoil proton spectra, σ(θ). 15F deduced resonance energies, J, π.
doi: 10.1103/PhysRevC.72.034312
2005PE12 Nucl.Instrum.Methods Phys.Res. A546, 418 (2005) K.Perajarvi, J.Cerny, J.Hakala, J.Huikari, A.Jokinen, P.Karvonen, J.Kurpeta, D.Lee, I.Moore, H.Penttila, A.Popov, J.Aysto New ion-guide for the production of beams of neutron-rich nuclei between Z = 20 - 28 NUCLEAR REACTIONS 197Au(65Cu, X)62Co/63Co, E ≈ 400-460 MeV; measured yields. Ion-guide isotope separator. RADIOACTIVITY 63Co(β-) [from 197Au(65Cu, X)]; measured β-delayed Eγ, Iγ. Ion-guide isotope separator.
doi: 10.1016/j.nima.2005.03.124
2005PE23 Eur.Phys.J. A 25, Supplement 1, 749 (2005) K.Perajarvi, J.Cerny, U.Hager, J.Hakala, J.Huikari, A.Jokinen, P.Karvonen, J.Kurpeta, D.Lee, I.Moore, H.Penttila, A.Popov, J.Aysto Production of beams of neutron-rich nuclei between Ca and Ni using the ion-guide technique RADIOACTIVITY 63Cu(EC) [from 197Au(65Cu, X)]; measured β-delayed Eγ, Iγ. NUCLEAR REACTIONS 197Au(65Cu, X)62Cu/63Cu, E=443 MeV; measured yields.
doi: 10.1140/epjad/i2005-06-060-x
2004PE17 Eur.Phys.J. A 21, 7 (2004) K.Perajarvi, J.Cerny, L.M.Fraile, A.Jokinen, A.Kankainen, U.Koster, J.Aysto, and the ISOLDE Collaboration The beta-decay scheme of 232Fr and the K = 0 ground-state band in 232Ra RADIOACTIVITY 232Fr(β-) [from U, Th(p, X)]; measured Eγ, Iγ, γγ-coin; deduced log ft. 232Ra deduced levels, J, π, β-feeding intensities. NUCLEAR REACTIONS U(p, X)223Fr/224Fr/225Fr/226Fr/227Fr/228Fr/230Fr/232Fr, E=1, 1.4 GeV; Th(p, X)223Fr/224Fr/225Fr/226Fr/228Fr, E=1.4 GeV; measured yields.
doi: 10.1140/epja/i2004-10038-4
2002BO61 Part. and Nucl., Lett. 113, 86 (2002) N.S.Borisov, J.Broz, J.Cerny, Z.Dolezal, A.N.Fedorov, G.M.Gurevich, M.P.Ivanov, P.Kodys, P.Kubik, E.S.Kuzmin, A.B.Lazarev, F.Lehar, A.A.Lukhanin, V.N.Matafonov, A.B.Neganov, I.L.Pisarev, Yu.A.Plis, S.N.Shilov, J.Svejda, A.I.Tsvetkov, Yu.A.Usov, I.Wilhelm Experimental Research of the NN Scattering with Polarized Particles at the VdG Accelerator of Charles University. Project "NN Interactions" NUCLEAR REACTIONS 2H(polarized n, n'), E=16.2 MeV; measured polarization observables. Polarized target.
2002RO17 Phys.Rev. C65, 054310 (2002) M.W.Rowe, J.C.Batchelder, T.N.Ginter, K.E.Gregorich, F.Q.Guo, F.P.Hessberger, V.Ninov, J.Powell, K.S.Toth, X.J.Xu, J.Cerny Decay of 178Tl RADIOACTIVITY 159Ta, 170,171Ir, 171,172,173Pt, 174,175,176Au, 175,176,177,178,179Hg, 178,179,179mTl(α) [from 102Pd(78Kr, xnyp) and subsequent decay]; measured Eα, T1/2, branching ratios. 174Au, 170Ir deduced levels. 178Tl, 170,171Ir deduced mass excess. NUCLEAR REACTIONS 102Pd(78Kr, np), E=340 MeV; measured delayed Eα, αα-, (recoil)α-coin; deduced σ lower limit.
doi: 10.1103/PhysRevC.65.054310
2001BA12 Phys.Rev.Lett. 86, 1454 (2001) G.C.Ball, S.Bishop, J.A.Behr, G.C.Boisvert, P.Bricault, J.Cerny, J.M.D'Auria, M.Dombsky, J.C.Hardy, V.Iacob, J.R.Leslie, T.Lindner, J.A.Macdonald, H.-B.Mak, D.M.Moltz, J.Powell, G.Savard, I.S.Towner Precise Half-Life Measurement for the Superallowed 0+ → 0+ β Emitter 74Rb: First results from the new radioactive beam facility (ISAC) at TRIUMF RADIOACTIVITY 74Rb(β+) [from Nb(p, X)]; measured superallowed decay T1/2.
doi: 10.1103/PhysRevLett.86.1454
2000JO12 Phys.Rev.Lett. 84, 5066 (2000) R.Joosten, J.Powell, F.Q.Guo, P.E.Haustein, R.-M.Larimer, M.A.McMahan, E.B.Norman, J.P.O'Neil, M.W.Rowe, H.F.VanBrocklin, D.Wutte, X.J.Xu, J.Cerny Measurement of Excitation Functions in the Reactions 197Au(11, xn)208-xAt Using a Radioactive 11C Beam NUCLEAR REACTIONS 197Au(11C, 3n), (11C, 4n), (11C, 5n), (11C, 6n), (11C, 7n), (11C, 8n), (11C, 9n), E=60-110 MeV; measured excitation functions. Comparison with model predictions.
doi: 10.1103/PhysRevLett.84.5066
1998RO13 Phys.Rev. C57, 2222 (1998) M.W.Rowe, D.M.Moltz, T.J.Ognibene, J.Powell, J.Cerny Search for Proton Decay from a Predicted Isomer of 77Rb NUCLEAR REACTIONS 40Ca(40Ca, 3p), E=110-160 MeV; measured isomeric state production σ upper limit. Helium-jet transport, on-line mass separation.
doi: 10.1103/PhysRevC.57.2222
1997BR21 Z.Phys. A359, 23 (1997) J.Broz, J.Cerny, Z.Dolezal, G.M.Gurevich, P.Kubik, A.A.Lukhanin, G.A.Lukhanin, J.Svejda, I.Wilhelm, N.S.Borisov, E.S.Kuzmin, V.N.Matafonov, A.B.Neganov, I.L.Pisarev, Y.A.Plis, Y.A.Usov Measurement of Spin-Dependent Total Cross-Section Difference Δσ(L) in Neutron-Proton Scattering at 16 MeV NUCLEAR REACTIONS 1H(polarized n, n), E=16.2 MeV; measured longitudinal spin-dependent total σ differences; deduced 3S1-3D1 mixing parameter. Comparisons with theoretical predictions, other data. Polarized target.
doi: 10.1007/s002180050362
1996BR16 Z.Phys. A354, 401 (1996) J.Broz, J.Cerny, Z.Dolezal, G.M.Gurevich, M.Jirasek, P.Kubik, A.A.Lukhanin, J.Svejda, I.Wilhelm, N.S.Borisov, Yu.M.Kazarinov, B.A.Khachaturov, E.S.Kuzmin, V.N.Matafonov, A.B.Neganov, I.L.Pisarev, Yu.A.Plis, Yu.A.Usov, M.Rotter, B.Sedlak Measurement of Spin-Dependent Total Cross-Section Difference Δσ(T) in Neutron-Proton Scattering at 16 MeV NUCLEAR REACTIONS 1H(polarized n, X), E=16 MeV; measured spin-dependent total cross section difference; deduced 3S1-3D1 mixing parameter related features. Frozen spin target, transmission technique.
doi: 10.1007/s002180050062
1996OG01 Phys.Rev. C54, 1098 (1996) T.J.Ognibene, J.Powell, D.M.Moltz, M.W.Rowe, J.Cerny Additional Results from the β-Delayed Proton Decays of 27P and 31Cl RADIOACTIVITY 28,27P, 31Cl(β+p) [from Zn, Si(p, X), E=28, 45 MeV]; measured β-delayed Ep, Ip; deduced log ft, branching ratios, β strength function. Compared to theory.
doi: 10.1103/PhysRevC.54.1098
1995TI08 Phys.Rev. C52, R2298 (1995) R.J.Tighe, J.C.Batchelder, D.M.Moltz, T.J.Ognibene, M.W.Rowe, J.Cerny, B.A.Brown Observation of Strong Isospin Mixing in Proton Emission from the Astrophysically Interesting Isobaric Analog State in 23Mg RADIOACTIVITY 23Al(β+p) [from 24Mg(p, 2n), E=40 MeV]; measured β-delayed Ep, Ip. 23Mg deduced levels, isospin mixing in IAS decay. Shell model wave comparison.
doi: 10.1103/PhysRevC.52.R2298
1994BA54 Phys.Rev. C50, 1807 (1994) J.C.Batchelder, R.J.Tighe, D.M.Moltz, T.J.Ognibene, M.W.Rowe, J.Cerny Observation of Beta-Delayed Proton Emission from 24Al RADIOACTIVITY 24Al(β+p) [from 24Mg(p, n), E=20, 28.5 MeV]; measured β-delayed protons spectra, T1/2; deduced delayed proton branching ratio. 24Mg levels deduced proton, α-decay competition. Gas-ΔE, Si-E triple telescopes.
doi: 10.1103/PhysRevC.50.1807
1994MO42 Nucl.Instrum.Methods Phys.Res. A349, 210 (1994) D.M.Moltz, J.D.Robertson, J.C.Batchelder, J.Cerny Development of Low-Energy Proton Detector Telescopes RADIOACTIVITY 25Si(β+p) [from 24Mg(3He, 2n), E=40 MeV]; measured β-decay Ep, Ip; deduced proton detector characteristics. One or two gas ΔE detectors followed by silicon E detector.
doi: 10.1016/0168-9002(94)90622-X
1994TI03 Phys.Rev. C49, R2871 (1994) R.J.Tighe, D.M.Moltz, J.C.Batchelder, T.J.Ognibene, M.W.Rowe, J.Cerny Evidence for the Ground-State Proton Decay of 105Sb RADIOACTIVITY 25Si(β+p) [from Mg(3He, X), E=40 MeV]; 105Sb(p), (β+) [from 50Cr(58Ni, 2np), E=370, 405 MeV]; measured β-delayed Ep, Ip. 105Sb deduced ground state proton branching ratio.
doi: 10.1103/PhysRevC.49.R2871
1993BA12 Phys.Rev. C47, 2038 (1993) J.C.Batchelder, D.M.Moltz, T.J.Ognibene, M.W.Rowe, J.Cerny Beta-Delayed Proton Decay of 65Se NUCLEAR REACTIONS 40Ca(28Si, 3n), E=175 MeV; measured β-delayed Ep, Ip. RADIOACTIVITY 65Se(β+p) [from 40Ca(28Si, 3n), E=175 MeV]; measured β-delayed Ep, Ip; deduced mass excess. 65As deduced levels, β-branching ratio.
doi: 10.1103/PhysRevC.47.2038
1993BA61 Phys.Rev. C48, 2593 (1993) J.C.Batchelder, D.M.Moltz, T.J.Ognibene, M.W.Rowe, R.J.Tighe, J.Cerny Beta-Delayed Proton Decay of 73Sr RADIOACTIVITY 73Sr(β+p) [from 40Ca(36Ar, 3n), E=245 MeV]; measured beta-delayed Ep, Ip; deduced mass excess, beta-branching ratio.
doi: 10.1103/PhysRevC.48.2593
1993RO06 Phys.Rev. C47, 1455 (1993) J.D.Robertson, D.M.Moltz, T.F.Lang, J.E.Reiff, J.Cerny, B.H.Wildenthal Beta-Delayed Proton Decay of 25Si NUCLEAR REACTIONS 24Mg(3He, 2n), E=40 MeV; measured β-delayed proton spectra. RADIOACTIVITY 25Si(β+p) [from 24Mg(3He, 2n), E=40 MeV]; measured β-delayed Ep, Ip; deduced log ft. 25Al deduced levels, J, π, T, branching ratios, Gamow-Teller transition strength.
doi: 10.1103/PhysRevC.47.1455
1992MO15 Z.Phys. A342, 273 (1992) D.M.Moltz, J.C.Batchelder, T.F.Lang, T.J.Ognibene, J.Cerny, P.E.Haustein, P.L.Reeder Beta-Delayed Two-Proton Decay of 39Ti RADIOACTIVITY 39Ti(β+p) [from Ca(3He, X), E=110 MeV]; measured two-proton energy sum spectra following β-decay; deduced decay scheme, energy available for two-proton emission. 39Sc deduced IAS.
doi: 10.1007/BF01291509
1990LA14 Phys.Rev. C42, R1175 (1990) T.F.Lang, D.M.Moltz, J.E.Reiff, J.C.Batchelder, J.Cerny, J.D.Robertson, C.W.Beausang Identification of the πg9/2 Band in 67As NUCLEAR REACTIONS 40Ca(32S, pα), (33S, pnα), E=95-110 MeV; measured Eγ, Iγ, γγ(θ), γ(θ), γγ-, nγγ-, αγγ-coin. 67As deduced levels, J, π.
doi: 10.1103/PhysRevC.42.R1175
1990RO15 Phys.Rev. C42, 1922 (1990) J.D.Robertson, J.E.Reiff, T.F.Lang, D.M.Moltz, J.Cerny Search for Ground State Proton Emission from 65As and 69Br RADIOACTIVITY 65As [from 40Ca(28Si, 2np), E=175 MeV; 40Ca(32S, 2npα), E=200 MeV]; 69Br [from 40Ca(32S, 2np), E=200 MeV]; measured β-delayed proton emission T1/2 upper limit.
doi: 10.1103/PhysRevC.42.1922
1989RE02 Nucl.Instrum.Methods Phys.Res. A276, 228 (1989) J.E.Reiff, M.A.C.Hotchkis, D.M.Moltz, T.F.Lang, J.D.Robertson, J.Cerny A Fast In-Beam Recoil Catcher Wheel and the Observation of Beta-Delayed Two-Proton Emission from 31Ar NUCLEAR REACTIONS Mg(3He, X), E=110, 135 MeV; measured β-delayed proton spectra for 17Ne, 21Mg, 25Si, 22Al, 31Ar. Fast in-beam recoil catcher foil wheel. RADIOACTIVITY 17Ne, 21Mg, 25Si(β+p) [from Mg(3He, X), E=110 MeV]; measured β-delayed proton spectra. 22Al, 31Ar(β+p) [from Mg(3He, X), E=135 MeV]; measured β-delayed two-proton spectra. 31Ar deduced Q(EC), mass excess, possible T1/2, decay systematics. 31Cl deduced IAS energy, possible decay systematics.
doi: 10.1016/0168-9002(89)90637-2
1988ZH15 Chin.J.Nucl.Phys. 10, 351 (1988) Zhou Zongyuan, J.Cerny, M.Cable, J.Honkanen, R.Parry Measurement of Half-Life of the β-Delayed Two-Proton Decay Nuclide 22Al RADIOACTIVITY 22Al(β+p); measured T1/2. Helium jet system.
1988ZH18 High Energy Phys. and Nucl.Phys. (China) 12, 246 (1988) Z.Zhou, J.Cerny, M.Cable, J.Honkanen, R.Parry Half-life measurement of the β-delayed two-proton decay nuclide 26P
1987BL14 Nucl.Instrum.Methods Phys.Res. B26, 328 (1987) F.B.Blonnigen, D.M.Moltz, T.F.Lang, W.F.Knoll, X.Xu, M.A.C.Hotchkis, J.E.Reiff, J.Cerny Improvements to the Helium-Jet Coupled On-Line Mass Separator RAMA NUCLEAR REACTIONS 142Nd(16O, xn)153Er, E=120 MeV; measured Eα, Iα. Improved on-line mass separator.
doi: 10.1016/0168-583X(87)90772-5
1987HO01 Phys.Rev. C35, 315 (1987) M.A.C.Hotchkis, J.E.Reiff, D.J.Vieira, F.Blonnigen, T.F.Lang, D.M.Moltz, X.Xu, J.Cerny Beta-Delayed Proton Decay of 61Ge RADIOACTIVITY 61Ge(β+p) [from 40Ca(24Mg, 3n), (28Si, α3n), E=73-128 MeV]; measured β-delayed Ep, T1/2. 61Ga deduced levels, possible J, π. ΔE-E telescopes.
doi: 10.1103/PhysRevC.35.315
1987SE07 Nucl.Phys. A467, 93 (1987) T.Sekine, J.Cerny, R.Kirchner, O.Klepper, V.T.Koslowsky, A.Plochocki, E.Roeckl, D.Schardt, B.Sherrill, B.A.Brown The Beta Decay of 48Mn: Gamow-Teller quenching in fp-shell nuclei NUCLEAR STRUCTURE 48V, 48Cr; calculated levels. 44V, 48Ca; calculated Gamow-Teller transition strength distribution. Shell model. RADIOACTIVITY 48Mn(β+p) [from 12C(40Ca, 3np), E=11.4 MeV/nucleon]; measured β-delayed E(p), I(p), Eγ, βγ-, γγ-coin, T1/2; deduced log ft. 48Cr deduced levels, I(β), γ-branching. Plastic scintillator, Ge(Li), surface barrier Si detectors. On-line mass separation.
doi: 10.1016/0375-9474(87)90330-7
1985AY01 Phys.Rev.Lett. 55, 1384 (1985) J.Aysto, D.M.Moltz, X.J.Xu, J.E.Reiff, J.Cerny Observation of the First T(z) = -5/2 Nuclide, 35Ca via Its β-Delayed Two-Proton Emission NUCLEAR REACTIONS 40Ca(3He, 4nα), E=135 MeV; measured β-delayed two-proton spectra, Ep, Ip. 35Ca deduced mass excess. Natural Ca target. RADIOACTIVITY 35Ca(β+2p) [from 40Ca(3He, 4nα), E=135 MeV]; measured β-delayed two-proton sum spectra, pp-coin, Ep, Ip; deduced T=1/2, (5/2)+ level decay characteristics, approximate T1/2. 35K level deduced proton decay characteristics. 34Ar, 33Cl levels deduced proton branching characteristics.
doi: 10.1103/PhysRevLett.55.1384
1985AY02 Phys.Rev. C32, 1700 (1985) J.Aysto, X.J.Xu, D.M.Moltz, J.E.Reiff, J.Cerny, B.H.Wildenthal Beta-Delayed Proton Decays of 27P and 31Cl: Gamow-Teller decays with large Q values RADIOACTIVITY 27P(β+p) [from 28Si(p, 2n), E=28-50 MeV]; 31Cl(β+p) [from 32S(p, 2n), E=28-50 MeV]; measured β-delayed Ep, Ip, T1/2; deduced β-branching, log ft. 27Si, 31S deduced Gamow-Teller strength function, levels, proton branching.
doi: 10.1103/PhysRevC.32.1700
1985JA07 Phys.Rev. C31, 1576 (1985) R.Jahn, R.L.McGrath, D.M.Moltz, J.E.Reiff, X.J.Xu, J.Aysto, J.Cerny Angular Correlations in the Beta-Delayed Two-Proton Decay of 22Al RADIOACTIVITY 22Al(β+p) [from 24Mg(3He, 4np), E=110 MeV]; measured β-delayed pp(θ); deduced decay scheme, diproton emission probability. 22Mg, 21Na levels deduced decay characteristics.
doi: 10.1103/PhysRevC.31.1576
1985ZH05 Phys.Rev. C31, 1941 (1985) Z.Y.Zhou, E.C.Schloemer, M.D.Cable, M.Ahmed, J.E.Reiff, J.Cerny Additional Beta-Delayed Protons form the T(z) = -(3/2) Nuclei 21Mg, 25Si, 29S, and 41Ti RADIOACTIVITY 21Mg, 25Si, 29S, 41Ti(β+p) [from 20Ne, 24Mg, 28Si, 40Ca(3He, 2n), E=31.5-41.5 MeV]; measured β-delayed Ep, Ip; deduced log ft. 21Na, 25Al, 29P, 41Sc levels deduced relative Ip.
doi: 10.1103/PhysRevC.31.1941
1984CA29 Phys.Rev. C30, 1276 (1984) M.D.Cable, J.Honkanen, E.C.Schloemer, M.Ahmed, J.E.Reiff, Z.Y.Zhou, J.Cerny Beta-Delayed Two-Proton Decays of 22Al and 26P RADIOACTIVITY 22Al(β+p) [from 24Mg(3He, p4n)]; 26P(β+p) [from 28Si(3He, p4n)]; measured beta-delayed two-proton pp-coin, Ep. 21Na, 25Al deduced levels, p-branching.
doi: 10.1103/PhysRevC.30.1276
1983CA01 Phys.Rev.Lett. 50, 404 (1983) M.D.Cable, J.Honkanen, R.F.Parry, S.H.Zhou, Z.Y.Zhou, J.Cerny Discovery of Beta-Delayed Two-Proton Radioactivity: 22Al RADIOACTIVITY 22Al(β+p) [from 24Mg(3He, 4np), E=110 MeV]; measured β-delayed pp-coin, total E(2p); deduced 2p, 1p emission relative intensity. Single step 2He emission, 21Na intermediate state sequential decay discussed.
doi: 10.1103/PhysRevLett.50.404
1983CA06 Phys.Lett. 123B, 25 (1983) M.D.Cable, J.Honkanen, R.F.Parry, S.H.Zhou, Z.Y.Zhou, J.Cerny Beta-Delayed Proton Decay of the T(z) = -2 Isotope 26P NUCLEAR REACTIONS 28Si(3He, 4np), E=110-130 MeV; measured Ep, Ip; deduced evidence for 26P. RADIOACTIVITY 26P(β+p) [from 28Si(3He, 4np), E=110-130 MeV]; measured β-delayed Ep, Ip. 26P deduced T1/2. 26Si deduced T=2 level mass excess.
doi: 10.1016/0370-2693(83)90950-4
1983HO23 Phys.Lett. 133B, 146 (1983) J.Honkanen, M.D.Cable, R.F.Parry, S.H.Zhou, Z.Y.Zhou, J.Cerny Beta-Delayed Two-Proton Decay of 26P RADIOACTIVITY 26P(β+p) [from 28Si(3He, xnyp), E=110 MeV]; measured β-delayed two-proton Ep, Ip, summed spectra; deduced two-proton emission mechanism, decay scheme.
doi: 10.1016/0370-2693(83)90547-6
1983WO04 Phys.Rev. C27, 1745 (1983) J.M.Wouters, H.M.Thierens, J.Aysto, M.D.Cable, P.E.Haustein, R.F.Parry, J.Cerny Beta-decay Energies and Masses of 103-105In RADIOACTIVITY 103In(β+), (EC) [from 92Mo(14N, 3n), E=80 MeV, 92Mo(16O, 4np), E=115 MeV]; 104In(β+), (EC) [from 92Mo(16O, 3np), E=95 MeV]; 105In(β+), (EC) [from Mo(14N, xn), E=100 MeV, 92Mo(16O, 2np), E=75 MeV]; measured βγ-coin, Eβ+; deduced Q(EC), mass excesses. On-line mass separated sources, enriched Mo targets, Ge(Li), scintillation telescope detectors.
doi: 10.1103/PhysRevC.27.1745
1982BI09 Nucl.Phys. A390, 161 (1982) A.N.Bice, A.C.Shotter, J.Cerny 12C and 8Be Production in 12C + 208Pb Collisions NUCLEAR REACTIONS 208Pb(12C, 12C'), (12C, 8Be), (12C, α), E=132, 187, 230 MeV; measured σ(absolute), σ(θ, E(α)), σ(θ), αd-coin; deduced reaction mechanism, projectile breakup contribution.
doi: 10.1016/0375-9474(82)90609-1
1982CA16 Phys.Rev. C26, 1778 (1982) M.D.Cable, J.Honkanen, R.F.Parry, H.M.Thierens, J.M.Wouters, Z.Y.Zhou, J.Cerny Beta-Delayed Proton Decay of an Odd-Odd T(z) = (-2) Isotope, 22Al RADIOACTIVITY 22Al(β+), (p) [from 24Mg(3He, 4np), E=110 MeV]; measured β-delayed Ep, Ip, T1/2. 22Mg level deduced mass excess, Iβ.
doi: 10.1103/PhysRevC.26.1778
1982SH01 J.Phys.(London) G8, 355 (1982) A.C.Shotter, A.N.Bice, D.P.Stahel, J.Cerny The Break-Up of 187 MeV 12C Ions into the 3α Channel NUCLEAR REACTIONS 208Pb(12C, 3α), E=187 MeV; measured σ(Eα), αα-coin, σ(quasielastic) vs θ; deduced projectile breakup mechanism.
doi: 10.1088/0305-4616/8/3/006
1982SH21 Phys.Lett. 116B, 99 (1982) R.Shyam, M.A.Nagarajan, A.C.Shotter, A.N.Bice, J.Cerny Inelastic Scattering of 12C from 208Pb to the Second 0+ State of 12C NUCLEAR REACTIONS 208Pb(12C, 12C'), E=132, 187, 230 MeV; measured σ(θ); deduced real potential characteristics. Microscopic DWBA, folding model.
doi: 10.1016/0370-2693(82)90984-4
1981AY01 Phys.Rev. C23, 879 (1981) J.Aysto, M.D.Cable, R.F.Parry, J.M.Wouters, D.M.Moltz, J.Cerny Decays of the T(z) = -2 Nuclei 20Mg, 24Si, and 36Ca RADIOACTIVITY 20Mg, 24Si, 36Ca [from Ne, Mg, Ca(3He, 3n), (3He, 3nα), E=40-100 MeV, mass separation]; measured β-delayed Ep, Ip; deduced T1/2, proton-branching; deduced coefficients of isobaric multiplet mass equation. 20Na, 24Al, 36K level deduced mass excess.
doi: 10.1103/PhysRevC.23.879
1981BI07 Phys.Lett. 101B, 27 (1981) A.N.Bice, A.C.Shotter, D.P.Stahel, J.Cerny Investigation of the (10B, 6Li(3+, 2.18 MeV)) Reaction as a Method for α-Cluster Transfer Studies NUCLEAR REACTIONS 12C(10B, 6Li), E=68 MeV; measured σ(θ, E(6Li')), αd-coin. Monte Carlo calculations.
doi: 10.1016/0370-2693(81)90481-0
1981SH01 Phys.Rev.Lett. 46, 12 (1981) A.C.Shotter, A.N.Bice, J.M.Wouters, W.D.Rae, J.Cerny Observation of the Direct and Sequential Breakup of 7Li from 12C and 208Pb Targets at 70 MeV NUCLEAR REACTIONS 12C, 208Pb(7Li, t), E=70 MeV; measured tα-coin, σ(θ(7Li')), σ(Et, θ). 7Li deduced direct, sequential breakup, α + t cluster structure of underlying level.
doi: 10.1103/PhysRevLett.46.12
1979AY01 Phys.Lett. 82B, 43 (1979) J.Aysto, D.M.Moltz, M.D.Cable, R.D.Von Dincklage, R.F.Parry, J.M.Wouters, J.Cerny Decay of a New Isotope, 24Si: A Test of the Isobaric Multiplet Mass Equation RADIOACTIVITY 24Si [from 24Mg(3He, 3n), E=70 MeV]; measured σ(Ep) of β-delayed protons; deduced T1/2. 24Al level deduced mass excess, fit to quadratic isobaric multiplet mass equation.
doi: 10.1016/0370-2693(79)90421-0
1979MO02 Phys.Rev.Lett. 42, 43 (1979) D.M.Moltz, J.Aysto, M.D.Cable, R.D.von Dincklage, R.F.Parry, J.M.Wouters, J.Cerny Completion of the Mass-20 Isospin Quintet by Employing a Helium-Jet-Fed on-Line Mass Separator RADIOACTIVITY 20Mg [from 20Ne(3He, n)]; measured β-delayed protons. 20Na deduced mass excess. Recoil-atom analyzer. Evidence for quadratic form of isobaric multiplet mass equation.
doi: 10.1103/PhysRevLett.42.43
1979ST15 Phys.Rev. C20, 1680 (1979) D.P.Stahel, R.Jahn, G.J.Wozniak, J.Cerny Charge-Exchange Reaction (d, 2He) NUCLEAR REACTIONS 6Li, 10B, 12C(d, 2p), E=55 MeV; measured σ(Ep1, Ep2, θ). Microscopic DWBA analysis. Kinematically complete experiment.
doi: 10.1103/PhysRevC.20.1680
1979VI01 Phys.Rev. C19, 177 (1979) D.J.Vieira, R.A.Gough, J.Cerny β-Delayed Proton Decay of 29S RADIOACTIVITY 29S [from 28Si(3He, 2n), E=32 MeV]; measured β-delayed protons, T1/2. 29P deduced levels, IAS-proton decay, log ft. Comparison with shell model.
doi: 10.1103/PhysRevC.19.177
1978JA10 Phys.Rev. C18, 9 (1978) R.Jahn, D.P.Stahel, G.J.Wozniak, R.J.de Meijer, J.Cerny Survey of the (α, 2He) Reaction on 1p- and 2s 1d-Shell Nuclei NUCLEAR REACTIONS 12,13C, 14,15N, 16,18O, 20,22Ne, 26Mg, 28,29Si, 32S, 36,38Ar(α, 2p), E=65 MeV; 40Ca(α, 2p), E=55 MeV; measured pp-coin, σ(θ). 14,15C, 16,17N, 18,20O, 22,24Ne, 28Mg, 30,31Si, 34S, 40,38Ar deduced levels, J, π, character.
doi: 10.1103/PhysRevC.18.9
1978JA22 Fizika, Suppl. 10, 33 (1978) R.Jahn, D.P.Stahel, G.J.Wozniak, R.J.de Meijer, J.Cerny Survey of the (α, 2He) Reaction on 1p- and 2s1d-Shell Nuclei NUCLEAR REACTIONS 12,13C, 14,15N, 16,18O, 20,22Ne, 24,26Mg, 28,29Si, 32S, 36,38Ar, 40Ca(α, 2p), E=55, 65 MeV; measured σ; deduced reaction mechanism.
1978KE06 Phys.Rev. C17, 1929 (1978) G.J.KeKelis, M.S.Zisman, D.K.Scott, R.Jahn, D.J.Vieira, J.Cerny, F.Ajzenberg-Selove Masses of the Unbound Nuclei 16Ne, 15F, and 12O NUCLEAR REACTIONS 16O, 20Ne(α, 8He), E=117 MeV; 20Ne(3He, 8Li), E=75, 88 MeV; measured σ(θ); deduced Q. 12O, 15F, 16Ne deduced mass excess, Γ(cm), diproton decay.
doi: 10.1103/PhysRevC.17.1929
1977CE05 Ann.Rev.Nucl.Part.Sci. 27, 333 (1977) Delayed Proton Radioactivities RADIOACTIVITY 9C, 13O, 17Ne, 21Mg, 25Si, 29S, 33Ar, 37Ca, 41Ti, 45Cr, 49Fe, 53Ni, 57Zn, 61Ge, 23Al, 65Ge, 69Se, 73Kr, 77Sr, 81Sr, 99Cd, 109,111Te, 113,115,117Xe, 114,116,118,120Cs, 117,119,121Ba, 129,131Nd, 133,135Sm, 179,181,183Hg(β+p); compiled, analyzed beta-delayed proton decay data.
doi: 10.1146/annurev.ns.27.120177.002001
1977ST20 Phys.Rev. C16, 1456 (1977) D.P.Stahel, G.J.Wozniak, M.S.Zisman, B.D.Jeltema, J.Cerny (9Be, 8Be) Reaction at 50 MeV NUCLEAR REACTIONS 12C, 16O, 26Mg, 28Si, 40Ca, 208Pb(9Be, 8Be), 12C, 28Si, 40Ca, 208Pb(9Be, 9Be), E=50 MeV; measured σ(θ). 13C, 17O, 27Mg, 29Si, 41Ca, 209Pb levels deduced relative, absolute S.
doi: 10.1103/PhysRevC.16.1456
1977WE03 Nucl.Phys. A280, 217 (1977) R.B.Weisenmiller, N.A.Jelley, D.Ashery, K.H.Wilcox, G.J.Wozniak, M.S.Zisman, J.Cerny Very Light Neutron-Rich Nuclei Studied with the (6Li, 8B) Reaction NUCLEAR REACTIONS 6Li(6Li, 8B), 7Li(6Li, 8B), 9Be(6Li, 8B), 11B(6Li, 8B), E=80.0, 93.3 MeV; measured σ(θ). 4H, 7He, 9Li deduced structure parameters.
doi: 10.1016/0375-9474(77)90305-0
1976AS01 Phys.Rev. C13, 1345 (1976) D.Ashery, M.S.Zisman, G.W.Goth, G.J.Wozniak, R.B.Weisenmiller, J.Cerny T = 2 States in 12C and 12B NUCLEAR REACTIONS 14C(p, t), (p, 3He), E=54 MeV; measured σ(θ). 14C(p, pt), (p, tα), E=54 MeV; measured pt-, tα-coin. 12C, 12B deduced IAS, J.
doi: 10.1103/PhysRevC.13.1345
1976HI10 Phys.Rev.Lett. 37, 130 (1976) G.T.Hickey, D.C.Weisser, J.Cerny, G.M.Crawley, A.F.Zeller, T.R.Ophel, D.F.Hebbard Use of the Four-Neutron Transfer Reaction 18O(18O, 14O)22O to Determine The Mass of 22O NUCLEAR REACTIONS 18O(18O, 14O), E=100 MeV; measured σ; deduced Q. 22O deduced mass excess.
doi: 10.1103/PhysRevLett.37.130
1976JA13 Phys.Rev.Lett. 37, 812 (1976) R.Jahn, G.J.Wozniak, D.P.Stahel, J.Cerny (α, 2He) Reaction as a Spectroscopic Tool for Investigating High-Spin States NUCLEAR REACTIONS 12,13C, 16O(α, 2p), E=65 MeV; measured σ(θ), pp-coin.
doi: 10.1103/PhysRevLett.37.812
1976JA17 Phys.Lett. 65B, 339 (1976) R.Jahn, D.P.Stahel, G.J.Wozniak, J.Cerny, H.P.Morsch Monopole Excitation of 4He in α-Particle Scattering from 12C, 13C, and 16O NUCLEAR REACTIONS 12,13C, 16O(α, α'), E=65 MeV; measured pt-coin, σ(θ). 4He deduced E0 transition.
doi: 10.1016/0370-2693(76)90237-9
1976VI02 Phys.Lett. 60B, 261 (1976) D.J.Vieira, D.F.Sherman, M.S.Zisman, R.A.Gough, J.Cerny Extension of the T(z) = -3/2 Beta-Delayed Proton Precursor Series to 57Zn RADIOACTIVITY 53Ni(β+)[from 40Ca(16O, 3n)], 57Zn(β+)[from 40Ca (20Ne, 3n)]; measured β-delayed protons, Ep, T1/2. 53Co, 57Cu; deduced levels.
doi: 10.1016/0370-2693(76)90295-1
1976WE09 Phys.Rev. C13, 1330 (1976) R.B.Weisenmiller, N.A.Jelley, K.H.Wilcox, G.J.Wozniak, J.Cerny Spectroscopic Utility of the Two-Proton Pickup (6Li, 8β) Reaction NUCLEAR REACTIONS 10B, 12,13C, 16O(6Li, 8B), E=80, 93 MeV; measured σ(E(8B), θ) to levels in 8Li, 10,11Be, 14C.
doi: 10.1103/PhysRevC.13.1330
1976WO11 Phys.Rev. C14, 815 (1976) G.J.Wozniak, D.P.Stahel, J.Cerny, N.A.Jelley (α, 8Be) Reaction in the 1p Shell NUCLEAR REACTIONS 9Be, 10,11B, 12,13C, 14,15N, 16O(α, 8Be), E=65-72.5 MeV; measured σ(E(8Be), θ). 5He, 6,7Li, 8,9Be, 10,11B, 12C levels deduced absolute, relative S α, L. DWBA analysis.
doi: 10.1103/PhysRevC.14.815
1975GE01 Phys.Rev.Lett. 34, 326 (1975) D.F.Geesaman, R.Malmin, R.L.McGrath, J.W.Noe, J.Cerny 52Fe(6.8 MeV) β-Decaying Isomeric State NUCLEAR REACTIONS 40Ca(14N, np), E=46 MeV; measured βγ(t). 52Fe deduced isomer J, π, T1/2, decay. RADIOACTIVITY 52Fe(β+) [from 40Ca(14N, np), E=46 MeV]; measured βγ(t). 52Fe deduced isomer J, π, T1/2, decay.
doi: 10.1103/PhysRevLett.34.326
1975JE02 Phys.Rev. C11, 2049 (1975) N.A.Jelley, J.Cerny, D.P.Stahel, K.H.Wilcox Predictions of the Masses of Highly Neutron-Righ Light Nuclei ATOMIC MASSES A=8-43; calculated mass excess, p-, n-binding energy, Q.
doi: 10.1103/PhysRevC.11.2049
1975WI26 Phys. Lett. 59B, 142 (1975) K.H.Wilcox, R.B.Weisenmiller, G.J.Wozniak, N.A.Jelley, D.Ashery, J.Cerny The (9Be, 8B) Reaction and the Unbound Nuclide 10Li NUCLEAR REACTIONS 9Be(9Be, 8B), E=121 MeV; measured σ(E(8B), θ); deduced Q. 10Li deduced mass excess.
doi: 10.1016/0370-2693(75)90687-5
1974CE05 Phys.Rev. C10, 2654 (1974) J.Cerny, N.A.Jelley, D.L.Hendrie, C.F.Maguire, J.Mahoney, D.K.Scott, R.B.Weisenmiller A More Accurate Mass for 8He NUCLEAR REACTIONS 26Mg(α, 8He), E=110.6 MeV; measured σ(E(8He)). 8He deduced mass excess. 8C, 20Mg; calculated mass excess.
doi: 10.1103/PhysRevC.10.2654
1974CE06 Phys.Lett. 53B, 247 (1974) J.Cerny, R.B.Weisenmiller, N.A.Jelley, K.H.Wilcox, G.J.Wozniak 7Li + 7Li Reaction Studies Leading to Multi-Neutron Final States NUCLEAR REACTIONS 7Li(7Li, X), (16O, X), (7Li, 11C), (7Li, 11B), (7Li, 12B), (7Li, 10C), E=79.6 MeV; measured σ.
doi: 10.1016/0370-2693(74)90471-7
1974JE01 Phys.Rev. C9, 2067 (1974) N.A.Jelley, K.H.Wilcox, R.B.Weisenmiller, G.J.Wozniak, J.Cerny Masses for 43Ar and the New Isotopes 45Ar and 46Ar NUCLEAR REACTIONS 48Ca(α, 9Be), (α, 7Be), (6Li, 8B), Eα=78 MeV, E(6Li)=80 MeV; measured σ(E(9Be), E(7Be), E(8B)), Q. 43,45,46Ar deduced levels.
doi: 10.1103/PhysRevC.9.2067
1974MA12 Phys.Rev. C9, 1694 (1974) J.A.Macdonald, J.Cerny, J.C.Hardy, H.L.Harney, A.D.Bacher, G.R.Plattner Analyzing Powers for Two-Nucleon Transfer Reactions in the 1p Shell NUCLEAR REACTIONS 16O, 15N(p, t), (p, 3He), E=43.8 MeV; 13C(p, t), (p, 3He), E=49.6 MeV; measured σ(Et, E(3He), θ), A(θ). 14O, 13,14N, 11,13C, 11B deduced levels, L.
doi: 10.1103/PhysRevC.9.1694
1974SE11 Nucl.Phys. A234, 130 (1974) R.G.Sextro, R.A.Gough, J.Cerny High-Resolution Measurements of Beta-Delayed Protons from 37Ca and 41Ti RADIOACTIVITY 41Ti [from 40Ca(3He, 2n)]; 37Ca [from 36Ar(3He, 2n), 40Ca(3He, 2nα)]; 40Sc [from 40Ca(p, n), (3He, 2np)]; measured delayed p, T1/2, Ep, Ip. 41Sc, 37K, 40Ca deduced levels, log ft. Natural 40Ca target, enriched 36Ar target.
doi: 10.1016/0375-9474(74)90383-2
1973GO06 Phys.Lett. 43B, 33 (1973) R.A.Gough, R.G.Sextro, J.Cerny On the Lowest T = 3/2 State in 41Sc RADIOACTIVITY 41Ti, 21Mg, 29S; measured β-delayed proton spectra; deduced Q. 29P deduced mass excess. 41Sc deduced T=3/2 state.
doi: 10.1016/0370-2693(73)90537-6
1973MA47 Phys.Lett. 47B, 237 (1973) J.A.MacDonald, N.A.Jelley, J.Cerny Analyzing Powers in 208Pb(p, t)206Pb Transitions NUCLEAR REACTIONS 208Pb(polarized p, t), E=40 MeV; measured σ(Et, θ), A(θ). 206Pb deduced transitions.
doi: 10.1016/0370-2693(73)90719-3
1973SE08 Phys.Rev. C8, 258 (1973) R.G.Sextro, R.A.Gough, J.Cerny β+-Delayed-Proton Decay of 21Mg RADIOACTIVITY 21Mg; measured T1/2, delayed protons. Deduced β+-branching, log ft. 21Na deduced levels, J, π, α-branching. 20Na measured delayed alphas.
doi: 10.1103/PhysRevC.8.258
1973WI06 Phys.Rev.Lett. 30, 866 (1973) K.H.Wilcox, N.A.Jelley, G.J.Wozniak, R.B.Weisenmiller, H.L.Harney, J.Cerny New Spectroscopic Measurements via Exotic Nuclear Rearrangement; the Reaction 26Mg(7Li, 8B)25Ne NUCLEAR REACTIONS 26Mg(7Li, 8B), E=79 MeV; measured σ(E(8B)), Q. 25Ne deduced levels.
doi: 10.1103/PhysRevLett.30.866
1973WO06 Phys.Rev.Lett. 31, 607 (1973) G.J.Wozniak, N.A.Jelley, J.Cerny Feasibility of α-Transfer Studies via the (α, 8Be) Reaction at High Energies NUCLEAR REACTIONS 11B, 12C, 16O(α, 8Be), 11B(α, 7Li), E=65 MeV; measured σ(E(8Be)), σ(θ), σ(E(7Li)).
doi: 10.1103/PhysRevLett.31.607
1972CE01 Nucl.Phys. A188, 666 (1972) J.Cerny, R.A.Gough, R.G.Sextro, J.E.Esterl Further Results on the Proton Radioactivity of 53mCo RADIOACTIVITY 53mCo; measured direct proton Ep, T1/2; deduced partial half-life; searched for second proton decay branch.
doi: 10.1016/0375-9474(72)90226-6
1972ES05 Phys.Rev. C6, 373 (1972) J.E.Esterl, D.Allred, J.C.Hardy, R.G.Sextro, J.Cerny β-Delayed Proton Decay of 9C RADIOACTIVITY 9C; measured β-delayed p-spectrum, T1/2.
doi: 10.1103/PhysRevC.6.373
1972GO03 Phys.Rev.Lett. 28, 510 (1972) R.A.Gough, R.G.Sextro, J.Cerny β-Delayed Proton Emission of 23Al RADIOACTIVITY 23Al; measured T1/2, delayed-p spectrum. NUCLEAR REACTIONS 24Mg(p, 2n), E=30-40 MeV; measured σ(E), delayed-p spectrum.
doi: 10.1103/PhysRevLett.28.510
1972MA21 Phys.Lett. 38B, 504 (1972) High-Spin Assignments in the 1p-Shell Obtained with the J-Dependent (p, α) Reaction NUCLEAR REACTIONS 16O, 12,13C, 14,15N(p, α), E=54, 43.7, 50.5 MeV; measured σ(Eα, θ). 11,12C, 13N, 9B, 10B levels deduced L. 9B, 13N high-lying states deduced J, π.
doi: 10.1016/0370-2693(72)90528-X
1972WO10 Phys.Rev.Lett. 28, 1278 (1972); Erratum Phys.Rev.Lett. 29, 760 (1972) G.J.Wozniak, H.L.Harney, K.H.Wilcox, J.Cerny α-Particle Transfer via the (12C, 8Be) Reaction: Application to Studies of 16O and 20Ne NUCLEAR REACTIONS 12C(12C, 8Be), 16O(12C, 8Be), E=62.6 MeV; measured σ(E(8Be)). 16O, 20Ne deduced levels.
doi: 10.1103/PhysRevLett.28.1278
1971CE02 Phys.Lett. 37B, 380 (1971) J.Cerny, D.R.Goosman, D.E.Alburger A Highly Neutron-Deficient Vanadium Isotope: 44V RADIOACTIVITY 44V[from 40Ca(6Li, 2n)]; measured T1/2, β-delayed α-spectra.
doi: 10.1016/0370-2693(71)90209-7
1971FL04 Nucl.Phys. A162, 225 (1971) D.G.Fleming, J.C.Hardy, J.Cerny Spin Dependence in the Reactions 16O(p, t)14O and 16O(p, 3He)14N NUCLEAR REACTIONS 16O(p, t), 16O(p, 3He), Ep=43.7, 54.1 MeV; measured σ(θ). 14N, 14O deduced levels, J, π, T, isobaric analogs.
doi: 10.1016/0375-9474(71)90981-X
1971HA05 Phys.Rev. C3, 700 (1971) J.C.Hardy, J.E.Esterl, R.G.Sextro, J.Cerny Isospin Purity and Delayed-Proton Decay: 17Ne and 33Ar RADIOACTIVITY 17Ne, 33Ar; measured β-delayed proton spectra, Eγ, Iγ, T1/2, pγ-coin; deduced log ft. 9C; measured T1/2. 17F deduced levels, antianalog state, isospin mixing. 33Cl deduced levels, isospin mixing.
doi: 10.1103/PhysRevC.3.700
1971HA10 Nucl.Phys. A162, 552 (1971) J.C.Hardy, J.M.Loiseaux, J.Cerny, G.T.Garvey The Reactions 11B(p, 3He)9Be and 11B(p, t)9B: Is There Strong Isospin Mixing in Mass 9 (Question) NUCLEAR REACTIONS 11B(p, t), (p, 3He), E=45 keV; measured σ(Et, θ), σ(E(3He), θ). 9B, 9Be deduced levels J, π, T, L, isobaric analogs. Enriched target.
doi: 10.1016/0375-9474(71)90254-5
1971MC04 Phys.Lett. 34B, 289 (1971) R.L.McGrath, D.L.Hendrie, E.A.McClatchie, B.G.Harvey, J.Cerny The (d, 6Li) Reaction on Light Nuclei NUCLEAR REACTIONS 12C, 16O, 20Ne, 24,25Mg(d, 6Li), E=55 MeV; measured σ(E(6Li)).
doi: 10.1016/0370-2693(71)90607-1
1970BA41 Nucl.Phys. A153, 409 (1970) A.D.Bacher, R.L.McGrath, J.Cerny, R.de Swiniarski, J.C.Hardy, R.J.Slobodrian The (3He, 6He) Reaction on 6Li and 7Li NUCLEAR REACTIONS 6,7Li(3He, 6He), E=53.2 MeV; measured σ(E(6He)) at θ=14.1°. 4Li deduced no T=2 states. Enriched target.
doi: 10.1016/0375-9474(70)90779-7
1970CE02 Phys.Rev.Lett. 24, 1128 (1970) J.Cerny, C.U.Cardinal, H.C.Evans, K.P.Jackson, N.A.Jelley 49Fe: A New T(z) = -3/2 Delayed-Proton Emitter RADIOACTIVITY 49Fe[from 40Ca(12C, 3n)]; measured T1/2, delayed proton spectrum. 33Ar; measured delayed proton spectrum. NUCLEAR REACTIONS 24Mg, 28Si(12C, 3n), 40Ca(12C, 3n), E=65 MeV; measured delayed proton spectrum.
doi: 10.1103/PhysRevLett.24.1128
1970CE03 Phys.Rev.Lett. 25, 676 (1970) J.Cerny, C.U.Cardinal, K.P.Jackson, D.K.Scott, A.C.Shotter Heavy-Ion Reactions as a Technique for Direct Mass Measurements of Unknown Z > N Nuclei NUCLEAR REACTIONS 40Ca(12C, t), (12C, 3He), E=27.5 MeV; measured σ(Et), σ(E(3He)). 49Mn deduced mass.
doi: 10.1103/PhysRevLett.25.676
1970CE04 Phys.Lett. 33B, 284 (1970) J.Cerny, J.E.Esterl, R.A.Gough, R.G.Sextro Confirmed Proton Radioactivity of 53mCo NUCLEAR REACTIONS 54Fe(p, 2n), E=25-45 MeV; measured σ(E), delayed-p spectrum. 53mCo deduced T1/2.
doi: 10.1016/0370-2693(70)90270-4
1970ES03 Phys.Lett. 33B, 287 (1970) J.E.Esterl, J.C.Hardy, R.G.Sextro, J.Cerny Beta-Delayed Proton Decay of 13O: A Violation of Mirror Symmetry RADIOACTIVITY 13O; measured delayed-p spectrum, T1/2; deduced log ft.
doi: 10.1016/0370-2693(70)90271-6
1970HA10 Phys.Rev. C1, 561 (1970) J.C.Hardy, H.Brunnader, J.Cerny T=2 and T=3 Analog States, 28 < A < 40 NUCLEAR REACTIONS 30Si, 34S, 38Ar, 40Ar, 42Ca(p, t), (p, 3He), E=45 MeV; measured σ(Et, θ), σ(E(3He), θ). 28Al, 28Si, 32P, 32S, 36Cl, 36Ar, 40K, 40Ca deduced T=2 isobaric analog states. 38Cl, 38Ar deduced T=3 isobaric analog states.
doi: 10.1103/PhysRevC.1.561
1970JA22 Phys.Lett. 33B, 281 (1970) K.P.Jackson, C.U.Cardinal, H.C.Evans, N.A.Jelley, J.Cerny 53Co-m: A Proton-Unstable Isomer NUCLEAR REACTIONS Ca(16O, 2np), E < 81 MeV; measured σ(E), delayed-p spectrum, (16O)(γ)-delay. 53mCo deduced T1/2.
doi: 10.1016/0370-2693(70)90269-8
1970MC04 Phys.Rev. C1, 184 (1970) R.L.McGrath, J.Cerny, J.C.Hardy, G.Goth, A.Arima Isospin-Forbidden Decay Properties of the Lowest T = 2 States of 20Ne, 24Mg, 28Si, 32S, and 40Ca NUCLEAR REACTIONS 22Ne, 26Mg, 30Si, 34S, 42Ca(p, t), E=42-46 MeV; measured σ(Et). 20Ne, 24Mg, 28Si, 32S, 40Ca T=2 states deduced p-widths, α-widths, branching ratios.
doi: 10.1103/PhysRevC.1.184
1970ME01 Phys.Lett. 31B, 126 (1970) R.Mendelson, J.C.Hardy, J.Cerny The Structure of 16O and 17O(p, d)16O Reaction NUCLEAR REACTIONS 17O(p, d), E = 31 MeV; measured σ(Ed, θ). 16O deduced levels, J, π, T, S.
doi: 10.1016/0370-2693(70)90129-2
1970ME11 Phys.Rev.Lett. 25, 533 (1970) R.Mendelson, G.J.Wozniak, A.D.Bacher, J.M.Loiseaux, J.Cerny Mass of 13O and the Isobaric Multiplet Mass Equation NUCLEAR REACTIONS 16O, 20Ne, 24Mg, 28Si(3He, 6He), E=65-75 MeV; measured σ(E(6He)), Q. 13O, 17Ne, 21Mg, 25Si deduced masses.
doi: 10.1103/PhysRevLett.25.533
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