NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = J.Jury Found 42 matches. 2001BO38 Phys.Rev. C64, 031601 (2001) M.J.Boland, M.A.Garbutt, R.P.Rassool, M.N.Thompson, A.J.Bennett, J.W.Jury, J.-O.Adler, B.Schroder, D.Nilsson, K.Hansen, M.Karlsson, M.Lundin, I.J.D.MacGregor Excitations in the Halo Nucleus 6He following the 7Li(γ, p)6He Reaction NUCLEAR REACTIONS 7Li(γ, p), E=50-70 MeV; measured proton spectra, σ(θ). 6He deduced resonance energy, width. Tagged photons. Comparison with cluster model predictions.
doi: 10.1103/PhysRevC.64.031601
2001GA65 Phys.Rev. C64, 064602 (2001) K.R.Garrow, F.Adimi, N.R.Kolb, J.Lu, R.E.Pywell, D.M.Skopik, J.M.Vogt, J.W.Jury, A.Kuzin, M.N.Thompson, J.Ryckebusch High Resolution Measurement of the 18O(γ, pn)14N0, 1, 2, ... Reaction NUCLEAR REACTIONS 16O(γ, np), E=98.5-141.0 MeV; measured Ep, En, np-coin, angular correlations, σ(E, θ); deduced reaction mechanism features. Comparison with model predictions.
doi: 10.1103/PhysRevC.64.064602
1994ZU01 Phys.Rev. C49, 1545 (1994) D.Zubanov, M.N.Thompson, J.W.Jury, K.Shoda 13C(e, p0, 1)12B Differential Cross Section NUCLEAR REACTIONS 13C(e, p), E=21-23 MeV; measured proton yields vs E, θ=90°; deduced σ(θ) for (γ, p) reaction. 13C deduced GDR, decay features, isospin splitting effects.
doi: 10.1103/PhysRevC.49.1545
1993MC02 Phys.Rev. C47, 1108 (1993) K.G.McNeill, M.N.Thompson, A.D.Bates, J.W.Jury, B.L.Berman Isospin Effects in the Photodisintegration of Light Nuclei NUCLEAR REACTIONS 13,14C, 15N, 17,18O, 25,26Mg, 29,30Si(γ, p), (γ, n), (γ, 2n), E < 36 MeV; analyzed σ(E); deduced isospin component splitting.
doi: 10.1103/PhysRevC.47.1108
1992ZU01 Phys.Rev. C45, 174 (1992); Erratum Phys.Rev. C46, 1147 (1992) D.Zubanov, M.N.Thompson, B.L.Berman, J.W.Jury, R.E.Pywell, K.G.McNeill Giant Dipole Resonance in 17O Observed with the (γ, p) Reaction NUCLEAR REACTIONS, ICPND 17O(γ, p), (γ, X), E=13.5-43.15 MeV; measured reaction yields; deduced σ(γ, p), σ. 17O deduced resonances, J, π, Γ, GDR. Activation technique.
doi: 10.1103/PhysRevC.45.174
1991MC01 Phys.Rev. C43, 489 (1991) K.G.McNeill, J.W.Jury, M.N.Thompson, B.L.Berman, R.E.Pywell 18O(γ, pn+np) Cross Section NUCLEAR REACTIONS 18O(γ, xnyp), E=19-43 MeV; measured two-nucleon production σ(E); deduced channel effect on total photoabsorption σ. Enriched target.
doi: 10.1103/PhysRevC.43.489
1991MC05 Phys.Rev. C44, 1137 (1991) D.J.McLean, M.N.Thompson, D.Zubanov, K.G.McNeill, J.W.Jury, B.L.Berman 14C Photoproton Cross Section NUCLEAR REACTIONS, ICPND 14C(γ, p), E=threshold-29.1 MeV; measured σ(E); deduced photoabsorption σ isospin fragmentation. 14C deduced GDR isospin splitting.
doi: 10.1103/PhysRevC.44.1137
1990MC06 Phys.Rev. C42, 2234 (1990) Isospin in 17O(γ, n0) Reactions NUCLEAR REACTIONS 17O(γ, n), E not given; analyzed data. 17O deduced levels, T.
doi: 10.1103/PhysRevC.42.2234
1989KU10 Nucl.Phys. A499, 328 (1989) P.C.-K.Kuo, J.W.Jury, K.G.McNeill, N.K.Sherman, W.F.Davidson Photoneutron Angular Distribution of 19F NUCLEAR REACTIONS 19F(γ, n), E=15-25 MeV; measured σ(θ); deduced σ(Eγ). 19F deduced E1 absorption strength, T=1/2 purity. Natural target, tof.
doi: 10.1016/0375-9474(89)90049-3
1988CA11 Phys.Lett. 203B, 33 (1988) P.J.Carlos, Ph.Bourgeois, J.Fagot, J.L.Fallou, P.Garganne, J.M.Laget, A.Lepretre, A.de Miniac, A.Veyssiere, J.Jury, D.Ryckbosch The 6Li(γ, p) Reaction in the 30-100 MeV Photon Energy Range NUCLEAR REACTIONS 6Li(γ, p), E=34.5-98.8 MeV; measured σ(θp, Ep), σ(θ) vs E; deduced reaction mechanism.
doi: 10.1016/0370-2693(88)91565-1
1988KU06 Nucl.Phys. A481, 217 (1988) P.C.-K.Kuo, J.W.Jury, W.F.Davidson, N.K.Sherman Photoneutron Angular Distributions for 32S NUCLEAR REACTIONS 32S(γ, n), E=18-29 MeV; measured σ(θ); deduced σ(Eγ). 32S deduced E1 absorption strength, T=1 purity. Natural target, tof.
doi: 10.1016/0375-9474(88)90493-9
1987BE37 Phys.Rev. C36, 1286 (1987) B.L.Berman, R.E.Pywell, S.S.Dietrich, M.N.Thompson, K.G.McNeill, J.W.Jury Absolute Photoneutron Cross Sections for Zr, I, Pr, Au, and Pb NUCLEAR REACTIONS Zr, 127I, 141Pr, 197Au, Pb(γ, n), E ≈ 12-17 MeV; Zr, 127I, 141Pr, 197Au, Pb(γ, 2n), E=threshold-17 MeV; measured absolute photonucleon σ(E).
doi: 10.1103/PhysRevC.36.1286
1987JU07 Phys.Rev. C36, 1243 (1987) J.W.Jury, P.C.-K.Kuo, K.G.McNeill, C.K.Ross, H.R.Weller, S.Raman Ground-State Photoneutron Reactions in 18O NUCLEAR REACTIONS 18O(γ, n), E=14-26 MeV; measured σ(θ). 18O deduced resonances, E1 transition strength. Direct-semidirect model.
doi: 10.1103/PhysRevC.36.1243
1987LE19 Nucl.Phys. A472, 533 (1987) A.Lepretre, R.Bergere, P.Bourgeois, P.Carlos, J.Fagot, J.L.Fallou, P.Garganne, A.Veyssiere, H.Ries, R.Goble, U.Kneissl, G.Mank, H.Stroher, W.Wilke, D.Ryckbosch, J.Jury Absolute Photofission Cross Sections for 232Th and 235,238U Measured with Monochromatic Tagged Photons (20 MeV < E(γ) < 110 MeV) NUCLEAR REACTIONS 232Th, 235,238U(γ, F), E=20-110 MeV; measured fission σ(E). 232Th, 235,238U deduced fission evaporation competition, fission probabilities. Hybrid model. Parallel plate avalanche detector, monochromatic tagged photons.
doi: 10.1016/0375-9474(87)90044-3
1987MC04 Phys.Rev. C36, 1621 (1987) K.G.McNeill, R.E.Pywell, B.L.Berman, J.G.Woodworth, M.N.Thompson, J.W.Jury Photoneutron Cross Section for 29Si NUCLEAR REACTIONS 29Si(γ, n), E=9.4-18.3 MeV; measured σ(E).
doi: 10.1103/PhysRevC.36.1621
1985JU02 Phys.Rev. C32, 1817 (1985) J.W.Jury, J.D.Watson, D.Rowley, T.W.Phillips, J.G.Woodworth Ground State Photoneutron Reactions in 17O NUCLEAR REACTIONS 17O(γ, n), E=10-24 MeV; measured σ(θ). 17O deduced resonances, J, π.
doi: 10.1103/PhysRevC.32.1817
1985KU01 Phys.Rev. C31, 318 (1985) P.C-K.Kuo, K.G.McNeill, N.K.Sherman, S.Landsberger, W.F.Davidson, J.W.Jury, J.R.C.Lafontaine Ground-State Photoneutron Reactions in 14C NUCLEAR REACTIONS 14C(γ, n), E=13.5-28.5 MeV bremsstrahlung; measured photoneutron σ(En), σ(θ), σ(E); deduced dominant E1 absorption. 14C deduced GDR strength in neutron decay channel, isospin character.
doi: 10.1103/PhysRevC.31.318
1985PY01 Phys.Rev. C32, 384 (1985) R.E.Pywell, B.L.Berman, J.G.Woodworth, J.W.Jury, K.G.McNeill, M.N.Thompson Photoneutron Cross Sections for 14C NUCLEAR REACTIONS 14C(γ, n), (γ, 2n), E=8.2-36 MeV; measured neutron yields, integrated σ. 14C deduced GDR, decay characteristics.
doi: 10.1103/PhysRevC.32.384
1984KU21 Phys.Rev. C30, 1789 (1984) P.C.-K.Kuo, J.W.Jury, N.K.Sherman, W.F.Davidson Electric Quadrupole Photoneutron Reactions in 16O NUCLEAR REACTIONS 16O(γ, n), E=30-35 MeV; measured σ(θ). 16O deduced E2 transition σ, EWSR.
doi: 10.1103/PhysRevC.30.1789
1984WO05 Phys.Rev. C29, 1186 (1984) J.G.Woodworth, R.A.August, N.R.Roberson, D.R.Tilley, H.R.Weller, J.W.Jury Polarized Neutron Capture into 13C: Evidence for a secondary doorway state effect NUCLEAR REACTIONS 12C(n, γ), (polarized n, γ), E=12-18.8 MeV; measured σ(θ), analyzing power. 13C deduced secondary doorway state. Other data input, Legendre polynomial analysis.
doi: 10.1103/PhysRevC.29.1186
1983BE01 Phys.Rev. C27, 1 (1983) B.L.Berman, J.W.Jury, J.G.Woodworth, R.E.Pywell, K.G.McNeill, M.N.Thompson Photoneutron Cross Section for 16O NUCLEAR REACTIONS 16O(γ, n), E=17-33 MeV bremsstrahlung; measured σ(photoproduction) vs E; deduced (γ, n0) dominance. Monoenergetic beam.
doi: 10.1103/PhysRevC.27.1
1983PY01 Phys.Rev. C27, 960 (1983) R.E.Pywell, B.L.Berman, J.W.Jury, J.G.Woodworth, K.G.McNeill, M.N.Thompson Photoneutron Cross Sections for the Silicon Isotopes NUCLEAR REACTIONS 28,29Si(γ, n), 30Si(γ, n), (γ, 2n), E=13.4-33.1 MeV; measured σ(E). 28,29,30Si deduced GDR fragmentation characteristics.
doi: 10.1103/PhysRevC.27.960
1983WA03 Phys.Rev. C27, 506 (1983) J.D.Watson, J.W.Jury, P.C.-K.Kuo, W.F.Davidson, N.K.Sherman, K.G.McNeill Ground-State Photoneutron Reactions in 15N NUCLEAR REACTIONS 15N(γ, n), E=15-25 MeV bremsstrahlung; measured σ(θ). 15N deduced levels, possible J, π, T, GDR fragmentation. Legendre polynomial analysis.
doi: 10.1103/PhysRevC.27.506
1983ZU02 Phys.Rev. C27, 1957 (1983) D.Zubanov, R.A.Sutton, M.N.Thompson, J.W.Jury 13C(γ, p) Cross Section RADIOACTIVITY 12B [from 13C(γ, p), E=17.5-28 MeV]; measured β-yield vs bremsstrahlung energy. NUCLEAR REACTIONS 13C(γ, p), E=17.5-28 MeV bremsstrahlung; measured σ(E). 13C deduced GDR isospin splitting. Activation technique.
doi: 10.1103/PhysRevC.27.1957
1982JU03 Phys.Rev. C26, 777 (1982) J.W.Jury, B.L.Berman, J.G.Woodworth, M.N.Thompson, R.E.Pywell, K.G.McNeill Photoneutron Cross Sections for 15N NUCLEAR REACTIONS 15N(γ, n), (γ, 2n), E=10.8-38 MeV; measured σ(E), total σ(photoproduction). 15N deduced resonances, decay characteristics.
doi: 10.1103/PhysRevC.26.777
1980JU01 Phys.Rev. C21, 503 (1980) J.W.Jury, B.L.Berman, D.D.Paul, P.Meyer, J.G.Woodworth Photoneutron Cross Sections for 17O NUCLEAR REACTIONS 17O(γ, n), 17O(γ, 2n), E=8.5-39.7 MeV; 16O(γ, n), E=15.9-39.7 MeV; measured σ(total). 17O deduced GDR isospin splitting. 4π neutron detector.
doi: 10.1103/PhysRevC.21.503
1980JU02 Nucl.Phys. A337, 503 (1980) J.W.Jury, C.K.Ross, N.K.Sherman Ground-State Photoneutron Angular Distribution for 14N NUCLEAR REACTIONS 14N(γ, n), E=17-26 MeV; measured σ(θn); deduced σ(Eγ), T=1 purity. Tof.
doi: 10.1016/0375-9474(80)90156-6
1979JO05 Phys.Rev. C20, 27 (1979) R.G.Johnson, B.L.Berman, K.G.McNeill, J.G.Woodworth, J.W.Jury Photoneutron Reaction in 17O: Ground-State Differential Cross Section At 98° NUCLEAR REACTIONS 17O(γ, n0), E=13.7, 16, 22, 28, 34 MeV bremsstrahlung; measured σ(E, θ). 17O deduced resonances, J, π, Γγ, GDR (T=1/2) strength.
doi: 10.1103/PhysRevC.20.27
1979JU01 Phys.Rev. C19, 1684 (1979) J.W.Jury, B.L.Berman, D.D.Faul, P.Meyer, K.G.McNeill, J.G.Woodworth Photoneutron Cross Sections for 13C NUCLEAR REACTIONS 13C(γ, n), E=7.6-41.8 MeV; measured 4π-neutron yield, integrated σ(γ, n), σ(γ, 2n); deduced isospin splitting of giant resonance.
doi: 10.1103/PhysRevC.19.1684
1979WO04 Phys.Rev. C19, 1667 (1979) J.G.Woodworth, K.G.McNeill, J.W.Jury, R.A.Alvarez, B.L.Berman, D.D.Paul, P.Meyer Photonuclear Cross Sections for 18O NUCLEAR REACTIONS 18O(γ, n), E=8.0-41.8 MeV; measured 4π-prompt, delayed n yield, integral σ(Eγ, n), integral σ(Eγ, 2n), integral σ(Eγ, p); deduced distribution of isospin strength.
doi: 10.1103/PhysRevC.19.1667
1979WO06 Nucl.Phys. A327, 53 (1979) J.G.Woodworth, K.G.McNeill, J.W. Jury, P.D.Georgopulos, R.G.Johnson Photoneutron Angular Distributions from the Reaction 13C(γ, n0)12C NUCLEAR REACTIONS 13C(γ, n0), E=7.6-24 MeV; measured photoneutron angular distributions, tof; deduced σ(Eγ, n).
doi: 10.1016/0375-9474(79)90317-8
1977WO04 Can.J.Phys. 55, 1704 (1977) J.G.Woodworth, K.G.McNeill, J.W.Jury, P.D.Georgopulos, R.G.Johnson The 98° Differential Cross Sections for the Reactions 13C(γ, n0)12C And 13C(γ, n1)12C NUCLEAR REACTIONS 13C(γ, n), E=6-35.5 MeV; measured σ(E). 13C deduced resonances, Γ.
doi: 10.1139/p77-215
1975AL03 Can.J.Phys. 53, 786 (1975) J.D.Allan, J.W.Jury, R.G.Johnson, K.G.McNeill, J.G.Woodworth, Y.S.Horowitz Photoneutron Reactions in 18O NUCLEAR REACTIONS 18O(γ, n), E=11-18 MeV bremsstrahlung; measured σ(E, En). 18O deduced resonances.
doi: 10.1139/p75-096
1975IR01 Can.J.Phys. 53, 802 (1975) J.D.Irish, R.G.Johnson, B.L.Berman, B.J.Thomas, K.G.McNeill, J.W.Jury Photoneutron Angular Distributions for 4He NUCLEAR REACTIONS 4He(γ, n), E=22-32 MeV; measured σ(E, En, θ). 4He deduced resonance character.
doi: 10.1139/p75-098
1975WO06 Can.J.Phys. 53, 795 (1975) J.G.Woodworth, J.W.Jury, K.H.Lokan, N.K.Sherman Photoneutrons from 20Ne NUCLEAR REACTIONS 20Ne(γ, n), E=19-32 MeV bremsstrahlung; measured σ(E, En). 20Ne deduced resonances.
doi: 10.1139/p75-097
1974IR02 Phys.Rev. C9, 2060 (1974) J.D.Irish, R.G.Johnson, K.G.McNeill, J.W.Jury Rationalization of Measurements of the 4He(γ, n)3He Cross Section NUCLEAR REACTIONS 4He(γ, n), E=35 MeV; measured σ(beam current).
doi: 10.1103/PhysRevC.9.2060
1973IR02 Phys.Rev. C8, 1211 (1973) J.D.Irish, R.G.Johnson, B.L.Berman, B.J.Thomas, K.G.McNeill, J.W.Jury 98° Differential Cross Section for the Reaction 4He(γ, n)3He NUCLEAR REACTIONS 4He(γ, n), E=22-33 MeV; measured σ(E).
doi: 10.1103/PhysRevC.8.1211
1973JU01 Can.J.Phys. 51, 1176 (1973) J.W.Jury, J.I.Lodge, K.H.Lokan, H.K.Sherman, R.W.Gellie Photoneutron Disintegration of 40Ar NUCLEAR REACTIONS 40Ar(γ, n), E=13-23 MeV; measured σ(En). 40Ar deduced levels.
doi: 10.1139/p73-156
1972LO09 Phys.Rev.Lett. 28, 1526 (1972) K.H.Lokan, N.K.Sherman, R.W.Gellie, J.W.Jury, J.I.Lodge, R.G.Johnson Excited States of 40Ar Observed in the Reaction 40Ar(γ, n0)39Ar NUCLEAR REACTIONS 40Ar(γ, n0), E < 12.5 MeV; measured σ(En). 40Ar deduced resonances, level-width.
doi: 10.1103/PhysRevLett.28.1526
1970HE19 Nucl.Instrum.Methods 80, 77 (1970) J.S.Hewitt, K.G.McNeill, J.W.Jury A Facility for Photoneutron Angular Distribution Measurements with High Neutron Energy Resolution NUCLEAR REACTIONS 16O(γ, n0), E < 31 MeV; measured σ(En, θ).
doi: 10.1016/0029-554X(70)90300-9
1970JU02 Can.J.Phys. 48, 1635 (1970) J.W.Jury, J.S.Hewitt, K.G.McNeill Ground State Photoneutron Angular Distributions in the Giant Resonance of O16 NUCLEAR REACTIONS 16O(γ, n), E < 30.5 MeV; measured σ(E;En, θ). 16O deduced giant resonance structure.
doi: 10.1139/p70-207
1970MC05 Can.J.Phys. 48, 950 (1970) K.G.McNeill, J.W.Jury, J.S.Hewitt Fine Structure in the Photoneutron Spectra from Praseodymium-141 and Lead NUCLEAR REACTIONS 141Pr, Pb(γ, n), E < 31 MeV; measured σ(En); deduced fine structure. 141Pr, 208Pb deduced giant resonance structure.
doi: 10.1139/p70-123
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