NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = A.Wolf Found 114 matches. Showing 1 to 100. [Next]2016BA23 Phys.Rev. A 93, 052703 (2016) N.R.Badnell, K.Spruck, C.Krantz, O.Novotny, A.Becker, D.Bernhardt, M.Grieser, M.Hahn, R.Repnow, D.W.Savin, A.Wolf, A.Muller, S.Schippers Recombination of W19+ ions with electrons: Absolute rate coefficients from a storage-ring experiment and from theoretical calculations NUCLEAR REACTIONS W(W, E), E ∼ 186 MeV; measured product ions; deduced recombination rate coefficient. Comparison with theoretical calculations.
doi: 10.1103/PhysRevA.93.052703
2013HA08 Astrophys.J. 767, 47 (2013) M.Hahn, A.Becker, D.Bernhardt, M.Grieser, C.Krantz, M.Lestinsky, A.Muller, O.Novotny, R.Repnow, S.Schippers, K.Spruck, A.Wolf, D.W.Savin Storage Ring Cross Section Measurements for Electron Impact Single and Double Ionization of Fe13 + and Single Ionization of Fe16 + and Fe17 + NUCLEAR REACTIONS Fe(E, E), E<3 keV; measured reaction products, decays of ion metastable states; deduced single and double ionization σ and uncertainties. Comparison with available data.
doi: 10.1088/0004-637X/767/1/47
2012TR04 New Journal of Physics 14, 023061 (2012) E.Trabert, M.Grieser, R.von Hahn, C.Krantz, R.Repnow, A.Wolf M1 and E2 decay-dependent lifetime of the lowest 1S0 level in C-like ions up to Ne4+ measured at a heavy-ion storage ring ATOMIC PHYSICS N, O, F, Ne; measured optical emission; deduced M1, E2 decay-dependent T1/2. Comparison with theoretical calculations, TSR heavy-ion storage ring.
doi: 10.1088/1367-2630/14/2/023061
2012WO03 Phys.Rev. C 85, 037304 (2012);Erratum Phys.Rev. C 86, 019902 (2012) A.Wolf, Z.Berant, V.Werner, A.Heinz, R.F.Casten, R.J.Casperson, D.S.Brenner, R.Chevrier, D.McCarthy, G.Ilie, E.Williams, J.Qian, J.R.Terry, T.Ahn, R.Winkler g factor of the 21+ state of 168Hf NUCLEAR MOMENTS 168Hf; measured g factor by perturbed angular correlation in a static external magnetic field. Comparisons with hydrodynamic model, semiempirical model, IBA-2 model, large-scale shell-model, pairing plus quadrupole model. Systematics of g factors of first 2+ states for 96,98,100,104,106,108Hf. RADIOACTIVITY 168Ta(EC), (β+)[from 159Tb(16O, 7n), E=130 MeV]; measured Eγ, γγ-coin, perturbed γγ(θ) in a magnetic field; deduced g factor.
doi: 10.1103/PhysRevC.85.037304
2009BE42 Phys.Rev. C 80, 057303 (2009) Z.Berant, E.Oster, R.J.Casperson, A.Wolf, V.Werner, A.Heinz, R.F.Casten, G.Gurdal, E.A.McCutchan, D.S.Brenner, J.R.Terry, R.Winkler, E.Williams, J.Qian, A.Schmidt, M.K.Smith, T.Ahn, C.W.Beausang, P.H.Regan, T.Ross, M.Bunce, B.Darakchieva, D.A.Meyer, J.LeBlanc, K.Dudziak, C.Bauer, G.Henning g factor of the 2+1 state of 172Hf NUCLEAR MOMENTS 172Hf; measured g factor of first 2+ state using integral perturbed angular correlation method. Comparisons with g factors of neighboring even-even Hf nuclei and with predictions of several nuclear models including interacting boson approximation (IBA-2). RADIOACTIVITY 172Ta(EC), (β+) [from 165Ho(12C, 5n), E=85 MeV]; measured Eγ, Iγ, γγ-coin, and cascade Iγ as a function of angle and magnetic field.
doi: 10.1103/PhysRevC.80.057303
2008MC01 Phys.Rev. C 77, 054304 (2008) E.A.McCutchan, R.F.Casten, V.Werner, E.Williams, R.Winkler, A.Wolf, Z.Berant, G.Gurdal, J.Qian, H.Ai, L.Amon, C.W.Beausang, D.S.Brenner, R.B.Cakirli, R.J.Casperson, C.R.Fitzpatrick, D.Frank, A.B.Garnsworthy, A.Heinz, R.Luttke, A.F.Mertz, Y.Oktem, N.Pietralla, P.H.Regan, B.Shoraka, J.R.Terry, N.J.Thompson Enhanced mixing of intrinsic states in deformed Hf nuclei RADIOACTIVITY 170,172,174Ta(β+), (EC) [from 159Tb(16O, 5n), E=100 MeV; 165Ho(12C, 5n), E=80 MeV; 168Er(11B, 5n), E=65 MeV]; measured Eγ, Iγ, γγ-coin, branching ratios. 170,172,174Hf; deduced levels, J, π. 166,168,170,172,174Hf; systematics.
doi: 10.1103/PhysRevC.77.054304
2007MC08 Phys.Rev. C 76, 064307 (2007) E.A.McCutchan, R.F.Casten, V.Werner, A.Wolf, Z.Berant, R.J.Casperson, A.Heinz, R.Luttke, B.Shoraka, J.R.Terry, E.Williams, R.Winkler β decay study of 168Hf and a test of new geometrical models RADIOACTIVITY 168Ta (β+), (EC) [from 159Tb(16O, 7n), E=130 MeV]; measured Eγ, Iγ, γγ-coin, γγ(θ). 168Hf; deduced levels, J, π, multipolarities, mixing ratios, B(E2). Compared with calculations using CBS and Davidson models and IBA model. 166,168Yb; measured Eγ.
doi: 10.1103/PhysRevC.76.064307
2007SC03 Phys.Rev.Lett. 98, 033001 (2007) S.Schippers, E.W.Schmidt, D.Bernhardt, D.Yu, A.Muller, M.Lestinsky, D.A.Orlov, M.Grieser, R.Repnow, A.Wolf Storage-Ring Measurement of the Hyperfine Induced 47Ti18+(2s2p3P0 → 2s21S0) Transition Rate NUCLEAR MOMENTS 47Ti; measured hyperfine-induced transition rate in beryllium-like ions. ATOMIC PHYSICS 47Ti; measured hyperfine-induced transition rate in beryllium-like ions.
doi: 10.1103/PhysRevLett.98.033001
2007WO08 Phys.Rev. C 76, 047308 (2007) A.Wolf, Z.Berant, A.Heinz, V.Werner, E.A.McCutchan, G.Gurdal, R.B.Cakirli, Y.Oktem, J.Ai, L.Amon, C.W.Beausang, D.S.Brenner, R.F.Casten, R.J.Casperson, K.Dusling, C.R.Fitzpatrick, A.B.Gransworthy, N.Pietralla, J.Qian, P.H.Regan, N.J.Thompson, E.Williams, R.Winkler g factor of the 2+1 state of 170Hf RADIOACTIVITY 170Ta(β+), (EC) [from 159Tb(16O, 5n), E=100 MeV]; measured Eγ, Iγ, γγ(θ) in static magnetic field. 170Hf; deduced levels, J, π, g-factor of first 2+ state.
doi: 10.1103/PhysRevC.76.047308
2006ZH08 Phys.Rev. C 73, 037301 (2006) J.Zhang, R.F.Casten, A.Wolf, Z.Berant, R.B.Cakirli, N.V.Zamfir, E.A.McCutchan Consistent interpretation of B(E2) values and g factors in deformed nuclei NUCLEAR STRUCTURE Z=64-74; analyzed g factors, B(E2) for even-even nuclides, effective size of valence space. Phenomenological model.
doi: 10.1103/PhysRevC.73.037301
2005WO06 Phys.Rev. C 72, 027301 (2005) A.Wolf, Z.Berant, N.V.Zamfir, D.S.Brenner, E.A.McCutchan, H.Ai, R.F.Casten, K.Dusling, A.Heinz, D.A.Meyer, E.A.Millman, N.Pietralla, C.Plettner, J.Qian, P.H.Regan, D.Swanson, J.Vinson, E.Williams, R.Winkler g factor of the 2+1 state of 160Er RADIOACTIVITY 160Yb, 160Tm(EC) [from 147Sm(18O, 5n) and subsequent decay]; measured β-delayed Eγ, Iγ(θ, H, t), γγ-coin. 160Er level deduced g factor. Perturbed angular correlation technique, systematics in neighboring nuclides discussed.
doi: 10.1103/PhysRevC.72.027301
2004BE13 Phys.Rev. C 69, 034320 (2004) Z.Berant, A.Wolf, N.V.Zamfir, M.A.Caprio, D.S.Brenner, N.Pietralla, R.L.Gill, R.F.Casten, C.W.Beausang, R.Krucken, C.J.Barton, J.R.Cooper, A.A.Hecht, D.M.Johnson, J.R.Novak, H.Cheng, B.F.Albanna, G.Gurdal g factor of the 2+1 state of 164Yb RADIOACTIVITY 164Lu(EC) [from 155Gd(14N, 5n)]; measured Eγ, Iγ(θ, H), γγ-coin. 164Yb level deduced g factor. Comparison with model predictions. Systematic trends discussed.
doi: 10.1103/PhysRevC.69.034320
2003BA18 Phys.Rev. C 67, 034310 (2003) C.J.Barton, D.S.Brenner, N.V.Zamfir, M.A.Caprio, A.Aprahamian, M.C.Wiescher, C.W.Beausang, Z.Berant, R.F.Casten, J.R.Cooper, R.L.Gill, R.Krucken, J.R.Novak, N.Pietralla, M.Shawcross, A.Teymurazyan, A.Wolf Mass measurement of 80Y by β-γ coincidence spectroscopy RADIOACTIVITY 80Y(EC), (β+) [from 58Ni(28Si, npα)]; measured Eγ, Eβ, βγ-coin; deduced Q(EC). 80Sr deduced transitions. Implications for astrophysical rp-process simulations discussed.
doi: 10.1103/PhysRevC.67.034310
2003HE25 Phys.Rev. C 68, 054310 (2003) A.A.Hecht, C.W.Beausang, H.Amro, C.J.Barton, Z.Berant, M.A.Caprio, R.F.Casten, J.R.Cooper, D.J.Hartley, R.Krucken, D.A.Meyer, H.Newman, J.R.Novak, N.Pietralla, J.J.Ressler, A.Wolf, N.V.Zamfir, J.-Y.Zhang, K.E.Zyromski Evidence for chiral symmetry breaking in 140Eu? NUCLEAR REACTIONS 92Mo(51V, n2p), E=205 MeV; measured Eγ, Iγ, γγ-, (X-ray)γ-coin. 140Eu deduced high-spin levels, J, π, configurations, B(M1)/B(E2), possible chiral symmetry breaking. Cranked mean field and total Routhian surface calculations. Rotational band systematics in neighboring nuclides discussed.
doi: 10.1103/PhysRevC.68.054310
2002CA49 Phys.Rev. C 66, 054310 (2002) M.A.Caprio, N.V.Zamfir, R.F.Casten, C.J.Barton, C.W.Beausang, J.R.Cooper, A.A.Hecht, R.Krucken, H.Newman, J.R.Novak, N.Pietralla, A.Wolf, K.E.Zyromski Low-spin structure of 156Dy through γ-ray spectroscopy RADIOACTIVITY 156Er, 156Ho(β+), (EC) [from 148Sm(12C, 4n) and subsequent decay]; measured Eγ, Iγ, γγ-coin. 156Dy deduced levels, J, π, B(E2), feeding intensities. Comparisons with neighboring isotones and with model predictions.
doi: 10.1103/PhysRevC.66.054310
2002WO10 Phys.Rev. C66, 024323 (2002) A.Wolf, N.V.Zamfir, M.A.Caprio, Z.Berant, D.S.Brenner, N.Pietralla, R.L.Gill, R.F.Casten, C.W.Beausang, R.Kruecken, K.E.Zyromski, C.J.Barton, J.R.Cooper, A.A.Hecht, H.Newman, J.R.Novak, J.Cederkall Structure of low-lying states in 128Ba from γ-γ angular correlations and polarization measurements RADIOACTIVITY 128La(EC) [from 116Sn(16O, 3np)]; measured Eγ, Iγ, γγ-coin, γ-ray polarization. 128Ba deduced levels, J, π, B(E2). Comparison with model predictions.
doi: 10.1103/PhysRevC.66.024323
2002ZA04 Phys.Rev. C65, 044325 (2002) N.V.Zamfir, M.A.Caprio, R.F.Casten, C.J.Barton, C.W.Beausang, Z.Berant, D.S.Brenner, W.T.Chou, J.R.Cooper, A.A.Hecht, R.Krucken, H.Newman, J.R.Novak, N.Pietralla, A.Wolf, K.E.Zyromski 102Pd: An E(5) nucleus ? RADIOACTIVITY 102Ag(β+), (EC) [from 89Y(16O, 3n)]; measured Eγ, Iγ. 102Pd deduced levels, J, π, symmetry features.
doi: 10.1103/PhysRevC.65.044325
2002ZA07 Phys.Rev. C65, 067305 (2002) N.V.Zamfir, H.G.Borner, N.Pietralla, R.F.Casten, Z.Berant, C.J.Barton, C.W.Beausang, D.S.Brenner, M.A.Caprio, J.R.Cooper, A.A.Hecht, M.Krticka, R.Krucken, P.Mutti, J.R.Novak, A.Wolf Lifetime and B(E2) Values for the 31+ Level in 152Sm NUCLEAR REACTIONS 151Sm(n, γ), E=reactor; measured Doppler-broadened Eγ, Iγ. 152Sm level deduced T1/2, B(E2), phase coexistence. Gamma-ray induced Doppler broadening technique. RADIOACTIVITY 152Eu(EC); measured γγ-coin, γ-ray polarization. 152Sm transition deduced δ.
doi: 10.1103/PhysRevC.65.067305
2001HE15 Phys.Rev. C63, 051302 (2001) A.A.Hecht, C.W.Beausang, K.E.Zyromski, D.L.Balabanski, C.J.Barton, M.A.Caprio, R.F.Casten, J.R.Cooper, D.J.Hartley, R.Krucken, D.Meyer, H.Newman, J.R.Novak, E.S.Paul, N.Pietralla, A.Wolf, N.V.Zamfir, J.-Y.Zhang, F.Donau Evidence for Chiral Symmetry Breaking in 136Pm and 138Eu NUCLEAR REACTIONS 116Sn(24Mg, 3np), E=130, 135 MeV; 106Cd(35Cl, n2p), E=150 MeV; measured Eγ, Iγ, γγ-coin, γ-ray polarization. 136Pm, 138Eu deduced high-spin levels, J, π, configurations, B(M1)/B(E2), chiral twin bands. Comparison with tilted axis cranking model calculations. Yrast ball, Eurogam I arrays.
doi: 10.1103/PhysRevC.63.051302
2001KR13 Phys.Rev. C64, 017305 (2001) R.Krucken, W.-T.Chou, J.R.Cooper, C.W.Beausang, C.J.Barton, M.A.Caprio, R.F.Casten, A.A.Hecht, J.R.Novak, N.Pietralla, A.Wolf, N.V.Zamfir Lifetimes in Neutron-Rich Fission Fragments using the Differential Recoil Distance Method RADIOACTIVITY 252Cf(SF); measured Doppler-shifted Eγ, Iγ, γγ-, (fragment)γ-coin. 104Mo, 110Ru, 144Ba deduced levels T1/2, transition quadrupole moments. Differential recoil distance method.
doi: 10.1103/PhysRevC.64.017305
2001NE11 Phys.Rev. C64, 027304 (2001) H.Newman, J.R.Novak, C.W.Beausang, C.J.Barton, M.A.Caprio, R.F.Casten, J.R.Cooper, A.A.Hecht, R.Krucken, N.Pietralla, A.Wolf, N.V.Zamfir, J.-Y.Zhang, K.E.Zyromski, I.Birriel, J.Saladin High-Spin States in 203Rn NUCLEAR REACTIONS 174Yb(34S, 5n), E=167 MeV; 168Er(40Ar, 5n), E=188 MeV; measured Eγ, Iγ, γγ-, (recoil)γ-coin. 203Rn deduced high-spin levels, J, π, configurations. Gammasphere, Yrast ball arrays, fragment mass analyzer.
doi: 10.1103/PhysRevC.64.027304
2001TO06 Phys.Rev. C63, 034314 (2001) B.E.Tomlin, C.J.Barton, N.V.Zamfir, M.A.Caprio, R.L.Gill, R.Krucken, J.R.Novak, J.R.Cooper, K.E.Zyromski, G.Cata-Danil, C.W.Beausang, A.Wolf, N.A.Pietralla, H.Newman, J.Cederkall, B.Liu, Z.Wang, R.F.Casten, D.S.Brenner Mass Measurements of 70Se, 71Se, 72Br, and 73Br RADIOACTIVITY 70,71Se, 72,73Br(β+) [from 58Ni(HI, xnyp)]; measured β-spectrum, βγ-coin; deduced Q(EC), mass excess. Comparison with model predictions.
doi: 10.1103/PhysRevC.63.034314
2001WO11 Nucl.Phys. A692, 153c (2001) Recombination Physics
doi: 10.1016/S0375-9474(01)01173-3
2000MA84 Eur.Phys.J. A 9, 69 (2000) T.Matulewicz, L.Aphecetche, Y.Charbonnier, H.Delagrange, K.K.Gudima, G.Martinez, M.Ploszajczak, Y.Schutz, V.D.Toneev, M.Appenheimer, R.Averbeck, J.Diaz, A.Doppenschmidt, M.J.van Goethem, S.Hlavac, M.Hoefman, R.Holzmann, F.Lefevre, A.Kugler, H.Lohner, A.Marin, V.Metag, R.Novotny, R.W.Ostendorf, R.H.Siemssen, R.S.Simon, R.Stratmann, H.Stroher, P.Tlusty, P.H.Vogt, V.Wagner, J.Weiss, H.W.Wilschut, F.Wissmann, A.R.Wolf, M.Wolf Observation of Δ+ → pπ0 Decay in Heavy-Ion Collisions NUCLEAR REACTIONS Ca(40Ar, X), E=180 MeV/nucleon; measured pion-proton invariant mass distributions; deduced Δ+ resonance decay features.
doi: 10.1007/s100500070057
1999MA57 Phys.Rev.Lett. 83, 1538 (1999) G.Martinez, Y.Charbonnier, L.Aphecetche, H.Delagrange, K.K.Gudima, T.Matulewicz, M.Ploszajczak, Y.Schutz, V.Toneev, R.Turrisi, M.Appenheimer, V.Metag, R.Novotny, H.Stroher, A.R.Wolf, M.Wolf, J.Weiss, R.Averbeck, S.Hlavac, R.Holzmann, F.Lefevre, R.S.Simon, R.Stratmann, F.Wissmann, H.Hoefman, M.J.van Goethem, H.Lohner, R.W.Ostendorf, R.H.Siemssen, P.Vogt, H.W.Wilschut, J.Diaz, A.Marin, A.Kugler, P.Tlusty, V.Wagner, A.Doppenschmidt Deep-Subthreshold η and π0 Production Probing Pion Dynamics in the Reaction Ar + Ca at 180A MeV NUCLEAR REACTIONS Ca(40Ar, X), E=180 MeV/nucleon; measured η mesons, neutral pions transverse mass distributions, production σ. Comparison with model predictions.
doi: 10.1103/PhysRevLett.83.1538
1999MA59 Phys.Lett. 461B, 28 (1999) G.Martinez, L.Aphecetche, Y.Charbonnier, H.Delagrange, D.d'Enterria, T.Matulewicz, Y.Schutz, R.Turrisi, M.Appenheimer, V.Metag, R.Novotny, H.Stroher, A.R.Wolf, M.Wolf, J.Weiss, R.Averbeck, S.Hlavac, R.Holzmann, F.Lefevre, R.S.Simon, R.Stratmann, F.Wissmann, M.Hoefman, M.J.van Goethem, H.Lohner, R.W.Ostendorf, R.H.Siemssen, P.Vogt, H.W.Wilschut, J.Diaz, A.Marin, A.Kugler, P.Tlusty, V.Wagner, A.Doppenschmidt Photon Production in Heavy-Ion Collisions Close to the Pion Threshold NUCLEAR REACTIONS Ca(40Ar, X), E=180 MeV/nucleon; measured Eγ, Iγ, neutral pions transverse mass distribution, hard photon multiplicity.
doi: 10.1016/S0370-2693(99)00851-5
1998BR16 Phys.Rev. C58, 1349 (1998) Interacting Boson-Fermion Model Calculation of the Level Scheme and Electromagnetic Properties of 99Zr NUCLEAR STRUCTURE 99Zr; calculated levels, J, π, B(λ). Interacting boson-fermion model.
doi: 10.1103/PhysRevC.58.1349
1998MA84 Nucl.Instrum.Methods Phys.Res. A417, 137 (1998) A.Marin, J.Diaz, R.Averbeck, A.Doppenschmidt, S.Hlavac, R.Holzmann, F.Lefevre, A.Schubert, R.S.Simon, Y.Charbonnier, G.Martinez, Y.Schutz, F.M.Marques, M.Appenheimer, F.D.Berg, V.Metag, R.Novotny, H.Stroher, J.Weiss, A.R.Wolf, M.Wolf, H.Lohner, R.W.Ostendorf, P.Vogt, H.W.Wilschut, A.Kugler, R.Pleskac, P.Tlusty, V.Wagner Detection of Charged Pions and Protons in the Segmented Electromagnetic Calorimeter TAPS NUCLEAR REACTIONS Ca(40Ar, X), E=0.8 GeV/nucleon; measured charged pions, proton spectra, (pion)(proton)-coin, inclusive σ. Segmented BaF2 calorimeter, new particle identification technique.
doi: 10.1016/S0168-9002(98)00683-4
1998TR06 Phys.Lett. 445B, 20 (1998) M.Q.Tran, J.Barth, C.Bennhold, M.Bockhorst, W.Braun, A.Budzanowski, G.Burbach, R.Burgwinkel, J.Ernst, K.H.Glander, S.Goers, B.Guse, K.-M.Haas, J.Hannappel, K.Heinloth, K.Honscheid, T.Jahnen, N.Jopen, H.Jungst, H.Kalinowsky, U.Kirch, F.J.Klein, F.Klein, E.Klempt, D.Kostrewa, A.Kozela, R.Lawall, L.Lindemann, J.Link, J.Manns, T.Mart, D.Menze, H.Merkel, R.Merkel, W.Neuerburg, M.Paganetti, E.Paul, R.Plotzke, U.Schenk, J.Scholmann, I.Schulday, M.Schumacher, P.Schutz, W.J.Schwille, F.Smend, J.Smyrski, W.Speth, H.N.Tran, H.van Pee, W.Vogel, R.Wedemeyer, F.Wehnes, B.Wiegers, F.W.Wieland, J.Wisskirchen, A.Wolf, and the SAPHIR Collaboration Measurement of γp → K+ Λ and γp → K+Σ0 at Photon Energies up to 2 GeV NUCLEAR REACTIONS 1H(γ, K+X), E=0.8-2 GeV; measured Λ, Σ0 hyperon production σ(θ), σ, polarizations. Tagged photons.
doi: 10.1016/S0370-2693(98)01393-8
1998WO04 Phys.Rev.Lett. 80, 5281 (1998) A.R.Wolf, M.Appenheimer, R.Averbeck, Y.Charbonnier, J.Diaz, A.Doppenschmidt, V.Hejny, S.Hlavac, R.Holzmann, A.Kugler, H.Lohner, A.Marin, V.Metag, R.Novotny, R.W.Ostendorf, R.Pleskac, A.Schubert, Y.Schutz, R.S.Simon, R.Stratmann, H.Stratmann, H.Stroher, P.Tlusty, P.H.Vogt, V.Wagner, J.Weiss, H.W.Wilschut, F.Wissmann, M.Wolf Multistep Production of η and Hard π0 Mesons in Subthreshold Au-Au Collisions NUCLEAR REACTIONS 197Au(197Au, X), E=800 MeV/nucleon; measured pion, eta meson σ(y), σ, multiplicity; deduced multistep meson production mechanism.
doi: 10.1103/PhysRevLett.80.5281
1997MA56 Phys.Lett. 409B, 77 (1997) A.Marin, J.Diaz, R.Averbeck, S.Hlavac, R.Holzmann, F.Lefevre, A.Schubert, R.S.Simon, Y.Charbonnier, G.Martinez, Y.Schutz, F.M.Marques, M.Appenheimer, F.D.Berg, V.Metag, R.Novotny, H.Stroher, J.Weiss, A.R.Wolf, M.Wolf, H.Lohner, R.W.Ostendorf, R.H.Siemssen, P.Vogt, H.W.Wilschut, A.Kugler, R.Pleskac, P.Tlusty, V.Wagner, Gy.Wolf Exclusive π0- and η-Meson Production in 40Ar + (nat)Ca at 800A MeV NUCLEAR REACTIONS Ca(40Ar, X), E=800 MeV/nucleon; measured π0, η production σ, multiplicities, transverse mass distributions; deduced reaction mechanism features. Model comparisons.
doi: 10.1016/S0370-2693(97)00937-4
1995BI08 Phys.Rev. C51, 3496 (1995) Y.Birenbaum, Z.Berant, S.Kahane, A.Wolf, R.Moreh Absolute Cross Sections for (γ, n) Transitions in Lead, Bismuth, and Terbium NUCLEAR REACTIONS Pb, 209Bi, Th(γ, n), E=6-11.4 MeV; measured absolute σ(E). Thermal neutron capture photons, 3Hen-spectrometer. Direct-semi-direct, compound nucleus models.
doi: 10.1103/PhysRevC.51.3496
1995WO01 Phys.Rev. C51, 2381 (1995) A.Wolf, R.L.Gill, Z.Berant, D.S.Brenner g Factor of the (3/2)+ 121.8-keV Level in 99Zr RADIOACTIVITY 99Y(β-) [from 235U(n, F), E=thermal]; measured γγ(θ, H). 99Zr level deduced g factor. Model comparison.
doi: 10.1103/PhysRevC.51.2381
1995ZA01 Phys.Rev. C51, 98 (1995) N.V.Zamfir, R.L.Gill, D.S.Brenner, R.F.Casten, A.Wolf Study of Low-Spin States in 122Cd RADIOACTIVITY 122Ag(β-); measured Eγ, Iγ, γγ-, βγγ-coin, γγ(θ), T1/2. 122Cd deduced levels, J, π, B(λ). Phonon, interacting boson model.
doi: 10.1103/PhysRevC.51.98
1994BO56 Z.Phys. C63, 37 (1994) M.Bockhorst, G.Burbach, R.Burgwinkel, J.Empt, B.Guse, K.-M.Haas, J.Hannappel, K.Heinloth, T.Hey, P.Hoffmann-Rothe, K.Honscheid, T.Jahnen, H.P.Jakob, N.Jopen, H.Jungst, U.Kirch, F.-J.Klein, D.Kostrewa, L.Lindemann, J.Link, J.Manns, D.Menze, H.Merkel, R.Merkel, W.Neuerburg, E.Paul, R.Plotzke, U.Schenk, S.Schmidt, J.Scholmann, P.Schutz, H.C.Schultz-Coulon, M.Schweitzer, W.J.Schwille, M.-Q.Tran, G.Umlauf, W.Vogl, R.Wedemeyer, F.Wehnes, J.Wisskirchen, A.Wolf Measurement of γp → K+ (Lambda) and γp → K+ Σ0 at Photon Energies up to 1.47 GeV NUCLEAR REACTIONS 1H(γ, X), E=0.96-1.47 GeV; measured invariant mass spectra for Lambda, Σ0 production, polarization.
doi: 10.1007/BF01577542
1994FI11 J.Labelled Compd.Radiopharm. 35, 208 (1994) M.L.Firouzbakht, D.J.Schlyer, A.P.Wolf The Yield of F-18 from Different Target Designs in the 18O(p, n)18F Reaction on Frozen [18O]CO2
1994FI12 J.Labelled Compd.Radiopharm. 35, 257 (1994) M.L.Firouzbakht, D.J.Schlyer, A.P.Wolf The Yield of I-124 from Different Target Materials in the 124Te(d, 2n)124I Reaction and an Inproved Recovery Method for Te-124 NUCLEAR REACTIONS, ICPND 124Te(d, n), E not given; measured γ spectra; deduced 124I yield for different target materials.
1994SC50 Nucl.Instrum.Methods Phys.Res. A344, 470 (1994) W.J.Schwille, M.Bockhorst, G.Burbach, R.Burgwinkel, J.Empt, B.Guse, K.-M.Haas, J.Hannappel, K.Heinloth, T.Hey, K.Honscheid, T.Jahnen, H.P.Jakob, N.Jopen, H.Jungst, U.Kirch, F.-J.Klein, D.Kostrewa, L.Lindemann, J.Link, J.Manns, D.Menze, H.Merkel, R.Merkel, W.Neuerburg, E.Paul, R.Plotzke, U.Schenk, S.Schmidt, J.Scholmann, P.Schutz, H.-C.Schultz-Coulon, M.Schweitzer, M.-Q.Tran, W.Vogl, R.Wedemeyer, F.Wehnes, J.Wisskirchen, A.Wolf Design and Construction of the SAPHIR Detector
doi: 10.1016/0168-9002(94)90868-0
1994WO01 Phys.Rev. C49, 802 (1994) A.Wolf, R.F.Casten, N.V.Zamfir, D.S.Brenner Evidence for Phase Transitional Behavior of Even-Even Nuclei from Differential Observables NUCLEAR STRUCTURE Z=52-70; N=84-104; 164,162,160,158,156Dy; analyzed radii, two-neutron separation energy, B(λ) differences, level energy data; deduced phase transitional behavior features.
doi: 10.1103/PhysRevC.49.802
1993FI08 Appl.Radiat.Isot. 44, 1081 (1993) M.L.Firouzbakht, D.J.Schlyer, S.J.Gatley, A.P.Wolf A Cryogenic Solid Target for the Production of [18F]Fluoride from Enriched [18O]Carbon Dioxide NUCLEAR REACTIONS, ICPND 18O(p, n), E=18 MeV; measured residual (in fluoride chemical form) production saturation yield. Cryogenic solid target.
doi: 10.1016/0969-8043(93)90109-N
1993FI09 Nucl.Instrum.Methods Phys.Res. B79, 909 (1993) M.L.Firouzbakht, D.J.Schlyer, R.D.Finn, G.Laguzzi, A.P.Wolf Iodine-124 Production: Excitation function for the 124Te(d, 2n)124I and 124Te(d, 3n)123I reactions from 7 to 24 MeV NUCLEAR REACTIONS, ICPND 124Te(d, 2n), (d, 3n), E=7.5-23.6 MeV; measured residuals yield, σ vs E.
doi: 10.1016/0168-583X(93)95496-R
1993TO01 J.Phys.(London) G19, 187 (1993) J.R.D.Todd, A.R.Wolf, J.J.Hogan, D.J.Parker Fission Events in the 120 MeV 12C + 238U System NUCLEAR REACTIONS 238U(12C, F), E=120 MeV; measured fission fragment σ(θ), differential range distribution, production σ, kinetic energy distributions. Recoil method.
doi: 10.1088/0954-3899/19/1/013
1993WO06 Phys.Lett. 312B, 372 (1993) A.Wolf, O.Scholten, R.F.Casten F-Spin Purity of 2+1 States in Even-Even Nuclei NUCLEAR STRUCTURE 110Pd, 152Sm, 154Gd, 168Er, 184W, 130,132Ba, 186,192Os, 146,148Ce, 150Nd, 192,194,196Pt, 170Yb, 180Hf; analyzed g factor data; deduced F-spin purity upper limits.
doi: 10.1016/0370-2693(93)90969-O
1993WO07 Phys.Rev. C48, 562 (1993) A.Wolf, R.L.Gill, D.S.Brenner, Z.Berant, R.B.Schuhmann, N.V.Zamfir g Factor of the (3/2)+ 93.6 keV Level in 91Sr RADIOACTIVITY 91Rb(β-) [from 235U(n, F), E=thermal]; measured γγ(θ), oriented nuclei. 91Sr level deduced g factor.
doi: 10.1103/PhysRevC.48.562
1992CA13 Phys.Lett. 281B, 1 (1992) Disentangling the Proton and Neutron Contributions to Collectivity. Effective Charges as Derivatives NUCLEAR STRUCTURE 144,148,150Sm, 104,106,108,110Pd; Z=42-96; analyzed E2 transition matrix elements, B(λ); deduced n-, p-effective charges, contributions to collectivity separated. Valence nuclear models.
doi: 10.1016/0370-2693(92)90263-4
1992FI03 Appl.Radiat.Isot. 43, 741 (1992) M.L.Firouzbakht, D.J.Schlyer, A.P.Wolf Effect of Foil Material on the Apparent Yield of the 124Xe(p, X)123I Reaction NUCLEAR REACTIONS 124Xe(p, 2n)123I, 124Xe(p, np)123I, E=cyclotron; measured residual yield following 123Cs, 123Xe decay; deduced material effect on 123Xe recovery.
doi: 10.1016/0883-2889(92)90236-8
1992WO11 Phys.Rev. C46, 1323 (1992) Effective Charges and Their Relation to Collectivity and Shell Structure NUCLEAR STRUCTURE 126,128,130,132,134Xe, 154,156,158,160Gd, 164,166,168,170,172,176Yb, 138,142,144Ba, 140,142,146Ce, 142,144,146Nd, 144,148,150Sm; analyzed B(E2) data; deduced effective charges relation to collectivity, shell structure.
doi: 10.1103/PhysRevC.46.1323
1991FI05 J.Labelled Compd.Radiopharm. 30, 111 (1991) M.Firouzbakht, D.J.Schlyer, A.P.Wolf Cross-Section Measurements for the 13C(p, n)13N and 12C(d, n)13N Nuclear Reactions NUCLEAR REACTIONS, ICPND 13C(p, n), E=2-20 MeV; 12C(d, n), E ≤ 20 MeV; measured σ(E).
1991FI06 J.Labelled Compd.Radiopharm. 30, 105 (1991) M.L.Firouzbakht, D.J.Schlyer, A.P.Wolf Production of Iodine-123 from Xenon-124: Comparison of results from different laboratories NUCLEAR REACTIONS, ICPND 124Xe(p, np), E=16-34 MeV; compiled residual production yield data.
1991FI11 Radiochim.Acta 55, 1 (1991) M.L.Firouzbakht, D.J.Schlyer, A.P.Wolf Cross-Section Measurements for the 13C(p, n)13N and 12C(d, n)13N Nuclear Reactions NUCLEAR REACTIONS, ICPND 13C(p, n), E=1-33 MeV; 12C(d, n), E=1-23 MeV; measured residual production absolute σ(E), thick target yields. Gaseous targets.
doi: 10.1524/ract.1991.55.1.1
1991WO01 Phys.Rev. C43, 2279 (1991) A.Wolf, O.Scholten, R.F.Casten Analytic Formula for B(E2) Values in Even-Even Nuclei with A > 60 NUCLEAR STRUCTURE A>60; calculated B(E2), even-even nuclei. Analytic formula.
doi: 10.1103/PhysRevC.43.2279
1990MA25 Phys.Rev. C41, R2469 (1990) H.Mach, W.Nazarewicz, D.Kusnezov, M.Moszynski, B.Fogelberg, M.Hellstrom, L.Spanier, R.L.Gill, R.F.Casten, A.Wolf Influence of Shell Effects and Stable Octupole Deformation on the E1 and E2 Transition Rates in the Heavy-Ba Region RADIOACTIVITY 142,144,146Cs(β-); measured βγγ-coin. 142,144,146Ba levels deduced T1/2, intrinsic dipole, quadrupole moments. Interacting boson model.
doi: 10.1103/PhysRevC.41.R2469
1989CA21 Phys.Rev. C40, 1806 (1989) R.F.Casten, K.Heyde, A.Wolf, P.von Brentano Saturation Effects in Gamma-Band Energies NUCLEAR STRUCTURE Er, Dy, Pu, U; calculated gamma-band energy difference vs valence nucleon number; deduced saturation effects features.
doi: 10.1103/PhysRevC.40.1806
1989WO05 Phys.Rev. C40, 932 (1989) A.Wolf, K.Sistemich, H.Mach, R.L.Gill, R.F.Casten, J.A.Winger Magnetic Moment of the 21+ State in 98Sr RADIOACTIVITY 98Rb(β-); measured γγ-coin, γγ(θ, H). 100Zr, 98Rb level deduced g. Other data input.
doi: 10.1103/PhysRevC.40.932
1988BI05 Phys.Rev.Lett. 61, 810 (1988); Erratum Phys.Rev.Lett. 62, 115 (1989) Y.Birenbaum, Z.Berant, A.Wolf, S.Kahane, R.Moreh Differential Cross Sections for the D(γ, n) Reaction below 10 MeV NUCLEAR REACTIONS 2H(γ, n), E=6-9 MeV; measured photodisintegration σ(θ), neutron yield. Monochromatic photon source, high resolution neutron spectrometer.
doi: 10.1103/PhysRevLett.61.810
1988CA13 Phys.Lett. 208B, 33 (1988) A Valence Space Solution to the B(E2) Saturation Problem in Deformed Nuclei NUCLEAR STRUCTURE Z=58-74; analyzed B(E2); deduced valence saturation cause.
doi: 10.1016/0370-2693(88)91198-7
1988KR04 Z.Phys. A329, 235 (1988) A.Kreissl, A.D.Hancock, H.Koch, Th.Kohler, H.Poth, U.Raich, D.Rohmann, A.Wolf, L.Tauscher, A.Nilsson, M.Suffert, M.Chardalas, S.Dedoussis, H.Daniel, T.von Egidy, F.J.Hartmann, W.Kanert, H.Plendl, G.Schmidt, J.J.Reidy First Direct Observation of Strong Interaction Spin-Orbit Effects in Antiprotonic Atoms ATOMIC PHYSICS 174Yb, 138Ba(p-bar, X), E not given; measured X-ray spectra; deduced strong interaction spin-orbit effects, energy shifts, widths.
1988WO03 Phys.Rev. C37, 1253 (1988) A.Wolf, R.L.Gill, H.Mach, R.F.Casten, J.A.Winger Systematics of g Factors in the Neutron-Rich 142,144,146Ba Isotopes RADIOACTIVITY 142,144,146Cs(β-); measured γγ(θ, H). 142,144,146Ba levels deduced g.
doi: 10.1103/PhysRevC.37.1253
1987BO17 Nucl.Instrum.Methods Phys.Res. B26, 491 (1987) J.W.Borgs, J.Chatzipetros, H.Lawin, G.Menzen, K.Sistemich, A.Wolf A Superconducting Magnet for γ-Factor Studies at JOSEF RADIOACTIVITY 102,104Nb(β-); measured γγ(θ, H). 102,104Mo deduced 2+ state g factors. Superconducting magnet.
doi: 10.1016/0168-583X(87)90799-3
1987FI08 Radiochim.Acta 41, 1 (1987) M.L.Firouzbakht, R.-R.Teng, D.J.Schlyer, A.P.Wolf Production of High Purity Iodine-123 from Xenon-124 at Energies between 15 and 34 MeV NUCLEAR REACTIONS, ICPND 124Xe(p, pn), E=15-34 MeV; measured residual production thick target yields. 124Xe(p, 2n), E=15-34 MeV; measured 123Xe thick target yield following residue decay; deduced 123I production consequences.
doi: 10.1524/ract.1987.41.1.1
1987PO05 Nucl.Phys. A466, 667 (1987) H.Poth, H.Barth, G.Buche, A.D.Hancock, H.Koch, Th.Kohler, A.Kreissl, U.Raich, D.Rohmann, A.Wolf, L.Tauscher, A.Nilsson, M.Suffert, M.Chardalas, S.Dedoussis, H.Daniel, T.von Egidy, F.J.Hartmann, W.Kanert, H.S.Plendl, G.Schmidt, J.J.Reidy Measurement of Strong-Interaction Effects in Light Antiprotonic Atoms ATOMIC PHYSICS 6,7Li, 14N, 19F, 23Na(p-bar, X), E at 300 MeV/c; measured X-ray spectra. 7,6Li, 14N, 19F, 23Na deduced antiprotonic strong interaction level shifts, widths.
doi: 10.1016/0375-9474(87)90462-3
1987WO03 Phys.Lett. 190B, 19 (1987) A.Wolf, R.F.Casten, D.D.Warner g Factors in Heavy Nuclei and the Proton-Neutron Interaction NUCLEAR STRUCTURE A=70-200; analyzed effective boson g factors, numbers; deduced systematics.
doi: 10.1016/0370-2693(87)90833-1
1987WO05 Phys.Rev. C36, 851 (1987) Effective Valence Proton and Neutron Numbers in Transitional A ≈ 150 Nuclei from B(E2) and g-Factor Data NUCLEAR STRUCTURE 142,144,146Ba, 146,148Ce, 144,146,148,150Nd, 148,150,152,154Sm; analyzed B(E2), g; deduced effective valence proton, neutron numbers.
doi: 10.1103/PhysRevC.36.851
1986BE30 Phys.Rev. C34, 1481 (1986) Z.Berant, J.Ivri, R.Moreh, A.Wolf 1+ State in 44Ca NUCLEAR REACTIONS 44Ca(γ, γ'), E=4-7 MeV; measured Eγ, Iγ, γ(θ), polarization; deduced σ. 44Ca deduced transition γ-multipolarity, δ, Γ, Γ0, Γ/Γ0.
doi: 10.1103/PhysRevC.34.1481
1986BI12 Phys.Rev. C34, 2055 (1986) Y.Birenbaum, Z.Berant, S.Kahane, R.Moreh, A.Wolf E1-E2 Interference in 159Tb(γ, n) and 209Bi(γ, n) Reactions NUCLEAR REACTIONS 159Tb, 209Bi(γ, n), E=7-11.4 MeV; measured σ(En), σ(θ); deduced angular distribution coefficients vs energies. 159Tb, 209Bi deduced strong E1, E2 interference effects. 3He spectrometer. Compound nucleus process, direct-semidirect model.
doi: 10.1103/PhysRevC.34.2055
1986GI05 Phys.Rev. C33, 1030 (1986) R.L.Gill, D.D.Warner, H.Mach, A.Piotrowski, A.Wolf, J.C.Hill, F.K.Wohn, J.A.Winger, B.Fogelberg Magnetic Moments of the 2+1 States in 146, 148Ce RADIOACTIVITY 146,148La(β-) [from 235U(n, F), E=thermal]; measured γγ(θ, H); deduced Z=64 subshell gradual dissipation. 146,148Ce levels deduced g.
doi: 10.1103/PhysRevC.33.1030
1986GI14 Phys.Rev. C34, 1983 (1986) R.L.Gill, D.D.Warner, A.Wolf, J.A.Winger g Factor of the 21+ State in 142Ba RADIOACTIVITY 142Cs(β-) [from 235U(n, F), E=thermal]; measured γγ(θ, H). 142Ba level deduced g. Hydrodynamic model, interacting boson approximation.
doi: 10.1103/PhysRevC.34.1983
1986KO22 Phys.Lett. 176B, 327 (1986) Th.Kohler, P.Blum, G.Buche, A.D.Hancock, H.Koch, A.Kreissl, H.Poth, U.Raich, D.Rohmann, G.Backenstoss, Ch.Findeisen, J.Repond, L.Tauscher, A.Nilsson, S.Carius, M.Suffert, S.Charalambus, M.Chardalas, S.Dedoussis, H.Daniel, T.von Egidy, F.J.Hartmann, W.Kanert, G.Schmidt, J.J.Reidy, M.Nicholas, A.Wolf Precision Measurement of Strong Interaction Isotope Effects in Antiprotonic 16O, 17O, and 18O Atoms NUCLEAR REACTIONS 16,17,18O(p-bar, X), E=low; measured antiprotonic X-rays. ATOMIC PHYSICS 16,17,18O(p-bar, X), E=low; measured antiprotonic X-rays; deduced strong interaction shifts, widths.
doi: 10.1016/0370-2693(86)90173-5
1986RO23 Z.Phys. A325, 261 (1986) D.Rohmann, H.Barth, A.D.Hancock, H.Koch, Th.Kohler, A.Kreissl, H.Poth, U.Raich, A.Wolf, L.Tauscher, M.Suffert, M.Chardalas, S.Dedoussis, A.Nilsson, W.Kanert, T.von Egidy, F.J.Hartmann, G.Schmidt, J.J.Reidy Measurement of the 4f Strong Interaction Level Width in Light Antiprotonic Atoms NUCLEAR REACTIONS 14N, 16,17,18O, 19F, 23Na(p-bar, X), E=200, 300 MeV/c; measured antiprotomic X-ray spectra; deduced target atomic 4f level Γ; calculated antiprotonic transition intensities. Scintillation counters. Cascade model. ATOMIC PHYSICS 14N, 16,17,18O, 19F, 23Na(p-bar, X), E=200, 300 MeV/c; measured antiprotonic X-ray spectra. 14N, 16,17,18O, 19F, 23Na deduced 4f level Γ; calculated antiprotonic transition intensities. Scintillator counters. Cascade model.
1986SA33 Radiochim.Acta 39, 165 (1986) M.Sajjad, R.M.Lambrecht, A.P.Wolf Cyclotron Isotopes and Radiopharmaceuticals. XXXVII. Excitation Functions for the 16O(p, α)13N and 14N(p, pn)13N Reactions NUCLEAR REACTIONS, ICPND 16O(p, α), E=6.5-16.5 MeV; 14N(p, pn), E=12-30 MeV; measured σ(E); deduced thick target yields. Enriched gas target, residual 13N activity. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0202. 1985BE04 Phys.Rev. C31, 570 (1985) Z.Berant, A.Wolf, J.C.Hill, F.K.Wohn, R.L.Gill, H.Mach, M.Rafailovich, H.Kruse, B.H.Wildenthal, G.Peaslee, A.Aprahamian, J.Goulden, C.Chung g Factor of 4+1 States in the N = 82 Isotones 136Xe and 138Ba RADIOACTIVITY 136I, 138Cs(β-); measured γγ(θ, H, t). 136Xe, 138Ba levels deduced g.
doi: 10.1103/PhysRevC.31.570
1985HI05 Hyperfine Interactions 22, 449 (1985) J.C.Hill, F.K.Wohn, A.Wolf, Z.Berant, R.L.Gill, H.Kruse Study of Magnetic Moments of Nuclear Excited States at TRISTAN NUCLEAR STRUCTURE 134Te, 136Xe, 138Ba, 140Ce; calculated g. Shell model. RADIOACTIVITY 136I, 138Cs(β-) [from 235U(n, F), E=thermal]; measured γγ(θ, H), γ(θ). 136Xe, 138Ba deduced levels, g, γ-branching.
doi: 10.1007/BF02064016
1985KA24 Phys.Rev. C32, 1944 (1985) Photofission of 238U with Neutron-Capture Gamma Rays NUCLEAR REACTIONS 238U(γ, F)132Te/135Xe/138Xe/143Ce/146Ce/85Kr/85mKr/101Tc/104Tc/105Ru/105Rh/87Kr/146Pr/138Cs/133I/135I/91Y/91mY/131Te/133Te/134Te/112Ag/142La/91Sr/97Nb/132I/134I/135I/92Y/89Rb/97Zr/129Sb, E=7.8 MeV; measured Eγ, Iγ, fission fragment cumulative yields, relative yields vs mass number, σ(fragment θ), most probable charge. 238U deduced Γn/Γf.
doi: 10.1103/PhysRevC.32.1944
1985ME13 Z.Phys. A321, 593 (1985) G.Menzen, A.Wolf, H.Lawin, G.Lhersonneau, K.Sistemich Magnetic Moments of the 2+1 States in 102,104Mo RADIOACTIVITY 102,104Nb(β-); measured γγ(θ, H, t). 102,104Mo levels deduced g.
doi: 10.1007/BF01432435
1985SA35 Radiochim.Acta 38, 57 (1985) M.Sajjad, R.M.Lambrecht, A.P.Wolf Cyclotron Isotopes and Radiopharmaceuticals. XXXVI. Investigation of Some Excitation Functions for the Preparation of 15O, 13N and 11C NUCLEAR REACTIONS, ICPND 14N(d, n), E=1.08-12.28 MeV; 15N(p, nα), (p, nd), (p, nt), E=12.55-29.78 MeV; 14N(d, nα), (d, nd), (d, nt), E=8-12.28 MeV; 16O(p, np), E=16.7-32.82 MeV; measured σ(E); calculated thick target yield vs E. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0316. 1985WO10 Phys.Lett. 158B, 7 (1985) A.Wolf, D.D.Warner, N.Benczer-Koller Effective g Factors and Proton-Boson Numbers in the Vicinity of Proton Subshell Closures NUCLEAR STRUCTURE 146,148Ce, 144,146,148,150Nd, 148,150,152,154Sm; analyzed g; deduced effective proton boson number. 90,92,94,96,98,102Kr, 92,94,96,98,100,102Sr; calculated g vs neutron number.
doi: 10.1016/0370-2693(85)90727-0
1984BO05 Nucl.Sci.Eng. 86, 106 (1984) Y.Boneh, S.Goshen, Z.Karpas, O.Shahal, A.Wolf Neutron Yields from Uranium-Fluorine Compounds NUCLEAR REACTIONS 19F(α, n), E=4.18, 4.4, 4.76 MeV; measured thick target neutron yield. Uranium-Fluorine compound α-source. Stopping power calculations.
doi: 10.13182/NSE84-A17973
1984SA30 J.Labelled Compd.Radiopharm. 21, 1260 (1984) M.Sajjad, R.M.Lambrecht, A.P.Wolf Excitation Function for the 15N(p, n)15O Reaction NUCLEAR REACTIONS, ICPND 15N(p, n), E=3.72-16.58 MeV; measured absolute σ(E). Activation technique, enriched target. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0313. 1984SA33 Radiochim.Acta 36, 159 (1984) M.Sajjad, R.M.Lambrecht, A.P.Wolf Cyclotron Isotopes and Radiopharmaceuticals. XXXIV. Excitation Function for the 15N(p, n)15O Reaction NUCLEAR REACTIONS, ICPND 15N(p, n), E=3.72-16.58 MeV; measured residuals absolute σ(E), thick target yield vs E. Enriched target, activation technique. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0313. 1983CH39 Phys.Rev. C28, 2099 (1983) C.Chung, W.B.Walters, D.S.Brenner, A.Aprahamian, R.L.Gill, M.Shmid, R.E.Chrien, L.-J.Yuan, A.Wolf, Z.Berant Decay of 142Ba to Levels of Odd-Odd 142La RADIOACTIVITY 142Ba(β-) [from 235U(n, F), E=thermal]; measured Eγ, Iγ, Eβ, γγ(t, θ), γγ(θ), βγ-coin; deduced Qβ, log ft. 142La deduced levels, J, π, Iβ, δ, ICC, T1/2. Hyperpure Ge, β, γ detectors, mass separated sources.
doi: 10.1103/PhysRevC.28.2099
1983GI04 Phys.Rev. C27, 1732 (1983) R.L.Gill, M.Shmid, R.E.Chrien, Y.Y.Chu, A.Wolf, D.S.Brenner, K.Sistemich, F.K.Wohn, H.Yamamoto, C.Chung, W.B.Walters Levels in 148Ce from the Decay of Mass Separated 148La RADIOACTIVITY 148La(β-) [from 235U(n, F), E=thermal]; measured T1/2, Eγ, Iγ, γγ(t), γγ(θ). 148Ce deduced levels, J, π, Iβ. Hyperpure Ge, Ge(Li) detectors. NUCLEAR STRUCTURE 144,146,150Ce; calculated levels. 148Ce; calculated levels, B(E2) ratios. Interacting boson approximation calculations.
doi: 10.1103/PhysRevC.27.1732
1983HI05 Phys.Rev. C27, 2857 (1983) Decay of Neutron-Rich 152Pr and 152Ce RADIOACTIVITY 152Pr, 152Ce(β+) [from 235U(n, F)]; measured Eγ, Iγ, γγ-, γ(X-ray)-coin, T1/2; deduced log ft. 152Nd, 152Pr deduced levels, J, π.
doi: 10.1103/PhysRevC.27.2857
1983WA11 Phys.Lett. 125B, 351 (1983) W.B.Walters, C.Chung, D.S.Brenner, A.Aprahamian, R.L.Gill, R.E.Chrien, M.Shmid, A.Wolf, L.-J.Yuan Parabolic Energy dependence of Odd-Odd Multiplets in N = 83 Nuclides NUCLEAR STRUCTURE 146Eu, 144Pm, 142Pr, 140La; analyzed level splitting, B(E2) data; deduced quasiparticle blocking effect. Odd proton, neutron quadrupole interaction.
doi: 10.1016/0370-2693(83)91300-X
1983WO03 Nucl.Instrum.Methods 206, 397 (1983) A.Wolf, C.Chung, W.B.Walters, G.Peaslee, R.L.Gill, M.Shmid, V.Manzella, E.Meier, M.L.Stelts, H.I.Liou, R.E.Chrien, D.S.Brenner A Four-Detector System for γ-γ Angular Correlation Studies RADIOACTIVITY 152Eu(EC), (β+); 146La(β-) [from 146Ba decay]; measured γγ(θ). 146Ce deduced dipole transitions. Multiple detector system.
doi: 10.1016/0167-5087(83)90375-7
1983WO05 Phys.Lett. 123B, 165 (1983) A.Wolf, Z.Berant, D.D.Warner, R.L.Gill, M.Shmid, R.E.Chrien, G.Peaslee, H.Yamamoto, J.C.Hill, F.K.Wohn, C.Chung, W.B.Walters Magnetic Moments of 2+1 States as a Probe of the Effective Proton Boson Number near the Z = 64 Subshell NUCLEAR STRUCTURE 144,146Ba, 146,148,150Nd, 148,150,152,154Sm, 154,156Gd; calculated 2+ level μ. Interacting boson model. RADIOACTIVITY 144,146Ba(β-); measured γγ(θ, H). 144,146Ba levels deduced g. Interacting boson model.
doi: 10.1016/0370-2693(83)90414-8
1983WO09 Phys.Rev. C28, 352 (1983) A.Wolf, C.Chung, W.B.Walters, R.L.Gill, M.Shmid, R.E.Chrien, G.Peaslee Gamma-Gamma Angular Correlation Studies for 142Ce RADIOACTIVITY 142La(β-) [from 235U(n, F), E=thermal]; measured γγ(θ). 142Ce levels deduced J, π, δ. Mass separation, Ge detectors.
doi: 10.1103/PhysRevC.28.352
1982BR23 Phys.Rev. C26, 2166 (1982) D.S.Brenner, M.K.Martel, A.Aprahamian, R.E.Chrien, R.L.Gill, H.I.Liou, M.Shmid, M.L.Stelts, A.Wolf, F.K.Wohn, D.M.Rehfield, H.Dejbakhsh, C.Chung Q Values for Neutron-Rich Rubidium and Lanthanum Isotopes RADIOACTIVITY 88Rb(β-), 94Rb(β-), 96Rb(β-), 98Rb(β-), 146La(β-), 148La(β-) [from 235U(n, F)]; measured Eγ, Iγ, Eβ, βγ-, γγ-coin; deduced Qβ, mass excess. On-line mass separation, Ge(Li), hyperpure Ge detectors.
doi: 10.1103/PhysRevC.26.2166
1982YA04 Phys.Rev. C26, 1215 (1982) H.Yamamoto, F.K.Wohn, K.Sistemich, A.Wolf, W.B.Walters, C.Chung, R.L.Gill, M.Shmid, R.E.Chrien, D.S.Brenner Decay of Mass-Separated 141Cs to 141Ba and Systematics of N = 85 Isotones RADIOACTIVITY 141Cs [from 235U(n, F), E=thermal]; measured Eγ, Iγ, γγ-coin, γγ(t), E(X-ray), I(X-ray); deduced log ft. 141Ba deduced levels, J, π, ICC, β-branching, δ(E2/M1). Mass separated source. Hyperpure Ge, Ge(Li) detectors.
doi: 10.1103/PhysRevC.26.1215
1981BI13 Nucl.Phys. A369, 483 (1981) Y.Birenbaum, Z.Berant, S.Kahane, A.Wolf, R.Moreh Angular Distributions of Photoneutrons from the 207,208Pb(γ, n0) Reactions NUCLEAR REACTIONS 208,207Pb(γ, n), E=7.0-11.4 MeV; measured σ(θ). 207,208Pb deduced E2-E1 and M1-E1 interference effects.
doi: 10.1016/0375-9474(81)90033-6
1980BI16 Radiochim.Acta 27, 181 (1980) Experimentally Determined Thick Target Yields for the 14N(p, α)11C Reaction NUCLEAR REACTIONS, ICPND 14N(p, α), E=threshold-18 MeV; measured absolute σ(E), thick target yields. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0286. 1980WO09 Phys.Lett. B97, 195 (1980) A.Wolf, G.Battistuzzi, K.Kawade, H.Lawin, K.Sistemich Magnetic Moment of the First Excited 2+ State in 100Zr RADIOACTIVITY 100Y [from gas-filled fission product separator]; measured γγ-coin, γγ(θ, H). 100Zr level deduced g. Air-jet, tape transport systems.
doi: 10.1016/0370-2693(80)90580-8
1979BI12 Phys.Lett. 88B, 239 (1979) Y.Birenbaum, Z.Berant, A.Wolf, R.Moreh Interference Effects between Multipole Resonances in the 206Pb(γ, n) Reaction NUCLEAR REACTIONS 206Pb(γ, n), E=8.5-11.4 MeV; measured σ(θ); deduced multipole mixing effects.
doi: 10.1016/0370-2693(79)90456-8
1979RU10 Radiochim.Acta 26, 21 (1979) Absolute Cross Sections for the Production of 18F via the 18O(p, n)18F Reaction NUCLEAR REACTIONS 18O(p, n), E=2.3-14.7 MeV; measured absolute production σ(E), saturation activities for 18F. Enriched gas target. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0235. 1978BE45 Nucl.Phys. A306, 101 (1978) Z.Berant, J.Tenenbaum, A.Wolf, R.Moreh Study of the Energy Levels of 93Nb and 123Sb Using Nuclear Photoexcitation NUCLEAR REACTIONS 93Nb, 123Sb(γ, γ'); measured Eγ, Iγ(θ). 93Nb, 123Sb deduced levels, J, π, M1, Γ.
doi: 10.1016/0375-9474(78)90314-7
1978CA29 Radiochim.Acta 25, 17 (1978) V.R.Casella, D.R.Christman, T.Ido, A.P.Wolf Excitation Function for the 14N(p, α)11C Reaction up to 15 MeV NUCLEAR REACTIONS 14N(p, α), E=4.5-15 MeV; measured absolute σ(E). 11C deduced thick target saturation activities. Gas target. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0177. 1978LA22 Int.J.Appl.Radiat.Isotop. 29, 341 (1978) R.M.Lambrecht, R.Fairchild, A.P.Wolf Comments on 'The Radionuclidic Parity and Quality of Iodine-123 Obtainable with the 124Te(p, 2n)123I Reaction' NUCLEAR REACTIONS 124Te(p, 2n), E=26 MeV; measured Eγ, FWHM; deduced production σ of 123I.
doi: 10.1016/0020-708X(78)90070-4
1978VE11 Radiochim.Acta 24, 65 (1978) Excitation Function for 15O Production via the 14N(d, n)15O Reaction NUCLEAR REACTIONS 14N(d, n), E=0.6-14.35 MeV; measured σ. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0125. 1977JA13 Nucl.Phys. A291, 1 (1977) Studies of Nuclear Levels Around 7.5 MeV Using a High Resolution γ-Monochromator NUCLEAR REACTIONS Cd, Ce, Ba, 139La, 141Pr, 209Bi(γ, γ'), E=7.28, 7.63 MeV; measured yields, scattering spectra. 139La, 209Bi deduced levels, gΓ0. Natural targets.
doi: 10.1016/0375-9474(77)90194-4
1977KO32 Int.J.Appl.Radiat.Isotop. 28, 395 (1977) K.Kondo, R.M.Lambrecht, A.P.Wolf Iodine-123 Production for Radiopharmaceuticals - XX NUCLEAR REACTIONS 124Te(p, n), (p, 2n), E=9.95-29.18 MeV; measured σ(E) for production of 123I.
doi: 10.1016/0020-708X(77)90132-6
1976LA20 Int.J.Appl.Radiat.Isotop. 27, 675 (1976) R.M.Lambrecht, A.P.Wolf, F.Helus, M.Untucht, W.Maier-Borst High Energy Alpha Reactions for the Production of the (123Cs 5.8 min β+ →)123Xe 2.1 hr β+, EC → 123I Generator and 125Xe and 127Cs for Radiopharmaceutical Applications NUCLEAR REACTIONS Te, I, 123Sb(α, X), E=70-102 MeV; measured production σ.
doi: 10.1016/0020-708X(76)90011-9
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