NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = C.Gaarde Found 77 matches. 2005AL37 Nucl.Instrum.Methods Phys.Res. A551, 290 (2005) G.D.Alkhazov, V.V.Astashin, A.G.Atamantchouk, W.Augustyniak, D.Bachelier, V.V.Baublis, M.Boivin, J.-L.Boyard, J.-F.Clavelin, P.Courtat, M.Denoit, R.Douet, C.Ellegaard, L.Farhi, C.Gaarde, R.Gacougnolle, V.Ya.Gerzenstein, V.L.Golovtsov, V.V.Golubev, T.Hennino, J.-C.Jourdain, A.V.Khanzadeev, B.G.Komkov, A.V.Kravtsov, L.G.Kudin, R.Kunne, J.Larsen, S.Lebon, L.V.Malinina, A.Maroni, J.-M.Martin, H.-P.Morsch, V.A.Mylnikov, E.M.Orischin, M.Osterlund, V.Poux, A.N.Prokofiev, P.Radvanyi, B.Ramstein, B.V.Razmyslovich, M.Roy-Stephan, V.M.Samsonov, R.Skowron, I.B.Smirnov, E.A.Strokovsky, I.I.Tkach, V.V.Vikhrov, S.S.Volkov, An.A.Vorobyov, A.A.Zhdanov, P.Zupranski SPES4-π: installation for exclusive study of nuclear reactions NUCLEAR REACTIONS 12C(3He, tπ+), E=2 GeV; measured excitation energy spectra. 1H(d, d'X), (α, α'X), E ≈ 1 GeV/nucleon; measured missing mass spectra.
doi: 10.1016/j.nima.2005.06.062
2005BO22 Nucl.Phys. A755, 507c (2005) J.-L.Boyard, W.Augustyniak, R.Dahl, M.Drews, C.Ellegaard, L.Farhi, C.Gaarde, T.Hennino, J.A.Jensen, J.-C.Jourdain, M.Kagarlis, R.Kunne, J.S.Larsen, P.Radvanyi, B.Ramstein, M.Roy-Stephan, P.Zupranski Coherent pion production in heavy ion charge exchange reactions NUCLEAR REACTIONS 12C(3He, tπ+), E=2 GeV; 12C(12C, 12Nπ-), E=1.1 GeV/nucleon; measured σ(E, θ).
doi: 10.1016/j.nuclphysa.2005.03.064
2003RA10 Eur.Phys.J. A 16, 583 (2003) B.Ramstein, C.Mosbacher, T.Hennino, W.Augustyniak, D.Bachelier, H.G.Bohlen, J.L.Boyard, R.Dahl, C.Ellegaard, C.Gaarde, J.Gosset, J.C.Jourdain, J.S.Larsen, M.C.Lemaire, D.L'Hote, H.P.Morsch, M.Osterlund, J.Poitou, P.Radvanyi, M.Roy-Stephan, T.Sams, M.Skousen, S.Tarle-Rousteau, P.Zupranski 2H(3He, t)2p reaction at 2 GeV NUCLEAR REACTIONS 2H(3He, t), (3He, tX), E=2 GeV; measured triton and proton spectra, σ(θ); deduced role of Δ excitation. Comparison with coupled channels model predictions.
doi: 10.1140/epja/i2002-10116-7
2001MA91 Phys.Rev. C64, 064001 (2001) L.V.Malinina, G.D.Alkhazov, W.Augustyniak, M.Boivin, J.-L.Boyard, R.Dahl, M.Drews, C.Ellegaard, L.Farhi, C.Gaarde, T.Hennino, J.C.Jourdain, M.Kagarlis, A.V.Kravtsov, R.Kunne, J.S.Larsen, P.Morsch, V.A.Mylnikov, E.M.Orichtchin, C.F.Perdrisat, N.M.Piskunov, A.N.Prokofiev, V.Punjabi, P.Radvanyi, B.Ramstein, B.V.Razmyslovich, M.Roy-Stephan, I.M.Sitnik, M.Skousen, E.A.Strokovsky, I.I.Tkach, E.Tomasi-Gustafsson, S.S.Volkov, A.A.Zhdanov, P.Zupranski Analyzing Power of Inelastic dp Scattering in the Energy Region of Δ and Roper Resonances Excitation NUCLEAR REACTIONS 1H(polarized d, dπ+), (polarized d, dπ0), (polarized d, dπX), E at 3.73 GeV/c; measured tensor and vector analyzing powers. Comparisons with previous results.
doi: 10.1103/PhysRevC.64.064001
2000BO47 Acta Phys.Pol. B31, 2139 (2000) J.L.Boyard, L.Farhi, T.Hennino, J.C.Jourdain, R.Kunne, P.Radvanyi, B.Ramstein, M.Roy-Stephan, R.Dahl, M.Drews, C.Ellegaard, C.Gaarde, J.Jensen, J.Larsen, M.Skousen, M.A.Kagarlis, W.Augustyniak, P.Zupranski Exploring the Collective Spin-Isospin Longitudinal Response of Nuclei with Coherent Pion Production in (3He, tπ+) NUCLEAR REACTIONS 12C, 40Ca, 208Pb(3He, tπ+), E=2 GeV; measured coherent pion production σ(θ), excitation energy spectra.
1999RA22 Eur.Phys.J. A 6, 225 (1999) B.Ramstein, C.A.Mosbacher, D.Bachelier, I.Bergqvist, M.Boivin, J.L.Boyard, A.Brockstedt, L.Carlen, R.Dahl, P.Ekstrom, C.Ellegaard, C.Gaarde, T.Hennino, J.C.Jourdain, C.Goodman, J.S.Larsen, P.Radvanyi, M.Roy-Stephan Inclusive 2(3He, t) Reaction at 2 GeV NUCLEAR REACTIONS 2H(3He, t), E=2 GeV; measured σ(E, θ), energy transfer spectra; deduced Δ resonance contributions, final state interaction role. Coupled channels analysis.
doi: 10.1007/s100500050338
1998DA25 Acta Phys.Pol. B29, 3009 (1998) R.Dahl, L.Farhi, W.Augustiniak, J.L.Boyard, M.Drews, C.Ellegaard, C.Gaarde, T.Hennino, J.Jensen, J.C.Jourdain, R.Kunne, J.Larsen, P.Radvanyi, B.Ramstein, M.Roy-Stephan, M.Skousen, P.Zupranski Evidence of Coherent π+ Production in (3He, t) Reactions NUCLEAR REACTIONS 12C(3He, tπ+), E=2 GeV; measured coherent pion production σ(θ); deduced ground-state conbtribution.
1996FA27 Acta Phys.Pol. B27, 3035 (1996) L.Farhi, M.Roy-Stephan, W.Augustiniak, J.L.Boyard, R.Dahl, C.Ellegaard, C.Gaarde, T.Hennino, J.C.Jourdain, M.Kagarlis, J.S.Larsen, P.Radvanyi, B.Ramstein, M.Skousen, P.Zupranski Coherent Production of Pions in Nuclei with (3He, t) Charge Exchange Reaction at 2 GeV
1996GA20 Nucl.Phys. A606, 227 (1996) The Spin-Isospin Response NUCLEAR REACTIONS 2H, 12C(p, n), E=795, 495 MeV; 12C(polarized p, n), E=795 MeV; 4He, 12C(3He, tπ+), E=2 GeV; analyzed data; deduced coherent pions evidence. Spin-isospin channel.
doi: 10.1016/0375-9474(96)00207-2
1996RA49 Acta Phys.Pol. B27, 3229 (1996) B.Ramstein, S.Rousteau, T.Hennino, J.L.Boyard, R.Dahl, C.Ellegaard, C.Gaarde, J.Gosset, J.C.Jourdain, M.Kagarlis, J.S.Larsen, M.C.Lemaire, D.L'Hote, H.P.Morsch, M.Osterlund, P.Radvanyi, M.Roy-Stephan, T.Sams, M.Skousen, W.Spang, P.Zupranski Δ Production and Propagation in Nuclei
1995SA06 Phys.Rev. C51, 1945 (1995) T.Sams, C.Ellegaard, C.Gaarde, J.S.Larsen, J.L.Boyard, T.Hennino, J.C.Jourdain, B.Ramstein, M.Roy-Stephan, P.Radvanyi, A.Brockstedt, M.Osterlund, P.Zupranski, C.D.Goodman, M.Ichimura, V.F.Dmitriev Quasifree (d(pol), 2He) Data NUCLEAR REACTIONS 2,1H, 12C(polarized d, X), E=1.6, 2 GeV; measured σ(θ), tensor analyzing powers vs momentum transfer; deduced spin-isospin response in the quasifree region.
doi: 10.1103/PhysRevC.51.1945
1994SN01 Phys.Rev. C50, 338 (1994) Cascade Simulation of a Δ Isobar Propagating in a Nucleus NUCLEAR REACTIONS 12C(3He, t), E=2 GeV; 12C(p, n), E=830 MeV; calculated energy transfer spectra, yield vs (π+p) invariant mass; deduced measurable consequences of Δ isobars related features. Cascade model.
doi: 10.1103/PhysRevC.50.338
1993GA14 Phys.Scr. 48, 81 (1993) Δ-Isobars in Nuclei or Off-Shell Pions in the Medium NUCLEAR REACTIONS 12C(p, n), E not given; analyzed σ(θ) vs neutron momentum; deduced Δ-isobar decay role, medium effects on Δ.
doi: 10.1088/0031-8949/48/1/013
1993HE03 Phys.Lett. 303B, 236 (1993) T.Hennino, B.Ramstein, D.Bachelier, J.L.Boyard, C.Ellegaard, C.Gaarde, J.Gosset, J.C.Jourdain, J.S.Larsen, M.C.Lemaire, D.L'Hote, H.P.Morsch, M.Osterlund, J.Poitou, P.Radvanyi, S.Rousteau, M.Roy-Stephan, T.Sams, P.Zupranski Coherent Pions in Charge-Exchange Reactions NUCLEAR REACTIONS 12C(3He, tπ+), E=2 GeV; measured tπ-coin, σ(θ, p(π)).
doi: 10.1016/0370-2693(93)91426-N
1993RO30 Acta Phys.Pol. B24, 1747 (1993) S.Rousteau, T.Hennino, B.Ramstein, J.L.Boyard, C.Ellegaard, C.Gaarde, J.Gosset, J.C.Jourdain, M.Kagarlis, J.S.Larsen, M.C.Lemaire, D.L'Hote, H.P.Morsch, M.Osterlund, J.Poitou, P.Radvanyi, M.Roy-Stephan, T.Sams, P.Zupranski Δ Resonance Decay and Absorption in Nuclei NUCLEAR REACTIONS 1,2H, 12C, 208Pb(3He, tX), E=2 GeV; measured 2p-event missing energy spectrum, energy transfer spectra; deduced Δ-resonance decay features, absorption mechanism.
1992HE08 Phys.Lett. 283B, 42 (1992) T.Hennino, B.Ramstein, D.Bachelier, H.G.Bohlen, J.L.Boyard, C.Ellegaard, C.Gaarde, J.Gosset, J.C.Jourdain, J.S.Larsen, M.C.Lemaire, D.L'Hote, H.P.Morsch, M.Osterlund, J.Poitou, P.Radvanyi, M.Roy-Stephan, T.Sams, K.Sneppen, O.Valette, P.Zupranski Study of Decay and Absorption of the Δ Resonance in Nuclei with a 4π Detector NUCLEAR REACTIONS 1,2H, 12C(3He, t), E=2 GeV; measured energy transfer spectra, (π+p)(t)-coin; deduced Δ-resonance decay, absorption mechanism.
doi: 10.1016/0370-2693(92)91423-7
1991BR20 Nucl.Phys. A530, 571 (1991) A.Brockstedt, I.Bergqvist, L.Carlen, L.P.Ekstrom, B.Jakobsson, C.Ellegaard, C.Gaarde, J.S.Larsen, C.Goodman, M.Bedjidian, D.Contardo, J.Y.Grossiord, A.Guichard, M.Roy-Stephan, M.Boivin, T.Hasegawa, P.Radvanyi The (3He, t) Reaction at Intermediate Energies Spin-Isospin Multipole Transitions NUCLEAR REACTIONS 26Mg, 40,48Ca, 54Fe, 90Zr, 208Pb(3He, t), E=0.9-2 GeV; measured σ(θ). 26Al, 40,48Sc, 54Co, 90Nb, 208Bi deduced spin multipole, Gamow-Teller transition strength distributions. DWIA calculations, quasi-elastic peak, distortion effects.
doi: 10.1016/0375-9474(91)90770-7
1990GA05 Nucl.Phys. A507, 79c (1990) Spin-Isospin Excitations
doi: 10.1016/0375-9474(90)90570-C
1990GA19 Phys.Scr. T32, 14 (1990) Spin Excitations in Nuclei NUCLEAR REACTIONS 208Pb, 90Zr(p, n), E=200 MeV; 12C, 90Zr(p, n), E=800 MeV; 90Zr(3He, t), E=900 MeV; 90Zr, 12C(p, n), E not given; 12C(3He, t), E=2 GeV; 208Pb(12C, 12N), E=1100 MeV/nucleon; 12C(40Ar, 40K), E=780 MeV/nucleon; compiled double differential data; deduced spin response features, Δ-excitation role.
doi: 10.1088/0031-8949/1990/T32/002
1990RA08 Phys.Rev. C41, 1920 (1990) J.Rapaport, C.C.Foster, C.D.Goodman, C.A.Goulding, T.N.Taddeucci, D.J.Horen, E.R.Sugarbaker, C.Gaarde, J.Larsen, J.A.Carr, F.Petrovich, M.J.Threapleton (p, n) Reaction on Li Isotopes for E(p) = 60-200 MeV NUCLEAR REACTIONS 7,6Li(p, n), (polarized p, n), E=60-200 MeV; measured σ(θ). 6Be deduced Gamow-Teller transition strength. 7Be deduced branching ratio, Gamow-Teller transition strength. DWIA analysis.
doi: 10.1103/PhysRevC.41.1920
1990TA11 Phys.Rev. C41, 2548 (1990) T.N.Taddeucci, W.P.Alford, M.Barlett, R.C.Byrd, T.A.Carey, D.E.Ciskowski, C.C.Foster, C.Gaarde, C.D.Goodman, C.A.Goulding, E.Gulmez, W.Huang, D.J.Horen, J.Larsen, D.Marchlenski, J.B.McClelland, D.Prout, J.Rapaport, L.J.Rybarcyk, W.C.Sailor, E.Sugarbaker, C.A.Whitten, Jr. Zero-Degree Cross Sections for the 7Li(p, n)7Be(g.s.+0.43-MeV) Reaction in the Energy Range 80-795 MeV NUCLEAR REACTIONS 7Li(p, n), E=80-795 MeV; measured σ(θ).
doi: 10.1103/PhysRevC.41.2548
1990TA15 Phys.Rev. C42, 935 (1990) T.N.Taddeucci, R.C.Byrd, T.A.Carey, D.E.Ciskowski, C.C.Foster, C.Gaarde, C.D.Goodman, E.Gulmez, W.Huang, D.J.Horen, J.Larsen, D.Marchlenski, J.B.McClelland, D.Prout, J.Rapaport, L.J.Rybarcyk, E.Sugarbaker, I.J.Van Heerden, C.A.Whitten, Jr. Gamow-Teller Transition Strengths from the 11B(p, n)11C Reaction in the Energy Range 160-795 MeV NUCLEAR REACTIONS 11B(p, n), E=160-795 MeV; measured σ(En, θ=0°). 11C levels deduced Gamow-Teller transition strengths.
doi: 10.1103/PhysRevC.42.935
1989EL05 Phys.Lett. 231B, 365 (1989) C.Ellegaard, C.Gaarde, T.S.Jorgensen, J.S.Larsen, B.Million, C.Goodman, A.Brockstedt, P.Ekstrom, M.Osterlund, M.Bedjidian, D.Contardo, D.Bachelier, J.L.Boyard, T.Hennino, J.C.Jourdain, M.Roy-Stephan, P.Radvanyi, P.Zupranski Spin Structure of the Δ Excitation NUCLEAR REACTIONS 1,2H, 12C(polarized d, 2p), E=1.6, 2 GeV; measured pp-coin spectra, tensor polarization response; deduced Δ excitation spin structure.
doi: 10.1016/0370-2693(89)90677-1
1989IC02 Phys.Rev. C39, 1446 (1989) M.Ichimura, K.Kawahigashi, T.S.Jorgensen, C.Gaarde Excitation of Spin-Isospin Modes in the Quasifree Scattering Region NUCLEAR REACTIONS 40Ca(p, p'), E=500 MeV; calculated longitudinal, transverse response functions, σ(θ(p)', E(p)'). DWIA, continuum RPA.
doi: 10.1103/PhysRevC.39.1446
1988WA07 Nucl.Phys. A480, 285 (1988) D.Wang, J.Rapaport, D.J.Horen, B.A.Brown, C.Gaarde, C.D.Goodman, E.Sugarbaker, T.N.Taddeucci The 52, 54Cr(p, n)52, 54Mn and 57, 58Fe(p, n)57, 58Co Reactions at E(p) = 120 MeV NUCLEAR REACTIONS, MECPD 52,54Cr, 57,58Fe(p, n), E=120 MeV; measured σ(θ). 52,54Mn, 57,58Co deduced Gamow-Teller resonances, transition strengths. Enriched targets. DWIA analysis.
doi: 10.1016/0375-9474(88)90398-3
1987BE25 Nucl.Phys. A469, 648 (1987) I.Bergqvist, A.Brockstedt, L.Carlen, L.P.Ekstrom, B.Jakobsson, C.Ellegaard, C.Gaarde, J.S.Larsen, C.Goodman, M.Bedjidian, D.Contardo, J.Y.Grossiord, A.Guichard, R.Haroutunian, J.R.Pizzi, D.Bachelier, J.l.Boyard, T.Hennino, J.C.Jourdain, M.Roy-Stephan, M.Boivin, P.Radvanyi The (3He, t) Reaction at Intermediate Energies: Spin-isospin transitions to states in 12N and 13N NUCLEAR REACTIONS 12,13C(3He, t), E=0.6-2.3 GeV; measured σ(Et, θt), σ(θ); deduced isovector strength ratio. 12,13N deduced spin-isospin transitions. Magnetic spectrometer. DWIA calculations.
doi: 10.1016/0375-9474(87)90019-4
1987EL08 Phys.Rev.Lett. 59, 974 (1987) C.Ellegaard, C.Gaarde, T.S.Jorgensen, J.S.Larsen, C.Goodman, I.Bergqvist, A.Brockstedt, P.Ekstrom, M.Bedjidian, D.Contardo, J.Y.Grossiord, A.Guichard, D.Bachelier, J.L.Boyard, T.Hennino, J.C.Jourdain, M.Roy-Stephan, P.Radvanyi, J.Tinsley Reaction (d(pol), 2He) at Intermediate Energies NUCLEAR REACTIONS 1H(d, 2p), E=0.65, 2 GeV; measured σ vs two-proton relative momentum. 1H(polarized d, 2p), E=2 GeV; measured σ(Ep, θp), tensor analyzing power. Drift chambers, tensor polarized beam.
doi: 10.1103/PhysRevLett.59.974
1987KR10 Phys.Lett. 189B, 299 (1987) D.Krofcheck, E.Sugarbaker, A.J.Wagner, J.Rapaport, D.Wang, J.N.Bahcall, R.C.Byrd, C.C.Foster, C.D.Goodman, C.Gaarde, D.J.Horen, T.Carey, T.N.Taddeucci Gamow-Teller Strength Distribution in 81Kr and the Consequences for a 81Br Solar Neutrino Detector NUCLEAR REACTIONS 81Br(p, n), E=190, 200 MeV; measured σ(En). 81Kr transitions deduced Gamow-Teller transition strength distribution. Tof.
doi: 10.1016/0370-2693(87)91436-5
1987RA15 Phys.Rev. C36, 500 (1987) J.Rapaport, D.Wang, J.A.Carr, F.Petrovich, C.C.Foster, C.D.Goodman, C.Gaarde, J.Larsen, C.A.Goulding, T.N.Taddeucci, D.Horen, E.Sugarbaker (p(pol), n) Reaction on Carbon Isotopes at E(p) = 160 MeV NUCLEAR REACTIONS 12,13,14C(polarized p, n), E=160 MeV; measured σ(θ), σ(θ, En), analyzing power. 15N(polarized p, n), E=160 MeV; analyzed data. 12,13,14N, 15O levels deduced Gamow-Teller transition strength.
doi: 10.1103/PhysRevC.36.500
1987TA13 Nucl.Phys. A469, 125 (1987) T.N.Taddeucci, C.A.Goulding, T.A.Carey, R.C.Byrd, C.D.Goodman, C.Gaarde, J.Larsen, D.Horen, J.Rapaport, E.Sugarbaker The (p, n) Reaction as a Probe of Beta Decay Strength NUCLEAR REACTIONS 12,14C, 42Ca, 28Si, 90Zr, 208Pb, 7Li, 54Fe(p, n), E=50-200 MeV; measured σ(Ep, θ=0°). 12,14N, 42Sc, 28P, 90Nb, 208Bi, 7Be, 54Co deduced reaction population, B(GT) proportionality.
doi: 10.1016/0375-9474(87)90089-3
1986BA16 Phys.Lett. 172B, 23 (1986) D.Bachelier, J.L.Boyard, T.Hennino, J.C.Jourdain, M.Roy-Stephan, D.Contardo, J.Y.Grossiord, A.Guichard, J.R.Pizzi, P.Radvanyi, J.Tinsley, C.Ellegaard, C.Gaarde, J.S.Larsen First Observation of the Δ Resonance in Relativistic Heavy-Ion Charge-Exchange Reactions NUCLEAR REACTIONS 12C(14N, 14C), E=880 MeV/nucleon; 12C(12C, 12N), E=900 MeV/nucleon; 27Al(20Ne, 20Na), (20Ne, 20F), E=950 MeV/nucleon; measured particle spectra; deduced isobar excitation.
doi: 10.1016/0370-2693(86)90209-1
1986CO03 Phys.Lett. 168B, 331 (1986) D.Contardo, M.Bedjidian, J.Y.Grossiord, A.Guichard, R.Haroutunian, J.R.Pizzi, C.Ellegaard, C.Gaarde, J.S.Larsen, C.Goodman, I.Bergqvist, A.Brockstedt, L.Carlen, P.Ekstrom, D.Bachelier, J.L.Boyard, T.Hennino, J.C.Jourdain, M.Roy-Stephan, M.Boivin, P.Radvanyi Study of the Δ Isobar Excitation in Nuclei with the (3He, t) Reaction NUCLEAR REACTIONS 12C, 48Ca, 54Fe, 89Y, 159Tb, 208Pb(3He, t), E=2 GeV; measured σ(θ) vs triton momentum; deduced isobar excitation.
doi: 10.1016/0370-2693(86)91639-4
1986TA05 Phys.Rev. C33, 746 (1986) T.N.Taddeucci, C.D.Goodman, R.C.Byrd, I.J.Van Heerden, T.A.Carey, D.J.Horen, J.S.Larsen, C.Gaarde, J.Rapaport, T.P.Welch, E.Sugarbaker Spin-Flip Decomposition of the Spectrum for 90Zr(p, n) at E(p) = 160 MeV NUCLEAR REACTIONS 90Zr(polarized p, n), E=160 MeV; measured σ(θ=0°), transverse polarization transfer. 90Nb deduced ΔL=0, ΔL=1 resonance excitations, transition strengths.
doi: 10.1103/PhysRevC.33.746
1985GO02 Phys.Rev.Lett. 54, 877 (1985); Erratum Phys.Rev.Lett. 54, 2060 (1985) C.D.Goodman, R.C.Byrd, I.J.Van Heerden, T.A.Carey, D.J.Horen, J.S.Larsen, C.Gaarde, J.Rapaport, T.P.Welch, E.Sugarbaker, T.N.Taddeucci Measurements of Gamow-Teller Strength Distributions in Masses 13 and 15 NUCLEAR REACTIONS 13C, 15N(polarized p, n), E=160 MeV; measured σ(θ), spin-flip probabilities. 13N, 15O deduced quenched Gamow-Teller transition strengths. Shell model comparison.
doi: 10.1103/PhysRevLett.54.877
1985KR10 Phys.Rev.Lett. 55, 1051 (1985) D.Krofcheck, E.Sugarbaker, J.Rapaport, D.Wang, J.N.Bahcall, R.C.Byrd, C.C.Foster, C.D.Goodman, I.J.Van Heerden, C.Gaarde, J.S.Larsen, D.J.Horen, T.N.Taddeucci Gamow-Teller Strength Function in 71Ge via the (p, n) Reaction at Medium Energies NUCLEAR REACTIONS 71Ga(p, n), E=120, 200 MeV; measured σ(En), σ(θ, En); deduced neutrino capture σ corrections in 71Ga detector. 71Ge deduced Gamow-Teller strength function, transition strength fragmentation.
doi: 10.1103/PhysRevLett.55.1051
1985RA11 Phys.Rev.Lett. 54, 2325 (1985) J.Rapaport, P.Welch, J.Bahcall, E.Sugarbaker, T.N.Taddeucci, C.D.Goodman, C.F.Foster, D.Horen, C.Gaarde, J.Larsen, T.Masterson Solar-Neutrino Detection: Experimental determination of Gamow-Teller strengths via the 98Mo and 115In(p, n) reactions NUCLEAR REACTIONS 98Mo, 115In(p, n), E=120, 200 MeV; measured σ(En, θ=0°); deduced target solar neutrino absorption σ. 98Tc, 115Sn deduced Gamow-Teller strengths.
doi: 10.1103/PhysRevLett.54.2325
1984GA11 Nucl.Phys. A422, 189 (1984) C.Gaarde, J.S.Larsen, H.Sagawa, N.Ohtsuka, J.Rapaport, T.N.Taddeucci, C.D.Goodman, C.C.Foster, C.A.Goulding, D.Horen, T.Masterson, E.Sugarbaker Spin-Dipole Strength in 12N NUCLEAR REACTIONS 12C(p, n), E=120, 160, 200 MeV; measured σ(θ). 12N deduced levels, J, π, analogs.
doi: 10.1016/0375-9474(84)90513-X
1984GA17 J.Phys.(Paris), Colloq.C4, 405 (1984); See 1984Ga36 Charge-Exchange Reactions and Spin-Isospin Modes
1984GA36 J.Phys.(Paris), Colloq.C-4, 405 (1984) Charge-Exchange Reactions and Spin-Isospin Modes NUCLEAR REACTIONS 12,14C, 208Pb(p, n), E=60-200 MeV; analyzed σ(En, θn). 12C, 90Zr(3He, t), E=200, 600 MeV; 12C, 40Ca, 54Fe, 90Zr, 208Pb(3He, t), E=1.5 GeV; 1H, C(3He, t), E=2 GeV; analyzed σ(Et, θt); deduced isobar resonance role.
1984LI02 Nucl.Phys. A412, 92 (1984) J.R.Lien, G.Lovhoiden, J.Rekstad, A.Henriques, C.Gaarde, J.S.Larsen, S.Y.Van Der Werf High-Spin Particle States in 153Sm Studied with the (α, 3He) Reaction NUCLEAR REACTIONS 152Sm(α, 3He), E=40 MeV; measured σ(E(3He), θ). 153Sm deduced levels, L, π, J. Enriched target.
doi: 10.1016/0375-9474(84)90386-5
1984RA15 Nucl.Phys. A427, 332 (1984) J.Rapaport, R.Alarcon, B.A.Brown, C.Gaarde, J.Larsen, C.D.Goodman, C.C.Foster, D.Horen, T.Masterson, E.Sugarbaker, T.N.Taddeucci The 51V(p, n)51Cr Reaction at E(p) = 160 MeV NUCLEAR STRUCTURE 40,42,44,46,48Ca, 50Ti, 51V, 52Cr, 54Fe; calculated B(M1). 22O, 23F, 24Ne, 25Na, 26Mg, 27Al, 28Si; calculated Gamow-Teller transition strength. Shell model. NUCLEAR REACTIONS 51V(p, n), E=159.4 MeV; measured σ(θ), σ(En). 51Cr deduced levels, analogs, Gamow-Teller transition strengths. 50Ti, 51V(p, p'), (e, e'), (p, n), E not given; calculated Gamow-Teller transition strengths. Shell model.
doi: 10.1016/0375-9474(84)90089-7
1984RA22 Nucl.Phys. A431, 301 (1984) J.Rapaport, C.Gaarde, J.Larsen, C.Goulding, C.D.Goodman, C.Foster, D.J.Horen, T.Masterson, E.Sugarbaker, T.N.Taddeucci The 19F(p, n)19Ne and 39K(p, n)39Ca Reactions at Intermediate Energies and Quenching of the Gamow-Teller Strength NUCLEAR REACTIONS 19F, 39K(p, n), E=120, 160 MeV; measured σ(En), σ(θ). 19Ne, 39Ca levels deduced Gamow-Teller transition strength distribution. DWBA analysis.
doi: 10.1016/0375-9474(84)90177-5
1984TA07 Phys.Rev.Lett. 52, 1960 (1984) T.N.Taddeucci, T.A.Carey, C.Gaarde, J.Larsen, C.D.Goodman, D.J.Horen, T.Masterson, J.Rapaport, T.P.Welch, E.Sugarbaker Measurement of the Tranverse Spin-Transfer Coefficient D(NN)(0°) for (p(pol), n(pol)) Reactions at 160 MeV NUCLEAR REACTIONS 6,7Li, 12,13,14C, 90Zr(polarized p, n), E=160 MeV; measured transverse spin transfer coefficient D(NN)(θ=0°), polarized neutrons. 6,7Be, 12,13,14N, 90Nb deduced L=0 Gamow-Teller transition expected average value.
doi: 10.1103/PhysRevLett.52.1960
1983EL05 Phys.Rev.Lett. 50, 1745 (1983) C.Ellegaard, C.Gaarde, J.S.Larson, C.Goodman, I.Bergqvist, L.Carlen, P.Ekstrom, B.Jakobsson, J.Lyttkens, M.Bedjidian, M.Chamcham, J.Y.Grossiord, A.Guichard, M.Gusakow, R.Haroutunian, J.R.Pizzi, D.Bachelier, J.L.Boyard, T.Hennino, J.C.Jourdain, M.Roy-Stephan, M.Boivin, P.Radvanyi (3He, t) Reaction at Intermediate Energies NUCLEAR REACTIONS C, 54Fe, 89Y(3He, t), E=0.6, 1.2, 2 GeV; measured σ(θ), σ(θ, Et); deduced spin-isospin excitation dominance, isobar resonance effects. DWIA, nucleon-nucleon data input.
doi: 10.1103/PhysRevLett.50.1745
1983GA15 Phys.Scr. T5, 55 (1983) Gamow-Teller Resonances NUCLEAR REACTIONS 89Y(3He, t), E=0.6, 1.2, 2 GeV; 12C(3He, t), E=2 GeV; measured σ(Et, θ=0°). 54Fe(3He, t), E=0.6 GeV; measured σ(Et, θ), θ=0-8°; deduced Gamow-Teller strength distribution systematics, isobar excitation role. 12N, 54Cr, 90Zr deduced selective spin-isospin mode excitation. Intermediate energy (p, n) data input.
doi: 10.1088/0031-8949/1983/T5/009
1983JA03 Nucl.Phys. A394, 39 (1983) J.Janecke, E.H.L.Aarts, A.G.Drentje, M.N.Harakeh, C.Gaarde Isobaric Analog States in Rare-Earth Nuclei Studied with the (3He, t) Charge Exchange Reaction at θ(L) = 0° NUCLEAR REACTIONS 152,154,156,158,160Gd, 160,162Dy, 162,164,166,168,170Er, 170,172,174,176Yb, 176,178,180Hf(3He, t), E=60.5 MeV; measured σ(E(t), θ=0°). 152,154,156,158,160Tb, 160,162Ho, 162,164,166,168,170Tm, 170,172,174,176Lu, 176,178,180Ta deduced IAS, Γ, Coulomb displacement energies. Enriched targets, magnetic spectrometer.
doi: 10.1016/0375-9474(83)90160-4
1983RA30 Nucl.Phys. A410, 371 (1983) J.Rapaport, T.Taddeucci, T.P.Welch, C.Gaarde, J.Larsen, D.J.Horen, E.Sugarbaker, P.Koncz, C.C.Foster, C.D.Goodman, C.A.Goulding, T.Masterson Excitation of Giant Spin-Isospin Multipole Vibrations in 54,56Fe and 58,60Ni NUCLEAR REACTIONS 58Ni(p, n), E=120 MeV; 54,56Fe, 58,60Ni(p, n), E=160 MeV; measured σ(θ, En), θ < 6°, σ(θ). 58Cu, 54,56Co deduced L=0 transition strengths, Gamow-Teller state strengths. Shell model.
doi: 10.1016/0375-9474(83)90632-2
1983TA16 Phys.Rev. C28, 2511 (1983) T.N.Taddeucci, J.Rapaport, C.C.Foster, C.D.Goodman, C.Gaarde, J.Larsen, C.A.Goulding, D.J.Horen, T.Masterson, E.Sugarbaker Spin Excitations in 40C(p, n) NUCLEAR REACTIONS 40Ca(p, n), E=59.3, 118.3, 159.3 MeV; measured σ(θ), σ(En). 40Sc level deduced Gamow-Teller transition strength. 42Ca(p, n), E=159.3 MeV; measured σ(θ). DWIA analyses.
doi: 10.1103/PhysRevC.28.2511
1982RA30 Phys.Lett. 119B, 61 (1982) J.Rapaport, T.Taddeucci, T.P.Welch, D.J.Horen, J.B.McGrory, C.Gaarde, J.Larsen, E.Sugarbaker, P.Koncz, C.C.Foster, C.D.Goodman, C.A.Goulding, T.Masterson Excitation of Gamow-Teller Resonances in A = 58 Nuclei NUCLEAR REACTIONS 58Ni(p, n), E=120, 160 MeV; measured σ(En, θ=0°). 58Cu deduced levels, isovector Gamow-Teller transition strength.
doi: 10.1016/0370-2693(82)90243-X
1982SU05 Phys.Lett. 116B, 91 (1982) On the Quenching of Spin-Dipole Transition Strength due to Isobar-Hole Mixing NUCLEAR STRUCTURE A=16, 208; calculated spin dipole excitation, quenching. Isobar, baryon resonance effects.
doi: 10.1016/0370-2693(82)90982-0
1982TA03 Phys.Rev. C25, 1094 (1982) T.N.Taddeucci, J.Rapaport, D.E.Bainum, C.D.Goodman, C.C.Foster, C.Gaarde, J.Larsen, C.A.Goulding, D.J.Horen, T.Masterson, E.Sugarbaker Energy Dependence of the Ratio of Isovector Effective Interaction Strengths [J(στ)/J(τ)] from 0° (p, n) Cross Sections NUCLEAR REACTIONS 7Li, 13,14C, 26Mg, 37Cl, 42Ca(p, n), E=60-200 MeV; measured σ(θ=0°); deduced isovector effective interaction strength ratio. 7Be, 13,14N, 26Al, 37Ar, 42Sc levels deduced Gamow-Teller transition strengths.
doi: 10.1103/PhysRevC.25.1094
1981GA08 Phys.Rev.Lett. 46, 902 (1981) C.Gaarde, J.S.Larsen, A.G.Drentje, M.N.Harakeh, S.Y.van der Werf Decay of the Giant Gamow-Teller Resonance in 208Bi NUCLEAR REACTIONS 208Pb(3He, t), E=81 MeV; measured σ(Et), σ(θp, θt, Ep). 208Bi deduced IAS, Gamow-Teller resonance decay.
doi: 10.1103/PhysRevLett.46.902
1981GA26 Nucl.Phys. A369, 258 (1981) C.Gaarde, J.Rapaport, T.N.Taddeucci, C.D.Goodman, C.C.Foster, D.E.Bainum, C.A.Goulding, M.B.Greenfield, D.J.Horen, E.Sugarbaker Excitation of Giant Spin-Isospin Multipole Vibrations NUCLEAR REACTIONS 40Ca, 90Zr, 112,124Sn, 208Pb, 169Tm(p, n), E=200 MeV; measured σ(En, θ). 40Sc, 90Nb, 112,124Sb, 169Yb, 208Bi deduced resonances, L, Gamow-Teller resonance characteristics, giant spin-isospin multipole vibrations. Enriched targets, time-compensated large volume detectors.
doi: 10.1016/0375-9474(81)90019-1
1981GO18 Phys.Lett. 107B, 406 (1981) C.D.Goodman, C.C.Foster, D.E.Bainum, S.D.Bloom, C.Gaarde, J.Larsen, C.A.Goulding, D.J.Horen, T.Masterson, S.Grimes, J.Rapaport, T.N.Taddeucci, E.Sugarbaker Missing Gamow-Teller Strength in Mass 42 NUCLEAR REACTIONS 42Ca(p, n), E=160 MeV; measured σ(θ, En). 42Sc deduced Gamow-Teller transition strength distribution. Shell model.
doi: 10.1016/0370-2693(81)91217-X
1981HO03 Phys.Lett. 99B, 383 (1981) D.J.Horen, C.D.Goodman, D.E.Bainum, C.C.Foster, C.Gaarde, C.A.Goulding, M.B.Greenfield, J.Rapaport, T.N.Taddeucci, E.Sugarbaker, T.Masterson, S.M.Austin, A.Galonsky, W.Sterrenburg Energy Systematics of the Giant Gamow-Teller Resonance and a Charge-Exchange Dipole Spin-Flip Resonance NUCLEAR REACTIONS 90,92,94Zr, 112,116,124Sn, 169Tm, 208Pb(p, n), E=120, 160, 200 MeV; measured σ(En, θ). 90,92,94Nb, 112,116,124Sb, 169Yb, 208Bi deduced giant Gamow-Teller, charge exchange dipole spin-flip resonance energy systematics. Tof.
doi: 10.1016/0370-2693(81)90553-0
1981LO14 Nucl.Phys. A369, 461 (1981) G.Lovhoiden, J.R.Lien, J.C.Waddington, J.Rekstad, I.Espe, C.Gaarde, J.S.Larsen, S.van der Werf High-Spin Particle States in 151Sm Studied with the (α, 3He) Reaction NUCLEAR REACTIONS 150Sm(α, 3He), E=40 MeV; measured σ(E(3He), θ). 151Sm deduced levels, J, π, S. QMG/2 spectrometer. DWBA analysis, Coriolis coupling calculation.
doi: 10.1016/0375-9474(81)90031-2
1981RA12 Phys.Rev. C24, 335 (1981) J.Rapaport, T.Taddeucci, C.Gaarde, C.D.Goodman, C.C.Foster, C.A.Goulding, D.Horen, E.Sugarbaker, T.G.Masterson, D.Lind 12C(p, n)12N Reaction at 120, 160, and 200 MeV NUCLEAR REACTIONS 12C(p, n), E=120, 160, 200 MeV; measured σ(En, θ); deduced energy independence of effective interaction spin-isospin term. Tof. Microscopic DWIA calculations.
doi: 10.1103/PhysRevC.24.335
1981RA19 Phys.Rev.Lett. 47, 1518 (1981) J.Rapaport, T.Taddeucci, P.Welch, C.Gaarde, J.Larsen, C.Goodman, C.C.Foster, C.A.Goulding, D.Horen, E.Sugarbaker, T.Masterson Empirical Evaluation of Gamow-Teller Strength Function for 37Cl → 37Ar and Its Implication in the Cross Section for Solar Neutrino Absorption by 37Cl NUCLEAR REACTIONS 37Cl(p, n), E=120 MeV; measured σ(En), σ(θ). 37Ar level deduced Gamow-Teller transition strengths, log ft. Tof.
doi: 10.1103/PhysRevLett.47.1518
1981RE10 Nucl.Phys. A369, 453 (1981) J.Rekstad, I.Espe, G.Lovhoiden, J.R.Lien, J.C.Waddington, C.Gaarde, J.S.Larsen, S.van der Werf An Investigation of the 144Sm(α, 3He)145Sm Reaction NUCLEAR REACTIONS 144Sm(α, 3He), E=40 MeV; measured σ(E(3He), θ). 145Sm deduced levels, L, π, S. Enriched target.
doi: 10.1016/0375-9474(81)90030-0
1980GA04 Nucl.Phys. A334, 248 (1980) C.Gaarde, J.S.Larsen, M.N.Harakeh, S.Y.van der Werf, M.Igarashi, A.Muller-Arnke The 48Ca(3He, t)48Sc Reaction at 66 and 70 Mev. Reaction Mechanism and Gamow-Teller Strength NUCLEAR REACTIONS 48Ca(3He, t), E=66, 70 MeV; measured σ(Et, θ); deduced reaction mechanism. 48Sc deduced Gamow-Teller strength distribution. Finite range two-step DWBA analysis, shell model.
doi: 10.1016/0375-9474(80)90067-6
1980GA20 Nucl.Phys. A346, 497 (1980) C.Gaarde, J.S.Larsen, A.G.Drentje, M.N.Harakeh, S.Y. Van Der Werf, A.Muller-Arnke The 54Fe(3He, t)54Co Reaction at 70 MeV, Gamow-Teller Strength. NUCLEAR REACTIONS 54Fe(3He, t), E=70 MeV; measured σ(Et, θ). 54Co deduced levels, J.π, Gamow-Teller strength distribution. Shell model, second-order, finite-range DWBA calculations.
doi: 10.1016/0375-9474(80)90482-0
1979TA03 Nucl.Phys. A316, 189 (1979) Tai Kuang-Hsi, T.Dossing, C.Gaarde, J.S.Larsen Angular Correlations in Compound Nucleus Decay Following the Reactions 16O + 27Al, 40Ca and 58Ni NUCLEAR REACTIONS 27Al(16O, 2α), (16O, αp), (16O, 2p), E=50, 60 MeV; 40Ca, 58Ni(16O, 2α), (16O, αp), (16O, 2p), E=70 MeV; measured αα(θ), αp(θ), pp(θ). Model calculation of αα(θ). Enriched 58Ni target.
doi: 10.1016/0375-9474(79)90679-1
1978FE04 Nucl.Phys. A306, 259 (1978) B.Fernandez, C.Gaarde, J.S.Larsen, S.Pontoppidan, F.Videbaek Fusion Cross Sections for the 16O + 16O Reaction NUCLEAR REACTIONS 16O, 12C(16O, X), E=35-80 MeV; measured σ(E, θ); deduced fusion σ(E).
doi: 10.1016/0375-9474(78)90327-5
1977BA36 Nucl.Phys. A285, 317 (1977) B.B.Back, R.R.Betts, C.Gaarde, J.S.Larsen, E.Michelsen, Tai Kuang-Hsi Fusion Cross Sections for the 16O + 27Al Reaction NUCLEAR REACTIONS 27Al(16O, X), E=50-80 MeV; measured σ(E, θ), fusion σ; deduced fusion barrier height, radius, critical radius.
doi: 10.1016/0375-9474(77)90255-X
1976BA05 Phys.Rev. C13, 875 (1976) B.B.Back, R.R.Betts, C.Gaarde, H.Oeschler High Spin States in 23Na and the E(c.m.) = 19.3 MeV 12C + 12C Resonance NUCLEAR REACTIONS 12C(12C, pγ), E=38.6 MeV; measured DSA, pγ(θ). 23Na deduced levels, T1/2, J, π, B(E2).
doi: 10.1103/PhysRevC.13.875
1975BE45 Nucl.Phys. A253, 380 (1975) R.R.Betts, C.Gaarde, O.Hansen, J.S.Larsen, S.Y.Van der Werf Deuteron Induced Pickup Reactions on 41Ca NUCLEAR REACTIONS 41Ca(d, t), (d, 3He), E=40 MeV; measured σ(Et, θ), σ(E(3He), θ). 40Ca, 40K deduced levels, L, J, π, S, T. Enriched radioactive target.
doi: 10.1016/0375-9474(75)90488-1
1975FO12 Nucl.Phys. A252, 343 (1975) Total (p, n) Cross Sections to Ground-State Analogue States of 48Ca, 50Ti, 52Cr and 58Ni NUCLEAR REACTIONS 48Ca(p, nγ), E=7.7-14.2 MeV; 50Ti(p, nγ), E=8.0-12.0 MeV; 52Cr(p, nγ), E=8.7-11.9 MeV; 58Ni(p, nγ), E=9.8-11.9 MeV; measured σ(E, En) to IAS of ground states. 48Ca(p, p), (p, p'), E=8.0-10.2 MeV; measured σ(E, Ep', θ). 49Sc deduced levels, resonances, J, π, Γ, p-width. Enriched targets.
doi: 10.1016/0375-9474(75)90504-7
1974GA11 Nucl.Phys. A221, 238 (1974) Study of the (6Li, 6He) Reaction on the Targets 19F, 27Al and 58,60,64Ni NUCLEAR REACTIONS 19F, 27Al(6Li, 6He), E=34 MeV; 58,60,64Ni(6Li, 6He), E=36 MeV; measured σ(θ). 64Cu deduced levels, L, J, π. 40Ca(6Li, 6He), 88Sr(6Li, 6He), E=38 MeV upper limits for σ(θ). Enriched targets.
doi: 10.1016/0375-9474(74)90316-9
1974GA17 Nucl.Phys. A222, 579 (1974) C.Gaarde, T.Kammuri, F.Osterfeld The (6Li, 6He) Spin-Isospin-Flip Reaction NUCLEAR REACTIONS 48Ca(6Li, 6He), E=34 MeV; measured nothing, calculated σ(E(6He), θ). 48Sc levels deduced wavefunctions.
doi: 10.1016/0375-9474(74)90340-6
1973GA21 Nucl.Phys. A215, 314 (1973) Study of the 48Ca(6Li, 6He)48Sc Reaction at 34 MeV NUCLEAR REACTIONS 48Ca(6Li, 6He), E=34 MeV; measured σ(E(6He), θ). 48Sc deduced levels, L, J, π. Enriched target.
doi: 10.1016/0375-9474(73)90658-1
1972GA09 Nucl.Phys. A184, 241 (1972) C.Gaarde, K.Kemp, C.Petresch, F.Folkmann Gamma-Ray Decay from the Analogue State of the 49Ca g.s. NUCLEAR REACTIONS 48Ca(p, γ), (p, p), (p, nγ);E=1.94-2.01 MeV; measured σ(E)σ, (E;Eγ, θ(γ)). 49Sc analog resonances deduced J, π, n-width, p-width, γ-width, γ-mixing, B(E1), B(M1), B(E2). Enriched targets, Ge(Li) detector.
doi: 10.1016/0375-9474(72)90455-1
1971GA40 Izv.Akad.Nauk SSSR, Ser.Fiz. 35, 687 (1971); Bull.Acad.Sci.USSR, Phys.Ser. 35, 629 (1972) Gamma Decay of the p3/2-Analog States in 43Sc NUCLEAR REACTIONS 42Ca(p, γ), E=1424 keV; measured Eγ, Iγ, Iγ(θ). 43Sc deduced levels, J, π, level-width, γ-mixing, analog state.
1970GA05 Nucl.Phys. A143, 497 (1970) C.Gaarde, K.Kemp, Y.V.Naumov, P.R.Amundsen Gamma Decay from the Analogue State of the 51Ti g.s. NUCLEAR REACTIONS 50Ti(p, p), (p, γ), E=1.36-1.38 MeV; measured σ(E), σ(E;Eγ, θ). 51V analog resonances deduced J, π, p-, γ-width, γ-mixing, B(M1), B(E2). Enriched targets, Ge(Li) detectors.
doi: 10.1016/0375-9474(70)90544-0
1968GA11 Nucl.Phys. A118, 641(1968) Fine Structure of Analogue Resonances in the 44Ca(p, p) and 50Ti(p, p) Reactions NUCLEAR REACTIONS 44Ca(p, p), E=1.62-1.69 MeV. 50Ti(p, p), E=2.45-2.65 MeV; measured σ(E). 45Sc, 51V resonances deduced J, π, p-width; analog state deduced α-width. Enriched targets.
doi: 10.1016/0375-9474(68)90446-6
1967GA05 Nucl.Phys. A102, 1 (1967) Isobaric Analogue States of 47Ca NUCLEAR REACTIONS 46Ca(p, p), E=1.8-4.2 MeV; 46Ca(p, p'), E=2.7-4.2 MeV; measured σ(E). 47Sc deduced isobaric analog states. 47Sc resonances deduced J, π, L, level-width, level-width p, level-width p'. Enriched target.
doi: 10.1016/0375-9474(67)90321-1
1966GA14 Phys.Lett. 22, 466 (1966) C.Gaarde, P.Wilhjelm, P.B.Jorgensen Spectroscopic Factors of Isobaric Analogue States from Proton Excitation of Some Medium Weight Even Nuclei NUCLEAR REACTIONS 44Ca, 62,64Ni, 64,66,68Zn, 74Ge(p, p), (p, p'), E =2.1-4.1 MeV; measured σ(E). 45Sc, 63,65Cu, 65,67,69Ga, 75As deduced isobaric analog resonances, level-width, S, Coulomb displacement energies.
doi: 10.1016/0031-9163(66)91229-7
1965FU05 Nucl.Phys. 66, 638 (1965) The Probability for Transitions Between the First 2+ and the First 0+ Excited States of O16 NUCLEAR REACTIONS 19F(p, αγ), E = 0.874 MeV; measured γ(E+E-)-coin. 16O deduced B(E2), deformation parameter.
doi: 10.1016/0029-5582(65)90791-1
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