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NSR database version of April 25, 2024.

Search: Author = J.Larsen

Found 65 matches.

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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
Citations: PlumX Metrics


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, 12-), E=1.1 GeV/nucleon; measured σ(E, θ).

doi: 10.1016/j.nuclphysa.2005.03.064
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0518.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0113.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1803.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0186.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2626.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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1975BA22      Nucl.Phys. A244, 341 (1975)

J.B.Ball, O.Hansen, J.S.Larsen, D.Sinclair, F.Videbaek

16O Induced One-Nucleon Transfer Reactions on Targets of 26Mg, 27Al, 30Si and 48Ca

NUCLEAR REACTIONS 26Mg, 27Al, 30Si, 48Ca(16O, 16O), E=60 MeV; 24Mg, 27Al, 30Si(16O, 16O), E=45 MeV; measured σ(θ). 48Ca(16O, 15N), E=56 MeV; 30Si(16O, 15N), E=50 MeV; 26Mg, 27Al, 30Si(16O, 15N), E=45, 60 MeV; measured σ(E(15N), θ). 48Ca(16O, 17O), E=60 MeV; measured σ(E(17O), θ). 27Al(16O, 17F), E=60 MeV; measured σ(E(17F), θ). 26Mg, 27Al, 28Si, 31P, 47Ca, 49Sc levels deduced L. DWBA analysis.

doi: 10.1016/0375-9474(75)90064-0
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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
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1975ME23      Phys.Rev. C12, 2010 (1975)

R.A.Meyer, R.G.Lanier, J.T.Larsen

Two-Particle, One-Hole States in Antimony Nuclei and the Decay of 121Te-m, g

RADIOACTIVITY 121m,121Te; measured Eγ, Iγ; deduced Q, log ft. 121Sb deduced levels. 119Te; measured Eγ, Iγ. 119Sb deduced levels.

doi: 10.1103/PhysRevC.12.2010
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1975WI07      Nucl.Phys. A244, 147 (1975)

J.Wilczynski, K.Siwek-Wilczynska, J.S.Larsen, J.C.Acquadro, P.R.Christensen

Optimum Q-Values for the 58Ni(16O, 12C) Reaction Well Above the Coulomb Barrier

NUCLEAR REACTIONS 58Ni(16O, 12C), E=60, 72, 81 MeV; measured σ(θ, E); deduced tangential friction parameter, energy dependence of optimum Q. Surface-barrier detector telescopes. Enriched target.

doi: 10.1016/0375-9474(75)90014-7
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1974BA31      Phys.Lett. 49B, 348 (1974)

J.B.Ball, O.Hansen, J.S.Larsen, D.Sinclair, F.Videbaek

The (16O, 15N) Reaction at Forward Angles

NUCLEAR REACTIONS 26Mg, 30Si(16O, 15N), E=45 MeV; 48Ca(16O, 15N), E=56 MeV; measured σ(E(15N), θ).

doi: 10.1016/0370-2693(74)90178-6
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1974KE01      Nucl.Phys. A221, 333 (1974)

J.Kern, G.Mauron, B.Michaud, K.Schreckenbach, T.Von Egidy, W.Mampe, H.R.Koch, H.A.Baader, D.Breitig, U.Gruber, B.P.K.Maier, O.W.B.Schult, J.T.Larsen, R.G.Lanier, J.J.Tambergs, M.K.Balodis

Nuclear Levels in 160Tb

NUCLEAR REACTIONS 159Tb(n, γ), E=thermal; measured Eγ, Iγ, E(ce), I(ce), γγ-coin; deduced Q. 160Tb deduced levels, J, π, K.

doi: 10.1016/0375-9474(74)90323-6
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1973BA26      Nucl.Phys. A207, 425 (1973)

J.B.Ball, C.B.Fulmer, J.S.Larsen, G.Sletten

Energy Levels of 94Ru Observed with the 96Ru(p, t) Reaction

NUCLEAR REACTIONS 96Ru(p, t), E=31.1 MeV; measured σ(Et, θ). 94Ru deduced levels, L(2n), J, π. Enriched target.

doi: 10.1016/0375-9474(73)90356-4
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1973BA56      Phys.Rev. C8, 1438 (1973)

J.B.Ball, J.J.Pinajian, J.S.Larsen, A.C.Rester

Study of 82Sr, 84Sr, and 86Sr with the (p, t) Reaction

NUCLEAR REACTIONS 84,86,87,88Sr(p, t), E=31 MeV; measured σ(Et, θ). Deduced Q. 82,84,86Sr deduced levels, J, π, L, enhancement factors.

doi: 10.1103/PhysRevC.8.1438
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1973CH23      Phys.Lett. 45B, 107 (1973)

P.R.Christensen, O.Hansen, J.S.Larsen, D.Sinclair, F.Videbaek

Abrupt Change between Smooth and Oscillatory Angular Distributions in 16O Induced Transfer Reactions on 26Mg

NUCLEAR REACTIONS 26Mg(16O, 15N), (16O, 14C), E=45, 60 MeV; measured σ(θ).

doi: 10.1016/0370-2693(73)90076-2
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1973LA04      Phys.Rev. C7, 751 (1973)

J.S.Larsen, J.B.Ball, C.B.Fulmer

Level Structure of 92Mo and 94Mo Studied with the (p, t) Reaction

NUCLEAR REACTIONS 94,96Mo(p, t), E=31 MeV; measured σ(Et, θ). 92,94Mo deduced levels, J, π, L.

doi: 10.1103/PhysRevC.7.751
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1972BA75      Phys.Rev.Lett. 29, 1014 (1972)

J.B.Ball, J.S.Larsen

Systematics of L = 0 Transitions Observed in the (p, t) Reaction of Nuclei Near N = 50

NUCLEAR REACTIONS 88Sr, 96Ru, 90,92Zr, 92,94Mo(p, t), E=31 MeV; measured σ(Et). 86Sr, 94Ru, 88,90Zr, 90,92Mo deduced L=0 strength systematics.

doi: 10.1103/PhysRevLett.29.1014
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1972BB08      Phys.Lett. 41B, 581 (1972)

J.B.Ball, J.B.McGrory, J.S.Larsen

Calculated Energy Levels for 89Y, 90Zr, 91Nb, 92Mo, 93Tc and 94Ru

NUCLEAR STRUCTURE 89Y, 90Zr, 91Nb, 92Mo, 93Tc, 94Ru; calculated levels, binding energies. Shell model, inert 88Sr core.

doi: 10.1016/0370-2693(72)90639-9
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1972LA38      Phys.Lett. 42B, 205 (1972)

J.S.Larsen, J.L.C.Ford, Jr., R.M.Gaedke, K.S.Toth, J.B.Ball, R.L.Hahn

Investigation of the 208Pb(12C, 11B)209Bi and 208Pb(12C, 13C)207Pb Reactions at High Bombarding Energies

NUCLEAR REACTIONS 208Pb(12C, 11B), (12C, 13C), E=77, 98, 116 MeV; measured σ(θ); analyzed reaction mechanisms.

doi: 10.1016/0370-2693(72)90061-5
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1971LA04      Phys.Rev. C3, 1372 (1971)

J.T.Larsen, W.L.Talbert, Jr., J.R.McConnell

Gamma-Ray Studies of the Decays of Xe142, Cs142, Ba142, and La142

RADIOACTIVITY 142mXe, 142mCs; measured Eγ, Iγ, γγ-coin. 142mBa, 142mLa; measured Eγ, Iγ, γγ-coin; deduced log ft. 142Cs, 142Ba, 142La, 142Ce deduced levels, J, π.

doi: 10.1103/PhysRevC.3.1372
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1970HU04      Phys.Rev. C1, 1845 (1970)

H.Hubel, R.A.Naumann, M.L.Andersen, J.S.Larsen, O.B.Nielsen, N.O.R.Poulsen

New High-Spin Isomer 179m2Hf and Intraband Branchings in the Ground-State Rotational Sequence of 179Hf

RADIOACTIVITY 179mHf[from 176Yb(α, n)]; measured Eγ, Iγ, T1/2, γγ-coin. 179Hf deduced high-spin isomer, levels, J, π, gR, gK, α(K), γ-multipolarity.

doi: 10.1103/PhysRevC.1.1845
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1969LA09      Nucl.Instr.Methods 69, 229 (1969)

J.T.Larsen, W.C.Schick, Jr., W.L.Talbert, Jr., D.I.Haddad

A Seven-Detector System for γ-γ Angular Correlations

RADIOACTIVITY 60Co, 152Eu; measured γγ(θ).

doi: 10.1016/0029-554X(69)90417-0
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1969LA23      Z.Physik 227, 65 (1969)

J.S.Larsen, B.C.Jorgensen

The Decay of 208Tl. Gamma-Ray Measurement

RADIOACTIVITY 208Tl; measured Eγ, Iγ, γγ-coin; deduced log ft. 208Pb deduced levels. Ge(Li) detector, separated 208Tl source.

doi: 10.1007/BF01396680
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1967LA13      Nucl.Phys. A100, 248 (1967)

J.S.Larsen, O.Skilbreid, L.Vistisen

High-Energy Spectra of 12-y 152Eu

RADIOACTIVITY 152Eu[from 151Eu(n, γ)]; measured Eβ, E(ce), Eγ, Iβ, I(ce), Iγ; deduced log ft. 152Sm deduced level, J, π. Enriched target.

doi: 10.1016/0375-9474(67)90407-1
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Note: The following list of authors and aliases matches the search parameter J.Larsen: , J.S.LARSEN, J.T.LARSEN