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NSR database version of April 11, 2024.

Search: Author = T.Taddeucci

Found 77 matches.

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2023KE09      Phys.Rev. C 108, 024603 (2023)

K.J.Kelly, M.Devlin, J.M.O'Donnell, D.Neudecker, A.E.Lovell, R.C.Haight, C.Y.Wu, R.Henderson, E.A.Bennett, T.Kawano, J.L.Ullmann, N.Fotiades, J.Henderson, S.M.Mosby, T.N.Taddeucci, P.Talou, M.C.White, J.A.Gomez, H.Y.Lee

Measurement of the 238U(n, f) prompt fission neutron spectrum from 10 keV to 10 MeV induced by neutrons with 1.5-20 MeV energy

NUCLEAR REACTIONS 238U(n, F), E=1.5-20 MeV; measured fission fragments, En, In, neutron time-of-flight, (fragment)n-coin; deduced prompt fission neutron spectrum (PFNS). Systematic trends in PFNS and PFNS ratios for 239Pu, 235U, and 238U obtained in series of Chi-Nu experiments. Comparison to other experimental results, CGMF calculations and data from JEFF-3.3, JENDL-5.0. ENDF/B-VIII libraries. Pulsed white neutron source at Weapons Neutron Research (WNR) facility of the Los Alamos Neutron Science Center (LANSCE). Li-glass array consisting of 22 detectors and liquid scintillator array consisting of 54 detector used for neutron detection, while PPAC used for detecting fission fragments in the frame of Chi-Nu experiment.

doi: 10.1103/PhysRevC.108.024603
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2022KE01      Phys.Rev. C 105, 044615 (2022)

K.J.Kelly, J.A.Gomez, M.Devlin, J.M.O'Donnell, D.Neudecker, A.E.Lovell, R.C.Haight, C.Y.Wu, R.Henderson, T.Kawano, E.A.Bennett, S.M.Mosby, J.L.Ullmann, N.Fotiades, J.Henderson, T.N.Taddeucci, H.Y.Lee, P.Talou, M.C.White

Measurement of the 235U(n, f) prompt fission neutron spectrum from 10 keV to 10 MeV induced by neutrons of energy from 1 MeV to 20 MeV

NUCLEAR REACTIONS 235U(n, F), E=0.01-10 MeV; measured In, En, neutron time-of-flight, fission fragments, neutrons angular distributions, (fragment)n-coin; deduced prompt fission neutron spectrum (PFNS), components corresponding to first-, second-, and third-chance fission as well as pre-equilibrium neutron emission preceding fission, mean PFNS energy, ratio to PFNMS obtained in 239Pu(n, F) reaction. Experiment performed as a part of Chi-Nu project aimed to measure the PFNS of major actinides with the Weapons Neutron Research (WNR) facility at the Los Alamos Neutron Science Center (LANSCE). The results are compared with other experimental data, CGMF calculations and selected nuclear data evaluations - ENDF/B-VIII.0, JEFF-3.3, JENDL-5.0.

doi: 10.1103/PhysRevC.105.044615
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2020KE05      Phys.Rev. C 102, 034615 (2020)

K.J.Kelly, M.Devlin, J.M.O'Donnell, J.A.Gomez, D.Neudecker, R.C.Haight, T.N.Taddeucci, S.M.Mosby, H.Y.Lee, C.Y.Wu, R.Henderson, P.Talou, T.Kawano, A.E.Lovell, M.C.White, J.L.Ullmann, N.Fotiades, J.Henderson, M.Q.Buckner

Measurement of the 239Pu(n, f) prompt fission neutron spectrum from 10 keV to 10 MeV induced by neutrons of energy 1-20 MeV

NUCLEAR REACTIONS 239Pu(n, F), E=1-20 MeV; measured outgoing prompt fission neutron spectrum (PFNS) in the range of E(n)=0.01-10 MeV, I(n) using Li-glass detector array and 54-detector EJ-309 liquid scintillator array in Chi-Nu experiment at the WNR-LANSCE-Los Alamos facility; deduced correlation matrix for PFNS from the Li-glass and the liquid scintillator. Comparison of present PFNS results with previous experimental results, and with evaluated data in ENDF/B-VIII.0 and JEFF-3.3 libraries.

doi: 10.1103/PhysRevC.102.034615
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14682.


2019KE04      Phys.Rev.Lett. 122, 072503 (2019)

K.J.Kelly, T.Kawano, J.M.O'Donnell, J.A.Gomez, M.Devlin, D.Neudecker, P.Talou, A.E.Lovell, M.C.White, R.C.Haight, T.N.Taddeucci, S.M.Mosby, H.Y.Lee, C.Y.Wu, R.Henderson, J.Henderson, M.Q.Buckner

Preequilibrium Asymmetries in the 239Pu(n, f) Prompt Fission Neutron Spectrum

NUCLEAR REACTIONS 239Pu(n, F), E=15-17.5 MeV; measured reaction products, En, In; deduced neutron excess of the preequilibrium prefission distribution above the postfission neutron spectrum. Comparison with theoretical calculations.

doi: 10.1103/PhysRevLett.122.072503
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2018DE08      Nucl.Data Sheets 148, 322 (2018)

M.Devlin, J.A.Gomez, K.J.Kelly, R.C.Haight, J.M.O'Donnell, T.N.Taddeucci, H.Y.Lee, S.M.Mosby, B.A.Perdue, N.Fotiades, J.L.Ullmann, C.Y.Wu, B.Bucher, M.Q.Buckner, R.A.Henderson, D.Neudecker, M.C.White, P.Talou, M.E.Rising, C.J.Solomon

The Prompt Fission Neutron Spectrum of 235U(n, f) below 2.5 MeV for Incident Neutrons from 0.7 to 20 MeV

NUCLEAR REACTIONS 235U(n, F), E=0.7-20 MeV; measured reaction products, En, In, TOF; deduced prompt fission neutron spectrum, σ(E).

doi: 10.1016/j.nds.2018.02.008
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2018NE02      Nucl.Data Sheets 148, 293 (2018)

D.Neudecker, P.Talou, T.Kawano, A.C.Kahler, M.C.White, T.N.Taddeucci, R.C.Haight, B.Kiedrowski, J.M.O'Donnell, J.A.Gomez, K.J.Kelly, M.Devlin, M.E.Rising

Evaluations of Energy Spectra of Neutrons Emitted Promptly in Neutron-induced Fission of 235U and 239Pu

NUCLEAR REACTIONS 235U, 239Pu(n, F)1NN, E<20 MeV; analyzed available data; deduced σ(E), total kinetic energies.

doi: 10.1016/j.nds.2018.02.006
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2016NE02      Nucl.Data Sheets 131, 289 (2016)

D.Neudecker, T.N.Taddeucci, R.C.Haight, H.Y.Lee, M.C.White, M.E.Rising

The Need for Precise and Well-documented Experimental Data on Prompt Fission Neutron Spectra from Neutron-induced Fission of 239Pu

NUCLEAR REACTIONS 239Pu(n, F), E<20 MeV; calculated prompt fission En, In. Comparison with available data.

doi: 10.1016/j.nds.2015.12.005
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2015HA01      Nucl.Data Sheets 123, 130 (2015)

R.C.Haight, C.Y.Wu, H.Y.Lee, T.N.Taddeucci, B.A.Perdue, J.M.O'Donnell, N.Fotiades, M.Devlin, J.L.Ullmann, T.A.Bredeweg, M.Jandel, R.O.Nelson, S.A.Wender, D.Neudecker, M.E.Rising, S.Mosby, S.Sjue, M.C.White, B.Bucher, R.Henderson

The LANL/LLNL Prompt Fission Neutron Spectrum Program at LANSCE and Approach to Uncertainties

NUCLEAR REACTIONS 239Pu(n, F), E<15 MeV; analyzed available data; deduced possible prompt fission neutron spectra σ, yields, correlation matrices.

doi: 10.1016/j.nds.2014.12.023
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2015JA07      Eur.Phys.J. A 51, 179 (2015)

M.Jandel, B.Baramsai, E.Bond, G.Rusev, C.Walker, T.A.Bredeweg, M.B.Chadwick, A.Couture, M.M.Fowler, A.Hayes, T.Kawano, S.Mosby, I.Stetcu, T.N.Taddeucci, P.Talou, J.L.Ullmann, D.J.Vieira, J.B.Wilhelmy

Capture and fission with DANCE and NEUANCE

doi: 10.1140/epja/i2015-15179-7
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2015NE02      Nucl.Data Sheets 123, 146 (2015)

D.Neudecker, P.Talou, T.N.Taddeucci, R.C.Haight, T.Kawano, H.Y.Lee, D.L.Smith, R.Capote, M.E.Rising, M.C.White

Preliminary Evaluation and Uncertainty Quantification of the Prompt Fission Neutron Spectrum of 239Pu

NUCLEAR REACTIONS 239Pu(n, X), E<20 MeV; calculated σ correlation matrices, prompt fission neutron spectrum and associated covariances. ENDF/B-VII.1 evaluated nuclear data library.

doi: 10.1016/j.nds.2014.12.026
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2015TA03      Nucl.Data Sheets 123, 135 (2015)

T.N.Taddeucci, R.C.Haight, H.Y.Lee, D.Neudecker, J.M.O'Donnell, M.C.White, B.A.Perdue, M.Devlin, N.Fotiadis, J.L.Ullmann, R.O.Nelson, T.A.Bredeweg, M.E.Rising, S.K.Sjue, S.A.Wender, C.Y.Wu, R.Henderson

Multiple-scattering Corrections to Measurements of the Prompt Fission Neutron Spectrum

NUCLEAR REACTIONS 239Pu(n, F), E<15 MeV; analyzed available data; deduced response functions, the shape of the prompt fission neutron spectrum.

doi: 10.1016/j.nds.2014.12.024
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2014HA27      Nucl.Data Sheets 119, 205 (2014)

R.C.Haight, H.Y.Lee, T.N.Taddeucci, J.M.O'Donnell, B.A.Perdue, N.Fotiades, M.Devlin, J.L.Ullmann, A.Laptev, T.Bredeweg, M.Jandel, R.O.Nelson, S.A.Wender, M.C.White, C.Y.Wu, E.Kwan, A.Chyzh, R.Henderson, J.Gostic

The Prompt Fission Neutron Spectrum (PFNS) Measurement Program at LANSCE

doi: 10.1016/j.nds.2014.08.057
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2014KW05      Nucl.Data Sheets 119, 221 (2014)

E.Kwan, C.Y.Wu, R.C.Haight, H.Y.Lee, T.A.Bredeweg, A.Chyzh, M.Devlin, N.Fotiades, J.M.Gostic, R.A.Henderson, M.Jandel, A.Laptev, R.O.Nelson, J.M.O'Donnell, B.A.Perdue, T.N.Taddeucci, J.L.Ullmann, S.A.Wender

Prompt Fission γ-rays Measured Using Liquid Scintillators

NUCLEAR REACTIONS 235U(n, F), E=1-20 MeV; measured prompt Eγ, Iγ, γγ-coin using FIGARO; deduced γ-ray spectrum, unfolded using SVD and iterative Bayesian techniques. Compared to 235Cf(SF).

RADIOACTIVITY 235Cf(SF); measured prompt Eγ, Iγ, γγ-coin using FIGARO; deduced γ-ray spectrum, unfolded using SVD and iterative Bayesian techniques. Compared to 235U(n, F).

doi: 10.1016/j.nds.2014.08.061
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2014PE14      Nucl.Data Sheets 119, 371 (2014)

B.A.Perdue, T.N.Taddeucci, R.C.Haight, T.Bredeweg, M.Devlin, N.Fotiades, M.Jandel, A.Laptev, H.Y.Lee, R.O.Nelson, J.M.O'Donnell, J.L.Ullmann, S.A.Wender, C.Y.Wu, E.Kwan, A.Chyzh, R.A.Henderson, J.M.Gostic

Development of an Array of Liquid Scintillators to Measure the Prompt Fission Neutron Spectrum at LANSCE

doi: 10.1016/j.nds.2014.08.102
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2013RU05      Phys.Rev. C 87, 054603 (2013)

G.Rusev, M.Jandel, M.Krticka, T.A.Bredeweg, A.Couture, T.N.Taddeucci, J.L.Ullmann

γ-ray cascade transitions in 112Cd and 114Cd following resonance capture of epithermal neutrons

NUCLEAR REACTIONS 111,113Cd(n, γ), E=epithermal; measured E(n), I(n), TOF, Eγ, Iγ, γγ-coin, σ, multiplicity distribution using DANCE calorimeter at LANSCE facility. 112,114Cd; deduced levels, resonances, J, π, neutron, two-step γ cascades and radiative width of s-wave resonances, E1, M1 and E2 strength function. Comparison with statistical-model calculations using DICEBOX code, SLO and KMF models.

doi: 10.1103/PhysRevC.87.054603
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2013UL01      Phys.Rev. C 87, 044607 (2013)

J.L.Ullmann, E.M.Bond, T.A.Bredeweg, A.Couture, R.C.Haight, M.Jandel, T.Kawano, H.Y.Lee, J.M.O'Donnell, A.C.Hayes, I.Stetcu, T.N.Taddeucci, P.Talou, D.J.Vieira, J.B.Wilhelmy, J.A.Becker, A.Chyzh, J.Gostic, R.Henderson, E.Kwan, C.Y.Wu

Prompt γ-ray production in neutron-induced fission of 239Pu

NUCLEAR REACTIONS 239Pu(n, F), E<30 keV; measured prompt Eγ, Iγ, fission σ(E), Gamma-ray multiplicity using DANCE γ-ray calorimeter at LANSCE facility; deduced average multiplicity, average total energy. GEANT4 simulation of DANCE detector. Fission Tagging. Comparison with Monte Carlo Hauser-Feshbach (MCHF) calculations, previous experimental studies, and with ENDF/B-VII.

doi: 10.1103/PhysRevC.87.044607
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2012KW01      Nucl.Instrum.Methods Phys.Res. A688, 55 (2012)

E.Kwan, C.Y.Wu, R.C.Haight, H.Y.Lee, T.A.Bredeweg, A.Chyzh, M.Devlin, N.Fotiades, J.M.Gostic, R.A.Henderson, M.Jandel, A.Laptev, R.O.Nelson, J.M.O'Donnell, B.A.Perdue, T.N.Taddeucci, J.L.Ullmann, S.A.Wender

Prompt energy distribution of 235U(n, f)γ at bombarding energies of 1-20 MeV

NUCLEAR REACTIONS 235U(n, F), E=1-20 MeV; measured reaction products, Eγ, Iγ; deduced prompt γ-rays distribution. Comparison with GEANT4 simulations.

RADIOACTIVITY 252Cf(SF); measured decay products, Eγ, Iγ; deduced prompt γ-rays distribution. Comparison with GEANT4 simulations.

doi: 10.1016/j.nima.2012.06.003
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14413.


2007SA14      Phys.Rev. C 75, 031001 (2007)

Y.Safkan, T.Akdogan, W.A.Franklin, J.L.Matthews, W.M.Schmitt, V.V.Zelevinsky, P.A.M.Gram, T.N.Taddeucci, S.A.Wender, S.F.Pate

Differential cross section for neutron-proton bremsstrahlung

NUCLEAR REACTIONS 1H(n, n'γ), E=175-275 MeV; measured Ep, En, σ(θ(n), θ(p), θ(γ)). Comparison with relativistic soft-photon and nonrelativistic models.

doi: 10.1103/PhysRevC.75.031001
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2002HA14      Phys.Rev. C65, 034612 (2002)

C.Hautala, J.Rapaport, M.Palarczyk, D.L.Prout, D.A.Cooper, G.Savopulos, B.Anderson, A.Baldwin, C.C.Foster, C.D.Goodman, K.Hicks, R.Howes, M.S.Islam, B.A.Luther, D.M.Manley, R.Madey, E.Sugarbaker, T.N.Taddeucci, I.Van Heerden, J.Watson, X.Yang, W.-M.Zhang

Polarization Transfer in Quasifree (p(pol), n(pol)) Reactions on C, Ca, and Pb Targets at 197 MeV

NUCLEAR REACTIONS 12C, 40Ca, Pb(polarized p, n), E=197 MeV; measured polarization transfer coefficients, σ(E, θ). Comparison with model predictions.

doi: 10.1103/PhysRevC.65.034612
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0864.


2002PR04      Phys.Rev. C65, 034611 (2002)

D.L.Prout, J.Rapaport, M.Palarczyk, D.A.Cooper, G.Savopulos, C.Hautala, B.Anderson, A.Baldwin, C.C.Foster, W.Gloeckle, C.D.Goodman, R.Howes, M.S.Islam, B.A.Luther, R.Madey, D.M.Manley, J.Sowinski, E.Sugarbaker, T.N.Taddeucci, I.Van Heerden, J.Watson, H.Witala, X.Yang, W.-M.Zhang

Polarization Transfer in Quasifree (p(pol), n(pol)) Reactions on 2H and 3, 4He Targets at 197 MeV

NUCLEAR REACTIONS 2H, 3,4He(polarized p, nX), E=197 MeV; measured polarization transfer coefficients, σ(E, θ). Comparison with model predictions.

doi: 10.1103/PhysRevC.65.034611
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0863.


2001PR02      Phys.Rev. C63, 014603 (2001)

D.L.Prout, J.Rapaport, E.Sugarbaker, D.Cooper, S.Delucia, B.Luther, C.D.Goodman, B.K.Park, L.Rybarcyk, T.N.Taddeucci, J.Ullmann

Observation of the Spin Isovector Monopole Resonance using the Pb(p(pol), n(pol))Bi Reaction at 795 MeV

NUCLEAR REACTIONS 12C, 90Zr, 208Pb(polarized p, n), E=795 MeV; measured neutron spectra, σ(E), polarization transfer observables; deduced spin isovector monopole resonance features. DWIA calculations. Comparison with previous results.

doi: 10.1103/PhysRevC.63.014603
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0792.


1999PA03      Phys.Rev. C59, 500 (1999)

M.Palarczyk, J.Rapaport, C.Hautala, D.L.Prout, C.D.Goodman, I.J.van Heerden, J.Sowinski, G.Savopulos, X.Yang, H.M.Sages, R.Howes, R.Carr, M.Islam, E.Sugarbaker, D.C.Cooper, K.Lande, B.Luther, T.N.Taddeucci

Measurement of Gamow-Teller Strength for 127I as a Solar Neutrino Detector

NUCLEAR REACTIONS 127I(p, n), E=94, 159, 197 MeV; measured neutrons σ(E, θ=0°). 127Xe deduced IAS energy, Coulomb displacement energy, B(GT) vs excitation energy. 127I deduced solar neutrino capture σ.

doi: 10.1103/PhysRevC.59.500
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0809.


1999VA04      Phys.Rev. C59, 1488 (1999)

I.J.van Heerden, M.Palarczyk, X.Wang, J.Rapaport, D.L.Prout, C.D.Goodman, B.A.Luther, E.Sugarbaker, T.N.Taddeucci, D.Dehnhard, C.C.Foster, K.Hicks, L.Wang, X.Yang, J.M.O'Donnell, H.Ohnuma, B.K.Park, G.R.Burleson, S.Blanchard

Zero-Degree Differential Cross Sections and DNN Values for the 17, 18O(p(pol), n(pol))17, 18F Reactions at Ep = 118 MeV

NUCLEAR REACTIONS 17,18O(polarized p, n), E=118 MeV; measured neutron spectra, σ(θ=0°), polarization transfer coefficients. 17,18F levels deduced B(GT), B(F). Implications for solar neutrino detection discussed.

doi: 10.1103/PhysRevC.59.1488
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1997TA03      Phys.Rev. C55, 1551 (1997)

T.N.Taddeucci, J.Ullmann, L.J.Rybarcyk, G.W.Butler, T.E.Ward

Total Cross Sections for Production of 7Be, 22Na, and 24Na in p + 7Li and p + 27Al Reactions at 495 and 795 MeV

NUCLEAR REACTIONS 7Li(p, n), 27Al(p, X), 7Be(p, 3n3p), (p, n3p), E=495, 795 MeV; measured residuals production σ; deduced energy dependence parameters.

doi: 10.1103/PhysRevC.55.1551
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0461.


1996PR03      Phys.Rev.Lett. 76, 4488 (1996)

D.L.Prout, S.DeLucia, D.Cooper, B.Luther, E.Sugarbaker, T.N.Taddeucci, L.J.Rybarcyk, J.Rapaport, B.K.Park, C.D.Goodman, G.Edwards, C.Glashausser, T.Sams, T.Udagawa, F.Osterfeld

Spin Decomposition of the Δ Resonance Cross Section using the 12C(p(pol), n(pol)) Reaction at E(p) = 795 MeV

NUCLEAR REACTIONS 12C(polarized p, n), E=795 MeV; measured polarization observables; deduced spin-longitudinal, spin-transverse, spin-independent partial σ, Δ-production related features.

doi: 10.1103/PhysRevLett.76.4488
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1995PR04      Phys.Rev. C52, 228 (1995)

D.L.Prout, C.Zafiratos, T.N.Taddeucci, J.Ullmann, R.C.Byrd, T.A.Carey, P.Lisowski, J.B.McClelland, L.J.Rybarcyk, W.Sailor, W.Amian, M.Braunstein, D.Lind, D.J.Mercer, D.Cooper, S.DeLucia, B.Luther, D.G.Marchlenski, E.Sugarbaker, J.Rapaport, B.K.Park, E.Gulmez, C.A.Whitten, Jr., C.D.Goodman, W.Huang, D.Ciskowski, W.P.Alford

Cross Sections and Analyzing Powers for Quasielastic Scattering at 795 and 495 MeV using the (p(pol), n) Reaction

NUCLEAR REACTIONS 12C, Pb(polarized p, n), E=495, 795 MeV; measured σ(θ), analyzing power vs energy loss. Models comparison.

doi: 10.1103/PhysRevC.52.228
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1995WA05      Phys.Rev. C51, 1345 (1995)

Y.Wang, X.Yang, J.Rapaport, C.D.Goodman, S.L.De Lucia, B.A.Luther, D.G.Marchlenski, B.K.Park, L.Rybarcyk, A.Smith, E.Sugarbaker, T.Taddeucci, L.Wang

Study of the (1/2)-(g.s.) → (1/2)+1 Transition in the 13C(p, n)13N Reaction at Intermediate Energies

NUCLEAR REACTIONS 13C(p, n), E=160, 186 MeV; measured σ(θ), σ(θ, En); deduced absolute σ for ΔJ(π)=0-, ΔJ(π)=1- transitions.

doi: 10.1103/PhysRevC.51.1345
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0443.


1995YA12      Phys.Rev. C52, 2535 (1995)

X.Yang, L.Wang, J.Rapaport, C.D.Goodman, C.C.Foster, Y.Wang, E.Sugarbaker, D.Marchlenski, S.de Lucia, B.Luther, L.Rybarcyk, T.N.Taddeucci, B.K.Park

Dipole Excitations in p-Shell Nuclei Via (p, n) Reactions

NUCLEAR REACTIONS 6,7Li, 10,11B, 12,13C(p, n), E=186 MeV; measured σ(θ, En); deduced quasifree reaction contribution in giant resonance region, ΔL=1 transitions energy spectra.

doi: 10.1103/PhysRevC.52.2535
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0428.


1994GI09      Nucl.Phys. A577, 227c (1994)

R.Gilman, E.Brash, G.Edwards, C.Glashausser, M.K.Jones, F.T.Baker, S.Bastea, D.P.Beatty, L.Bimbot, J.Brusoe, J.Chiba, D.Cooper, G.Kumbartzki, C.Mauger, T.Nagae, B.Park, D.Prout, R.D.Ransome, M.Rawool-Sullivan, P.Rutt, B.Storm, E.Sugarbaker, T.Taddeucci, J.Zumbro

Coherent Pion Production in 12C(p, nπ) at 800 MeV

NUCLEAR REACTIONS 12C(p, nπ+), E=800 MeV; measured neutron, pion spectra.

doi: 10.1016/0375-9474(94)90860-5
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1994ME07      Phys.Rev. C49, 3104 (1994)

D.J.Mercer, J.Rapaport, C.A.Whitten, Jr., D.Adams, R.Byrd, X.Y.Chen, A.Fazely, T.Gaussiran, E.Gulmez, C.Goodman, D.W.Huang, G.Igo, A.Ling, D.Marchlenski, D.Prout, L.Rybarcyk, E.Sugarbaker, T.N.Taddeucci

Multipole Decomposition of the 16O(p, n)16F and 18O(p, n)18F Reactions at 494 MeV

NUCLEAR REACTIONS 16,18O(p, n), E=494 MeV; measured σ(θ); deduced transition multipole components for ΔL=0, ΔL=1, ΔL ≥ 2. 18,16F deduced Gamow-Teller strength B(GT).

doi: 10.1103/PhysRevC.49.3104
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0170.


1994PR08      Nucl.Phys. A577, 233c (1994)

D.Prout, S.Delucia, E.Sugarbaker, B.Luther, D.Cooper, T.Taddeucci, L.Rybarcyk, J.McClelland, C.Goodman, B.Park, J.Rapaport, T.Sams, G.Edwards, C.Glashausser

Spin-Longitudinal and Spin-Transverse Cross Section for Δ Production in the 12C(p(pol), n(pol)) Reaction

NUCLEAR REACTIONS 2H, 12C(polarized p, n), E=795 MeV; measured spin observables; deduced spin-longitudinal, spin-transverse σ(θ) vs energy transfer.

doi: 10.1016/0375-9474(94)90861-3
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1994TA15      Nucl.Phys. A577, 105c (1994)

T.N.Taddeucci

Nuclear Isovector Spin Responses from (p(pol), n(pol)) Reactions at 494 MeV

NUCLEAR REACTIONS 2H, C, Ca(polarized p, n), E=494 MeV; measured σ(θ) vs energy transfer, polarization transfer coefficients; deduced transverse, longitudinal isovector spin responses.

doi: 10.1016/0375-9474(94)90842-7
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1994TA24      Phys.Rev.Lett. 73, 3516 (1994)

T.N.Taddeucci, B.A.Luther, L.J.Rybarcyk, R.C.Byrd, J.B.McClelland, D.L.Prout, S.DeLucia, D.A.Cooper, D.G.Marchlenski, E.Sugarbaker, B.K.Park, T.Sams, C.D.Goodman, J.Rapaport, M.Ichimura, K.Kawahigashi

Momentum Dependence of the Nuclear Isovector Spin Responses from (p(pol), n(pol)) Reactions at 494 MeV

NUCLEAR REACTIONS 2H, 12C, 40Ca(polarized p, n), E=494 MeV; measured polarization transfer coefficients; deduced longitudinal, transverse isovector spin responses.

doi: 10.1103/PhysRevLett.73.3516
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1994WA22      Phys.Rev. C50, 2438 (1994)

L.Wang, X.Yang, J.Rapaport, C.D.Goodman, C.C.Foster, Y.Wang, J.Piekarewicz, E.Sugarbaker, D.Marchlenski, S.de Lucia, B.Luther, L.Rybarcyk, T.N.Taddeucci, B.K.Park

(p, n) Quasifree Excitations in p-Shell Nuclei at 186 MeV

NUCLEAR REACTIONS 6,7Li, 10,11B, 12,13C(p, n), (polarized p, n), E=186 MeV; measured σ(θ, En), polarization transfer coefficient, analyzing power vs θ. Quasifree model analysis.

doi: 10.1103/PhysRevC.50.2438
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1993CH13      Phys.Rev. C47, 2159 (1993)

X.Y.Chen, T.N.Taddeucci, J.B.McClelland, T.A.Carey, R.C.Byrd, L.J.Rybarcyk, W.C.Sailor, D.J.Mercer, D.L.Prout, S.DeLucia, B.Luther, D.G.Marchlenski, E.Sugarbaker, J.Rapaport, E.Gulmez, C.A.Whitten, Jr., C.D.Goodman, W.Huang, Y.Wang, W.P.Alford

Polarization Transfer in Quasifree (p(pol), n(pol) Reactions at 495 MeV

NUCLEAR REACTIONS 2H, 12C, 40Ca(polarized p, n), E=495 MeV; measured σ(θ), analyzing power, polarization transfer coefficient vs energy loss; deduced response functions, residual interaction modifications.

doi: 10.1103/PhysRevC.47.2159
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1993ME06      Phys.Rev.Lett. 71, 684 (1993)

D.J.Mercer, T.N.Taddeucci, L.J.Rybarcyk, X.Y.Chen, D.L.Prout, R.C.Byrd, J.B.McClelland, W.C.Sailor, S.DeLucia, B.Luther, D.G.Marchlenski, E.Sugarbaker, E.Gulmez, C.A.Whitten, Jr., C.D.Goodman, J.Rapaport

Polarization Transfer in (p(pol), n(pol)) Reactions at 318 and 494 MeV and the Effective Interaction

NUCLEAR REACTIONS 2H, 12,14C(polarized p, n), E=318, 494 MeV; measured polarization transfer observable; deduced medium effects modification to effective interaction.

doi: 10.1103/PhysRevLett.71.684
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1993WA06      Phys.Rev. C47, 2123 (1993)

L.Wang, X.Yang, J.Rapaport, C.D.Goodman, C.C.Foster, Y.Wang, R.A.Lindgren, E.Sugarbaker, D.Marchlenski, S.de Lucia, B.Luther, L.Rybarcyk, T.N.Taddeucci, B.K.Park

10B(p, n)10C Reaction at 186 MeV

NUCLEAR REACTIONS 10B(p, n), (polarized p, n), E=186 MeV; measured σ(θn, En), analyzing power, polarization, polarization transfer. 10C deduced resonances, J, π, possible IAS character.

doi: 10.1103/PhysRevC.47.2123
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1993YA11      Phys.Rev. C48, 1158 (1993)

X.Yang, L.Wang, J.Rapaport, C.D.Goodman, C.Foster, Y.Wang, W.Unkelbach, E.Sugarbaker, D.Marchlenski, S.de Lucia, B.Luther, J.L.Ullmann, A.G.Ling, B.K.Park, D.S.Sorenson, L.Rybarcyk, T.N.Taddeucci, C.R.Howell, W.Tornow

Dipole and Spin-Dipole Resonances in Charge-Exchange Reactions on 12C

NUCLEAR REACTIONS 12C(n, p), E=60-260 MeV; measured σ(θ, Ep); 12C(p, n), E=186 MeV; 12C(polarized p, n), E=160 MeV; measured σ(θ, En), polarization, spin observables, analyzing power; deduced dipole, spin-dipole resonances.

doi: 10.1103/PhysRevC.48.1158
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1992MC09      Phys.Rev.Lett. 69, 582 (1992)

J.B.McClelland, T.N.Taddeucci, X.Y.Chen, W.P.Alford, R.C.Byrd, T.A.Carey, S.DeLucia, C.D.Goodman, E.Gulmez, W.Huang, B.Luther, D.G.Marchlenski, D.J.Mercer, D.L.Prout, J.Rapaport, L.J.Rybarcyk, W.Sailor, E.Sugarbaker, Y.Wang, C.Whitten, Jr.

Quasifree Polarization-Transfer Measurements in the (p(pol), n(pol)) Reaction at 495 MeV

NUCLEAR REACTIONS 2H, C, Ca(polarized p, n), E=495 MeV; measured polarization transfer variables, complete set; deduced longitudinal to spin-transverse responses ratio. Distorted waves, RPA nuclear response.

doi: 10.1103/PhysRevLett.69.582
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1991CH31      Phys.Rev. C44, 2041 (1991)

X.Y.Chen, J.R.Shepard, M.R.Braunstein, T.A.Carey, K.W.Jones, J.B.McClelland, L.Rees, T.N.Taddeucci, N.Tanaka, A.D.Bacher

Complete Spin-Transfer Measurements for Inelastic Polarized Proton Scattering from 12C

NUCLEAR REACTIONS 12C(polarized p, p'), E=500 MeV; measured σ(θ), spin-transfer observables vs θ, analyzing power. 12C levels deduced spin responses.

doi: 10.1103/PhysRevC.44.2041
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1991GL01      Phys.Rev. C43, 1664 (1991)

C.W.Glover, C.C.Foster, P.Schwandt, J.R.Comfort, J.Rapaport, T.N.Taddeucci, D.Wang, G.J.Wagner, J.Seubert, A.W.Carpenter, J.A.Carr, F.Petrovich, R.J.Philpott, M.J.Threapleton

Scattering of Polarized Protons from 7Li at 200 MeV

NUCLEAR REACTIONS 7Li(polarized p, p), (polarized p, p'), E=200 MeV; measured σ(θ), analyzing power vs θ. 6,7Li deduced radial density shape differences. Single scattering model.

doi: 10.1103/PhysRevC.43.1664
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1991TA13      Nucl.Phys. A527, 393c (1991)

T.N.Taddeucci, R.C.Byrd, T.A.Carey, D.E.Ciskowski, C.D.Goodman, E.Gulmez, W.Huang, D.Marchlenski, J.B.McClelland, D.Prout, J.Rapaport, L.J.Rybarcyk, W.C.Sailor, E.Sugarbaker

Cross Section and Analyzing Power for Quasifree (p, n) Reactions

NUCLEAR REACTIONS 12C(polarized p, n), E=494, 795 MeV; measured σ(θ), analyzing power; deduced quasifree neutron knockout. Relativistic fermi gas model.

doi: 10.1016/0375-9474(91)90128-S
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1990GL04      Phys.Rev. C41, 2487 (1990)

C.W.Glover, C.C.Foster, P.Schwandt, J.R.Comfort, J.Rapaport, T.N.Taddeucci, D.Wang, G.J.Wagner, J.Seubert, A.W.Carpenter, J.A.Carr, F.Petrovich, R.J.Philpott, M.J.Threapleton

Scattering of Polarized Protons from 6Li at 200 MeV

NUCLEAR REACTIONS 6Li(polarized p, p), (polarized p, p'), E=200 MeV; measured σ(θ), analyzing power vs (θ). Microscopic single scattering model with free, Pauli corrected effective nucleon-nucleon interactions.

doi: 10.1103/PhysRevC.41.2487
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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
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1990SU12      Phys.Rev.Lett. 65, 551 (1990)

E.Sugarbaker, D.Marchlenski, T.N.Taddeucci, L.J.Rybarcyk, J.B.McClelland, T.A.Carey, R.C.Byrd, C.D.Goodman, W.Huang, J.Rapaport, D.Mercer, D.Prout, W.P.Alford, E.Gulmez, C.A.Whitten, D.Ciskowski

Isovector Effective Interactions from 14C(p, n)14N Studies between 500 and 800 MeV

NUCLEAR REACTIONS 14C(p, n), E=494, 644, 795 MeV; measured σ(θ=0°); deduced effective nucleon interaction components.

doi: 10.1103/PhysRevLett.65.551
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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
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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
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1989RA09      Phys.Rev. C39, 1929 (1989)

J.Rapaport, P.W.Lisowski, J.L.Ullmann, R.C.Byrd, T.A.Carey, J.B.McClelland, L.J.Rybarcyk, T.N.Taddeucci, R.C.Haight, N.S.P.King, G.L.Morgan, D.A.Clark, D.E.Ciskowski, D.A.Lind, R.Smythe, C.D.Zafiratos, D.Prout, E.R.Sugarbaker, D.Marchlenski, W.P.Alford, W.G.Love

Fermi and Gamow-Teller Strength in p-Shell Nuclei from (p, n) Reactions at 492 and 590 MeV

NUCLEAR REACTIONS 7Li, 11B, 12,13,14C(p, n), E=492 MeV; 13C, 11B(p, n), E=590 MeV; measured σ(θ, E); deduced unit σ(ratio).

doi: 10.1103/PhysRevC.39.1929
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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
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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
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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
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1987SA02      Phys.Rev. C35, 344 (1987)

H.Sakai, T.A.Carey, J.B.McClelland, T.N.Taddeucci, R.C.Byrd, C.D.Goodman, D.Krofcheck, L.J.Rybarcyk, E.Sugarbaker, A.J.Wagner, J.Rapaport

Cross Section and Transverse Polarization Transfer for the 2H(p, n)2p Reaction at 160 MeV

NUCLEAR REACTIONS, MECPD 2H(p, n), E=160 MeV; measured σ(En, θ), transverse polarization coefficient. Plastic scintillators. Impulse approximation analysis.

doi: 10.1103/PhysRevC.35.344
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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
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1987TA22      Can.J.Phys. 65, 557 (1987)

T.N.Taddeucci

Polarization Transfer in (p, n) Reactions

NUCLEAR REACTIONS 13,14C(p, n), E=80, 120, 160 MeV; compiled excitation energy spectra data; 14C(p, n), E=60-200 MeV; compiled effective analyzing power data. 2H, 7Li, 12,13,14C(p, n), E ≤ 220 MeV; compiled σ(E), σ(En, θn), D(NN) data. 40Ca, 90Zr(p, n), E=120, 160, 200 MeV; compiled σ(θ) vs excitation energy, D(NN) data.

doi: 10.1139/p87-079
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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
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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
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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
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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
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1985TA23      Nucl.Instrum.Methods 241, 448 (1985)

T.N.Taddeucci, C.D.Goodman, R.C.Byrd, T.A.Carey, D.J.Horen, J.Rapaport, E.Sugarbaker

A Neutron Polarimeter for (p, n) Measurements at Intermediate Energies

NUCLEAR REACTIONS 14C(polarized p, n), E=80, 120, 160 MeV; measured transverse polarization transfer, σ(En). Large volume, large acceptance neutron polarimeter, plastic scintillator.

doi: 10.1016/0168-9002(85)90597-2
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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
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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
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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
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1984TA02      Phys.Rev. C29, 764 (1984)

T.N.Taddeucci, R.R.Doering, A.Galonsky, S.M.Austin

(p, n) Reactions on 14C and 14N and the Effective Nucleon-Nucleon Interaction

NUCLEAR REACTIONS 14N(p, n), E=35.2 MeV; 14C(p, n), E=25.7, 35, 45 MeV; measured σ(θ); deduced optical potential isovector component energy dependence. 14N levels deduced spectroscopic coefficients, Gamow-Teller transition strengths. DWBA, Lane model analyses.

doi: 10.1103/PhysRevC.29.764
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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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1983TA12      Phys.Rev. C28, 969 (1983)

T.N.Taddeucci, J.Rapaport, C.C.Foster, J.R.Comfort

14N(p(pol), p')14N(2.31 MeV) Reaction at 159.4 MeV

NUCLEAR REACTIONS 12C, 14N(polarized p, p), (polarized p, p'), E=159.4 MeV; measured σ(θ), analyzing power vs θ. Single-step DWBA, DWIA analyses.

doi: 10.1103/PhysRevC.28.969
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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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1983WA10      Phys.Rev. C27, 2777 (1983)

G.E.Walker, T.N.Taddeucci

Energy-Dependent Signature of the Spin-Orbit Interaction in Inelastic Nucleon-Nucleus Scattering

NUCLEAR REACTIONS 12C(p, p'), E=135 MeV; 40Ca(p, p'), E=140 MeV; calculated σ(θ) vs momentum transfer; deduced effective spin-orbit interaction. DWIA, energy dependent t-matrix.

doi: 10.1103/PhysRevC.27.2777
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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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1982TA06      Phys.Rev. C25, 2130 (1982)

T.N.Taddeucci, J.Rapaport, C.D.Goodman

Comment on ' Giant M1 States in Zr Isotopes within the Simple Shell Model '

NUCLEAR REACTIONS 90Zr(p, n), E=120, 200 MeV; 90Zr(p, p'), E=200 MeV; analyzed σ(θ); deduced optical model distortion energy dependence. 90Zr deduced M1 transition strength quenching factor. DWBA analysis.

doi: 10.1103/PhysRevC.25.2130
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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
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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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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
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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
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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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1979DO14      Phys.Rev. C20, 1627 (1979)

R.R.Doering, T.N.Taddeucci, A.Galonsky, D.M.Patterson

14C(p, n)14N and the Isovector Tensor Component of the Effective Two-Nucleon Interaction

NUCLEAR REACTIONS 14C(p, n), E=35 MeV; measured σ(θ); deduced tensor force. DWBA analysis.

doi: 10.1103/PhysRevC.20.1627
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