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NSR database version of April 11, 2024.

Search: Author = T.Massey

Found 98 matches.

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2023BR02      Nucl.Sci.Eng. 197, 510 (2023)

K.Brandenburg, G.Hamad, Z.Meisel, C.R.Brune, D.E.Carter, J.Derkin, D.C.Ingram, Y.Jones-Alberty, B.Kenady, T.N.Massey, M.Saxena, D.Soltesz, S.K.Subedi, J.Warren

Measurements of the 27Al(α, n) Thick Target Yield near Threshold

NUCLEAR REACTIONS 27Al(n, α), E=3-5 MeV; measured reaction products, En, In; deduced thick-target-yields. Comparison with available data. The 3HeBF3 Giant Barrel (HeBGB) neutron detector at the Edwards Accelerator Laboratory at Ohio University.

doi: 10.1080/00295639.2022.2118483
Citations: PlumX Metrics


2023BR13      Phys.Rev. C 108, L061601 (2023)

K.Brandenburg, G.Hamad, Z.Meisel, C.R.Brune, D.E.Carter, R.J.deBoer, J.Derkin, C.Feathers, D.C.Ingram, Y.Jones-Alberty, B.Kenady, T.N.Massey, M.Saxena, D.Soltesz, S.K.Subedi, A.V.Voinov, J.Warren, M.Wiescher

Measurements of the 13C(α, n)16O cross section up to Eα=8 MeV

doi: 10.1103/PhysRevC.108.L061601
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2023VO08      Phys.Rev. C 108, 034302 (2023)

A.V.Voinov, N.Alanazi, S.Akhtar, S.Dhakal, C.R.Brune, S.M.Grimes, T.N.Massey, Z.Meisel, C.E.Parker, A.L.Richard

Spin cutoff factor and level density for 59Ni from an analysis of compound nuclear reactions

doi: 10.1103/PhysRevC.108.034302
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2022HA25      Phys.Rev. C 106, 025804 (2022)

G.Hamad, K.Brandenburg, Z.Meisel, C.R.Brune, D.E.Carter, D.C.Ingram, Y.Jones-Alberty, T.N.Massey, M.Saxena, D.Soltesz, S.K.Subedi, A.V.Voinov

Measurements of the 96Zr(α, n)99Mo cross section for astrophysics and applications

doi: 10.1103/PhysRevC.106.025804
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2807.


2022MA27      Phys.Rev. C 105, 054612 (2022)

T.N.Massey, J.E.O'Donnell, J.Ralston, S.M.Grimes, C.R.Brune, R.C.Haight

Charged-particle emission in neutron reactions on 10B

NUCLEAR REACTIONS 10B(n, p), (n, d), (n, t), (n, α), E=1-20 MeV; measured reaction products, Ep, Ip, Eα, Iα, deuteron spectra, triton spectra, In, angular distributions; deduced partial σ(E), σ(θ, E) for the emission of p0, p1, d0, t0, t1, α0, α1, α2, α3. 11B; deduced levels, J, π, molecular and cluster states. R-matrix analysis. Comparison to other experimental data and ENDF/B-VIII.0, ENDF/B-VII evaluations. Spallation neutron source at the Weapons Nuclear Research Facility (WNR) at the Los Alamos Neutron Science Center (LANSCE).

doi: 10.1103/PhysRevC.105.054612
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14663.


2022NE12      Phys.Rev. C 106, 044320 (2022)

S.Neupane, J.Heideman, R.Grzywacz, M.Cooper, J.Hooker, K.L.Jones, T.T.King, N.Kitamura, M.Madurga, K.Siegl, C.R.Thornsberry, P.Wagenknecht, Z.Y.Xu, L.H.Heilbronn, M.M.Rajabali, A.Chester, A.Richard, Y.Alberty-Jones, J.Derkin, T.N.Massey, D.Soltesz, N.T.Brewer, B.C.Rasco, K.P.Rykaczewski, M.Wolinska-Cichocka, J.Clark, D.Santiago-Gonzalez, G.Savard

Demonstration of the neutron tracking capability of NEXT array in time-of-flight measurements to improve energy resolution

RADIOACTIVITY 17N, 104Nb(β-n); measured neutron time-of-flight (ToF), En, In. Data on the commissioning of the Neutron dEtector with Xn Tracking (NEXT) array consisting of 8x4 optically separated segments. Measurement of 17N decay at National Superconducting Cyclotron Laboratory (NSCL), 106Nb decay Argonne National Laboratory (ANL, CARIBU Facility).

NUCLEAR REACTIONS 27Al(d, n), E=7.44 MeV; measured neutron time-of-flight (ToF), En, In. Data on the commissioning of the Neutron dEtector with Xn Tracking (NEXT) array consisting of 8x4 optically separated segments. Deuteron beam from Ohio University Edwards Accelerator Laboratory (EAL).

doi: 10.1103/PhysRevC.106.044320
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2022VA04      Phys.Rev. C 105, 055802 (2022)

B.Vande Kolk, K.T.Macon, R.J.deBoer, T.Anderson, A.Boeltzig, K.Brandenburg, C.R.Brune, Y.Chen, A.M.Clark, T.Danley, B.Frentz, R.Giri, J.Gorres, M.Hall, S.L.Henderson, E.Holmbeck, K.B.Howard, D.Jacobs, J.Lai, Q.Liu, J.Long, K.Manukyan, T.Massey, M.Moran, L.Morales, D.Odell, P.O'Malley, S.N.Paneru, A.Richard, D.Schneider, M.Skulski, N.Sensharma, C.Seymour, G.Seymour, D.Soltesz, S.Strauss, A.Voinov, L.Wustrich, M.Wiescher

Investigation of the 10B (p, α)7Be reaction from 0.8 to 2.0 MeV

NUCLEAR REACTIONS 10B(p, α), (p, p), E=0.8-2.0 MeV; measured Eα, Iα, Ep, Ip; deduced σ(θ), σ(E) S-factor, resonance parameters of 10B+p system - energy, spin, partial (p0, α0, α1) and total width. 10B(p, γ), E=0 .1-2.0 MeV; deduced σ(θ). 11C; deduced levels, J, π. R-matrix analysis. Measurements were made at the University of Notre Dame (UND) Nuclear Science Laboratory (NSL) using a degrader foil method, while those at the Edwards AcceleratorLaboratory at Ohio University (OU) were performed using the time-of-flight (ToF)technique. Comparison with other experimental data.

doi: 10.1103/PhysRevC.105.055802
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2767. Data from this article have been entered in the XUNDL database. For more information, click here.


2021MC05      Phys.Rev. C 103, 064607 (2021)

A.M.McEvoy, H.W.Herrmann, Y.Kim, T.S.Sedillo, H.Geppert-Kleinrath, C.R.Brune, T.N.Massey, A.V.Voinov, C.E.Parker, M.S.Rubery, W.Stoeffl

13C(n, 2nγ)12C γ-ray production in the 14-16 MeV incident neutron energy range

NUCLEAR REACTIONS 12,13C(n, 2nγ), (n, n'γ), E=14.4 to 15.8 MeV; measured Eγ, Iγ using Gas Cherenkov Detector (GCD) and enriched targets at the Omega Laser Facility and at the Ohio University Edwards Accelerator Laboratory; deduced σ(E), and compared with MCNP6.1 predictions. Relevance to feasibility of using 13C-based plastic ablators with embedded 12C layers for 'dark mix' diagnosis of inertial confinement fusion (ICF) implosions.

doi: 10.1103/PhysRevC.103.064607
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14710.


2021SO05      Phys.Rev. C 103, 015802 (2021)

D.Soltesz, M.A.A.Mamun, A.V.Voinov, Z.Meisel, B.A.Brown, C.R.Brune, S.M.Grimes, H.Hadizadeh, M.Hornish, T.N.Massey, J.E.O'Donnell, W.E.Ormand

Determination of the 60Zn level density from neutron evaporation spectra

NUCLEAR REACTIONS 58Ni(3He, n), E=10 MeV; measured E(n), I(n) by time-of-flight method using NE213 liquid organic scintillators at Edwards Accelerator Laboratory; deduced differential σ(En) and for σ(Ep), the latter from experimental data in 2007Vo08, and compared to theoretical calculations using TALYS-V1.8. 60Zn; deduced level density for 60Zn as function of excitation energy up to 10 MeV, and compared to global theoretical models, including phenomenological, microscopic, and shell-model based calculations. Relevance to confirmation of Hauser-Feshbach formalism for 59Cu(p, γ)60Zn reaction rate at x-ray burst temperatures.

doi: 10.1103/PhysRevC.103.015802
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2593.


2021VO11      Phys.Rev. C 104, 015805 (2021)

A.V.Voinov, K.Brandenburg, C.R.Brune, R.Giri, S.M.Grimes, T.Massey, Z.Meisel, S.N.Paneru, A.L.Richard, G.Perdikakis, A.Falduto

Reduction of the neutron imaginary potential off the stability line and its possible impact on neutron capture rates

NUCLEAR REACTIONS 48Ca(11B, X)59Mn*, E=21.8 MeV; measured E(n), I(n), E(p), I(p), Eα, Iα emitted by the compound nucleus 59Mn using ΔE-E Si detector telescope at the Edwards Accelerator Laboratory; analyzed optical model potentials (OMP) with their original parametrizations as well as with adjusted isovector imaginary components using EMPIRE code and BSFG Egidy level-density parametrization; deduced importance of inclusion of isovector component of the imaginary potential; discussed consequences for astrophysical reaction-rate calculations.

doi: 10.1103/PhysRevC.104.015805
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2654.


2020GA12      Phys.Rev. C 101, 055805 (2020)

P.Gastis, G.Perdikakis, J.Dissanayake, P.Tsintari, I.Sultana, C.R.Brune, T.N.Massey, Z.Meisel, A.V.Voinov, K.Brandenburg, T.Danley, R.Giri, Y.Jones-Alberty, S.Paneru, D.Soltesz, S.Subedi

Constraining the destruction rate of 40K in stellar nucleosynthesis through the study of the 40Ar(p, n)40K reaction

NUCLEAR REACTIONS 40Ar(p, n)40K, E(cm)=3.3-3.9 MeV; measured In, Eγ, Iγ, and differential σ(θ, E) using neutron time-of-flight technique with plastic scintillators for neutron detection and LaBr3 scintillator for γ detection at the Edwards Accelerator Laboratory of Ohio University; deduced total σ(E), and partial σ(E) populating discrete states. 40K(n, p), E(cm)=3.3-3.9 MeV; deduced thermonuclear reaction rates for the forward and reverse reactions. Comparison with Hauser-Feshbach calculations using the statistical model code TALYS, and with theoretical rates in the REACLIB library. Relevance to yield of 40K in nucleosynthesis, and impact on galactic chemical evolution models for the study of properties of exoplanets.

doi: 10.1103/PhysRevC.101.055805
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2570.


2020KO12      Nucl.Sci.Eng , 194, 335 (2020)

N.V.Kornilov, S.M.Grimes, T.N.Massey, C.E.Brient, D.E.Carter, J.E.O'Donnell, K.W.Cooper, A.D.Carlson, F.B.Bateman, C.R.Heimbach, N.Boukharouba

A High-Precision Tagged Neutron n-p Scattering Measurement at 14.9 MeV

NUCLEAR REACTIONS 1H(n, n), E=14.9 MeV; measured reaction products, Ep, Ip; deduced σ(θ). Comparison with ENDF/B-VII evaluated library.

doi: 10.1080/00295639.2019.1702408
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14656.


2020VO12      Phys.Rev. C 102, 064005 (2020)

A.V.Voinov, S.Akhtar, N.Alanazi, K.Brandenburg, C.R.Brune, T.W.Danley, S.Dhakal, R.Giri, T.N.Massey, S.N.Paneru, C.E.Parker, A.L.Richard, C.J.Forrest, D.Schneider, G.Grim

Cross section of neutrons from the 2H(n, 2n) reaction at En = 15 MeV

NUCLEAR REACTIONS 16O(n, n), 2H(n, 2n), E=15 MeV; measured reaction products, En, In; deduced cross sections using H2O and D2O targets and NE213 liquid scintillator at the Swinger neutron facility of Edwards Accelerator Laboratory. Comparison with models based on phase-space approximation used in the ENDF/B-VIII.0 data library and in the MCNP neutron transport code, and using the rigorous model based on Faddeev equations.

doi: 10.1103/PhysRevC.102.064005
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14681.


2019DH01      Nucl.Sci.Eng. 193, 1033 (2019)

S.Dhakal, C.R.Brune, T.N.Massey, S.M.Grimes, A.V.Voinov, S.Akhtar, An.P.D.Ramirez, A.L.Richard

Investigation of Neutron Cross Section for Iron in the ENDF Library wiTh. Pulsed Sphere Measurements

NUCLEAR REACTIONS 56Fe(n, n), (n, n'), E=7.2-10 MeV; measured reaction products, En, In; deduced σ. Comparison with MCNP simulations, ENDF/B libraries.

doi: 10.1080/00295639.2019.1591095
Citations: PlumX Metrics


2019GR05      Phys.Rev. C 99, 064331 (2019)

S.M.Grimes, T.N.Massey, A.V.Voinov

Level density rotational enhancement factor

NUCLEAR STRUCTURE 24Na, 25,26Mg, 159,161,162,163,164,165Dy, 235,238U; analyzed level densities for deformed nuclei with spherical and deformed spin distributions using resonance counting method, average level spacing at neutron separation energy, S(n), rotational enhancement factor. Comparison with level density predictions using the Bethe spin distribution for spherical nuclei.

doi: 10.1103/PhysRevC.99.064331
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2019VO05      Phys.Rev. C 99, 054609 (2019)

A.V.Voinov, T.Renstrom, D.L.Bleuel, S.M.Grimes, M.Guttormsen, A.C.Larsen, S.N.Liddick, G.Perdikakis, A.Spyrou, S.Akhtar, N.Alanazi, K.Brandenburg, C.R.Brune, T.W.Danley, S.Dhakal, P.Gastis, R.Giri, T.N.Massey, Z.Meisel, S.Nikas, S.N.Paneru, C.E.Parker, A.L.Richard

Level densities of 74, 76Ge from compound nuclear reactions

NUCLEAR STRUCTURE 68,70Zn(7Li, p), E=16 MeV; measured evaporated proton spectra from 2-25 MeV, σ, yields using silicon ΔE-E telescope at the Edwards tandem accelerator laboratory, Athens, Ohio. 74,76Ge; deduced nuclear level densities. Comparison with theoretical calculations using coupled-channel model of the EMPIRE code, GCM-RIPL-global, and BSFG-RIPL-global density models.

doi: 10.1103/PhysRevC.99.054609
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2018YU02      Phys.Rev. C 97, 024613 (2018)

M.Yuly, T.Eckert, G.Hartshaw, S.J.Padalino, D.N.Polsin, M.Russ, A.T.Simone, C.R.Brune, T.N.Massey, C.E.Parker, R.Fitzgerald, T.C.Sangster, S.P.Regan

12C(n, 2n)11C cross section from threshold to 26.5 MeV

NUCLEAR REACTIONS 12C(n, 2n)11C, E=19.7-26.4 MeV; measured Eγ, Iγ, positron annihilation radiation from the decay of 11C, σ(E) using the Pelletron accelerator at Ohio University. Comparison with previous measurements in E(n)=20-30 MeV range. Relevance to deuterium-tritium (DT) implosion compression of an inertial confinement fusion (ICF) burn.

doi: 10.1103/PhysRevC.97.024613
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14497.


2016GR08      Phys.Rev. C 94, 014308 (2016)

S.M.Grimes, A.V.Voinov, T.N.Massey

Mass-number and excitation-energy dependence of the spin cutoff parameter

NUCLEAR STRUCTURE A=10-250; calculated spin cutoff parameters σ2 as function of mass number and compared with experimental values deduced from isomeric ratios using microscopic model. Comparison with previous semiempirical calculations. Recommend reanalysis of neutron resonance data for deformed nuclei using a corrected factor to convert s-wave resonance level density to the total level density.

doi: 10.1103/PhysRevC.94.014308
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2015RA11      Phys.Rev. C 92, 014303 (2015)

A.P.D.Ramirez, A.V.Voinov, S.M.Grimes, Y.Byun, C.R.Brune, T.N.Massey, S.Akhtar, S.Dhakal, C.E.Parker

Level density and mechanism of deuteron-induced reactions on 54, 56, 58Fe

NUCLEAR REACTIONS 54,56,58Fe(d, d), (d, n), (d, p), (d, α), E=5, 7, 9 MeV; measured neutron, protons, deuterons, and α particle spectra, σ(θ, E) at Ohio University tandem accelerator facility. 55,57,59Co, 55,57Fe, 52,54,56Mn; deduced nuclear level densities of the residual nuclei from best fit to compound double differential cross sections, and compared with Gilbert-Cameron model using Iljinov parameter systematics. Comparison with theoretical cross sections using Hartree-Fock-Bogoliubov method (HFBM) and Gilbert-Cameron model (GCM).

doi: 10.1103/PhysRevC.92.014303
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2164.


2014BY06      Phys.Rev. C 90, 044303 (2014)

Y.Byun, A.P.D.Ramirez, S.M.Grimes, A.V.Voinov, C.R.Brune, T.N.Massey

Deuteron-induced reactions on 89Y and nuclear level density of 90Zr

NUCLEAR REACTIONS 89Y(d, d), (d, n), (d, p), E=5, 6, 7.44 MeV; measured deuteron spectra, E(n), I(n), E(p), I(p), σ(E, θ), angle-integrated σ(E) at Ohio University tandem accelerator facility. 90Zr; deduced levels, J, π, configuration, level densities. Comparison with microscopic HFB model calculations using EMPIRE code.

doi: 10.1103/PhysRevC.90.044303
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2014KO33      Nucl.Data Sheets 119, 413 (2014)

N.V.Kornilov, S.M.Grimes, T.N.Massey, C.E.Brient, D.E.Carter, J.E.O'Donnell, F.B.Bateman, A.D.Carlson, R.C.Haight, N.Boukharouba

Development of a New Method for Measurement of Neutron Detector Efficiency up to 20 MeV

doi: 10.1016/j.nds.2014.08.116
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2014LO09      Nucl.Data Sheets 119, 383 (2014)

W.Loveland, L.Yao, D.M.Asner, R.G.Baker, J.Bundgaard, E.Burgett, M.Cunningham, J.Deaven, D.L.Duke, U.Greife, S.Grimes, M.Heffner, T.Hill, D.Isenhower, J.L.Klay, V.Kleinrath, N.Kornilov, A.B.Laptev, T.N.Massey, R.Meharchand, H.Qu, J.Ruz, S.Sangiorgio, B.Selhan, L.Snyder, S.Stave, G.Tatishvili, R.T.Thornton, F.Tovesson, D.Towell, R.S.Towell, S.Watson, B.Wendt, L.Wood

Targets for Precision Measurements

doi: 10.1016/j.nds.2014.08.106
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2014MA58      Nucl.Data Sheets 119, 107 (2014)

T.N.Massey, J.Ralston, S.M.Grimes, R.C.Haight

10B(n, Z) Measurements in the Energy Range 0.7 to 5.0 MeV

NUCLEAR REACTIONS 10B(n, x), E=0.7-5.5 MeV; measured charged particles to discrete states using proportional ΔE and Si E detector and ToF; deduced σ, resonances; calculated σ using simple R-matrix. Compared with ENDF/B/VII. Preliminary. Further analysis in progress.

doi: 10.1016/j.nds.2014.08.030
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14663.


2014ME09      Nucl.Data Sheets 119, 373 (2014)

R.Meharchand, D.M.Asner, R.G.Baker, J.Bundgaard, E.Burgett, M.Cunningham, J.Deaven, D.L.Duke, U.Greife, S.Grimes, M.Heffner, T.Hill, D.Isenhower, J.L.Klay, V.Kleinrath, N.Kornilov, A.B.Laptev, W.Loveland, T.N.Massey, H.Qu, J.Ruz, S.Sangiorgio, B.Seilhan, L.Snyder, S.Stave, G.Tatishvili, R.T.Thornton, F.Tovesson, D.Towell, R.S.Towell, S.Watson, B.Wendt, L.Wood

Commissioning the NIFFTE Time Projection Chamber: Towards the 238U/235U(n, f) Cross-section Ratio

doi: 10.1016/j.nds.2014.08.103
Citations: PlumX Metrics


2014SN02      Nucl.Data Sheets 119, 386 (2014)

L.Snyder, D.M.Asner, R.G.Baker, J.Bundgaard, E.Burgett, M.Cunningham, J.Deaven, D.L.Duke, U.Greife, S.Grimes, M.Heffner, T.Hill, D.Isenhower, J.L.Klay, V.Kleinrath, N.Kornilov, A.B.Laptev, W.Loveland, T.N.Massey, R.Meharchand, H.Qu, J.Ruz, S.Sangiorgio, B.Seilhan, S.Stave, G.Tatishvili, R.T.Thornton, F.Tovesson, D.Towell, R.S.Towell, S.Watson, B.Wendt, L.Wood, for the NIFFTE Collaboration

Measuring the α/SF Branching Ratio of 252Cf with the NIFFTE TPC

doi: 10.1016/j.nds.2014.08.107
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2014ST15      Nucl.Data Sheets 119, 380 (2014)

S.Stave, D.M.Asner, R.G.Baker, J.Bundgaard, E.Burgett, M.Cunningham, J.Deaven, D.L.Duke, U.Greife, S.Grimes, M.Heffner, T.Hill, D.Isenhower, J.L.Klay, V.Kleinrath, N.Kornilov, A.B.Laptev, W.Loveland, T.N.Massey, R.Meharchand, H.Qu, J.Ruz, S.Sangiorgio, B.Seilhan, L.Snyder, G.Tatishvili, R.T.Thornton, F.Tovesson, D.Towell, R.S.Towell, S.Watson, B.Wendt, L.Wood, for the NIFFTE Collaboration

The Data Analysis Framework for the NIFFTE Fission Time Projection Chamber

doi: 10.1016/j.nds.2014.08.105
Citations: PlumX Metrics


2014VO07      Nucl.Data Sheets 119, 255 (2014)

A.V.Voinov, S.M.Grimes, C.R.Brune, A.Burger, A.Gorgen, M.Guttormsen, A.C.Larsen, T.N.Massey, S.Siem

Level Density Inputs in Nuclear Reaction Codes and the Role of the Spin Cutoff Parameter

NUCLEAR REACTIONS 57Fe(α, p), E=2-16 MeV; measured Ep, Ip(θ), Eα, Iα(θ) using ΔE-E Si telescope; deduced unnormalized σ; calculated σ using EMPIRE code with different level density models from RIPL-3 database.

doi: 10.1016/j.nds.2014.08.070
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2014WO02      Nucl.Data Sheets 119, 377 (2014)

L.Wood, D.M.Asner, R.G.Baker, J.Bundgaard, E.Burgett, M.Cunningham, J.Deaven, D.L.Duke, U.Greife, S.Grimes, M.Heffner, T.Hill, D.Isenhower, J.L.Klay, V.Kleinrath, N.Kornilov, A.B.Laptev, W.Loveland, T.N.Massey, R.Meharchand, H.Qu, J.Ruz, S.Sangiorgio, B.Seilhan, L.Snyder, S.Stave, G.Tatishvili, R.T.Thornton, F.Tovesson, D.Towell, R.S.Towell, S.Watson, B.Wendt, for the NIFFTE Collaboration

An Ethernet-based Data Acquisition System for the NIFFTE Time Projection Chamber

doi: 10.1016/j.nds.2014.08.104
Citations: PlumX Metrics


2013CO12      Nucl.Instrum.Methods Phys.Res. B305, 45 (2013)

K.W.Cooper, T.N.Massey, D.E.Carter, D.C.Ingram

Measurements of the 11B(d, nγ15.1)12C differential cross-section on thick and thin targets

NUCLEAR REACTIONS 11B(d, n), E<5 MeV; measured reaction products, Eγ, Iγ; deduced thin and thick target yields, σ(θ). Comparison with available data.

doi: 10.1016/j.nimb.2013.04.048
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1960.


2013RA32      Phys.Rev. C 88, 064324 (2013)

A.P.D.Ramirez, A.V.Voinov, S.M.Grimes, A.Schiller, C.R.Brune, T.N.Massey, A.Salas-Bacci

Nuclear level densities of 64, 66Zn from neutron evaporation

NUCLEAR REACTIONS 63Cu(d, n)64Zn, 65Cu(d, n)66Zn, E=6, 7.5 MeV; measured E(n), I(n), n(θ), σ(E, θ) using TOF technique at Edwards accelerator facility, Ohio University. Analysis by exciton model of nuclear reactions. Comparison with Hauser-Feshbach model calculations using EMPIRE and TALYS computer codes. Tested Fermi gas model, Gilber-Cameron model, and microscopic combinatorial approach with Hartree-Fock-Bogoliubov method (HFBM). 64,66Zn; deduced level densities versus the excitation energy.

doi: 10.1103/PhysRevC.88.064324
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2087.


2013VO12      Phys.Rev. C 88, 054607 (2013)

A.V.Voinov, S.M.Grimes, C.R.Brune, A.Burger, A.Gorgen, M.Guttormsen, A.C.Larsen, T.N.Massey, S.Siem

Experimental differential cross sections, level densities, and spin cutoffs as a testing ground for nuclear reaction codes

NUCLEAR REACTIONS 57Fe(α, p)60Co, 59Co(α, p)62Ni, E=21 MeV; 56Fe(7Li, p)62Ni, 55Mn(6Li, p)60Co, E=15 MeV; measured Ep, Ip, double-differential σ(θ); deduced spin cutoff parameter. Comparison with calculations using the EMPIRE reaction code, and different level density models. Excitation energy dependencies found to be inconsistent with the Fermi-gas model.

doi: 10.1103/PhysRevC.88.054607
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2349.


2012AD05      Phys.Rev. C 85, 037601 (2012)

A.S.Adekola, C.R.Brune, D.W.Bardayan, J.C.Blackmon, K.Y.Chae, J.A.Cizewski, K.L.Jones, R.L.Kozub, T.N.Massey, C.D.Nesaraja, S.D.Pain, J.F.Shriner, M.S.Smith, J.S.Thomas

19Ne levels studied with the 18F(d, n)19Ne*(18F+p) reaction

NUCLEAR REACTIONS 2H(18F, n), E=150 MeV; measured α and proton spectra from 19Ne breakup, p(18F)-, α(15O)-coin, angular distributions. 19Ne; deduced resonances, levels, proton widths, α widths, spectroscopic factors, decay branching ratios. DWBA analysis. Comparison with earlier studies. Relevance to destruction of long-lived 18F in novae.

doi: 10.1103/PhysRevC.85.037601
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2012AL11      Phys.Rev. C 86, 025801 (2012); Pub.Note. Phys.Rev. C 86, 029901 (2012)

S.Almaraz-Calderon, W.P.Tan, A.Aprahamian, B.Bucher, A.Roberts, M.Wiescher, C.R.Brune, T.N.Massey, N.Ozkan, R.T.Guray, H.Mach

Level structure of 18Ne and its importance in the 14O(α, p)17F reaction rate

NUCLEAR REACTIONS 16O(3He, n), E=15 MeV; measured neutron and charged particle spectra, (particle)n-coin, neutron time-of-flight spectrum, p(θ), branching ratios for proton, 2p and α decays of excited states. 18Ne; deduced levels, resonances, J, π, decay modes, widths. 14,16O, 17F; populated g.s. from p, 2p and α decays of 18Ne resonances, and first excited state in 17F from p decay of 18Ne resonances. 14O(α, p)17F, T=0.1-5 GK; calculated reaction rates of astrophysical interest for Hot CNO cycles and their breakout paths towards the rp process. Comparison with previous studies.

doi: 10.1103/PhysRevC.86.025801
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2012AL23      Phys.Rev. C 86, 065805 (2012); Erratum Phys.Rev. C 88, 059902 (2013)

S.Almaraz-Calderon, W.P.Tan, A.Aprahamian, M.Beard, G.P.A.Berg, B.Bucher, M.Couder, J.Gorres, S.O'Brien, D.Patel, A.Roberts, K.Sault, M.Wiescher, C.R.Brune, T.N.Massey, K.Fujita, K.Hatanaka, D.Ishiwaka, H.Matsubara, H.Okamura, H.J.Ong, Y.Sakemi, Y.Shimizu, T.Suzuki, Y.Tameshige, A.Tamii, J.Zenihiro, T.Kubo, Y.Namiki, Y.Ohkuma, Y.Shimbara, S.Suzuki, R.Watanabe, R.Yamada, T.Adachi, Y.Fujita, H.Fujita, M.Dozono, T.Wakasa

Level structure of 30S and its importance in the 26Si(α, p)29P and 29P(p, γ)30S reaction rates

NUCLEAR REACTIONS 32S(p, t), E=98.7 MeV; measured triton spectra at two angles using Grand Raiden (GR) magnetic spectrometer at RCNP facility. 28Si(3He, n), E=15 MeV; measured neutron (TOF) spectra, charged-particle spectra, (charged-particle)n-coin, angular distributions using LESA array and scintillation detectors at Notre Dame NSL facility. 30S; deduced levels, proton- and α- unbound levels, J, π, proton branching ratios, partial proton widths. DWBA analysis. Comparison with several previous experimental studies. 29P(p, γ)30S, 26Si(α, p)29P, T9=0.01-10 GK; deduced astrophysical reaction rates. Comparison with previous theoretical calculations. Contribution of resonances to total reaction rates.

doi: 10.1103/PhysRevC.86.065805
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2012SA44      Phys.Rev.Lett. 109, 142501 (2012)

D.B.Sayre, C.R.Brune, D.E.Carter, D.K.Jacobs, T.N.Massey, J.E.O'Donnell

E2 Interference Effects in the 12C(α, γ0)16O Reaction

NUCLEAR REACTIONS 12C(α, γ), E<4.5 MeV; measured reaction products, Eγ, Iγ; deduced g-ray yields, resonance parameters, E1-E2 asymmetry, S-factors. Comparison with available data.

doi: 10.1103/PhysRevLett.109.142501
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2011AD05      Phys.Rev. C 83, 052801 (2011)

A.S.Adekola, D.W.Bardayan, J.C.Blackmon, C.R.Brune, K.Y.Chae, C.Domizioli, U.Greife, Z.Heinen, M.J.Hornish, K.L.Jones, R.L.Kozub, R.J.Livesay, Z.Ma, T.N.Massey, B.Moazen, C.D.Nesaraja, S.D.Pain, J.F.Shriner Jr, N.D.Smith, M.S.Smith, J.S.Thomas, D.W.Visser, A.V.Voinov

First proton-transfer study of 18F + p resonances relevant for novae

NUCLEAR REACTIONS 2H(18F, n), E=150 MeV; measured α- and 15O-particle spectra. α(15O)-coin, σ(θ), DWBA analysis. 19Ne; deduced levels, J, π, L-transfers, resonances, proton and α-widths. 19Ne-19F mirror symmetry. 18F(p, α)15O; deduced reaction rates. Relevance to nova nucleosynthesis of 18F.

doi: 10.1103/PhysRevC.83.052801
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2011AD24      Phys.Rev. C 84, 054611 (2011)

A.S.Adekola, C.R.Brune, D.W.Bardayan, J.C.Blackmon, K.Y.Chae, C.Domizioli, U.Greife, Z.Heinen, M.J.Hornish, K.L.Jones, R.L.Kozub, R.J.Livesay, Z.Ma, T.N.Massey, B.Moazen, C.D.Nesaraja, S.D.Pain, J.F.Shriner, Jr., N.D.Smith, M.S.Smith, J.S.Thomas, D.W.Visser, A.V.Voinov

Single-nucleon transfer reactions on 18F

NUCLEAR REACTIONS 2H(18F, n)19Ne, (18F, p)19F, [secondary 18F beam from 16O(α, np)18F, E=85 MeV primary reaction], E=150 MeV; measured particle spectra, (15O)α-, (15N)α-coin, σ(θ), proton. 19F, 19Ne; deduced levels, J, π, l-values, spectroscopic factors, proton widths, asymptotic normalization coefficients, isospin mirror levels. DWBA analysis of σ(θ) data. Monte-Carlo simulations. Comparison with previous studies.

doi: 10.1103/PhysRevC.84.054611
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2011KO47      J.Korean Phys.Soc. 59, 1404s (2011)

N.V.Kornilov, T.Massey, S.Grimes

Evaluation of the Experimental np-Angular Distribution at 14.1 MeV Neutron Energy

NUCLEAR REACTIONS 1H(n, n'), E=14.1 MeV; reanalyzed, re-evaluated σ(θ). Comparison with data, ENDF/B-VII.

doi: 10.3938/jkps.59.1404
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2011VO06      Phys.Rev. C 83, 054605 (2011)

A.V.Voinov, S.M.Grimes, C.R.Brune, A.Burger, A.Gorgen, M.Guttormsen, A.C.Larsen, T.N.Massey, S.Siem, C.Kalbach

Equilibrium and pre-equilibrium processes in the 55Mn(6Li, x p) and 57Fe(α, x p) reactions

NUCLEAR REACTIONS 55Mn(6Li, xp), (6Li, xn), E=15 MeV; 57Fe(α, xp), E=30 MeV; measured neutron, proton and scattered α-particle spectra, cross sections, angular distributions. Comparison with calculations performed using the exciton pre-equilibrium model and Hauser-Feshbach evaporation model.

doi: 10.1103/PhysRevC.83.054605
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2010BO07      Phys.Rev. C 82, 014001 (2010)

N.Boukharouba, F.B.Bateman, A.D.Carlson, C.E.Brient, S.M.Grimes, T.N.Massey, R.C.Haight, D.E.Carter

Measurement of the n-p elastic scattering angular distribution at En=14.9 MeV

NUCLEAR REACTIONS 1H(n, n), E=14.9 MeV; measured Ep, Ip, σ, σ(θ). Comparison with predictions of phase-shift analysis and the ENDF/B-VII.0 evaluation.

doi: 10.1103/PhysRevC.82.014001
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2010TA17      Nucl.Phys. A834, 679c (2010)

W.P.Tan, S.Almaraz, A.Aprahamian, B.Bucher, J.Gorres, H.Mach, M.Wiescher, C.Brune, Z.Heinen, T.Massey

α-Induced Reaction Rates for Accreting Compact Stars

NUCLEAR REACTIONS 16O, 28Si(3He, n), E=15 MeV; measured ToF neutron σ(E). 18Ne, 30S; deduced energies of levels.

doi: 10.1016/j.nuclphysa.2010.01.123
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2010VO01      Phys.Rev. C 81, 024319 (2010)

A.Voinov, S.M.Grimes, C.R.Brune, M.Guttormsen, A.C.Larsen, T.N.Massey, A.Schiller, S.Siem

γ-strength functions in 60Ni from two-step cascades following proton capture

NUCLEAR REACTIONS 59Co(p, 2γ), E=1.85 MeV; measured Eγ; analyzed two-step γ cascades populating 2+ state; deduced E1 and M1 γ-strength functions. Comparison with other studies.

doi: 10.1103/PhysRevC.81.024319
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2009OG06      Phys.Rev. C 80, 034305 (2009)

B.M.Oginni, S.M.Grimes, A.V.Voinov, A.S.Adekola, C.R.Brune, D.E.Carter, Z.Heinen, D.Jacobs, T.N.Massey, J.E.O'Donnell, A.Schiller

Test of level density models from reactions of 6Li on 58Fe and 7Li on 57Fe

NUCLEAR REACTIONS 58Fe(6Li, X), E=15 MeV; 57Fe(7Li, X), E=15 MeV; measured particle spectra, σ, angular distributions; deduced optical model parameters. 60Co, 63Ni; deduced level densities. Comparison with Hauser-Feshbach model calculations.

doi: 10.1103/PhysRevC.80.034305
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2009VO02      Phys.Rev. C 79, 031301 (2009)

A.V.Voinov, B.M.Oginni, S.M.Grimes, C.R.Brune, M.Guttormsen, A.C.Larsen, T.N.Massey, A.Schiller, S.Siem

Nuclear excitations at constant temperature

NUCLEAR REACTIONS 55Mn(6Li, X), (7Li, X), E=15 MeV; 59Co(d, p), (d, α), E=7.5 MeV; measured neutron and proton evaporation spectra, α spectra, σ. Hauser-Feshbach analysis. Comparison with predictions of constant temperature, Fermi-gas, and Hartree-Fock-BCS models.

doi: 10.1103/PhysRevC.79.031301
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2008BO37      Int.J.Mod.Phys. E17, 2067 (2008)

H.G.Bohlen, W.Von Oertzen, Tz.Kokalova, Ch.Schulz, R.Kalpakchieva, T.N.Massey, M.Milin

Band structures in 12Be: Experimental results

NUCLEAR REACTIONS 14C(12C, 14O), 10Be(14N, 12N), 9Be(12C, 9C), (15N, 12N), E=231, 216, 231, 240 MeV; measured reaction products; deduced 12Be energy levels, J, π.

doi: 10.1142/S0218301308011100
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2008DI10      Nucl.Sci.Eng. 159, 346 (2008)

A.R.Di Lullo, T.N.Massey, S.M.Grimes, D.E.Carter, J.E.O'Donnell, D.Jacobs

A Fission Chamber Measurement of the natB(d, n) Cross Section for Use in Neutron Detector Calibration

NUCLEAR REACTIONS B(d, n), E=7.5 MeV; 235U(n, F), E=0.9-19.6 MeV;measured neutron spectra, σ. Fission chamber, Calibration of neutron detector

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2008HA27      Phys.Rev. C 78, 014319 (2008)

P.J.Haigh, N.I.Ashwood, T.Bloxham, N.Curtis, M.Freer, P.McEwan, D.Price, V.Ziman, H.G.Bohlen, Tz.Kokalova, Ch.Schulz, R.Torabi, W.von Oertzen, C.Wheldon, W.Catford, C.Harlin, R.Kalpakchieva, T.N.Massey

Measurement of α and neutron decay widths of excited states of 14C

NUCLEAR REACTIONS 12C(16O, 14O), E=234 MeV; measured charged particle spectra. 14C; deduced levels, J, π, configurations, widths of excited states. 7Li(9Be, 14C);14C(13C, 14C), (14C, 14C); 9Be(7Li, d); 13C(polarized p, π+), (n, n); comparison of levels.

RADIOACTIVITY 14C(n)(α); measured partial decay widths. 10Be, 13C; deduced levels, J, π, angular distributions, configurations. Comparison with model calculations.

doi: 10.1103/PhysRevC.78.014319
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2008MA51      Phys.Rev. C 78, 065801 (2008)

C.Matei, C.R.Brune, T.N.Massey

Measurements of branching ratios from the 7.12-MeV state in 16O and the 12C(α, γ)16O reaction cross section

NUCLEAR REACTIONS 19F(p, αγ), E≈2 MeV; measured Eγ, Iγ, γγ coin, angular distributions. 12C(α, γ)16O; analyzed widths, S-factor, Asymptotic Normalization Coefficient.

doi: 10.1103/PhysRevC.78.065801
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2008VO02      Phys.Rev. C 77, 034613 (2008)

A.V.Voinov, S.M.Grimes, A.C.Larsen, C.R.Brune, M.Guttormsen, T.Massey, A.Schiller, S.Siem, N.U.H.Syed

Level densities of 44Sc and 47Ti from different experimental techniques

NUCLEAR REACTIONS 45Sc(3He, α), (3He, p), E=11 Mev; measured Eγ, Iγ, particle spectra, α particle angular distributions; deduced level density, αγ-coin. 44Sc, 47Ti; deduced level density. Comparison with theory.

doi: 10.1103/PhysRevC.77.034613
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2007AL49      Phys.Atomic Nuclei 70, 1634 (2007)

E.Algin, A.Schiller, A.Voinov, U.Agvaanluvsan, T.Belgya, L.A.Bernstein, C.R.Brune, R.Chankova, P.E.Garrett, S.M.Grimes, M.Guttormsen, M.Hjorth-Jensen, M.J.Hornish, C.W.Johnson, T.Massey, G.E.Mitchell, J.Rekstad, S.Siem, W.Younes

Bulk properties of iron isotopes

NUCLEAR REACTIONS 57Fe(3He, α), (3He, 3He'), E=45 MeV; 56Fe(n, γ), E=thermal; 55Mn(d, n), E=7.0 MeV; measured Eγ, Iγ. Deduced nuclear level densities and radiative strength functions. Compared results to model calculations.

doi: 10.1134/S1063778807090232
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2007BO10      Eur.Phys.J. A 31, 279 (2007)

H.G.Bohlen, R.Kalpakchieva, W.von Oertzen, T.N.Massey, A.A.Ogloblin, G.de Angelis, M.Milin, Ch.Schulz, Tz.Kokalova, C.Wheldon

Spectroscopy of 17C and (sd)3 structures in heavy carbon isotopes

NUCLEAR REACTIONS 12,14C(12C, 9C), E=231 MeV; measured particle spectra, σ(E, θ). 15,17C deduced levels, J, π, configurations.

NUCLEAR STRUCTURE 15,16,17C, 19O; calculated levels, J, π. Shell model.

doi: 10.1140/epja/i2006-10275-5
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2007VO08      Phys.Rev. C 76, 044602 (2007)

A.V.Voinov, S.M.Grimes, C.R.Brune, M.J.Hornish, T.N.Massey, A.Salas

Test of nuclear level density inputs for Hauser-Feshbach model calculations

NUCLEAR REACTIONS 59Co(d, n), (d, p), (d, α), 58Fe(3He, n), (3He, p), (3He, α)61Ni, E=7.5, 10 MeV; measured neutron, proton and α particle spectra, reaction cross sections. 57Fe, 60Ni, 60Cu; deduced level densities.

doi: 10.1103/PhysRevC.76.044602
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2006VO06      Phys.Rev. C 74, 014314 (2006)

A.V.Voinov, S.M.Grimes, U.Agvaanluvsan, E.Algin, T.Belgya, C.R.Brune, M.Guttormsen, M.J.Hornish, T.Massey, G.E.Mitchell, J.Rekstad, A.Schiller, S.Siem

Level density of 56Fe and low-energy enhancement of γ-strength function

NUCLEAR REACTIONS 55Mn(d, n), E=7 MeV; measured En, σ(E, θ). 56Fe deduced level density, γ-strength function.

doi: 10.1103/PhysRevC.74.014314
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2005BO39      J.Phys.(London) G31, S1461 (2005)

H.G.Bohlen, R.Kalpakchieva, W.von Oertzen, T.N.Massey, A.A.Ogloblin, G.de Angelis, Ch.Schulz, Tz.Kokalova, C.Wheldon

Structure studies of excited states of 17C and 16C

NUCLEAR REACTIONS 13,14C(12C, 9C), E=231 MeV; measured excitation energy spectra. 16,17C deduced levels, J, π, configurations.

doi: 10.1088/0954-3899/31/10/014
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2005MC12      J.Phys.(London) G31, S1921 (2005)

P.McEwan, M.Freer, N.Ashwood, N.Curtis, D.Price, V.Ziman, H.G.Bohlen, Tz.Kokalova, Ch.Schulz, R.Torabi, W.von Oertzen, C.Wheldon, T.N.Massey, R.Kalpakchieva, W.Catford

Investigation into the structure of 14C using recoil co-incidence techniques

NUCLEAR REACTIONS 12C(16O, 14O), E not given; measured excitation energy spectra. 14C deduced decay branch widths.

doi: 10.1088/0954-3899/31/10/102
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2005PA50      Phys.Rev. C 72, 025802 (2005)

Y.Parpottas, S.M.Grimes, S.Al-Quraishi, C.R.Brune, T.N.Massey, J.E.O'Donnell, J.E.Oldendick, A.Salas, R.T.Wheeler

The 17F(p, γ)18Ne3+ resonance state studied with the 16O(3He, n)18Ne reaction

NUCLEAR REACTIONS 16O(3He, n), E=9.9-10.4 MeV; measured neutron spectra, σ(θ). 18Ne deduced resonance energy, width. Comparison with previous results.

doi: 10.1103/PhysRevC.72.025802
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2005WH05      Eur.Phys.J. A 26, 321 (2005)

C.Wheldon, Tz.Kokalova, W.von Oertzen, S.Thummerer, H.G.Bohlen, B.Gebauer, A.Tumino, T.N.Massey, G.de Angelis, M.Axiotis, A.Gadea, Th.Kroll, N.Marginean, D.R.Napoli, M.De Poli, C.Ur, D.Bazzacco, S.M.Lenzi, C.Rossi Alvarez, S.Lunardi, R.Menegazzo, P.G.Bizzeti, A.M.Bizzeti-Sona

Octupole-deformed molecular bands in 21Ne

NUCLEAR REACTIONS 16O(7Li, np), E=29.4 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-coin. 21Ne deduced levels, J, π, configurations, dipole moment. GASP, ISIS arrays.

doi: 10.1140/epja/i2005-10186-y
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2004BO12      Nucl.Phys. A734, 345 (2004)

H.G.Bohlen, R.Kalpakchieva, W.von Oertzen, T.N.Massey, B.Gebauer, S.M.Grimes, T.Kokalova, A.Lenz, M.Milin, Ch.Schulz, S.Thummerer, S.Torilov, A.Tumino

Particle-hole structures of neutron-rich Be- and C-isotopes

NUCLEAR REACTIONS 9Be(16O, 14O), E=233.5 MeV; 13C(12C, 14O), E not given; 13C(12C, 9C), E=230.7 MeV; measured σ(E, θ). 11Be, 16C deduced levels, J, π, configurations.

doi: 10.1016/j.nuclphysa.2004.01.063
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2004BO23      Nucl.Phys. A738, 333 (2004)

H.G.Bohlen, R.Kalpakchieva, W.von Oertzen, T.N.Massey, B.Gebauer, T.Kokalova, A.A.Ogloblin, Ch.Schulz, S.Thummerer

Structure of neutron-rich Beryllium and Carbon isotopes

NUCLEAR REACTIONS 9Be, 13,14C(12C, 9C), E=231 MeV; measured excitation energy spectra. 12Be, 16,17C deduced levels, J, π.

doi: 10.1016/j.nuclphysa.2004.04.056
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2004PA42      Phys.Rev. C 70, 065805 (2004); Erratum Phys.Rev. C 73, 049907 (2006)

Y.Parpottas, S.M.Grimes, S.Al-Quraishi, C.R.Brune, T.N.Massey, J.E.Oldendick, A.Salas, R.T.Wheeler

Astrophysically important 26Si states studied with the (3He, n) reaction and the 25Al(p, γ)26Si reaction rates in explosive hydrogen burning environments

NUCLEAR REACTIONS 24Mg(3He, n), E=7.9, 8.11, 10.0 MeV; measured En, σ(θ). 26Si deduced levels, J, π. 25Al(p, γ), E=low; calculated astrophysical reaction rates.

doi: 10.1103/PhysRevC.70.065805
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2004SA40      Phys.Rev. C 70, 024311 (2004)

A.Salas-Bacci, S.M.Grimes, T.N.Massey, Y.Parpottas, R.T.Wheeler, J.E.Oldendick

Level widths and level densities in 28Si, 46Ti, 52Cr, and 60Ni from Ericson fluctuations

NUCLEAR REACTIONS 27Al(p, n), E=7.4 MeV; 45Sc(p, n), E=5.2 MeV; 51V(p, n), E=3.1 MeV; 59Co(p, n), E=3.4 MeV; measured En, σ(E, θ). 28Si, 46Ti, 52Cr, 60Ni deduced level widths, level density parameters.

doi: 10.1103/PhysRevC.70.024311
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2004VO10      Eur.Phys.J. A 21, 193 (2004)

W.von Oertzen, H.G.Bohlen, M.Milin, Tz.Kokalova, S.Thummerer, A.Tumino, R.Kalpakchieva, T.N.Massey, Y.Eisermann, G.Graw, T.Faestermann, R.Hertenberger, H.-F.Wirth

Search for cluster structure of excited states in 14C

NUCLEAR REACTIONS 12C(16O, 14O), (14N, 12N), (15N, 13N), E ≈ 15 MeV/nucleon; 16O(15N, 17N), E=16 MeV/nucleon; 8Be(7Li, d), E=44 MeV; measured particle spectra. 14C deduced levels, J, π, configurations, deformation, rotational bands, α-cluster features. Other data analyzed.

doi: 10.1140/epja/i2003-10188-9
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2003AL03      Phys.Rev. C 67, 015803 (2003)

S.I.Al-Quraishi, S.M.Grimes, T.N.Massey, D.A.Resler

Level densities for 20≤A≤110

NUCLEAR STRUCTURE 30P, 56Ni, 91Mo, 100Pd, 106Sn; A=20-110; analyzed level densities; deduced Z, N dependence features. Comparison with earlier analysis.

doi: 10.1103/PhysRevC.67.015803
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2003BO24      Yad.Fiz. 66, 1539 (2003); Phys.Atomic Nuclei 66, 1494 (2003)

H.G.Bohlen, W.von Oertzen, R.Kalpakchieva, B.Gebauer, S.M.Grimes, A.Lenz, T.N.Massey, M.Milin, Ch.Schulz, Tz.Kokalova, S.Torilov, S.Thummerer

Structure of Neutron-Rich Be and C Isotopes

NUCLEAR REACTIONS 9,10Be(14N, 13N), E=217.9 MeV; 9Be(13C, 11C), E=379 MeV; 9Be(15N, 12N), E=240 MeV; 10Be(14N, 12N), E=216 MeV; 12,13C(12C, 9C), E=230.7 MeV; measured excitation energy spectra. 9Be(16O, 14O), E=233.5 MeV; 13C(12C, 14O), E=230.7 MeV; measured σ(θ). 10,11,12Be deduced levels, J, π, configurations, rotational bands. 15,16C deduced level energies, widths, configurations.

doi: 10.1134/1.1601755
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2003BO38      Nucl.Phys. A722, 3c (2003)

H.G.Bohlen, R.Kalpakchieva, W.von Oertzen, T.N.Massey, B.Gebauer, S.M.Grimes, T.Kokalova, H.Lenske, A.Lenz, M.Milin, Ch.Schulz, S.Thummerer, S.Torilov, A.Tumino

Structure studies of neutron-rich Beryllium and Carbon isotopes

NUCLEAR REACTIONS 9Be(14N, 13N), E=217.9 MeV; 9Be(15N, 12N), E=240 MeV; 9Be(13C, 11C), E=379 MeV; 13C(12C, 9C), E=230.7 MeV; measured particle spectra, σ(E, θ). 10,11,12Be, 16C; deduced levels, J, π.

doi: 10.1016/S0375-9474(03)01327-7
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2003BO41      Phys.Rev. C 68, 054606 (2003)

H.G.Bohlen, R.Kalpakchieva, B.Gebauer, S.M.Grimes, H.Lenske, K.P.Lieb, T.N.Massey, M.Milin, W.von Oertzen, Ch.Schulz, T.Kokalova, S.Torilov, S.Thummerer

Spectroscopy of particle-hole states of 16C

NUCLEAR REACTIONS 12,13C(12C, 9C), E=230.7 MeV; measured particle spectra, σ(θ). 15,16C deduced levels, J, π, configurations.

doi: 10.1103/PhysRevC.68.054606
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2003BO50      Acta Phys.Hung.N.S. 18, 179 (2003)

H.G.Bohlen, W.von Oertzen, R.Kalpakchieva, B.Gebauer, S.M.Grimes, T.N.Massey, H.Lenske, A.Lenz, M.Milin, Ch.Schulz, T.Kokalova, S.Torilov, S.Thummerer

Structure Studies of Neutron-Rich Beryllium and Carbon Isotopes

NUCLEAR REACTIONS 9Be(13C, 11C), E=379 MeV; 9Be(14N, 13N), E=217.9 MeV; 9Be(15N, 12N), E=240 MeV; measured particle spectra. 10,11,12Be deduced rotational bands. 9Be(16O, 14O), E=233.5 MeV; 13C(12C, 14O), E=230.7 MeV; measured σ(E, θ). 11Be deduced levels, J, π. 13C(12C, 9C), E=230.7 MeV; measured particle spectra. 16C deduced levels. Quasiparticle RPA calculations.

doi: 10.1556/APH.18.2003.2-4.10
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2003FI06      Nucl.Instrum.Methods Phys.Res. A505, 5 (2003)

C.L.Fink, D.L.Smith, B.J.Micklich, T.N.Massey

Gamma rays produced by 1.75- to 4-MeV proton bombardment of thick aluminum targets

NUCLEAR REACTIONS 27Al(p, p'), (p, α), (p, γ), E=1.75-4 MeV; measured Eγ, thick-target γ-ray yields.

doi: 10.1016/S0168-9002(03)01007-6
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2003MI10      Nucl.Instrum.Methods Phys.Res. A505, 1 (2003)

B.J.Micklich, D.L.Smith, T.N.Massey, C.L.Fink, D.Ingram

Measurement of thick-target high-energy γ-ray yields from the 19F(p, αγ)16O reaction

NUCLEAR REACTIONS 19F(p, α), E=1.5-4.25 MeV; measured Eγ, thick-target γ-ray yields.

doi: 10.1016/S0168-9002(03)01006-4
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2003TH01      J.Phys.(London) G29, 509 (2003)

S.Thummerer, W.von Oertzen, Tz.Kokalova, H.G.Bohlen, B.Gebauer, A.Tumino, T.N.Massey, G.de Angelis, M.Axiotis, A.Gadea, Th.Kroll, N.Marginean, D.R.Napoli, M.De Poli, C.Ur, D.Bazzacco, S.M.Lenzi, C.R.Alvarez, S.Lunardi, R.Menegazzo, P.G.Bizzeti, A.M.Bizzeti-Sona

Gamma-decay study of 21Na and 21Ne, octupole bands in 21Ne

NUCLEAR REACTIONS 16O(7Li, 2n), (7Li, np), E=27 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-coin. 21Ne, 21Na deduced levels, J, π, configurations, Coulomb energy differences. GASP, ISIS arrays.

doi: 10.1088/0954-3899/29/3/305
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2003TH04      Yad.Fiz. 66, 1474 (2003); Phys.Atomic Nuclei 66, 1428 (2003)

S.Thummerer, W.von Oertzen, Tz.Kokalova, H.G.Bohlen, B.Gebauer, A.Tumino, T.N.Massey, G.de Angelis, M.Axiotis, A.Gadea, Th.Kroll, N.Marginean, D.R.Napoli, M.De Poli, C.Ur, D.Bazzacco, S.M.Lenzi, C.Rossi Alvarez, S.Lunardi, R.Menegazzo, P.G.Bizzeti, A.M.Bizzeti-Sona

A Study of γ Decays and Octupole Bands in 21Ne and 21Na

NUCLEAR REACTIONS 16O(7Li, 2n), (7Li, np), E=27 MeV; measured Eγ, Iγ, γγ-coin. 21Ne, 21Na deduced levels, J, π, rotational bands. GASP array.

doi: 10.1134/1.1601745
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2002BO01      Phys.Rev. C65, 014004 (2002); Erratum Phys.Rev. C 82, 039901 (2010)

N.Boukharouba, F.B.Bateman, C.E.Brient, A.D.Carlson, S.M.Grimes, R.C.Haight, T.N.Massey, O.A.Wasson

Measurement of the n-p Elastic Scattering Angular Distribution at En = 10 MeV

NUCLEAR REACTIONS 1H(n, p), E=10 MeV; measured reaction products, Ep, Ip; deduced σ(θ). Comparison with ENDF/B-V, ENDF/B-VI evaluated nuclear libraries, experimental data.

doi: 10.1103/PhysRevC.65.014004
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2002BO16      Yad.Fiz. 65, 635 (2002); Phys.Atomic Nuclei 65, 603 (2002)

H.G.Bohlen, W.von Oertzen, A.Blazevic, B.Gebauer, S.M.Grimes, R.Kalpakchieva, T.N.Massey, S.Thummerer

Structure Studies of 11Be and 12Be: Observation of molecular rotational bands

NUCLEAR REACTIONS 9Be(14N, 12N), E=217.9 MeV; 9Be(13C, 11C), E=379 MeV; 9Be(15N, 13N), E=240 MeV; 12C(14C, 14O), E=336 MeV; 9Be(15N, 12N), E not given; measured excitation energy spectra. 11,12Be deduced level energies, possible J, π, rotational band features.

doi: 10.1134/1.1471258
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2001AL20      Phys.Rev. C63, 065803 (2001)

S.I.Al-Quraishi, S.M.Grimes, T.N.Massey, D.A.Resler

Are the Level Densities for r- and rp-Process Nuclei Different from Nearby Nuclei in the Valley of Stability ?

NUCLEAR STRUCTURE A=20-70; analyzed level densities parameters; deduced N and Z dependence.

doi: 10.1103/PhysRevC.63.065803
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2001BO35      Phys.Rev. C64, 024312 (2001)

H.G.Bohlen, R.Kalpakchieva, A.Blazevic, B.Gebauer, T.N.Massey, W.von Oertzen, S.Thummerer

Spectroscopy of 7He States using the (15N, 17F) Reaction on 9Be

NUCLEAR REACTIONS 9Be, 12C, 16O(15N, 17F), E=240, 318.5 MeV; measured particle spectra, angular distributions. 7He deduced levels, J, π, resonance parameters. 10Be deduced levels, J, π.

doi: 10.1103/PhysRevC.64.024312
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1677.


2001HO13      Nucl.Sci.Eng. 138, 145 (2001)

W.B.Howard, S.M.Grimes, T.N.Massey, S.I.Al-Quraishi, D.K.Jacobs, C.E.Brient, J.C.Yanch

Measurement of the Thick-Target 9Be(p, n) Neutron Energy Spectra

NUCLEAR REACTIONS 9Be(p, n), E=3.0, 3.4, 3.7, 4.0, 5.0 MeV; measured thick-target neutron spectra, angular distributions. Comparison with previous results, model predictions.

doi: 10.13182/NSE01-A2206
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0838.


2000AL35      Phys.Rev. C62, 044616 (2000)

S.I.Al-Quraishi, C.E.Brient, S.M.Grimes, T.N.Massey, J.Oldendick, R.Wheeler

Low Energy Deuteron-Induced Reactions on 27Al and 56Fe

NUCLEAR REACTIONS 27Al, 56Fe(d, d), (d, d'), (d, p), (d, α), (d, n), E=5, 7 MeV; measured particle spectra, σ(E, θ); deduced optical model parameters, reaction mechanism features.

doi: 10.1103/PhysRevC.62.044616
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2000FE10      Nucl.Instrum.Methods Phys.Res. A450, 353 (2000)

A.Fessler, T.N.Massey, B.J.Micklich, D.L.Smith

Thick Target Photon Yields and Angular Distributions for the 19F(p, αγ)16O Source Reaction at Incident Proton Energies between 1.5 and 4.0 MeV

NUCLEAR REACTIONS 19F(p, α), E=1.5-4.0 MeV; measured Eγ, Iγ, thick target photon yields, angular distributions. Monte Carlo calculations for detector response function.

doi: 10.1016/S0168-9002(00)00303-X
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2000HU10      Phys.Rev. C62, 024002 (2000); Erratum Phys.Rev. C64, 019902 (2001)

P.-L.Huang, S.M.Grimes, T.N.Massey

Level Densities for Nuclei with 20 ≤ A ≤ 41

NUCLEAR STRUCTURE 24Na, 24,25Mg, 25,28Al, 28,29Si, 29P, 36Cl, 36,37Ar, 37K; analyzed level densities; deduced parameters.

doi: 10.1103/PhysRevC.62.024002
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2000KA21      Eur.Phys.J. A 7, 451 (2000)

R.Kalpakchieva, H.G.Bohlen, W.von Oertzen, B.Gebauer, M.von Lucke-Petsch, T.N.Massey, A.N.Ostrowski, Th.Stolla, M.Wilpert, Th.Wilpert

Spectroscopy of 13B, 14B, 15B and 16B using Multi-Nucleon Transfer Reactions

NUCLEAR REACTIONS 12,13,14C(14C, 12N), E ≈ 335 MeV; 12C(14C, 13N), (13C, 12N), E ≈ 335 MeV; 12C(15N, 14O), E=240 MeV; 16O(14C, 17F), E=334 MeV; measured excitation energy spectra, σ(θ). 13,16B deduced excited states. 14,15B deduced levels, J, π. 16B deduced mass excess.

doi: 10.1007/PL00013641
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1999BO26      Prog.Part.Nucl.Phys. 42, 17 (1999)

H.G.Bohlen, A.Blazevic, B.Gebauer, W.von Oertzen, S.Thummerer, R.Kalpakchieva, S.M.Grimes, T.N.Massey

Spectroscopy of Exotic Nuclei with Multi-Nucleon Transfer Reactions

NUCLEAR REACTIONS 9Be(15N, 17F), E=240 MeV; 9,10Be(14C, 14O), E ≈ 335 MeV; 10Be(12C, 14O), (12C, 12N), E=357 MeV; 12C(12C, 12N), E=357 MeV; 9Be, 12C(13C, 13N), E=379 MeV; 9Be(13C, 12N), E=336 MeV; measured residual nuclei spectra. 7,8,9,10He deduced levels, possible J, π. 10Li deduced levels, J, π, configurations. 11Be deduced molecular rotational band.

doi: 10.1016/S0146-6410(99)00056-3
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1998BO38      Nuovo Cim. 111A, 841 (1998)

H.G.Bohlen, W.von Oertzen, R.Kalpakchieva, A.Blazevic, B.Gebauer, S.M.Grimes, A.Lepine-Szily, T.N.Massey, W.Mittig, A.N.Ostrowski, J.M.Oliveira, P.Roussel-Chomaz, S.Thummerer, M.Wilpert

Nuclear Structure Studies of Bound and Unbound States in Drip-Line Nuclei

NUCLEAR REACTIONS 9Be(15N, 17F), (15N, 14O), E=240 MeV; 10Be(12C, 12N), E=357 MeV; 9Be(13C, 12N), E=336.4 MeV; 9Be(13C, 11C), E=379 MeV; 12C(14N, 15C), E=426 MeV; measured particle spectra. 7He, 10Li, 11N deduced resonances, J, π. 11Be deduced molecular rotational band.


1998MA96      Nucl.Sci.Eng. 129, 175 (1998)

T.N.Massey, S.Al-Quraishi, C.E.Brient, J.F.Guillemette, S.M.Grimes, D.Jacobs, J.E.O'Donnell, J.Oldendick, R.Wheeler

A Measurement of the 27Al(d, n) Spectrum for Use in Neutron Detector Calibration

NUCLEAR REACTIONS 27Al(d, n), E=7.44 MeV; measured neutron spectra. Application to detector calibration.

doi: 10.13182/NSE98-A1971
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1997BA01      Phys.Rev. C55, 133 (1997)

F.B.Bateman, S.M.Grimes, N.Boukharouba, V.Mishra, C.E.Brient, R.S.Pedroni, T.N.Massey, R.C.Haight

Determination of the 29Si Level Density from 3 to 22 MeV

NUCLEAR REACTIONS 27Al(d, n), E=2-6 MeV; measured neutron spectra, σ(θ) vs E. 28Si(n, p), E=5.52-12.97 MeV; measured σ(θ) vs E. 28Si(n, α), E=9.02 MeV; measured spectra. 29Si deduced level density. Three different data analysis techniques.

doi: 10.1103/PhysRevC.55.133
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1997BO10      Nucl.Phys. A616, 254c (1997)

H.G.Bohlen, W.von Oertzen, Th.Stolla, R.Kalpakchieva, B.Gebauer, M.Wilpert, Th.Wilpert, A.N.Ostrowski, S.M.Grimes, T.N.Massey

Study of Weakly Bound and Unbound States of Exotic Nuclei with Binary Reactions

NUCLEAR REACTIONS 10Be(12C, 12N), E=357 MeV; 9Be(13C, 12N), E=336.4 MeV; measured spectra. 10Li deduced resonance.

doi: 10.1016/S0375-9474(97)00096-1
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1996ST29      Z.Phys. A356, 233 (1996)

Th.Stolla, H.G.Bohlen, B.Gebauer, S.M.Grimes, R.Kalpakchieva, T.N.Massey, W.von Oertzen, A.N.Ostrowski, M.Wilpert, Th.Wilpert

Spectroscopy of Excited States of 8He

NUCLEAR REACTIONS 10Be(12C, 14O), E=357 MeV; 12C, 16O(12C, 14O), E=357 MeV; measured ejectile energy spectra. 8He deduced levels, Γ

doi: 10.1007/BF02769222
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1995BO10      Nucl.Phys. A583, 775c (1995)

H.G.Bohlen, B.Gebauer, Th.Kirchner, M.von Lucke-Petsch, W.von Oertzen, A.N.Ostrowski, Ch.Seyfert, Th.Stolla, M.Wilpert, Th.Wilpert, S.M.Grimes, T.N.Massey, R.Kalpakchieva, Y.E.Penionzhkevich, D.V.Alexandrov, I.Mukha, A.A.Ogloblin, C.Detraz

Study of Light Neutron-Rich Nuclei with 14C-Induced Reactions

NUCLEAR REACTIONS 2H, 6Li(14C, 13N), E=336 MeV; 10Be, 12,14C, 16O(14C, 14O), 14C(14C, 12N), E=336 MeV; measured particle spectra, σ(θ) in some cases. 10He deduced resonances, possible J, π, Γ. 14Be, 16B deduced levels.

doi: 10.1016/0375-9474(94)00757-E
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1995BO15      Z.Phys. A351, 7 (1995)

H.G.Bohlen, R.Kalpakchieva, D.V.Aleksandrov, B.Gebauer, S.M.Grimes, T.Kirchner, M.von Lucke-Petsch, T.N.Massey, I.Mukha, W.von Oertzen, A.A.Ogloblin, A.N.Ostrowski, C.Seyfert, T.Stolla, M.Wilpert, T.Wilpert

Spectroscopy of Excited States of 11Li

NUCLEAR REACTIONS 10Be(14C, 13N), E=334.4 MeV; 14C(14C, 17F), E=335.6 MeV; measured spectra. 11Li deduced resonances energy, Γ.

doi: 10.1007/BF01292778
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1995GR01      Phys.Rev. C51, 606 (1995)

S.M.Grimes, T.N.Massey

New Expansion Technique for Spectral Distribution Calculations

doi: 10.1103/PhysRevC.51.606
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1995GR26      Nucl.Instrum.Methods Phys.Res. B99, 678 (1995)

S.M.Grimes, T.Covell, D.Jacobs, H.Zhou, F.B.Bateman, C.E.Brient, T.N.Massey

High Accuracy Determination of Neutron Energies from 300 keV to 5 MeV

NUCLEAR REACTIONS 57Fe(p, n), E=8.7 MeV; K, Br(p, n), E=3.4 MeV; measured neutron spectra. High accuracy tof spectrometer plus electrostatic accelerator system.

doi: 10.1016/0168-583X(94)00676-8
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1995VO05      Nucl.Phys. A588, 129c (1995)

W.von Oertzen, H.G.Bohlen, B.Gebauer, M.von Lucke-Petsch, A.N.Ostrowski, Ch.Seyfert, Th.Stolla, M.Wilpert, Th.Wilpert, D.V.Alexandrov, A.A.Korsheninnikov, I.Mukha, A.A.Ogloblin, R.Kalpakchieva, Y.E.Penionzhkevich, S.Piskor, S.M.Grimes, T.N.Massey

Nuclear Structure Studies of Very Neutron-Rich Isotopes of 7-10He, 9-11Li and 12-14Be Via Two-Body Reactions

NUCLEAR REACTIONS 6Li(14C, 13N), 12,14C(14C, 14O), (14C, 17F), E=335.9 MeV; 9Be(13C, 14O), (14C, 14O), E=337 MeV; 10Be(14C, 14O), (14C, 13N), E=334.4 MeV; measured residual nucleus spectra.

doi: 10.1016/0375-9474(95)00111-D
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1994OS04      Phys.Lett. 338B, 13 (1994)

A.N.Ostrowski, H.G.Bohlen, B.Gebauer, S.M.Grimes, R.Kalpakchieva, Th.Kirchner, T.N.Massey, W.von Oertzen, Th.Stolla, M.Wilpert, Th.Wilpert

Spectroscopy of 10He

NUCLEAR REACTIONS 10Be, 16O, 12C(14C, 14O), E=334.4 MeV; measured spectra. 10He deduced mass, mass excess, two-neutron separation energy, resonances, Γ, possible J, π.

doi: 10.1016/0370-2693(94)91336-6
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1990DE22      Z.Phys. A336, 375 (1990)

G.de Angelis, P.Kleinheinz, B.Rubio, J.L.Tain, K.Zuber, B.Brinkmoller, P.von Rossen, J.Romer, D.Paul, J.Meissburger, G.P.A.Berg, A.Magiera, G.Hlawatsch, L.G.Mann, T.N.Massey, D.Decman, G.L.Struble, J.Blomqvist

Collective Excitations in 148Gd Populated in the pp'-Reaction on a Radioactive Target

NUCLEAR REACTIONS 148Gd(p, p'), E=25 MeV; measured σ(Ep'), σ(θ). 148Gd deduced levels, B(λ), configuration, J, π. DWBA analysis.


1990MA68      Z.Phys. A337, 301 (1990)

L.G.Mann, D.J.Decman, H.E.Martz, T.N.Massey, G.L.Struble, P.Kleinheinz, H.J.Scheerer, D.G.Burke, G.Kajrys

Occupancy of Single-Proton Orbitals in 148Gd

NUCLEAR REACTIONS 148Gd(3He, d), E=30 MeV; 148Gd(t, α), E=18 MeV; measured σ(θ), σ(Ed), σ(Eα); deduced model parameters. 149Tb levels deduced L, spectroscopic factors. 147Eu deduced levels, L, spectroscopic factors. 148Gd deduced ground state proton pair probability. DWBA analysis.


1989KA21      Phys.Lett. 227B, 325 (1989)

H.Kader, G.Graw, F.J.Eckle, G.Eckle, P.Schiemenz, P.Kleinheinz, B.Rubio, G.de Angelis, T.N.Massey, L.G.Mann, J.Blomqvist

Particle-Octupole Coupling in N = 83 Nuclei from Neutron Transfer Studies with Polarized Deuterons

NUCLEAR REACTIONS 148Gd, 146Sm(polarized d, t), E=22 MeV; 144Nd(polarized d, t), E=20 MeV; measured σ(θ). 147Gd, 145Sm, 143Nd deduced level, J, π, configuration. Radioactive targets from Ta(p, X) reaction.

doi: 10.1016/0370-2693(89)90938-6
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1987ZE03      Nucl.Instrum.Methods Phys.Res. A256, 180 (1987)

M.Zendel, S.G.Prussin, K.Rengan, T.N.Massey, R.A.Meyer

Modification of a Gas Jet Transport System for the Supression of Heavy-Mass Fission Product Homologues

NUCLEAR REACTIONS 235U(n, F), E=thermal; measured fission product Eγ, Iγ; deduced fission fragment mean penetration depths into Al. Ge(Li) detector.

doi: 10.1016/0168-9002(87)91054-0
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1986RU04      Z.Phys. A324, 27 (1986)

B.Rubio, A.Ercan, G.de Angelis, P.Kleinheinz, J.L.Tain, B.Brinkmoller, D.Paul, J.Meissburger, L.G.Mann, D.J.Decman, T.N.Massey, G.L.Struble, H.J.Scheerer, J.Blomqvist

The Ground State Mass of 147Gd from Single-Neutron-Transfer Reactions and Its Impact on Derived Mass Values

NUCLEAR REACTIONS 148Gd(p, d), E=25 MeV; 148Gd(d, t), E=22 MeV; 148Gd(3He, α), E=30 MeV; measured σ(Ed), σ(Et), σ(Eα); deduced Q-value differences. 147Gd deduced mass. 148Gd deduced neutron separation energy. Shell model comparison.


1983ME17      Int.J.Appl.Radiat.Isotop. 34, 1073 (1983)

R.A.Meyer, T.N.Massey

Multigamma-Ray Calibration Sources

RADIOACTIVITY 88Br(β-); 152Eu(β-), (β+), (EC); 56Co(EC), (β+); 110mAg(β-); 168Tm(EC), (β-); measured Iγ. Automated multi-spectrometer γ-ray counting, large volume hyperpure Ge detectors, mass separated sources.

doi: 10.1016/0020-708X(83)90173-4
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Note: The following list of authors and aliases matches the search parameter T.Massey: , T.A.MASSEY, T.N.MASSEY