NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = D.Dehnhard Found 90 matches. 2004RI05 Phys.Rev. C 69, 024616 (2004) C.M.Riedel, D.Dehnhard, M.Palarczyk, M.A.Espy, M.A.Franey, J.L.Langenbrunner, L.C.Bland, D.S.Carman, B.Brinkmoller, R.Madey, Y.Wang, J.W.Watson Measurement of 4He(p(pol), n) at 100 and 200 MeV: Analysis with recoil-corrected continuum shell model NUCLEAR REACTIONS 4He(polarized p, n), E=100, 200 MeV; measured σ(E, θ), Ay(θ); deduced core contributions and ground-state correlation effects. Recoil-corrected continuum shell model analysis.
doi: 10.1103/PhysRevC.69.024616
2003AH09 Phys.Rev. C 68, 064004 (2003) M.W.Ahmed, X.Cui, A.Empl, E.V.Hungerford, K.J.Lan, M.Youn, R.E.Chrien, R.Gill, P.Pile, A.Rusek, R.Sutter, J.Bjoraker, D.Dehnhard, J.M.O'Donnell, J.Gerald, H.Juengst, J.H.Liu, J.C.Peng, C.L.Morris, C.M.Riedel, H.A.Thiessen, D.Androic, I.Bertovic, M.Furic, T.Petkovic, M.Planinic, L.Tang, V.Zeps Experimental study of the 12C(K-stopped, π0)12ΛB reaction NUCLEAR REACTIONS 12C(K-, π0), E at rest; measured pion spectra; deduced hypernucleus production ground and excited state branching ratios. 12B deduced hyperon binding energy.
doi: 10.1103/PhysRevC.68.064004
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
1999ZH22 Phys.Rev. C60, 024001 (1999) Q.Zhao, G.Burleson, S.Blanchard, T.Chang, W.Gibbs, J.Haas, B.Park, M.Whitton, M.Espy, D.Dehnhard, B.Larson, J.O'Donnell, M.Palarczyk, W.Cummings, P.Delheij, O.Hausser, E.Pasyuk, M.Gostkin, J.Amann, R.Boudrie, C.Riedel, C.Morris, S.Pentilla, D.Swenson, D.Tupa, J.Comfort, C.Gaulard, K.Maeda, G.Glass, I.Supek Measurements of Asymmetries of Pion Single Charge Exchange on Polarized 3He at 200 MeV NUCLEAR REACTIONS 3He(π-, π0), E=200 MeV; measured triton, neutral pion spectra, σ(θ), Ay(θ); deduced small contributions from SS' and SD overlaps. Polarized target. Comparison with theoretical predictions.
doi: 10.1103/PhysRevC.60.024001
1998PA22 Phys.Rev. C58, 645 (1998) M.Palarczyk, C.M.Riedel, D.Dehnhard, M.A.Espy, M.A.Franey, J.L.Langenbrunner, L.C.Bland, D.S.Carman, B.Brinkmoller, R.Madey, Y.Wang, J.W.Watson, N.S.Chant Cross Sections and Analyzing Powers for the (p(pol), n) Reaction on 3He and 4He at 200 MeV NUCLEAR REACTIONS 3,4He(polarized p, n), E=200 MeV; measured neutron spectra, σ(Ex, θ), A(y)(θ). DWIA analysis.
doi: 10.1103/PhysRevC.58.645
1997ES05 Phys.Rev. C56, 2607 (1997) M.A.Espy, J.M.O'Donnell, B.Davis, D.Dehnhard, J.L.Langenbrunner, B.Larson, M.Palarczyk, C.M.Riedel, K.Wick, S.Blanchard, G.R.Burleson, W.R.Gibbs, B.Lail, B.Nelson, B.K.Park, Q.Zhao, W.J.Cummings, P.P.J.Delheij, B.K.Jennings, O.Hausser, R.Henderson, D.Thiessen, E.Brash, M.K.Jones, B.Brinkmoller, K.Maeda, F.Merrill, C.L.Morris, S.Penttila, D.Swenson, D.Tupa, C.Bennhold, S.S.Kamalov Asymmetries for Elastic Scattering of π- from Polarized 3He atΔ Resonance Energies NUCLEAR REACTIONS 3He(π+, π+), E=142, 180, 256 MeV; 3He(π-, π-), E=180 MeV; measured σ(θ); deduced asymmetries, Δ-n spin-spin interaction. Optically pumped spin polarized target, large acceptance spectrometer. Model comparisons.
doi: 10.1103/PhysRevC.56.2607
1996DE70 Acta Phys.Pol. B27, 3019 (1996) New Results on Spin Effects in Pion-Nucleus Elastic Scattering and Single-Charge Exchange
1996ED02 Phys.Lett. 368B, 39 (1996); Erratum Phys.Lett. 380B, 493 (1996) C.M.Edwards, M.Palarczyk, D.Dehnhard, M.A.Espy, M.A.Franey, J.L.Langenbrunner, L.C.Bland, D.S.Carman, B.Brinkmoller, R.Madey, Y.Wang, J.W.Watson, L.Bildsten The 4He(p, n)4Li(*) Reaction at 100 and 200 MeV; Implications for the mass-four system and for astrophysics NUCLEAR REACTIONS 4He(p, nX), E=100, 200 MeV; measured inclusive σ(θ, En). 4Li deduced evidence for narrow states.
doi: 10.1016/0370-2693(95)01499-3
1996ES04 Phys.Rev.Lett. 76, 3667 (1996) M.A.Espy, D.Dehnhard, C.M.Edwards, M.Palarczyk, J.L.Langenbrunner, B.Davis, G.R.Burleson, S.Blanchard, W.R.Gibbs, B.Lail, B.Nelson, B.K.Park, Q.Zhao, W.J.Cummings, P.P.J.Delheij, B.K.Jennings, R.Henderson, O.Hausser, D.Thiessen, E.Brash, M.K.Jones, B.Larson, B.Brinkmoller, K.Maeda, C.L.Morris, J.M.O'Donnell, S.Penttila, D.Swenson, D.Tupa, C.Bennhold, S.S.Kamalov Asymmetries for Elastic Scattering of π+ from Polarized 3He and the Δ-Neutron Spin-Spin Interaction NUCLEAR REACTIONS 3He(π+, π+), E=142-256 MeV; measured energy spectra, asymmetry vs θ; deduced Δ-n spin-spin interaction role. Polarized target.
doi: 10.1103/PhysRevLett.76.3667
1995OU01 Nucl.Phys. A586, 20 (1995) M.Oura, H.Orihara, M.Hosaka, G.C.Jon, A.Terakawa, K.Ishii, A.Narita, K.Hosomi, T.Nakagawa, K.Miura, H.Ohnuma, T.Niizeki, D.Dehnhard The 17,18O(p, n)17,18F Reaction at E(p) = 35 MeV NUCLEAR REACTIONS 17,18O(p, n), E=35 MeV; measured σ(θ). DWBA analysis.
doi: 10.1016/0375-9474(94)00772-F
1995RA14 Phys.Rev. C52, R445 (1995) B.A.Raue, L.C.Bland, D.S.Carman, G.M.Huber, B.C.Markham, D.W.Miller, K.Murphy, S.F.Pate, J.A.Templon, B.Brinkmoller, D.Dehnhard, S.M.Sterbenz Study of the Isospin Response of the 4He Continuum using the 4He(p, p'X) Reaction NUCLEAR REACTIONS 4He(p, p't), (p, p'3He), (p, p'd), (p, p'X), E=101.2 MeV; measured (particle)(particle)(θ), σ(E) ratio in some cases. 4He deduced resonances single nucleon decay characteristics.
doi: 10.1103/PhysRevC.52.R445
1994YE06 Phys.Rev. C50, 897 (1994) Y.-F.Yen, B.Brinkmoller, D.Dehnhard, M.A.Franey, S.M.Sterbenz, Y.-J.Yu, B.Berman, G.R.Burleson, K.Cranston, A.Klein, G.S.Kyle, R.Alarcon, T.Averett, J.R.Comfort, J.J.Gorgen, B.G.Ritchie, J.R.Tinsley, M.Barlett, G.W.Hoffmann, K.Johnson, C.F.Moore, M.Purcell, H.Ward, A.Williams, J.A.Faucett, S.J.Greene, J.J.Jarmer, J.A.McGill, C.L.Morris, S.I.Penttila, N.Tanaka, H.T.Fortune, E.Insko, R.Ivie, J.M.O'Donnell, D.Smith, M.A.Khandaker, S.Chakravarti Pion Elastic Scattering from Polarized 13C in the Energy Region of the P33 Resonance NUCLEAR REACTIONS 13C(π+, π+), (π-, π-), E=130-180 MeV; 13C(π+, π+), E=223 MeV; 13C(π-, π-), E=226 MeV; measured analyzing power A(y)(θ), σ(θ); deduced spin-flip transition quadrupole component role. Polarized, unpolarized target. DWIA calculations, optical, Δ-hole models.
doi: 10.1103/PhysRevC.50.897
1992JO03 Phys.Rev. C46, 52 (1992) M.K.Jones, D.Dehnhard, S.K.Nanda, S.M.Sterbenz, C.L.Morris, M.Plum, J.D.Zumbro, A.H.Hussein, D.S.Oakley, M.J.Smithson, A.L.Williams, J.McDonald, M.A.Bryan, A.H.Fuentes, M.Lynker, D.Crockett, M.A.Machuca, S.Mordechai, C.F.Moore 4He(π, π'p)3H Reaction Near the P33 π-Nucleon Resonance NUCLEAR REACTIONS 4He(π+, π+'p), (π-, π-'p), E=140, 180 MeV; measured σ(θ(π'), σ(p)) vs excitation energy; deduced reaction mechanisms.
doi: 10.1103/PhysRevC.46.52
1992LA17 Phys.Rev.Lett. 69, 1508 (1992) J.Langenbrunner, M.K.Jones, D.Dehnhard, C.L.Morris, W.R.Gibbs Evidence for Direct Triton Knockout in the 4He(π, π't)p Reaction NUCLEAR REACTIONS 4He(π+, π+t), (π-, π-t), E=180 MeV; measured σ(θ(π), θ(p)); deduced direct triton knockout mechanism role.
doi: 10.1103/PhysRevLett.69.1508
1992ST03 Phys.Rev. C45, 2578 (1992); Erratum Phys.Rev. C46, 2117 (1992) S.M.Sterbenz, D.Dehnhard, M.K.Jones, S.K.Nanda, C.E.Parman, Y.-F.Yen, K.W.Jones, C.L.Morris Inelastic Scattering of Polarized Protons from 4He at 500 and 800 MeV NUCLEAR REACTIONS 4He(polarized p, p'), E=500, 800 MeV; measured σ(θ), analyzing powers vs θ; deduced optical potential parameters. 4He deduced monopole strength. DWIA analysis, recoil corrected continuum shell model wave functions.
doi: 10.1103/PhysRevC.45.2578
1991BR21 Phys.Rev. C44, 2031 (1991) B.Brinkmoller, C.L.Blilie, D.Dehnhard, M.K.Jones, G.M.Martinez, S.K.Nanda, S.M.Sterbenz, Y.-F.Yen, L.G.Atencio, S.J.Greene, C.L.Morris, S.J.Seestrom, G.R.Burleson, K.S.Dhuga, J.A.Faucett, R.W.Garnett, K.Maeda, C.F.Moore, S.Mordechai, A.Williams, S.H.Yoo, L.C.Bland Elastic Scattering of π+ and π- from 4He between 90 and 240 MeV NUCLEAR REACTIONS 4He(π+, π+), (π-, π-), E=90-240 MeV; measured σ(θ); deduced phase shifts. Optical model analysis.
doi: 10.1103/PhysRevC.44.2031
1991GO14 Phys.Rev.Lett. 66, 2193 (1991) J.J.Gorgen, J.R.Comfort, J.R.Tinsley, T.Averett, J.DeKorse, G.Franklin, B.G.Ritchie, G.Kyle, A.Klein, B.Berman, G.Burleson, K.Cranston, J.A.Faucett, J.J.Jarmer, J.N.Knudson, S.Penttila, N.Tanaka, B.Brinkmoller, D.Dehnhard, Y.-F.Yen, S.Hoibraten, H.Breuer, B.S.Flanders, M.A.Khandaker, D.L.Naples, D.Zhang, M.L.Barlett, G.W.Hoffmann, M.Purcell Analyzing Powers for Pion Charge Exchange on Polarized 13C NUCLEAR REACTIONS 13C(π+, π0), E=163 MeV; measured σ(θ), analyzing power vs θ. Polarized target.
doi: 10.1103/PhysRevLett.66.2193
1991YE01 Phys.Rev.Lett. 66, 1959 (1991) Y.-F.Yen, B.Brinkmoller, D.Dehnhard, S.M.Sterbenz, Y.-J.Yu, B.Berman, G.R.Burleson, K.Cranston, A.Klein, G.S.Kyle, R.Alarcon, T.Averett, J.R.Comfort, J.J.Gorgen, B.G.Ritchie, J.R.Tinsley, M.Barlett, G.W.Hoffmann, K.Johnson, C.F.Moore, M.Purcell, H.Ward, A.Williams, J.A.Faucett, S.J.Greene, J.J.Jarmer, J.A.McGill, C.L.Morris, S.Penttila, N.Tanaka, H.T.Fortune, E.Insko, R.Ivie, J.M.O'Donnell, D.Smith, M.A.Khandaker, S.Chakravarti Asymmetry Measurement of Pion Elastic Scattering from Polarized 13C in the Energy Region of the P33 Resonance NUCLEAR REACTIONS 13C(π+, π+), (π-, π-), E=132-226 MeV; measured analyzing power vs θ. Polarized target.
doi: 10.1103/PhysRevLett.66.1959
1990GO36 J.Phys.(Paris), Colloq.C-6, 583 (1990) J.Gorgen, J.Comfort, T.Averett, J.DeKorse, G.Franklin, B.Ritchie, J.Tinsley, G.Kyle, B.Berman, G.R.Burleson, K.Cranston, A.Klein, J.A.Faucett, J.Jarmer, J.N.Knudson, S.Penttila, N.Tanaka, B.Brinkmoller, D.Dehnhard, Y.F.Yen, H.Breuer, M.A.Khandaker, D.L.Naples, B.S.Flanders, D.Zhang, M.Barlett, G.W.Hoffmann, M.Purcell, S.Hoibraten Analyzing Power Measurements for the (π+, π0) Reaction on a Polarized 13C Target at T(π+) = 163 MeV NUCLEAR REACTIONS 13C(π+, π0), E=163 MeV; measured σ(θ), analyzing power vs θ. Polarized target. DWIA analyses.
1990JO04 Phys.Rev. C42, R807 (1990) M.K.Jones, D.Dehnhard, S.K.Nanda, S.M.Sterbenz, C.L.Morris, M.Plum, J.D.Zumbro, A.Hussein, D.S.Oakley, M.J.Smithson, A.L.Williams, J.McDonald, M.A.Bryan, A.H.Fuentes, M.Lynker, D.Crockett, M.A.Machuca, S.Mordechai, C.F.Moore 4He(π, π'p)3H Reaction: Quasifree and resonance scattering NUCLEAR REACTIONS 4He(π+, π+'p), (π-, π-'p), E=180 MeV; measured σ(θ(π), θp); deduced σ(π+)/σ(π-). DWIA calculation.
doi: 10.1103/PhysRevC.42.R807
1990OH04 Nucl.Phys. A514, 273 (1990) H.Ohnuma, N.Hoshino, K.Ieki, M.Iwase, H.Shimizu, H.Toyokawa, T.Hasegawa, K.Nisimura, M.Yasue, H.Kabasawa, T.Nakagawa, T.Tohei, H.Orihara, S.I.Hayakawa, K.Miura, T.Suehiro, S.K.Nanda, D.Dehnhard, M.A.Franey The 16O(p(pol), p) Reaction at 35 MeV NUCLEAR REACTIONS 16O(polarized p, p'), E=35 MeV; measured σ(θ), A(θ). DWBA analysis, shell model wave functions, electron scattering transition densities, density independent, dependent interactions.
doi: 10.1016/0375-9474(90)90070-3
1990YE06 J.Phys.(Paris), Colloq.C-6, 587 (1990) Y.-F.Yen, B.Brinkmoller, D.Dehnhard, S.M.Sterbenz, Y.-J.Yu, B.Berman, G.R.Burleson, K.Cranston, A.Klein, G.S.Kyle, R.Alarcon, T.Averett, J.R.Comfort, J.Gorgen, B.Ritchie, J.R.Tinsley, G.W.Hoffmann, K.Johnson, C.F.Moore, M.Purcell, H.Ward, A.Williams, J.A.Faucett, S.J.Greene, J.Jarmer, J.A.McGill, C.L.Morris, S.Penttila, N.Tanaka, H.T.Fortune, E.Insko, R.Ivie, J.M.O'Donnell, D.Smith, S.Hoibraten, M.Khandaker, S.Chakravarti Pion Elastic Scattering from Polarized 13C in the Energy Region of the [3, 3] Resonance NUCLEAR REACTIONS 13C(π+, π+), (π-, π-), E=114-226 MeV; measured analyzing power vs θ. Polarized target. DWIA analyses.
1990YO02 J.Phys.(London) G16, L89 (1990) S.H.Yoo, A.Williams, S.Mordechai, C.F.Moore, C.L.Morris, S.J.Seestrom, M.Jones, S.Sterbenz, D.Dehnhard, D.S.Oakley, A.Fazely 208Pb(π±, π±'n) Reaction in the Giant-Resonance Region NUCLEAR REACTIONS 208Pb(π+, π+'n), (π-, π-'n), E=180 MeV; measured σ(θn, θπ), missing mass spectra. 208Pb deduced giant resonance neutron decay features.
doi: 10.1088/0954-3899/16/5/002
1989YO06 Phys.Rev.Lett. 63, 738 (1989) S.H.Yoo, A.Williams, S.Mordechai, C.F.Moore, C.L.Morris, S.J.Seestrom-Morris, M.K.Jones, S.M.Sterbenz, D.Dehnhard, D.S.Oakley, A.Fazely 12C(π±, π±'p)11B Reaction Near the Giant Dipole Region NUCLEAR REACTIONS 12C(π+, π+'p), (π-, π-'p), E=180 MeV; measured σ(θ(π), θ(p), E(π)); deduced σ(π+, π+p)/σ(π-, π-p) near GDR. DWIA analysis.
doi: 10.1103/PhysRevLett.63.738
1988BA27 Phys.Rev. C37, 2892 (1988) R.Baran, J.Gotz, A.Hofmann, D.Malz, R.Muller, R.Olszewski, H.W.Ortner, D.Dehnhard Excitation Function of the 15.11 MeV (1+, T=1) State in 12C from (π, π'γ) Angular Correlations NUCLEAR REACTIONS 12C(π, π'γ), E=116, 140, 162, 180, 226 MeV; measured σ(E(π)), πγ-coin. 12C levels deduced relative σ(ratio) vs E.
doi: 10.1103/PhysRevC.37.2892
1988HA14 Phys.Rev. C37, 1554 (1988) A.C.Hayes, S.Chakravarti, D.Dehnhard, P.J.Ellis, D.B.Holtkamp, L.-P.Lung, S.J.Seestrom-Morris, H.Baer, C.L.Morris, S.J.Greene, C.J.Harvey Structure of the Low-Lying 2+ States in 14C from Inelastic Pion Scattering NUCLEAR STRUCTURE 14C, 14N, 14O; calculated levels, B(λ). Shell model. NUCLEAR REACTIONS 14C(π, π'), E=164 MeV; analyzed σ(θ). 14C level deduced isovector component quenching.
doi: 10.1103/PhysRevC.37.1554
1988OL02 Phys.Rev. C37, 2665 (1988) R.Olszewski, R.Baran, A.Hofmann, S.Krell, H.W.Ortner, J.Orzechowsky, G.Schmidtlein, F.Vogler, W.List, G.R.Smith, D.Dehnhard, M.Thies Medium Effects in (π, π'γ) Angular Correlations on 12C(2+) NUCLEAR REACTIONS 12C(π, π'γ), E=116, 140, 162, 180, 226 MeV; measured π(γ)-coin, πγ(θ). Isobar-hole model.
doi: 10.1103/PhysRevC.37.2665
1988SE04 Phys.Rev. C37, 2057 (1988) S.J.Seestrom-Morris, D.Dehnhard, M.A.Franey, D.B.Holtkamp, C.L.Blilie, C.L.Morris, J.D.Zumbro, H.T.Fortune Pion Inelastic Scattering to the Three Lowest 2+ States of 18O NUCLEAR REACTIONS 18O(π+, π+'), (π-, π-'), E=164 MeV; measured σ(θ). 18O levels deduced matrix elements, transition densities. Gas Target. DWIA analysis.
doi: 10.1103/PhysRevC.37.2057
1987CH14 Phys.Rev. C35, 2197 (1987) S.Chakravarti, D.Dehnhard, M.A.Franey, S.J.Seestrom-Morris, D.B.Holtkamp, C.L.Blilie, A.C.Hayes, C.L.Morris, D.J.Millener Distorted-Wave Impulse Approximation and Coupled-Channels Analysis of Inelastic Pion Scattering from 18O NUCLEAR REACTIONS 18O(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=164 MeV; calculated σ(θ). 18O levels deduced transition densities. DWIA, coupled-channels calculations.
doi: 10.1103/PhysRevC.35.2197
1987MO07 Phys.Rev. C35, 1388 (1987) C.L.Morris, S.J.Seestrom-Morris, D.Dehnhard, C.L.Blilie, R.Gilman, G.P.Gilfoyle, J.D.Zumbro, M.G.Burlein, S.Mordechai, H.T.Fortune, L.C.Bland, M.Brown, D.P.Saunders, P.A.Seidl, C.F.Moore, K.Maeda, G.S.Blanpied, B.A.Brown Neutron and Proton Matrix Elements for 2+1 Transitions in T = 1 Nuclei from Pion Inelastic Scattering NUCLEAR REACTIONS 18O, 22Ne, 26Mg, 30Si, 34S(π+, π+'), (π-, π-'), E=180 MeV; measured σ(θ). 18O, 22Ne, 26Mg, 30Si, 34S transitions deduced neutron, proton quadrupole matrix elements. DWIA analysis.
doi: 10.1103/PhysRevC.35.1388
1986BL07 Phys.Rev.Lett. 57, 543 (1986) C.L.Blilie, D.Dehnhard, D.B.Holtkamp, S.J.Seestrom-Morris, S.K.Nanda, W.B.Cottingame, D.Halderson, C.L.Morris, C.F.Moore, P.A.Seidl, H.Ohnuma, K.Maeda Measurement of Isospin Mixing in 4He and Its Implications for Charge-Symmetry Breaking NUCLEAR REACTIONS 4He(π+, π+'), (π-, π-'), E=180 MeV; measured σ(E(π), θ(π)); deduced σ(π+)/σ(π-). 4He deduced very weak 1- state isospin mixing. DWIA analysis.
doi: 10.1103/PhysRevLett.57.543
1986BU13 Nucl.Instrum.Methods Phys.Res. A247, 327 (1986) G.R.Burleson, W.B.Cottingame, K.S.Dhuga, J.A.Faucett, C.P.Fontenla, J.F.Amann, R.L.Boudrie, S.J.Greene, C.L.Morris, N.Tanaka, Z.F.Wang, D.Yusnukis, M.Brown, R.R.Kiziah, E.C.Milner, C.F.Moore, S.Mordechai, D.Oakley, P.A.Seidl, C.L.Blilie, D.Dehnhard, S.Nanda, S.J.Seestrom-Morris, J.D.Zumbro, K.Maeda A Large-Angle Pion-Nucleus Scattering Facility for EPICS at LAMPF NUCLEAR REACTIONS 12C(π+, π+), E=162 MeV; 16O(π-, π-), E=114 MeV; measured σ(θ), θ=115°-180°. Energetic pion channel, spectrometer.
doi: 10.1016/0168-9002(86)91314-8
1986OH03 Nucl.Phys. A456, 61 (1986) H.Ohnuma, B.A.Brown, D.Dehnhard, K.Furukawa, T.Hasegawa, S.Hayakawa, N.Hoshino, K.Ieki, M.Kabasawa, K.Maeda, K.Miura, K.Muto, T.Nakagawa, K.Nisimura, H.Orihara, T.Suehiro, T.Tohei, M.Yasue A Comparative Study of the 13C(p, p')13C and 13C(p, n)13N Reactions at E(p) = 35 MeV NUCLEAR REACTIONS 13C(polarized p, n), (polarized p, p'), E=35 MeV; measured σ(θ), A(θ). 13C level deduced transition isoscalar component. Enriched target. DWBA analysis.
doi: 10.1016/0375-9474(86)90366-0
1986OL07 Phys.Rev.Lett. 57, 2143 (1986) R.Olszewski, R.Baran, A.Hofmann, S.Krell, H.W.Ortner, J.Orzechowski, G.Schmidtlein, F.Vogler, G.R.Smith, W.List, D.Dehnhard, M.Thies Test of the Δ-Hole Model through the Energy Dependence of (π, π'γ) Angular Correlations on 12C NUCLEAR REACTIONS 12C(π, π'γ), E=116, 140, 162, 180, 226 MeV; measured πγ(θ), πγ(φ); deduced isobar-nucleus dynamics role. NaI detectors. Isobar-hole model.
doi: 10.1103/PhysRevLett.57.2143
1985DH01 Phys.Rev. C32, 2208 (1985) K.S.Dhuga, G.R.Burleson, J.A.Faucett, R.L.Boudrie, W.B.Cottingame, S.J.Greene, C.L.Morris, N.Tanaka, Z.F.Wang, S.Nanda, D.Dehnhard, J.D.Zumbro, S.Mordechai, C.F.Moore, D.J.Ernst Large-Angle Elastic Scattering of π+ and π- from 16O at 114 MeV NUCLEAR REACTIONS 16O(π+, π+), (π-, π-), E=114 MeV; measured σ(θ); deduced large σ(π+)/σ(π-) differences. First-, second-order optical model calculations.
doi: 10.1103/PhysRevC.32.2208
1985HO07 Phys.Rev. C31, 957 (1985); Erratum Phys.Rev. C41, 1319 (1990) D.B.Holtkamp, S.J.Seestrom-Morris, D.Dehnhard, H.W.Baer, C.L.Morris, S.J.Greene, C.J.Harvey, D.Kurath, J.A.Carr Pion Scattering to 4- States in 14C NUCLEAR REACTIONS 14C(π+, π+'), (π-, π-'), E=164 MeV; measured σ(θ), σ(E(π)). 14C deduced levels, J, π, neutron, proton amplitudes, ratios. DWIA, shell model wave functions.
doi: 10.1103/PhysRevC.31.957
1985SE06 Phys.Rev. C31, 923 (1985) S.J.Seestrom-Morris, D.Dehnhard, C.L.Morris, L.C.Bland, R.Gilman, H.T.Fortune, D.J.Millener, D.P.Saunders, P.A.Seidl, R.R.Kiziah, C.F.Moore M4 Transitions Observed in Pion Inelastic Scattering on 15N NUCLEAR REACTIONS 15N(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=164 MeV; measured σ(θ(π), E(π)), σ(θ). 15N levels deduced M4 transition strength, form factors.
doi: 10.1103/PhysRevC.31.923
1984BL17 Phys.Rev. C30, 1989 (1984) C.L.Blilie, D.Dehnhard, M.A.Franey, D.H.Gay, D.B.Holtkamp, S.J.Seestrom-Morris, P.J.Ellis, C.L.Morris, D.J.Millener Isospin Structure of Transitions in 17O from Inelastic Pion Scattering at 164 MeV NUCLEAR REACTIONS 16,17O(π+, π+'), (π-, π-'), E=164 MeV; measured σ(θ), σ(E(π)). 17O deduced M4, E2 transition strength distribution. Microscopic DWIA calculations.
doi: 10.1103/PhysRevC.30.1989
1984DE19 Phys.Rev. C30, 242 (1984) D.Dehnhard, D.H.Gay, C.L.Blilie, S.J.Seestrom-Morris, M.A.Franey, C.L.Morris, R.L.Boudrie, T.S.Bhatia, C.F.Moore, L.C.Bland, H.Ohnuma Excitation of the 1+ State in 48Ca(10.2 MeV) by Inelastic Scattering of π- and π+ NUCLEAR REACTIONS 48Ca(π+, π+'), (π-, π-'), E=116-180 MeV; measured σ(E(π)), σ(θ). 48Ca level deduced σ(π-)/σ(π+), isoscalar, isovector rescaling factor dependence. DWIA analysis.
doi: 10.1103/PhysRevC.30.242
1984HI10 Phys.Rev. C30, 1976 (1984) N.M.Hintz, M.A.Franey, M.M.Gazzaly, D.Cook, G.S.Kyle, D.Dehnhard, S.J.Seestrom-Morris, G.W.Hoffmann, M.Barlett, G.S.Blanpied, J.A.McGill, J.B.McClelland, R.L.Boudrie, F.Irom, G.Pauletta High Spin States in 28Si and 58Ni NUCLEAR REACTIONS 28Si, 58Ni(p, p'), E=333, 498, 800 MeV; measured σ(θ), σ(Ep). 28Si, 58Ni levels deduced transition densities. DWIA, other (p, p'), (e, e') data analysis.
doi: 10.1103/PhysRevC.30.1976
1984MO18 Phys.Rev. C30, 662 (1984) C.L.Morris, N.Tanaka, R.L.Boudrie, L.C.Bland, H.T.Fortune, R.Gilman, S.J.Seestrom-Morris, C.F.Moore, D.Dehnhard Small Angle Pion Inelastic Scattering from 12C at 162 MeV NUCLEAR REACTIONS 12C(π+, π+), (π+, π+'), E=162 MeV; measured σ(θ), missing mass spectra. DWIA analysis.
doi: 10.1103/PhysRevC.30.662
1984SE12 Phys.Rev. C30, 270 (1984) S.J.Seestrom-Morris, M.A.Franey, D.Dehnhard, D.B.Holtkamp, R.L.Boudrie, J.F.Amann, G.C.Idzorek, C.A.Goulding 13C(p(pol), p')13C Reaction at T(p) = 547 MeV NUCLEAR REACTIONS 13C(polarized p, p'), E=547 MeV; measured σ(Ep'), σ(θ), analyzing power vs θ. DWIA analysis, shell model transition densities.
doi: 10.1103/PhysRevC.30.270
1984VO04 Phys.Lett. 134B, 161 (1984) F.Vogler, R.Olszewski, M.Meyer, E.L.Mathie, G.R.Smith, E.Boschitz, S.Chakravarti, D.Dehnhard, M.Thies Measurement of the 12C(π, π'γ)12C(2+, T = 0; 4.44 MeV) Angular Correlations: A test of the isobar-hole model NUCLEAR REACTIONS 12C(π+, π+'), E=162 MeV; measured σ(θ), σ(θπ, θγ); deduced isobar-hole model validity.
doi: 10.1016/0370-2693(84)90662-2
1983SE15 Phys.Rev. C28, 1301 (1983) S.J.Seestrom-Morris, D.Dehnhard, M.A.Franey, C.L.Morris, R.L.Boudrie, H.A.Thiessen Analysis of Elastic and Inelastic Scattering of 162 MeV Pions from 13C by an Optical Potential and a Collective Model NUCLEAR REACTIONS 13C(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=162 MeV; measured σ(θ). 13C levels deduced neutron, proton B(λ) components. Optical, collective model analyses.
doi: 10.1103/PhysRevC.28.1301
1983SH18 Phys.Rev. C28, 717 (1983) V.Shkolnik, D.Dehnhard, M.A.Franey Elastic Scattering of 16O by 28Si NUCLEAR REACTIONS 28,29,30Si(16O, 16O), E=45-63 MeV; measured σ(θ) vs E; deduced optical model parameters, potential strength ambiguities, L-dependent potential resonances.
doi: 10.1103/PhysRevC.28.717
1982BL01 Phys.Rev. C25, 422 (1982) G.S.Blanpied, N.M.Hintz, G.S.Kyle, M.A.Franey, S.J.Seestrom-Morris, R.K.Owen, J.W.Palm, D.Dehnhard, M.L.Barlett, C.J.Harvey, G.W.Hoffmann, J.A.McGill, R.P.Liljestrand, L.Ray Elastic and Inelastic Scattering of 0.8 GeV Protons from 24Mg and 26Mg NUCLEAR REACTIONS 24,26Mg(p, p), (p, p'), E=0.8 GeV; measured σ(θ). 24,26Mg deduced deformation lengths, multipole moments. Optical model, DWBA, coupled-channels analyses, rotational model.
doi: 10.1103/PhysRevC.25.422
1982SE04 Phys.Rev. C26, 594 (1982) S.J.Seestrom-Morris, D.Dehnhard, M.A.Franey, G.S.Kyle, C.L.Morris, R.L.Boudrie, J.Piffaretti, H.A.Thiessen Inelastic Pion Scattering from 13C at 162 MeV NUCLEAR REACTIONS 13C(π+, π+'), (π-, π-'), E=162 MeV; measured σ(θ). 13C levels deduced L. Microscopic DWIA analysis, shell model wave functions.
doi: 10.1103/PhysRevC.26.594
1981HO14 Phys.Rev.Lett. 47, 216 (1981) D.B.Holtkamp, S.J.Seestrom-Morris, S.Chakravarti, D.Dehnhard, H.W.Baer, C.L.Morris, S.J.Greene, C.J.Harvey Strong Cancellations of Neutron and Proton Transition Amplitudes Observed in Pion Inelastic Scattering NUCLEAR REACTIONS 14C(π+, π+'), (π-, π-'), E=164 MeV; measured σ(θ, E(π)); deduced neutron, proton transition amplitude cancellations. 14C deduced levels, J, π, configuration.
doi: 10.1103/PhysRevLett.47.216
1981SE08 Phys.Rev.Lett. 46, 1447 (1981) S.J.Seestrom-Morris, D.Dehnhard, D.B.Holtkamp, C.L.Morris Identification of ΔS = 1 Transitions in 13C by Measurement of Pion Inelastic Excitation Functions NUCLEAR REACTIONS 13C(π+, π+'), (π-, π-'), E=100-300 MeV; measured σ(θ, E). 13C deduced dominant ΔS=1 transitions. One-step mechanism, fixed scatterer impulse approximation.
doi: 10.1103/PhysRevLett.46.1447
1980HO13 Phys.Rev.Lett. 45, 420 (1980) D.R.Holtkamp, W.J.Braithwaite, W.Cottingame, S.J.Greene, R.J.Joseph, C.F.Moore, C.L.Morris, J.Piffaretti, E.R.Siciliano, H.A.Thiessen, D.Dehnhard Isospin Mixing of 4- Particle-Hole States in 16O NUCLEAR REACTIONS 16O(π+, π+'), (π-, π-'), E=164 MeV; measured σ(θ(π), E(π')); deduced off-diagonal charge-dependent matrix elements. 16O levels deduced isospin mixing.
doi: 10.1103/PhysRevLett.45.420
1980KU04 Nucl.Phys. A334, 336 (1980) S.Kubono, D.A.Lewis, D.Dehnhard The j-Dependence of the (19F, 16O) Reaction NUCLEAR REACTIONS 28,30Si(19F, 19F), (19F, 16O), E=60 MeV; 60Ni(19F, 19F), (19F, 16O), E=75 MeV; 31P(16O, 16O), E=63 MeV; measured σ(θ). 31,33P, 63Cu levels deduced J-dependence. Enriched targets, magnetic spectrograph. DWBA analysis, spin-orbit forces in heavy-ion optical potentials.
doi: 10.1016/0375-9474(80)90073-1
1979DE16 Z.Phys. A291, 71 (1979) D.Dehnhard, W.Saathoff, T.S.Bhatia, K.Wannebo, C.-A.Wiedner Two-Proton Transfer Reaction 48Ca(18O, 16C)50Ti at 102 MeV NUCLEAR REACTIONS 48Ca(18O, 16C), (18O, 17N), E=102 MeV; measured σ(θ); deduced reaction mechanism. DWBA calculations, finite range, recoil effects.
doi: 10.1007/BF01415818
1979DE34 Phys.Rev.Lett. 43, 1091 (1979) D.Dehnhard, S.J.Tripp, M.A.Franey, G.S.Kyle, C.L.Morris, R.L.Boudrie, J.Piffaretti, H.A.Thiessen Pure Neutron and Pure Proton Transitions in Inelastic Scattering of Pions by 13C NUCLEAR REACTIONS 13C(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=162 MeV; measured σ(θ). 13C deduced pure n, p transitions. Shell-model, weak coupling-model configurations.
doi: 10.1103/PhysRevLett.43.1091
1979FR01 Phys.Lett. 81B, 132 (1979) M.A.Franey, V.Shkolnik, D.Dehnhard Elastic Transfer in the Scattering of 16O by 28Si NUCLEAR REACTIONS 28Si(16O, 16O), E=30-60 MeV; measured σ(E, θ); deduced interference of potential scattering, elastic transfer amplitude, Sα.
doi: 10.1016/0370-2693(79)90505-7
1979IV03 Phys.Lett. 82B, 51 (1979) S.Iversen, H.Nann, A.Obst, K.K.Seth, N.Tanaka, C.L.Morris, H.A.Thiessen, K.Boyer, W.Cottingame, C.F.Moore, R.L.Boudrie, D.Dehnhard Neutron-Proton Radius Differences and Isovector Deformations from π+ and π- Inelastic Scattering from 18O NUCLEAR REACTIONS 18O(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=164 MeV; measured σ(θ). 18O levels deduced isovector deformations, neutron-proton radius differences.
doi: 10.1016/0370-2693(79)90423-4
1979KU01 Nucl.Phys. A313, 434 (1979) S.Kubono, T.K.Li, D.Dehnhard, D.A.Lewis, J.F.Petersen, J.L.Artz The 18O(18O, 16O)20O Reaction at 52 MeV NUCLEAR REACTIONS 18O(18O, 16O), 18O(18O, 18O), E(lab)=52 MeV; measured σ(θ). Enriched target. Microscopic analysis, exact finite-range DWBA.
doi: 10.1016/0375-9474(79)90511-6
1978DE09 Phys.Rev.Lett. 40, 1549 (1978) D.Dehnhard, V.Shkolnik, M.A.Franey Parity Dependence of the Heavy-Ion Optical Potential NUCLEAR REACTIONS 28Si(16O, 16O), E=30-65 MeV; calculated σ(E, θ).
doi: 10.1103/PhysRevLett.40.1549
1978DU07 Phys.Rev. C18, 158 (1978) A.Dudek-Ellis, V.Shkolnik, J.L.Artz, D.Dehnhard, P.J.Ellis, H.P.Morsch 30Si(16O, 16O')30Si* Reaction at 60 MeV NUCLEAR REACTIONS 30Si(16O, 16O), (16O, 16O'), E=60 MeV; measured σ(θ). Coupled channels analysis.
doi: 10.1103/PhysRevC.18.158
1978DU10 Phys.Rev. C18, 1039 (1978) A.Dudek-Ellis, V.Shkolnik, D.Dehnhard Coupled Channels Calculations for 28Si + 16O and the Energy Dependence of the Optical Potential NUCLEAR REACTIONS 28Si(16O, 16O), (16O, 16O'), E=45, 55, 63 MeV; analyzed σ(θ). Coupled channels.
doi: 10.1103/PhysRevC.18.1039
1978KU10 Phys.Rev. C18, 1929 (1978) S.Kubono, S.J.Tripp, D.Dehnhard, T.Udagawa, T.Tamura Forbidden Transitions in the 40Ca(15N, 16O)39K Reaction and the L = 1 Problem NUCLEAR REACTIONS 40Ca(15N, 16O), E=60 MeV; measured σ(θ). CCBA, DWBA analyses.
doi: 10.1103/PhysRevC.18.1929
1978SH02 Phys.Lett. 74B, 195 (1978) V.Shkolnik, D.Dehnhard, S.Kubono, M.A.Franey, S.Tripp Potential Description of Elastic Scattering of 28Si + 16O between 45 and 63 MeV NUCLEAR REACTIONS 28Si(16O, 16O), E=45-63 MeV; measured σ(E, θ).
doi: 10.1016/0370-2693(78)90551-8
1977KU04 Phys.Rev.Lett. 38, 817 (1977) S.Kubono, D.Dehnhard, D.A.Lewis, T.K.Li, J.L.Artz, D.J.Weber, P.J.Ellis, A.Dudek-Ellis j Dependence of the (19F, 16O) Reaction and Spin-Orbit Forces in the Heavy-Ion Optical Potential NUCLEAR REACTIONS 28,30Si(19F, 16O), E=60 MeV; measured σ(θ).
doi: 10.1103/PhysRevLett.38.817
1977PE08 Phys.Rev. C15, 1719 (1977) J.F.Petersen, D.Dehnhard, B.F.Bayman Single-Neutron Transfer to 29Si, 41,49Ca, and 55Fe States Induced by the (18O, 17O(g.s.)) And (18O, 17O(0.87 MeV)) Reactions NUCLEAR REACTIONS 28Si, 40,48Ca, 54Fe(18O, 17O), E=50 MeV; measured σ(θ). 17O, 29Si, 41,49Ca, 55Fe levels deduced S.
doi: 10.1103/PhysRevC.15.1719
1976DE03 Phys.Rev. C13, 164 (1976) D.Dehnhard, J.L.Artz, D.J.Weber, V.Shkolnik, R.M.DeVries 29,30Si(16O, 15N) Proton Stripping Reaction at 60 MeV NUCLEAR REACTIONS 29,30Si(16O, 15N), E=60 MeV; measured σ(E(15N), θ). 30,31P levels deduced S.
doi: 10.1103/PhysRevC.13.164
1976DY01 Phys.Rev. C13, 80 (1976) Single Proton Transfer to 29,30P States NUCLEAR REACTIONS 28,29,30Si(3He, 3He), E=25 MeV; measured σ(θ); deduced optical model parameters. 28,29Si(3He, d), E=25 MeV; measured σ(Ed, θ). 29,30P deduced levels, J, π, T, S, L. Enriched target.
doi: 10.1103/PhysRevC.13.80
1976LI01 Phys.Rev. C13, 55 (1976) T.K.Li, D.Dehnhard, R.E.Brown, P.J.Ellis Investigation of the (d, 5/2)2 and (d5/2s1/2) Two-Particle Configurations in 18O Using the 17O(d, p)18O Reaction at 18 MeV NUCLEAR REACTIONS 17O(d, d), E=18.0 MeV; measured σ(θ); deduced optical model parameters. 17O(d, p), E=18.0 MeV; measured σ(Ep, θ). 18O levels deduced L, S. Enriched target.
doi: 10.1103/PhysRevC.13.55
1976PE01 Phys.Rev.Lett. 36, 307 (1976) J.F.Petersen, D.A.Lewis, D.Dehnhard, H.P.Morsch, B.F.Bayman Two-Neutron Stripping Reaction (18O, 16O) on 48Ca NUCLEAR REACTIONS 48Ca(18O, 16O), E=50 MeV; measured σ(E(16O), θ). DWBA analysis.
doi: 10.1103/PhysRevLett.36.307
1975MO09 Phys.Rev.Lett. 34, 1527 (1975); Erratum Phys.Rev.Lett. 35, 192 (1975) H.P.Morsch, D.Dehnhard, T.K.Li Strong Polarization of the 1p-Shell Core in the Lowest 0+ States of 24Mg and 28Si NUCLEAR REACTIONS 24Mg, 28Si(α, α'), E=23.5 MeV; measured σ(Eα', θ). 24Mg, 28Si levels deduced E0 matrix elements, S.
doi: 10.1103/PhysRevLett.34.1527
1975WE14 Nucl.Instrum.Methods 124, 317 (1975) D.J.Weber, N.M.Hintz, D.Dehnhard Equilibrium Charge-State Distributions for 16O Ions at 20-65 MeV NUCLEAR REACTIONS Au(16O, 16O), E=20-65 MeV; measured charge-state distribution.
doi: 10.1016/0029-554X(75)90578-9
1974DE36 Nucl.Phys. A230, 393 (1974) Proton Occupation Numbers for 44Ca NUCLEAR REACTIONS 44Ca(d, 3He), E=19.0 MeV; measured σ(E(3He), θ). 43K deduced levels, L, π, partial strengths. Enriched target.
doi: 10.1016/0375-9474(74)90145-6
1974HO30 Nucl.Phys. A233, 361 (1974) H.Ho, W.Dunnweber, D.Dehnhard, K.Mudersbach, J.P.Wurm Study of the (12C, 8Be(g.s.)) Reaction and Four-Nucleon Transfer on 24Mg NUCLEAR REACTIONS 24Mg(12C, 8Be), 12C(12C, 2α), E=31.8 MeV; measured αα-coin; deduced σ(E(8Be), θ). 28Si deduced levels.
doi: 10.1016/0375-9474(74)90462-X
1973DE23 Z.Phys. 260, 247 (1973) A.v.d.Decken, M.Goldschmidt, A.Heusler, H.V.Klapdor, W.Reiter, D.Rieck, W.Saathoff, C.A.Wiedner, D.Dehnhard Study of the Ground State Doublet in 57Fe NUCLEAR REACTIONS 56Fe(d, p), E=10.25 MeV; measured σ(Ep). 57Fe deduced levels, S.
doi: 10.1007/BF01395983
1973KR20 Nucl.Phys. A216, 549 (1973) T.P.Krick, N.M.Hintz, D.Dehnhard The Distribution of Electric Multipole Strength in 19F from Inelastic Scattering of 25 MeV α-Particles NUCLEAR REACTIONS 19F(α, α'), (α, α), E=25.0 MeV; measured σ(θ). Deduced optical potential. 19F levels deduced J, π, β(L) deformation parameters by DWBA, coupled channels analyses. Natural target.
doi: 10.1016/0375-9474(73)90169-3
1973MA06 Nucl.Phys. A202, 497 (1973) H.Mackh, H.Oeschler, G.J.Wagner, D.Dehnhard, H.Ohnuma Energy Levels in 30Si from the 29Si(d, p)30Si Reaction NUCLEAR REACTIONS 29Si(d, p), E=11.5, 16.0, 20.0 MeV, measured σ(P)(θ). 30Si deduced levels, J, π, S. Enriched target.
doi: 10.1016/0375-9474(73)90638-6
1972DE14 Phys.Lett. 38B, 389 (1972) Possible Solution to the 27Al Puzzle NUCLEAR STRUCTURE 27Al; calculated levels, B(E2), S for (p, d), (d, 3He). Coriolis band-mixing model.
doi: 10.1016/0370-2693(72)90163-3
1972VO18 Phys.Lett. 41B, 477 (1972) A.Von der Decken, D.Dehnhard, M.Goldschmidt, W.Reiter, D.Rieck, W.Saathoff, C.-A.Wiedner The d3/2 Hole Strength in the Ground State of 44Ca NUCLEAR REACTIONS 44Ca(3He, d), E=24 MeV; measured σ(Ed, θ); deduced d3/2 hold state transition strength.
doi: 10.1016/0370-2693(72)90679-X
1971BE29 Nucl.Phys. A168, 151 (1971) F.D.Becchetti, D.Dehnhard, T.G.Dzubay Coulomb Displacement Energies for 1f-2p Shell Nuclei NUCLEAR REACTIONS 42,43,44,46,48Ca, 45Sc, 46,47,48,49,50Ti, 51V, 50,52,53,54Cr, 55Mn, 54,56,57,58Fe, 59Co, 58,60,61,62,64Ni, 63,65Cu, 64,66,67,68Zn(3He, t), E=24.6 MeV; measured σ(Et, θ), Q(IAS). Ca-Sc, Sc-Ti, Ti-V, V-Cr, Cr-Mn, Mn-Fe, Fe-Co, Co-Ni, Ni-Cu, Zn-Ga, Cu-Zn isotopes deduced Coulomb displacement energies. Enriched, natural targets. Magnetic particle spectrometer, position-sensitive detector.
doi: 10.1016/0375-9474(71)90656-7
1970DE06 Phys.Rev. C1, 460 (1970) Octupole and Quadrupole Transition Rates in F19 from Scattering of 15-MeV Deuterons NUCLEAR REACTIONS 19F(d, d), (d, d'), E=15 MeV; measured σ(Ed', θ). 19F levels deduced B(EL), β(L).
doi: 10.1103/PhysRevC.1.460
1970DE31 Phys.Rev. C2, 1390 (1970) Study of Energy Levels of 29Si NUCLEAR REACTIONS 30Si(3He, α), E=12 MeV; measured σ(Eα, θ). 29Si deduced levels, L(n), S.
doi: 10.1103/PhysRevC.2.1390
1970DZ01 Nucl.Phys. A142, 488 (1970) T.G.Dzubay, R.Sherr, F.D.Becchetti, Jr., D.Dehnhard Isospin Mixing for Bound Analog States in 56Co and 58Co NUCLEAR REACTIONS 54,56,58Fe(3He, t), E=24.6 MeV; measured σ(Et, θ). 56,58Co deduced analog states, J, π, isospin mixing.
doi: 10.1016/0375-9474(70)90807-9
1969DE10 Phys.Rev. 180, 967 (1969); Erratum Phys.Rev. C1, 366 (1970) D.Dehnhard, N.Williams, J.L.Yntema B11(He3, α)B10 Reaction at 33 MeV NUCLEAR REACTIONS 11B(3He, α), E=33 MeV; measured σ(Eα, θ). 10B levels deduced S.
doi: 10.1103/PhysRev.180.967
1968DZ03 COO-1265-67, p.136 (1968) T.G.Dzubay, F.D.Becchetti, D.Dehnhard (He3, t) Reactions on Several Isotopes Within the f7/2 Shell NUCLEAR REACTIONS 50,52,53,54Cr, 54,56,57,58Fe, 46,47,48,49,50Ti(3He, t), E=24.6 MeV; measured σ(Et). 50,53,54Mn, 54,56,57,58Co, 46,47,48,49,50V deduced isobaric analog, Coulomb displacement energies.
1967DE04 Phys.Rev. 155, 1261 (1967) Evidence for Target-Excitation Effects in a Single-Particle-Transfer Reaction NUCLEAR STRUCTURE 25Mg; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.155.1261
1967DE06 Nucl.Phys. A97, 164(1967) The 25Mg(3He, α) Reaction at E(3He) = 33.0 MeV NUCLEAR REACTIONS 25Mg(3He, 3He), E = 33 MeV; measured σ(θ). 25Mg(3He, α), E = 33 MeV; measured σ(Eα, θ); deduced L. 24Mg levels deduced S. Enriched target.
doi: 10.1016/0375-9474(67)90776-2
1967DE10 Phys.Rev. 160, 964 (1967) Neutron-Pickup Reactions on Mg26 NUCLEAR STRUCTURE 25Mg; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.160.964
1967DE14 Nucl.Phys. A104, 202(1967) D.Dehnhard, D.S.Gemmell, Z.Vager Heavy-Particle Emission from the Reactions 19F+d and 19F+3He NUCLEAR REACTIONS 19F(d, 6Li), 19F(d, 9Be), 19F(3He, 10B), E=7.5-13.0 MeV; measured σ(E, θ); deduced reaction mechanism.
doi: 10.1016/0375-9474(67)90764-6
1967DE17 Phys.Rev. 163, 1198 (1967) Neutron Pickup Reactions on Si30 NUCLEAR STRUCTURE 29Si; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.163.1198
1965SI21 ANL-7108, p.31(1965) R.H.Siemssen, T.H.Braid, D.Dehnhard, B.Zeidman Scattering of Charged Particles NUCLEAR STRUCTURE 58Ni, 60Ni, 62Ni, 64Ni; measured not abstracted; deduced nuclear properties.
1961DE29 Proc.Rutherford Jubilee Intern.Conf., Manchester, England, J.B.Birks, Ed., Academic Press Inc., New York, p.821 (1961) Evidence for Three Alpha Particle Break-Up of C12* (16.11 MeV) NUCLEAR STRUCTURE 11B; measured not abstracted; deduced nuclear properties.
1961DE31 Z.Naturforsch. 16a, 1245 (1961) Drei-Alpha-Zerfall von C12*(16, 11, MeV) NUCLEAR STRUCTURE 11B; measured not abstracted; deduced nuclear properties.
doi: 10.1515/zna-1961-1125
Back to query form |