NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = H.Clark Found 54 matches. 2022BU13 Phys.Rev. C 105, 045805 (2022) S.Burcher, K.A.Chipps, R.O.Hughes, C.S.Reingold, A.Saastamoinen, J.T.Harke, N.Cooper, S.Ahn, J.M.Allmond, H.Clark, J.A.Cizewski, M.R.Hall, J.Hooker, H.Jayatissa, K.L.Jones, S.Ota, S.D.Pain, K.Schmidt, A.Simon, S.Upadhyayula Developing the32S(p, d)31S*(p)(γ) reaction to probe the 30P(p, γ)31S reaction rate in classical novae NUCLEAR REACTIONS 32S(p, d), E=33 MeV; measured reaction products, Ep, Ip, Eγ, Iγ, deuteron spectra, (deuteron)p-coin, (particle)γ-coin, angular distributions; deduced s(θ). 31S; deduced levels, J, π, proton decay width of excited states, proton decay branching ratios. DWBA analysis. Comparison to other experimental data. Discussed relevance to resonances investigations in astrophysically important 30P(p, γ) reaction. Hyperion setup consisting of 12 Compton-suppressed HPGe clover detectors, a silicon telescope downstream of the target, and a single silicon detector upstream of the target at K150 cyclotron (Texas A-M Cyclotron Institute).
doi: 10.1103/PhysRevC.105.045805
2014AL05 Phys.Rev. C 89, 025809 (2014) T.Al-Abdullah, F.Carstoiu, X.Chen, H.L.Clark, C.A.Gagliardi, Y.-W.Lui, A.Mukhamedzhanov, G.Tabacaru, Y.Tokimoto, L.Trache, R.E.Tribble, Y.Zhai Astrophysical reaction rate for 17F(p, γ)18Ne from the transfer reaction 13C(17O, 18O)12C NUCLEAR REACTIONS 13C(17O, 18O), 12C(18O, 18O), E=12 MeV/nucleon; measured particle spectra using multipole dipole-multipole (MDM) magnetic spectrometer, σ(θ) at Texas A and M facility. 18O; deduced levels, J, asymptotic normalization coefficients (ANCs) of ground state, first two 2+ states and first 4+ state. 17F(p, γ)18Ne, at T9=0.1-1; deduced reaction rates, astrophysical S factor from mirror analogy of states in 18O and 18Ne. Optical model parameters and DWBA analysis. Discussed production of 18F at stellar energies in ONe novae.
doi: 10.1103/PhysRevC.89.025809
2010AL10 Phys.Rev. C 81, 035802 (2010) T.Al-Abdullah, F.Carstoiu, X.Chen, H.L.Clark, C.Fu, C.A.Gagliardi, Y.-W.Lui, A.Mukhamedzhanov, G.Tabacaru, Y.Tokimoto, L.Trache, R.E.Tribble Stellar reaction rate for 22Mg+p → 23Al from the asymptotic normalization coefficient in the mirror nuclear system 22Ne+n → 23Ne NUCLEAR REACTIONS 13C(12C, 13C), (12C, 12C), E=10.6 MeV/nucleon; 12C(22Ne, 22Ne), (22Ne, 22Ne'), 13C(22Ne, 22Ne), (22Ne, 23Ne), E=12 MeV/nucleon; measured particle spectra, σ and σ(θ); deduced optical model parameters and asymptotic normalization coefficients (ANC). 22Mg(p, γ); deduced direct and resonant capture rates, and effect on the depletion of 22Na in O-Ne Novae.
doi: 10.1103/PhysRevC.81.035802
2009CH06 Phys.Rev. C 79, 024320 (2009) X.Chen, Y.-W.Lui, H.L.Clark, Y.Tokimoto, D.H.Youngblood Giant resonances in 116Sn from 240 MeV 6Li scattering NUCLEAR REACTIONS 116Sn(6Li, 6Li'), E=240 MeV; measured 6Li spectra, angular distributions, cross sections. 116Sn; deduced energies, widths, energy weighted sum strength distributions for isoscalar E0, E1, E2, E3 giant resonances using double-folding model analysis. DWBA analysis of angular distributions. Comparison with corresponding data from inelastic α scattering.
doi: 10.1103/PhysRevC.79.024320
2009CH33 Phys.Rev. C 80, 014312 (2009) X.Chen, Y.-W.Lui, H.L.Clark, Y.Tokimoto, D.H.Youngblood Giant resonances in 24Mg and 28Si from 240 MeV 6Li scattering NUCLEAR REACTIONS 24Mg, 28Si(6Li, 6Li), (6Li, 6Li'), E=240 MeV; measured particle spectra, σ and σ(θ); deduced optical potential model parameters using two folding model potentials and a Woods-Saxon potential. 24Mg, 28Si; deduced E0, E1, E2 and E3 giant resonance strength distributions, multipole parameters, B(E2) and B(E3) probabilities for first 2+ and 3- states. Comparisons with distorted-wave Born approximation (DWBA) calculations and earlier α scattering and 6Li scattering data.
doi: 10.1103/PhysRevC.80.014312
2009YO09 Phys.Rev. C 80, 064318 (2009) D.H.Youngblood, Y.-W.Lui, X.F.Chen, H.L.Clark Isoscalar giant resonance strength in 24Mg NUCLEAR REACTIONS 24Mg(α, α'), E=240 MeV; measured Eα, Iα, σ(θ); deduced strength distributions, widths, EWSR and other parameters for isoscalar E0-GMR, E1-GDR, E2-GQR and E3-GOR giant excitations in 9-60 MeV region, DWBA analysis.
doi: 10.1103/PhysRevC.80.064318
2007CH76 Phys.Rev. C 76, 054606 (2007) X.Chen, Y.-W.Lui, H.L.Clark, Y.Tokimoto, D.H.Youngblood Folding model analysis of 240 MeV 6Li elastic scattering on 116Sn and inelastic scattering to low-lying states of 116Sn NUCLEAR REACTIONS 116Sn(6Li, 6Li'), E=240 MeV; measured particle spectra, angular distributions, cross sections; deduced B(E2), B(E3). Comparison with 90Zr. 116Sn; deduced J, π. DWBA calculations.
doi: 10.1103/PhysRevC.76.054606
2007CH91 Phys.Rev. C 76, 54606 (2007) X.Chen, Y.W.Lui, H.L.Clark, Y.Tokimoto, D.H.Youngblood Folding model analysis of 240 MeV 6Li elastic scattering on 116Sn and inelastic scattering to low-lying states of 116Sn NUCLEAR REACTIONS 116Sn(6Li, 6Li), 116Sn(6Li, 6Li'), E=240 MeV; measured products, 116Sn; deduced σ(θ). Data were imported from EXFOR entry C1587.
doi: 10.1103/PhysRevC.76.054606
2007YO02 Phys.Rev. C 76, 027304 (2007) D.H.Youngblood, Y.-W.Lui, H.L.Clark Isoscalar giant resonance strength in 28Si NUCLEAR REACTIONS 28Si(α, α'), E=240 MeV; analyzed σ, and angular distributions. Deduced giant resonance strength.
doi: 10.1103/PhysRevC.76.027304
2006LU01 Phys.Rev. C 73, 014314 (2006) Y.-W.Lui, D.H.Youngblood, H.L.Clark, Y.Tokimoto, B.John Isoscalar giant resonances for nuclei with mass between 56 and 60 NUCLEAR REACTIONS 56Fe, 60Ni(α, α'), E=240 MeV; measured Eα, σ(θ). 58Ni(α, α'), E=240 MeV; analyzed Eα, σ(θ). 56Fe, 58,60Ni deduced isoscalar strength distributions, giant resonance parameters.
doi: 10.1103/PhysRevC.73.014314
2006TO10 Phys.Rev. C 74, 044308 (2006) Y.Tokimoto, Y.-W.Lui, H.L.Clark, B.John, X.Chen, D.H.Youngblood Giant resonances in 46, 48Ti NUCLEAR REACTIONS 46,48Ti(α, α'), E=240 MeV; measured Eα, σ(E, θ). 46,48Ti deduced isoscalar monopole, dipole, and quadrupole strength distributions, resonance features.
doi: 10.1103/PhysRevC.74.044308
2005LU06 Acta Phys.Pol. B36, 1107 (2005) Y.-W.Lui, D.H.Youngblood, H.L.Clark, Y.Tokimoto, B.John Giant monopole resonance in Cd and Sn isotopes NUCLEAR REACTIONS 110,116Cd, 112,124Sn(α, α'), E=240 MeV; measured Eα, σ(θ). 110,116Cd, 112,124Sn deduced electric monopole strength distributions, resonance parameters. Comparison with model predictions.
2004LU04 Nucl.Phys. A731, 28 (2004) Y.-W.Lui, X.Chen, H.L.Clark, B.John, Y.Tokimoto, D.H.Youngblood Isoscalar giant dipole resonance for several nuclei with A ≥ 90 NUCLEAR REACTIONS 90Zr, 144Sm, 208Pb(α, α'), E=240 MeV; measured Eα, Iα, σ(θ). 90Zr, 144Sm, 208Pb deduced isoscalar GDR strength functions, related features.
doi: 10.1016/j.nuclphysa.2003.11.016
2004LU05 Phys.Rev. C 69, 034611 (2004) Y.-W.Lui, D.H.Youngblood, Y.Tokimoto, H.L.Clark, B.John Isoscalar multipole strength in 110Cd and 116Cd NUCLEAR REACTIONS 110,116Cd(α, α'), E=240 MeV; measured Eα, σ(E, θ). 110,116Cd deduced giant resonance features, multipole strength distributions.
doi: 10.1103/PhysRevC.69.034611
2004LU14 Phys.Rev. C 70, 014307 (2004) Y.-W.Lui, D.H.Youngblood, Y.Tokimoto, H.L.Clark, B.John Giant resonances in 112Sn and 124Sn: Isotopic dependence of monopole resonance energies NUCLEAR REACTIONS 112,124Sn(α, α'), E=240 MeV; measured Eα, σ(E, θ). 112,124Sn deduced isoscalar giant resonance strength distributions. Comparison with model predictions.
doi: 10.1103/PhysRevC.70.014307
2004YO02 Phys.Rev. C 69, 034315 (2004) D.H.Youngblood, Y.-W.Lui, H.L.Clark, B.John, Y.Tokimoto, X.Chen Isoscalar E0 - E3 strength in 116Sn, 144Sm, 154Sm, and 208Pb NUCLEAR REACTIONS 116Sn, 144,154Sm, 208Pb(α, α'), E=240 MeV; measured Eα, σ(E, θ). 116Sn, 144,154Sm, 208Pb deduced giant resonance energies, widths, isoscalar strength distributions.
doi: 10.1103/PhysRevC.69.034315
2004YO05 Phys.Rev. C 69, 054312 (2004) D.H.Youngblood, Y.-W.Lui, B.John, Y.Tokimoto, H.L.Clark, X.Chen Compression mode resonances in 90Zr NUCLEAR REACTIONS 90Zr(α, α'), E=240 MeV; measured Eα, σ(E, θ). 90Zr deduced isoscalar giant resonance energies, widths.
doi: 10.1103/PhysRevC.69.054312
2003JO07 Phys.Rev. C 68, 014305 (2003) B.John, Y.Tokimoto, Y.-W.Lui, H.L.Clark, X.Chen, D.H.Youngblood Isoscalar electric multipole strength in 12C NUCLEAR REACTIONS 12C(α, α), (α, α'), E=240 MeV; measured Eα, σ(θ), σ(E, θ). 12C deduced transitions B(EL), energy-weighted sum rules. Folding model analysis.
doi: 10.1103/PhysRevC.68.014305
2003TR04 Phys.Rev. C 67, 062801 (2003) L.Trache, A.Azhari, F.Carstoiu, H.L.Clark, C.A.Gagliardi, Y.-W.Lui, A.M.Mukhamedzhanov, X.Tang, N.Timofeyuk, R.E.Tribble Asymptotic normalization coefficients for 8B → 7Be + p from a study of 8Li → 7Li + n NUCLEAR REACTIONS 13C(7Li, 8Li), E=63 MeV; measured σ(θ); deduced spectroscopic factors, asymptotic normalization coefficients. 7Be(p, γ), E=low; deduced astrophysical S-factor.
doi: 10.1103/PhysRevC.67.062801
2003YO11 Phys.Rev. C 68, 057303 (2003) D.H.Youngblood, Y.-W.Lui, H.L.Clark, Y.Tokimoto, B.John Isoscalar E0 strength between 6 and 11 MeV in 40Ca NUCLEAR REACTIONS 40Ca(α, α'), E=240 MeV; measured Eα, σ(θ). 40Ca deduced isoscalar E0 strength distribution.
doi: 10.1103/PhysRevC.68.057303
2002YO01 Phys.Rev. C65, 034302 (2002) D.H.Youngblood, Y.-W.Lui, H.L.Clark Isoscalar Giant Resonances in 28Si and the Mass Dependence of Nuclear Compressibility NUCLEAR REACTIONS 28Si(α, α'), E=240 MeV; measured Eα, σ(θ). 28Si deduced isoscalar giant resonance features, multipole strength distributions. Mass dependence of nuclear compressibility discussed.
doi: 10.1103/PhysRevC.65.034302
2001BR17 Nucl.Phys. A688, 659 (2001) M.E.Brandan, A.Menchaca-Rocha, L.Trache, H.L.Clark, A.Azhari, C.A.Gagliardi, Y.-W.Lui, R.E.Tribble, R.L.Varner, J.R.Beene, G.R.Satchler Refractive Elastic Scattering of 16O by 12C at 300 MeV NUCLEAR REACTIONS 12C(16O, 16O), (16O, 12C), E=300 MeV; measured σ(θ); deduced optical model parameters, potential characteristics. Airy structure, nuclear rainbow.
doi: 10.1016/S0375-9474(00)00588-1
2001CL01 Phys.Rev. C63, 031301 (2001) H.L.Clark, Y.-W.Lui, D.H.Youngblood Isoscalar Giant Resonance in 90Zr, 116Sn, and 208Pb NUCLEAR REACTIONS 90Zr, 116Sn, 208Pb(α, α'), E=240 MeV; measured α spectrum, σ(θ). 90Zr, 116Sn, 208Pb deduced GDR components. DWBA analysis. Comparison with Random Phase approximations Hartree-Fock calculations.
doi: 10.1103/PhysRevC.63.031301
2001CL03 Nucl.Phys. A687, 80c (2001) H.L.Clark, Y.-W.Lui, D.H.Youngblood Sensitivity of the Isoscalar Giant Dipole Resonance to Optical Potentials NUCLEAR REACTIONS 90Zr, 144Sm, 208Pb(α, α), (α, α'), E=240 MeV; measured σ(θ); deduced optical model parameters, isoscalar and isovector GDR σ. DWBA.
doi: 10.1016/S0375-9474(01)00604-2
2001GA19 Nucl.Phys. A682, 369c (2001) C.A.Gagliardi, A.Azhari, P.Bem, V.Burjan, F.Carstoiu, J.Cejpek, H.L.Clark, V.Kroha, Y.-W.Lui, A.M.Mukhamedzhanov, J.Novak, S.Piskor, A.Sattarov, E.Simeckova, X.Tang, L.Trache, R.E.Tribble, J.Vincour Asymptotic Normalization Coefficients from Direct Transfer Reactions and Astrophysical S Factors NUCLEAR REACTIONS 10B, 14N(7Be, 7Be), (7Be, 8B), E=12 MeV/nucleon; measured σ(θ). 7Be(p, γ), E not given; deduced asymptotic nomalization coefficients, astrophysical capture rate. Other reactions discussed.
doi: 10.1016/S0375-9474(00)00662-X
2001LU18 Phys.Rev. C64, 064308 (2001) Y.-W.Lui, H.L.Clark, D.H.Youngblood Giant Resonances in 16O NUCLEAR REACTIONS 16O(α, α'), E=240 MeV; measured Eα, σ(E, θ). 16O deduced giant resonance strength distributions.
doi: 10.1103/PhysRevC.64.064308
2001YO07 Phys.Rev. C63, 067301 (2001); Erratum Phys.Rev. C64, 049901 (2001) D.H.Youngblood, Y.-W.Lui, H.L.Clark Isoscalar E0, E1, and E2 Strength in 40Ca NUCLEAR REACTIONS 40Ca(α, α'), E=240 MeV; measured Eα, σ(θ). 40Ca deduced E0, E1, E2 strength distributions, giant resonance features.
doi: 10.1103/PhysRevC.63.067301
2000LU09 Phys.Rev. C61, 067307 (2000) Y.-W.Lui, H.L.Clark, D.H.Youngblood Giant Monopole Strength in 58Ni NUCLEAR REACTIONS 58Ni(α, α'), E=240 MeV; measured α spectra, σ(θ). 58Ni deduced giant monopole resonance strength distribution.
doi: 10.1103/PhysRevC.61.067307
2000TR01 Phys.Rev. C61, 024612 (2000) L.Trache, A.Azhari, H.L.Clark, C.A.Gagliardi, Y.-W.Lui, A.M.Mukhamedzhanov, R.E.Tribble, F.Carstoiu Optical Model Potentials Involving Loosely Bound p-Shell Nuclei Around 10 MeV/nucleon NUCLEAR REACTIONS 9Be(10B, 10B), E=100 MeV; 9Be(13C, 13C), E=130 MeV; 13C(14N, 14N), E=162 MeV; 9Be, 13C(7Li, 7Li), E=63, 130 MeV; measured σ(θ); deduced optical model parameters. 10B, 14N(7Be, X), 9Be, 13C(8B, X), E ≈ 80 MeV; deduced optical model potentials. Semi-microscopic double folding analysis with various effective interactions.
doi: 10.1103/PhysRevC.61.024612
1999CL05 Nucl.Phys. A649, 57c (1999) H.L.Clark, Y.-W.Lui, D.H.Youngblood, K.Bachtr, U.Garg, M.N.Harakeh, N.Kalantar-Nayestanaki Isoscalar Giant Dipole Resonance in 90Zr, 116Sn, 144Sm and 208Pb Excited by 240 MeV α-Particle Scattering NUCLEAR REACTIONS 90Zr, 116Sn, 144Sm, 208Pb(α, α'), E=240 MeV; measured α spectra, σ(θ). 90Zr, 116Sn, 144Sm, 208Pb deduced isoscalar GDR energies, widths.
doi: 10.1016/S0375-9474(99)00039-1
1999GA03 Phys.Rev. C59, 1149 (1999) C.A.Gagliardi, R.E.Tribble, A.Azhari, H.L.Clark, Y.-W.Lui, A.M.Mukhamedzhanov, A.Sattarov, L.Trache, V.Burjan, J.Cejpek, V.Kroha, S.Piskor, J.Vincour Tests of Transfer Reaction Determinations of Astrophysical S Factors NUCLEAR REACTIONS 16O(3He, d), E=29.75 MeV; measured σ(E, θ); deduced asymptotic normalization coefficients. 16O(p, γ), E=0.2-1.4 MeV; calculated astrophysical S factors.
doi: 10.1103/PhysRevC.59.1149
1999TR12 Pramana 53, 585 (1999) R.E.Tribble, A.Azhari, H.L.Clark, C.A.Gagliardi, Y.-W.Lui, A.M.Mukhamedzhanov, A.Sattaroy, X.Tang, L.Trache, V.Burjan, J.Cejpek, V.Kroha, S.Piskor, J.Vincour, F.Carstoiu Astrophysical S-Factors from Asymptotic Normalization Coefficients
doi: 10.1007/s12043-999-0035-6
1999YO01 Phys.Rev.Lett. 82, 691 (1999) D.H.Youngblood, H.L.Clark, Y.-W.Lui Incompressibility of Nuclear Matter from the Giant Monopole Resonance NUCLEAR REACTIONS 90Zr, 116Sn, 144Sm, 208Pb(α, α'), E=240 MeV; measured α spectra, σ(Ex) at small angles. 90Zr, 116Sn, 144Sm, 208Pb deduced giant monopole resonance centroids, E0 strength distributions, nuclear matter compression modulus. Comparison with previous data. Microscopic calculations with Gogny interaction.
doi: 10.1103/PhysRevLett.82.691
1999YO04 Nucl.Phys. A649, 49c (1999) D.H.Youngblood, H.L.Clark, Y.-W.Lui Compressibility of Nuclear Matter from the Giant Monopole Resonance NUCLEAR REACTIONS 90Zr, 116Sn, 144Sm, 208Pb(α, α'), E=240 MeV; measured α spectra, σ(θ). 90Zr, 116Sn, 144Sm, 208Pb deduced giant monopole resonance energies, widths, incompressibility. Comparison with model predictions.
doi: 10.1016/S0375-9474(99)00038-X
1999YO05 Phys.Rev. C60, 014304 (1999) D.H.Youngblood, Y.-W.Lui, H.L.Clark Giant Resonances in 24Mg NUCLEAR REACTIONS 24Mg(α, α'), E=240 MeV; measured Eα, σ(E, θ). 24Mg deduced levels B(λ), giant resonance features, monopole strength distribution.
doi: 10.1103/PhysRevC.60.014304
1999YO07 Phys.Rev. C60, 067302 (1999) D.H.Youngblood, Y.-W.Lui, H.L.Clark Splitting of the Giant Monopole and Quadrupole Resonances in 154Sm NUCLEAR REACTIONS 154Sm(α, α'), E=240 MeV; measured Eα, Iα, σ(θ). 154Sm deduced strength functions for giant monopole, quadrupole resonances. Comparison with model predictions.
doi: 10.1103/PhysRevC.60.067302
1998CL02 Phys.Rev. C57, 2887 (1998) H.L.Clark, Y.-W.Lui, D.H.Youngblood Folding Model Analysis of the Excitation of Low-Lying States and the High Energy Octupole Resonance in 116Sn by 240 MeV Alpha Scattering NUCLEAR REACTIONS 116Sn(α, α), (α, α'), E=240 MeV; measured σ(θ); deduced transition rates, sum rule strength for high energy octupole resonance, optical model parameters. Deformed potential, folding model analysis.
doi: 10.1103/PhysRevC.57.2887
1998MU09 Nucl.Phys. A631, 788c (1998) A.M.Mukhamedzhanov, H.L.Clark, H.Dejbakhsh, C.A.Gagliardi, Y.-W.Lui, L.Trache, R.E.Tribble, H.M.Xu, V.Burjan, J.Cejpek, V.Kroha, S.Piskor, J.Vincour, F.Carstoiu, A.Sattarov Asymptotic Normalization Coefficients and Astrophysical Radiative Capture Reactions NUCLEAR REACTIONS 9Be(10B, 9Be), E=100 MeV; 16O(3He, d), E=29.75 MeV; measured σ(θ); deduced virtual decays asymptotic normalization coefficients. 16O(p, γ), E < 2.5 MeV; deduced S-factor.
doi: 10.1016/S0375-9474(98)00110-9
1998TR04 Phys.Rev. C58, 2715 (1998) L.Trache, A.Azhari, H.L.Clark, C.A.Gagliardi, Y.-W.Lui, A.M.Mukhamedzhanov, R.E.Tribble, F.Carstoiu Asymptotic Normalization Coefficients for 13C + p → 14N NUCLEAR REACTIONS 13C(14N, 14N), (14N, 13C), E=162 MeV; measured σ(θ); deduced optical model parameters. 14N deduced asymptototic normalization coefficients for ground, excited states. DWBA analysis.
doi: 10.1103/PhysRevC.58.2715
1998YO01 Phys.Rev. C57, 1134 (1998) D.H.Youngblood, H.L.Clark, Y.-W.Lui Giant Monopole Resonance Strength in 28Si NUCLEAR REACTIONS 28Si(α, α), (α, α'), E=240 MeV; measured σ(E, θ); deduced optical model parameters. 28Si deduced giant monopole resonance strength distribution, related features.
doi: 10.1103/PhysRevC.57.1134
1998YO02 Phys.Rev. C57, 2748 (1998) D.H.Youngblood, Y.-W.Lui, H.L.Clark High Lying E0 Strength in 12C NUCLEAR REACTIONS 12C(α, α'), E=240 MeV; measured σ(Ex, θ). 12C deduced levels, E0 continuum strength distribution.
doi: 10.1103/PhysRevC.57.2748
1997MA25 Phys.Rev.Lett. 78, 4343 (1997) M.May, D.Alburger, S.Bart, R.Chrien, R.Sawafta, M.Deutsch, V.Lia, S.W.Wissink, J.Lisantti, S.P.Wells, S.M.Bowyer, W.A.Franklin, K.Hicks, H.Clark, R.Michael, L.Lee, H.Funsten, C.Kormanyos, J.Wise, M.B.Barakat, R.Stearns First Observation of the p(Λ) → s(Λ) γ-Ray Transition in 13C(Λ) NUCLEAR REACTIONS 13C(K-, π-), E at 750 MeV/c; measured γ(hypernucleus)-coin, excitation spectra; deduced p(λ) → s(λ) transition in hypernucleus 13C(λ).
doi: 10.1103/PhysRevLett.78.4343
1997MU19 Phys.Rev. C56, 1302 (1997) A.M.Mukhamedzhanov, H.L.Clark, C.A.Gagliardi, Y.-W.Lui, L.Trache, R.E.Tribble, H.M.Xu, X.G.Zhou, V.Burjan, J.Cejpek, V.Kroha, F.Carstoiu Asymptotic Normalization Coefficients for 10B → 9Be + p NUCLEAR REACTIONS 9Be(10B, 9Be), (10B, 10B), E=100 MeV; measured σ(E, θ); deduced optical model parameters, 9Be(10B, 9Be) reaction σ, asymptotic normalization coefficients for 10B → 9Be+p virtual decays. DWBA approach.
doi: 10.1103/PhysRevC.56.1302
1997YO07 Phys.Rev. C55, 2811 (1997) D.H.Youngblood, Y.-W.Lui, H.L.Clark Giant Monopole Resonance Strength in 40Ca NUCLEAR REACTIONS 40Ca(α, α), (α, α'), E=240 MeV; measured σ(θ), spectra; deduced optical model parameters. 40Ca deduced giant monopole strength function, B(λ). Folding model analysis.
doi: 10.1103/PhysRevC.55.2811
1996CL02 Phys.Rev. C54, 72 (1996) H.L.Clark, D.H.Youngblood, Y.-W.Lui High Energy Octupole Resonance in 116Sn NUCLEAR REACTIONS 116Sn(α, α'), E=240 MeV; measured σ(θ). 116Sn deduced giant multipole, octupole resonances, Γ. EWSR strengths, DWBA calculations.
doi: 10.1103/PhysRevC.54.72
1996LU02 Nucl.Phys. A598, 263 (1996) Y.-W.Lui, H.L.Clark, D.H.Youngblood Optical Potentials for 14N on 92Mo and 197Au NUCLEAR REACTIONS 92Mo, 197Au(14N, 14N), E=490 MeV; 92Mo(14N, 14N'), E=490 MeV; measured σ(θ); deduced optical-model parameters. DWBA calculations.
doi: 10.1016/0375-9474(95)00429-7
1996YO02 Nucl.Phys. A599, 387c (1996) D.H.Youngblood, H.L.Clark, Y.-W.Lui Isoscalar Monopole Strength in 56Fe and 58Ni NUCLEAR REACTIONS 56Fe, 58Ni(α, α'), E=240 MeV; measured spectra, σ(θ). 58Ni, 56Fe deduced giant resonances, widths, energy-weighted sum rule strengths related features.
doi: 10.1016/0375-9474(96)00081-4
1996YO03 Phys.Rev.Lett. 76, 1429 (1996) D.H.Youngblood, H.L.Clark, Y.-W.Lui Missing Isoscalar Monopole Strength in 58Ni NUCLEAR REACTIONS 58Ni(α, α'), E=240 MeV; measured σ(θ), spectra. 58Ni deduced giant monopole resonance centroid, isoscalar monopole strength.
doi: 10.1103/PhysRevLett.76.1429
1995CL03 Nucl.Phys. A589, 416 (1995) H.L.Clark, Y.-W.Lui, D.H.Youngblood Alpha Particle Optical Potentials at 240 MeV NUCLEAR REACTIONS 58Ni, 116Sn, 197Au(α, α'), E=240 MeV; measured σ(θ); deduced optical-model parameters. 58Ni, 116Sn, 197Au levels deduced deformation lengths. DWBA calculations.
doi: 10.1016/0375-9474(95)00121-G
1981DO10 Nucl.Phys. A371, 225 (1981) Sr.M.A.Doyle, H.W.Clark, L.J.Dries, J.L.Regner, T.R.Donoghue, G.M.Hale Comparison of Analyzing Power and Polarization in the Reaction 3H(p, n)3He (I). New Analyzing Power Results below 4 MeV NUCLEAR REACTIONS 3H(polarized p, n), E=1.75-4 MeV; measured A(E, θ). 4He deduced levels, J, π, T. Charge-independent R-matrix fits.
doi: 10.1016/0375-9474(81)90065-8
1980DR01 Phys.Rev. C21, 475 (1980) L.J.Dries, H.W.Clark, R.Detoma, Jr., J.L.Regner, T.R.Donoghue A(zz)(0°) for the Charge-Symmetric 3He(d, p)4He and 3H(d, n)4He Reactions below 6.75 MeV NUCLEAR REACTIONS 3He(polarized d, p), 3H(polarized d, n), E=0.24-6.75 MeV; measured tensor analyzing power.
doi: 10.1103/PhysRevC.21.475
1979DE04 Nucl.Phys. A313, 269 (1979) R.Detoma, Jr., H.W.Clark, L.J.Dries, J.L.Regner, T.R.Donoghue Analyzing Power Measurements for p-3He Elastic Scattering from 1.75 to 4.50 MeV NUCLEAR REACTIONS 3He(polarized p, p), E=1.75-4.50 MeV; measured A(Ep, θ). 4He deduced low-lying T=1 level ordering.
doi: 10.1016/0375-9474(79)90499-8
1979DR01 Phys.Lett. 80B, 176 (1979) L.J.Dries, H.W.Clark, R.Detoma, Jr., T.R.Donoghue Comparison of Analyzing Powers for the Charge Symmetric Reactions 2H(d, n)3He and 2H(d, p)3H below 5.5 MeV NUCLEAR REACTIONS 2H(polarized d, n), (polarized d, p), E=0.5-5.5 MeV; measured A(E, θ).
doi: 10.1016/0370-2693(79)90191-6
1976DO07 Phys.Rev.Lett. 37, 981 (1976) T.R.Donoghue, S.M.A.Doyle, H.W.Clark, L.J.Dries, J.L.Regner, W.Tornow, R.C.Byrd, P.W.Lisowski, R.L.Walter Equality of Analyzing Power and Polarization in the Reaction 3H(p, n)3He NUCLEAR REACTIONS 3H(polarized p, n), E < 4 MeV; measured A(θ). 3H(p, n), E < 4 MeV; measured P(θ).
doi: 10.1103/PhysRevLett.37.981
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