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NSR database version of May 24, 2024.

Search: Author = D.H.Youngblood

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2021BO09      Nucl.Phys. A1010, 122159 (2021)

G.Bonasera, S.Shlomo, D.H.Youngblood, Y.-W.Lui, J.Button, X.Chen

Isoscalar and isovector giant resonances in 44Ca, 54Fe, 64, 68Zn and 56, 58, 60, 68Ni

NUCLEAR STRUCTURE 44Ca, 54Fe, 64,68Zn, 56,58,60,68Ni; calculated centroid energies for isoscalar and isovector giant dipole, quadrupole, octupole resonances within the spherical Hartree-Fock (HF)-based random phase approximation (RPA) theory with 33 distinct Skyrme-like effective nucleon-nucleon interactions.

doi: 10.1016/j.nuclphysa.2021.122159
Citations: PlumX Metrics


2019BO16      Nucl.Phys. A992, 121612 (2019)

G.Bonasera, S.Shlomo, D.H.Youngblood, Y.-W.Lui, Krishichayan, J.Button

Isoscalar and isovector giant resonances in 92, 94, 96, 98, 100Mo and 90, 92, 94Zr

NUCLEAR STRUCTURE 92,94,96,98,100Mo, 90,92,94Zr; calculated response function S(E), centroid energies ECEN of the isoscalar and isovector giant resonances of multipolarity, centroid energy vs nuclear matter incompressibility using spherical Hartree-Fock based RPA with Skyrme-type nucleon-nucleon interaction, difference between the centroid energies vs asymmetrycoefficient for each isotope I=(N-Z)/A, ECEN vs m*/m; compared with data; deduced nuclear matter properties, ECEN for ISGMR, for ISGDR, ISGOR, ISGQR, IVGMR, IVGDR, IVGQR.

doi: 10.1016/j.nuclphysa.2019.121612
Citations: PlumX Metrics


2019BU26      Phys.Rev. C 100, 064318 (2019)

J.Button, Y.-W.Lui, D.H.Youngblood, X.Chen, G.Bonasera, S.Shlomo

Isoscalar E0, E1, and E2 strength in 54Fe and 64, 68Zn

NUCLEAR REACTIONS 54Fe, 64,68Zn(α, α'), E=240 MeV; measured Eα, Iα, σ(θ) at the Texas A and M K500 superconducting cyclotron. 54Fe, 64,68Zn; deduced centroid energies, EWSR, widths, strengths and moments of isoscalar E0(ISGMR), E1(ISGDR) and E2(ISGQR) giant resonances using single-folding DWBA calculations with optical model potentials. Comparison with the predictions from HF-RPA calculations using the KDE0v1 Skyrme interaction. Systematics of centroids for E0, E1 and E2 isoscalar giant resonances for 40,44,48Ca, 45,48Ti, 54,56Fe, 56,58,60,68Ni, 64,68Zn.

doi: 10.1103/PhysRevC.100.064318
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Data from this article have been entered in the XUNDL database. For more information, click here.


2017BU16      Phys.Rev. C 96, 054330 (2017)

J.Button, Y.-W.Lui, D.H.Youngblood, X.Chen, G.Bonasera, S.Shlomo

Isoscalar E0, E1, and E2 strength in 44Ca

NUCLEAR REACTIONS 44Ca(α, α'), E=240 MeV; measured Eα, Iα, angular distributions using multipole-dipole-multipole (MDM) spectrometer at Texas A and M K500 superconducting cyclotron. 40Ca; deduced isoscalar giant monopole and quadrupole resonances (ISGMR and ISGQR), widths, E0, E1 and E2 strengths, energy-weighted sum rule (EWSR). Strength distributions compared with the predictions of Hartree-Fock based random phase approximation calculations with the KDE0v1 Skyrme-type interaction.

doi: 10.1103/PhysRevC.96.054330
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Data from this article have been entered in the XUNDL database. For more information, click here.


2016BU19      Phys.Rev. C 94, 034315 (2016)

J.Button, Y.-W.Lui, D.H.Youngblood, X.Chen, G.Bonasera, S.Shlomo

Isoscalar E0, E1, E2, and E3 strength in 94Mo

NUCLEAR REACTIONS 94Mo(α, α'), E=240 MeV; measured Eα, Iα, σ(θ) at Texas A and M K500 cyclotron facility; deduced moments, widths, E0, E1, E2 and E3 strength distributions, EWSR for isoscalar giant resonances. Comparison with spherical Hartree-Fock RPA calculations using KDE0v1 Skyrme-type interaction.

doi: 10.1103/PhysRevC.94.034315
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Data from this article have been entered in the XUNDL database. For more information, click here.


2015KR08      Phys.Rev. C 92, 044323 (2015)

Krishichayan, Y.-W.Lui, J.Button, D.H.Youngblood, G.Bonasera, S.Shlomo

Isoscalar giant resonances in 90, 92, 94Zr

NUCLEAR REACTIONS 90,92,94Zr(α, α'), E=240 MeV; measured inelastic α spectra, σ(θ) distributions using multipole-dipole-multipole (MDM) spectrometer at Texas A and M. 90,92,94Zr; deduced E0 (ISGMR), E1 (ISGDR), E2 (ISGQR) and E3 (ISGOR) isoscalar giant resonances, centroid energies, FWHM, widths, strengths EWSR. Comparison with previous experimental studies. DWBA calculations using density-dependent single-folding model. Systematics of centroid energies, widths and strengths for A=90-100, even-even Mo and Zr isotopes. Comparison of strength distributions with Hartree-Fock based RPA calculations using KDE0v1 Skyrme type interaction.

doi: 10.1103/PhysRevC.92.044323
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2194. Data from this article have been entered in the XUNDL database. For more information, click here.


2015YO04      Phys.Rev. C 92, 014318 (2015)

D.H.Youngblood, Y.-W.Lui, Krishichayan, J.Button, G.Bonasera, S.Shlomo

Isoscalar E0, E1, E2, and E3 strength in 92, 96, 98, 100Mo

NUCLEAR REACTIONS 92,96,98,100Mo(α, α'), E=240 MeV; measured Eα, Iα, angular distributions using multipole-dipole-multipole (MDM) spectrometer and a focal plane detector at Texas A and M K500 superconducting cyclotron facility. DWBA analysis of σ(θ) data. 92,96,98,100Mo; deduced isoscalar giant resonances and E0, E1, E2, and E3 transition strengths and EWSR. Comparison with spherical Hartree-Fock-RPA calculations using KDE0v1 Skyrme-type interaction.

doi: 10.1103/PhysRevC.92.014318
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Data from this article have been entered in the XUNDL database. For more information, click here.


2013AN05      Phys.Rev. C 87, 024303 (2013)

M.R.Anders, S.Shlomo, T.Sil, D.H.Youngblood, Y.-W.Lui, Krishichayan

Giant resonances in 40Ca and 48Ca

NUCLEAR STRUCTURE 40,48Ca; calculated strength functions S(E), centroid energies of isoscalar and isovector (monopole, dipole, quadrupole, and octupole) giant resonances. Self-consistent Hartree-Fock-based random phase approximation calculations with 18 Skyrme-type nucleon-nucleon effective interaction. Comparison with experimental data.

doi: 10.1103/PhysRevC.87.024303
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2013YO07      Phys.Rev. C 88, 021301 (2013)

D.H.Youngblood, Y.-W.Lui, Krishichayan, J.Button, M.R.Anders, M.L.Gorelik, M.H.Urin, S.Shlomo

Unexpected characteristics of the isoscalar monopole resonance in the A ≈ 90 region: Implications for nuclear incompressibility

NUCLEAR REACTIONS 90,92,94Zr, 92,96,98,100Mo(α, α'), E=240 MeV; measured α spectra, σ at low angles using Texas A-M cyclotron facility; deduced energies, centroids, widths, E0-EWSR for isoscalar giant monopole resonances (ISGMR), nuclear incompressibility. Comparison with HF-RPA calculations.

doi: 10.1103/PhysRevC.88.021301
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2093.


2011LU07      Phys.Rev. C 83, 044327 (2011)

Y.-W.Lui, D.H.Youngblood, S.Shlomo, X.Chen, Y.Tokimoto, Krishichayan, M.Anders, J.Button

Isoscalar giant resonances in 48Ca

NUCLEAR REACTIONS 48Ca(α, α'), E=240 MeV; measured Eα, Iα, cross sections, σ(θ) for isoscalar giant resonances. 48Ca; deduced B(E2), B(E3), E0, E1, E2 E3+E4 energy-weighted sum rules (EWSR), isoscalar strength distributions, giant resonances, centroid energies. Comparison with mean-field-based random-phase approximation.

doi: 10.1103/PhysRevC.83.044327
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1845. Data from this article have been entered in the XUNDL database. For more information, click here.


2010KR01      Phys.Rev. C 81, 014603 (2010)

Krishichayan, X.Chen, Y.-W.Lui, Y.Tokimoto, J.Button, D.H.Youngblood

Elastic and inelastic scattering to low-lying states of 58Ni and 90Zr using 240-MeV 6Li

NUCLEAR REACTIONS 58Ni, 90Zr(6Li, 6Li), (6Li, 6Li'), E=240 MeV; measured particle spectra, σ(θ) using multipole dipole-multipole (MDM) magnetic spectrometer. 58Ni, 90Zr; deduced levels, J, π, B(E2) for first 2+, and B(E3) for first 3- states. Comparison with deformed potential (DP) model and density-dependent double-folding (DDF) calculations using M3Y NN effective interaction and phenomenological Woods-Saxon potential.

doi: 10.1103/PhysRevC.81.014603
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1782.


2010KR06      Phys.Rev. C 81, 044612 (2010)

Krishichayan, X.Chen, Y.-W.Lui, J.Button, D.H.Youngblood

Elastic and inelastic scattering of 240-MeV 6Li ions from 40Ca and 48Ca and tests of a systematic optical potential

NUCLEAR REACTIONS 40,48Ca(6Li, 6Li), (6Li, 6Li'), E=240 MeV; measured σ, σ(θ); deduced optical model parameters B(E2) for first 2+ states, B(E3) for first 3- states, isoscalar giant-monopole resonance (ISGMR) strength, EWSR. DWBA analysis. Comparison with theoretical calculations using density-dependent double-folding (DDF) model with M3Y-NN effective interaction.

doi: 10.1103/PhysRevC.81.044612
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1780. Data from this article have been entered in the XUNDL database. For more information, click here.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1687. Data from this article have been entered in the XUNDL database. For more information, click here.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1720. Data from this article have been entered in the XUNDL database. For more information, click here.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1768.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1587. Data from this article have been entered in the XUNDL database. For more information, click here.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1439.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1507.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1107.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1108.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1104.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1114.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1109.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1105.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1110.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1115.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1112.


2001YO06      Nucl.Phys. A687, 1c (2001)

D.H.Youngblood

Isoscalar Giant Resonances and Nuclear Matter Compressibility

NUCLEAR REACTIONS 28Si, 40Ca, 90Zr, 116Sn, 144Sm, 208Pb(α, α'), E=240 MeV; measured excitation energy spectra, σ(θ) at small angles, multipole decomposition, energy weighted sum rule distributions, centroids, widths and strengths for giant magnetic resonances, isoscalar and isovector giant dipole resonances position; deduced nuclear matter compressibility. Comparison with other nuclei.

doi: 10.1016/S0375-9474(01)00593-0
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1106.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1152.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1156.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0817.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1066.


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1113.


1997YO02      Phys.Rev. C55, 950 (1997)

D.H.Youngblood

Monopole Resonance Strengths in 58Ni and 208Pb

NUCLEAR REACTIONS 58Ni, 208Pb(α, α'), E=129 MeV; analyzed σ(θ). 58Ni, 208Pb deduced giant monopole resonance strength related features. Folding model analyses.

doi: 10.1103/PhysRevC.55.950
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0117.


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
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1996UT01      Nucl.Instrum.Methods Phys.Res. A371, 514 (1996)

H.Utsunomiya, Y.-W.Lui, D.H.Youngblood, D.O'Kelly, R.P.Schmitt

Identification of Heavy Ions in Magnetic Spectrograph Measurements using a Plastic Phoswich

NUCLEAR REACTIONS 90Zr(40Ar, X), 208Pb(16O, X), E=30 MeV/nucleon; measured heavy-ion production associated light output spectra, scatter plots. Magnetic spectrograph with plastic phoswich detectors.

doi: 10.1016/0168-9002(95)00828-4
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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
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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
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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
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1994SH08      Nucl.Phys. A569, 303c (1994)

S.Shlomo, D.H.Youngblood

Nuclear Matter Incompressibility Coefficient and Giant Monopole Resonance

NUCLEAR STRUCTURE A=24-232; analyzed isoscalar giant monopole resonance data; deduced nuclear matter compressibility range limits related features.

doi: 10.1016/0375-9474(94)90121-X
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1993SH03      Phys.Rev. C47, 529 (1993)

S.Shlomo, D.H.Youngblood

Nuclear Matter Compressibility from Isoscalar Giant Monopole Resonance

NUCLEAR STRUCTURE A=28-232; analyzed giant monopole resonance data; deduced matter compressibility.

doi: 10.1103/PhysRevC.47.529
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1992YO01      Phys.Rev. C45, 2172 (1992)

D.H.Youngblood, Y.-W.Lui, U.Garg, R.J.Peterson

Giant Quadrupole Resonance in Ni Isotopes

NUCLEAR REACTIONS 58,60,62,64Ni(α, α'), E=130 MeV; measured σ(θ). 58,60,62,64Ni deduced giant quadrupole resonances position, width, EWSR, strength distribution.

doi: 10.1103/PhysRevC.45.2172
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1991YO03      Phys.Rev. C44, 1878 (1991)

D.H.Youngblood, Y.-W.Lui

Monopole Strength in 58Ni

NUCLEAR REACTIONS 58Ni(α, α'), E=129.5 MeV; measured σ(θ). 58Ni deduced E0 centroid, width, EWSR.

doi: 10.1103/PhysRevC.44.1878
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1990GA07      Phys.Rev. C41, 1845 (1990)

U.Garg, K.B.Beard, D.Ye, A.Galonsky, T.Murakami, J.S.Winfield, Y.-W.Lui, D.H.Youngblood

Experimental Test of a Newly Proposed Empirical Relationship between the Centroid and Width of the Giant Quadrupole Resonance and the Neutron Binding Energy of the Nucleus

NUCLEAR REACTIONS 58,64Ni(14N, 14N'), E=700 MeV; measured σ(E(14N)). 58,64Ni deduced GDR parameters.

doi: 10.1103/PhysRevC.41.1845
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1990TO04      Phys.Rev. C41, 1417 (1990)

Y.Toba, Y.-W.Lui, D.H.Youngblood, U.Garg, P.Grabmayr, K.T.Knopfle, H.Riedesel, G.J.Wagner

Charged Particle Decay from Giant Monopole Resonance in 28Si

NUCLEAR REACTIONS 28Si(α, α), (α, 2α), (α, pα), E=129 MeV; measured Eα, Iα, σ(θα1, θα2), σ(θα, θp). 28Si deduced giant monopole resonance decay.

doi: 10.1103/PhysRevC.41.1417
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1987NA01      Phys.Rev. C35, 149 (1987)

M.N.Namboodiri, R.K.Choudhury, L.Adler, J.D.Bronson, D.Fabris, U.Garg, P.L.Gonthier, K.Hagel, D.R.Haenni, Y.W.Lui, Z.Majka, G.Mouchaty, T.Murakami, J.B.Natowitz, G.Nebbia, R.P.Schmitt, S.Simon, J.P.Sullivan, D.H.Youngblood

Linear Momentum and Angular Momentum Transfer in the Reactions of 16O with 154Sm

NUCLEAR REACTIONS 154Sm(16O, X), E=180, 310 MeV; measured (ejectile)γ-, (residue)γ-coin, σ(fragment θ, E), < Eγ > vs fragment for X=6,7Li, 7,9,10Be, 10,11B, 11,12,13,14C, 13,14,15N, 15,16,17O; deduced angular, linear momentum transfer correlation.

doi: 10.1103/PhysRevC.35.149
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1987SH15      Phys.Rev.Lett. 59, 1054 (1987)

S.Shlomo, D.H.Youngblood, T.Udagawa, T.Tamura

Excitation of the Isovector Giant Dipole by α-Particle Scattering

NUCLEAR REACTIONS 116Sn(α, α'), E=129 MeV; analyzed σ(θ). 116Sn deduced isovector giant dipole excitation role.

doi: 10.1103/PhysRevLett.59.1054
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1987SH20      Phys.Rev. C36, 1317 (1987)

S.Shlomo, Y.-W.Lui, D.H.Youngblood, T.Udagawa, T.Tamura

Coulomb and Nuclear Excitation of Giant Dipole Resonances in (α, α') Inelastic Scattering

NUCLEAR REACTIONS, MECPD 90Zr(α, α'), E=96 MeV; 116Sn(α, α'), E=129 MeV; 208Pb(α, α'), E=96, 129, 172, 218 MeV; calculated σ(θ); deduced negligible GDR contributions in monopole resonance excitation.

doi: 10.1103/PhysRevC.36.1317
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1986GR10      Phys.Rev. C34, 322 (1986)

P.Grabmayr, G.J.Wagner, K.T.Knopfle, H.Riedesel, P.Bogucki, J.D.Bronson, Y.W.Lui, U.Garg, D.H.Youngblood

Direct Contributions to the Decay of Isoscalar Giant Resonances in 58Ni

NUCLEAR REACTIONS 58Ni(α, 2α), (α, pα), E=129 MeV; measured σ(θ1, θ2, Eα), αα(θ), αp(θ); deduced reaction mechanism. 58Ni deduced isoscalar giant resonance decay mechanism.

doi: 10.1103/PhysRevC.34.322
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1985LU04      Phys.Rev. C31, 1643 (1985)

Y.-W.Lui, J.D.Bronson, D.H.Youngblood, Y.Toba, U.Garg

Giant Quadrupole and Monopole Resonances in 28Si

NUCLEAR REACTIONS 28Si(α, α'), E=129 MeV; measured σ(Eα, θα), σ(θ). 28Si levels deduced isoscalar, electromagnetic transition rates, EWSR.

doi: 10.1103/PhysRevC.31.1643
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1984GA02      Phys.Rev. C29, 93 (1984)

U.Garg, P.Bogucki, J.D.Bronson, Y.-W.Lui, D.H.Youngblood

Giant Monopole Resonance in Transitional and Deformed Nuclei

NUCLEAR REACTIONS 144,148Sm, 142,146,150Nd(α, α'), E=129 MeV; measured σ(Eα'), σ(θ). 142,146Nd deduced giant resonances, Γ, L. 148Sm deduced giant resonances, L, multipole mixing, Γ. 150Nd deduced giant resonance, monopole splitting, Γ, L.

doi: 10.1103/PhysRevC.29.93
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1984LU06      Phys.Rev. C30, 51 (1984)

Y.-W.Lui, P.Bogucki, J.D.Bronson, D.H.Youngblood, U.Garg

Giant Resonances in 112Sn

NUCLEAR REACTIONS 112Sn(α, α'), E=129.1 MeV; measured σ(θ); deduced nuclear incompressibility parameters. 112Sn deduced isoscalar GQR, giant monopole resonances.

doi: 10.1103/PhysRevC.30.51
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1982GA16      Phys.Rev. C25, 3204 (1982)

U.Garg, P.Bogucki, J.D.Bronson, Y.-W.Lui, C.M.Rozsa, D.H.Youngblood

Comment on the Evidence for a Monopole Resonance at Approximately 20 MeV in 58Ni

NUCLEAR REACTIONS 58Ni(α, α'), E=129 MeV; measured σ(θ), σ(Eα'). 58Ni deduced giant resonances, L, possible monopole. DWBA analysis.

doi: 10.1103/PhysRevC.25.3204
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1981IZ02      Phys.Rev. C24, 2179 (1981)

T.Izumoto, Y.-W.Lui, D.H.Youngblood, T.Udagawa, T.Tamura

Coulomb Excitation of the Giant Dipole Resonance in Light-Ion Inelastic Scattering from 208Pb

NUCLEAR REACTIONS 208Pb(α, α'), E=96, 129, 172, 218 MeV; 208Pb(3He, 3He'), E=108.5, 217 MeV; 208Pb(d, d'), E=86, 108 MeV; 208Pb(p, p'), E=201 MeV; analyzed σ(θ). Coupled-channels analysis, GDR excitation.

doi: 10.1103/PhysRevC.24.2179
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1981LU05      Phys.Rev. C24, 884 (1981)

Y.-W.Lui, J.D.Bronson, C.M.Rozsa, D.H.Youngblood, P.Bogucki, U.Garg

Giant Resonances in 40Ca

NUCLEAR REACTIONS 40Ca(α, α'), E=98.5, 116.8, 129.4 MeV; measured σ(Eα, θ). 40Ca deduced giant resonances, L, EWSR, Γ, J, π. DWBA analysis.

doi: 10.1103/PhysRevC.24.884
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1981YO04      Phys.Rev. C23, 1997 (1981)

D.H.Youngblood, P.Bogucki, J.D.Bronson, U.Garg, Y.-W.Lui, C.M.Rozsa

Systematics of the Giant Monopole Resonance from Inelastic Alpha Scattering

NUCLEAR REACTIONS 12C, 27Al, 40Ca, 48Ti, 58Ni, 64,66Zn, 90Zr, 116,118,120,124Sn, 144,154Sm, 208Pb(α, α'), E=99, 117, 129 MeV; measured σ(θ, Eα); deduced nuclear incompressibility vs mass. 27Al, 40Ca, 48Ti, 58Ni deduced GQR, Γ. 64,66Zn, 90Zr, 116,118,120,124Sn, 144,154Sm, 208Pb deduced GQR, giant monopole resonances, Γ, EWSR.

doi: 10.1103/PhysRevC.23.1997
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1980GA15      Phys.Lett. 93B, 39 (1980)

U.Garg, P.Bogucki, J.D.Bronson, Y.-W.Lui, K.Nagatani, E.Takada, N.Takahashi, T.Tamaya, D.H.Youngblood

Excitation of Giant Resonances in 208Pb Using Inelastic 14N Scattering

NUCLEAR REACTIONS 208Pb(14N, 14N'), E=266 MeV; measured σ(θ, E(14N')). 208Pb deduced GQR, Γ.

doi: 10.1016/0370-2693(80)90090-8
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1980GA21      Phys.Rev.Lett. 45, 1670 (1980)

U.Garg, P.Bogucki, J.D.Bronson, Y.-W.Lui, C.M.Rozsa, D.H.Youngblood

Splitting of the Giant Monopole Resonance with Deformation in Sm Nuclei

NUCLEAR REACTIONS 144,154Sm(α, α'), E=96, 129 MeV; measured σ(θ, Eα). 144,154Sm deduced GQR, giant monopole resonances, Γ, EWSR strengths. 154Sm deduced giant monopole resonance fragmentation. Schematic model.

doi: 10.1103/PhysRevLett.45.1670
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1980LU06      Phys.Lett. 93B, 31 (1980)

Y.-W.Lui, P.Bogucki, J.D.Bronson, U.Garg, C.M.Rozsa, D.H.Youngblood

Observation of the Giant Monopole Resonance in 64,66Zn

NUCLEAR REACTIONS 64,66Zn(α, α), E=129 MeV; measured σ(θ). 64,66Zn, 90Zr, 115In, 116,118,120,124Sn, 144,148Sm, 197Au, 208Pb deduced surface, symmetry term contributions to nuclear compressibility. 64,66Zn deduced T=0 giant monopole resonance, energy-weighted sum rule.

doi: 10.1016/0370-2693(80)90088-X
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1980RO08      Phys.Rev. C21, 1252 (1980)

C.M.Rozsa, D.H.Youngblood, J.D.Bronson, Y.-W.Lui, U.Garg

Isoscalar Breathing Mode State in 90Zr and 116Sn

NUCLEAR REACTIONS 90Zr, 116Sn(α, α'), E=96, 129 MeV; measured σ(θ). 90Zr, 116Sn deduced T=0, giant monopole resonance, GQR, Γ, energy-weighted sum rule, β, nuclear incompressibility. DWBA, liquid drop models.

doi: 10.1103/PhysRevC.21.1252
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1979BR02      Nucl.Phys. A313, 157 (1979)

D.R.Brown, J.M.Moss, C.M.Rozsa, D.H.Youngblood, J.D.Bronson

Proton Pickup by α-Particles to Unbound States

NUCLEAR REACTIONS 40Ca, 90Zr, 208Pb(α, αp), E=96.8 MeV; measured σ(Eα, θα, Ep, θp); deduced σ for proton pickup to unbound states.

doi: 10.1016/0375-9474(79)90573-6
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1978MO10      Phys.Rev. C18, 741 (1978)

J.M.Moss, D.R.Brown, D.H.Youngblood, C.M.Rozsa, J.D.Bronson

Inelastic Alpha Scattering Studies of the Low-Energy Octupole Resonance

NUCLEAR REACTIONS 40Ca, 66Zn, 75As, 89Y, 90Zr, 92,100Mo, Ag, 116,118,124Sn, 142Nd, 144,148,154Sm, 197Au, 208Pb(α, α'), E=96, 115 MeV; measured σ(θ). 40Ca, 66Zn, 75As, 89Y, 90Zr, 92,100Mo, 107Ag, 116,118,124Sn, 142Nd, 144,148,154Sm, 197Au, 208Pb deduced transition strengths, L, β.

doi: 10.1103/PhysRevC.18.741
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1977BI02      Phys.Rev. C15, 2006 (1977)

P.K.Bindal, D.H.Youngblood, R.L.Kozub

Neutron Hole States of 93,95Mo

NUCLEAR REACTIONS 94,96Mo(p, d), (d, t), E ≈ 40 MeV; measured σ(θ). 93,95Mo deduced levels L, S, J, π. Quasiparticle-core coupling model.

doi: 10.1103/PhysRevC.15.2006
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1977YO01      Phys.Rev. C15, 246 (1977)

D.H.Youngblood, A.D.Bacher, D.R.Brown, J.D.Bronson, J.M.Moss, C.M.Rozsa

Particle Decay from the Giant Resonance Region of 40Ca

NUCLEAR REACTIONS 40Ca(α, αp), (α, 2α), E=115 MeV; measured σ(θ), αp(θ) in kinematically complete experiments. 40Ca deduced resonances, branching.

doi: 10.1103/PhysRevC.15.246
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1977YO03      Phys.Rev. C15, 1644 (1977)

D.H.Youngblood, C.M.Rozsa, J.M.Moss, D.R.Brown, J.D.Bronson

Giant Quadrupole Resonance in 24Mg, 27Al, and 28Si

NUCLEAR REACTIONS 24Mg, 27Al, 28Si(α, α'), E=126 MeV; measured σ(θ). 24Mg, 27Al, 28Si deduced giant resonances, L, sum rule fraction.

doi: 10.1103/PhysRevC.15.1644
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1977YO05      Phys.Rev.Lett. 39, 1188 (1977)

D.H.Youngblood, C.M.Rozsa, J.M.Moss, D.R.Brown, J.D.Bronson

Isoscalar Breathing-Mode State in 144Sm and 208Pb

NUCLEAR REACTIONS 144Sm, 208Pb(α, α'), E=96 MeV; measured σ(Eα', θ). 144Sm, 208Pb deduced giant resonances, Γ, L, J, π, β.

doi: 10.1103/PhysRevLett.39.1188
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1976BI07      Phys.Rev. C14, 521 (1976)

P.K.Bindal, D.H.Youngblood, R.L.Kozub

(3He, d) Reaction to Bound and Quasibound Levels in 59Cu

NUCLEAR REACTIONS 58Ni(3He, d), E=35.0, 39.1 MeV; measured σ(Ed, θ). 59Cu deduced levels deduced L, S, J, π, analog states. Particle-core-coupling model.

doi: 10.1103/PhysRevC.14.521
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1976MO21      Phys.Rev.Lett. 37, 816 (1976)

J.M.Moss, D.H.Youngblood, C.M.Rozsa, D.R.Brown, J.D.Bronson

Observation of a Low-Energy Octupole Resonance in Medium-Mass Nuclei

NUCLEAR REACTIONS 90Zr, 118Sn, 142Nd, 144,148,154Sm(α, α'), E ≈ 105 MeV; measured σ(Eα', θ). 90Zr, 118Sn, 142Nd, 144,148,154Sm deduced giant resonance structure, J, π, L.

doi: 10.1103/PhysRevLett.37.816
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1976YO02      Phys.Rev. C13, 994 (1976)

D.H.Youngblood, J.M.Moss, C.M.Rozsa, J.D.Bronson, A.D.Bacher, D.R.Brown

Giant Resonances Observed in the Scattering of 96- and 115-MeV Alpha Particles

NUCLEAR REACTIONS 14N, 16O, 20Ne, 27Al, 28Si, 32S, 36,40Ar, 40Ca, 48Ti, 56Fe, 58,60Ni, 59Co, 66Zn, 90Zr, 94,96,100Mo, 141Pr, 142Nd, 144,148,154Sm, 159Tb, 174Yb, 208Pb(α, α'), E=96, 115 MeV; measured σ(Eα', θ). 32S, 36,40Ar, 40Ca, 48Ti, 56Fe, 58,60Ni, 59Co, 66Zn, 90Zr, 94,96,100Mo, 141Pr, 142Nd, 144,148,154Sm, 159Tb, 174Yb, 208Pb deduced resonances, Γ, β, L. 32S, 36,40Ar, 40Ca, 58Ni, 90Zr, 148Sm, 208Pb deduced B(λ).

doi: 10.1103/PhysRevC.13.994
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1975BI10      Phys.Rev. C12, 390 (1975)

P.K.Bindal, D.H.Youngblood, R.L.Kozub, P.H.Hoffmann-Pinther

98Mo(p, d)97Mo Reaction and Core Coupling in 97Mo and 97Nb

NUCLEAR REACTIONS 98Mo(p, d), E=38.6 MeV; measured σ(Ed, θ). 97Mo deduced levels, L, S, J, π, B(λ). 97Nb; calculated levels. 98Mo; calculated quadrupole moment.

doi: 10.1103/PhysRevC.12.390
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1975BI15      Phys.Rev. C12, 1826 (1975)

P.K.Bindal, D.H.Youngblood, R.L.Kozub, P.H.Hoffmann-Pinther

Neutron Hole States of 99Mo

NUCLEAR REACTIONS 100Mo(p, d), (d, t), E ≈ 40 MeV; measured σ(θ). 99Mo deduced levels, L, J, π, S. DWBA analysis.

doi: 10.1103/PhysRevC.12.1826
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1975KI12      Phys.Rev.Lett. 35, 552 (1975)

T.Kishimoto, J.M.Moss, D.H.Youngblood, J.D.Bronson, C.M.Rozsa, D.R.Brown, A.D.Bacher

Giant Quadrupole Resonance in Deformed Nuclei

NUCLEAR REACTIONS 144,148,154Sm(α, α'), E=115 MeV; measured σ(Eα', θ). 144,148,154Sm GQR deduced Γ.

doi: 10.1103/PhysRevLett.35.552
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1975MO04      Phys.Rev.Lett. 34, 748 (1975)

J.M.Moss, C.M.Rozsa, D.H.Youngblood, J.D.Bronson, A.D.Bacher

Isoscalar Giant Resonance in Light Nuclei (A ≤ 40)

NUCLEAR REACTIONS 40Ca, 36,40Ar, 32S, 28Si, 27Al, 20Ne, 16O(α, α), E=96.6 MeV; measured σ(θ). 32S, 36,40Ar, 40Ca giant resonances deduced level-width, S.

doi: 10.1103/PhysRevLett.34.748
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1974BI03      Phys.Rev. C9, 1618 (1974)

P.K.Bindal, D.H.Youngblood

Core Coupling in 99Nb

NUCLEAR STRUCTURE 99Nb; calculated levels, S.

NUCLEAR REACTIONS 100Mo(d, 3He), E=40.7 MeV; measured σ(E(3He), θ). 99Nb deduced levels, L, S.

doi: 10.1103/PhysRevC.9.1618
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1974BI08      Phys.Rev. C10, 729 (1974)

P.K.Bindal, D.H.Youngblood, R.L.Kozub

Proton Hole States of 95,97,99Nb

NUCLEAR REACTIONS 96,98,100Mo(d, 3He), E=40.7 MeV; measured σ(E(3He), θ). 100Mo(d, 3He), E=40.7 MeV, measured Q. 95,97,99Nb deduced levels, J, π, L, S. 99Nb deduced mass excess.

doi: 10.1103/PhysRevC.10.729
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1974MO22      Phys.Lett. 53B, 51 (1974)

J.M.Moss, C.M.Rozsa, J.D.Bronson, D.H.Youngblood

Systematics of Giant Resonances from Inelastic Alpha-Particle Scattering

NUCLEAR REACTIONS 27Al, 40Ca, 90Zr, Pb, 24Mg(α, α'), E=96, 115 MeV; measured σ(Eα'). 40Ca, 90Zr, 208Pb deduced resonance.

doi: 10.1016/0370-2693(74)90341-4
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1973KO03      Phys.Rev. C7, 404 (1973)

R.L.Kozub, D.H.Youngblood

Structure of 91Mo via the (p, d) and (d, t) Reactions

NUCLEAR REACTIONS 92Mo(p, d), 92Mo(d, t), E=38.6, 40.6 MeV; measured Q, σ(θ). 91Mo deduced levels, J, π, L(n), S.

doi: 10.1103/PhysRevC.7.404
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1973KO04      Phys.Rev. C7, 410 (1973)

R.L.Kozub, D.H.Youngblood

Study of Hole-State Analogs in Mo Isotopes

NUCLEAR REACTIONS 92,94,96Mo(p, d), (d, t), E=38.6, 40.6 MeV; 92,94,96Mo(3He, α), E=35 MeV; 98Mo(p, d), E=38.6 MeV; measured σ(θ). 91,93,95,97Mo deduced IAS, Coulomb energies, S.

doi: 10.1103/PhysRevC.7.410
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1973NA09      Phys.Rev.Lett. 31, 250 (1973)

K.Nagatani, D.H.Youngblood, R.Kenefick, J.Bronson

(10B, 7Li) and (10B, 7Be) Analog Reactions on 12C

NUCLEAR REACTIONS 12C(10B, 7Li), (10B, 7Be), E=100 MeV; measured σ(E(7Li), θ), σ(E(7Be), θ). 15O, 15N deduced levels.

doi: 10.1103/PhysRevLett.31.250
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1972KO02      Phys.Rev. C5, 413 (1972)

R.L.Kozub, D.H.Youngblood

Single-Particle Strengths for Quasibound Levels in 33Cl

NUCLEAR REACTIONS 32S(3He, d), E=29.7, 34.5 MeV; measured σ(Ed, θ). 33Cl deduced levels, L(p), J, π, S.

doi: 10.1103/PhysRevC.5.413
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2197.


1972KO11      Phys.Rev.Lett. 28, 1529 (1972)

R.L.Kozub, D.H.Youngblood

Hole-Strength Variations in Neutron Pickup Reactions to Isobaric-Analog States in Mo Isotopes

NUCLEAR REACTIONS 92,94,96,98Mo(p, d), E=38.6 MeV; 92,94,96Mo(d, t), E=40.6 MeV; measured σ(θ). 91,93,95,97Mo deduced levels, S, isobaric analogs.

doi: 10.1103/PhysRevLett.28.1529
Citations: PlumX Metrics


1972YO01      Nucl.Phys. A183, 197 (1972)

D.H.Youngblood, R.L.Kozub, J.C.Hill

Lifetimes of Levels in 66Zn

NUCLEAR REACTIONS 66Zn(α, α'γ), E=25 MeV; measured DSA, σ(Eα', Eγ). 66Zn levels deduced T1/2.

doi: 10.1016/0375-9474(72)90939-6
Citations: PlumX Metrics


1972YO05      Nucl.Phys. A192, 442 (1972)

D.H.Youngblood, R.L.Kozub

Level Structure of 90Mo via the 92Mo(p, t)90Mo Reaction

NUCLEAR REACTIONS 92Mo(p, t), E=39 MeV; measured σ(Et, θ). 90Mo deduced levels, J, π, L.

doi: 10.1016/0375-9474(72)90272-2
Citations: PlumX Metrics


1971KO16      Phys.Rev. C4, 535 (1971)

R.L.Kozub, D.H.Youngblood

(3He, d) Reaction to Bound and Quasibound Levels in 93Tc

NUCLEAR REACTIONS 92Mo(3He, d), E=35 MeV; measured σ(Ed, θ). 93Tc deduced levels, L(p), J, π, S, isobaric analogs.

doi: 10.1103/PhysRevC.4.535
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2198.


1971TH02      Phys.Rev. C3, 536 (1971)

M.J.Throop, D.H.Youngblood, G.C.Morrison

Lifetime of the 981-keV State in Li8

NUCLEAR REACTIONS 2H(7Li, pγ), E=7.4 MeV; measured Doppler shift attenuation. 8Li level deduced T1/2.

doi: 10.1103/PhysRevC.3.536
Citations: PlumX Metrics


1971YO01      Phys.Rev.Lett. 26, 572 (1971)

D.H.Youngblood, R.L.Kozub

Spectroscopic Factors for Stripping to Unbound Isobaric Analog States

NUCLEAR REACTIONS 92Mo(3He, d), E=35 MeV; measured σ(θ). 93Tc deduced levels, S, isobaric analogs.

doi: 10.1103/PhysRevLett.26.572
Citations: PlumX Metrics


1971YO02      Nucl.Phys. A166, 198 (1971)

D.H.Youngblood, R.L.Kozub, J.C.Hill

Mean Lifetimes of Levels in 92Mo

NUCLEAR REACTIONS 92Mo(α, α'γ), E=25 MeV; measured attenuated-Doppler-shift. 92Mo levels deduced T1/2.

doi: 10.1016/0375-9474(71)90422-2
Citations: PlumX Metrics


1970YO01      Nucl.Phys. A143, 512 (1970)

D.H.Youngblood, R.L.Kozub, J.C.Hiebert, R.A.Kenefick

(α, 3He) and (α, t) Rections on 40Ca

NUCLEAR REACTIONS 40Ca(α, 3He), (α, t), E=40 MeV; measured σ(E(3He), θ), σ(Et, θ). 41Ca, 41Sc deduced levels, L, S.

doi: 10.1016/0375-9474(70)90545-2
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0275.


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