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NSR database version of April 11, 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, 68}Zn and ^{56, 58, 60, 68}Ni

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
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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, 100}Mo and ^{90, 92, 94}Zr

NUCLEAR STRUCTURE ^{92,94,96,98,100}Mo, ^90,92,94Zr; calculated response function S(E), centroid energies E_CEN 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, E_CEN vs m^*/m; compared with data; deduced nuclear matter properties, E_CEN 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, 68}Zn

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, 94}Zr

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, 100}Mo

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
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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
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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, 48}Ti

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
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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
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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
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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
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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
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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
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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
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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
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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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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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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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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, ^{116,118,120,124}Sn, ^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, ^{116,118,120,124}Sn, ^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, ^{116,118,120,124}Sn, ^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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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0587.

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
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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
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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 T_1/2.

doi: 10.1016/0375-9474(72)90939-6
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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
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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
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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 T_1/2.

doi: 10.1103/PhysRevC.3.536
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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
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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 T_1/2.

doi: 10.1016/0375-9474(71)90422-2
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0275.