References quoted in the ENSDF dataset: 208PB 208PB(A,A'),(A,A'G),(A,A'N)
55 references found.
Clicking on a keynumber will list datasets that reference the given article.
Phys.Letters 16, 52 (1965)
G.R.Satchler, H.W.Broek, J.L.Yntema
Coulomb Excitation and the Scattering of 43 MeV Alpha Particles by Pb208
NUCLEAR STRUCTURE 208Pb; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(65)90400-2
Phys.Letters 25B, 459 (1967)
J.Alster
Nuclear Transition Strength Systematics in the Pb Region
NUCLEAR STRUCTURE 206Pb, 204Pb; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(67)90106-2
Nucl.Phys. A146, 597 (1970)
G.Bruge, J.C.Faivre, H.Faraggi, A.Bussiere
44 MeV α-Particle Scattering on Doubly Even Spherical Nuclei Near Closed Shells and Nuclear Structure of Collective States
NUCLEAR REACTIONS 40Ca, 46,48,50Ti, 52Cr, 54,56,58Fe, 58,60,62,64Ni, 64Zn, 112,114,116,118,120,122,124Sn, 208Pb(α, α'), Eα=44 MeV; measured σ(Eα', θ). 40Ca, 46,48,50Ti, 52Cr, 54,56,58Fe, 58,60,62,64Ni, 64Zn, 112,114,116,118,120,122,124Sn, 208Pb deduced levels, deformation lengths, B(E2), B(E3). Enriched targets.
doi: 10.1016/0375-9474(70)90747-5
Nucl.Phys. A232, 22 (1974)
F.E.Cecil, G.T.Garvey, W.J.Braithwaite
Search for Giant Spin-Flip Transitions in 90Zr and 208Pb
NUCLEAR REACTIONS 90Zr, 208Pb(p, p'), (p, p'γ), E=24 MeV; 90Zr, 208Pb(α, α'), E=48 MeV; measured σ(Ep', θ), σ(Eα', θ), pγ-coin. 90Zr deduced levels, J, π, γ-branching ratio. 208Pb deduced levels, π.
doi: 10.1016/0375-9474(74)90643-5
J.Phys.(Paris), Suppl.Lett. 35, L-11 (1974)
G.Gregoire, J.Lega, J.Renuart
Diffusion Inelastique de Particules Alpha de 40 MeV par le Noyau 208Pb Aux Petits Angles
NUCLEAR REACTIONS 208Pb(α, α'), E=40 MeV; measured σ(Eα, θ).
Phys.Rev.Lett. 34, 1296 (1975)
R.Del Vecchio, S.Freedman, G.T.Garvey, M.Oothoudt
Spin and Parity of the 4.841-MeV Level of 208Pb
NUCLEAR REACTIONS 208Pb(α, α'), E=34.6 MeV; measured σ(Eα'), 208Pb level deduced π.
doi: 10.1103/PhysRevLett.34.1296
Phys.Rev. C13, 2089 (1976)
R.M.Del Vecchio, S.J.Freedman, G.T.Garvey, M.A.Oothoudt
Jπ Assignment to the 4.841 MeV Level in 208Pb
NUCLEAR REACTIONS 208Pb(α, α'γ), E=35 MeV; measured α'γ(θ). 208Pb level deduced J, π.
Z.Phys. A279, 55 (1976)
H.J.Gils, H.Rebel, J.Buschmann, H.Klewe-Nebenius, G.P.Nowicki, W.Nowatzke
Nuclear Matter Sizes and Isoscalar Octupole Transition Rates of 204,206,208Pb from 104 MeV α-Particle Scattering
NUCLEAR REACTIONS 204,206,208Pb(α, α), (α, α'), E=104 MeV; measured σ(θ). 204,206,208Pb deduced rms radii, isoscalar octupole transition probabilities. Folding model analysis.
Phys.Rev. C13, 1072 (1976)
L.L.Rutledge, Jr., J.C.Hiebert
Isoscalar Transition Rates via 40Ca, 208Pb(α, α') at 79 MeV
NUCLEAR REACTIONS 40Ca, 208Pb(α, α'), E=79.1 MeV; measured σ(Eα', θ). 208Pb, 40Ca deduced reduced transition rates. DWBA analysis.
Phys.Rev.Lett. 38, 676 (1977)
M.N.Harakeh, K.van der Borg, T.Ishimatsu, H.P.Morsch, A.van der Woude, F.E.Bertrand
Direct Evidence for a New Giant Resonance at 80A-1/3 MeV in the Lead Region
NUCLEAR REACTIONS 206,208Pb, 197Au, 209Bi(α, α'), E=120 MeV; measured σ(θ). 206,208Pb, 197Au, 209Bi deduced giant resonance structure.
doi: 10.1103/PhysRevLett.38.676
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
Nucl.Phys. A297, 317 (1978)
H.P.Morsch, P.Decowski, W.Benenson
Fine Structure in the Giant Resonance Region and the Collective Dipole Spin-Flip Excitation in 208Pb
NUCLEAR REACTIONS 208Pb(p, p'), E=40, 45 MeV; 208Pb(α, α'), E=48 MeV; measured σ(θ). 208Pb deduced strengths for J=1, 2, 3 transitions in the region 6-12 MeV excitation, B(M2).
doi: 10.1016/0375-9474(78)90279-8
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.
Phys.Rev.Lett. 42, 366 (1979)
P.Doll, D.L.Hendrie, J.Mahoney, A.Menchaca-Rocha, D.K.Scott, T.J.M.Symons, K.Van Bibber, Y.P.Viyogi, H.Wieman
Giant-Resonance Studies with High-Energy Heavy Ions
NUCLEAR REACTIONS 12C, 58Ni, 208Pb(16O, 16O'), E=315 MeV; measured σ(θ); deduced evidence for GMR. DWBA analysis.
doi: 10.1103/PhysRevLett.42.366
Phys.Rev.Lett. 43, 1369 (1979)
W.Eyrich, A.Hofmann, U.Scheib, S.Schneider, F.Vogler, H.Rebel
Decay of the Isoscalar Giant Resonances in 208Pb
NUCLEAR REACTIONS 208Pb(α, α'), E=104 MeV; measured α'γ(θ). 208Pb deduced T=0, GQR, fine structure following n decay.
doi: 10.1103/PhysRevLett.43.1369
Nucl.Phys. A327, 373 (1979)
M.N.Harakeh, B.van Heyst, K.van der Borg, A.van der Woude
Isoscalar Excitations in the Lead Region Observed in Inelastic α-Scattering at Eα = 120 MeV
NUCLEAR REACTIONS 197Au, 206Pb, 208Pb, 209Bi(α, α'), E=120 MeV; measured σ(θ). 206Pb, 208Pb, 209Bi deduced resonances, L, β, isoscalar multipole strength. DWBA, collective analysis. Enriched targets.
doi: 10.1016/0375-9474(79)90265-3
Phys.Rev. C20, 1600 (1979)
H.P.Morsch, M.Rogge, P.Turek, C.Sukosd, C.Mayer-Boricke
Evidence for the Giant Monopole Resonance in 208Pb from Strong Energy Dependence in α Scattering
NUCLEAR REACTIONS 208Pb(α, α'), E=100-172 MeV; measured σ(θ, E); deduced E0 strength; calculated σ for L=0, L=2.
Phys.Rev. C22, 1832 (1980)
F.E.Bertrand, G.R.Satchler, D.J.Horen, J.R.Wu, A.D.Bacher, G.T.Emery, W.P.Jones, D.W.Miller, A. van der Woude
Giant Multipole Resonances from Inelastic Scattering of 152-MeV Alpha Particles
NUCLEAR REACTIONS 208Pb, 120Sn, 90Zr, 58Ni, 46Ti(α, α), (α, α'), E=152 MeV; measured σ(Eα, θ). 46Ti, 58Ni, 90Zr, 120Sn, 208Pb deduced GQR, giant monopole resonances, Γ, L, T, β(L), B(λ), EWSR. Folding model analysis.
Phys.Rev. C22, 1420 (1980)
T.Chapuran, R.Vodhanel, M.K.Brussel
Resonant Photon Scattering from 206,207,208Pb and 209Bi
NUCLEAR REACTIONS 206,207,208Pb, 209Bi(γ, γ); E=7.0, 7.6, 8.0, 8.5 MeV bremsstrhalung; measured Eγ, Iγ, self absorption. 206,207,208Pb, 209Bi deduced resonances, J, absolute γ-transition strength, Γγ/Γ. Enriched target, resonance fluorescence technique.
Z.Phys. A298, 79 (1980)
C.Djalali, N.Marty, M.Morlet, A.Willis, V.Comparat, R.Frascaria
Excitation of the Giant Monopole Resonance and Coulomb Excitation of the Giant Dipole Resonance in Hadron Inelastic Scattering from 208Pb
NUCLEAR REACTIONS 208Pb(α, α'), E=218 MeV; 208Pb(d, d'), E=108 MeV; 208Pb(p, p'), E=201 MeV; measured σ(Eα), σ(Ed), σ(Ep). 208Pb deduced giant monopole resonance, Coulomb effects on GDR excitation. DWBA analysis.
Nucl.Phys. A342, 165 (1980)
J.S.Lilley, M.A.Franey, D.H.Feng
Alpha Inelastic Scattering by 208Pb Near the Coulomb Barrier
NUCLEAR REACTIONS 208Pb(α, α), (α, α'), E=23.5 MeV; measured σ(θ); deduced nuclear matter surface distribution, transition density, potential parameters. 208Pb level deduced B(E3), β. Deformed potential model, folding model.
doi: 10.1016/0375-9474(80)90512-6
Phys.Rev.Lett. 45, 337 (1980)
H.P.Morsch, M.Rogge, P.Turek, C.Mayer-Boricke
New Giant Resonances in 172-MeV α Scattering from 208Pb
NUCLEAR REACTIONS 208Pb(α, α'), E=172 MeV; measured σ(θ, Eα). 208Pb deduced T=0, giant octupole, dipole resonances, Γ, energy-weighted sum rule strength.
doi: 10.1103/PhysRevLett.45.337
Phys.Rev. C22, 489 (1980)
H.P.Morsch, C.Sukosd, M.Rogge, P.Turek, H.Machner, C.Mayer-Boricke
Giant Monopole and Quadrupole Resonances and Other Multipole Excitations in 208Pb Studied in 43 MeV/Nucleon α-Particle and Deuteron Scattering
NUCLEAR REACTIONS 208Pb(α, α'), E=172 MeV; 208Pb(d, d'), E=86 MeV; measured σ(θ). 208Pb levels deduced transition radii, B(λ), βL, giant resonance character, EWSR.
Nucl.Phys. A369, 25 (1981)
A.M.Baxter, S.Hinds, R.H.Spear, T.H.Zabel, R.Smith
Octupole Vibrations in the Even Mercury and Lead Isotopes
NUCLEAR REACTIONS 198,200,202,204Hg, 204,206,208Pb(α, α'), E=24, 27 MeV; measured σ(Eα'). 198,200,202,204Hg, 204,206,208Pb deduced levels. 204Hg, 204,206,208Pb(α, α'), E=27 MeV; measured σ(Eα, θ). 204Hg, 204,206,208Pb levels deduced J, π, L, β2, β3. Enriched targets.
doi: 10.1016/0375-9474(81)90004-X
Phys.Lett. 101B, 147 (1981)
P.Decowski, H.P.Morsch, W.Benenson
Low-Lying Isoscalar Dipole Excitations in 208Pb
NUCLEAR REACTIONS 208Pb(α, α'), E=48 MeV; measured σ(Eα, θ). 208Pb deduced T=0, dipole states, Γ, EWSR. Microscopic DWBA analysis, nuclear diffuseness dipole oscillation.
doi: 10.1016/0370-2693(81)90661-4
Phys.Rev.Lett. 47, 1702 (1981)
H.Steuer, W.Eyrich, A.Hofmann, H.Ortner, U.Scheib, R.Stamminger, D.Steuer, H.Rebel
Neutron Decay of the Giant Quadrupole Resonance Region in 208Pb
NUCLEAR REACTIONS 208Pb(α, α'n), E=104 MeV; measured nα-coin, Eα, En. 208Pb deduced GQR branching ratio. 207Pb levels deduced populating γ-multipolarity.
doi: 10.1103/PhysRevLett.47.1702
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.
Phys.Lett. 119B, 311 (1982)
H.P.Morsch, M.Rogge, P.Turek, P.Decowski, L.Zemlo, C.Mayer-Boricke, S.A.Martin, G.P.A.Berg, I.Katayama, J.Meissburger, J.G.M.Romer, J.Reich, P.Wucherer, W.Brautigam
The Giant Octupole Resonance in Deformed Nuclei
NUCLEAR REACTIONS 120Sn, 140Ce, 159Tb, 169Tm, 175Lu, 181Ta, Pt, 208Pb, 232Th, 238U(α, α'), E=172 MeV; measured σ(Eα') vs θ; deduced giant octupole excitation mass dependence. 120Sn, 140Ce, 159Tb, 169Tm, 175Lu, 181Ta, Pt, 208Pb, 232Th, 238U deduced giant octupole parameters, EWSR. DWBA analysis.
doi: 10.1016/0370-2693(82)90677-3
Nucl.Phys. A381, 277 (1982)
T.Yamagata, S.Kishimoto, K.Yuasa, B.Saeki, K.Iwamoto, M.Tanaka, T.Fukuda, I.Miura, M.Inoue, H.Ogata
Excitation of Giant Monopole Resonances in 144Sm and 208Pb by (α, α') Reactions at Eα = 84-119 MeV
NUCLEAR REACTIONS 144Sm(α, α'), E=83.8, 99.1, 108.6 MeV; 208Pb(α, α'), E=83.8, 89, 118.7 MeV; measured σ(θ, E). 144Sm, 208Pb deduced giant monopole, quadrupole resonances, Γ, deformation parameters β(L). Dipole plus triplet quadrupole magnetic detection system, enriched target. DWBA analysis.
doi: 10.1016/0375-9474(82)90144-0
J.Phys.(London) G9, 177 (1983)
V.Corcalciuc, H.Rebel, R.Pesl, H.J.Gils
Isoscalar Octupole Transition Rates in 50Ti, 52Cr and 208Pb from Model-Independent Analyses of 104 MeV α-Particle Scattering
NUCLEAR REACTIONS 50Ti, 52Cr, 208Pb(α, α), (α, α'), E=104 MeV; analyzed σ(θ). 50Ti, 52Cr, 208Pb deduced volume integrals, rms, transition radii, T=0 octupole transition strength. Model independent analysis.
doi: 10.1088/0305-4616/9/2/010
Phys.Rev. C28, 1947 (1983)
H.P.Morsch, P.Decowski, M.Rogge, P.Turek, L.Zemlo, S.A.Martin, G.P.A.Berg, W.Hurlimann, J.Meissburger, J.G.M.Romer
Isoscalar Giant Resonances on 208Pb - in Particular 2(h-bar x omega) L = 0, 2, 4, and 6 Excitations - Studied in Small Angle α Scattering
NUCLEAR REACTIONS 208Pb(α, α'), E=172 MeV; measured σ(θ). 208Pb deduced giant resonances, T, Γ, L, EWSR, multipolarity.
Nucl.Phys. A430, 349 (1984)
B.Bonin, N.Alamanos, B.Berthier, G.Bruge, H.Faraggi, D.Legrand, J.C.Lugol, W.Mittig, L.Papineau, A.I.Yavin, D.K.Scott, M.Levine, J.Arvieux, L.Farvacque, M.Buenerd
Response Functions of 58Ni, 116Sn and 208Pb to the Excitation of Intermediate-Energy α-Particles
NUCLEAR REACTIONS 208Pb, 116Sn, 58Ni(α, α'), E=340, 480 MeV; measured σ(θ). 208Pb, 116Sn, 58Ni deduced giant resonance excitation strength, collective states. Macroscopic DWBA, multipole analyses.
doi: 10.1016/0375-9474(84)90044-7
Phys.Rev. C29, 418 (1984)
W.Eyrich, K.Fuchs, A.Hofmann, U.Scheib, H.Steuer, H.Rebel
Direct Decay Component of the Giant-Monopole-Resonance Region in 208Pb
NUCLEAR REACTIONS 208Pb(α, α'n), E=104 MeV; measured σ(Eα'), σ(θα, θn); deduced preequilibrium neutron decay. 208Pb deduced giant monopole resonance decay characteristics.
Phys.Rev. C31, 1715 (1985)
H.P.Morsch, D.Cha, J.Wambach
Analysis of Giant Resonances in Proton, 3He, and α Scattering and the Spin-Flip Strength in 208Pb
NUCLEAR STRUCTURE 208Pb, 208Bi; calculated isovector spin-flip response. Microscopic particle-hole model, nuclear matter response.
NUCLEAR REACTIONS 208Pb(α, α'), E=172 MeV; 208Pb(3He, 3He'), E=140 MeV; 208Pb(p, p'), E=200 MeV; analyzed σ(θ). 208Pb deduced isoscalar, isovector spin-flip giant resonance excitations. DWBA, double folding form factors.
Phys.Rev. C33, 2054 (1986)
G.S.Adams, T.A.Carey, J.B.McClelland, J.M.Moss, S.J.Seestrom-Morris, D.Cook
Inelastic Proton Excitation of High-Lying Giant Resonances
NUCLEAR REACTIONS 208Pb, 144Sm, 116Sn(p, p'), E=800 MeV; measured σ(Ep'), σ(θ). 208Pb, 144Sm, 116Sn deduced giant resonances, parameters, J, π, EWSR. DWBA analysis.
Nucl.Phys. A466, 29 (1987)
S.Brandenburg, W.T.A.Borghols, A.G.Drentje, L.P.Ekstrom, M.N.Harakeh, A.Van Der Woude, A.Hakansson, L.Nilsson, N.Olsson, M.Pignanelli, R.De Leo
Decay of the Isoscalar Giant Monopole Resonance in 208Pb
NUCLEAR REACTIONS 208Pb(α, α'n)E=120 MeV; measured σ(θ). 208Pb deduced giant monopole resonance, neutron decay characteristics. Statistical model calculations.
doi: 10.1016/0375-9474(87)90344-7
Nucl.Phys. A482, 453c (1988)
A.van der Woude
Neutron Decay of the Isoscalar Giant Monopole Resonance in 124Sn and 208Pb
NUCLEAR REACTIONS 208Pb(α, α'), E=120 MeV; 124Sn, 208Pb(α, nα), E=120 MeV; analyzed data. 208Pb, 124Sn deduced giant resonance decay features.
doi: 10.1016/0375-9474(88)90603-3
Phys.Rev.Lett. 62, 16 (1989)
T.D.Poelhekken, S.K.B.Hesmondhalgh, H.J.Hofmann, H.W.Wilschut, A.van der Woude, M.N.Harakeh
Excitation of the Isovector Giant Dipole Resonance by Inelastic α Scattering: An Experimental Approach
NUCLEAR REACTIONS 208Pb(α, α'γ), E=120 MeV; measured Eγ, Iγ. 208Pb(α, α'), E=120 MeV; calculated σ(θ). 208Pb deduced GDR decay branching ratio.
doi: 10.1103/PhysRevLett.62.16
Phys.Rev. C45, 993 (1992)
Y.Fujita, T.Shimoda, H.Miyatake, N.Takahashi, M.Fujiwara, S.Morinobu, T.Yamagata, J.Takamatsu, A.Terakawa, H.Folger
Observation of the Low-Energy Octupole Resonance in 208Pb by Inelastic α Scattering
NUCLEAR REACTIONS 208Pb(α, α'), E=70 MeV; measured σ(θ). 208Pb levels deduced L-assignment, EWSR fractions, isoscalar nature of low energy octupole resonance. Enriched target, DWBA analysis, comparison with (p, p') data.
Phys.Lett. 278B, 423 (1992)
T.D.Poelhekken, S.K.B.Hesmondhalgh, H.J.Hofmann, A.van der Woude, M.N.Harakeh
Low-Energy Isoscalar Dipole Strength in 40Ca, 58Ni, 90Zr and 208Pb
NUCLEAR REACTIONS 208Pb, 90Zr, 58Ni, 40Ca(α, α'γ), E=120 MeV; measured σ(θα, θγ). 40Ca, 58Ni, 90Zr, 208Pb deduced isoscalar dipole strength, EWSR.
doi: 10.1016/0370-2693(92)90579-S
Thesis, Eberhard Karls Univ. Tubingen (1995)
U.K.H.Atzrott
Untersuchungen zur Systematik von α-Kernpotentialen bei mittelschweren und schweren Kernen
Nucl.Phys. A599, 277c (1996)
B.F.Davis, H.Akimune, A.Bacher, G.P.A.Berg, C.C.Foster, M.Fujiwara, U.Garg, M.N.Harakeh, J.Janecke, J.Lisantti, K.Pham, W.Reviol, D.Roberts, E.J.Stephenson, Y.Wang
The ' Other ' Giant Dipole Resonance: Evidence for the isoscalar giant dipole resonance in 208Pb from inelastic α scattering at 0°
NUCLEAR REACTIONS 208Pb(α, α'), E=200 MeV; measured 0° spectra. 208Pb deduced evidence for isoscalar GDR.
doi: 10.1016/0375-9474(96)00070-X
Phys.Rev.Lett. 79, 609 (1997)
B.F.Davis, U.Garg, W.Reviol, M.N.Harakeh, A.Bacher, G.P.A.Berg, C.C.Foster, E.J.Stephenson, Y.Wang, J.Janecke, K.Pham, D.Roberts, H.Akimune, M.Fujiwara, J.Lisantti
Evidence for the Isoscalar Giant Dipole Resonance in 208Pb using Inelastic α Scattering at and Near 0°
NUCLEAR REACTIONS 208Pb(α, α'), E=200 MeV; measured σ(θ), α spectra. 208Pb deduced isoscalar GDR.
doi: 10.1103/PhysRevLett.79.609
Thesis, Ludwig-Maximilians Unversitat Munchen (1997)
B.D.Valnion
Leichtionen-induzierte Anregungen in 178Hf und 208Pb
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
Phys.Rev. C63, 024318 (2001)
B.D.Valnion, V.Yu.Ponomarev, Y.Eisermann, A.Gollwitzer, R.Hertenberger, A.Metz, P.Schiemenz, G.Graw
Excitation of 208Pb in Light Ion Induced Reactions and the Two Octupole Phonon Multiplet
NUCLEAR REACTIONS 208Pb(p, p'), (d, d'), E=22 MeV; 208Pb(α, α'), E=40 MeV; measured Ep, Eα, deuteron spectra, σ(θ). 208Pb(polarized d, p), E not given; measured proton spectra, Ay(θ). 208Pb deduced levels, J, π, spectroscopic factors, two-octupole-phonon multiplet states. Comparison with quasiparticle phonon model results.
doi: 10.1103/PhysRevC.63.024318
Phys.Lett. B 576, 253 (2003)
M.Hunyadi, A.M.van den Berg, N.Blasi, C.Baumer, M.Csatlos, L.Csige, B.Davids, U.Garg, J.Gulyas, M.N.Harakeh, M.A.de Huu, B.C.Junk, A.Krasznahorkay, S.Rakers, D.Sohler, H.J.Wortche
Direct proton decay of the isoscalar giant dipole resonance
NUCLEAR REACTIONS 208Pb(α, α'p), E=200 MeV; measured Eα, Ep, pα-coin, σ(E, θ). 208Pb deduced isoscalar GDR energy, width, direct proton decay features.
doi: 10.1016/j.physletb.2003.10.016
Phys.Lett. B 557, 12 (2003)
M.Uchida, H.Sakaguchi, M.Itoh, M.Yosoi, T.Kawabata, H.Y.Yasuda, T.Murakami, T.Ishikawa, T.Taki, N.Tsukahara, S.Terashima, U.Garg, M.Hedden, B.Kharraja, M.Koss, B.K.Nayak, S.Zhu, M.Fujiwara, H.Fujimura, K.Hara, E.Obayashi, H.P.Yoshida, H.Akimune, M.N.Harakeh, M.Volkerts
Isoscalar giant dipole resonance in 208Pb via inelastic α scattering at 400 MeV and nuclear incompressibility
NUCLEAR REACTIONS 208Pb(α, α'), E=400 MeV; measured Eα, σ(E, θ). 208Pb deduced isoscalar GDR strength distribution. Multipole-decomposition analysis.
doi: 10.1016/S0370-2693(03)00137-0
Nucl.Phys. A731, 3 (2004)
U.Garg
The Isoscalar Giant Dipole Resonance: A Status Report
doi: 10.1016/j.nuclphysa.2003.11.013
Nucl.Phys. A731, 49 (2004)
M.Hunyadi, C.Baumer, A.M.van den Berg, N.Blasi, M.Csatlos, L.Csige, B.Davids, U.Garg, J.Gulyas, M.N.Harakeh, M.de Huu, B.C.Junk, A.Krasznahorkay, S.Rakers, D.Sohler, H.J.Wortche
Particle decay of the isoscalar giant dipole resonance in 208Pb
NUCLEAR REACTIONS 208Pb(α, α'n), (α, α'p), E=200 MeV; measured En, Ep, Eα, nα-, pα-coin, σ(E, θ). 208Pb deduced branching ratios for direct-proton and direct-neutron decay of isoscalar GDR.
doi: 10.1016/j.nuclphysa.2003.11.018
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
Phys.Rev. C 69, 051301 (2004)
M.Uchida, H.Sakaguchi, M.Itoh, M.Yosoi, T.Kawabata, Y.Yasuda, H.Takeda, T.Murakami, S.Terashima, S.Kishi, U.Garg, P.Boutachkov, M.Hedden, B.Kharraja, M.Koss, B.K.Nayak, S.Zhu, M.Fujiwara, H.Fujimura, H.P.Yoshida, K.Hara, H.Akimune, M.N.Harakeh
Systematics of the bimodal isoscalar giant dipole resonance
NUCLEAR REACTIONS 90Zr, 116Sn, 144Sm, 208Pb(α, α'), E=386 MeV; measured Eα, σ(E, θ). 90Zr, 116Sn, 144Sm, 208Pb deduced isoscalar GDR strength distributions, bimodal structures.
doi: 10.1103/PhysRevC.69.051301
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
Acta Phys.Pol. B36, 1115 (2005)
M.Hunyadi, A.M.van den Berg, M.Csatlos, L.Csige, B.Davids, U.Garg, J.Gulyas, M.N.Harakeh, M.A.de Huu, A.Krasznahorkay, D.Sohler, H.J.Wortche
Overtones of isoscalar giant resonances studied in direct particle decay measurements
NUCLEAR REACTIONS 90Zr, 116Sn, 208Pb(α, α'n), E=200 MeV; 208Pb(α, α'p), E=200 MeV; measured Eα, σ(θ), pα-, nα-coin. 90Zr, 116Sn, 208Pb deduced isoscalar GDR parameters, particle decay features.
Phys.Rev. C 75, 014606 (2007)
M.Hunyadi, A.M.van den Berg, B.Davids, M.N.Harakeh, M.A.de Huu, H.J.Wortche, M.Csatlos, J.Gulyas, A.Krasznahorkay, D.Sohler, U.Garg, M.Fujiwara, N.Blasi
Evidence for direct neutron decay of the isoscalar giant dipole resonances in 90Zr, 116Sn, and 208Pb
NUCLEAR REACTIONS 90Zr, 116Sn, 208Pb(α, α'), (α, nα), E=200 MeV; measured Eγ, Eα, En, σ(E, θ). 90Zr, 116Sn, 208Pb deduced isoscalar GDR neutron decay features.
doi: 10.1103/PhysRevC.75.014606