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NSR database version of May 30, 2024.

Search: Author = H.V.Geramb

Found 33 matches.

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1983PA08      Nucl.Phys. A403, 134 (1983)

G.Palla, H.V.Geramb, C.Pegel

Elastic and Inelastic Scattering of 25.6 MeV Protons from Even Samarium Isotopes

NUCLEAR REACTIONS 144,148,150,152,154Sm(p, p), (p, p'), E=25.6 MeV; measured σ(θ); deduced optical model potentials, deformation paramters. Enriched targets. Coupled-channels analysis, phenomenological, microscopic optical model potential comparison.

doi: 10.1016/0375-9474(83)90193-8
Citations: PlumX Metrics


1979DE07      Phys.Rev. C19, 646 (1979)

R.De Leo, G.D'Erasmo, A.Pantaleo, G.Pasquariello, G.Viesti, M.Pignanelli, H.V.Geramb

14-40 MeV Proton Scattering from Low-Lying States of 28Si

NUCLEAR REACTIONS 28Si(p, p'γ), E=14-40 MeV; measured σ(Ep, θp', θγ=90°). 28Si levels deduced β(L), E1, E2, E3 giant resonance strength, optical-model parameters. Natural targets.

doi: 10.1103/PhysRevC.19.646
Citations: PlumX Metrics


1979DE11      Can.J.Phys. 57, 540 (1979)

R.de Swiniarski, Dinh-Lien Pham, G.Bagieu, H.V.Geramb

Elastic and Inelastic Scattering of 40 MeV Polarized Protons from 90Zr and 92Zr

NUCLEAR REACTIONS 90,92Zr(polarized p, p), (polarized p, p'), E=40 MeV; measured σ(θ), A(θ). Microscopic, macroscopic, DWBA analysis, coupled-channels calculations with vibrational model.


1979DE20      Phys.Rev. C20, 13 (1979)

R.De Leo, G.D'Erasmo, E.M.Fiore, A.Pantaleo, M.Pignanelli, H.V.Geramb

Two-Step Effects in 15-35 MeV Proton Scattering from 24Mg Low-Lying States

NUCLEAR REACTIONS 24Mg(p, p'), E=15-35 MeV; measured σ(θ); deduced optical model parameters. 24Mg levels deduced deformation parameters, reaction mechanism. Enriched target. Optical model, coupled-channels, compound nuclear model analysis.

doi: 10.1103/PhysRevC.20.13
Citations: PlumX Metrics


1979GA13      Nucl.Phys. A327, 349 (1979)

Y.R.Gaillard, P.Martin, G.Perrin, P.Desaintignon, M.Buenerd, J.M.Loiseaux, J.L.Escudie, A.Tarrats, H.V.Geramb

Excitation Function of Giant Resonances as Doorway States in the 12C(P, P)12C Reaction between 19 and 23 MeV

NUCLEAR REACTIONS 12C(p, p), E=19.15-23.34 MeV; measured σ(E, θ)A(E, θ). 13N deduced giant resonance strength distribution. Optical model, coupled channel, anti-symmetrized distorted-wave approximation.

doi: 10.1016/0375-9474(79)90264-1
Citations: PlumX Metrics


1978BR30      Phys.Lett. 79B, 177 (1978)

F.A.Brieva, H.V.Geramb, J.R.Rook

A Realistic Complex Interaction for Elastic and Inelastic Nucleon Scattering

NUCLEAR REACTIONS 27Al(p, n), E=40 MeV; calculated σ(θ) for 27Si ground state; 40Ca(p, p'), E=30, 35.8, 40 MeV; calculated σ(θ) for 3.74-MeV (3-) state in 40Ca. Complex nuclear t-matrix interaction.

doi: 10.1016/0370-2693(78)90216-2
Citations: PlumX Metrics


1978BU27      Nuovo Cim. 48A, 100 (1978)

A.Budzanowski, K.Grotowski, S.Micek, Z.Rogalska, A.Strzalkowski, E.Witkos, T.Delbar, G.Gregoire, J.Lega, G.Paic, P.Wastyn, H.V.Geramb

Giant-Resonance Effects in the 12C(α, p)15N (3/2-, 6.328 MeV) Transition

NUCLEAR REACTIONS 12C(α, p), E=24-33 MeV; measured σ(Ep, θp). 14N level deduced GQR effects, reaction mechanism.

doi: 10.1007/BF02786590
Citations: PlumX Metrics


1978HE03      Z.Phys. A284, 413 (1978)

E.F.Hefter, H.V.Geramb, F.Osterfeld, T.Udagawa

Two-Step Processes in Inelastic Proton Scattering

NUCLEAR REACTIONS 16O, 40Ca(p, p'), 16O(p, d), E=25-46 MeV; calculated σ(θ). Reaction mechanism study.

doi: 10.1007/BF01422110
Citations: PlumX Metrics


1977PE09      Phys.Lett. 68B, 55 (1977)

G.Perrin, D.Lebrun, J.Chauvin, P.Martin, P.De Saintignon, D.Eppel, H.V.Geramb, H.L.Yadav, V.A.Madsen

The Octupole Giant Resonance Strength in 16O

NUCLEAR REACTIONS 16O(polarized p, p'), E=42.5, 44.0, 49.3 MeV; measured σ(Ep', θ), A(θ). 16O deduced octupole strength.

doi: 10.1016/0370-2693(77)90033-8
Citations: PlumX Metrics


1976AM02      Lett.Nuovo Cim. 16, 165 (1976)

K.Amos, H.V.Geramb

Strength Estimate of Inelastic Hadron Scattering to Giant Resonances in 16O

NUCLEAR STRUCTURE 16O; calculated isoscalar resonance characteristics.

doi: 10.1007/BF02746958
Citations: PlumX Metrics


1976DA17      Z.Phys. A278, 281 (1976)

P.David, J.Debrus, H.Essen, F.Lubke, H.Mommsen, R.Schoenmackers, W.Soyez, H.V.v.Geramb, E.F.Hefter

Elastic and Inelastic 4He-Scattering on 208Pb, 232Th and 234,236,238U

NUCLEAR REACTIONS 208Pb, 232Th, 234,236,238U(α, α), (α, α'), measured E=50 MeV; measured σ(θ). 232Th, 234,236,238U deduced β.

doi: 10.1007/BF01409180
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6114.


1976LE16      Nucl.Phys. A265, 291 (1976)

D.Lebrun, G.Perrin, P.Martin, P.de Saintignon, J.Arvieux, M.Buenerd, H.V.Geramb, K.A.Amos

Evidence of an Isoscalar E3 Giant Resonance in 16O

NUCLEAR REACTIONS 16O(polarized p, p'), E=31.7, 33.8, 35.8, 36.8, 39.9 MeV; measured σ(Ep', θ), A(θ). 16O deduced isoscalar resonance, E3 strengths. Distorted wave analyses include giant resonance effects.

doi: 10.1016/0375-9474(76)90355-9
Citations: PlumX Metrics


1976YA08      Phys.Rev. C14, 1369 (1976)

H.L.Yadav, H.V.Geramb

Microscopic Study of Doorway States in the Giant Resonance Region of 16O

NUCLEAR REACTIONS 16O(p, p'), E=24-40 MeV; calculated σ. Microscopic study, RPA wave functions.

doi: 10.1103/PhysRevC.14.1369
Citations: PlumX Metrics


1975GE05      Nucl.Phys. A246, 173 (1975)

H.V.Geramb, P.E.Hodgson

Microscopic Analyses of Proton Inelastic Scattering by 16O and 40Ca Using a Complex t-Matrix

NUCLEAR REACTIONS 16O, 40Ca(p, p'), E=25-61 MeV; calculated σ(Ep', θ).

doi: 10.1016/0375-9474(75)90570-9
Citations: PlumX Metrics


1975GE15      Phys.Rev. C12, 1697 (1975)

H.V.Geramb, K.Amos, R.Sprickmann, K.T.Knopfle, M.Rogge, D.Ingham, C.Mayer-Boricke

Investigation of Giant Resonances as Doorway States in Inelastic Nucleon Scattering from 12C

NUCLEAR REACTIONS 12C(p, p'), E=22.5-45 MeV; measured σ(E, Ep', θ). 12C deduced giant dipole, quadrupole strength distribution. DWBA analysis, resonance effects included.

doi: 10.1103/PhysRevC.12.1697
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0740.


1975GE17      Lett.Nuovo Cim. 14, 526 (1975)

H.V.Geramb, K.Amos

Indication of E4 Giant-Resonance Strength

NUCLEAR REACTIONS 89Y(p, p'), E=155 MeV; analyzed data, calculated σ(θ); deduced angular momentum transfer.


1975GE18      Z.Phys. A275, 373 (1975)

H.V.Geramb, T.Terasawa, K.Amos

An Estimate of Giant Resonance Effects in (α, p) Transitions

NUCLEAR REACTIONS 16O(α, p), E=20 MeV; calculated contributions to 19F 110-keV state due to virtual formation of GQR as doorway state in semi-direct process.


1975NE08      Aust.J.Phys. 28, 659 (1975)

P.Nesci, R.Smith, K.Amos, H.V.Geramb

Shell Structure of the Even Tellurium Isotopes and Inelastic Proton Scattering

NUCLEAR REACTIONS 122,126,128,130Te(p, p'), E=51.9 MeV; calculated σ(θ). Shell structure of Te isotopes.

doi: 10.1071/PH750659
Citations: PlumX Metrics


1975SP07      Z.Phys. A274, 339 (1975)

R.Sprickmann, K.T.Knopfle, D.Ingham, M.Rogge, C.Mayer-Boricke, H.V.Geramb

Optical Model Analysis of Proton-Carbon Elastic Scattering in the Range 20 to 50 MeV

NUCLEAR REACTIONS 12C(p, p), E=20-50 MeV; analyzed σ(E, θ).

doi: 10.1007/BF01434044
Citations: PlumX Metrics


1974AM04      Z.Phys. 270, 149 (1974)

K.A.Amos, H.V.Geramb

Giant Multipole Resonance Effects in 27Al(p, n)27Si

NUCLEAR REACTIONS 27Al(p, n), E=10-40 MeV; calculated σ(E, En, θ). 28Si giant resonances deduced coupling constants.

doi: 10.1007/BF01677446
Citations: PlumX Metrics


1974AM05      Phys.Lett. 52B, 138 (1974)

K.A.Amos, H.V.Geramb, R.Sprickmann, J.Arvieux, M.Buenerd, G.Perrin

Resonance Effects in the 12C(p, p')12C*, 1+ Transition

NUCLEAR REACTIONS 12C(polarized p, p'), E=22.3, 26.7, 30.5 MeV; measured σ(E, Ep', θ), A(E, θ). 12C deduced resonance coupling strengths.

doi: 10.1016/0370-2693(74)90071-9
Citations: PlumX Metrics


1974GE04      Z.Phys. 267, 367 (1974)

H.V.Geramb, K.Amos

Inelastic Proton Scattering to the Lowest 1+ State in 58Ni

NUCLEAR REACTIONS 58Ni(p, p'); measured nothing, calculated σ.


1974GE15      Nuovo Cim. 23A, 447 (1974)

H.V.Geramb, G.L.Strobel, R.Sprickmann

Giant-Dipole-Resonance Effects in the 90Zr(p, p') 0+1 to 0+2 Transition

NUCLEAR REACTIONS 90Zr(p, p'), E=12.7, 18.8, 40 MeV; calculated σ(E, Ep', θ).


1974ME29      Nucl.Phys. A232, 472 (1974)

G.Mertens, M.Thumm, H.V.Geramb

Spin-Flip Probability in the Inelastic Scattering of 16.9 MeV Neutrons From 12C

NUCLEAR REACTIONS 12C(n, n'γ), E=16.9 MeV; measured n'γ(θ); deduced neutron spin-flip probabilities. Polyvinyltoluene target. MADWBA analysis with resonance terms.

doi: 10.1016/0375-9474(74)90633-2
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset20710.


1973GE01      Nucl.Phys. A199, 545 (1973)

H.V.Geramb, R.Sprickmann, G.L.Strobel

Excitation of Giant Multipole Resonances L = 1-4 in the 16O(p, p') Spin-Flip Transition

NUCLEAR REACTIONS 16O(p, p'), E=23-46 MeV; analyzed σ(E;θ) 17F deduced resonances, level-width.

doi: 10.1016/0375-9474(73)90597-6
Citations: PlumX Metrics


1973GE07      Z.Phys. 261, 177 (1973)

H.V.Geramb, D.Eppel

Excitation of Giant Multipole Resonances L = 1, 2 and 3 in the 16O(p, 2p) Reaction

NUCLEAR REACTIONS 16O(p, 2p), E=45 MeV; measured nothing, calculated giant multipole resonances, σ(θ).


1973ST16      Nucl.Phys. A210, 67 (1973)

G.L.Strobel, H.V.Geramb

The Continuous 3He Spectrum from Deuterons Incident on 12C

NUCLEAR REACTIONS 12C(d, 3He), E=52 MeV; calculated σ(E(3He)).

doi: 10.1016/0375-9474(73)90504-6
Citations: PlumX Metrics


1972GE01      Nucl.Phys. A183, 582 (1972)

H.V.Geramb

Features of Core Polarization Knock-Out Exchange Contributions to Inelastic Nucleon Scattering

NUCLEAR REACTIONS 89Y(p, p'), E=24 MeV; calculated core polarization σ(θ). Collective virtual core excitation model.

doi: 10.1016/0375-9474(72)90356-9
Citations: PlumX Metrics


1972GE07      Phys.Lett. 39B, 611 (1972)

H.V.Geramb, G.L.Strobel

Two Step Process in the 16O(p, 2p)15N Reaction

NUCLEAR REACTIONS 16O(p, 2p), E=45 MeV; calculated σ(Ep, θ(p)). 2-step mechanism, core polarization term.

doi: 10.1016/0370-2693(72)90010-X
Citations: PlumX Metrics


1972GE16      Lett.Nuovo Cim. 5, 333 (1972)

H.V.Geramb, G.L.Strobel, R.Sprickmann

Evidence for Core Polarization Exchange Contribution in Inelastic Scattering


1971GE03      Nucl.Phys. A163, 337 (1971)

H.V.Geramb, K.A.Amos

Antisymmetrized Distorted Wave Theory of Inelastic Nucleon Scattering

NUCLEAR REACTIONS 89Y(p, p'), E=18.8, 24.5, 61.2 MeV; measured nothing; analyzed σ(θ). Antisymmetrized DW theory.

doi: 10.1016/0375-9474(71)90495-7
Citations: PlumX Metrics


1971GE12      Phys.Lett. 37B, 351 (1971)

H.V.Geramb

A Microscopic Analysis of 13C(p, n)13N(gs), Including the Core Polarization Exchange Process

NUCLEAR REACTIONS 13C(p, n), E=12.2, 13.3 MeV; calculated σ(θ). Antisymmetrized DWBA, core polarization exchange.

doi: 10.1016/0370-2693(71)90199-7
Citations: PlumX Metrics


1970GE11      Phys.Lett. 32B, 665 (1970)

H.V.Geramb, K.Amos

Proton Scattering to the 3/2- State of 207Pb

NUCLEAR REACTIONS 207Pb(p, p'), E=20.2 MeV; measured nothing; analyzed σ(θ).

doi: 10.1016/0370-2693(70)90438-7
Citations: PlumX Metrics


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Note: The following list of authors and aliases matches the search parameter H.V.Geramb: , H.V.GERAMB