NSR Query Results


Output year order : Descending
Format : Normal

NSR database version of April 27, 2024.

Search: Author = L.T.van der Bijl

Found 7 matches.

Back to query form



1985MI15      Phys.Rev. C32, 805 (1985)

T.E.Milliman, J.H.Heisenberg, F.W.Hersman, J.P.Connelly, C.N.Papanicolas, J.E.Wise, H.P.Blok, L.T.van der Bijl

Determination of the π1g9/2 Orbit Size in 88Sr, 90Zr, and 92Mo from Inelastic Electron Scattering

NUCLEAR STRUCTURE 88Sr, 90Zr, 92Mo; calculated spectroscopic amplitudes for 8+ transitions, rms radii of 1g9/2 proton orbit. Shell model, electron scattering data input.

NUCLEAR REACTIONS 88Sr, 90Zr, 92Mo(e, e'), E=100-370 MeV; measured σ(E, θ) vs momentum transfer for 8+ states. 88Sr, 90Zr, 92Mo deduced point proton density. Shell model.

doi: 10.1103/PhysRevC.32.805
Citations: PlumX Metrics


1984VA16      J.Phys.(Paris), Colloq.C4, 465 (1984); See 1984Va42

L.T.van der Bijl, H.Blok, H.P.Blok, R.Ent, J.Heisenberg, O.Schwentker, A.Richter, P.K.A.de Witt Huberts

Electro-Excitation of the 1+ State at 3.486 MeV in 88Sr


1984VA21      Nucl.Phys. A423, 365 (1984)

L.T.Van Der Bijl, H.Blok, H.P.Blok, R.Ent, J.Heisenberg, O.Schwentker, A.Richter, P.K.A.De Witt Huberts

Electro-Excitation of the 1+ State at E(x) = 3.486 MeV in 88Sr

NUCLEAR REACTIONS 88Sr(e, e'), E=23.7-261.6 MeV; measured σ(θ), σ(E(e')); deduced form factor, core, isobar-hole polarization effects.

doi: 10.1016/0375-9474(84)90029-0
Citations: PlumX Metrics


1984VA42      J.Phys.(Paris), Colloq.C-4, 465 (1984)

L.T.van der Bijl, H.Blok, H.P.Blok, R.Ent, J.Heisenberg, O.Schwentker, A.Richter, P.K.A.de Witt Huberts

Electro-Excitation of the 1+ State at 3, 486 MeV in 88Sr

NUCLEAR REACTIONS 88Sr(e, e'), E=81.4, 209.5 MeV; measured σ(Ee', θe'), form factor. 88Sr transition deduced B(M1) reduction. Enriched target. Theoretical analyses.


1983SC01      Phys.Rev.Lett. 50, 15 (1983)

O.Schwentker, J.Dawson, J.Robb, J.Heisenberg, J.Lichtenstadt, C.N.Papanicolas, J.Wise, J.S.McCarthy, L.T.van der Bijl, H.P.Blok

E2 Transition Densities and Proton Shell Structure in 88Sr, 89Y, and 90Zr

NUCLEAR REACTIONS 88Sr, 89Y, 90Zr(e, e'), E not given; measured σ(θ). 89Y, 90Zr levels deduced E2 transition charge densities. 88Sr levels deduced spectroscopic amplitudes, E2 transition charge densities. Fourier-Bessel expansion, RPA, broken pair calculations.

doi: 10.1103/PhysRevLett.50.15
Citations: PlumX Metrics


1983VA03      Nucl.Phys. A393, 173 (1983)

L.T.Van Der Bijl, H.P.Blok, J.F.A.Van Hienen, J.Blok

High Resolution Investigation of 90Zr with (p, p') Scattering at 25 MeV

NUCLEAR REACTIONS 90Zr(p, p'), E=25.05 MeV; measured σ(θ); deduced two-step excitation effects. 90Zr deduced levels, L, β(L), J, π, enhancement factors. Enriched target. Macroscopic, microscopic DWBA analysis, broken pair wave functions.

doi: 10.1016/0375-9474(83)90071-4
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0733.


1982VA05      Z.Phys. A305, 231 (1982)

L.T.van der Bijl, H.P.Blok, R.Frey, D.Meuer, A.Richter, P.K.A.de Witt Huberts

Quenching of the Electron Scattering Form Factor of the 1+ State at 3.48 MeV in 88Sr and the Influence of the Δ(1232)-Isobar

NUCLEAR REACTIONS 88Sr(e, e'), E=36, 42, 50 MeV; measured σ(E(e'), θ=165°), form factor. 88Sr deduced isobar role in M1 transition strength quenching.


Back to query form