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NSR database version of April 27, 2024.

Search: Author = D.Evers

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1984SK03      Nuovo Cim. 81A, 331 (1984)

S.J.Skorka, D.Evers, K.E.G.Lobner, R.Pengo, U.Quade, K.Rudolph, I.Weidl

Experiments with the Munich Recoil Spectrometer

NUCLEAR REACTIONS, ICPND ^{100,98,96,94,92}Mo(³²S, X), (³⁶S, X), E(cm) ≈ 74-90 MeV; measured fusion σ(E). ¹²C(¹⁶O, p), E(cm)=19-26 MeV; measured σ(Ep), σ(θ) vs E. ²⁷Al deduced high-spin state decay characteristics. Recoil spectrometer.

doi: 10.1007/BF02724173
Citations: PlumX Metrics

1984WE16      Z.Phys. A319, 67 (1984)

I.Weidl, D.Evers, P.Konrad, K.E.G.Lobner, U.Quade, K.Rudolph, S.J.Skorka

Properties of Unbound High-Spin States in ²⁷Al

NUCLEAR REACTIONS ¹²C(¹⁶O, p), E(cm)=18.7-30.1 MeV; measured σ(Ep), σ(θ) vs E, recoil velocity spectra. ²⁷Al deduced resonances, J, π, α-, γ-, n-branching ratios, shape characteristics, (Γγ/Γ), (Γn/Γ).

doi: 10.1007/BF01429769
Citations: PlumX Metrics

1983RU01      Nucl.Instrum.Methods 204, 407 (1983)

K.Rudolph, D.Evers, P.Konrad, K.E.G.Lobner, U.Quade, S.J.Skorka, I.Weidl

The Munich RF-Recoil Spectrometer for the Observation of Heavy-Ion Reaction Products at Zero Degree

NUCLEAR REACTIONS ¹²C(¹⁶O, X), E=53.6 MeV; measured σ(fragment) vs Z, σ(fragment) vs mass for Mg isotopes, (²⁴Mg)(α)-coin; ¹²C(¹⁶O, p), (¹⁶O, pn), E=53.6 MeV; measured residual nuclei recoils. ¹⁰⁴Ru(³⁶S, X), E=100 MeV; measured evaporation residue transmission. RF recoil spectrometer.

doi: 10.1016/0167-5087(83)90069-8
Citations: PlumX Metrics

1981GR10      Phys.Scr. 24, 337 (1981)

E.Grosse, A.Balanda, H.Emling, F.Folkmann, P.Fuchs, R.B.Piercey, D.Schwalm, R.S.Simon, H.J.Wollersheim, D.Evers, H.Ower

Collective Rotation of ²³⁸U at High Spins

NUCLEAR REACTIONS ²³⁸U(²⁰⁸Pb, ²⁰⁸Pb'), E=5.3, 5.9 MeV/nucleon; measured Eγ, Iγ, γγ-coin, Coulomb excitation, DSA. ²³⁸U deduced ground state band B(E2), T_1/2, octupole bands, high-spin state collectivity. Rigid rotor description.

doi: 10.1088/0031-8949/24/1B/033
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1978EV03      Fizika, Suppl. 10, 5 (1978)

D.Evers, W.Assmann, J.Ehrenberg, P.Konrad, K.E.G.Lobner

Evidence for a Non-Statistical Population of High Spin States in ²⁴Mg Via the ¹²C(¹³C, n) Reaction

NUCLEAR REACTIONS ¹²C(¹³C, n), E(cm)=14.08-15.26 MeV; measured σ(θ). ²⁴Mg levels deduced evidence for non-statistical population mechanism. DWBA, Hauser-Feshbach analysis.

1977EV01      Nucl.Phys. A275, 363 (1977)

D.Evers, C.Ley, E.Spindler, W.Assmann, K.Rudolph, P.Konrad, P.Sperr

The (³He, n) Reaction on ¹⁶O and ¹⁸O

NUCLEAR REACTIONS ¹⁶O(³He, n), E=15, 18, 21 MeV; ¹⁸O(³He, n), E=18 MeV; measured σ(θ, En). ^18,20Ne deduced levels, J, π. Natural ¹⁶O, enriched ¹⁸O targets.

doi: 10.1016/0375-9474(77)90458-4
Citations: PlumX Metrics

1977EV02      Z.Phys. A280, 287 (1977)

D.Evers, G.Denhofer, W.Assmann, A.Harasim, P.Konrad, C.Ley, K.Rudolph, P.Sperr

Investigation of High Spin States in ²³Na and ²³Mg and the ¹²C + ¹²C Resonance at E(c.m.) = 19.3 MeV

NUCLEAR REACTIONS ¹²C(¹²C, nγ), (¹²C, pγ), (¹²C, np), E=19.3 MeV; measured particle γ-coin, DSA. ²³Na, ²³Mg levels deduced T_1/2, J, π. ²³Mg deduced resonances, proton branching.

doi: 10.1007/BF01434357
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1977EV03      Phys.Rev. C15, 1690 (1977)

D.Evers, A.Harasim, R.L.McGrath, W.Assmann

Gamma Spectroscopy of ⁵²Fe, ⁵²Mn, and ⁵²Cr from α + ⁵⁰Cr Reactions

NUCLEAR REACTIONS ⁵⁰Cr(α, X), E=23.5, 27.2 MeV; measured relative σ(Eγ), particle-γ triple coin, γγ-coin. ⁵²Cr, ⁵²Mn, ⁵²Fe deduced levels, J, π. ⁴⁹V, ⁵⁰Cr, ⁵³Mn, ⁵⁴Fe deduced transitions. Enriched target.

doi: 10.1103/PhysRevC.15.1690
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1975SP05      Phys.Lett. 57B, 438 (1975)

P.Sperr, D.Evers, A.Harasim, W.Assmann, P.Konrad, K.Rudolph, G.Denhoefer, C.Ley

The Neutron Decay of the Resonance in the ¹²C + ¹⁶O System at E(c.m.) = 19.7 MeV

NUCLEAR REACTIONS ¹²C(¹⁶O, n), E=19.39, 19.70, 20.6, 22.0, 22.6 MeV; measured σ(E, En, θ). ²⁸Si deduced resonances.

doi: 10.1016/0370-2693(75)90262-2
Citations: PlumX Metrics

1974EV02      Nucl.Phys. A230, 109 (1974)

D.Evers, W.Assmann, K.Rudolph, S.J.Skorka, P.Sperr

The (³He, n) Reaction on Even (f, p) Shell Nuclei at 15, 18 and 21 MeV (II)

NUCLEAR REACTIONS ^40,42,44,48Ca, ^46,48,50Ti, ^58,60Ni, ⁶⁴Zn, ^50,52,54Cr, ⁵⁴Fe(³He, n), E=15, 18, 21 MeV; measured σ(θ, En). ^42,44,46,50Ti, ^48,50,52Cr, ^60,62Zn, ⁶⁶Ge, ^52,54,56Fe, ⁵⁶Ni deduced levels, J, π. Enriched targets.

doi: 10.1016/0375-9474(74)90533-8
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1974HI06      Nucl.Phys. A232, 157 (1974)

P.Hille, P.Sperr, M.Hille, K.Rudolph, W.Assmann, D.Evers

Spin Dependence of the Nuclear Level Density from Angular Distributions of (α, n) Reactions

NUCLEAR REACTIONS ⁴⁶Ti, ^54,56Fe, ^58,60,62Ni, ⁹⁰Zr, ⁹³Nb, ⁹²Mo, ¹¹⁵In(α, n), E approx 15.3 MeV; ⁵⁹Co(α, n), E=14.0 MeV; measured σ(En, θ). ⁴⁹Cr, ^57,59Ni, ⁶²Cu, ^61,63,65Zn, ⁹³Mo, ⁹⁶Tc, ⁹⁵Ru, ¹¹⁸Sb deduced spin cut-off factors. Isotopically separated, natural targets.

doi: 10.1016/0375-9474(74)90650-2
Citations: PlumX Metrics

1974SP03      Phys.Lett. 49B, 345 (1974)

P.Sperr, D.Evers, K.Rudolph, W.Assmann, E.Spindler, P.Konrad, G.Denhofer

Study of the ¹²C(¹²C, n)²³Mg Reaction Around the Resonance at E(cm) = 19.3 MeV

NUCLEAR REACTIONS ¹²C(¹²C, n), E(cm)=19.3 MeV; measured σ(Eγ, En, θ(n)), nγ-coin. ²³Mg deduced levels. ²⁴Mg deduced resonance.

doi: 10.1016/0370-2693(74)90177-4
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1972EV02      Nucl.Phys. A198, 268 (1972)

D.Evers, W.Assmann, K.Rudolph, S.J.Skorka, P.Sperr

The (³He, n) Reaction on Even (f, p) Shell Nuclei at 18 and 21 MeV (I)

NUCLEAR REACTIONS ^50,52,54Cr, ^54,56,58Fe(³He, n), E(³He)=18, 21 MeV; measured σ(θ, En). ^52,54,56Fe, ^56,58,60Ni deduced levels, J, π. Enriched targets.

doi: 10.1016/0375-9474(72)90784-1
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1970EV02      Phys.Lett. 33B, 559 (1970)

D.Evers, W.Stocker

Shell Model Calculations for ³⁴Cl and ³⁸K with the Modified Surface Delta Interaction Including a Tensor Force

NUCLEAR STRUCTURE ³⁴Cl, ³⁸K; calculated levels, wave functions, log ft, branching ratios. Shell model, surface delta interaction with tensor force.

doi: 10.1016/0370-2693(70)90348-5
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1968EV03      Phys.Letters 27B, 423 (1968)

D.Evers, G.Flugge, J.Morgenstern, T.W.Retz-Schmidt, H.Schmidt, J.W.Schmidt, S.J.Skorka

Widths of the 6.92(2⁺) and 7.12(1^-) MeV Levels in ¹⁶O

NUCLEAR STRUCTURE ¹⁶O; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(68)90225-6
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1967EV01      Nucl.Phys. A91, 472(1967)

D.Evers, J.Hertel, T.W.Retz-Schmidt, S.J.Skorka

Lifetime of the 3/2+, 1.013 MeV State and the Excited-Core Model of ²⁷Al

NUCLEAR REACTIONS ²⁷Al(γ, γ), E = 1.013 MeV; measured σ. ²⁷Al level deduced level-width.

doi: 10.1016/0375-9474(67)90056-5
Citations: PlumX Metrics

1966SK01      Nucl.Phys. 81, 370(1966)

S.J.Skorka, D.Evers, J.Hertel, J.Morgenstern, T.W.Retz-Schmidt, H.Schmidt

Nuclear Resonance Fluorescence and the Slowing Down of Recoil Nuclei in Matter

NUCLEAR REACTIONS ²³Na, ²⁴Mg, ²⁸Si, ³¹P(γ, γ), E = 0.440, 1.368, 1.772, 1.265 MeV; measured σ; deduced de/dx for heavy nuclei. ²³Na, ²⁴Mg, ²⁸Si, ³¹P deduced T_1/2 (level). Enriched ²⁴Mg target.

doi: 10.1016/S0029-5582(66)80028-7
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1965SK01      Nucl.Phys. 68, 177(1965)

S.J.Skorka, T.W.Retz-Schmidt, H.Schmidt, J.Morgenstern, D.Evers

Width of the 4.931 MeV Level in Si²⁹

NUCLEAR REACTIONS ²⁹Si(γ, γ) [from ²⁸Si(d, pγ)], E approx 4.9, 6.4 MeV; measured σ. ²⁹Si deduced level-width, T_1/2. Natural target.

doi: 10.1016/0029-5582(65)90378-0
Citations: PlumX Metrics