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Search: Author = W.Schneider

Found 40 matches.

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1995PR02      Phys.Rev. C51, R2283 (1995)

J.W.Price, G.Anton, J.Arends, W.Beulertz, A.Bock, M.Breuer, K.Buchler, M.Clajus, P.Detemple, J.Hey, D.Kramer, W.Meyer, B.M.K.Nefkens, G.Noldeke, W.Schneider, B.Zucht

(Eta) Meson Photoproduction on Hydrogen Near Threshold

NUCLEAR REACTIONS 1H(γ, X), E=707.2-717.7 MeV; measured eta production σ(E); deduced S-wave production.

doi: 10.1103/PhysRevC.51.R2283
Citations: PlumX Metrics


1994BU10      Nucl.Phys. A570, 580 (1994)

K.Buchler, K.H.Althoff, G.Anton, J.Arends, W.Beulertz, M.Breuer, P.Detemple, H.Dutz, E.Kohlgarth, D.Kramer, W.Meyer, G.Noldeke, W.Schneider, W.Thiel, B.Zucht

Photoproduction of Positive Pions from Hydrogen with PHOENICS at ELSA

NUCLEAR REACTIONS 1H(γ, π+), E=220-900 MeV bremsstrahlung; measured σ(θ). Model comparison.

doi: 10.1016/0375-9474(94)90074-4
Citations: PlumX Metrics


1988ST20      Nucl.Phys. A489, 146 (1988)

H.Stege, H.-J.Keim, H.A.Bosser, B.Kohlmeyer, F.Puhlhofer, W.F.W.Schneider

Evidence for Cluster Emission in Fusion Reactions between 48Ti and 45Sc at 16 MeV/u

NUCLEAR REACTIONS 45Sc(48Ti, X), E=767 MeV; measured evaporation residue like products σ(θ, mass) vs velocity for A(X) ≥ 53; deduced (cm) velocity distributions, relation to the emitted particles.

doi: 10.1016/0375-9474(88)90058-9
Citations: PlumX Metrics


1987KE02      Z.Phys. A327, 101 (1987)

H.-J.Keim, B.Kohlmeyer, H.Stege, H.A.Bosser, F.Puhlhofer, W.F.W.Schneider

Particle Emission in Central Nuclear Collisions between 48Ti and 45Sc at 16 MeV/u

NUCLEAR REACTIONS 45Sc(48Ti, pX), (48Ti, αX), E=16 MeV/nucleon; measured p-spectra, α-spectra, velocity distributions, fragment mass, p(fragment)-, α(fragment)-coin. ΔE-E telescopes.


1987SO09      Nucl.Phys. A467, 349 (1987)

H.Sohlbach, H.Freiesleben, W.F.W.Schneider, D.Schull, P.Braun-Munzinger, B.Kohlmeyer, M.Marinescu, F.Puhlhofer

Excitation Energy Sharing in 86Kr-Induced Quasielastic Reactions on 197Au and 208Pb between 10 and 18.2 MeV/u

NUCLEAR REACTIONS 197Au(86Kr, X), E=13 MeV/nucleon; 208Pb(86Kr, X), E=10, 13, 18.2 MeV/nucleon; measured total kinetic energy loss spectra of projectile-like fragments; deduced fragment mass, charge, average value, fluctuations of excitation energy sharing for quasielastic reactions. Monte Carlo simulation of sequential neutron emission.

doi: 10.1016/0375-9474(87)90534-3
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1987SO14      Z.Phys. A328, 205 (1987)

H.Sohlbach, H.Freiesleben, W.F.W.Schneider, D.Schull, B.Kohlmeyer, M.Marinescu, F.Puhlhofer

Inelastic Excitation and Nucleon Transfer in Quasielastic Reactions between 86Kr and 208Pb at 18.2 MeV/u Beam Energy

NUCLEAR REACTIONS 208Pb(86Kr, 86Kr), (86Kr, 86Kr'), (86Kr, X), (86Kr, xnyp), E=18.2 MeV/nucleon; measured σ(θ), transfer reaction σ(θ), total kinetic energy spectra for fragment mass=81-88, Z=34-37; deduced transfer probabilities for production of 84,85,87,88Kr, 85Br, 87Rb.


1986BA34      Nucl.Phys. A456, 489 (1986)

D.Bangert, F.Busch, B.Kohlmeyer, F.Puhlhofer, H.Freiesleben, B.Heusch, K.D.Hildenbrand, W.F.W.Schneider, D.Schull

Symmetric Fragmentation in the System 132Xe + 56Fe at 5.0, 5.7 and 8.5 MeV/u Beam Energy

NUCLEAR REACTIONS 56Fe(132Xe, X), E=5, 5.7, 8.5 MeV/nucleon; measured σ(fragment θ); deduced fission, capture σ(E), compound nucleus formation mechanisms.

doi: 10.1016/0375-9474(86)90407-0
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1986HE28      J.Less-Common Met. 122, 445 (1986)

F.P.Hessberger, G.Munzenberg, S.Hofmann, P.Armbruster, Y.K.Agarwal, W.Reisdorf, K.Poppensieker, K.-H.Schmidt, J.R.H.Schneider, W.F.W.Schneider, H.J.Schott, C.-C.Sahm, D.Vermeulen, B.Thuma

Experiments on the Synthesis of Neutron-Deficient Isotopes with Atomic Numbers in the Region from Z = 102 to Z = 105

RADIOACTIVITY 258,257Db, 256,255Rf, 254,253Lr(α) [from 206,208Pb(48Ca, xn), E ≈ 15-30 MeV/nucleon; 207,208Pb, 209Bi(50Ti, xn), E=20-35 MeV/nucleon]; measured Eα, T1/2. 256,255Rf(SF); measured total kinetic energy release.

NUCLEAR REACTIONS 206,208Pb(48Ca, xn), E ≈ 15-30 MeV/nucleon; 207,208Pb, 209Bi(50Ti, xn)258Db/257Db/255Rf/256Rf/254Lr/253Lr, E ≈ 20-35 MeV/nucleon; measured evaporation residue, Z=104, 105, Lr isotope production σ(E).

doi: 10.1016/0022-5088(86)90440-6
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1985AR02      Phys.Rev.Lett. 54, 406 (1985)

P.Armbruster, Y.K.Agarwal, W.Bruchle, M.Brugger, J.P.Dufour, H.Gaggeler, F.P.Hessberger, S.Hofmann, P.Lemmertz, G.Munzenberg, K.Poppensieker, W.Reisdorf, M.Schadel, K.-H.Schmidt, J.H.R.Schneider, W.F.W.Schneider, K.Summerer, D.Vermeulen, G.Wirth, A.Ghiorso, K.E.Gregorich, D.Lee, M.Leino, K.J.Moody, G.T.Seaborg, R.B.Welch, P.Wilmarth, S.Yashita, C.Frink, N.Greulich, G.Herrmann, U.Hickmann, N.Hildebrand, J.V.Kratz, N.Trautmann, M.M.Fowler, D.C.Hoffman, W.R.Daniels, H.R.von Gunten, H.Dornhofer

Attempts to Produce Superheavy Elements by Fusion of 48Ca with 248Cm in the Bombarding Energy Range of 4.5-5.2 MeV/u

NUCLEAR REACTIONS 248Cm(48Ca, X), E=4.5-5.2 MeV/nucleon; measured superheavy production σ upper limits vs T1/2. Different separation techniques.

doi: 10.1103/PhysRevLett.54.406
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1985HE17      Z.Phys. A322, 309 (1985)

B.Heusch, H.Freiesleben, W.F.W.Schneider, B.Kohlmeyer, H.Stege, F.Puhlhofer

A Fast-Fission Component with Small Mass Drift in the Reaction 84Kr + 27Al at E(lab) = 5.9 MeV/u

NUCLEAR REACTIONS 27Al(84Kr, X), E=5.94 MeV/nucleon; measured σ(fragment θ) for fragment Z=10-41; deduced total, reaction, deep inelastic, quasielastic, evaporation, fast fission σ, maximum (L).

doi: 10.1007/BF01411896
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1985HE22      Z.Phys. A322, 557 (1985)

F.P.Hessberger, G.Munzenberg, S.Hofmann, Y.K.Agarwal, K.Poppensieker, W.Reisdorf, K.-H.Schmidt, J.R.H.Schneider, W.F.W.Schneider, H.J.Schott, P.Armbruster, B.Thuma, C.-C.Sahm, D.Vermeulen

The New Isotopes 258105, 257105, 254Lr and 253Lr

RADIOACTIVITY 258Db, 257Db, 253,254Lr(α) [from 209Bi(50Ti, X), E=4.65-4.95 MeV/nucleon]; measured Eα, Iα, T1/2. 258Rf(SF) [from 258Db(EC-decay)]; measured T1/2, fission fragment total kinetic energy.

NUCLEAR REACTIONS 209Bi(50Ti, X), E=4.65-4.95 MeV/nucleon; measured Eα, Iα, evaporation residue σ(E) for one-, two-neutron emission; deduced evidence for 258Db, 257Db, 253,254Lr.


1985RE03      Nucl.Phys. A438, 212 (1985)

W.Reisdorf, F.P.Hessberger, K.D.Hildenbrand, S.Hofmann, G.Munzenberg, K.-H.Schmidt, J.H.R.Schneider, W.F.W.Schneider, K.Summerer, G.Wirth, J.V.Kratz, K.Schlitt

Fusion Near the Threshold: A comparative study of the system 40Ar + 112,116,112Sn and 40Ar + 144,148,154Sm

NUCLEAR REACTIONS 112,116,122Sn, 144,148,154Sm(40Ar, X), (40Ar, F), E=125-179 MeV; measured evaporation residues, fission; deduced fusion σ around, below Coulomb barrier. 152,156,162Er, 184,188,194Hg, 144,148,154Sm deduced barrier height, barrier fluctuation, role of coupling to inelastic, transfer channels, partial wave distribution above barrier. Enriched targets, velocity filter, K X-ray and γ-ray activation method, ionization chamber.

doi: 10.1016/0375-9474(85)90125-3
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1985RE11      Nucl.Phys. A444, 154 (1985)

W.Reisdorf, F.P.Hessberger, K.D.Hildenbrand, S.Hofmann, G.Munzenberg, K.-H.Schmidt, W.F.W.Schneider, K.Summerer, G.Wirth, J.V.Kratz, K.Schlitt, C.-C.Sahm

Fusability and Fissionability in 86Kr-Induced Reactions Near and Below the Fusion Barrier

NUCLEAR REACTIONS 70,76Ge, 92,100Mo, 99,102,104Ru(86Kr, X), E=257-369 MeV; measured evaporation residues; deduced evaporation residue σ at, below Coulomb barrier, barrier height, barrier fluctuation, role of coupling to inelastic channels. 156,162Er, 178,186Pt, 185,188,190Hg deduced effective fission barriers. Enriched targets, velocity filter, K X-ray activation method.

doi: 10.1016/0375-9474(85)90296-9
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1985SO04      Phys.Lett. 153B, 386 (1985)

H.Sohlbach, H.Freiesleben, P.Braun-Munzinger, W.F.W.Schneider, D.Schull, B.Kohlmeyer, M.Marinescu, F.Puhlhofer

Channel-Dependent Sharing of the Excitation Energy in Quasielastic Reactions between 208Pb + 86Kr

NUCLEAR REACTIONS 208Pb(86Kr, 84Kr), (86Kr, 85Kr), (86Kr, 86Kr), (86Kr, 87Kr), E=18.2 MeV/nucleon; measured ejectile spectra; deduced primary fragment excitation energy sharing. Monte Carlo simulation.

doi: 10.1016/0370-2693(85)90478-2
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1984MU07      Z.Phys. A315, 145 (1984)

G.Munzenberg, W.Reisdorf, S.Hofmann, Y.K.Agarwal, F.P.Hessberger, K.Poppensieker, J.R.H.Schneider, W.F.W.Schneider, K.-H.Schmidt, H.-J.Schott, P.Armbruster, C.-C.Sahm, D.Vermeulen

Evidence for Element 109 from One Correlated Decay Sequence following the Fusion of 58Fe with 209Bi

RADIOACTIVITY 266Mt(SF) [from 209Bi(58Fe, X), E=5.15 MeV/nucleon]; measured Eα, Iα, αα-coin, SF-decay.

NUCLEAR REACTIONS 209Bi(58Fe, X), E=4.95, 5.05, 5.15 MeV/nucleon; measured σ(fragment) vs mass, Eα, Iα, SF-decay; deduced evidence for compound nucleus 266Mt.


1982MU15      Z.Phys. A309, 89 (1982)

G.Munzenberg, P.Armbruster, F.P.Hessberger, S.Hofmann, K.Poppensieker, W.Reisdorf, J.H.R.Schneider, W.F.W.Schneider, K.-H.Schmidt, C.-C.Sahm, D.Vermeulen

Observation of One Correlated α-Decay in the Reaction 58Fe on 209Bi → 267109

RADIOACTIVITY 266Mt [from 209Bi(58Fe, n), E=4.95-5.15 MeV/nucleon]; measured Eα, time correlated α-spectra; deduced α-decay chain correlation followed by 258Rf fission. Evaporation residue implantation technique.

NUCLEAR REACTIONS 209Bi(58Fe, n), E=4.95-5.15 MeV/nucleon; measured Eα, time correlated α-spectra; deduced evidence for 266Mt. Evaporation residue implantation technique.


1982RE18      Phys.Rev.Lett. 49, 1811 (1982)

W.Reisdorf, F.P.Hessberger, K.D.Hildenbrand, S.Hofmann, G.Munzenberg, K.-H.Schmidt, J.H.R.Schneider, W.F.W.Schneider, K.Summerer, G.Wirth, J.V.Kratz, K.Schlitt

Influence of Collective Surface Motion on the Threshold Behavior of Nuclear Fusion

NUCLEAR REACTIONS, ICPND 112,116,122Sn, 144,148,154Sm(40Ar, X), E=3.2-4.5 MeV/nucleon; measured fusion σ vs E; deduced barrier fluctuation effects.

doi: 10.1103/PhysRevLett.49.1811
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1981KO21      Z.Phys. A301, 349 (1981)

B.Kohlmeyer, F.Puhlhofer, G.Sletten, H.Freiesleben, W.Schafer, W.F.W.Schneider, R.Bock

Search for Delayed α-Decay of High Spin Isomers in Heavy-Ion Induced Fusion Reactions

NUCLEAR REACTIONS 12C, 16O, 24Mg, 27Al, 28Si, 51V, 55Mn, 56Fe, 58Ni, 63Cu(132Xe, α), E=5.4 MeV/nucleon; 56Fe, Zr, Mo, 100Mo, 102,104Ru, 103Rh, 104,106,108,110Pd, 107,109Ag, 112Cd, 116Sn(50Ti, α), E=4.8 MeV/nucleon; measured compound nuclear recoil, possible delayed α-emission; deduced no α-decaying high-spin isomers.

doi: 10.1007/BF01421700
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1979BU04      Z.Phys. A290, 167 (1979)

F.Busch, M.J.Canty, W.Pfeffer, B.Kohlmeyer, W.Schafer, W.F.W.Schneider, H.Freiesleben, F.Puhlhofer

A Study of the Influence of Shell Effects in Nuclear Level Densities on the Decay of the Compound Nucleus 58Ni

NUCLEAR REACTIONS 12C(46Ti, xnyα), E=5.8 MeV/nucleon; measured fragment mass, charge distribution, σ(fusion), σ(θ) of evaporation residues for X=2-4, y=1, 2. Monte Carlo calculations.

doi: 10.1007/BF01408111
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1979FR10      Z.Phys. A292, 171 (1979)

H.Freiesleben, K.D.Hildenbrand, F.Puhlhofer, W.F.W.Schneider, R.Bock, D.v.Harrach, H.J.Specht

The Reaction 238U + 238U at 7.42 MeV/u

NUCLEAR REACTIONS 238U(238U, 238U), 238U(238U, X), E=1766 MeV; measured σ(θ), σ(Eα), α(X-ray)-coin; deduced production σ for 208,210Po, 211At, 222Rn, 223,224,225Ra, 225,226Ac, 227,228Th, 230U, 230Pa, superheavy nuclei.

doi: 10.1007/BF01441624
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1978HE20      Z.Phys. A288, 391 (1978)

B.Heusch, C.Volant, H.Freiesleben, R.P.Chestnut, K.D.Hildenbrand, F.Puhlhofer, W.F.W.Schneider, B.Kohlmeyer, W.Pfeffer

The Reaction Mechanism in the System 132Xe + 56Fe at 5.73 MeV/u: Evidence for a New Type of Strongly Damped Collisions

NUCLEAR REACTIONS 56Fe(132Xe, X), E=5.73 MeV/nucleon; measured σ(E, θ) for target-, projectile-like fragments; deduced evidence for a new type of damped collision.

doi: 10.1007/BF01417723
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1978HI09      Nukleonika 23, 347 (1978)

K.D.Hildenbrand, H.Freiesleben, F.Puhlhofer, W.F.W.Schneider, R.Bock, D.v.Harrach, H.J.Specht

Reactions Induced by 238U on 238U at 1766 MeV

NUCLEAR REACTIONS 238U(238U, X), E=1766 MeV; measured σ(E(A), Z, θ).


1977FR10      Z.Phys. A282, 39 (1977)

K.Freitag, K.Krien, J.C.Soares, P.Herzog, W.D.Schneider, E.Bodenstedt

The Penetration Parameter λ of the Anomalous M1-Conversion of the 482 keV Transition in 181Ta

RADIOACTIVITY 181Hf; measured γγ(θ, H, t), γce-coin. 181Ta deduced δ, ICC, penetration parameter of M1 transition.

doi: 10.1007/BF01881004
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1977GU05      Phys.Rev. C15, 1298 (1977)

C.Gunther, H.Hubel, A.Kleinrahm, D.Mertin, B.Richter, W.D.Schneider, R.Tischler

High-Spin States in Even Hg Nuclei and Rotation Alignment in 198Hg

NUCLEAR REACTIONS 194,196,198Pt(α, xnγ), E=28, 31, 34, 48 MeV; measured Eγ, Iγ, γγ-coin, γ(θ, t), ce(t). 194,196,198,200Hg deduced levels, J, π, T1/2, ICC, λ, B(λ). Rotation-alignment model.

doi: 10.1103/PhysRevC.15.1298
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1977HI08      Phys.Rev.Lett. 39, 1065 (1977)

K.D.Hildenbrand, H.Freiesleben, W.F.W.Schneider, R.Bock, D.v.Harrach, H.J.Specht

Reaction between 238U and 238U at 7.42 MeV/Nucleon

NUCLEAR REACTIONS 238U(238U, X), E=7.42 MeV/nucleon; measured σ(A, Z); deduced upper limit σ for production of superheavy elements.

doi: 10.1103/PhysRevLett.39.1065
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1977PU05      Phys.Rev. C16, 1010 (1977)

F.Puhlhofer, W.F.W.Schneider, F.Busch, J.Barrette, P.Braun-Munzinger, C.K.Gelbke, H.E.Wegner

Isotope and Element Distributions of the Evaporation Residues from Fusion of 160 MeV 32S with 24,25,26Mg and 27Al

NUCLEAR REACTIONS 24,25,26Mg, 27Al(32S, X), E=160 MeV; measured σ(A, Z, θ) for fusion products. Systematics of nuclide distributions as function of compound-nucleus mass are discussed. Comparison with evaporation calculations; shell effects in level densities.

doi: 10.1103/PhysRevC.16.1010
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1976ST18      Phys.Rev. C14, 1824 (1976)

R.Stock, U.Jahnke, D.L.Hendrie, J.Mahoney, C.F.Maguire, W.F.W.Schneider, D.K.Scott, G.Wolschin

Contribution of Alpha Cluster Exchange to Elastic and Inelastic 16O + 20Ne Scattering

NUCLEAR REACTIONS 16O(20Ne, 16O), (20Ne, 20Ne), E=50 MeV; measured σ(θ). Optical model, DWBA, CCBA analyses.

doi: 10.1103/PhysRevC.14.1824
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1975GU04      Nucl.Phys. A244, 287 (1975)

C.Gunther, M.V.Banaschik, H.Hubel, W.D.Schneider, K.H.Gonsior, P.Herzog

High Spin States in 93Mo Populated in the (p, n) Reaction

NUCLEAR REACTIONS 93Nb(p, n), E=7, 10, 14 MeV; measured Eγ, Iγ, γ(t), γγ-coin, I(ce), ce(t). 93Mo deduced levels, J, π, T1/2, ICC, λ, B(λ).

doi: 10.1016/0375-9474(75)90059-7
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1975PU02      Nucl.Phys. A244, 329 (1975)

F.Puhlhofer, W.Pfeffer, B.Kohlmeyer, W.F.W.Schneider

Mass Distributions of Fusion Products in Reactions between 19F and 12C

NUCLEAR REACTIONS 12C(19F, X), E=50, 63.2, 76 MeV; measured σ(E, E(fragment mass), θ), A=11-30, total fusion, direct cross section.

doi: 10.1016/0375-9474(75)90063-9
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1975SC30      Nucl.Phys. A249, 103 (1975)

W.D.Schneider, K.H.Gonsior, C.Gunther

E2 Transition Rates and Seniority Mixing in the Proton 1g9/2 Orbit

NUCLEAR REACTIONS 93Nb(α, 4n), 93Nb(α, α'2n), E=48 MeV; measured I(ce), αce(t). 91Nb, 93Tc levels deduced T1/2, B(E2).

doi: 10.1016/0375-9474(75)90094-9
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1975SC35      Nucl.Phys. A251, 331 (1975)

W.F.W.Schneider, B.Kohlmeyer, F.Puhlhofer, R.Bock

Interfering Transfer Processes in Heavy-Ion Reactions

NUCLEAR REACTIONS 14C(16O, 17O), (16O, 18O), E=20, 25, 30 MeV; measured σ(θ). 11B(16O, 15N), E=27-35 MeV; analyzed σ(θ). DWBA analysis of interference structure in σ(θ). Enriched targets.

doi: 10.1016/0375-9474(75)90075-5
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1975SC42      Z.Phys. A275, 249 (1975)

W.F.W.Schneider, B.Kohlmeyer, F.Puhlhofer

Single-Nucleon Transfer Reactions Induced by 16O on 14C

NUCLEAR REACTIONS 14C(16O, 15N), (16O, 17O), E=20, 25, 30 MeV; measured σ(θ). DWBA analysis.

doi: 10.1007/BF01409292
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1975SC45      Nucl.Instrum.Methods 130, 165 (1975)

W.D.Schneider, K.H.Gonsior

Conversion-Electron and Nuclear Lifetime Measurements with an in-Beam Iron-Free Orange Spectrometer

NUCLEAR REACTIONS 93Nb(p, nγ), E=10 MeV; measured ce(t). 93Mo level deduced T1/2. 208Pb(α, 2nγ), E=30 MeV; measured I(ce). 210Po deduced transitions, λ.

doi: 10.1016/0029-554X(75)90169-X
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1974RI01      Nucl.Instrum.Methods 115, 401 (1974)

B.Richter, V.Martini, W.-D.Schneider, L.Ley, V.Schoner

Lifetime Measurements of Excited States in 219Rn by Observation of Conversion-Electron Doppler Shifts Following α-Decay

RADIOACTIVITY 223Ra; measured αce-coin, recoil distance. 219Rn levels deduced T1/2.

doi: 10.1016/0029-554X(74)90239-0
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1974TA18      Z.Phys. 271, 409 (1974)

L.Tauscher, W.Schneider

Optical Potential Calculations for the 1s Level in Pionic Atoms

NUCLEAR REACTIONS 4He, 6,7Li, 9Be, 10,11B, 12C, 14N, 16,18O, 19F, 20Ne(π, π); calculated optical potential.

doi: 10.1007/BF02126196
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1973SC24      Phys.Lett. 46B, 195 (1973)

W.F.W.Schneider, B.Kohlmeyer, F.Puhlhofer, R.Bock

Interference of Two-Neutron and α-Transfer in the Reaction 14C(16O, 18O)12C

NUCLEAR REACTIONS 14C(16O, 18O), E=20, 25, 30 MeV; measured σ(θ).

doi: 10.1016/0370-2693(73)90682-5
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1962ST24      TID-17089 (Pt. II) (1962)

R.M.Steffen, E.Matthias, W.Schneider

Tables of Directional Correlation Attenuation Coefficients for Combined Magentic Dipole and Randomly Oriented Electric Quadrupole Interactions


1962ST25      TID-17089 (Pt.I) (1962)

R.M.Steffen, E.Matthias, W.Schneider

Tables of Directional Correlation Attenuation Coefficients for Combined Magnetic Dipole and Randomly Oriented Electric Quadrupole Interactions


1961HA44      Proc.Conf.Electromagnetic Lifetimes and Properties Nuclear States, Gatlinburg, Tennessee (October 1961); NAS-NRC Publ. 974, p.230 (1962)

U.Hauser, E.N.Hatch, K.Runge, G.Knissel, W.Schneider

Measurements of E1 Transition Probabilities in Several Deformed Odd-A Nuclei as a Study of a Single Particle Motion

NUCLEAR STRUCTURE 169Tm, 175Lu, 177Hf, 155Gd; measured not abstracted; deduced nuclear properties.


1960SC14      Nuclear Phys. 21, 55 (1960)

W.Schneider

Contributions to the Decay of Eu152

NUCLEAR STRUCTURE 152Eu; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(60)90031-6
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Note: The following list of authors and aliases matches the search parameter W.Schneider: , W.D.SCHNEIDER, W.E.SCHNEIDER, W.F.SCHNEIDER