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NSR database version of April 26, 2024.

Search: Author = C.Stoller

Found 19 matches.

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1993MO03      Phys.Rev.Lett. 70, 537 (1993)

J.D.Molitoris, W.E.Meyerhof, Ch.Stoller, R.Anholt, D.W.Spooner, L.G.Moretto, L.G.Sobotka, R.J.McDonald, G.J.Wozniak, M.A.McMahan, L.Blumenfeld, N.Colonna, M.Nessi, E.Morenzoni

Molecular-Orbital Study of Late-Fission Times in Deep-Inelastic 238U + 238U Collisions

NUCLEAR REACTIONS 238U(238U, X), (238U, F), E=7.5 MeV/nucleon; measured K-vacancy production probability for no-fission, single-, double fission channels; deduced U-like products late fission time scales.

doi: 10.1103/PhysRevLett.70.537
Citations: PlumX Metrics

1988BA05      Phys.Rev.Lett. 60, 913 (1988)

O.K.Baker, W.E.Meyerhof, D.W.Spooner, Ch.Stoller, J.N.Scheurer

Nuclear Resonance Effect in Atomic Electron Capture by Protons

ATOMIC PHYSICS 20Ne(p, p), E ≈ 1.5-1.52 MeV; measured electron capture probability vs E; deduced nuclear resonance effect dominance.

doi: 10.1103/PhysRevLett.60.913
Citations: PlumX Metrics

1987BA33      Nucl.Instrum.Methods Phys.Res. B24/25, 89 (1987)

O.K.Baker, C.Stoller, W.E.Meyerhof, J.N.Scheurer

The Interplay between Nuclear and Atomic Physics: Electron capture in the presence of a nuclear resonance

ATOMIC PHYSICS 12C, 14N, 20Ne(p, p), E=0.5-1.525 MeV; 22Ne(p, p), E=1.5-1.525 MeV; measured total electron capture probabilities in resonance region.

doi: 10.1016/0168-583X(87)90596-9
Citations: PlumX Metrics

1987NE06      Phys.Rev. C36, 143 (1987)

M.Nessi, Ch.Stoller, E.Morenzoni, W.Wolfli, W.E.Meyerhof, J.D.Molitoris, E.Grosse, Ch.Michel

Time Delay Effects on K X-Ray Production Probability in Deep Inelastic U + U and U + Pb Nuclear Reactions

ATOMIC PHYSICS 208Pb, 238U(238U, X), E=7.5 MeV/nucleon; measured E(K X-ray), I(K X-ray); deduced time delay, inner shell ionization probability.

doi: 10.1103/PhysRevC.36.143
Citations: PlumX Metrics

1987SP01      Phys.Rev.Lett. 58, 341 (1987)

D.W.Spooner, Ch.Stoller, J.-F.Chemin, W.E.Meyerhof, J.-N.Scheurer, X.-Y.Xu

Large Resonance Effect in K-Shell Ionization Probability in Elastic Proton Backscattering on 138Ba

NUCLEAR REACTIONS 138Ba(p, p), E=9.8-10.2 MeV; measured σ(θ), K-shell ionization probability vs E; deduced atomic parameters. 139La deduced IAR, Γ, Γp.

doi: 10.1103/PhysRevLett.58.341
Citations: PlumX Metrics

1986MO29      Z.Phys. D2, 91 (1986)

J.D.Molitoris, Ch.Stoller, R.Anholt, W.E.Meyerhof, D.W.Spooner, R.J.McDonald, L.G.Sobotka, G.J.Wozniak, L.G.Moretto, M.A.McMahan, E.Morenzoni, M.Nessi, W.Wolfli

K-Shell Ionization in 7.5- and 8.6-MeV/a.m.u. U + U Collisions at Very Small Impact Parameters

NUCLEAR REACTIONS 238U(238U, X), E=7.5, 8.6 MeV/nucleon; measured X-ray spectra; deduced K-vacancy production probability.

doi: 10.1007/BF01438230
Citations: PlumX Metrics

1985ST30      Nucl.Instrum.Methods Phys.Res. B10/11, 432 (1985)

Ch.Stoller

K X-Rays and Nuclear Reaction Times in the Deep Inelastic Reactions U + U and U + Pb at 7.5 MeV/amu

NUCLEAR REACTIONS 208Pb, 238U(238U, X), E=7.5 MeV/nucleon; measured K X-ray spectra; deduced heavy reaction product K-shell ionization probability.

doi: 10.1016/0168-583X(85)90284-8
Citations: PlumX Metrics

1984ST19      Phys.Rev.Lett. 53, 1329 (1984)

Ch.Stoller, M.Nessi, E.Morenzoni, W.Wolfli, W.E.Meyerhof, J.D.Molitoris, E.Grosse, Ch.Michel

Nuclear Reaction Times in the Deep-Inelastic U + U Collision deduced from K-Shell Ionization Proabilities

NUCLEAR REACTIONS U(U, X), E=7.5 MeV/nucleon; measured K-shell ionization probability.

doi: 10.1103/PhysRevLett.53.1329
Citations: PlumX Metrics

1983CH41      Phys.Lett. 130B, 246 (1983)

J.F.Chemin, S.Andriamonje, E.Morenzoni, Ch.Stoller, R.Anholt, W.E.Meyerhof, O.K.Baker, J.D.Molitoris

Compound Elastic Cross Sections in the Isobaric Analog Resonances 88Sr(p, p0) at 5.06 MeV and 86Sr(p, p0) at 6.02 MeV

NUCLEAR REACTIONS 88Sr(p, p), E=5-5.2 MeV; 86Sr(p, p), E=5.95-6.1 MeV; measured σ(θ), K-shell ionization probability vs E in IAR region. 89,87Y deduced IAR compound elastic contribution.

doi: 10.1016/0370-2693(83)91134-6
Citations: PlumX Metrics

1983ST02      Z.Phys. A310, 9 (1983)

C.Stoller, J.F.Chemin, R.Anholt, W.E.Meyerhof, W.Wolfli

X-Ray Study of the Deep Inelastic Reactions 1, 160-MeV 136Xe + Pb and 136Xe + 232Th

ATOMIC PHYSICS 232Th, Pb(136Xe, X), E=1160 MeV; measured E(X-ray), I(X-ray); deduced production mechanism.

doi: 10.1007/BF01433605
Citations: PlumX Metrics

1982CH24      Phys.Rev. A26, 1239 (1982)

J.-F.Chemin, W.E.Meyerhof, R.Anholt, J.D.Molitoris, Ch.Stoller

Measurement of the K-Shell Ionization Probability across a Wide Resonance: 88Sr(p, p0) at 6.06 MeV

NUCLEAR REACTIONS 88Sr(p, p), E=6.06 MeV; measured σ(θ), K-shell ionization probability vs E; deduced nuclear resonance role in ionization probability time delay. Blair-Anholt theory.

doi: 10.1103/PhysRevA.26.1239
Citations: PlumX Metrics

1981BU09      Z.Phys. A300, 105 (1981)

P.Burgy, G.Bonani, E.Morenzoni, M.Stockli, Ch.Stoller, M.Suter, W.Wolfli

Azimuthal Angle Dependence of Molecular Orbital K X-rays in Heavy Ion Collisions

NUCLEAR REACTIONS Al(19F, X), E=20 MeV; Cl(Cl, X), E=48 MeV; measured 19FX-ray-, ClX-ray-coin; deduced molecular X-ray anistropy vs impact parameter. NaCl target.

1981CH27      Phys.Rev. A24, 1218 (1981)

J.F.Chemin, R.Anholt, Ch.Stoller, W.E.Meyerhof, P.A.Amundsen

Measurement of 88Sr K-Shell Ionization Probability across the Nuclear Elastic-Scattering Resonance at 5060 keV

NUCLEAR REACTIONS 88Sr(p, p), E=4965-5212 keV; measured p(X-ray)-coin; deduced K-shell ionization probability. Enriched target.

doi: 10.1103/PhysRevA.24.1218
Citations: PlumX Metrics

1980ST23      Z.Phys. A297, 93 (1980)

Ch.Stoller, E.Morenzoni, W.Wolfli, W.E.Meyerhof, F.Folkmann, P.Vincent, P.H.Molker, P.Armbruster

MO X-Ray Angular Distribution from 1 GeV 208Pb+208Pb and 209Bi+209Bi Collisions

NUCLEAR REACTIONS 208Pb(208Pb, X), 209Bi(209Bi, X), E=4.2-4.8 MeV/nucleon; measured molecular orbital X-ray Doppler shift, anisotropy.

doi: 10.1007/BF01421464
Citations: PlumX Metrics

1979AN10      Z.Phys. A291, 287 (1979)

R.Anholt, W.E.Meyerhof, C.Stoller

Impact-Parameter Dependence of 1sσ Vacancy Production in 4.6-MeV/a.m.u. Xe + Pb Collisions

ATOMIC PHYSICS Pb(Xe, X), E=4.6 MeV/amu; measured X-ray(particle)-coin. Pb deduced probability of 1sσ vacancy.

doi: 10.1007/BF01409197
Citations: PlumX Metrics

1979MO23      Helv.Phys.Acta 52, 422 (1979)

E.Morenzoni, C.Stoller, W.Wolfli, W.E.Meyerhof, D.L.Clark, F.Folkmann, P.Vincent, P.H.Mokler, P.Armbruster

X-Rays from 1 GeV 208Pb + 208Pb and 209Bi + 209Bi Collisions

NUCLEAR REACTIONS 208Pb, 209Bi(208Pb, X), (209Bi, X), E=4.5-4.8 MeV/nucleon; measured continuum E(X), I(X-ray).

1977WO01      J.Phys.(London) G3, L33 (1977)

W.Wolfli, J.Lang, G.Bonani, M.Suter, C.Stoller, H.-U.Nissen

Evidence for Primordial Superheavy Elements (Question)

NUCLEAR STRUCTURE A > 200; calculated X-ray lines in monazites, cheralites; deduced no evidence for superheavy elements.

doi: 10.1088/0305-4616/3/2/004
Citations: PlumX Metrics

1976SU12      Helv.Phys.Acta 49, 863 (1976)

M.Suter, W.Wolfli, G.Bonani, C.Stoller, R.Muller

Proton-Proton bremsstrahlung bei 11 und 13 MeV

NUCLEAR REACTIONS 1H(p, p), E=11, 13 MeV; measured σ.

1975SU04      Phys.Lett. 58B, 36 (1975)

M.Suter, W.Wolfli, G.Bonani, C.Stoller, R.Muller

Proton-Proton Bremsstrahlung at 11 and 13 MeV

NUCLEAR REACTIONS 1H(p, p), E=11, 13 MeV; measured σ.

doi: 10.1016/0370-2693(75)90720-0
Citations: PlumX Metrics

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