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NSR database version of April 29, 2024.

Search: Author = K.Mohring

Found 13 matches.

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1993SC10      Z.Phys. A345, 29 (1993)

C.Schwarz, H.Fuchs, H.Homeyer, K.Mohring, T.Schmidt, A.Siwek, A.Sourell, W.Terlau, A.Budzanowski

Projectile Break-Up with Two Outgoing Intermediate-Mass Fragments in 26 AMeV ³²S + ¹⁹⁷Au

NUCLEAR REACTIONS ¹⁹⁷Au(³²S, X), E=840 MeV; measured intermediate mass (fragment)(fragment)(θ); deduced fragment pair production mechanism.

doi: 10.1007/BF01290336
Citations: PlumX Metrics

1992SC06      Phys.Lett. 279B, 223 (1992)

C.Schwarz, H.Fuchs, H.Homeyer, K.Mohring, T.Schmidt, A.Siwek, A.Sourell, W.Terlau, A.Budzanowski

Non-Thermal Projectile Breakup Due to Friction Forces

NUCLEAR REACTIONS ¹⁹⁷Au(³²S, X), E=26 MeV/nucleon; measured σ(θα, fragment θ); deduced projectile breakup mechanism.

doi: 10.1016/0370-2693(92)90383-F
Citations: PlumX Metrics

1992SU13      Nucl.Phys. A548, 353 (1992)

J.Suro, Y.D.Chan, J.A.Scarpaci, R.G.Stokstad, K.Mohring, T.C.Schmidt

Projectile Breakup of ¹⁶O at 32.5 MeV/A Comparison of a Classical Dynamical Model with Experiment

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁶O, 4α), E=32.5 MeV/nucleon; measured multiple breakup of projectile. Comparison with classical dynamical reaction model.

doi: 10.1016/0375-9474(92)90015-C
Citations: PlumX Metrics

1991MO18      Nucl.Phys. A533, 333 (1991)

K.Mohring, T.Srokowski, D.H.E.Gross

Modelling Dissipative Break-Up of Heavy Ions

NUCLEAR REACTIONS ¹⁹⁷Au(²⁰Ne, X), E=150-400 MeV; calculated σ(fragment θ) for X=⁹Be-¹⁹F, fusion σ(E); deduced reaction mechanism. Classical dynamical model.

doi: 10.1016/0375-9474(91)90494-Q
Citations: PlumX Metrics

1991SZ02      Z.Phys. A338, 187 (1991)

A.Szczurek, A.Budzanowski, L.Jarczyk, A.Magiera, K.Mohring, R.Siudak, T.Srokowski

Alpha Particles from the Reaction ¹²C + ¹²C at 28.7 MeV/Nucleon

NUCLEAR REACTIONS ¹²C(¹²C, α), E=28.7 MeV/nucleon; measured σ(θ), σ(θ, Eα); deduced α-production mechanism. Hauser-Feshbach model.

doi: 10.1007/BF01284793
Citations: PlumX Metrics

1988MO05      Phys.Lett. 203B, 210 (1988)

K.Mohring, T.Srokowski, D.H.E.Gross, H.Homeyer

A Dynamical Model for Projectile Break-Up and Incomplete Fusion

NUCLEAR REACTIONS ¹⁹⁷Au, ²⁰Ne(²⁰Ne, X), E ≈ 100-400 MeV; measured fusion σ(E), σ(θ(X), θα). Dynamical model. Projectile breakup.

doi: 10.1016/0370-2693(88)90540-0
Citations: PlumX Metrics

1985MO12      Nucl.Phys. A440, 89 (1985)

K.Mohring, W.J.Swiatecki, M.Zielinska-Pfabe

Simple Estimates for Fermi Jets

NUCLEAR REACTIONS ¹⁵⁸Gd(¹²C, xn), E=152 MeV; ⁹³Nb(¹⁶O, xn), E=204 MeV; calculated jetted neutron σ(En). Fermi jets, two colliding potential wells.

doi: 10.1016/0375-9474(85)90044-2
Citations: PlumX Metrics

1983KR16      Z.Phys. A314, 23 (1983)

H.J.Krappe, K.Mohring, M.C.Nemes, H.Rossner

On the Interpretation of Heavy-Ion Sub-Barrier Fusion Data

NUCLEAR REACTIONS, ICPND ¹⁰B(¹⁰B, X), E(cm) ≈ 2-4 MeV; ¹⁴N(¹⁰B, X), E(cm) ≈ 2.75-7 MeV; ¹²C(¹⁶O, X), E(cm)=4-12 MeV; ¹⁴N(¹⁶O, X), E(cm)=5.5-12 MeV; ²⁰Ne(¹²C, X), E(cm)=6-15 MeV; ⁹Be(¹⁶O, X), E(cm)=2.5-5 MeV; ¹²C(¹²C, X), E(cm)=2.5-5.5 MeV; ¹⁴N(¹²C, X), E(cm)=3.5-10 MeV; ¹⁴N(¹⁴N, X), E(cm)=4.5-11 MeV; ¹⁶O(¹⁶O, X), E(cm)=7-14.5 MeV; ¹¹⁰Pd(¹²C, X), E(cm)=30-50 MeV; ^64,58Ni(⁵⁸Ni, X), ⁶⁴Ni(⁶⁴Ni, X), E(cm)=90-110 MeV; ¹²²Sn(⁴⁰Ar, X), E=102.5-130 MeV; calculated fusion σ(E); deduced subbarrier fusion characteristics, neck formation role. Two-dimensional tunneling model.

doi: 10.1007/BF01411825
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1976FR04      Phys.Rev. C13, 430 (1976)

P.Frobrich, Q.K.K.Liu, K.Mohring

Comment on a Dynamically Exact Classical Description of Coulomb Excitation of Very Heavy Deformed Nuclei

NUCLEAR REACTIONS ²³⁸U, ²³²Th(⁸⁴Kr, ⁸⁴Kr'γ), ²³⁸U(¹³²Xe, ¹³²Xe'γ); analyzed Coulomb excitation. Classical theory.

doi: 10.1103/PhysRevC.13.430
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1975MO10      Nucl.Phys. A243, 365 (1975)

K.Mohring, R.Lipperheide, B.J.Cole

Neutron Transfer into Resonant States

NUCLEAR REACTIONS ¹⁵N, ³²S, ²⁴Mg(n, X), ¹⁵N, ³²S, ²⁴Mg(d, p), E=12 MeV; calculated σ.

doi: 10.1016/0375-9474(75)90284-5
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1973MO16      Nucl.Phys. A211, 136 (1973)

K.Mohring, R.Lipperheide

Application of Off-Shell R-Matrix Theory to the Description of Resonances Observed in ¹⁵N(d, p)¹⁶N(Unbound)

NUCLEAR REACTIONS ¹⁵N(d, p);E=12 MeV; calculated σ(Ep, θ). ¹⁶N analyzed resonances, L, R-matrix theory.

doi: 10.1016/0375-9474(73)90768-9
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1972FU16      Nucl.Phys. A196, 286 (1972)

H.Fuchs, H.Homeyer, H.Oeschler, R.Lipperheide, K.Mohring

Study of the Off-Energy-Shell n-¹⁵N Total Cross Section by Means of ¹⁵N(d, p) Stripping into the Continuum of ¹⁶N

NUCLEAR REACTIONS ¹⁵N(d, p), E=12.0 MeV; measured σ(Ep, θ). ¹⁶N deduced levels, J, π, S. Enriched target.

doi: 10.1016/0375-9474(72)90965-7
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1972LI13      Phys.Lett. 39B, 323 (1972)

R.Lipperheide, K.Mohring

The Reaction ¹⁵N(d, p)¹⁶N(Unbound) and the Off-Energy-Shell n-¹⁵N Total Cross Section

NUCLEAR REACTIONS ¹⁵N(d, p), E=12 MeV; measured σ(Ep) from ¹⁵N(n) total σ.

doi: 10.1016/0370-2693(72)90128-1
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