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NSR database version of May 3, 2024.

Search: Author = R.Larsen

Found 14 matches.

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2019DI05      Nucl.Phys. A982, 715c (2019)

H.-T.Ding, O.Kaczmarek, A.-L.Kruse, R.Larsen, L.Mazur, S.Mukherjee, H.Ohno, H.Sandmeyer, H.-T.Shu

Charmonium and bottomonium spectral functions in the vector channel

doi: 10.1016/j.nuclphysa.2018.09.075
Citations: PlumX Metrics

2016LA13      Nucl.Phys. A950, 110 (2016)

R.Larsen, E.Shuryak

Classical interactions of the instanton-dyons with antidyons

doi: 10.1016/j.nuclphysa.2016.03.013
Citations: PlumX Metrics

2016LA23      Nucl.Phys. A956, 789 (2016)

R.Larsen, E.Shuryak

Recent progress in understanding gauge topology, confinement and chiral symmetry breaking

doi: 10.1016/j.nuclphysa.2016.01.067
Citations: PlumX Metrics

2001HE39      Appl.Radiat.Isot. 54, 839 (2001)

G.Henriksen, S.Messelt, E.Olsen, R.H.Larsen

Optimisation of cyclotron production parameters for the ²⁰⁹Bi(α, 2n) ²¹¹At reaction related to biomedical use of ²¹¹At

NUCLEAR REACTIONS ²⁰⁹Bi(α, 2n), (α, 3n), E=27.6-30.1 MeV; measured yields. comparison with previous results.

doi: 10.1016/S0969-8043(00)00346-8
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0167.

1996LA19      Appl.Radiat.Isot. 47, 135 (1996)

R.H.Larsen, B.W.Wieland, M.R.Zalutsky

Evaluation of an Internal Cyclotron Target for the Production of ²¹¹At via the ²⁰⁹BI(α, 2n)²¹¹At Reaction

NUCLEAR REACTIONS ²⁰⁹Bi(α, 2n), E=28 MeV; measured residual production efficiency. Metal Bi internal cyclotron targets.

doi: 10.1016/0969-8043(95)00285-5
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0494.

1974LA05      Nucl.Phys. A221, 26 (1974)

R.D.Larsen, W.R.Lutz, T.V.Ragland, R.P.Scharenberg

Determination of the Static Quadrupole Moment of the First 2⁺ States of ¹²²Te, ¹²⁴Te, and ¹³⁰Te by Heavy-Ion Coulomb Excitation

NUCLEAR REACTIONS ^122,124,130Te(³²S, ³²S'γ), E=57.5-65.0 MeV; measured σ(Eγ, θ(³²S)). ^122,124,130Te deduced quadrupole moment of the first 2+ states. Enriched targets.

doi: 10.1016/0375-9474(74)90096-7
Citations: PlumX Metrics

1974LA17      Nucl.Sci.Eng. 54, 263 (1974)

R.P.Larsen, N.D.Dudey, R.R.Heinrich, R.D.Oldham, R.J.Armani, R.J.Popek, R.Gold

The Yield of Short-Lived Gamma-Ray Emitting Nuclides from Fast- and Thermal-Neutron Fission

NUCLEAR REACTIONS ²³⁵U, ²³⁹Pu(n, F), E=thermal, fast; ²³⁸U(n, F), E=fast; measured Eγ, deduced yields for ^95,97Zr, ¹⁰³Ru, ¹³¹I, ¹⁴⁰Ba, ⁹⁹Mo.

doi: 10.13182/NSE74-A23417
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12771.

1973LU02      Phys.Rev. C8, 391 (1973)

W.R.Lutz, J.A.Thomson, R.F.Scharenberg, R.D.Larsen, R.G.Kerr

Determination of the Static Quadrupole Moment of the First 2⁺ State in ¹⁷⁰Er by Coulomb Excitation Using ⁸¹Br Projectiles

NUCLEAR REACTIONS ¹⁷⁰Er(⁸¹Br, ⁸¹Br'γ), E=55 MeV; measured σ(θ). ¹⁷⁰Er level deduced quadrupole moment.

doi: 10.1103/PhysRevC.8.391
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1973TH03      Phys.Rev. C7, 1413 (1973)

J.A.Thomson, R.P.Scharenberg, W.R.Lutz, R.D.Larsen

Static Quadrupole Moment of the Ground State of ⁵³Cr Determined by Coulomb Excitation

NUCLEAR REACTIONS ⁵³Cr(³²S, ³²S'), E=55, 59 MeV; measured σ(θ); ⁵³Cr deduced quadrupole moment.

doi: 10.1103/PhysRevC.7.1413
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1972LA17      Phys.Lett. 40B, 360 (1972)

R.D.Larsen, J.A.Thomson, R.G.Kerr, R.P.Scharenberg, W.R.Lutz

Multipole Coulomb Interference Effects on the Quadrupole Moment of ¹¹⁴Cd

NUCLEAR REACTIONS ¹¹⁴Cd(³²S, ³²S'γ), E=50 MeV; measured (³²S')(γ)-coin. ¹¹⁴Cd level deduced quadrupole moment. Coulomb excitation, reorientation expt.

doi: 10.1016/0370-2693(72)90820-9
Citations: PlumX Metrics

1972LA25      Nucl.Phys. A195, 119 (1972)

R.D.Larsen, J.A.Thomson, R.G.Kerr, R.P.Scharenberg, W.R.Lutz

The Sign of the Multiple Coulomb Excitation Interference Term and the Static Quadrupole Moment of the First 2⁺ State of ¹¹⁴Cd

NUCLEAR REACTIONS ¹¹⁴Cd(³²S, ³²S'γ), E=50 MeV; measured σ(Eγ, θ(³²S), θ((³²S)(γ))). ¹¹⁴Cd level deduced quadrupole moment. Enriched targets.

doi: 10.1016/0375-9474(72)90725-7
Citations: PlumX Metrics

1972LU08      Phys.Rev. C6, 1385 (1972)

W.R.Lutz, J.A.Thomson, R.P.Scharenberg, R.D.Larsen

Measurement of the Static Quadrupole Moment of the First 2⁺ State in ¹⁰⁸Pd by Heavy-Ion Coulomb Excitation and a Discussion of the Higher-State Interference

NUCLEAR REACTIONS ¹⁰⁸Pd(³²S, ³²S'γ), E not given; measured σ(E(³²S'), Eγ, θ(γ)). ¹⁰⁸Pd level deduced quadrupole moment. ^106,110Pd levels reevaluated quadrupole moment.

doi: 10.1103/PhysRevC.6.1385
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1971LA26      Trans.Amer.Nucl.Soc. 14, 370 (1971)

R.P.Larsen, R.R.Heinrich, N.D.Dudey, R.D.Oldham, R.J.Popek

²³⁵U and ²³⁹Pu Fast Fission Yields as a Function of Neutron Energy

NUCLEAR REACTIONS ²³⁵U, ²³⁹Pu(n, F)⁹⁵Zr/¹⁰³Ru/¹³¹I, E<2 MeV; measured reaction products, Eγ, Iγ; deduced fission yields relative to ¹⁴⁰Ba.

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12771.

1969PI16      J.Radioanal.Chem. 3, 233 (1969)

K.K.S.Pillay, R.J.Meyer, R.P.Larsen

Determination of the fast fission yield of ¹⁴¹Pr using neutron activation analysis

NUCLEAR REACTIONS ²³⁸U(n, F)¹⁴¹Pr, E ∼ 2 MeV; measured fission products, Eγ, Iγ; deduced yields.

doi: 10.1007/bf02513717
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13354.

Note: The following list of authors and aliases matches the search parameter R.Larsen: , R.D.LARSEN, R.H.LARSEN, R.P.LARSEN