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NSR database version of May 8, 2024.

Search: Author = Y.Ronen

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2012RO16      Phys.Scr. 85, 065203 (2012)

Y.Ronen

On the light particles in ternary fission

NUCLEAR REACTIONS ²³³U, ^239,241Pu, ²⁴²Am, ²⁴⁹Cf(n, F), E not given; analyzed experimental data; deduced ternary fission yields trends. Comparison with available data.

doi: 10.1088/0031-8949/85/06/065203
Citations: PlumX Metrics

2009RO14      Nucl.Sci.Eng. 163, 91 (2009)

Y.Ronen

The Systemic Behavior of the Binding Energy of Heavy Isotopes

COMPILATION Z ≥ 65; analyzed binding energy for actinides; deduced correlations for 2Z-N=constant.

doi: 10.13182/NSE163-91
Citations: PlumX Metrics

2006RO02      Nucl.Technology 153, 224 (2006)

Y.Ronen, M.Aboudy, D.Regev

Breeding of ^242mAm in a fast reactor

doi: 10.13182/NT06-A3702
Citations: PlumX Metrics

2006RO05      Nucl.Sci.Eng. 152, 334 (2006)

Y.Ronen

A Rule for Determining Fissile Isotopes

NUCLEAR STRUCTURE Z=90-100; analyzed thermal fission σ, related features. ²⁴⁸Bk deduced fissility.

doi: 10.13182/NSE06-A2588
Citations: PlumX Metrics

2006RO23      Few-Body Systems 38, 97 (2006)

Y.Ronen, N.Barnea, W.Leidemann

An α-Particle Model for ¹⁶O: Is There a New Four-Body Scale?

NUCLEAR STRUCTURE ¹²C; calculated ground and excited states energies, radii. ¹²C, ¹⁶O, ²⁰Ne; calculated ground state energies. α-cluster model.

doi: 10.1007/s00601-005-0147-6
Citations: PlumX Metrics

2004RO01      Ann.Nucl.Energy 31, 323 (2004)

Y.Ronen

Indications of the validity of the liquid drop model for spontaneous fission half-lives

RADIOACTIVITY ^230,232Th, ²³¹Pa, ^{232,233,234,235,236,238}U, ²³⁷Np, ^{236,238,239,240,241,242,244}Pu, ^241,243Am, ^{240,242,243,244,245,246,248,250}Cm, ^{246,248,249,250,252,254,256}Cf, ^253,254,255Es, ^{246,248,250,252,254,255,256,257,258,259}Fm, ²⁵⁹Md, ^{250,252,256,258}No, ^{253,254,255,256,257,258,259,260,262}Rf, ^{255,256,257,261,262}Db, ^259,260,263Sg, ²⁶¹Bh(SF); analyzed spontaneous fission T_1/2 relative to liquid drop model predictions.

doi: 10.1016/S0306-4549(03)00221-4
Citations: PlumX Metrics

2002RO07      Ann.Nucl.Energy 29, 1013 (2002)

Y.Ronen

The Relation between Ternary Fission and Cluster Decay

NUCLEAR REACTIONS ²⁴¹Pu(n, F), E=thermal; analyzed light particle yields in ternary fission; deduced relation to cluster decay.

doi: 10.1016/S0306-4549(01)00090-1
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1998RO17      Ann.Nucl.Energy 25, 983 (1998)

Y.Ronen

Applying the 2Z-N Correlation to Predict the Fissility of ²⁴⁸Bk

NUCLEAR STRUCTURE ^230,232Pa, ²³⁶Np, ²⁴²Am, ²⁵⁴Es; analyzed thermal fission σ, decay T_1/2. ²⁴⁸Bk deduced thermal fission σ.

doi: 10.1016/S0306-4549(97)00096-0
Citations: PlumX Metrics

1998RO21      Phys.Rev. C58, 884 (1998)

Y.Ronen, S.Shlomo

Magnetic Dipole Moments of Odd-Odd N = Z Nuclei

NUCLEAR STRUCTURE ²H, ⁶Li, ¹⁰B, ¹⁴N, ¹⁸F, ²²Na, ²⁶Al, ³⁸K, ⁴⁶V; calculated ground, low-lying states μ. Core-deuteron cluster model. Comparison with data.

doi: 10.1103/PhysRevC.58.884
Citations: PlumX Metrics

1997RO12      Ann.Nucl.Energy 24, 1457 (1997)

Y.Ronen

Predictions of Some Spontaneous Fission Decay Modes

RADIOACTIVITY ²³²Th, ^{234,235,236,238}U, ^{236,238,239,240,242,244}Pu, ^241,241m,243Am, ^{240,242,243,244,245,246,248,250}Cm, ²⁴⁹Bk, ^{237,238,240,248,249,250,252,254,256}Cf, ^253,255,257Es, ^242,244Fm(SF); analyzed SF systematics. ²⁶¹Md, ²⁶²Sg deduced probability of SF decay mode.

doi: 10.1016/S0306-4549(97)00014-5
Citations: PlumX Metrics

1995RO19      Ann.Nucl.Energy 22, 559 (1995)

Y.Ronen

Prediction of the Average Number of Prompt Neutrons from Fissioning of Some Actinides

NUCLEAR STRUCTURE ²³⁵U, ^238,239Pu, ²⁴²Am, ^244,245Cm, ^250,251Cf, ²⁵⁴Es, ²⁵⁶Fm; analyzed fission data. ²²⁷Th, ²³⁰Pa, ²³⁶Np, ²⁴⁸Bk, ²⁵⁷Fm, ²³²U deduced average prompt neutron number following SF-decay .

doi: 10.1016/0306-4549(94)00090-2
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1995RO36      Nucl.Sci.Eng. 121, 483 (1995)

Y.Ronen

Correlations of the Independent Fission Product Yields of Different Isotopes

NUCLEAR REACTIONS ²³²Th, ^233,235,238U, ^239,240,241Pu(n, F)¹³⁷Cs/⁹⁶Y/¹⁴⁶Pr/¹²⁰Sn/¹²³Sn/¹⁴⁷Cs/¹⁴²Xe/⁹⁴Rb/¹¹⁷Sn/¹¹²Cd/¹⁰²Zr/¹¹¹Cd/^111mCd/¹¹¹Ag/³H/⁴He/⁸Li/¹³⁵Te/¹³⁵Sb/¹³⁵I/¹³⁵Xe/¹⁴⁹Ce/¹⁴⁹La/¹⁴⁹Pr/¹⁴⁹Nd/¹⁴⁹Sm/¹⁴⁹Pm/¹³⁷Cs, E=fast; analyzed independent fission product yields; deduced correlation to isotopes 2Z-N values.

doi: 10.13182/NSE95-A24149
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1992RO02      Phys.Rev. C45, R525 (1992)

Y.Ronen

Prediction of First Level Isomeric Half-Lives of Some Even-Even Actinides

NUCLEAR STRUCTURE ²²⁴Th, ²⁴⁰U, ^246,236Pu, ^252,242Cm, ^248,254,256Cf, ²²⁰Ra; calculated isomeric level T_1/2.

doi: 10.1103/PhysRevC.45.R525
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1991RO03      Phys.Rev. C44, R594 (1991)

Y.Ronen

Significance of the Light Clusters in Exotic Nuclear Decay

RADIOACTIVITY ^{222,223,224,226}Ra(¹⁴C), ²³⁰Th, ²³¹Pa, ^232,233,234U(²⁴Ne); ²³⁴U, ^236,238Pu(²⁸Mg), ²³⁸Pu(³²Si), (³⁴Si), ²³³U(²⁵Ne), ²³⁴U(²⁶Ne), ²³⁸Pu(³⁰Mg); analyzed decay data; deduced T_1/2, Q relationship, cluster decay features.

doi: 10.1103/PhysRevC.44.R594
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1990RO21      J.Phys.(London) G16, 1891 (1990)

Y.Ronen

Some 2Z-N Nuclear Correlations

NUCLEAR STRUCTURE A=230-259; analyzed SF decay T_1/2, other fission data; deduced (2Z-N) correlations rule, other nuclear properties.

doi: 10.1088/0954-3899/16/12/014
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1990RO23      J.Radioanal.Nucl.Chem. 142, 417 (1990)

Y.Ronen

Prediction and Correlations of Some Delayed Neutron Precursor Yields for Certain Actinide Nuclides

NUCLEAR REACTIONS ²³²Th, ^{233,234,235,236,238}U, ²³¹Pa, ^{241,242,240,239}Pu, ²³⁷Np(n, F), E=fast, thermal, 2.37 MeV; analyzed delayed neutron precursor yields following fission; deduced correlations. ²³⁶Np, ^242mAm, ^245,247Cm, ²⁵¹Cf deduced thermal neutron induced fission σ.

doi: 10.1007/BF02040311
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1989RO23      Ann.Nucl.Energy 16, 647 (1989)

Y.Ronen

Prediction of the Delayed Neutron Yields for Actinide Nuclides

NUCLEAR REACTIONS ^236,237Np, ^238,244Pu, ^241,242m,243Am, ^{244,245,246,247,248}Cm, ²⁴⁷Bk, ^249,250,251Cf(n, F), E=thermal, fast; calculated delayed neutron yields following fission.

doi: 10.1016/0306-4549(89)90141-2
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