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Search: Author = W.Loveland

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2022MO03      Nucl.Instrum.Methods Phys.Res. A1021, 165864 (2022)

M.Monterial, K.T.Schmitt, C.Prokop, E.Leal-Cidoncha, M.Anastasiou, N.S.Bowden, J.Bundgaard, R.J.Casperson, D.A.Cebra, T.Classen, D.H.Dongwi, N.Fotiades, J.Gearhart, V.Geppert-Kleinrath, U.Greife, C.Hagmann, M.Heffner, D.Hensle, D.Higgins, L.D.Isenhower, K.Kazkaz, A.Kemnitz, J.King, J.L.Klay, J.Latta, W.Loveland, J.A.Magee, B.Manning, M.P.Mendenhall, S.Mosby, D.Neudecker, S.Sangiorgio, B.Seilhan, L.Snyder, F.Tovesson, R.S.Towell, N.Walsh, T.S.Watson, L.Yao, W.Younes

Measurement of material isotopics and atom number ratio with α-particle spectroscopy for a NIFFTE fission Time Projection Chamber actinide target

NUCLEAR REACTIONS ²³⁵U, ²³⁹Pu(n, F), E not given; measured fission products, Eα, Iα; deduced isotopic concentrations and atomic number ratio.

doi: 10.1016/j.nima.2021.165864
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2022PI04      Phys.Rev. C 106, 044603 (2022)

A.Pica, A.T.Chemey, W.Loveland

Fast-neutron-induced fission of ²⁴⁰Pu and ²⁴²Pu

NUCLEAR REACTIONS ^240,242Pu(n, F), E=1-100 MeV; measured reaction products, fission fragments, time-of-flight, En, event-by-event analysis of fission fragment energy, (fragment)n-coin; deduced pre- and postneutron total kinetic energy, neutron multiplicity, mass yield distribution, width of the fission fragment mass distribution, ratio of the distance between charge centers at scission and that of spherical touching nuclei. Comparison to the predictions of the GEF model, the CGMF model, and the model of Denisov and Sedykh and to the previous experimental results. "White" spectrum neutrons from 15R beamline at the Los Alamos Neutron Science Center at the Weapons Neutron Research (LANSCE-WNR, LANL).

doi: 10.1103/PhysRevC.106.044603
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2020CH50      Eur.Phys.J. A 56, 297 (2020)

A.Chemey, A.Pica, L.Yao, W.Loveland, H.Y.Lee, S.A.Kuvin

Total kinetic energy and mass yields from the fast neutron-induced fission of ²³⁹Pu

NUCLEAR REACTIONS ²³⁹Pu(n, F), E=2.4-100 MeV; measured reaction products; deduced fission fragment mass distributions, mass yields, total kinetic energy (TKE) release in fission. Comparison with available data. The Los Alamos National Lab (LANL) WNR facility, on Flight Path 15R (FP15R).

doi: 10.1140/epja/s10050-020-00295-6
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14715.

2020DE09      Phys.Rev. C 101, 034612 (2020)

V.V.Desai, A.Pica, W.Loveland, J.S.Barrett, E.A.McCutchan, S.Zhu, A.D.Ayangeakaa, M.P.Carpenter, J.P.Greene, T.Lauritsen, R.V.F.Janssens, B.M.S.Amro, W.B.Walters

Multinucleon transfer in the interaction of 977 MeV and 1143 MeV ²⁰⁴Hg with ²⁰⁸Pb

NUCLEAR REACTIONS ²⁰⁸Pb(²⁰⁴Hg, X)⁷²Ga/^81mRb/⁸⁵Kr/⁹¹Sr/⁹²Sr/⁹⁷Zr/⁹⁰Nb/⁹⁹Mo/⁹³Tc/⁹⁹Tc/⁹⁷Ru/¹⁰³Ru/¹¹²Ag/¹¹⁵Cd/¹¹⁷Sb/¹³¹I/¹²⁵Xe/¹³⁵Xe/¹⁴⁰Ba/¹⁴³Ce/¹⁵⁶Sm/¹⁵⁴Tb/¹⁶⁷Ho/¹⁶⁹Lu/^180mHf/¹⁸¹Re/¹⁸²Re/¹⁸⁸Re/¹⁹¹Os/¹⁸⁸Ir/¹⁹⁰Ir/¹⁹⁵Pt/¹⁹²Au/¹⁹³Au/¹⁹⁴Au/¹⁹⁶Au/¹⁹⁸Au/¹⁹⁹Au/^200mAu/^195mHg/¹⁹⁷Hg/²⁰³Hg/¹⁹⁸Tl/¹⁹⁹Tl/²⁰⁰Tl/²⁰¹Tl/²⁰²Tl/²⁰⁰Pb/²⁰¹Pb/^202mPb/²⁰³Pb/²⁰⁴Pb/²⁰²Bi/²⁰³Bi/²⁰⁴Bi/²⁰⁵Bi/²⁰⁶Bi/²⁰⁶Po/²⁰⁸At/²⁰⁹At/²¹⁰At/²¹¹Rn, E=977 MeV; ²⁰⁸Pb(²⁰⁴Hg, X)⁶⁹Zn/⁷²Zn/⁸²Br/⁸⁶Y/⁸⁷Y/⁹¹Sr/⁹⁶Nb/⁹⁵Tc/⁹⁶Tc/⁹⁷Zr/⁹⁷Ru/⁹⁹Mo/¹⁰¹Rh/¹⁰³Ru/¹⁰⁵Ru/¹¹¹In/¹¹⁵Cd/¹¹⁷Sb/^120mSb/¹²²Sb/¹²⁸Sb/¹³²Cs/^135mBa/¹⁴⁰Ba/¹⁴³Ce/¹⁴⁷Gd/¹⁷²Er/¹⁶⁵Tm/¹⁶⁹Lu/¹⁷¹Lu/¹⁷⁰Hf/¹⁷³Hf/^180mHf/¹⁷⁶Ta/¹⁷⁷Ta/¹⁷⁸Ta/¹⁸³Ta/¹⁸¹Re/¹⁸²Re/¹⁸⁸Re/¹⁸⁹Re/¹⁸³Os/¹⁸⁵Os/¹⁸⁶Ir/¹⁸⁸Ir/¹⁹⁰Ir/¹⁸⁸Pt/¹⁹¹Pt/^197mPt/¹⁹³Au/¹⁹⁴Au/¹⁹⁶Au/¹⁹⁸Au/¹⁹⁹Au/^200mAu/^193mHg/^195mHg/¹⁹⁷Hg/²⁰³Hg/¹⁹⁷Tl/¹⁹⁹Tl/²⁰⁰Tl/²⁰¹Tl/²⁰²Tl/²⁰⁰Pb/²⁰¹Pb/^202mPb/²⁰³Pb/²⁰³Bi/²⁰⁴Bi/²⁰⁵Bi/²⁰⁶Bi/²⁰⁶Po/²⁰⁷Po/²⁰⁹At/²¹⁰At/²¹¹Rn, E=1143 MeV; measured Eγ, Iγ, fragment cumulative and independent σ for nuclei produced in multi-nucleon transfer (MNT) reactions using Gammasphere array for off-line γ counting at ANT-ATLAS facility. Comparison with theoretical predictions of GRAZING-F, dinuclear systems (DNS), and improved quantum molecular dynamics (ImQMD) models, and with previous experimental results from MNT reactions: ²⁴⁸Cm(¹⁶O, X), (⁸⁶Kr, X), (¹²⁹Xe, X), (¹³²Xe, X), (¹³⁶Xe, X), ¹⁹⁷Au(²³⁸U, X), ²³⁸U(¹⁸O, X), (²³⁸U, X), ²⁰⁸Pb(¹⁸O, X), (⁶⁴Ni, X), (¹³⁶Xe, X), ¹⁹⁸Pt(¹³⁶Xe, X). No evidence for production of nuclei near the N=126 shell.

doi: 10.1103/PhysRevC.101.034612
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2515.

2020DE18      Eur.Phys.J. A 56, 150 (2020)

V.V.Desai, W.Loveland, R.Yanez, G.Lane, S.Zhu, A.D.Ayangekaa, J.P.Greene, F.G.Kondev, R.V.F.Janssens, P.A.Copp

The ¹³⁶Xe + ¹⁹⁸Pt reaction: a detailed re-examination

doi: 10.1140/epja/s10050-020-00154-4
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2020PI16      Phys.Rev. C 102, 064612 (2020)

A.Pica, A.T.Chemey, L.Yao, W.Loveland, H.Y.Lee, S.A.Kuvin

Total kinetic energy release in the fast-neutron-induced fission of ²³⁷Np

NUCLEAR REACTIONS ²³⁷Np(n, F), E=2.6-100 MeV; measured fission fragments, time of flight of each interacting neutron using two arrays of nine Si PIN photodiodes at the LANSCE-WNR facility; deduced mass yield distributions, post- and pre-neutron emission total kinetic energy (TKEs), σ(E), product mass TKE distributions as function of neutron energy, dependence of asymmetric TKE events on neutron energy. Comparison with predictions of GEF (GEneral description of Fission observables) model.

doi: 10.1103/PhysRevC.102.064612
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14677.

2019DE15      Phys.Rev. C 99, 044604 (2019)

V.V.Desai, W.Loveland, K.McCaleb, R.Yanez, G.Lane, S.S.Hota, M.W.Reed, H.Watanabe, S.Zhu, K.Auranen, A.D.Ayangeakaa, M.P.Carpenter, J.P.Greene, F.G.Kondev, D.Seweryniak, R.V.F.Janssens, P.A.Copp

The ¹³⁶Xe + ¹⁹⁸Pt reaction: A test of models of multi-nucleon transfer reactions

NUCLEAR REACTIONS ¹⁹⁸Pt(¹³⁶Xe, X)⁴³K/^69mZn/⁷²Zn/⁷²As/⁷³Ga/⁹⁶Nb/⁹⁷Zr/⁹⁹Mo/^99mTc/¹⁰⁵Rh/¹¹⁰In/¹¹²Pd/^115mIn/^120mSb/¹²²Sb/¹²⁴I/¹²⁵Xe/¹²⁶Sb/¹²⁷Sb/¹²⁷Xe/¹²⁷Cs/¹²⁸Sb/¹³⁰I/¹³²I/^131mTe/¹³¹Ba/¹³²I/¹³²Cs/¹³³I/^133mXe/¹³⁵I/¹³⁵Xe/^135mBa/¹³⁶Cs/¹⁴⁰Ba/¹⁴⁰La/¹⁴²Pr/¹⁴³Ce/¹⁵³Sm/¹⁵⁴Tb/¹⁵⁷Dy/¹⁶⁹Lu/¹⁷³Hf/¹⁷⁵Hf/¹⁷⁶Ta/¹⁷⁷Ta/^180mHf/¹⁸¹Re/¹⁸²Re/¹⁸²Os/¹⁸³Os/¹⁸⁴Ta/¹⁸⁸Re/¹⁸⁸Ir/¹⁸⁹Re/¹⁹⁰Ir/¹⁹¹Pt/¹⁹³Au/¹⁹⁴Ir/¹⁹⁴Au/^195mIr/^195mPt/^195mHg/^196mIr/^196mAu/¹⁹⁷Hg/¹⁹⁸Au/¹⁹⁹Au/^200mAu/²⁰⁰Tl/²⁰⁰Pb/²⁰¹Tl/²⁰¹Pb/²⁰²Tl/^202mPb/²⁰³Hg/²⁰³Pb/²⁰⁴Bi, E=760.5 MeV; measured Eγ, Iγ, cumulative and independent yields and σ of projectile-like, fission and target-like fragments using Gammasphere array for online γ detection and an HPGe detector for offline γ spectroscopy at ATLAS-ANL facility. Comparison with predictions of GRAZING, di-nuclear systems (DNS), and improved quantum molecular dynamics (ImQMD) models for multi-nucleon transfer reactions, and with previous experimental results.

doi: 10.1103/PhysRevC.99.044604
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2398.

2018LO19      Eur.Phys.J. A 54, 140 (2018)

W.Loveland, A.M.Vinodkumar, R.Yanez, L.Yao, J.King, J.Lassen, A.Rojas

Sub-barrier fusion of ¹¹Li with ²⁰⁸Pb

NUCLEAR REACTIONS ²⁰⁸Pb(¹¹Li, x), E=26.1-32.7[sub-barrier]; measured reaction products isotopes; deduced complete, incomplete, total fusion σ, added published σ of the same group at different energies; calculated nuclidic σ using HIVAP statistical model code.

doi: 10.1140/epja/i2018-12572-8
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2567.

2018WA06      Phys.Rev. C 97, 021602 (2018)

A.Wakhle, K.Hammerton, Z.Kohley, D.J.Morrissey, K.Stiefel, J.Yurkon, J.Walshe, K.J.Cook, M.Dasgupta, D.J.Hinde, D.J.Jeung, E.Prasad, D.C.Rafferty, C.Simenel, E.C.Simpson, K.Vo-Phuoc, J.King, W.Loveland, R.Yanez

Capture cross sections for the synthesis of new heavy nuclei using radioactive beams

NUCLEAR REACTIONS ¹⁸¹Ta(³⁹K, X), E=180-210 MeV; ¹⁸¹Ta(⁴⁶K, X), E=190-215 MeV; measured time of flight and relative position of fission fragments, capture-fission σ(E) from a binary event using 14UD Heavy-ion accelerator facility of Australian National University (ANU), and Coupled Cyclotron Facility (CCF) projectile fragmentation facility at NSCL-MSU, and the Coincident Fission Fragment Detector (CFFD) at the ReA3 facility at NSCL; deduced velocity vectors of the coincident fragments, masses and angular distributions of fission fragments. Comparison with several phenomenological models and microscopic time-dependent Hartree-Fock calculations. Discussed implications for the synthesis of heavy nuclei at radioactive beam facilities. ¹⁹⁷Au(³¹Al, X), E(cm), ²⁴⁸Cm(²⁶Mg, X), E(cm)=110-160 MeV; ²⁴⁸Cm(⁴⁸Ca, X), E(cm)=195-230 MeV; ¹⁵⁴Sm(³¹Al, X), E(cm)=125-190 MeV; ²³⁸U(⁴⁸Ca, X), E(cm)=185-235 MeV; ²³⁸U(⁶⁴Ni, X), E(cm)=260-300 MeV; compiled theoretical and experimental values of capture fission σ(E). Comparison with several theoretical results.

doi: 10.1103/PhysRevC.97.021602
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2285.

2018YA03      Phys.Rev. C 97, 014608 (2018)

L.Yao, W.Loveland

Survival-mediated capture and fusion cross sections for heavy-element synthesis

NUCLEAR REACTIONS ²⁴⁹Cf(p, 3n)²⁵⁰Es*, E=23 MeV; ²³³U(³He, 5n)²³⁶Pu*, E=44.7 MeV; ²⁴⁹Cf(¹¹B, 3n)²⁶⁰Lr*, E=63 MeV; ²⁰⁴Pb(¹²C, 5n)²¹⁶Rn*, E=78 MeV; ²³²Th(¹²C, 4n)²⁴⁴Cm*, E=74 MeV; ²³²Th(¹²C, 5n)²⁴⁴Cm*, E=74 MeV; ²³³U(¹²C, 3n)²⁴⁵Cf*, E=67 MeV; ²³⁴U(¹²C, 4n)²⁴⁶Cf*, E=72 MeV; ²³⁵U(¹²C, 3n)²⁴⁷Cf*, E=67.5 MeV; ²³⁵U(¹²C, 4n)²⁴⁷Cf*, E=70.5 MeV; ²³⁵U(¹²C, 5n)²⁴⁷Cf*, E=77.5 MeV; ²³⁶U(¹²C, 3n)²⁴⁸Cf*, E=67.5 MeV; ²³⁶U(¹²C, 4n)²⁴⁸Cf*, E=70 MeV; ²³⁶U(¹²C, 5n)²⁴⁸Cf*, E=77.5 MeV; ²³⁸U(¹²C, 4n)²⁵⁰Cf*, E=67.5 MeV; ²³⁸U(¹²C, 5n)²⁵⁰Cf*, E=73.5 MeV; ²³⁷Np(¹²C, 4n)²⁴⁹Es*, E=67.6 MeV; ²³⁷Np(¹²C, 5n)²⁴⁹Es*, E=81 MeV; ²³⁹Pu(¹²C, 4n)²⁵¹Fm*, E=74 MeV; ²³⁹Pu(¹²C, 5n)²⁵¹Fm*, E=78 MeV; ²⁴¹Pu(¹³C, 4n)²⁵⁴Fm*, E=67.3 MeV; ²⁴⁰Pu(¹²C, 4n)²⁵²Fm*, E=71 MeV; ²⁴²Pu(¹²C, 4n)²⁵⁴Fm*, E=64 MeV; ²⁴¹Am(¹²C, 4n)²⁵³Md*, E=72 MeV; ²⁴¹Am(¹²C, 5n)²⁵³Md*, E=81 MeV; ²⁴³Am(¹²C, 4n)²⁵⁵Md*, E=71 MeV; ²⁴³Am(¹²C, 5n)²⁵⁵Md*, E=81 MeV; ²⁴³Am(¹³C, 3n)²⁵⁶Md*, E=70 MeV; ²⁴³Am(¹³C, 4n)²⁵⁶Md*, E=70 MeV; ²⁴³Am(¹³C, 5n)²⁵⁶Md*, E=81 MeV; ²⁴⁴Cm(¹²C, 4n)²⁵⁶No*, E=73.3 MeV; ²⁴⁴Cm(¹²C, 5n)²⁵⁶No*, E=83 MeV; ²⁴⁴Cm(¹³C, 3n)²⁵⁷No*, E=69.8 MeV; ²⁴⁴Cm(¹³C, 4n)²⁵⁷No*, E=72.8 MeV; ²⁴⁴Cm(¹³C, 5n)²⁵⁷No*, E=82 MeV; ²⁴⁶Cm(¹²C, 4n)²⁵⁸No*, E=72 MeV; ²⁴⁶Cm(¹²C, 5n)²⁵⁸No*, E=83 MeV; ²⁴⁶Cm(¹³C, 3n)²⁵⁹No*, E=67.5 MeV; ²⁴⁶Cm(¹³C, 4n)²⁵⁹No*, E=69.5 MeV; ²⁴⁶Cm(¹³C, 5n)²⁵⁹No*, E=78.5 MeV; ²⁴⁸Cm(¹²C, 3n)²⁶⁰No*, E=69.2 MeV; ²⁴⁸Cm(¹²C, 4n)²⁶⁰No*, E=71.2 MeV; ²⁴⁸Cm(¹²C, 5n)²⁶⁰No*, E=77.8 MeV; ²⁴⁸Cm(¹³C, 4n)²⁶¹No*, E=70.5 MeV; ²⁴⁸Cm(¹³C, 5n)²⁶¹No*, E=74.8 MeV; ²⁴⁹Cf(¹²C, 4n)²⁶¹Rf*, E=71 MeV; ²⁴⁹Cf(¹²C, 5n)²⁶¹Rf*, E=85 MeV; ²⁴⁹Cf(¹³C, 4n)²⁶²Rf*, E=72 MeV; ²³⁵U(¹⁵N, 4n)²⁵⁰Es*, E=78 MeV; ²³⁸U(¹⁴N, 5n)²⁵²Es*, E=83 MeV; ²⁰⁸Pb(¹⁶O, 4n)²²⁴Th*, E=91 MeV; ²⁰⁹Bi(¹⁸O, 3n)²²⁷Pa*, E=92.6 MeV; ²⁴¹Am(¹⁵N, 4n)²⁵⁶No*, E=82.9 MeV; ²⁴³Am(¹⁵N, 4n)²⁵⁸No*, E=83 MeV; ²⁴⁸Cm(¹⁵N, 3n)²⁶³Lr*, E=78 MeV; ²⁴⁸Cm(¹⁵N, 4n)²⁶³Lr*, E=81 MeV; ²⁴⁸Cm(¹⁵N, 5n)²⁶³Lr*, E=88 MeV; ⁵⁸Ni(⁵⁰Cr, 3n)¹⁰⁸Te*, E=214 MeV; ²⁴⁹Bk(¹⁵N, 4n)²⁶⁴Rf*, E=81.6 MeV; ²⁴⁹Cf(¹⁵N, 4n)²⁶⁴Db*, E=86 MeV; ²⁵⁰Cf(¹⁵N, 4n)²⁶⁵Rf*, E=84 MeV; ²³³U(¹⁶O, 4n)²⁴⁹Fm*, E=93 MeV; ²³³U(¹⁶O, 5n)²⁴⁹Fm*, E=97 MeV; ²³⁸U(¹⁶O, 4n)²⁵⁴Fm*, E=91 MeV; ²³⁸U(¹⁶O, 5n)²⁵⁴Fm*, E=91 MeV; ²³⁸U(¹⁸O, 3n)²⁵⁶Fm*, E=88 MeV; ²³⁸U(¹⁸O, 4n)²⁵⁶Fm*, E=88 MeV; ²³⁸U(¹⁸O, 5n)²⁵⁶Fm*, E=94 MeV; ²³⁹Pu(¹⁸O, 4n)²⁵⁷No*, E=91 MeV; ²³⁹Pu(¹⁸O, 4n)²⁵⁷Fm*, E=91 MeV; ²³⁹Pu(¹⁸O, 5n)²⁵⁷Fm*, E=96 MeV; ²⁴²Pu(¹⁶O, 4n)²⁵⁸Fm*, E=89 MeV; ²⁴⁵Cm(¹⁸O, 4n)²⁶³Rf*, E=93 MeV; ²⁴⁶Cm(¹⁶O, 4n)²⁶²Rf*, E=95 MeV; ²⁴⁸Cm(¹⁶O, 4n)²⁶⁴Rf*, E=92 MeV; ²⁴⁸Cm(¹⁸O, 4n)²⁶⁶Rf*, E=89 MeV; ²⁴⁸Cm(¹⁸O, 4n)²⁶⁶Rf*, E=94 MeV; ²⁴⁹Bk(¹⁶O, 4n)²⁶⁵Db*, E=92 MeV; ²⁴⁹Bk(¹⁶O, 5n)²⁶⁵Db*, E=92 MeV; ²⁴⁹Bk(¹⁸O, 4n)²⁶⁷Db*, E=91 MeV; ²⁴⁹Bk(¹⁸O, 5n)²⁶⁷Db*, E=91 MeV; ²⁴⁹Cf(¹⁸O, 4n)²⁶⁷Sg*, E=95 MeV; ²⁰⁵Tl(²²Ne, 3n)²²⁷Pa*, E=97 MeV; ²³⁸U(¹⁹F, 4n)²⁵⁷Md*, E=96 MeV; ²³⁸U(¹⁹F, 5n)²⁵⁷Md*, E=103 MeV; ²⁰⁹Bi(²²Ne, 4n)²³¹Np*, E=121 MeV; ²⁰⁹Bi(²²Ne, 5n)²³¹Np*, E=121 MeV; ²⁴⁸Cm(¹⁹F, 4n)²⁶⁷Db*, E=98 MeV; ²⁴⁸Cm(¹⁹F, 5n)²⁶⁷Db*, E=106 MeV; ²³²Th(²²Ne, 4n)²⁵⁴Fm*, E=106 MeV; ²³⁶U(²²Ne, 4n)²⁵⁸No*, E=112 MeV; ²³⁶U(²²Ne, 5n)²⁵⁸No*, E=124 MeV; ²³⁸U(²²Ne, 5n)²⁶⁰No*, E=117 MeV; ²⁴²Pu(²²Ne, 4n)²⁶⁴Rf*, E=114 MeV; ²⁴²Pu(²²Ne, 5n)²⁶⁴Rf*, E=114 MeV; ²⁴⁴Pu(²²Ne, 5n)²⁶⁶Rf*, E=114 MeV; ²⁴¹Am(²²Ne, 4n)²⁶³Db*, E=118 MeV; ²⁴¹Am(²²Ne, 5n)²⁶³Db*, E=118 MeV; ²⁴³Am(²²Ne, 4n)²⁶⁵Db*, E=116 MeV; ²⁴⁸Cm(²²Ne, 5n)²⁷⁰Sg*, E=117.8 MeV; ²⁴⁹Bk(²²Ne, 4n)²⁷¹Bh*, E=120 MeV; ²⁴⁹Bk(²²Ne, 5n)²⁷¹Bh*, E=120 MeV; ²⁰⁸Pb(²⁴Mg, 3n)²³²Pu*, E=132 MeV; ²⁰⁸Pb(²⁴Mg, 4n)²³²Pu*, E=132 MeV; ²⁰⁸Pb(²⁶Mg, 4n)²³⁴Pu*, E=135 MeV; ²⁴⁸Cm(²³Na, 5n)²⁷¹Bh*, E=132 MeV; ²³²Th(²⁶Mg, 4n)²⁵⁸No*, E=136 MeV; ²³²Th(²⁶Mg, 5n)²⁵⁸No*, E=136 MeV; ²³⁸U(²⁶Mg, 3n)²⁶⁴Rf*, E=121.8 MeV; ²³⁸U(²⁶Mg, 4n)²⁶⁴Rf*, E=128.1, 134 MeV; ²³⁸U(²⁶Mg, 5n)²⁶⁴Rf*, E=138.5, 140 MeV; ²⁴³Am(²⁶Mg, 4n)²⁶⁹Bh*, E=168 MeV; ²⁴³Am(²⁶Mg, 5n)²⁶⁹Bh*, E=168 MeV; ²⁴⁸Cm(²⁵Mg, 4n)²⁷³Hs*, E=140 MeV; ²⁴⁸Cm(²⁵Mg, 5n)²⁷³Hs*, E=140 MeV; ²⁴⁸Cm(²⁶Mg, 3n)²⁷⁴Hs*, E=145 MeV; ²⁴⁸Cm(²⁶Mg, 4n)²⁷⁴Hs*, E=145 MeV; ²⁴⁸Cm(²⁶Mg, 5n)²⁷⁴Hs*, E=145 MeV; ¹⁸²W(³²S, 3n)²¹⁴Th*, E=195 MeV; ¹⁸²W(³²S, 4n)²¹⁴Th*, E=195 MeV; ²³⁶U(²⁷Al, 5n)²⁶³Db*, E=154 MeV; ¹⁸¹Ta(³⁵Cl, 5n)²¹⁶Th*, E=190.5 MeV; ¹⁹⁸Pt(³⁴S, 4n)²³²Pu*, E=171 MeV; ²³⁸U(³⁰Si, 3n)²⁶⁸Sg*, E=151 MeV; ²³⁸U(³⁰Si, 4n)²⁶⁸Sg*, E=151 MeV; ²³⁸U(³⁰Si, 5n)²⁶⁸Sg*, E=161 MeV; ¹⁷⁶Hf(⁴⁰Ar, 3n)²¹⁶Th*, E=172.5 MeV; ¹⁷⁸Hf(⁴⁰Ar, 3n)²¹⁸Th*, E=167.6 MeV; ¹⁷⁸Hf(⁴⁰Ar, 4n)²¹⁸Th*, E=178.6 MeV; ¹⁸⁰Hf(⁴⁰Ar, 3n)²²⁰Th*, E=167 MeV; ¹⁸⁰Hf(⁴⁰Ar, 4n)²²⁰Th*, E=177 MeV; ¹⁸⁰Hf(⁴⁰Ar, 3n)²²⁰Th*, E=187.5 MeV; ²⁰⁷Pb(³⁴S, 3n)²⁴¹Cf*, E=172 MeV; ²⁰⁴Pb(³⁶S, 2n)²⁴⁰Cf*, E=163.6 MeV; ²⁰⁴Pb(³⁶S, 3n)²⁴⁰Cf*, E=172.6 MeV; ²⁰⁶Pb(³⁶S, 2n)²⁴²Cf*, E=163.6 MeV; ²⁰⁶Pb(³⁶S, 3n)²⁴²Cf*, E=162.6 MeV; ²⁰⁷Pb(³⁶S, 2n)²⁴³Cf*, E=165.5 MeV; ²⁰⁷Pb(³⁶S, 3n)²⁴³Cf*, E=170.3 MeV; ¹⁸¹Ta(⁴⁰Ar, 3n)²²¹Pa*, E=177 MeV; ¹⁸¹Ta(⁴⁰Ar, 4n)²²¹Pa*, E=179.4 MeV; ¹⁸²W(⁴⁰Ar, 3n)²²²U*, E=194 MeV; ¹⁸²W(⁴⁰Ar, 4n)²²²U*, E=194 MeV; ¹⁴⁴Sm(⁴⁶Ti, 3n)¹⁹⁰Po*, E=222 MeV; ¹⁷²Yb(⁴⁸Ca, 3n)²²⁰Th*, E=196.3 MeV; ¹⁷²Yb(⁴⁸Ca, 4n)²²⁰Th*, E=210.2 MeV; ¹⁷²Yb(⁴⁸Ca, 5n)²²⁰Th*, E=225.1 MeV; ¹⁷³Yb(⁴⁸Ca, 4n)²²¹Th*, E=210.2 MeV; ¹⁷³Yb(⁴⁸Ca, 5n)²²¹Th*, E=210.2 MeV; ¹⁷⁶Yb(⁴⁸Ca, 4n)²²⁴Th*, E=208.4 MeV; ²⁰⁹Bi(³⁷Cl, 2n)²⁴⁶Fm*, E=220 MeV; ¹⁴⁴Sm(⁵¹V, 3n)¹⁹⁵At*, E=230 MeV; ¹⁸⁰Hf(⁴⁸Ca, 3n)²²⁸U*, E=203.5 MeV; ¹⁴²Nd(⁵⁰Cr, 3n)¹⁹²Po*, E=231.4 MeV; ¹⁴²Nd(⁵⁰Cr, 4n)¹⁹²Po*, E=245 MeV; ¹⁴²Nd(⁵²Cr, 2n)¹⁹⁴Po*, E=221.8 MeV; ¹⁴²Nd(⁵²Cr, 3n)¹⁹⁴Po*, E=235.5 MeV; ¹⁴²Nd(⁵²Cr, 4n)¹⁹⁴Po*, E=250.5 MeV; ¹⁴²Nd(⁵²Cr, 5n)¹⁹⁴Po*, E=271 MeV; ²³⁸U(³⁴S, 4n)²⁷²Hs*, E=176 MeV; ²³⁸U(³⁴S, 5n)²⁷²Hs*, E=187.4 MeV; ²³⁸U(³⁶S, 3n)²⁷⁴Hs*, E=170 MeV; ²³⁸U(³⁶S, 4n)²⁷⁴Hs*, E=177 MeV; ²³⁸U(³⁶S, 5n)²⁷⁴Hs*, E=188 MeV; ²³⁸U(³⁴S, 5n)²⁷²Hs*, E=186 MeV; ²⁰⁶Pb(⁴⁰Ar, 4n)²⁴⁶Fm*, E=236 MeV; ²⁰⁷Pb(⁴⁰Ar, n)²⁴⁷Fm*, E=220 MeV; ²⁰⁸Pb(⁴⁰Ar, 2n)²⁴⁸Fm*, E=236 MeV; ²⁰⁸Pb(⁴⁰Ar, 3n)²⁴⁸Fm*, E=191 MeV; ¹⁸⁴W(⁴⁸Ca, 3n)²³²Pu*, E=201.6 MeV; ²⁰⁹Bi(⁴⁰Ar, 2n)²⁴⁹Md*, E=187 MeV; ²⁰⁹Bi(⁴⁰Ar, 3n)²⁴⁹Md*, E=198 MeV; ¹⁷⁰Er(⁵¹V, 3n)²²¹Pa*, E=220 MeV; ¹⁷⁰Er(⁵¹V, 4n)²²¹Pa*, E=234.7 MeV; ²⁰⁴Hg(⁴⁸Ca, 2n)²⁵²Fm*, E=207 MeV; ⁹⁰Zr(⁹⁰Zr, γ)¹⁸⁰Hg, E=362 MeV; ⁹⁰Zr(⁹⁰Zr, n)¹⁸⁰Hg*, E=362 MeV; ⁹⁰Zr(⁹⁰Zr, 2n)¹⁸⁰Hg*, E=362 MeV; ²⁰⁵Tl(⁴⁸Ca, 2n)²⁵³Md*, E=209 MeV; ²⁰⁸Pb(⁴⁸Ca, n)²⁵⁶No*, E=209 MeV; ²⁰⁸Pb(⁴⁸Ca, 2n)²⁵⁶No*, E=214 MeV; ²⁰⁸Pb(⁴⁸Ca, 3n)²⁵⁶No*, E=225 MeV; ²⁰⁸Pb(⁴⁸Ca, 4n)²⁵⁶No*, E=237 MeV; ²⁰⁶Pb(⁴⁸Ca, n)²⁵⁴No*, E=209 MeV; ²⁰⁶Pb(⁴⁸Ca, 2n)²⁵⁴No*, E=215 MeV; ²⁰⁶Pb(⁴⁸Ca, 3n)²⁵⁴No*, E=226 MeV; ²⁰⁶Pb(⁴⁸Ca, 4n)²⁵⁴No*, E=238 MeV; ²⁰⁴Pb(⁴⁸Ca, 2n)²⁵²No*, E=216.7 MeV; ²⁰⁴Pb(⁴⁸Ca, 2n)²⁵²No*, E=220 MeV; ²⁰⁴Pb(⁴⁸Ca, 3n)²⁵²No*, E=227 MeV; ²⁰⁸Pb(⁴⁴Ca, 2n)²⁵²No*, E=214 MeV; ²⁰⁸Pb(⁴⁴Ca, 3n)²⁵²No*, E=225 MeV; ²⁰⁷Pb(⁴⁸Ca, 2n)²⁵⁵No*, E=215 MeV; ¹⁰⁶Pd(⁸³Kr, 3n)¹⁸⁹Pb*, E=357 MeV; ²⁰⁹Bi(⁴⁸Ca, n)²⁵⁷Lr*, E=212.2 MeV; ²⁰⁹Bi(⁴⁸Ca, 2n)²⁵⁷Lr*, E=219.4 MeV; ²⁰⁹Bi(⁴⁸Ca, 3n)²⁵⁷Lr*, E=230.2 MeV; ²⁰⁹Bi(⁴⁸Ca, 4n)²⁵⁷Lr*, E=240 MeV; ¹⁹⁸Pt(⁵⁰Ti, 2n)²⁵⁷Lr*, E=219.5 MeV; ¹⁹⁸Pt(⁵⁰Ti, 3n)²⁵⁷Lr*, E=232 MeV; ⁹³Nb(⁹⁴Mo, 2n)¹⁸⁷Bi*, E=403 MeV; ⁹³Nb(⁹⁴Mo, 3n)¹⁸⁷Bi*, E=428.8 MeV; ⁹³Nb(⁹⁵Mo, n)¹⁸⁸Bi*, E=379.5 MeV; ⁹³Nb(⁹⁵Mo, 2n)¹⁸⁸Bi*, E=403.7 MeV; ⁹³Nb(⁹⁵Mo, 3n)¹⁸⁸Bi*, E=424 MeV; ¹¹⁴Cd(⁸³Kr, 3n)¹⁹⁷Po*, E=375 MeV; ¹⁵⁴Sm(⁶⁰Ni, 3n)²¹⁴Th*, E=278 MeV; ¹⁵⁴Sm(⁶⁰Ni, 4n)²¹⁴Th*, E=278 MeV; ²²⁶Ra(⁴⁸Ca, 3n)²⁷⁴Hs*, E=229 MeV; ²²⁶Ra(⁴⁸Ca, 4n)²⁷⁴Hs*, E=234 MeV; ²²⁶Ra(⁴⁸Ca, 5n)²⁷⁴Hs*, E=241 MeV; ⁹⁴Mo(¹⁰⁰Mo, n)¹⁹⁴Po*, E=385 MeV; ⁹⁴Mo(¹⁰⁰Mo, 2n)¹⁹⁴Po*, E=403.7 MeV; ⁹⁴Mo(¹⁰⁰Mo, 3n)¹⁹⁴Po*, E=424.3 MeV; ¹⁰⁰Mo(¹⁰⁰Mo, n)²⁰⁰Po*, E=372 MeV; ¹⁰⁰Mo(¹⁰⁰Mo, 2n)²⁰⁰Po*, E=384 MeV; ¹⁰⁰Mo(¹⁰⁰Mo, 3n)²⁰⁰Po*, E=400 MeV; ¹⁰⁰Mo(¹⁰⁰Mo, 4n)²⁰⁰Po*, E=420 MeV; ¹⁰⁰Mo(¹⁰⁰Mo, 5n)²⁰⁰Po*, E=436 MeV; ²³²Th(⁴⁸Ca, 3n)²⁸⁰Ds*, E=260 MeV; ²⁰⁸Pb(⁴⁸Ti, n)²⁵⁶Rf*, E=223.3 MeV; ²⁰⁸Pb(⁴⁸Ti, 2n)²⁵⁶Rf*, E=232 MeV; ²⁰⁸Pb(⁴⁹Ti, 2n)²⁵⁷Rf*, E=271 MeV; ²⁰⁸Pb(⁵⁰Ti, n)²⁵⁸Rf*, E=229 MeV; ²⁰⁸Pb(⁵⁰Ti, n)²⁵⁸Rf*, E=230.5 MeV; ²⁰⁸Pb(⁵⁰Ti, 2n)²⁵⁸Rf*, E=239, 243 MeV; ²⁰⁸Pb(⁵⁰Ti, 3n)²⁵⁸Rf*, E=247.6 MeV; ²⁰⁷Pb(⁵⁰Ti, n)²⁵⁷Rf*, E=242.5 MeV; ²⁰⁷Pb(⁵⁰Ti, 2n)²⁵⁷Rf*, E=242.5 MeV; ²⁰⁶Pb(⁵⁰Ti, n)²⁵⁶Rf*, E=237.3 MeV; ²⁰⁶Pb(⁵⁰Ti, 2n)²⁵⁶Rf*, E=237.3 MeV; ²⁰⁹Bi(⁵⁰Ti, n)²⁵⁹Db*, E=232.6 MeV; ²⁰⁹Bi(⁵⁰Ti, 2n)²⁵⁹Db*, E=240.7 MeV; ²⁰⁹Bi(⁵⁰Ti, 3n)²⁵⁹Db*, E=254 MeV; ¹²¹Sb(⁸⁶Kr, 2n)²⁰⁷Fr*, E=343.6 MeV; ¹²¹Sb(⁸⁶Kr, 3n)²⁰⁷Fr*, E=361.1 MeV; ¹²¹Sb(⁸⁶Kr, 4n)²⁰⁷Fr*, E=388.7 MeV; ¹²³Sb(⁸⁶Kr, 4n)²⁰⁹Fr*, E=379.1 MeV; ¹²³Sb(⁸⁶Kr, 5n)²⁰⁹Fr*, E=388.7 MeV; ²⁰⁸Pb(⁵¹V, n)²⁵⁹Db*, E=239.7 MeV; ²⁰⁸Pb(⁵¹V, 2n)²⁵⁹Db*, E=247.2 MeV; ²⁰⁹Bi(⁵¹V, 2n)²⁶⁰Sg*, E=250.4 MeV; ²⁰⁸Pb(⁵²Cr, n)²⁶⁰Sg*, E=254 MeV; ²⁰⁸Pb(⁵²Cr, 2n)²⁶⁰Sg*, E=262 MeV; ²⁰⁷Pb(⁵⁴Cr, n)²⁶¹Sg*, E=262 MeV; ²⁰⁷Pb(⁵⁴Cr, 2n)²⁶¹Sg*, E=262 MeV; ²⁰⁸Pb(⁵⁴Cr, n)²⁶²Sg*, E=257.1 MeV; ²⁰⁸Pb(⁵⁴Cr, 2n)²⁶²Sg*, E=268.5 MeV; ²⁰⁸Pb(⁵⁴Cr, 3n)²⁶²Sg*, E=297 MeV; ²⁰⁹Bi(⁵²Cr, n)²⁶¹Bh*, E=252.8 MeV; ²⁰⁹Bi(⁵⁴Cr, n)²⁶³Bh*, E=257.1 MeV; ²⁰⁹Bi(⁵⁴Cr, 2n)²⁶³Bh*, E=260.9 MeV; ⁹⁰Zr(¹²⁴Sn, n)²¹⁴Th*, E=503.4 MeV; ⁹²Zr(¹²⁴Sn, n)²¹⁶Th*, E=492.3 MeV; ⁹⁴Zr(¹²⁴Sn, n)²¹⁸Th*, E=493.5 MeV; ⁹⁴Zr(¹²⁴Sn, 2n)²¹⁸Th*, E=506.4 MeV; ⁹⁴Zr(¹²⁴Sn, 3n)²¹⁸Th*, E=518.8 MeV; ⁹⁴Zr(¹²⁴Sn, 4n)²¹⁸Th*, E=545 MeV; ⁹⁶Zr(¹²⁴Sn, n)²²⁰Th*, E=494.6 MeV; ⁹⁶Zr(¹²⁴Sn, 2n)²²⁰Th*, E=494.6 MeV; ⁹⁶Zr(¹²⁴Sn, 3n)²²⁰Th*, E=519.2 MeV; ⁹⁶Zr(¹²⁴Sn, 4n)²²⁰Th*, E=531.7 MeV; ⁹⁶Zr(¹²⁴Sn, 5n)²²⁰Th*, E=567.7 MeV; ²⁰⁸Pb(⁵⁵Mn, n)²⁶³Bh*, E=265.5 MeV; ²⁰⁸Pb(⁵⁵Mn, 2n)²⁶³Bh*, E=273 MeV; ²⁰⁹Bi(⁵⁵Mn, n)²⁶⁴Hs*, E=302.5 MeV; ²⁰⁸Pb(⁵⁶Fe, n)²⁶⁴Hs*, E=275 MeV; ²⁰⁸Pb(⁵⁸Fe, n)²⁶⁶Hs*, E=283.9 MeV; ²⁰⁸Pb(⁵⁸Fe, 2n)²⁶⁶Hs*, E=291.2, 294.1 MeV; ²⁰⁷Pb(⁵⁸Fe, n)²⁶⁵Hs*, E=285 MeV; ²⁰⁶Pb(⁵⁸Fe, n)²⁶⁴Hs*, E=287.7 MeV; ²⁰⁹Bi(⁵⁸Fe, n)²⁶⁷Mt*, E=287.6 MeV; ¹⁷⁰Er(⁷⁶Ge, 2n)²⁴⁶Fm*, E=357.5 MeV; ²⁰⁸Pb(⁵⁹Co, n)²⁶⁷Mt*, E=291.5 MeV; ²⁰⁹Bi(⁵⁹Co, n)²⁶⁸Ds*, E=300.9 MeV; ²⁰⁸Pb(⁶²Ni, n)²⁷⁰Ds*, E=311 MeV; ²⁰⁸Pb(⁶⁴Ni, n)²⁷²Ds*, E=314 MeV; ²⁰⁷Pb(⁶⁴Fe, n)²⁷¹Ds*, E=317 MeV; ¹⁶⁰Gd(⁸⁶Kr, 2n)²⁴⁶Fm*, E=380.5 MeV; ¹¹⁰Pd(¹³⁶Xe, 2n)²⁴⁶Fm*, E=633.5 MeV; calculated capture cross section and evaporation residue formation cross section as function of spin, fusion probability P_CN, survival probability, mean spins for the capture process and for the calculated evaporation residues (EVR); compiled experimental cross sections for evaporation residues. Comparison with available experimental data. List of reactions, experimental σ(EVR) and theoretical results in a table in Supplementary Material (ref. 17 in 2018Ya03). Relevance to heavy element formation.

doi: 10.1103/PhysRevC.97.014608
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2018YA05      Nucl.Phys. A970, 65 (2018)

R.Yanez, J.King, J.S.Barrett, W.Loveland, N.Fotiades, H.Y.Lee

Total kinetic energy release in the fast neutron induced fission of ²³⁵U

NUCLEAR REACTIONS ²³⁵U(n, F), E=2-100 MeV; measured En, In, fission products; deduced (post neutron emission) TKE. Fusion σ calculated within semi-empirical GEF model.

doi: 10.1016/j.nuclphysa.2017.11.007
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14513.

2017AM01      Phys.Rev. C 95, 014330 (2017)

B.M.S.Amro, C.J.Lister, E.A.McCutchan, W.Loveland, P.Chowdhury, S.Zhu, A.D.Ayangeakaa, J.S.Barrett, M.P.Carpenter, C.J.Chiara, J.P.Greene, J.L.Harker, R.V.F.Janssens, T.Lauritsen, A.A.Sonzogni, W.B.Walters, R.Yanez

γ-ray spectroscopy of ²⁰⁹Tl

NUCLEAR REACTIONS ²⁰⁸Pb(¹³⁶Xe, X)²⁰⁹Tl, E=785 MeV; measured Eγ, Iγ, γΓ-coin, delayed γ, half-lives of isomers using Gammasphere array at ATLAS-ANL facility. ²⁰⁹Tl; deduced levels, J, π, internal conversion coefficients, multipolarities, B(E2), configurations.

doi: 10.1103/PhysRevC.95.014330
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Data from this article have been entered in the XUNDL database. For more information, click here.

2017KI14      Eur.Phys.J. A 53, 238 (2017)

J.King, R.Yanez, W.Loveland, J.S.Barrett, B.Oscar, N.Fotiades, F.Tovesson, H.Y.Lee

The total kinetic energy release in the fast neutron-induced fission of ²³²Th

NUCLEAR REACTIONS ²³²Th(n, F), E=3-91 MeV; measured post-emission TKE release; calculated compound nucleus E^* vs En, neutron multiplicity; deduced fragment mass distribution, average excitation energy of the fissioning system vs En, neutron multiplicity. Compared to ²³²Th(p, F) published data.

doi: 10.1140/epja/i2017-12436-9
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14517.

2017WE06      Phys.Lett. B 771, 119 (2017)

T.Welsh, W.Loveland, R.Yanez, J.S.Barrett, E.A.McCutchan, A.A.Sonzogni, T.Johnson, S.Zhu, J.P.Greene, A.D.Ayangeakaa, M.P.Carpenter, T.Lauritsen, J.L.Harker, W.B.Walters, B.M.S.Amro, P.Copp

Modeling multi-nucleon transfer in symmetric collisions of massive nuclei

NUCLEAR REACTIONS ¹⁹⁸Pt(²⁰⁴Hg, X), E=1360 MeV; measured reaction products, Eγ, Iγ; deduced fragment yields, σ. Comparison with GRAZING and DNS models.

doi: 10.1016/j.physletb.2017.05.044
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2016VO13      Phys.Rev. C 94, 064611 (2016)

N.Vonta, G.A.Souliotis, W.Loveland, Y.K.Kwon, K.Tshoo, S.C.Jeong, M.Veselsky, A.Bonasera, A.Botvina

Neutron-rich rare-isotope production from projectile fission of heavy nuclei near 20 MeV/nucleon beam energy

NUCLEAR REACTIONS ²⁰⁸Pb(²³⁸U, F), E=20 MeV/nucleon; ¹⁹⁷Au(¹⁹⁷Au, F), E=20 MeV/nucleon; analyzed experimental data obtained at NSCL-MSU using A1200 fragment separator; calculated isobaric yield distributions or cross sections, average Z/A versus A, mass distributions of projectile fission fragments, production cross sections and rates of accessible neutron-rich nuclides of Z=26-71 and N=26-116. Phenomenological deep-inelastic transfer model (DIT), and microscopic constrained molecular dynamics model (CoMD), with the statistical multifragmentation model (SMM) for the de-excitation or fission of the hot heavy projectile fragments. Comparison with experimental data. Relevance to r-process path and neutron dripline.

doi: 10.1103/PhysRevC.94.064611
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2015BA20      Phys.Rev. C 91, 064615 (2015)

J.S.Barrett, W.Loveland, R.Yanez, S.Zhu, A.D.Ayangeakaa, M.P.Carpenter, J.P.Greene, R.V.F.Janssens, T.Lauritsen, E.A.McCutchan, A.A.Sonzogni, C.J.Chiara, J.L.Harker, W.B.Walters

¹³⁶Xe+²⁰⁸Pb reaction: A test of models of multinucleon transfer reactions

NUCLEAR REACTIONS ²⁰⁸Pb(¹³⁶Xe, X), E=85 MeV; measured Eγ, Iγ, γγ-coin using Gammasphere at ATLAS-ANL facility, σ for projectile-like fragments (PLFs) and target-like fragments (TLFs) by off-line γ-ray spectroscopy for radioactive decay measurements (RD), prompt γ decays recorded during the beam burst (IB), and delayed γ decays recorded between the beam bursts (OB). ^116,118Cd, ^119,121In, ^{118,120,122,123,124,126}Sn, ^{119,121,123,125,126,127,128,130}Sb, ^{124,126,128,130,131,132,134}Te, ^{127,128,129,130,131,132,133,135,136}I, ^128,130,132Xe, ^{133,134,135,136,137,138}Xe, ^{131,132,133,134,136,137,139,141}Cs, ¹³⁰Ba, ^{132,134,136,138,139,140,141,142,143}Ba, ^{132,135,136,137,139,140,143}La, ^{136,138,139,140,141,142,143,144,145,146}Ce, ^139,141,142Pr, ^{140,142,143,144,145,146,147,148,149}Nd, ^{142,143,145,147,149}Pm, ^{145,146,147,148,149,150,151,152,154}Sm, ^147,149,151Eu, ^152,154,156Gd, ^{156,158,160,162,164}Dy, ^160,161Er, ¹⁷⁶Yb, ^{176,178,180,181,182}Hf, ^179,181Ta, ^{176,180,182,184,186,187}W, ^179,185,187Re, ^{186,188,190,191,192,194,197}Os, ^188,190,192Ir, ^{190,191,192,194,196,197,198,200,201,202}Pt, ^{191,192,193,194,196,198,199}Au, ^{194,196,198,200,202,203,204,205,206,208}Hg, ^{196,197,198,199,201,202,203,204,205,206,207}Tl, ^{198,201,202,203,204,206,207,208,209,210,211}Pb, ^{199,201,202,203,204,205,206,207,209,211}Bi, ^{202,204,205,206,207,208,209,210,212,213,214}Po, ^{207,208,209,210,211,213}At, ^{210,211,212,213,214,215,216,218}Rn, ^{211,212,213,215,216}Fr, ²¹⁴Ra; deduced projectile-like fragment cumulative and independent production yields. Comparison with predictions of GRAZING model, and those of Zagrebaev and Greiner model using a quantitative metric. Discussed correlations between TLF and PLF yields.

doi: 10.1103/PhysRevC.91.064615
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2015GA24      Phys.Rev. C 92, 021301 (2015)

J.M.Gates, K.E.Gregorich, O.R.Gothe, E.C.Uribe, G.K.Pang, D.L.Bleuel, M.Block, R.M.Clark, C.M.Campbell, H.L.Crawford, M.Cromaz, A.Di Nitto, Ch.E.Dullmann, N.E.Esker, C.Fahlander, P.Fallon, R.M.Farjadi, U.Forsberg, J.Khuyagbaatar, W.Loveland, A.O.Macchiavelli, E.M.May, P.R.Mudder, D.T.Olive, A.C.Rice, J.Rissanen, D.Rudolph, L.G.Sarmiento, J.A.Shusterman, M.A.Stoyer, A.Wiens, A.Yakushev, H.Nitsche

Decay spectroscopy of element 115 daughters: ²⁸⁰Rg → ²⁷⁶Mt and ²⁷⁶Mt → ²⁷²Bh

NUCLEAR REACTIONS ²⁴³Am(⁴⁸Ca, 3n)²⁸⁸Mc, E=262 MeV; measured evaporation residues (EVRs) by magnetic rigidities, Eα, SF-like events, decay chains using corner-cube-clover (C3) focal plane detector consisting of silicon-strip detectors surrounded by HPGe clover-type detectors, and DSSSDs for α particles at LBNL cyclotron facility; deduced data for forty-six decay chains from the decay of ²⁸⁸Mc and its α daughter products ²⁸⁴Nh, ²⁸⁰Rg, ²⁷⁶Mt, ²⁷²Bh, ²⁶⁸Db, the ²⁶⁸Db decaying by SF events.

RADIOACTIVITY ²⁷⁶Mt, ²⁸⁰Rg(α)[from α decay chain of ²⁸⁸Mc formed in ²⁴³Am(⁴⁸Ca, 3n), E=262 MeV at LBNL cyclotron facility]; measured Eα, Iα, Eγ, Iγ, E(x rays), αγ-, α(x ray)-, γγ-coin, half-lives of ²⁷⁶Mt and ²⁸⁰Rg isotopes. ²⁷²Bh, ²⁷⁶Mt; deduced levels, multipolarities, α hindrance factors. GEANT4 simulations of α and photon spectra. No K-x rays were definitely assigned thus uncertain Z identification.

doi: 10.1103/PhysRevC.92.021301
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2015KR09      Nucl.Phys. A944, 117 (2015)

J.V.Kratz, W.Loveland, K.J.Moody

Syntheses of transuranium isotopes with atomic numbers Z ≤ 103 in multi-nucleon transfer reactions

doi: 10.1016/j.nuclphysa.2015.06.004
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2015LO10      Eur.Phys.J. A 51, 120 (2015)

W.Loveland

An experimentalist's view of the uncertainties in understanding heavy element synthesis

doi: 10.1140/epja/i2015-15120-2
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2015YA08      Phys.Rev. C 91, 044608 (2015)

R.Yanez, W.Loveland

Predicting the production of neutron-rich heavy nuclei in multinucleon transfer reactions using a semi-classical model including evaporation and fission competition, GRAZING-F

NUCLEAR REACTIONS ²⁰⁸Pb(¹³⁶Xe, X), E(cm)=423.0, 450.0, 526.0, 617.0 MeV; ¹⁹⁸Pt(¹³⁶Xe, X), E(cm)=604.9 MeV; ²⁴⁸Cm(⁸⁶Kr, X), E=323.0, 339.3, 385.1, 494.0 MeV; ²⁴⁸Cm(⁹⁴Kr, X), E(cm)=490.0 MeV; ²⁴⁴Pu(¹³⁶Xe, X), E(cm)=528.8 MeV; ²⁴⁸Cm(¹²⁹Xe, X), E(cm)=511.6 MeV; ²⁴⁸Cm(¹³²Xe, X), E(cm)=508.9, 523.8 MeV; ²⁴⁸Cm(¹³⁶Xe, X), E(cm)=496.6, 505.6 MeV; ²⁴⁸Cm(¹⁴⁴Xe, X), E(cm)=504.7 MeV; ²⁴⁹Cf(¹³⁶Xe, X), E(cm)=483.1, 524.3, 565.4 MeV; ²³⁸U(²³⁸U, X), E(cm)=769.8, 811.0, 899.9, 1024.8 MeV; ²⁴⁸Cm(²³⁸U, X), E(cm)=894.6 MeV; ²⁴⁹Bk(²³⁸U, X), E(cm)=809.0, 1117.0 MeV; calculated Coulomb and interaction barriers, cross sections of surviving nuclei; deduced predicted production σ for neutron-rich heavy nuclei ²⁰¹Re, ²⁰²Os, ²⁰³Ir, ²⁰⁴Pt, ^{243,244,245,246,247,248,249,250}U, ^{248,249,250,251,252,253,254}Pu, ^245,246,247Np, ²⁶¹Md, ²⁶¹No, ²⁶³Lr. Semiclassical model GRAZING coupled to an evaporation and fission competition model using computer code GRAZING with fission competition (GRAZING-F) for production rates of neutron-rich N=126 nuclei, actinides, and transactinides. Comparison with available experimental data.

doi: 10.1103/PhysRevC.91.044608
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2014LO09      Nucl.Data Sheets 119, 383 (2014)

W.Loveland, L.Yao, D.M.Asner, R.G.Baker, J.Bundgaard, E.Burgett, M.Cunningham, J.Deaven, D.L.Duke, U.Greife, S.Grimes, M.Heffner, T.Hill, D.Isenhower, J.L.Klay, V.Kleinrath, N.Kornilov, A.B.Laptev, T.N.Massey, R.Meharchand, H.Qu, J.Ruz, S.Sangiorgio, B.Selhan, L.Snyder, S.Stave, G.Tatishvili, R.T.Thornton, F.Tovesson, D.Towell, R.S.Towell, S.Watson, B.Wendt, L.Wood

Targets for Precision Measurements

doi: 10.1016/j.nds.2014.08.106
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2014ME09      Nucl.Data Sheets 119, 373 (2014)

R.Meharchand, D.M.Asner, R.G.Baker, J.Bundgaard, E.Burgett, M.Cunningham, J.Deaven, D.L.Duke, U.Greife, S.Grimes, M.Heffner, T.Hill, D.Isenhower, J.L.Klay, V.Kleinrath, N.Kornilov, A.B.Laptev, W.Loveland, T.N.Massey, H.Qu, J.Ruz, S.Sangiorgio, B.Seilhan, L.Snyder, S.Stave, G.Tatishvili, R.T.Thornton, F.Tovesson, D.Towell, R.S.Towell, S.Watson, B.Wendt, L.Wood

Commissioning the NIFFTE Time Projection Chamber: Towards the ²³⁸U/²³⁵U(n, f) Cross-section Ratio

doi: 10.1016/j.nds.2014.08.103
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2014SN02      Nucl.Data Sheets 119, 386 (2014)

L.Snyder, D.M.Asner, R.G.Baker, J.Bundgaard, E.Burgett, M.Cunningham, J.Deaven, D.L.Duke, U.Greife, S.Grimes, M.Heffner, T.Hill, D.Isenhower, J.L.Klay, V.Kleinrath, N.Kornilov, A.B.Laptev, W.Loveland, T.N.Massey, R.Meharchand, H.Qu, J.Ruz, S.Sangiorgio, B.Seilhan, S.Stave, G.Tatishvili, R.T.Thornton, F.Tovesson, D.Towell, R.S.Towell, S.Watson, B.Wendt, L.Wood, for the NIFFTE Collaboration

Measuring the α/SF Branching Ratio of ²⁵²Cf with the NIFFTE TPC

doi: 10.1016/j.nds.2014.08.107
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2014ST15      Nucl.Data Sheets 119, 380 (2014)

S.Stave, D.M.Asner, R.G.Baker, J.Bundgaard, E.Burgett, M.Cunningham, J.Deaven, D.L.Duke, U.Greife, S.Grimes, M.Heffner, T.Hill, D.Isenhower, J.L.Klay, V.Kleinrath, N.Kornilov, A.B.Laptev, W.Loveland, T.N.Massey, R.Meharchand, H.Qu, J.Ruz, S.Sangiorgio, B.Seilhan, L.Snyder, G.Tatishvili, R.T.Thornton, F.Tovesson, D.Towell, R.S.Towell, S.Watson, B.Wendt, L.Wood, for the NIFFTE Collaboration

The Data Analysis Framework for the NIFFTE Fission Time Projection Chamber

doi: 10.1016/j.nds.2014.08.105
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2014WO02      Nucl.Data Sheets 119, 377 (2014)

L.Wood, D.M.Asner, R.G.Baker, J.Bundgaard, E.Burgett, M.Cunningham, J.Deaven, D.L.Duke, U.Greife, S.Grimes, M.Heffner, T.Hill, D.Isenhower, J.L.Klay, V.Kleinrath, N.Kornilov, A.B.Laptev, W.Loveland, T.N.Massey, R.Meharchand, H.Qu, J.Ruz, S.Sangiorgio, B.Seilhan, L.Snyder, S.Stave, G.Tatishvili, R.T.Thornton, F.Tovesson, D.Towell, R.S.Towell, S.Watson, B.Wendt, for the NIFFTE Collaboration

An Ethernet-based Data Acquisition System for the NIFFTE Time Projection Chamber

doi: 10.1016/j.nds.2014.08.104
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2014YA07      Phys.Rev.Lett. 112, 152702 (2014)

R.Yanez, W.Loveland, L.Yao, J.S.Barrett, S.Zhu, B.B.Back, T.L.Khoo, M.Alcorta, M.Albers

Measurement of the Survival Probabilities for Hot Fusion Reactions

RADIOACTIVITY ²⁷⁴Hs(n) [from ²⁴⁸Cm(²⁵Mg, X), E=144.2 MeV; ²⁴⁸Cm(²⁶Mg, X), E=160.7 MeV]; measured decay products, En, In; deduced neutron multiplicities, elastic and fission resonance widths, survival probability of excited superheavy nuclei.

doi: 10.1103/PhysRevLett.112.152702
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2014YA10      Phys.Rev. C 89, 051604 (2014)

R.Yanez, L.Yao, J.King, W.Loveland, F.Tovesson, N.Fotiades

Excitation energy dependence of the total kinetic energy release in ²³⁵U(n, f)

NUCLEAR REACTIONS ²³⁵U(n, F), E=3.2-50 MeV; measured (fission fragment)(fission fragment)-coin, time-of-flight, total kinetic energy (E_TKE) release as function of incident neutron energy at WNR-LANSCE-LANL facility; deduced dependence of E_TKE and total excitation energy (E_TXE) on E(n). Comparison with GEF model predictions, and with previous experimental results.

doi: 10.1103/PhysRevC.89.051604
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2013VI01      Phys.Rev. C 87, 044603 (2013)

A.M.Vinodkumar, W.Loveland, R.Yanez, M.Leonard, L.Yao, P.Bricault, M.Dombsky, P.Kunz, J.Lassen, A.C.Morton, D.Ottewell, D.Preddy, M.Trinczek

Interaction of ¹¹Li with ²⁰⁸Pb

NUCLEAR REACTIONS ²⁰⁸Pb(¹¹Li, X)²¹²At/²¹³At/²¹⁴At/²¹⁵At/²¹⁶At, E=39.9, 36.5, 32.7, 28.6 MeV; measured Eα, Iα from evaporation residues, production σ(E), complete and incomplete fusion σ(E), breakup σ(E) at TRIUMF-ISAC2 facility. ²⁰⁹Bi(⁷Li, X)²¹²Rn/²¹³Rn, E=34.90 MeV; measured complete fusion σ, and compared to earlier experimental results. Comparison with theoretical predictions, and with results from experimental results of other reaction.

doi: 10.1103/PhysRevC.87.044603
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2013YA12      Phys.Rev. C 88, 014606 (2013)

R.Yanez, W.Loveland, J.S.Barrett, L.Yao, B.B.Back, S.Zhu, T.L.Khoo

Measurement of the fusion probability, P_CN, for hot fusion reactions

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁸O, F), E=101.2 MeV; ¹⁹⁷Au(²⁶Mg, F), E=147.3 MeV; ¹⁹⁷Au(³⁰Si, F), E=170.9 MeV; ¹⁹⁷Au(³⁶S, F), E=195.3 MeV; measured particle spectra, time-of-flight, fission fragment angular distributions at ATLAS-ANL facility; deduced fusion-fission and quasifission cross sections using formalism of Back, fusion probabilities P_CN. Comparison with previous measurements, and with systematic dependence of P_CN on fissility. Compiled experimental P_CN values for several reactions.

doi: 10.1103/PhysRevC.88.014606
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2012KO18      Phys.Rev. C 85, 054603 (2012)

J.J.Kolata, A.Roberts, A.M.Howard, D.Shapira, J.F.Liang, C.J.Gross, R.L.Varner, Z.Kohley, A.N.Villano, H.Amro, W.Loveland, E.Chavez

Fusion of ^{124, 132}Sn with ^{40, 48}Ca

NUCLEAR REACTIONS ^40,48Ca(¹²⁴Sn, X), (¹³²Sn, X), E(cm)=105-165 MeV; measured evaporation residue spectra, fusion σ(E); deduced reduced fusion σ(E), fusion barriers. Inverse kinematics. Wong model and PACE2 fits. Comparison with time-dependent Hartree-Fock (TDHF) and coupled-channels Born approximation (CCBA) calculations.

doi: 10.1103/PhysRevC.85.054603
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2012YA04      Phys.Rev. C 85, 044620 (2012)

R.Yanez, W.Loveland, J.Beckerman, M.Leonard, C.J.Gross, D.Shapira, J.F.Liang, Z.Kohley, R.L.Varner

Search for inverse fission of uranium

NUCLEAR REACTIONS ¹⁰⁰Mo(¹²⁴Sn, X)²²²U, E=595, 650 MeV; ¹⁰⁰Mo (¹³²Sn, X)²³⁰U, E=560 MeV; measured Eα, Iα, (ER)α-coin, cross section upper limits; calculated σ(E). ⁹⁶Zr(¹²⁴Sn, X), E=200-280 MeV; comparison between measured and predicted σ(E). Statistical model calculations. No evidence for inverse fission.

doi: 10.1103/PhysRevC.85.044620
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2011LO10      Phys.Rev. C 83, 044610 (2011)

W.Loveland, A.M.Vinodkumar, D.Peterson, J.P.Greene

Synthesis of heavy nuclei using damped collisions: A test

NUCLEAR REACTIONS ¹⁸⁶W(¹⁶⁰Gd, X), E=860 MeV; measured Eγ, Iγ, yields of the reaction products by activation method; deduced σ and σ(θ) as a function of charge and mass number. Synthesis of heavy nuclei. Comparison with the predictions of Zagrebaev and Greiner.

doi: 10.1103/PhysRevC.83.044610
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2011LO27      Radiochim.Acta Supp 1, Proc.in Radiochemistry 141 (2011)

W.Loveland

Fusion of ⁹Li with ⁷⁰Zn and ²⁰⁸Pb

NUCLEAR REACTIONS ⁷⁰Zn(⁹Li, X), E(cm)<15 MeV; ²⁰⁸Pb(⁹Li, X), E(cm)<45 MeV; measured reaction products; deduced fusion excitation functions. Comparison with coupled channels calculations code CCFULL.

doi: 10.1524/rcpr.2011.0026
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2010EL06      Phys.Rev.Lett. 105, 182701 (2010)

P.A.Ellison, K.E.Gregorich, J.S.Berryman, D.L.Bleuel, R.M.Clark, I.Dragojevic, J.Dvorak, P.Fallon, C.Fineman-Sotomayor, J.M.Gates, O.R.Gothe, I.Y.Lee, W.D.Loveland, J.P.McLaughlin, S.Paschalis, M.Petri, J.Qian, L.Stavsetra, M.Wiedeking, H.Nitsche

New Superheavy Element Isotopes: ²⁴²Pu(⁴⁸Ca, 5n)²⁸⁵114

NUCLEAR REACTIONS ²⁴²Pu(⁴⁸Ca, Xn)²⁸⁵Fl/²⁸⁶Fl/²⁸⁷Fl/²⁸⁸Fl, E=256 MeV; measured reaction products, Eα, Iα; deduced σ, Q-values. Comparison with experimental values.

RADIOACTIVITY ^285,286Fl, ²⁸¹Cn, ²⁷⁷Ds, ²⁷³Hs, ²⁶⁹Sg(α); measured Eα; deduced Q(α). ²⁶⁵Rf, ²⁸²Cn(SF); measured SF decay energy.

doi: 10.1103/PhysRevLett.105.182701
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2010YA21      Phys.Rev. C 82, 054615 (2010)

R.Yanez, W.Loveland, A.M.Vinodkumar, P.H.Sprunger, L.Prisbrey, D.Peterson, S.Zhu, J.J.Kolata, A.Villano, J.F.Liang

Isospin dependence of capture cross sections: The ³⁶S+²⁰⁸Pb reaction

NUCLEAR REACTIONS ²⁰⁸Pb(³⁶S, X), E(cm)=147.5, 151.7, 156.0, 160.6, 169.2, 186.3, 210.2 MeV; measured fission fragments, angular distributions, capture fission cross sections. Comparison of results to empirical prescriptions, QMD model and couple-channel calculations.

doi: 10.1103/PhysRevC.82.054615
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2009FO05      Phys.Rev. C 79, 064318 (2009)

C.M.Folden III, A.S.Nettleton, A.M.Amthor, T.N.Ginter, M.Hausmann, T.Kubo, W.Loveland, S.L.Manikonda, D.J.Morrissey, T.Nakao, M.Portillo, B.M.Sherrill, G.A.Souliotis, B.F.Strong, H.Takeda, O.B.Tarasov

New neutron-rich microsecond isomers observed among fission products of ²³⁸U at 80 MeV/nucleon

NUCLEAR REACTIONS ⁹Be(²³⁸U, X)^60mMn/^78mGa/^82mGa/^92mBr/^95mRb/^98mRb/^92mY/^101mY/^112mTc, E=80 MeV/nucleon; measured Eγ, Iγ, γγ-coin, isomer half-lives. ⁶⁰Mn, ^78,82Ga, ⁹²Br, ^95,98Rb, ^92,101Y, ¹¹²Tc; deduced levels, J, π. ^66mCu, ^78mZn, ^88mBr, ^95mKr, ^96mRb, ^97m,100mSr, ^99mMo, ^121mPd, ^124mSn, ^125mXe; measured Eγ and half-lives. ^91,92,93Y; measured Eγ.

doi: 10.1103/PhysRevC.79.064318
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2009PE09      Phys.Rev. C 79, 044607 (2009)

D.Peterson, W.Loveland, O.Batenkov, M.Majorov, A.Veshikov, K.Aleklett, C.Rouki

Direct observation of first-chance fission of ²⁵⁸No

NUCLEAR REACTIONS ²³²Th(²⁵Mg, X), E=132 MeV; ²³²Th(²⁶Mg, X), E=148 MeV; measured σ, mass and energy distributions of fission fragments, neutrons by time-of-flight method. ²⁵⁸No; deduced ratio of widths for neutron emission and fission (Γ_n/Γ_f) for the compound nucleus. Implications for survival probabilities of excited heavy nuclei formed in hot fusion reactions.

doi: 10.1103/PhysRevC.79.044607
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2009VI09      Phys.Rev. C 80, 054609 (2009)

A.M.Vinodkumar, W.Loveland, P.H.Sprunger, L.Prisbrey, M.Trinczek, M.Dombsky, P.Machule, J.J.Kolata, A.Roberts

Fusion of ⁹Li with ²⁰⁸Pb

NUCLEAR REACTIONS ²⁰⁸Pb(⁹Li, nx)²¹¹At/²¹²At/²¹³At/²¹⁴At, E(cm)=24.84, 27.35, 29.86, 32.36, 34.87, 37.37, 39.88, 42.38, 44.89 MeV; ²⁰⁹Bi(⁷Li, nx)²¹²Rn/²¹³Rn, E(cm)=34.95 MeV; measured nuclidic yields, and fusion σ using ISAC2 facility at TRIUMF. Comparison with HVAP statistical model code and coupled-channel calculations.

RADIOACTIVITY ^{211,212,212m,213,214,214m}At(α); measured Eα.

doi: 10.1103/PhysRevC.80.054609
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2008GA08      Phys.Rev. C 77, 034603 (2008)

J.M.Gates, M.A.Garcia, K.E.Gregorich, Ch.E.Dullmann, I.Dragojevic, J.Dvorak, R.Eichler, C.M.Folden III, W.Loveland, S.L.Nelson, G.K.Pang, L.Stavsetra, R.Sudowe, A.Turler, H.Nitsche

Synthesis of rutherfordium isotopes in the ²³⁸U(²⁶Mg, xn)^264-xRf reaction and study of their decay properties

NUCLEAR REACTIONS ²³⁸U(²⁶Mg, 3n), (²⁶Mg, 4n), (²⁶Mg, 5n), (²⁶Mg, 6n), E=4.9-6.0 MeV/nucleon; measured excitation functions, σ, half-lives, cross sections.

RADIOACTIVITY ²⁵⁸Rf(α) [from ²³⁸U(²⁶Mg, 6n), E=4.9-6.0 MeV/nucleon]; ²⁵⁹Rf(EC) [from ²³⁸U(²⁶Mg, 5n), E=4.9-6.0 MeV/nucleon]; ²⁶⁰Rf(α), (SF) [from ²³⁸U(²⁶Mg, 4n), E=4.9-6.0 MeV/nucleon]; ²⁶¹Rf(α), (SF) [from ²³⁸U(²⁶Mg, 3n), E=4.9-6.0 MeV/nucleon]; ²⁵⁴No(α); measured α spectra, Q-values, charged particle spectra.^{242,244,246,248,250,252,254,256,258}Fm, ^{248,250,252,254,256}No, ^{250,252,254,256}Rf, ^{252,254,256,258,260}Sg; systematics.

doi: 10.1103/PhysRevC.77.034603
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2008VI08      Phys.Rev. C 78, 054608 (2008)

A.M.Vinodkumar, W.Loveland, J.J.Neeway, L.Prisbrey, P.H.Sprunger, D.Peterson, J.F.Liang, D.Shapira, C.J.Gross, R.L.Varner, J.J.Kolata, A.Roberts, A.L.Caraley

¹³²Sn+⁹⁶Zr reaction: A study of fusion enhancement/hindrance

NUCLEAR REACTIONS ⁹⁶Zr(¹²⁴Sn, X), E(cm)=600 MeV; ⁹⁶Zr(¹³²Sn, X), E(cm)=192.8-249.1 MeV; calculated σ. Comparison with coupled channels calculations.

doi: 10.1103/PhysRevC.78.054608
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1795.

2007LI27      Phys.Rev. C 75, 054607 (2007)

J.F.Liang, D.Shapira, J.R.Beene, C.J.Gross, R.L.Varner, A.Galindo-Uribarri, J.Gomez del Campo, P.A.Hausladen, P.E.Mueller, D.W.Stracener, H.Amro, J.J.Kolata, J.D.Bierman, A.L.Caraley, K.L.Jones, Y.Larochelle, W.Loveland, D.Peterson

Fusion of radioactive ¹³²Sn with ⁶⁴Ni

NUCLEAR REACTIONS ⁶⁴Ni(¹³²Sn, X), E=453-620 MeV; measured cross sections and angular distributions. Compared results to statistical model calculations.

doi: 10.1103/PhysRevC.75.054607
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2007LI82      Eur.Phys.J. Special Topics 150, 35 (2007)

J.F.Liang, D.Shapira, C.J.Gross, R.L.Varner, H.Amro, J.R.Beene, J.D.Bierman, A.L.Caraley, A.Galindo-Uribarri, J.Gomez del Campo, P.A.Hausladen, K.L.Jones, J.J.Kolata, Y.Larochelle, W.Loveland, P.E.Mueller, D.Peterson, D.C.Radford, D.W.Stracener

Measurements of fusion reactions induced by radioactive ¹³²Sn on ⁶⁴Ni

NUCLEAR REACTIONS ¹³²Sn(⁶⁴Ni, X), E(cm) < 220 MeV; measured evaporation residue and fission cross sections. Compared results to model calculations.

doi: 10.1140/epjst/e2007-00259-7
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2007LO06      Phys.Rev. C 75, 069801 (2007)

W.Loveland

Comment on "Possibility of synthesizing a doubly magic superheavy nucleus"

doi: 10.1103/PhysRevC.75.069801
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2007LO07      Phys.Rev. C 76, 014612 (2007)

W.Loveland

Synthesis of transactinide nuclei using radioactive beams

COMPILATION Z=102-120; compiled and analyzed cold and hot fusion production cross sections.

doi: 10.1103/PhysRevC.76.014612
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2007NA27      Phys.Rev. C 76, 054604 (2007)

R.S.Naik, W.Loveland, P.H.Sprunger, A.M.Vinodkumar, D.Peterson, C.L.Jiang, S.Zhu, X.Tang, E.F.Moore, P.Chowdhury

Measurement of the fusion probability P_CN for the reaction of ⁵⁰Ti with ²⁰⁸Pb

NUCLEAR REACTIONS ²⁰⁸Pb(⁵⁰Ti, X), E(cm)=183.7, 186.2, 190.2, 194.2, 202.3 MeV; measured fission fragments, cross sections, angular distributions; deduced fusion probabilities and survival probabilities for compound nuclei Z=102-113.

doi: 10.1103/PhysRevC.76.054604
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2006LO13      Phys.Rev. C 74, 044607 (2006)

W.Loveland, D.Peterson, A.M.Vinodkumar, P.H.Sprunger, D.Shapira, J.F.Liang, G.A.Souliotis, D.J.Morrissey, P.Lofy

Fusion enhancement in the ³⁸S + ²⁰⁸Pb reaction

NUCLEAR REACTIONS ²⁰⁸Pb(³⁸S, X), E(cm)=160-265 MeV; measured capture-fission excitation function; deduced interaction barrier features.

doi: 10.1103/PhysRevC.74.044607
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2006LO16      Phys.Rev.C 74, 064609 (2006)

W.Loveland, A.M.Vinodkumar, R.S.Naik, P.H.Sprunger, B.Matteson, J.Neeway, M.Trinczek, M.Dombsky, P.Machule, D.Ottewell, D.Cross, K.Gagnon, W.J.Mills

Subbarrier fusion of ⁹Li with ⁷⁰Zn

NUCLEAR REACTIONS ⁷⁰Zn(⁹Li, X), E=11-15 MeV; measured fusion σ; deduced subbarrier enhancement. Comparison with model predictions.

doi: 10.1103/PhysRevC.74.064609
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2006ST07      Phys.Rev. C 73, 047602 (2006)

R.W.Stoenner, R.L.Klobuchar, P.E.Haustein, G.J.Virtes, J.B.Cumming, W.Loveland

Angular distributions in multifragmentation

NUCLEAR REACTIONS ¹⁹⁷Au(²⁰Ne, X)³⁷Ar/¹²⁷Xe, E=8 GeV; ¹⁹⁷Au(¹²C, X)³⁷Ar/¹²⁷Xe, E=25 GeV; ¹⁹⁷Au(²⁸Si, X)³⁷Ar/¹²⁷Xe, E=381 GeV; ¹⁹⁷Au(p, X)²⁴Na/²⁸Mg/⁴⁸Sc/⁴⁸V/⁵⁸Co/⁵⁹Fe/⁶⁵Zn/⁷⁴As/⁹⁰Nb/¹⁰⁰Pd/¹⁰⁰Rh/¹³¹Ba/¹⁴⁹Gd, E=28 GeV; measured fragments angular distributions; deduced sideward peaking enhancements for heavy ions. Kinetic-focusing model analysis.

doi: 10.1103/PhysRevC.73.047602
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2006VI10      Phys.Rev.C 74, 064612 (2006)

A.M.Vinodkumar, W.Loveland, P.H.Sprunger, D.Peterson, J.F.Liang, D.Shapira, R.L.Varner, C.J.Gross, J.J.Kolata

Capture cross sections for the near symmetric ¹²⁴Sn+⁹⁶Zr reaction

NUCLEAR REACTIONS ⁹⁶Zr(¹²⁴Sn, X), E(cm)=195-265 MeV; measured capture-fission σ. Comparison with model predictions.

doi: 10.1103/PhysRevC.74.064612
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1795.

2005GR19      Phys.Rev. C 72, 014605 (2005)

K.E.Gregorich, W.Loveland, D.Peterson, P.M.Zielinski, S.L.Nelson, Y.H.Chung, Ch.E.Dullmann, C.M.Folden III, K.Aleklett, R.Eichler, D.C.Hoffman, J.P.Omtvedt, G.K.Pang, J.M.Schwantes, S.Soverna, P.Sprunger, R.Sudowe, R.E.Wilson, H.Nitsche

Attempt to confirm superheavy element production in the ⁴⁸Ca + ²³⁸U reaction

NUCLEAR REACTIONS ²³⁸U(⁴⁸Ca, 3n), E=230.3, 235.6 MeV; measured σ upper limits; deduced no evidence for ²⁸³Cn. Comparison with previous results.

doi: 10.1103/PhysRevC.72.014605
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2005LI55      Eur.Phys.J. A 25, Supplement 1, 239 (2005)

J.F.Liang, D.Shapira, C.J.Gross, R.L.Varner, H.Amro, J.R.Beene, J.D.Bierman, A.L.Caraley, A.Galindo-Uribarri, J.Gomez del Campo, P.A.Hausladen, K.L.Jones, J.J.Kolata, Y.Larochelle, W.Loveland, P.E.Mueller, D.Peterson, D.C.Radford, D.W.Stracener

Sub-barrier fusion induced by neutron-rich radioactive ¹³²Sn

NUCLEAR REACTIONS ⁶⁴Ni(¹³²Sn, X), E=560 MeV; measured fission fragments and evaporation residues spectra, yields.

doi: 10.1140/epjad/i2005-06-117-x
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2005LO13      Eur.Phys.J. A 25, Supplement 1, 233 (2005)

W.Loveland

Fusion studies with RIBs

doi: 10.1140/epjad/i2005-06-118-9
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2005SH54      Eur.Phys.J. A 25, Supplement 1, 241 (2005)

D.Shapira, J.F.Liang, C.J.Gross, R.L.Varner, J.R.Beene, A.Galindo-Uribarri, J.Gomez Del Campo, P.E.Mueller, D.W.Stracener, P.A.Hausladen, C.Harlin, J.J.Kolata, H.Amro, W.Loveland, K.L.Jones, J.D.Bierman, A.L.Caraley

Measurement of evaporation residue cross sections from reactions with radioactive neutron-rich beams

NUCLEAR REACTIONS ⁶⁴Ni(¹³²Sn, X), (¹²⁴Sn, X), (¹³⁴Te, X), E not given; measured evaporation residue σ.

doi: 10.1140/epjad/i2005-06-190-1
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2004LI55      Prog.Theor.Phys.(Kyoto), Suppl. 154, 106 (2004)

J.F.Liang, D.Shapira, C.J.Gross, J.R.Beene, J.D.Bierman, A.Galindo-Uribarri, J.Gomez del Campo, P.A.Hausladen, Y.Larochelle, W.Loveland, P.E.Mueller, D.Peterson, D.C.Radford, D.W.Stracener, R.L.Varner

Sub-Barrier Fusion Enhancement in Neutron-Rich Radioactive ¹³²Sn on ⁶⁴Ni

NUCLEAR REACTIONS ⁶⁴Ni(¹³²Sn, X), E(cm)=140-200 MeV; measured evaporation residue excitation function; deduced sub-barrier fusion enhancement.

doi: 10.1143/PTPS.154.106
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2004LI71      Nucl.Phys. A746, 103c (2004)

J.F.Liang, D.Shapira, C.J.Gross, J.R.Beene, J.D.Bierman, A.Galindo-Uribarri, J.Gomez del Campo, P.A.Hausladen, Y.Larochelle, W.Loveland, P.E.Mueller, D.Peterson, D.C.Radford, D.W.Stracener, R.L.Varner

Enhanced evaporation residue cross sections in neutron-rich radioactive ¹³²Sn on ⁶⁴Ni

NUCLEAR REACTIONS ⁶⁴Ni(¹³²Sn, X), (¹²⁴Sn, X), E(cm) ≈ 150-200 MeV; measured evaporation residue σ; deduced sub-barrier fusion enhancement for heavier beam. Comparison with previous results, model predictions.

doi: 10.1016/j.nuclphysa.2004.09.057
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2004LO19      Nucl.Phys. A746, 108c (2004)

W.Loveland

Synthesis of heavy nuclei using radioactive nuclear beams

NUCLEAR REACTIONS ¹⁹⁶Pt(⁸⁸Kr, n), ²⁰⁴Hg(⁹⁴Kr, n), ²⁰⁹Bi(⁶⁶Cu, n), ²⁰⁸Pb(⁶¹Fe, n), (⁵⁹Cr, n), E not given; calculated fusion σ. A=256-272; calculated production rates at rare isotope accelerator.

doi: 10.1016/j.nuclphysa.2004.09.066
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2003CH23      Phys.Rev. C 67, 044611 (2003)

R.J.Charity, L.G.Sobotka, J.F.Dempsey, M.Devlin, S.Komarov, D.G.Sarantites, A.L.Caraley, R.T.deSouza, W.Loveland, D.Peterson, B.B.Back, C.N.Davids, D.Seweryniak

Temperature and n-p asymmetry dependencies of the level-density parameter in Ni+Mo fusion reactions

NUCLEAR REACTIONS ^92,100Mo(⁶⁰Ni, X), E=5-9 MeV/nucleon; measured evaporation residue velocity and angular distributions, mass distributions, neutron and light charged particle spectra; deduced reaction mechanism features. Comparison with statistical model predictions.

doi: 10.1103/PhysRevC.67.044611
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2003GI05      Phys.Rev. C 67, 064609 (2003); Erratum Phys.Rev. C 68, 029901 (2003)

T.N.Ginter, K.E.Gregorich, W.Loveland, D.M.Lee, U.W.Kirbach, R.Sudowe, C.M.Folden III, J.B.Patin, N.Seward, P.A.Wilk, P.M.Zielinski, K.Aleklett, R.Eichler, H.Nitsche, D.C.Hoffman

Confirmation of production of element 110 by the ²⁰⁸Pb(⁶⁴Ni, n) reaction

NUCLEAR REACTIONS ²⁰⁸Pb(⁶⁴Ni, n), E=312.5, 315, 317.5 MeV: measured delayed (recoil)α-coin; deduced production σ.

RADIOACTIVITY ²⁷¹Ds, ²⁶⁷Hs, ²⁶³Sg, ²⁵⁹Rf, ²⁵⁵No(α) [from ²⁰⁸Pb(⁶⁴Ni, n) and subsequent decay]; measured Eα.

doi: 10.1103/PhysRevC.67.064609
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1698.

2003GR26      Eur.Phys.J. A 18, 633 (2003)

K.E.Gregorich, T.N.Ginter, W.Loveland, D.Peterson, J.B.Patin, C.M.Folden III, D.C.Hoffman, D.M.Lee, H.Nitsche, J.P.Omtvedt, L.A.Omtvedt, L.Stavsetra, R.Sudowe, P.A.Wilk, P.M.Zielinski, K.Aleklett

Cross-section limits for the ²⁰⁸Pb(⁸⁶Kr, n)²⁹³118 reaction

NUCLEAR REACTIONS ²⁰⁸Pb(⁸⁶Kr, X), E=449 MeV; measured evaporation residue yields; deduced no evidence for ²⁹³Og. ²⁰⁸Pb(⁸⁶Kr, n), E=449 MeV; deduced production σ upper limit.

doi: 10.1140/epja/i2002-10165-x
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2003LI41      Phys.Rev.Lett. 91, 152701 (2003); Erratum Phys.Rev.Lett. 96, 029903 (2006)

J.F.Liang, D.Shapira, C.J.Gross, J.R.Beene, J.D.Bierman, A.Galindo-Uribarri, J.Gomez del Campo, P.A.Hausladen, Y.Larochelle, W.Loveland, P.E.Mueller, D.Peterson, D.C.Radford, D.W.Stracener, R.L.Varner

Enhanced Fusion-Evaporation Cross Sections in Neutron-Rich ¹³²Sn on ⁶⁴Ni

NUCLEAR REACTIONS ⁶⁴Ni(¹³²Sn, X), E=453-560 MeV; measured fusion-evaporation excitation function; deduced sub-barrier enhancement, role of multinucleon transfer. Coupled channels calculation.

doi: 10.1103/PhysRevLett.91.152701
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2002LO15      Phys.Rev. C66, 044617 (2002)

W.Loveland, K.E.Gregorich, J.B.Patin, D.Peterson, C.Rouki, P.M.Zielinski, K.Aleklett

Search for the production of element 112 in the ⁴⁸Ca+²³⁸U reaction

NUCLEAR REACTIONS ²³⁸U(⁴⁸Ca, 3n), E=231 MeV; measured Eα, (recoil)α-coin following residual nucleus decay; deduced σ upper limit.

doi: 10.1103/PhysRevC.66.044617
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2002NI10      Phys.Rev.Lett. 89, 039901 (2002); see also 1999Ni03

V.Ninov, K.E.Gregorich, W.Loveland, A.Ghiorso, D.C.Hoffman, D.M.Lee, H.Nitsche, W.J.Swiatecki, U.W.Kirbach, C.A.Laue, J.L.Adams, J.B.Patin, D.A.Shaughnessy, D.A.Strellis, P.A.Wilk

Editorial Note: Observation of Superheavy Nuclei Produced in the Reaction of ⁸⁶Kr with ²⁰⁸Pb

doi: 10.1103/PhysRevLett.89.039901
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2002SO06      Nucl.Phys. A705, 279 (2002)

G.A.Souliotis, W.Loveland, K.Hanold, G.J.Wozniak, D.J.Morrissey

Heavy Residue Formation in 20 MeV/nucleon ¹⁹⁷Au + ⁹⁰Zr Collisions

NUCLEAR REACTIONS ⁹⁰Zr(¹⁹⁷Au, X), E=20 MeV/nucleon; measured fragment yields, velocity distributions; deduced incomplete fusion, deep inelastic scattering. Comparison with model predictions.

doi: 10.1016/S0375-9474(02)00673-5
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1690.

2001CH39      J.Korean Phys.Soc. 38, 10 (2001)

Y.H.Chung, W.Loveland

Synthesis of Heavy Elements with Z = 110 - 114 using a Complete Fusion Reaction

NUCLEAR REACTIONS ²⁰⁹Bi(⁵⁹Co, n), (⁵⁸Ni, n), (⁶⁴Ni, n), ²⁰⁸Pb(⁶²Ni, n), (⁶³Cu, n), (⁷⁰Zn, n), ²³²Th(⁴⁰Ca, n), (⁴⁸Ti, n), (⁵⁰Cr, n), ²³⁸U(³⁹K, n), (⁴⁴Ca, n), (⁴⁵Sc, n), (⁴⁹Ti, n), E^* ≈ 15 MeV; calculated σ. Comparisons with data.

2001DJ01      Phys.Rev. C64, 034603 (2001)

B.Djerroud, D.K.Agnihotri, S.P.Baldwin, W.Skulski, J.Toke, W.U.Schroder, R.J.Charity, J.F.Dempsey, D.G.Sarantites, L.G.Sobotka, B.Lott, W.Loveland, K.Aleklett

Heavy Residues and Intermediate-Mass Fragment Production in Dissipative ¹⁹⁷Au + ⁸⁶Kr Collisions at E/A = 35 MeV

NUCLEAR REACTIONS ¹⁹⁷Au(⁸⁶Kr, X), E=35 MeV/nucleon; measured neutron spectra, light charged particle, intermediate mass fragment, projectile-like and target-like fragments spectra, yields, angular distributions, and correlations; deduced heavy residue survival features, related reaction mechanism features.

doi: 10.1103/PhysRevC.64.034603
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2001NI02      Nucl.Phys. A682, 98c (2001)

V.Ninov, K.E.Gregorich, T.N.Ginter, F.P.Hessberger, R.Krucken, D.M.Lee, W.Loveland, W.D.Myers, J.Patin, M.W.Rowe, N.K.Seward, W.J.Swiatecki, A.Turler, P.A.Wilk

Production and Structure of the Heaviest Elements

doi: 10.1016/S0375-9474(00)00627-8
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2001ZY01      Phys.Rev. C63, 024615 (2001)

K.E.Zyromski, W.Loveland, G.A.Souliotis, D.J.Morrissey, C.F.Powell, O.Batenkov, K.Aleklett, R.Yanez, I.Forsberg

Fusion Enhancement in the ^{32, 38}S + ¹⁸¹Ta Reaction

NUCLEAR REACTIONS ¹⁸¹Ta(³²S, F), E=157-300 MeV; ¹⁸¹Ta(³⁸S, F), E ≈ 8 MeV/nucleon; measured σ(E, θ), fission fragments angular distributions; deduced fusion barriers, fusion and quasi-fission σ, enhancemant with radioactive beam. Coupled-channels calculations.

doi: 10.1103/PhysRevC.63.024615
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2000LO02      J.Radioanal.Nucl.Chem. 243, 147 (2000)

W.Loveland

Recent Advances in Understanding Nuclear Reactions

doi: 10.1023/A:1006735802115
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1999LO03      Phys.Rev. C59, 1472 (1999)

W.Loveland, M.Andersson, K.E.Zyromski, N.Ham, B.Altschul, J.Vlcakova, D.Menge, J.O.Liljenzin, R.Yanez, K.Aleklett

Heavy Residue Production in the Interaction of 29 MeV/Nucleon ²⁰⁸Pb with ¹⁹⁷Au

NUCLEAR REACTIONS ¹⁹⁷Au(²⁰⁸Pb, X), E=29 MeV/nucleon; measured fragments isotopic yields, velocity and angular distributions; deduced reaction mechanism features. Comparison with nucleon transport model.

doi: 10.1103/PhysRevC.59.1472
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1999NI03      Phys.Rev.Lett. 83, 1104 (1999); Erratum Phys.Rev.Lett. 89, 039901 (2002); see also 2002GrZZ

V.Ninov, K.E.Gregorich, W.Loveland, A.Ghiorso, D.C.Hoffman, D.M.Lee, H.Nitsche, W.J.Swiatecki, U.W.Kirbach, C.A.Laue, J.L.Adams, J.B.Patin, D.A.Shaughnessy, D.A.Strellis, P.A.Wilk

Observation of Superheavy Nuclei Produced in the Reaction of ⁸⁶Kr with ²⁰⁸Pb

NUCLEAR REACTIONS ²⁰⁸Pb(⁸⁶Kr, n), E=449 MeV; measured α-spectra, (recoil)α-, αα-coin following residual nucleus decay, production σ; deduced evidence for ²⁹³Og, ²⁸⁹Lv, ²⁸⁵Fl, ²⁸¹Cn, ²⁷⁷Ds, ²⁷³Hs, ²⁶⁹Sg. Gas-filled separator.

RADIOACTIVITY ²⁹³Og, ²⁸⁹Lv, ²⁸⁵Fl, ²⁸¹Cn, ²⁷⁷Ds, ²⁷³Hs(α) [from ²⁰⁸Pb(⁸⁶Kr, n) and subsequent α-decay]; measured Eα, T_1/2.

doi: 10.1103/PhysRevLett.83.1104
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1998SO11      Phys.Rev. C57, 3129 (1998)

G.A.Souliotis, K.Hanold, W.Loveland, I.Lhenry, D.J.Morrissey, A.C.Veeck, G.J.Wozniak

Heavy Residue Formation in 20 MeV/nucleon ¹⁹⁷Au-¹²C and ¹⁹⁷Au-²⁷Al Collisions

NUCLEAR REACTIONS ¹²C, ²⁷Al(¹⁹⁷Au, X), E=20 MeV/nucleon; measured fragments isotopic yields vs momentum transfer, velocity distributions; deduced fission delay times. Comparison with statistical models. Fragment separator.

doi: 10.1103/PhysRevC.57.3129
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1997LO11      J.Phys.(London) G23, 1251 (1997)

W.Loveland, K.E.Zyromski, G.A.Souliotis, D.J.Morrissey, C.F.Powell, O.Batenkov, K.Aleklett, R.Yanez, I.Forsberg

Fusion Enhancement with Neutron-Rich Radioactive Beams

NUCLEAR REACTIONS, ICPND ¹⁸¹Ta(³²S, X), (³²S, F), E(cm)=120-260 MeV; ¹⁸¹Ta(³⁸S, X), (³⁸S, F), E(cm)=120-220 MeV; measured fusion, fission σ; deduced heavy elements systhesis implications. Coupled-channels calculations. Radioactive beam.

doi: 10.1088/0954-3899/23/10/012
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1997SO07      Phys.Rev. C55, R2146 (1997)

G.A.Souliotis, W.Loveland, K.E.Zyromski, G.J.Wozniak, D.J.Morrissey, J.O.Liljenzin, K.Aleklett

Production of Neutron Rich Nuclides and Radioactive Beams by Intermediate Energy ²³⁸U Fission

NUCLEAR REACTIONS, ICPND ²⁰⁸Pb(²³⁸U, F)¹⁰⁶Zr/¹⁰⁷Zr/¹¹¹Mo/¹¹⁴Tc/¹¹⁶Ru/¹¹⁷Ru/¹¹⁸Rh/¹²¹Pd/¹²²Pd/¹²⁵Ag, E=20 MeV/nucleon; measured fragment production σ vs Z, mass for very neutron rich fission fragments; deduced residuals production σ, production rates of radioactive beams of neutron rich nuclei in projectile fragmentation facilities.

doi: 10.1103/PhysRevC.55.R2146
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1997ZY01      Phys.Rev. C55, R562 (1997)

K.E.Zyromski, W.Loveland, G.A.Souliotis, D.J.Morrissey, C.F.Powell, O.Batenkov, K.Aleklett, R.Yanez, I.Forsberg, M.Sanchez-Vega, J.R.Dunn, B.G.Glagola

Fusion Enhancement with Neutron-Rich Radioactive Beams

NUCLEAR REACTIONS, ICPND ¹⁸¹Ta(³²S, F), E(cm)=150-300 MeV; ¹⁸¹Ta(³⁸S, X), E(cm)=125-220 MeV; measured fusion-fission σ(E); deduced fusion barrier heights.

doi: 10.1103/PhysRevC.55.R562
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1996SK02      Phys.Rev. C53, R2594 (1996)

W.Skulski, B.Djerroud, D.K.Agnihotri, S.P.Baldwin, J.Toke, X.Zhao, W.U.Schroder, L.G.Sobotka, R.J.Charity, J.Dempsey, D.G.Sarantites, B.Lott, W.Loveland, K.Aleklett

Origin of Slow, Heavy Residues Observed in Dissipative ¹⁹⁷Au + ⁸⁶Kr Collisions at E/A = 35 MeV

NUCLEAR REACTIONS ¹⁹⁷Au(⁸⁶Kr, X), (⁸⁶Kr, F), E=35 MeV/nucleon; measured neutron, charged particle multiplicities, fragment energy, (fragment)(fragment)-coin; deduced heavy fragment production σ, reaction mechanism.

doi: 10.1103/PhysRevC.53.R2594
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1996YA05      Phys.Lett. 376B, 29 (1996)

R.Yanez, W.Loveland, D.J.Morrissey, K.Aleklett, J.O.Liljenzin, E.Hagebo, D.Jerrestam, L.Westerberg

Systematics of Angular Momentum Transfer in Intermediate Energy Nuclear Collisions

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁶O, F), E=22, 30 MeV/nucleon; measured fission (fragment)(fragment)(θ, φ); deduced angular momentum transfer and alignment, systematics of angular momentum transfer.

doi: 10.1016/0370-2693(96)00260-2
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1995GH04      Nucl.Phys. A583, 861c (1995)

A.Ghiorso, D.Lee, L.P.Somerville, W.Loveland, J.M.Nitschke, W.Ghiorso, G.T.Seaborg, P.Wilmarth, R.Leres, A.Wydler, M.Nurmia, K.Gregorich, R.Gaylord, T.Hamilton, N.J.Hannink, D.C.Hoffman, C.Jarzynski, C.Kacher, B.Kadkhodayan, S.Kreek, M.Lane, A.Lyon, M.A.McMahan, M.Neu, T.Sikkeland, W.J.Swiatecki, A.Turler, J.T.Walton, S.Yashita

Evidence for the Synthesis of ²⁶⁷110 Produced by the ⁵⁹Co + ²⁰⁹Bi Reaction

NUCLEAR REACTIONS ²⁰⁹Bi(⁵⁹Co, n), E ≈ 5.1 MeV/nucleon; measured Eα, production σ; deduced evidence for ²⁶⁷Ds.

doi: 10.1016/0375-9474(94)00775-I
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1995GH05      Phys.Rev. C51, R2293 (1995)

A.Ghiorso, D.Lee, L.P.Somerville, W.Loveland, J.M.Nitschke, W.Ghiorso, G.T.Seaborg, P.Wilmarth, R.Leres, A.Wydler, M.Nurmia, K.Gregorich, K.Czerwinski, R.Gaylord, T.Hamilton, N.J.Hannink, D.C.Hoffman, C.Jarzynski, C.Kacher, B.Kadkhodayan, S.Kreek, M.Lane, A.Lyon, M.A.McMahan, M.Neu, T.Sikkeland, W.J.Swiatecki, A.Turler, J.T.Walton, S.Yashita

Evidence for the Possible Synthesis of Element 110 Produced by the ⁵⁹Co + ²⁰⁹Bi Reaction

NUCLEAR REACTIONS ²⁰⁹Bi(⁵⁹Co, n), E=5.1 MeV/nucleon; measured implanted recoil Bρ, dE/dx, recoil energy; deduced ²⁶⁷Ds synthesis evidence, production σ.

doi: 10.1103/PhysRevC.51.R2293
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1995YA08      Phys.Rev. C52, 203 (1995)

R.Yanez, W.Loveland, K.Aleklett, A.Srivastava, J.O.Liljenzin

Heavy-Residue Production in Ar-Th Collisions at 44, 77, and 95 MeV/nucleon

NUCLEAR REACTIONS, ICPND ²³²Th(⁴⁰Ar, X), E=44, 77 MeV/nucleon; ²³²Th(³⁶Ar, X), E=95 MeV/nucleon; measured yields for nuclides with mass=24-124, fragment mass distributions, average energies, linear momentum transfer.

doi: 10.1103/PhysRevC.52.203
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1993LO08      Phys.Lett. 312B, 53 (1993)

W.Loveland, K.Aleklett, R.Yanez, A.Srivastava, J.O.Liljenzin

Properties of Target-Like Fragments of Xe-Au Collisions at Intermediate Energies

NUCLEAR REACTIONS ¹⁹⁷Au(¹²⁹Xe, X), E=21-44 MeV/nucleon; ¹⁹⁷Au(¹³²Xe, X), E=26 MeV/nucleon; measured σ(fragment θ), fragment production σ, total kinetic energy, isobaric yield distributions; deduced phenomenological model inadequacies. Activation technique, target-like fragments.

doi: 10.1016/0370-2693(93)90486-2
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1992YO03      Phys.Rev. C46, 647 (1992)

A.Yokoyama, W.Loveland, J.O.Liljenzin, K.Aleklett, D.J.Morrissey, G.T.Seaborg

Fragmentation of ¹⁹⁷Au by 21 MeV/Nucleon ¹²⁹Xe

NUCLEAR REACTIONS ¹⁹⁷Au(¹²⁹Xe, X), (¹²⁹Xe, F), E=21 MeV/nucleon; measured residuals production σ, independent yield distribution, intermediate mass, fission fragment recoils, X=²⁴Na-¹⁹⁸Tl; deduced fragment mass distribution, velocities, momenta. Stochastic nucleon exchange model.

doi: 10.1103/PhysRevC.46.647
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1990AL03      Phys.Lett. 236B, 404 (1990)

K.Aleklett, W.Loveland, M.De Saint-Simon, L.Sihver, J.O.Liljenzin, G.T.Seaborg

Heavy Residue Linear Momenta in Intermediate Energy Krypton-Gold Collisions

NUCLEAR REACTIONS ¹⁹⁷Au(⁸⁶Kr, X), E=35, 43 MeV/nucleon; measured heavy residues energy, velocity; deduced momentum transfer features.

doi: 10.1016/0370-2693(90)90373-E
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1990LO01      Phys.Rev. C41, 973 (1990)

W.Loveland, K.Aleklett, L.Sihver, Z.Xu, C.Casey, D.J.Morrissey, J.O.Liljenzin, M.de Saint-Simon, G.T.Seaborg

Changes in Target Fragmentation Mechanisms with Increasing Projectile Energy in Intermediate Energy Nuclear Collisions

NUCLEAR REACTIONS, ICPND ¹⁹⁷Au(³²S, X), E=512 MeV; ¹⁹⁷Au(⁴⁰Ar, X), E=1280, 1760 MeV; measured σ(fragment Z, A, θ); deduced fission σ(E), reaction mechanism, fragment isobaric yield distributions.

doi: 10.1103/PhysRevC.41.973
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1990LO12      Phys.Rev. C42, 1753 (1990)

W.Loveland, M.Hellstrom, L.Sihver, K.Aleklett

Target Fragment Mass Distribution for the Reaction of 13.3 GeV/Nucleon ²⁸Si with ¹⁹⁷Au

NUCLEAR REACTIONS, MECPD ¹⁹⁷Au(²⁸Si, X), E=13.3 GeV/nucleon; measured fragment production σ.

doi: 10.1103/PhysRevC.42.1753
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1989AL13      Nucl.Phys. A499, 591 (1989)

K.Aleklett, M.Johansson, L.Sihver, W.Loveland, H.Groening, P.L.McGaughey, G.T.Seaborg

Heavy-Residue Spectra in the Interaction of 85 A MeV ¹²C with ¹⁹⁷Au

NUCLEAR REACTIONS ¹⁹⁷Au(¹²C, X), E=1032 MeV; measured fragment differential ranges; deduced σ(θ, E), heavy residue longitudinal momenta.

doi: 10.1016/0375-9474(89)90547-2
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1989CA18      Phys.Rev. C40, 1244 (1989)

C.Casey, W.Loveland, Z.Xu, L.Sihver, K.Aleklett, G.T.Seaborg

Nonequilibrium Fission and Heavy Residue Production in the Interaction of 12-16 MeV/Nucleon ³²S with ¹⁶⁵Ho

NUCLEAR REACTIONS ¹⁶⁵Ho(³²S, X), E=12-16 MeV/nucleon; measured σ(fragment Z, A, θ, E); deduced fragment production σ(A), σ(θ), fast nonequilibrium fission.

doi: 10.1103/PhysRevC.40.1244
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1988AL26      Phys.Rev. C38, 1658 (1988), Erratum Phys. Rev. C44, 566 (1991)

K.Aleklett, R.Brandt, G.Dersch, G.Feige, E.M.Friedlander, E.Ganssauge, G.Haase, D.C.Hoffman, J.Herrmann, B.Judek, W.Loveland, P.L.McGaughey, N.T.Porile, W.Shulz, G.T.Seaborg

Unusual Behavior of Projectile Fragments Produced by the Interactions of Relativistic Ar Ions with Copper

NUCLEAR REACTIONS Cu(⁴⁰Ar, X), E=0.9, 1.8 GeV/nucleon; measured reaction products, Eγ, Iγ; deduced target fragment production σ, projectile fragment secondary interaction properties.

doi: 10.1103/PhysRevC.38.1658
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1988LO02      Phys.Rev. C37, 1311 (1988)

W.Loveland, K.Aleklett, M.Bronikowski, Y.Y.Chu, J.B.Cumming, P.E.Haustein, S.Katcoff, N.T.Porile, L.Sihver

Unusual Backward Emission of Multifragmentation Products in Ultrarelativistic Nucleus-Nucleus Collisions

NUCLEAR REACTIONS ⁵¹V, Cu, Ag, ¹⁹⁷Au(¹⁶O, X)²⁴Na, E=232 GeV; measured residual fragment forward to backward emission ratio; deduced σ(θ). Thick-target, thick-catcher method.

doi: 10.1103/PhysRevC.37.1311
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1988LO10      Phys.Rev. C38, 2094 (1988)

W.Loveland, Z.Xu, C.Casey, K.Aleklett, J.O.Liljenzin, D.Lee, G.T.Seaborg

Total Projectile Kinetic Energy Scaling in Energetic Nucleus-Nucleus Collisions

NUCLEAR REACTIONS ¹⁹⁷Au(¹³⁹La, X), E=150 MeV/nucleon; measured σ(fragment Z, A); deduced σ(A). Total kinetic energy scaling, target fragmentation, intranuclear cascade model.

doi: 10.1103/PhysRevC.38.2094
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1987AL15      Fizika(Zagreb) 19, Supplement 1, 63 (1987)

K.Aleklett, W.Loveland, L.Sihver, Z.Xu, C.Casey, G.T.Seaborg

Formation of Large Residues in Intermediate Energy Nuclear Collisions

NUCLEAR REACTIONS ¹⁹⁷Au(¹²C, X), (²⁰Ne, X), (³²S, X), (⁴⁰Ar, X), (⁸⁴Kr, X), (¹³⁹La, X), E=intermediate; measured fragment yields, velocity spectra, σ(fragment θ); deduced fragment production mechanism.

1987LO14      Nucl.Phys. A471, 175c (1987)

W.Loveland, K.Aleklett, L.Sihver, Z.Xu, C.Casey, G.T.Seaborg

Formation of Large Target Residues in Intermediate Energy Nuclear Collisions

NUCLEAR REACTIONS ¹⁹⁷Au(¹²C, X), E=35, 85 MeV/nucleon; ¹⁹⁷Au(⁴⁰Ar, X), E=32 MeV/nucleon; ¹⁹⁷Au(⁸⁴Kr, X), E=35 MeV/nucleon; ¹⁹⁷Au(¹³⁹La, X), E=150 MeV/nucleon; measured fragment isobaric yield distributions, σ(fragment θ(moving frame)) for X=⁹⁹Mo, ¹³¹Ba, ¹⁷¹Lu, ⁵⁸Co, ⁸⁷Y, ¹⁴⁶Gd; deduced fragment production mechanism. Boltzmann transport equation.

doi: 10.1016/0375-9474(87)90250-8
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1986AL02      Phys.Rev. C33, 885 (1986)

K.Aleklett, W.Loveland, T.Lund, P.L.McGaughey, Y.Morita, G.T.Seaborg, E.Hagebo, I.Haldorsen

Fast and Slow Processes in the Fragmentation of ²³⁸U by 85 MeV/Nucleon ¹²C

NUCLEAR REACTIONS ²³⁸U(¹²C, X), (¹²C, F), E=85 MeV/nucleon; measured fission, projectile breakup fragment σ(θ, Z, A); deduced fragment σ(θ), fragmentation mechanism, average fissioning system angular momentum.

doi: 10.1103/PhysRevC.33.885
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1986AL25      Phys.Scr. 34, 489 (1986)

K.Aleklett, W.Loveland, T.T.Sugihara, A.N.Behkami, D.J.Morrissey, Li Wenxin, Wing Kot, G.T.Seaborg

Incomplete and Complete Fusion in Intermediate Energy Heavy Ion Reactions

NUCLEAR REACTIONS ¹⁵⁴Sm(¹⁶O, X)¹⁵¹Tb/¹⁵⁶Tb/¹⁵¹Gd, E=19 MeV/nucleon; ¹⁵⁴Sm(¹²C, X)¹⁴⁵Eu/¹⁴⁷Eu/¹³⁵Ce/¹³¹Ba/¹²³I/¹²¹Te/¹⁰⁵Ag, E=35, 85 MeV/nucleon; measured residual nuclei yields, σ(θ), differential range spectra; deduced isobaric yields, velocity spectra. Enriched target, activation method. Boltzmann master equation.

doi: 10.1088/0031-8949/34/6A/004
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1985DE61      Phys.Rev.Lett. 55, 1176 (1985)

G.Dersch, R.Beckmann, G.Feige, T.Lund, P.Vater, R.Brandt, E.Ganssauge, K.Aleklett, E.M.Friedlander, P.L.McGaughey, G.T.Seaborg, W.Loveland, J.Herrmann, N.T.Porile

Unusual Behavior of Projectile Fragments from the Interaction of Copper with Relativistic Ar Ions

NUCLEAR REACTIONS Cu(⁴⁰Ar, X), E=0.9, 1.8 GeV/A; measured reaction products, Eγ, Iγ; deduced fragments σ.

doi: 10.1103/PhysRevLett.55.1176
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1985KR02      Nucl.Phys. A432, 525 (1985)

R.H.Kraus, Jr., W.Loveland, K.Aleklett, P.L.McGaughey, T.T.Sugihara, G.T.Seaborg, T.Lund, Y.Morita, E.Hagebo, I.R.Haldorsen

Target-Fragment Angular Distributions for the Interaction of 86 MeV/A ¹²C with ¹⁹⁴Au

NUCLEAR REACTIONS ¹⁹⁷Au(¹²C, X), E=1032 MeV; measured σ(fragment Z, A); deduced fissioning system angular momentum. Intermediate-energy heavy ions. Fire-streak model, fission, two-step, hydrodynamical models.

doi: 10.1016/0375-9474(85)90258-1
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1985MC01      Phys.Rev. C31, 896 (1985); Erratum Phys.Rev. C32, 1107 (1985)

P.L.McGaughey, W.Loveland, D.J.Morrissey, K.Aleklett, G.T.Seaborg

Uranium Target Fragmentation by Intermediate and High Energy ¹²C and ²⁰Ne Ions

NUCLEAR REACTIONS ²³⁸U(¹²C, X), E=1, 3, 4.8, 12 GeV; ²³⁸U(²⁰Ne, X), E=8, 20 GeV; measured σ(fragment Z, A); deduced σ(A). Nuclear firestreak model, intranuclear cascade model, target fragmentation, fission, spallation.

doi: 10.1103/PhysRevC.31.896
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1983JA11      Can.J.Chem. 61, 701 (1983)

B.V.Jacak, W.Loveland, D.J.Morrissey, P.L.McGaughey, G.T.Seaborg

Heavy Target Fragment Yields in the Interaction of 28 GeV Protons with ²³⁸U

NUCLEAR REACTIONS ²³⁸U(p, X)⁷¹As/⁷²As/⁷⁴As/⁷⁶As/⁸⁴Rb/⁸⁶Y/⁸⁷Y/^87mY/⁸⁸Zr/⁸⁹Zr/⁹⁰Nb/⁹¹Sr/⁹²Nb/^92mNb/⁹⁵Zr/⁹⁵Nb/⁹⁵Tc/⁹⁷Zr/⁹⁹Mo/¹⁰⁰Rh/¹⁰¹Rh/^101mRh/¹⁰⁵Ru/¹⁰⁵Rh/¹⁰⁶Ag/^106mAg/¹¹¹In/¹¹⁸Sb/^118mSb/¹¹⁹Te/^119mTe/¹²⁰Sb/¹²¹Te/¹²²Sb/¹²³I/¹²⁴Sb/¹²⁴I/¹²⁵Xe/¹²⁶Sb/¹²⁷Sb, E=28 GeV; measured fragment yields, charge dispersion; deduced isobar production σ, reaction mechanism.

doi: 10.1139/v83-130
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1983MO22      Phys.Rev. C28, 2519 (1983)

Y.Morita, W.Loveland, G.T.Seaborg

Target Fragment Angular Distributions for the Interaction of 25.2 GeV ¹²C with ¹⁹⁷Au

NUCLEAR REACTIONS ¹⁹⁷Au(¹²C, X), E=25.2 GeV; measured σ(fragment θ) for X=^44mSc, ⁹⁷Ru, ¹⁴⁵Eu, ¹⁴⁹Gd, ¹⁷¹Lu. Two-step, firestreak model analyses.

doi: 10.1103/PhysRevC.28.2519
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1982GR20      Nucl.Phys. A389, 80 (1982)

H.Groening, K.Aleklett, K.J.Moody, P.L.McGaughey, W.Loveland, G.T.Seaborg

Isomer Ratio Measurements for the Reaction ²⁹Si(¹⁸O, p2n)^44m,44gSc

NUCLEAR REACTIONS, ICPND ²⁹Si(¹⁸O, 2np), E=30-99 MeV; measured isomer relative σ(E). Enriched targets. Statistical model.

doi: 10.1016/0375-9474(82)90292-5
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1982MO31      Phys.Rev. C 26, 511 (1982)

Y.Morita, W.Loveland, P.L.McGaughey, G.T.Seaborg

Target fragment angular distributions from the interaction of 3.0 GeV and 12.0 GeV ¹²C with ¹⁹⁷Au and ²³⁸U

NUCLEAR REACTIONS ¹⁹⁷Au(¹²C, X)⁸⁹Zr/⁹⁰Nb/⁹⁷Ru/¹²³I/¹⁴⁵Eu/¹⁴⁹Gd/¹⁵²Tb/¹⁵⁵Dy, E=3, 12 GeV; ²³⁸U(¹²C, X)⁴³K/⁷²As/⁸⁹Zr/⁹⁹Mo/¹³³I/¹⁴⁹Gd, E=3, 12 GeV; measured reaction products, Eγ, Iγ; deduced σ(θ).

doi: 10.1103/PhysRevC.26.511
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Note: The following list of authors and aliases matches the search parameter W.Loveland: , W.D.LOVELAND