Toward the Discovery of New Elements: Production of Livermorium (Z=116) with Ti 50

J. M. Gates, R. Orford, D. Rudolph, C. Appleton, B. M. Barrios, J. Y. Benitez, M. Bordeau, W. Botha, C. M. Campbell, J. Chadderton, A. T. Chemey, R. M. Clark, H. L. Crawford, J. D. Despotopulos, O. Dorvaux, N. E. Esker, P. Fallon, C. M. Folden, B. J.P. Gall, F. H. GarciaP. Golubev, J. A. Gooding, M. Grebo, K. E. Gregorich, M. Guerrero, R. A. Henderson, R. D. Herzberg, Y. Hrabar, T. T. King, M. Kireeff Covo, A. S. Kirkland, R. Krücken, E. Leistenschneider, E. M. Lykiardopoulou, M. McCarthy, J. A. Mildon, C. Müller-Gatermann, L. Phair, J. L. Pore, E. Rice, K. P. Rykaczewski, B. N. Sammis, L. G. Sarmiento, D. Seweryniak, D. K. Sharp, A. Sinjari, P. Steinegger, M. A. Stoyer, J. M. Szornel, K. Thomas, D. S. Todd, P. Vo, V. Watson, P. T. Wooddy

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Abstract

The Pu244(Ti50,xn)Lv294-x reaction was investigated at Lawrence Berkeley National Laboratory's 88-Inch Cyclotron. The experiment was aimed at the production of a superheavy element with Z≥114 by irradiating an actinide target with a beam heavier than Ca48. Produced Lv ions were separated from the unwanted beam and nuclear reaction products using the Berkeley Gas-filled Separator and implanted into a newly commissioned focal-plane detector system. Two decay chains were observed and assigned to the decay of Lv290. The production cross section was measured to be σprod=0.44(-0.28+0.58) pb at a center-of-target center-of-mass energy of 220(3) MeV. This represents the first published measurement of the production of a superheavy element near the "island of stability,"with a beam of Ti50 and is an essential precursor in the pursuit of searching for new elements beyond Z=118.

Original languageEnglish
Article number172502
JournalPhysical Review Letters
Volume133
Issue number17
DOIs
StatePublished - Oct 25 2024

Funding

We gratefully acknowledge the operations staff of the 88-Inch Cyclotron for providing the intense beams of and stable operating conditions. This work was supported in part by the U.S. Department of Energy, Office of Science, Office of Nuclear Physics under Contracts No. DE-AC02-05CH11231 (LBNL), No. DE-AC02-06CH11357 (ANL), and No. DE-FG02-93ER40773 (TAMU); U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences under Contracts No. DE-AC02-05CH11231 (LBNL); the Swedish Knut and Alice Wallenberg Foundation (Grant No. KAW 2015.0021), the Wenner-Gren Foundations (Grant No. SSv2020-0003), the Carl Trygger Foundation (Grant No. CTS 20\u22361146), and the Royal Physiographic Society in Lund; UK Science and Technology Facilities Council under Grants No. ST/V001027/1 (Liverpool), No. ST/T004797/1, and No. ST/V001116/1 (Manchester); startup package from the Oregon State University College of Engineering; Office of Nuclear Regulatory Research, Nuclear Regulatory Commission under Grant No. 31310022M0019 (SJSU); U.S. Department of Energy under Contracts No. DE-AC52-07NA27344 (LLNL) and No. DE-AC05-00OR22725 (ORNL); Swiss National Science Foundation under Grant No. 200020_196981; CNRS research funds (IPHC). The authors are indebted (for the use of ) to the U.S. Department of Energy, through the transplutonium element production facilities at Oak Ridge National Laboratory.

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