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The beam passes through the target and reaches the next chamber, the separator; if a new nucleus is produced, it is carried with this beam.<ref name="SHEhowvideo">{{Cite web|url=https://www.scientificamerican.com/article/how-to-make-superheavy-elements-and-finish-the-periodic-table-video/|title=How to Make Superheavy Elements and Finish the Periodic Table [Video]|author=Chemistry World|date=2016|website=[[Scientific American]]|language=en|url-status=live|access-date=2020-01-27}}</ref> In the separator, the newly produced nucleus is separated from other nuclides (that of the original beam and any other reaction products){{Efn|This separation is based on that the resulting nuclei move past the target more slowly then the unreacted beam nuclei. The separator contains electric and magnetic fields whose effects on a moving particle cancel out for a specific velocity of a particle.{{sfn|Hoffman|2000|p=334}} Such separation can also be aided by a [[Time-of-flight mass spectrometry|time-of-flight measurement]] and a recoil energy measurement; a combination of the two may allow to estimate the mass of a nucleus.{{sfn|Hoffman|2000|p=335}}}} and transferred to a [[Semiconductor detector|surface-barrier detector]], which stops the nucleus. The exact ___location of the upcoming impact on the detector is marked; also marked are its energy and the time of the arrival.<ref name="SHEhowvideo" /> The transfer takes about 10<sup>−6</sup> seconds; in order to be detected, the nucleus must survive this long.{{sfn|Zagrebaev|2013|page=3}} The nucleus is recorded again once its decay is registered, and the ___location, the [[Decay energy|energy]], and the time of the decay are measured.<ref name="SHEhowvideo" />
Stability of a nucleus is provided by the strong interaction. However, its range is very short; as nuclei become larger, its influence on the outermost [[nucleon]]s ([[proton]]s and neutrons) weakens. At the same time, the nucleus is torn apart by electrostatic repulsion between protons, as it has unlimited range.{{sfn|Beiser|2003|p=432}} Superheavy nuclei are thus theoretically predicted<ref>{{Cite journal|last=Staszczak|first=A.|last2=Baran|first2=A.|last3=Nazarewicz|first3=W.|date=2013|title=Spontaneous fission modes and lifetimes of superheavy elements in the nuclear density functional theory|url=|journal=Physical Review C|volume=87|issue=2|
The information available to physicists aiming to synthesize a superheavy element is thus the information collected at the detectors: ___location, energy, and time of arrival of a particle to the detector, and those of its decay. The physicists analyze this data and seek to conclude that it was indeed caused by a new element and could not have been caused by a different nuclide than the one claimed. Often, provided data is insufficient for a conclusion that a new element was definitely created and there is no other explanation for the observed effects; errors in interpreting data have been made.{{Efn|For instance, element 102 was mistakenly identified in 1957 at the Nobel Institute of Physics in [[Stockholm]], [[Stockholm County]], [[Sweden]].<ref name=RSC>{{Cite web|url=https://www.rsc.org/periodic-table/element/102/nobelium|title=Nobelium - Element information, properties and uses {{!}} Periodic Table|website=[[Royal Society of Chemistry]]|access-date=2020-03-01}}</ref> There were no earlier definitive claims of creation of this element, and the element was assigned a name by its Swedish, American, and British discoverers, ''nobelium''. It was later shown that the identification was incorrect.{{sfn|Kragh|2018|pp=38–39}} The following year, RL was unable to reproduce the Swedish results and announced instead their synthesis of the element; that claim was also disproved later.{{sfn|Kragh|2018|pp=38–39}} JINR insisted that they were the first to create the element and suggested a name of their own for the new element, ''joliotium'';{{sfn|Kragh|2018|p=40}} the Soviet name was also not accepted (JINR later referred to the naming of element 102 as "hasty").<ref name="1993 responses">{{Cite journal|year=1993|title=Responses on the report 'Discovery of the Transfermium elements' followed by reply to the responses by Transfermium Working Group|url=https://www.iupac.org/publications/pac/1993/pdf/6508x1815.pdf|url-status=live|journal=Pure and Applied Chemistry|volume=65|issue=8|pages=1815–1824|doi=10.1351/pac199365081815|archiveurl=https://web.archive.org/web/20131125223512/http://www.iupac.org/publications/pac/1993/pdf/6508x1815.pdf|archivedate=25 November 2013|access-date=7 September 2016|last1=Ghiorso|first1=A.|last2=Seaborg|first2=G. T.|authorlink2=Glenn T. Seaborg|last3=Oganessian|first3=Yu. Ts.|last4=Zvara|first4=I|last5=Armbruster|first5=P|last6=Hessberger|first6=F. P|last7=Hofmann|first7=S|last8=Leino|first8=M|last9=Munzenberg|first9=G|last10=Reisdorf|first10=W|last11=Schmidt|first11=K.-H|displayauthors=3}}</ref> The name "nobelium" remained unchanged on account of its widespread usage.<ref name=IUPAC97>{{Cite journal|doi=10.1351/pac199769122471|title=Names and symbols of transfermium elements (IUPAC Recommendations 1997)|date=1997|journal=Pure and Applied Chemistry|volume=69|pages=2471–2474|issue=12|author=Commission on Nomenclature of Inorganic Chemistry|url=http://publications.iupac.org/pac/pdf/1997/pdf/6912x2471.pdf}}</ref>}}</onlyinclude>
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