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Nihonium-290

Main isotopes of nihonium
Iso­tope Decay
abun­dance half-life (t1/2) mode pro­duct
290Nh syn 2 s? α 286Rg
286Nh syn 8 s α 282Rg
285Nh syn 4 s α 281Rg
284Nh syn 1 s α 280Rg
EC 284Cn
283Nh syn 0.1 s α 279Rg
282Nh syn 70 ms α 278Rg
278Nh syn 1.4 ms α 274Rg

Nihonium (113Nh) is a synthetic element. Being synthetic, a standard atomic weight cannot be given and like all artificial elements, it has no stable isotopes. The first isotope to be synthesized was 284Nh as a decay product of 288Mc in 2003. The first isotope to be directly synthesized was 278Nh in 2004. There are 6 known radioisotopes from 278Nh to 286Nh, along with the unconfirmed 290Nh. The longest-lived isotope is 286Nh with a half-life of 19.6 seconds.

Super-heavy elements such as nihonium are produced by bombarding lighter elements in particle accelerators that induce fusion reactions. Whereas most of the isotopes of nihonium can be synthesized directly this way, some heavier ones have only been observed as decay products of elements with higher atomic numbers.

Depending on the energies involved, the former are separated into "hot" and "cold". In hot fusion reactions, very light, high-energy projectiles are accelerated toward very heavy targets (actinides), giving rise to compound nuclei at high excitation energy (~40–50 MeV) that may either fission or evaporate several (3 to 5) neutrons. In cold fusion reactions, the produced fused nuclei have a relatively low excitation energy (~10–20 MeV), which decreases the probability that these products will undergo fission reactions. As the fused nuclei cool to the ground state, they require emission of only one or two neutrons, and thus, allows for the generation of more neutron-rich products. The latter is a distinct concept from that of where nuclear fusion claimed to be achieved at room temperature conditions (see cold fusion).


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