Meitnerium

Meitnerium, ₁₀₉Mt

Meitnerium
Pronunciation	/maɪtˈnɪəriəm/ [1] (myte-NEER-ee-əm) /ˈmaɪtnəriəm/ [2] (MYTE-nər-ee-əm)
Mass number	[278] (data not decisive) [a]
Meitnerium in the periodic table
Hydrogen Helium Lithium Beryllium Boron Carbon Nitrogen Oxygen Fluorine Neon Sodium Magnesium Aluminium Silicon Phosphorus Sulfur Chlorine Argon Potassium Calcium Scandium Titanium Vanadium Chromium Manganese Iron Cobalt Nickel Copper Zinc Gallium Germanium Arsenic Selenium Bromine Krypton Rubidium Strontium Yttrium Zirconium Niobium Molybdenum Technetium Ruthenium Rhodium Palladium Silver Cadmium Indium Tin Antimony Tellurium Iodine Xenon Caesium Barium Lanthanum Cerium Praseodymium Neodymium Promethium Samarium Europium Gadolinium Terbium Dysprosium Holmium Erbium Thulium Ytterbium Lutetium Hafnium Tantalum Tungsten Rhenium Osmium Iridium Platinum Gold Mercury (element) Thallium Lead Bismuth Polonium Astatine Radon Francium Radium Actinium Thorium Protactinium Uranium Neptunium Plutonium Americium Curium Berkelium Californium Einsteinium Fermium Mendelevium Nobelium Lawrencium Rutherfordium Dubnium Seaborgium Bohrium Hassium Meitnerium Darmstadtium Roentgenium Copernicium Nihonium Flerovium Moscovium Livermorium Tennessine Oganesson Ir ↑ Mt ↓ — hassium ← meitnerium → darmstadtium
Atomic number (Z)	109
Group	group 9
Period	period 7
Block	d-block
Electron configuration	[ Rn ] 5f14 6d7 7s2(predicted) [6] [7]
Electrons per shell	2, 8, 18, 32, 32, 15, 2 (predicted)
Physical properties
Phase at  STP	solid (predicted) [8]
Density (near  r.t.)	27–28 g/cm3(predicted) [9] [10]
Atomic properties
Oxidation states	common: (none) (+1), (+3), (+6) [6]
Ionization energies	1st: 800 kJ/mol 2nd: 1820 kJ/mol 3rd: 2900 kJ/mol (more)(all estimated) [6]
Atomic radius	empirical:128  pm (predicted) [6] [11]
Covalent radius	129 pm(estimated) [12]
Other properties
Natural occurrence	synthetic
Crystal structure	​ face-centered cubic (fcc) (predicted) [8]
Magnetic ordering	paramagnetic (predicted) [13]
CAS Number	54038-01-6
History
Naming	after Lise Meitner
Discovery	Gesellschaft für Schwerionenforschung (1982)
Isotopes of meitnerium v e
Main isotopes [3] Decay abun­dance half-life (t1/2) mode pro­duct 274Mt synth 0.64 s α 270Bh 276Mt synth 0.62 s α 272Bh 278Mt synth 4 s α 274Bh 282Mt synth 67 s? [5] α 278Bh
Category: Meitnerium view talk edit | references

Meitnerium is a synthetic chemical element; it has symbol Mt and atomic number 109. It is an extremely radioactive synthetic element (an element not found in nature, but can be created in a laboratory). The most stable known isotope, meitnerium-278, has a half-life of 4.5 seconds, although the unconfirmed meitnerium-282 may have a longer half-life of 67 seconds. The element was first synthesized in August 1982 by the GSI Helmholtz Centre for Heavy Ion Research near Darmstadt, Germany, and it was named after Lise Meitner in 1997.

In the periodic table, meitnerium is a d-block transactinide element. It is a member of the 7th period and is placed in the group 9 elements, although no chemical experiments have yet been carried out to confirm that it behaves as the heavier homologue to iridium in group 9 as the seventh member of the 6d series of transition metals. Meitnerium is calculated to have properties similar to its lighter homologues, cobalt, rhodium, and iridium.

Introduction

This section is an excerpt from Superheavy element § Introduction.[ edit ]

Synthesis of superheavy nuclei

A graphic depiction of a nuclear fusion reaction. Two nuclei fuse into one, emitting a neutron. Reactions that created new elements to this moment were similar, with the only possible difference that several singular neutrons sometimes were released, or none at all.

A superheavy ^[b] atomic nucleus is created in a nuclear reaction that combines two other nuclei of unequal size ^[c] into one; roughly, the more unequal the two nuclei in terms of mass, the greater the possibility that the two react. ^[19] The material made of the heavier nuclei is made into a target, which is then bombarded by the beam of lighter nuclei. Two nuclei can only fuse into one if they approach each other closely enough; normally, nuclei (all positively charged) repel each other due to electrostatic repulsion. The strong interaction can overcome this repulsion but only within a very short distance from a nucleus; beam nuclei are thus greatly accelerated in order to make such repulsion insignificant compared to the velocity of the beam nucleus. ^[20] The energy applied to the beam nuclei to accelerate them can cause them to reach speeds as high as one-tenth of the speed of light. However, if too much energy is applied, the beam nucleus can fall apart. ^[20]

Coming close enough alone is not enough for two nuclei to fuse: when two nuclei approach each other, they usually remain together for about 10⁻²⁰ seconds and then part ways (not necessarily in the same composition as before the reaction) rather than form a single nucleus. ^{[20] [21]} This happens because during the attempted formation of a single nucleus, electrostatic repulsion tears apart the nucleus that is being formed. ^[20] Each pair of a target and a beam is characterized by its cross section—the probability that fusion will occur if two nuclei approach one another expressed in terms of the transverse area that the incident particle must hit in order for the fusion to occur. ^[d] This fusion may occur as a result of the quantum effect in which nuclei can tunnel through electrostatic repulsion. If the two nuclei can stay close past that phase, multiple nuclear interactions result in redistribution of energy and an energy equilibrium. ^[20]

External videos
Visualization of unsuccessful nuclear fusion, based on calculations from the Australian National University [23]

The resulting merger is an excited state ^[24] —termed a compound nucleus—and thus it is very unstable. ^[20] To reach a more stable state, the temporary merger may fission without formation of a more stable nucleus. ^[25] Alternatively, the compound nucleus may eject a few neutrons, which would carry away the excitation energy; if the latter is not sufficient for a neutron expulsion, the merger would produce a gamma ray. This happens in about 10⁻¹⁶ seconds after the initial nuclear collision and results in creation of a more stable nucleus. ^[25] The definition by the IUPAC/IUPAP Joint Working Party (JWP) states that a chemical element can only be recognized as discovered if a nucleus of it has not decayed within 10⁻¹⁴ seconds. This value was chosen as an estimate of how long it takes a nucleus to acquire electrons and thus display its chemical properties. ^{[26] [e]}

Decay and detection

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. ^[28] In the separator, the newly produced nucleus is separated from other nuclides (that of the original beam and any other reaction products) ^[f] and transferred to a 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. ^[28] The transfer takes about 10⁻⁶ seconds; in order to be detected, the nucleus must survive this long. ^[31] The nucleus is recorded again once its decay is registered, and the location, the energy, and the time of the decay are measured. ^[28]

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 nucleons (protons and neutrons) weakens. At the same time, the nucleus is torn apart by electrostatic repulsion between protons, and its range is not limited. ^[32] Total binding energy provided by the strong interaction increases linearly with the number of nucleons, whereas electrostatic repulsion increases with the square of the atomic number, i.e. the latter grows faster and becomes increasingly important for heavy and superheavy nuclei. ^{[33] [34]} Superheavy nuclei are thus theoretically predicted ^[35] and have so far been observed ^[36] to predominantly decay via decay modes that are caused by such repulsion: alpha decay and spontaneous fission. ^[g] Almost all alpha emitters have over 210 nucleons, ^[38] and the lightest nuclide primarily undergoing spontaneous fission has 238. ^[39] In both decay modes, nuclei are inhibited from decaying by corresponding energy barriers for each mode, but they can be tunneled through. ^{[33] [34]}

Scheme of an apparatus for creation of superheavy elements, based on the Dubna Gas-Filled Recoil Separator set up in the Flerov Laboratory of Nuclear Reactions in JINR. The trajectory within the detector and the beam focusing apparatus changes because of a dipole magnet in the former and quadrupole magnets in the latter.

Alpha particles are commonly produced in radioactive decays because the mass of an alpha particle per nucleon is small enough to leave some energy for the alpha particle to be used as kinetic energy to leave the nucleus. ^[41] Spontaneous fission is caused by electrostatic repulsion tearing the nucleus apart and produces various nuclei in different instances of identical nuclei fissioning. ^[34] As the atomic number increases, spontaneous fission rapidly becomes more important: spontaneous fission partial half-lives decrease by 23 orders of magnitude from uranium (element 92) to nobelium (element 102), ^[42] and by 30 orders of magnitude from thorium (element 90) to fermium (element 100). ^[43] The earlier liquid drop model thus suggested that spontaneous fission would occur nearly instantly due to disappearance of the fission barrier for nuclei with about 280 nucleons. ^{[34] [44]} The later nuclear shell model suggested that nuclei with about 300 nucleons would form an island of stability in which nuclei will be more resistant to spontaneous fission and will primarily undergo alpha decay with longer half-lives. ^{[34] [44]} Subsequent discoveries suggested that the predicted island might be further than originally anticipated; they also showed that nuclei intermediate between the long-lived actinides and the predicted island are deformed, and gain additional stability from shell effects. ^[45] Experiments on lighter superheavy nuclei, ^[46] as well as those closer to the expected island, ^[42] have shown greater than previously anticipated stability against spontaneous fission, showing the importance of shell effects on nuclei. ^[h]

Alpha decays are registered by the emitted alpha particles, and the decay products are easy to determine before the actual decay; if such a decay or a series of consecutive decays produces a known nucleus, the original product of a reaction can be easily determined. ^[i] (That all decays within a decay chain were indeed related to each other is established by the location of these decays, which must be in the same place.) ^[28] The known nucleus can be recognized by the specific characteristics of decay it undergoes such as decay energy (or more specifically, the kinetic energy of the emitted particle). ^[j] Spontaneous fission, however, produces various nuclei as products, so the original nuclide cannot be determined from its daughters. ^[k]

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. ^[l]

History

Meitnerium was named after the physicist Lise Meitner, one of the discoverers of nuclear fission.

Discovery

Meitnerium was first synthesized on August 29, 1982, by a German research team led by Peter Armbruster and Gottfried Münzenberg at the Institute for Heavy Ion Research (Gesellschaft für Schwerionenforschung) in Darmstadt. ^[57] The team bombarded a target of bismuth-209 with accelerated nuclei of iron-58 and detected a single atom of the isotope meitnerium-266: ^[58]

²⁰⁹
₈₃Bi
+ ⁵⁸
₂₆Fe
→ ²⁶⁶
₁₀₉Mt
+
n

This work was confirmed three years later at the Joint Institute for Nuclear Research at Dubna (then in the Soviet Union). ^[58]

Naming

Using Mendeleev's nomenclature for unnamed and undiscovered elements, meitnerium should be known as eka-iridium . In 1979, during the Transfermium Wars (but before the synthesis of meitnerium), IUPAC published recommendations according to which the element was to be called unnilennium (with the corresponding symbol of Une), ^[59] a systematic element name as a placeholder, until the element was discovered (and the discovery then confirmed) and a permanent name was decided on. Although widely used in the chemical community on all levels, from chemistry classrooms to advanced textbooks, the recommendations were mostly ignored among scientists in the field, who either called it "element 109", with the symbol of E109, (109) or even simply 109, or used the proposed name "meitnerium". ^[6]

The naming of meitnerium was discussed in the element naming controversy regarding the names of elements 104 to 109, but meitnerium was the only proposal and thus was never disputed. ^{[60] [61]} The name meitnerium (Mt) was suggested by the GSI team in September 1992 in honor of the Austrian physicist Lise Meitner, a co-discoverer of protactinium (with Otto Hahn), ^{[62] [63] [64] [65] [66]} and one of the discoverers of nuclear fission. ^[67] In 1994 the name was recommended by IUPAC, ^[60] and was officially adopted in 1997. ^[61] It is thus the only element named specifically after a non-mythological woman (curium being named for both Pierre and Marie Curie). ^[68]

Isotopes

Main article: Isotopes of meitnerium

Meitnerium has no stable or naturally occurring isotopes. Several radioactive isotopes have been synthesized in the laboratory, either by fusing two atoms or by observing the decay of heavier elements. Eight different isotopes of meitnerium have been reported with mass numbers 266, 268, 270, and 274–278, two of which, meitnerium-268 and meitnerium-270, have unconfirmed metastable states. A ninth isotope with mass number 282 is unconfirmed. Most of these decay predominantly through alpha decay, although some undergo spontaneous fission. ^[69]

Stability and half-lives

List of meitnerium isotopes

• v
• t
• e

Isotope	Half-life [m]		Decay mode	Discovery year	Discovery reaction
	Value	ref
266Mt	2.0 ms	[3]	α, SF	1982	209Bi(58Fe,n)
268Mt	23 ms	[3]	α	1994	272Rg(—,α)
270Mt	800 ms	[3]	α	2004	278Nh(—,2α)
274Mt	640 ms	[4]	α	2006	282Nh(—,2α)
275Mt	20 ms	[4]	α	2003	287Mc(—,3α)
276Mt	620 ms	[4]	α	2003	288Mc(—,3α)
277Mt	5 ms	[70]	SF	2012	293Ts(—,4α)
278Mt	4.5 s	[70]	α	2010	294Ts(—,4α)
282Mt [n]	1.1 min	[5]	α	1998	290Fl(e−,νe2α)

All meitnerium isotopes are extremely unstable and radioactive; in general, heavier isotopes are more stable than the lighter. The most stable known meitnerium isotope, ²⁷⁸Mt, is also the heaviest known; it has a half-life of 4.5 seconds. The unconfirmed ²⁸²Mt is even heavier and appears to have a longer half-life of 67 seconds. With a half-life of 0.8 seconds, the next most stable known isotope is ²⁷⁰Mt. ^[3] The isotopes ²⁷⁶Mt and ²⁷⁴Mt have half-lives of 0.62 and 0.64 seconds respectively. ^[4]

The isotope ²⁷⁷Mt, created as the final decay product of ²⁹³Ts for the first time in 2012, was observed to undergo spontaneous fission with a half-life of 5 milliseconds. Preliminary data analysis considered the possibility of this fission event instead originating from ²⁷⁷Hs, for it also has a half-life of a few milliseconds, and could be populated following undetected electron capture somewhere along the decay chain. ^{[71] [72]} This possibility was later deemed very unlikely based on observed decay energies of ²⁸¹Ds and ²⁸¹Rg and the short half-life of ²⁷⁷Mt, although there is still some uncertainty of the assignment. ^[72] Regardless, the rapid fission of ²⁷⁷Mt and ²⁷⁷Hs is strongly suggestive of a region of instability for superheavy nuclei with N  = 168–170. The existence of this region, characterized by a decrease in fission barrier height between the deformed shell closure at N = 162 and spherical shell closure at N = 184, is consistent with theoretical models. ^[71]

Predicted properties

Other than nuclear properties, no properties of meitnerium or its compounds have been measured; this is due to its extremely limited and expensive production ^[o] and the fact that meitnerium and its parents decay very quickly. Properties of meitnerium metal remain unknown and only predictions are available.

Chemical

Meitnerium is the seventh member of the 6d series of transition metals, and should be much like the platinum group metals. ^[65] Calculations on its ionization potentials and atomic and ionic radii are similar to that of its lighter homologue iridium, thus implying that meitnerium's basic properties will resemble those of the other group 9 elements, cobalt, rhodium, and iridium. ^[6]

Prediction of the probable chemical properties of meitnerium has not received much attention recently. Meitnerium is expected to be a noble metal. The standard electrode potential for the Mt³⁺/Mt couple is expected to be 0.8 V. Based on the most stable oxidation states of the lighter group 9 elements, the most stable oxidation states of meitnerium are predicted to be the +6, +3, and +1 states, with the +3 state being the most stable in aqueous solutions. In comparison, rhodium and iridium show a maximum oxidation state of +6, while the most stable states are +4 and +3 for iridium and +3 for rhodium. ^[6] The oxidation state +9, represented only by iridium in [IrO₄]⁺, might be possible for its congener meitnerium in the nonafluoride (MtF₉) and the [MtO₄]⁺ cation, although [IrO₄]⁺ is expected to be more stable than these meitnerium compounds. ^[74] The tetrahalides of meitnerium have also been predicted to have similar stabilities to those of iridium, thus also allowing a stable +4 state. ^[75] It is further expected that the maximum oxidation states of elements from bohrium (element 107) to darmstadtium (element 110) may be stable in the gas phase but not in aqueous solution. ^[6]

Physical and atomic

Meitnerium is expected to be a solid under normal conditions and assume a face-centered cubic crystal structure, similarly to its lighter congener iridium. ^[8] It should be a very heavy metal with a density of around 27–28 g/cm³, which would be among the highest of any of the 118 known elements. ^{[9] [10]} Meitnerium is also predicted to be paramagnetic. ^[13]

Theoreticians have predicted the covalent radius of meitnerium to be 6 to 10 pm larger than that of iridium. ^[76] The atomic radius of meitnerium is expected to be around 128 pm. ^[11]

Experimental chemistry

Meitnerium is the first element on the periodic table whose chemistry has not yet been investigated. Unambiguous determination of the chemical characteristics of meitnerium has yet to have been established ^{[77] [78]} due to the short half-lives of meitnerium isotopes ^[6] and a limited number of likely volatile compounds that could be studied on a very small scale. One of the few meitnerium compounds that are likely to be sufficiently volatile is meitnerium hexafluoride (MtF
_⁶), as its lighter homologue iridium hexafluoride (IrF
_⁶) is volatile above 60 °C and therefore the analogous compound of meitnerium might also be sufficiently volatile; ^[65] a volatile octafluoride (MtF
_⁸) might also be possible. ^[6] For chemical studies to be carried out on a transactinide, at least four atoms must be produced, the half-life of the isotope used must be at least 1 second, and the rate of production must be at least one atom per week. ^[65] Even though the half-life of ²⁷⁸Mt, the most stable confirmed meitnerium isotope, is 4.5 seconds, long enough to perform chemical studies, another obstacle is the need to increase the rate of production of meitnerium isotopes and allow experiments to carry on for weeks or months so that statistically significant results can be obtained. Separation and detection must be carried out continuously to separate out the meitnerium isotopes and have automated systems experiment on the gas-phase and solution chemistry of meitnerium, as the yields for heavier elements are predicted to be smaller than those for lighter elements; some of the separation techniques used for bohrium and hassium could be reused. However, the experimental chemistry of meitnerium has not received as much attention as that of the heavier elements from copernicium to livermorium. ^{[6] [77] [79]}

The Lawrence Berkeley National Laboratory attempted to synthesize the isotope ²⁷¹Mt in 2002–2003 for a possible chemical investigation of meitnerium, because it was expected that it might be more stable than nearby isotopes due to having 162 neutrons, a magic number for deformed nuclei; its half-life was predicted to be a few seconds, long enough for a chemical investigation. ^{[6] [80] [81]} However, no atoms of ²⁷¹Mt were detected; ^[82] this isotope of meitnerium is currently unknown. ^[69]

An experiment determining the chemical properties of a transactinide would need to compare a compound of that transactinide with analogous compounds of some of its lighter homologues: ^[6] for example, in the chemical characterization of hassium, hassium tetroxide (HsO₄) was compared with the analogous osmium compound, osmium tetroxide (OsO₄). ^[83] In a preliminary step towards determining the chemical properties of meitnerium, the GSI attempted sublimation of the rhodium compounds rhodium(III) oxide (Rh₂O₃) and rhodium(III) chloride (RhCl₃). However, macroscopic amounts of the oxide would not sublimate until 1000 °C and the chloride would not until 780 °C, and then only in the presence of carbon aerosol particles: these temperatures are far too high for such procedures to be used on meitnerium, as most of the current methods used for the investigation of the chemistry of superheavy elements do not work above 500 °C. ^[78]

Following the 2014 successful synthesis of seaborgium hexacarbonyl, Sg(CO)₆, ^[84] studies were conducted with the stable transition metals of groups 7 through 9, suggesting that carbonyl formation could be extended to further probe the chemistries of the early 6d transition metals from rutherfordium to meitnerium inclusive. ^{[85] [86]} Nevertheless, the challenges of low half-lives and difficult production reactions make meitnerium difficult to access for radiochemists, though the isotopes ²⁷⁸Mt and ²⁷⁶Mt are long-lived enough for chemical research and may be produced in the decay chains of ²⁹⁴ Ts and ²⁸⁸ Mc respectively. ²⁷⁶Mt is likely more suitable, since producing tennessine requires a rare and rather short-lived berkelium target. ^[87] The isotope ²⁷⁰Mt, observed in the decay chain of ²⁷⁸Nh with a half-life of 0.69 seconds, may also be sufficiently long-lived for chemical investigations, though a direct synthesis route leading to this isotope and more precise measurements of its decay properties would be required. ^[81]

Notes

1. The most stable isotope of meitnerium cannot be determined based on existing data due to uncertainty that arises from the low number of measurements. The half-life of ²⁷⁸Mt corresponding to two standard deviations is, based on existing data, 4.5+7.0
   −2.6 seconds ^[3] , whereas that of ²⁷⁴Mt is 0.64+1.52
   −0.46 seconds ^[4] ; these measurements have overlapping confidence intervals. It is also possible that the unconfirmed ²⁸²Mt is more stable than both of these, with its half-life being 67 seconds. ^[5]
2. In nuclear physics, an element is called heavy if its atomic number is high; lead (element 82) is one example of such a heavy element. The term "superheavy elements" typically refers to elements with atomic number greater than 103 (although there are other definitions, such as atomic number greater than 100 ^[14] or 112; ^[15] sometimes, the term is presented an equivalent to the term "transactinide", which puts an upper limit before the beginning of the hypothetical superactinide series). ^[16] Terms "heavy isotopes" (of a given element) and "heavy nuclei" mean what could be understood in the common language—isotopes of high mass (for the given element) and nuclei of high mass, respectively.
3. In 2009, a team at the JINR led by Oganessian published results of their attempt to create hassium in a symmetric ¹³⁶Xe + ¹³⁶Xe reaction. They failed to observe a single atom in such a reaction, putting the upper limit on the cross section, the measure of probability of a nuclear reaction, as 2.5  pb. ^[17] In comparison, the reaction that resulted in hassium discovery, ²⁰⁸Pb + ⁵⁸Fe, had a cross section of ~20 pb (more specifically, 19⁺¹⁹
   _-11 pb), as estimated by the discoverers. ^[18]
4. The amount of energy applied to the beam particle to accelerate it can also influence the value of cross section. For example, in the ²⁸
   ₁₄Si
   + ¹
   ₀n
   → ²⁸
   ₁₃Al
   + ¹
   ₁p
   reaction, cross section changes smoothly from 370 mb at 12.3 MeV to 160 mb at 18.3 MeV, with a broad peak at 13.5 MeV with the maximum value of 380 mb. ^[22]
5. This figure also marks the generally accepted upper limit for lifetime of a compound nucleus. ^[27]
6. 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. ^[29] Such separation can also be aided by a time-of-flight measurement and a recoil energy measurement; a combination of the two may allow to estimate the mass of a nucleus. ^[30]
7. Not all decay modes are caused by electrostatic repulsion. For example, beta decay is caused by the weak interaction. ^[37]
8. It was already known by the 1960s that ground states of nuclei differed in energy and shape as well as that certain magic numbers of nucleons corresponded to greater stability of a nucleus. However, it was assumed that there was no nuclear structure in superheavy nuclei as they were too deformed to form one. ^[42]
9. Since mass of a nucleus is not measured directly but is rather calculated from that of another nucleus, such measurement is called indirect. Direct measurements are also possible, but for the most part they have remained unavailable for superheavy nuclei. ^[47] The first direct measurement of mass of a superheavy nucleus was reported in 2018 at LBNL. ^[48] Mass was determined from the location of a nucleus after the transfer (the location helps determine its trajectory, which is linked to the mass-to-charge ratio of the nucleus, since the transfer was done in presence of a magnet). ^[49]
10. If the decay occurred in a vacuum, then since total momentum of an isolated system before and after the decay must be preserved, the daughter nucleus would also receive a small velocity. The ratio of the two velocities, and accordingly the ratio of the kinetic energies, would thus be inverse to the ratio of the two masses. The decay energy equals the sum of the known kinetic energy of the alpha particle and that of the daughter nucleus (an exact fraction of the former). ^[38] The calculations hold for an experiment as well, but the difference is that the nucleus does not move after the decay because it is tied to the detector.
11. Spontaneous fission was discovered by Soviet physicist Georgy Flerov, ^[50] a leading scientist at JINR, and thus it was a "hobbyhorse" for the facility. ^[51] In contrast, the LBL scientists believed fission information was not sufficient for a claim of synthesis of an element. They believed spontaneous fission had not been studied enough to use it for identification of a new element, since there was a difficulty of establishing that a compound nucleus had only ejected neutrons and not charged particles like protons or alpha particles. ^[27] They thus preferred to link new isotopes to the already known ones by successive alpha decays. ^[50]
12. For instance, element 102 was mistakenly identified in 1957 at the Nobel Institute of Physics in Stockholm, Stockholm County, Sweden. ^[52] 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. ^[53] 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. ^[53] JINR insisted that they were the first to create the element and suggested a name of their own for the new element, joliotium; ^[54] the Soviet name was also not accepted (JINR later referred to the naming of the element 102 as "hasty"). ^[55] This name was proposed to IUPAC in a written response to their ruling on priority of discovery claims of elements, signed 29 September 1992. ^[55] The name "nobelium" remained unchanged on account of its widespread usage. ^[56]
13. Different sources give different values for half-lives; the most recently published values are listed.
14. This isotope is unconfirmed
15. In the millions of dollars ^[73]

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External links

• Meitnerium Archived October 22, 2012, at the Wayback Machine at The Periodic Table of Videos (University of Nottingham)