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{{Infobox untriseptium}}
'''Untriseptium''' ({{IPAc-en|icon|ˌ|uː|n|t|r|aɪ|ˈ|s|ɛ|p|t|i|əm}}), also known as ''']-]'''{{Citation needed|date=February 2012}} or element 137, is a hypothetical ] which has not been observed to occur naturally, nor has it yet been synthesised. Due to ], it is not known if this element is physically possible, as the drip instabilities may imply that the periodic table ends soon after the ] at ]. <ref name=EB>{{cite web|author=Seaborg, G. T.|url=http://www.britannica.com/EBchecked/topic/603220/transuranium-element|title=transuranium element (chemical element)|publisher=Encyclop&aelig;dia Britannica|date=ca. 2006|accessdate=2010-03-16}}</ref><ref>{{ cite journal|first1=S. |last1=Cwiok|first2= P.-H.|last2= Heenen |first3= W.|last3= Nazarewicz |year=2005|title=Shape coexistence and triaxiality in the superheavy nuclei|journal=Nature|volume=433| page= 705|bibcode = 2005Natur.433..705C |doi = 10.1038/nature03336|issue=7027 |pmid=15716943|pages=705–9}}</ref> Its atomic number is 137 and symbol is Uts.


{{Redirect category shell|1=
The name ''untriseptium'' is a temporary ] ].
{{R with Wikidata item}}
{{R with possibilities}}
{{R from subtopic}}
{{R adr|Superactinides}}
{{R printworthy}}
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]
==Synthesis==

===Target-projectile combinations leading to Z=137 compound nuclei

{|class="wikitable" style="text-align:center"
|-
! Target !! Projectile !! CN !! Attempt result
|-
!<sup>208</sup>Pb
|<sup>137</sup>Cs||<sup>345</sup>Uts||{{unk|Reaction yet to be attempted}}
|-
!<sup>209</sup>Bi
|<sup>136</sup>Xe||<sup>345</sup>Uts||{{unk|Reaction yet to be attempted}}
|-
!<sup>228</sup>Ra
|<sup>115</sup>In||<sup>343</sup>Uts||{{unk|Reaction yet to be attempted}}
|-
!<sup>227</sup>Ac
|<sup>116</sup>Cd||<sup>343</sup>Uts||{{unk|Reaction yet to be attempted}}
|-
!<sup>232</sup>Th
|<sup>109</sup>Ag||<sup>341</sup>Uts||{{unk|Reaction yet to be attempted}}
|-
!<sup>231</sup>Pa
|<sup>106</sup>Pd||<sup>337</sup>Uts||{{unk|Reaction yet to be attempted}}
|-
!<sup>238</sup>U
|<sup>103</sup>Rh||<sup>341</sup>Uts||{{unk|Reaction yet to be attempted}}
|-
!<sup>237</sup>Np
|<sup>104</sup>Ru||<sup>341</sup>Uts||{{unk|Reaction yet to be attempted}}
|-
!<sup>244</sup>Pu
|<sup>99</sup>Tc||<sup>343</sup>Uts||{{unk|Reaction yet to be attempted}}
|-
!<sup>243</sup>Am
|<sup>100</sup>Mo||<sup>343</sup>Uts||{{unk|Reaction yet to be attempted}}
|-
!<sup>250</sup>Cm
|<sup>93</sup>Nb||<sup>343</sup>Uts||{{unk|Reaction yet to be attempted}}
|-
!<sup>249</sup>Bk
|<sup>96</sup>Zr||<sup>345</sup>Uts||{{unk|Reaction yet to be attempted}}
|-
!<sup>252</sup>Cf
|<sup>89</sup>Y||<sup>341</sup>Uts||{{unk|Reaction yet to be attempted}}
|-
!<sup>254</sup>Es
|<sup>88</sup>Sr||<sup>342</sup>Uts||{{unk|Reaction yet to be attempted}}
|-
!<sup>257</sup>Fm
|<sup>87</sup>Rb||<sup>344</sup>Uts||{{unk|Reaction yet to be attempted}}
|-
!<sup>258</sup>Md
|<sup>86</sup>Kr||<sup>344</sup>Uts||{{unk|Reaction yet to be attempted}}
|-
!<sup>259</sup>No
|<sup>81</sup>Br||<sup>340</sup>Uts||{{unk|Reaction yet to be attempted}}
|-
!<sup>262</sup>Lr
|<sup>82</sup>Se||<sup>344</sup>Uts||{{unk|Reaction yet to be attempted}}
|-
!<sup>267</sup>Rf
|<sup>75</sup>As||<sup>342</sup>Uts||{{unk|Reaction yet to be attempted}}
|-
!<sup>268</sup>Db
|<sup>76</sup>Ge||<sup>344</sup>Uts||{{unk|Reaction yet to be attempted}}
|-
!<sup>271</sup>Sg
|<sup>71</sup>Ga||<sup>342</sup>Uts||{{unk|Reaction yet to be attempted}}
|-
!<sup>274</sup>Bh
|<sup>70</sup>Zn||<sup>344</sup>Uts||{{unk|Reaction yet to be attempted}}
|-
|}

== Significance ==
Untriseptium is sometimes called '''feynmanium''' (symbol Fy) because ] noted<ref>
{{cite web
|first=G.|last= Elert
|date=
|title=Atomic Models
|url=http://physics.info/atomic-models/
|work=The Physics Hypertextbook
|accessdate=2009-10-09
}}</ref> that a simplistic interpretation of the ] ] runs into problems with electron orbitals at ''Z'' > 1/α = 137, suggesting that neutral atoms cannot exist beyond untriseptium, and that a periodic table of elements based on electron orbitals therefore breaks down at this point. However, a more rigorous analysis calculates the limit to be ''Z'' ≈ 173.<ref name=Greiner>{{cite journal|author=Walter Greiner and Stefan Schramm|title=Resource Letter QEDV-1: The QED vacuum|journal=American Journal of Physics|volume=76|page=509|year=2008|doi=10.1119/1.2820395|bibcode = 2008AmJPh..76..509G|issue=6 }}, and references therein.</ref>

=== Bohr model breakdown {{Anchor|Bohr model}} ===
The ] exhibits difficulty for atoms with atomic number greater than 137, for the speed of an electron in a ], ''v'', is given by

:<math>v = Z \alpha c \approx \frac{Z c}{137.036}</math>

where ''Z'' is the ], and ''α'' is the ], a measure of the strength of electromagnetic interactions.<ref>{{cite book
|first1=R. |last1=Eisberg|first2= R.|last2= Resnick
|year=1985
|title=Quantum Physics of Atoms, Molecules, Solids, Nuclei and Particles
|publisher=]
|isbn=
}}</ref> Under this approximation, any element with an atomic number of greater than 137 would require 1s electrons to be traveling faster than ''c'', the ]. Hence the non-relativistic Bohr model is clearly inaccurate when applied to such an element.

=== The Dirac equation ===
The ] ] also has problems for ''Z''&nbsp;>&nbsp;137, for the ground state energy is

:<math>E=m c^2 \sqrt{1-Z^2 \alpha^2}</math>

where ''m'' is the rest mass of the electron. For ''Z''&nbsp;>&nbsp;137, the wave function of the Dirac ground state is oscillatory, rather than bound, and there is no gap between the positive and negative energy spectra, as in the ].<ref>
{{cite book
|first1=J. D.|last1= Bjorken|first2=S. D.|last2= Drell
|year=1964
|title=Relativistic Quantum Mechanics
|publisher=]
|isbn=
}}</ref>

More accurate calculations including the effects of the finite size of the nucleus indicate that the binding energy first exceeds 2''mc''<sup>2</sup> for ''Z''&nbsp;>&nbsp;''Z''<sub>cr</sub>&nbsp;≈&nbsp;173. For ''Z''&nbsp;>&nbsp;''Z''<sub>cr</sub>, if the innermost orbital is not filled, the electric field of the nucleus will pull an electron out of the vacuum, resulting in the ].<ref>
{{cite journal
|first1=W. |last1=Greiner|first2= S. |last2=Schramm
|year=2008
|title=]
|volume=76 |pages=509
|doi=
}}, and references therein.</ref>

==See also==
* ]
* ] &ndash; ]
* ]
* ]

== References ==
{{Reflist}}

{{Compact extended periodic table}}

]
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Latest revision as of 04:14, 2 February 2023

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