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{{main|Unsepttrium}} {{main|Unsepttrium}}

=====Significance=====


The ] ] also has problems for ''Z'' > 137, for the ground state energy is The ] ] also has problems for ''Z'' > 137, for the ground state energy is

Revision as of 06:17, 16 August 2012

A period 9 element is any one of 50 hypothetical chemical elements (unhexennium through biunoctium) belonging to an eighth period of the periodic table of the elements. They may be referred to using IUPAC systematic element names. None of these elements have been synthesized, and it is possible that none have isotopes with stable enough nuclei to receive significant attention in the near future. It is also probable that, due to drip instabilities,none of the period 9 elements are physically possible and the periodic table may end soon after the island of stability at unbihexium with atomic number 126. Period 9 is likely to be the last period in the periodic table.

If it were possible to produce sufficient quantities of these elements that would allow the study of their chemistry, these elements may well behave very differently from those of previous periods. This is because their electronic configurations may be altered by quantum and relativistic effects, as the energy levels of the 6g, 7f and 8d orbitals are so close to each other that they may well exchange electrons with each other. This would result in a large number of elements in the superactinide series that would have extremely similar chemical properties that would be quite unrelated to elements of lower atomic number.

The names given to these unattested elements are all IUPAC systematic names.

History

There are currently seven periods in the periodic table of chemical elements, culminating with atomic number 118. If further elements with higher atomic numbers than this are discovered, they will be placed in additional periods (likely 8 and 9), laid out (as with the existing periods) to illustrate periodically recurring trends in the properties of the elements concerned. Any additional periods are expected to contain a larger number of elements than the seventh period, as they are calculated to have an additional so-called g-block, containing 18 elements with partially filled g-orbitals in each period. An eight-period table containing this block was suggested by Glenn T. Seaborg in 1969. While Seaborg's version of the extended period had the heavier elements following the pattern set by lighter elements, other models do not. Pekka Pyykkö, for example, used computer modeling to calculate the positions of elements up to Z = 172, and found that several were displaced from the Madelung rule.

Elements

Period 9 is divided into five blocks, and it is the second period that includes the g-block; however, spin-orbit coupling effects reduce the validity of the orbital approximation substantially for elements of high atomic number.

169
Uhe
170
Usn
171
Usu
172
Usb
173
Ust
174
Usq
175
Usp
176
Ush
177
Uss
178
Uso
179
Use
180
Uon
181
Uou
182
Uob
183
Uot
184
Uoq
185
Uop
186
Uoh
187
Uos
188
Uoo
189
Uoe
190
Uen
191
Ueu
192
Ueb
193
Uet
194
Ueq
195
Uep
196
Ueh
197
Ues
198
Ueo
199
Uee
200
Bnn
201
Bnu
202
Bnb
203
Bnt
204
Bnq
205
Bnp
206
Bnh
207
Bns
208
Bno
209
Bne
210
Bun
211
Buu
212
Bub
213
But
214
Buq
215
Bup
216
Buh
217
Bus
218
Buo

Attempts at synthesis

No synthesis has been attempted for period 9 elements.

Groups of elements

Main articles: Eka-Superactinide and g-block

Period 9 is the second period to have g-block elements, which have atomic numbers from 171 onwards, but it is not clear when the filling of the 6g subshell ends. These elements belong to the chemical series of eka-superactinides, characterised by the filling of the 6g and 7f subshells, and they could therefore have different chemical properties that are reminiscent of the actinides; however, the proximity of the 6g and 7f subshells and the small gap between them and the 8d and 9p subshells could lead to a large number of elements whose properties are independent of their position in the periodic table.

The period 9 elements are likely to be too unstable to be detected.

Unsepttrium

Main article: Unsepttrium
Significance

The relativistic Dirac equation also has problems for Z > 137, for the ground state energy is

E = m c 2 1 Z 2 α 2 {\displaystyle E=mc^{2}{\sqrt {1-Z^{2}\alpha ^{2}}}}

where m is the rest mass of the electron. For Z > 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 Klein paradox.

More accurate calculations including the effects of the finite size of the nucleus indicate that the binding energy first exceeds 2mc for Z > Zcr ≈ 173. For Z > Zcr, if the innermost orbital is not filled, the electric field of the nucleus will pull an electron out of the vacuum, resulting in the spontaneous emission of a positron.

f-block elements

Main article: Superactinide

The relativstic and quantum effects for the electron clouds of these elements are expected to be even greater than those for the g-block elements, because these elements have higher atomic number. If these elements could actually be observed, they would likely be observed to have similar chemical properties, but the effect of the closeness of the 6g and 7f (and possibly also the 8d and 9p) subshells is unclear and difficult to predict because of the relativistic and quantum effects. These orbitals, being so close in energy, may fill together all at the same time, resulting in a series of very similar elements with many barely distinguishable oxidation states. The basis of periodic trends based on electron configurations may thus no longer hold.

The existence of such atoms is probably theoretically possible as the upper limit for atomic number is likely Z = 173 due to the light-speed limit, after which assigning electron shells would be nonsensical and elements would only be able to exist as ions, but it is not clear if our technology will ever be enough to synthesise them.

d-block and p-block elements

Although element 203 would likely be taken to be the last eka-superactinide based on previous periods, the electron configurations for the d-block and p-block period 9 elements would likely be nothing more than mathematical extrapolation because of the extreme quantum and relativistic effects the electron clouds will experience. In the unlikely case that their chemical properties may eventually be studied, it is likely that all existing classifications will be inadequate to describe them. Due to the breakdown of periodic trends expected in this region due to the closeness of energy of the 6g, 7f, 8d and 9p orbitals and other relativistic effects, it seems likely that the properties and placement in the periodic table of these elements may be of only formal significance.

Characteristics

No period 9 element has been synthesized.

Chemical

Periodic trends may not continue to hold at such high atomic number, and in fact may already break down in the late seventh period. For example, chemical studies performed in 2007 indicate that flerovium may possess some non-eka-lead properties and may behave as the first superheavy element that portrays some noble-gas-like properties due to relativistic effects.

Physical and atomic

Isotopes

Isotopes of period 9 elements may contain more than 220 neutrons, such as Ust. Mass numbers will be in the 400s (and probably also the 500s).

Electron configurations

Chemical element Chemical series Electron configuration
169 Uhe Unhexennium Alkali metal 9s
170 Usn Unseptnilium Alkaline earth metal 9s
171 Usu Unseptunium Superactinide 9s 6g
172 Usb Unseptbium Superactinide 9s 6g
173 Ust Unsepttrium Superactinide 9s 6g
174 Usq Unseptquadium Superactinide 9s 6g
175 Usp Unseptpentium Superactinide 9s 6g
176 Ush Unsepthexium Superactinide 9s 6g
177 Uss Unseptseptium Superactinide 9s 6g
178 Uso Unseptoctium Superactinide 9s 6g
179 Use Unseptennium Superactinide 9s 6g
180 Uon Unoctnilium Superactinide 9s 6g
181 Uou Unoctunium Superactinide 9s 6g
182 Uob Unoctbium Superactinide 9s 6g
183 Uot Unocttrium Superactinide 9s 6g
184 Uoq Unoctquadium Superactinide 9s 6g
185 Uop Unoctpentium Superactinide 9s 6g
186 Uoh Unocthexium Superactinide 9s 6g
187 Uos Unoctseptium Superactinide 9s 6g
188 Uoo Unoctoctium Superactinide 9s 6g
189 Uoe Unoctennium Superactinide 9s 7f 6g
190 Uen Unennilium Superactinide 9s 7f 6g
191 Ueu Unennunium Superactinide 9s 7f 6g
192 Ueb Unennbium Superactinide 9s 7f 6g
193 Uet Unenntrium Superactinide 9s 7f 6g
194 Ueq Unennquadium Superactinide 9s 7f 6g
195 Uep Unennpentium Superactinide 9s 7f 6g
196 Ueh Unennhexium Superactinide 9s 7f 6g
197 Ues Unennseptium Superactinide 9s 7f 6g
198 Ueo Unennoctium Superactinide 9s 7f 6g
199 Uee Unennennium Superactinide 9s 7f 6g
200 Bnn Binilnilium Superactinide 9s 7f 6g
201 Bnu Binilunium Superactinide 9s 6f 6g
202 Bnb Binilbium Superactinide 9s 6f 6g
203 Bnt Biniltrium Superactinide 9s 8d 7f 6g
204 Bnq Binilquadium Transition metal 9s 8d 7f 6g
205 Bnp Binilpentium Transition metal 9s 8d 7f 6g
206 Bnh Binilhexium Transition metal 9s 8d 7f 6g
207 Bns Binilseptium Transition metal 9s 8d 7f 6g
208 Bno Biniloctium Transition metal 9s 8d 7f 6g
209 Bne Binilennium Transition metal 9s 8d 7f 6g
210 Bun Biunnilium Transition metal 9s 8d 7f 6g
211 Buu Biununium Transition metal 9s 8d 7f 6g
212 Bub Biunbium Transition metal 9s 8d 7f 6g
213 But Biuntrium Post-transition metal 9s 9p 8d 7f 6g
214 Buq Biunquadium Post-transition metal 9s 9p 8d 7f 6g
215 Bup Biunpentium Post-transition metal 9s 9p 8d 7f 6g
216 Buh Biunhexium Post-transition metal 9s 9p 8d 7f 6g
217 Bus Biunseptium Halogen 9s 9p 8d 7f 6g
218 Buo Biunoctium Noble gas 9s 9p 8d 7f 6g

See also

Notes

  1. The heaviest element that has been synthesized to date is ununoctium with atomic number 118, which is the last period 7 element.

References

  1. ^ Seaborg (ca. 2006). "transuranium element (chemical element)". Encyclopædia Britannica. Retrieved 2010-03-16. {{cite web}}: Check date values in: |date= (help)
  2. ^ "Extended elements: new periodic table". 2010.
  3. J.D. Bjorken, S.D. Drell (1964). Relativistic Quantum Mechanics. McGraw-Hill.
  4. W. Greiner, S. Schramm (2008). "American Journal of Physics". 76: 509. {{cite journal}}: Cite journal requires |journal= (help), and references therein.
  5. Walter Greiner and Stefan Schramm (2008). "Resource Letter QEDV-1: The QED vacuum". American Journal of Physics. 76 (6): 509. Bibcode:2008AmJPh..76..509G. doi:10.1119/1.2820395., and references therein.
  6. Cite error: The named reference LBNL was invoked but never defined (see the help page).
  7. Gas Phase Chemistry of Superheavy Elements, lecture by Heinz W. Gäggeler, Nov. 2007. Last accessed on Dec. 12, 2008.
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