Unquadennium, Uqe, is the temporary name for element 149. Isotopes are predicted for 477Uqe to 475Uqe. and for 471Uqe to 416Uqe. Reported half-lives are all less than 1 hr, and most are under 1 sec. Thirteen isotopes in the band 456Uqe to 435Uqe can form. Beyond the region for which predictions are available, 535Uqe is likely, and may form. 440Uqe and 438Uqe are expected to persist slightly more than 2 days after the event which led to their formation, while 435Uqe is expected to persist for somewhat less than 2 days. All other Uqe isotopes are expected to vanish within 1000 sec.
NUCLEAR PROPERTIES
Between Z = 175 and Z near 130, one set of predictions for half-life and principal decay mode has been published(1). Ref. 1 is publicly available and can be found via a search by paper title. Anyone interested in this element should study pp 15 and 18, which allow a given element to be understood in the context of adjacent nuclides.
These data are limited to nuclides for which N <= 333. Half-lives are presented in bands covering 3 orders of magnitude (0.001 sec to 1 sec, for instance) and are accurate to within +/- 3 orders of magnitude, which seems rather crude until the enormous extrapolation from what is known is taken into account, Minimum half-life is set at 10-09 sec, rather than 10-14 sec; which introduces a little uncertainty, but not a great deal because fission half-lives tend to transition quickly from values well above 10-09 sec to values well below 10-14 sec; and, while alpha-decay half-lives change more slowly, alpha emission is rarely dominant except where fission is suppressed. Significantly, beta-decay half-lives do not decline far below 10-03 sec, even for highly energetic decays, so there is little uncertainty about neutron-rich nuclides.
Ref. 1 does have one significant weakness. Nuclides which are beta-stable are identified by black squares, overwriting decay mode and half-life information. In many cases, these data can be estimated from adjacent nuclides.
No predictions exist for N > 333. The liquid-drop sketch developed in "The Final Element" (this wiki) for Z = 176 and above can be used to guess at where nuclides with Z < 175 and N > 333 may exist. Probability criteria for this purpose were set in "Nuclear Guesswork" (this wiki). Below Z = 171, it is necessary to look only at nuclear drops which are not expected to decay by neutron emission and require only normal amounts of structural correction energy in order to suppress spontaneous fission.
PREDICTED PROPERTIES
Ref. 1 predicts isotopes ranging from 477Uqe to 416Uqe. Format used to display isotope properties is: isotope(s); half-life in seconds; dominant decay mode; comments.
477Uqe - 468Uqe; <10-06; fission.
467Uqe - 466Uqe; 0.001 - 1; fission. A fission half-life this long is plausible only if there is a shell closure at N = 318(2). It is too far above N = 308 for stabilization against fission. Beta decay seems more likely.
465Uqe - 442Uqe; 0.001 - 1; beta.
441Uqe - 439Uqe; 1 - 1000; fission. Ref 1 predicts a band of fission-decaying nuclides with N between 285 and 295. It appears to be possible for structure to destabilize a nuclide(3), so short partial half-lives against fission in this region are plausible.
438Uqe; 0.001 - 1; fission. Half-life is probably close to 1 second.
437Uqe; 1 - 1000; alpha. Fission is probably a competing decay mode.
436Uqe - 435Uqe; 1 - 1000; fission. Alpha emission is likely to be a competing decay mode.
434Uqe; 0.001 - 1; fission. Alpha emission is likely to be a competing decay mode.
433Uqe - 432Uqe; 1 - 1000; alpha.
431Uqe; 1 - 1000; fission.
430Uqe - 426Uqe; 1 - 1000; alpha. Fission may not be a factor in these isotopes of Uqe.
425Uqe; 0.001 - 1; fission.
424Uqe - 423Uqe; 0.001 - 1; alpha.
422Uqe - 420Uqe; 0.001 - 1; fission. Alpha emission is likely to be a competing decay mode.
419Uqe; 0.001 - 1; alpha. Fission is likely to be a competing decay mode.
418Uqe; 10-06 - 0.001; fission.
417Uqe; 10-06 - 0.001; fission. This nuclide is predicted to be beta-stable, so its half-life and decay mode are estimated.
416Uqe; 10-09 - 10-06; fission.
This pattern is generally to be expected, given a neutron shell closure at N = 308. Presence of a fission-decaying band in the N = 285 - 295 range indicates requires nuclear structure.
GUESSED PROPERTIES
The nuclear drop 534Uqe is unlikely to decay by neutron emission and is stable against fission. It is likely to be a nuclide. Drops in the band 533Uqe to 483Uqe are unlikely to decay by neutron emission and require a moderate amount of structural correction energy. Nuclides in this band are unlikely. Below 483Uqe, predictions are available.
OCCURRENCE
FORMATION
535Uqe is likely to be a nuclide. Depending on the neutron dripline's actual location, nuclei of this A value may form when material over 700 - 800 meters deep is ejected from a neutron star during a merger. (See "Neutron Star", this Wiki.). This nuclide can form directly as neutron star material breaks up or by a beta-decay chain from lower-Z nuclides. The isotope 535Uqe is outside the range in which half-life predictions exist. It is very neutron-rich, which implies a half-life under 1 sec(1),(4) is likely.
Nuclear drops 477Uqe to 475Uqe and all the drops in the band 471Uqe to 416Uqe are predicted to be nuclides. They are all too far from the neutron dripline to form directly. All beta-decay chains which would lead to 457Uqe or heavier isotopes are terminated at Z < 149 by nuclides which fission so quickly that no beta-decay branch is possible.
In order to determine whether 456Uqe and lighter isotopes can form, it is necessary to model the evolution of initial material by radioactive decay. Details of the model are provided in "Nuclear Decay Chains at High A" in this wiki. Per that model, 13 isotopes; 456Uqe to 447Uqe, 440Uqe, 438Uqe, and 435Uqe; can form. The three lightest are predicted by the model which populated all nuclides at time zero, and due to infall from long-lived beta-alpha-fission decay chains.
It is implausible that neutron capture can form any Uqe isotope.
PERSISTENCE
457Uqe and heavier isotopes will decay to nothing within 1000 sec after a neutron star merger which led to their formation.
456Uqe through 447Uqe, are all part of long-lived decay chains, but have half-lives under 1 sec themselves and no precursors whose half-lives exceed 1 sec. All will vanish within 1000 sec.
446Uqe through 418Uqe are blocked from forming via beta decay from the dripline by fission at Z < 149.
440Uqe has a predicted half-life in the 1 - 1000 sec range, and has four precursors with half-lives in the same range. It is the last step in a decay chain whose total time to extinction, under 125000 sec, has been computed.
435Uqe has a predicted half-life under 1 sec range, but has three precursors with half-lives in the 1 - 100 sec range. 435Uqe is the last step in a decay chain whose total time to extinction, under 120000 sec, has been computed .
No other isotopes of Uqe persist for a significant time.
Calculations done under maximum half-life assumptions and with all nuclides initially populated still point to all isotopes of Uqe vanishing within 105.5 (3.16E05) sec.
ATOMIC PROPERTIES
Electron structure of Uqe has been predicted by several sources (see "Extended Periodic Table" in Wikipedia). However, these predictions should be used with caution. Uqe is large enough that nuclear shape may have an effect on electron structure, which might cause different isotopes of Uqe to have different electronic structures. (That means it is no longer an element in the chemical sense.)
If this effect is small, Uqe will be an active (superactinide) metal of the 8th period. Its electron configuration has been predicted(5) to be [Og] 5g18 6f6 7d3 8s2 8p21/2.
REFERENCES
1. "Decay Modes and a Limit of Existence of Nuclei"; H. Koura; 4th Int. Conf. on the Chemistry and Physics of Transactinide Elements; Sept. 2011.
2. “The Highest Limiting Z in the Extended Periodic Table”; Y.K. Gambhir, A. Bhagwat, and M. Gupta; Journal of Physics G: Nuclear and Particle Physics. 42 (12): 125105. DOI:10.1088/0954 3899/42/12/ 125105.
3. "Magic Numbers of Ultraheavy Nuclei"; Vitali Denisov; Physics of Atomic Nuclei; researchgate.net/publications/225734594; July 2005.
4. "Nuclear Properties for Astrophysical Applications"; P. Moller & J. R. Nix; Los Alamos National Laboratory website; search by "LANL, T2", then "Nuclear Properties for Astrophysical Applications".
5. "Extended Periodic Table", Wikipedia.
6. Other references are found in the wiki articles cited.
9-Period Periodic Table of Elements | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
1 | 1 H |
2 He | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
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2 | 3 Li |
4 Be |
5 B |
6 C |
7 N |
8 O |
9 F |
10 Ne | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
3 | 11 Na |
12 Mg |
13 Al |
14 Si |
15 P |
16 S |
17 Cl |
18 Ar | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
4 | 19 K |
20 Ca |
21 Sc |
22 Ti |
23 V |
24 Cr |
25 Mn |
26 Fe |
27 Co |
28 Ni |
29 Cu |
30 Zn |
31 Ga |
32 Ge |
33 As |
34 Se |
35 Br |
36 Kr | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
5 | 37 Rb |
38 Sr |
39 Y |
40 Zr |
41 Nb |
42 Mo |
43 Tc |
44 Ru |
45 Rh |
46 Pd |
47 Ag |
48 Cd |
49 In |
50 Sn |
51 Sb |
52 Te |
53 I |
54 Xe | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
6 | 55 Cs |
56 Ba |
57 La |
58 Ce |
59 Pr |
60 Nd |
61 Pm |
62 Sm |
63 Eu |
64 Gd |
65 Tb |
66 Dy |
67 Ho |
68 Er |
69 Tm |
70 Yb |
71 Lu |
72 Hf |
73 Ta |
74 W |
75 Re |
76 Os |
77 Ir |
78 Pt |
79 Au |
80 Hg |
81 Tl |
82 Pb |
83 Bi |
84 Po |
85 At |
86 Rn | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
7 | 87 Fr |
88 Ra |
89 Ac |
90 Th |
91 Pa |
92 U |
93 Np |
94 Pu |
95 Am |
96 Cm |
97 Bk |
98 Cf |
99 Es |
100 Fm |
101 Md |
102 No |
103 Lr |
104 Rf |
105 Db |
106 Sg |
107 Bh |
108 Hs |
109 Mt |
110 Ds |
111 Rg |
112 Cn |
113 Nh |
114 Fl |
115 Mc |
116 Lv |
117 Ts |
118 Og | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
8 | 119 Uue |
120 Ubn |
121 Ubu |
122 Ubb |
123 Ubt |
124 Ubq |
125 Ubp |
126 Ubh |
127 Ubs |
128 Ubo |
129 Ube |
130 Utn |
131 Utu |
132 Utb |
133 Utt |
134 Utq |
135 Utp |
136 Uth |
137 Uts |
138 Uto |
139 Ute |
140 Uqn |
141 Uqu |
142 Uqb |
143 Uqt |
144 Uqq |
145 Uqp |
146 Uqh |
147 Uqs |
148 Uqo |
149 Uqe |
150 Upn |
151 Upu |
152 Upb |
153 Upt |
154 Upq |
155 Upp |
156 Uph |
157 Ups |
158 Upo |
159 Upe |
160 Uhn |
161 Uhu |
162 Uhb |
163 Uht |
164 Uhq |
165 Uhp |
166 Uhh |
167 Uhs |
168 Uho |
169 Uhe |
170 Usn |
171 Usu |
172 Usb | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
9 | 173 Ust |
174 Usq | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
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(06-22-20)