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This article is about an undiscovered element. Once it is discovered, this article will be edited with more information.

Unbitrium, Ubt, is the temporary name for element 123. Isotopes are predicted between the dripline and 344Ubt; between 322Ubt and 318Ubt; and between 316Ubt and 286Ubt. All of them have half-lives less than 1 day, and most are under 1 sec. 350Ubt may persist up to 2 hours after an event which led to its formation. All other isotopes will vanish in less than 1000 sec.

The ground state electron configuration of Ubt is uncertain, and may even be a superposition of two different configurations.

Ubt has the lowest atomic number of any element physicists have not attempted to synthesize.

NUCLEAR PROPERTIES

INFORMATION SOURCES

There has been considerable study of the decay properties of Ubt. Most of these have been limited to N < 220, but I know of only one which which reports decay properties of Ubt to the neutron dripline(1). Maps on pp 15 & 18 address the entire (Z,N) region covered, but report only the dominant decay mode and report half-lives only to within a band three orders of magnitude wide (0.001 - 1 sec, for example). More detailed estimates of these properties can be extracted from maps on pp 11 & 12, but only for a limited range of Z and N. Half-life data are reported by colors, which makes numerical estimates laborious to produce. Ref. 1 will be used as the primary reference in this article. Predictions from other sources will be compared to it.

An independent map of half-lives and decay modes exists(2). The map shows a stabilized region in a band apparently ending near Z = 132. That band ends at Z = 118. Neutron counts in the region lie between N = 191 and N = 202, but the most stabilized nuclides lie in a band 195 <= N <= 200. Ref. 1 does not show this region.

An interactive site exists which has tables of b-, b+, and alpha decay(1) half-lives for Z up to 135 and A up to 339(3). Total half-lives and branch ratios can be computed from these to provide a third pair of maps. This model does not show particular stabilization around N = 200, aligning with Ref. 1 in this regard.

PREDICTED PROPERTIES

Even-N isotopes from the neutron dripline down to 398Ubt decay predominantly by beta emission with half-lives in the 0.001 - 1 sec range. Half-lives aren't reported, but the properties of beta decay indicate that half-lives close to 0.001 sec are likely(3). Odd-N drops in this band decay by neutron emission.

All isotopes in the band 397Ubt to 377Ubt are predicted to have half-lives in the 0.001 - 1 sec range. Beta emission is reported as the dominant decay mode of heavier isotopes in the band, while lighter isotopes have either beta emission or fission as dominant modes. It is likely that both modes are important in most isotopes.

Between 376Ubt and 367Ubt, decay modes and half-lives are complicated. Both fission and beta decay occur, and half-lives range from 10-09 to 0.001 sec for fission decaying isotopes. Two beta-decaying isotopes, 375Ubt and 372Ubt, are predicted to have half-lives predicted to lie in the 0.001 - 1 sec range. Decay properties seem to be defined by N count, with the pattern extending across a range of Z values. It is likely that those properties are a result of the model, although they may be real.

Isotopes in the band 366Ubt to 364Ubt are all predicted to decay by fission, but with with half-lives in the range 0.001 - 1 sec.

Isotopes in the band 363Ubt to 352Ubt are predicted to decay by beta emission and have half-lives in the 0.001 - 1 sec range.

Isotopes in the band 351Ubt to 346Ubt are predicted to decay by beta emission and have half-lives in the 1 - 1000 sec range. Note that neutron count for 351Ubt is 228. A closer look at half-lives (p 12) indicates that none of them have half-lives exceeding a few seconds.

345Ubt to 342Ubt are predicted to decay by fission. Their half-lives decline rapidly as N decreases.

Ref 1 predicts a gap from 341Ubt to 317Ubt, which is predicted to be occupied by nuclear drops or very short-lived nuclides.

Ref, 2 reports isotopes with half-lives above 10-06 sec in the band 322Ubt - 318Ubt. Of these, 322Ubt to 320Ubt have half-lives in the 1 sec - 1 day band; and the other two have half-lives in the 0.001 - 1 sec band. Aside from these it predicts a wide band of isotopes predicted to decay by <10-06 sec. These can't be compared with Ref. 1 due to the difference in half-life cutoff.

Ref 1 predicts 316Ubt to 314Ubt will decay by quickly and by fission.

It also predicts that 313Ubt through 290Ubt should decay by alpha emission. Half-lives for most are short, but 307Ubt to 298Ubt are predicted to have half-lives in the 10-06 - 0.001 sec range. (Note that neutron count for 307Ubt is 184.) Ref 2 predicts fission down as far as 306Ubt.

Finally, 289Ubt to 286Ubt are predicted to decay rapidly by proton emission.

OCCURRENCE

FORMATION

All even-N nuclear drops from the neutron dripline to 398Ubt are predicted to be nuclides. All nuclear drops in the bands 397Ubt to 342Ubt are predicted to be nuclides. Some of the heavier isotopes in that band can form directly as a neutron star disintegrates. Most of them however require a chain of beta decays to form. 373Ubt, 372Ubt, and 369Ubt to 367Ubt cannot form because their beta decay chains are interrupted by fission at lower Z. All the others down to 342Ubt can form. Ref 2 shows nuclides in the band from 322Ubt to 318Ubt. Beta decay chains leading to them are all interrupted. None of them can form. Ref. 1 also predicts all drops in the band 316Ubt to 286Ubt are nuclides. None of them can form. It is possible to simulate the formation of nuclides via beta decay chains using data from Ref. 3 and assuming an initial distribution close to the neutron dripline. Details of the model are provided in "Nuclear Decay Chains at High A" in this wiki. Per that model, at least 59 isotopes between 401Ubt and 343Ubt can form.

Neutron capture may be able to produce nuclides up to A around 380 before fission attrition stops further growth. Neutron capture is expected to contribute to formation of all significant Ubt isotopes.

PERSISTENCE

351Ubt and heavier isotopes will vanish within 1000 sec after a supernova or neutron star merger which led to their formation, or lie at higher Z than beta-decay chains which end in nuclides which fission with a half-life not much greater than 1 sec.

350Ubt through 347Ubt are not formed via alpha infall, but only beta decay chains from the dripline. None of these isotopes is expected to persist more than 3600 sec.

346Ubq and lighter isotopes all have nothing but short-lived precursors, or will lie at a Z beyond the point at which a short-lived beta decay chain terminates. All of those isotopes are expected to vanish within 1000 sec; they are not expected to persist a significant amount of time.

ATOMIC PROPERTIES

Ubt is expected to be an 8th period active metal (superactinide). Its electron configuration has been predicted(4) to be [Og] 6f1 7d1 8s2 8p11/2. However, at least one alternate configuration may be the ground state(5). Its ground state may even be a superposition of two configurations.

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. “Systematic Study of Decay Properties of Heaviest Elements.”; Y. M. Palenzuelaa, L. F. Ruiza, A. Karpov, and W. Greiner; Bulletin of the Russian Academy of Sciences, Physics.  Vol . 76, No.11, pp 1165 – 1177; 2012

3. "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".

4. "Extended Periodic Table", Wikipedia

5. "Electronic structure of element 123"; Koen van der Schoor; Rijksuniversiteit Groningen Bachelor Research Project; 2016. (Accessible via Wikipedia's article "Extended Periodic Table".)

6. Other references are found in the wiki articles cited.

9-Period Periodic Table of Elements
1 1
H
2
He
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
Alkali metal Alkaline earth metal Lanthanide Actinide Superactinide Transition metal Post-transition metal Metalloid Other nonmetal Halogen Noble gas
predicted predicted predicted predicted predicted predicted predicted predicted predicted

(09-15-20)

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