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Unseptnilium, Usn, is the temporary name for element 170. Isotopes are predicted between 482Usn and 461Usn (excluding probable artifacts), none of which have half-lives exceeding 0.001 sec. None of these predicted isotopes can form. Isotopes in the band 580Usn to 561Usn are likely, most of which may form. All Usn isotopes will be gone less than 1000 sec. after the event which led to their formation.

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 502Usn to 439Usn.

502Usn and 499Usn appear to be artifacts. N = 318 has been predicted(2) to be a neutron closure, but N = 229 or 232 is far above that closure.

498Usn to 483Usn is a gap, which might mean half-lives below 10-09 sec or might mean the model is going ragged at its edges.

The main band lies between 482Usn and 461Usn. Format used to display these is: isotope(s); half-life in seconds; dominant decay mode; comments.

482Usn - 480Usn; 10-09 - 10-06; alpha; These are not unrealistic, particularly if N = 318 is also neutron-magic like N = 308.

479Usn - 468Usn; 10-06 - 0.001; alpha.

467Usn - 465Usn; 10-09 - 10-06; alpha.

464Usn; < 10-09; decay mode probably fission

463Usn - 461Usn; 10-09 - 10-06; fission.

This pattern is to be expected, given a neutron shell closure at N = 308.

Isotopes decaying by alpha emission and having half-lives between 10-09 and 10-06 sec are also predicted in the band from 440Usn to 439Usn. Despite their short half-lives, the isotopes in this band are probably artifacts connected to those reported for Usu and Usb.

GUESSED PROPERTIES

Drops in the bands 580Usn to 561Usn and 479Usn to 474Usn are unlikely to decay by neutron emission and are stable against fission. Nuclides in these bands are likely. Drops in the bands 616Usn to 581Usn, 560Usn to 480Usn, and 473Usn to 436Usn are unlikely to decay by neutron emission and require a moderate amount of structural correction energy. Nuclides in these bands are unlikely.

COMPARISON

In the region where predictions and guesses overlap, the estimating technique lists only 479Usn to 474Usn as "likely". Ref. 1 predicts a much wider band of existing Usn isotopes.

OCCURRENCE

FORMATION

580Usn to 561Usn are likely to be nuclides. Depending on the neutron dripline's actual location, nuclei in this A range may form when material over 700 - 800 meters deep is ejected from a neutron star during a merger. (See "Neutron Star", this Wiki.). Isotopes in this band may form directly or via beta decay chains from lower Z nuclides. Attrition from decay chains due to fission or beta+neutron(s) emission can be expected.

Many nuclear drops in the band 502Usn to 439Usn are predicted to be nuclides. They are all too far from the neutron dripline to form directly, and cannot form from lower Z nuclides because beta decay chains terminate at Z < 170.

It is implausible that neutron capture can form any Usn isotope.

PERSISTENCE

All Usn isotopes are expected to decay away to nothing within 1000 sec after the neutron star merger which led to their formation.

ATOMIC PROPERTIES

Electron structure of Usn has been predicted by several sources (see "Extended Periodic Table" in Wikipedia). However, these predictions should be used with caution. Orbital theory may break down at Z = 170. While only the innermost electrons would be qualitatively different, other orbitals are likely to be affected sufficiently to change the ground state occupation. Usn is also large enough that nuclear shape may have an effect on electron structure, which might cause different isotopes of Usn to have different electronic structures. (That means it is no longer an element in the chemical sense.)

If these effects are small, Usn will be a p-block metal of the 8th period. Its electron configuration has been predicted(3) to be [Og] 5g18 6f14 7d10 8s2 8p21/2 8p23/2 9s2 9p21/2.

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. "Extended Periodic Table", Wikipedia.

4. 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

(06-08-20)

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