Unbiseptium (Ubs)
Superactinide標準原子量
データなし電子配置
[Og] 5g⁷ 8s²融点
データなし沸点
データなし密度
データなし酸化数
データなし電気陰性度（Pauling）
データなし第1イオン化エネルギー
データなし発見年
データなし原子半径
データなしUnbiseptium is the temporary systematic name for element 127, a predicted superheavy element that has not been synthesized or observed in nature. It would lie in period 8, beyond the known elements, where relativistic effects and closely spaced electron shells make chemical behavior especially uncertain. Its chemistry, isotopes, phase, and lifetimes remain matters of nuclear and quantum-chemical prediction rather than experiment.
This element has not been synthesized or experimentally confirmed. All listed physicochemical properties are calculated, extrapolated, or model-dependent.
No macroscopic sample of unbiseptium exists, and even individual atoms have not been confirmed. Its color, density, melting point, crystal structure, and ordinary physical form are unknown. Any proposed metallic appearance is only a model-based expectation for a superheavy element.
Unbiseptium has no confirmed practical, commercial, medical, or industrial use. If atoms were ever produced, their use would be limited to basic research in nuclear structure, decay modes, and the behavior of electrons in extremely high nuclear charge. Such experiments would involve detecting single atoms or decay chains, not handling material quantities.
No compound of unbiseptium has been made or detected. Calculations for elements in this region suggest that valence levels may involve 5g, 6f, 7d, and 8p orbitals, so simple placement in a familiar periodic group may be misleading. Oxidation states, bonding preferences, and possible halides or oxides are therefore speculative. Formulas such as UbsFₙ or UbsOₙ should be read only as generic placeholders, not known substances.
The safety properties of unbiseptium are not experimentally known because no isotope has been confirmed. Any produced atoms would almost certainly be radioactive and short-lived, with hazards depending on isotope-specific decay modes and energies. In practice, risks would come from accelerator operations, radioactive targets, recoil products, and decay radiation, rather than from chemical toxicity of bulk unbiseptium.
Unbiseptium has no confirmed natural occurrence and no observed environmental chemistry. Predicted isotopes would not persist long enough to form natural reservoirs, circulate through ecosystems, or accumulate in minerals. If produced in a laboratory, quantities would be far below environmental relevance and would decay within controlled experimental systems.
There is no commodity market, industrial demand, recycling stream, or practical supply chain for unbiseptium. Production, if achieved, would require atom-at-a-time heavy-ion nuclear reactions using rare targets and high-intensity accelerators. Expected yields for such high atomic numbers are extremely small, and isolation of weighable material is not realistic with known methods. Its economic context is therefore research cost and facility capability, not material supply.
Unbiseptium is not known in the Sun, meteorites, Earth, or astronomical spectra. Very heavy nuclei near this region might be transiently formed in extreme neutron-rich nucleosynthesis environments, but they would be expected to decay rapidly. No stable or long-lived isotope of element 127 is known or predicted with confidence.
- Unbiseptium is still a systematic placeholder name, not a discovery name.
- No isotope of element 127 has been confirmed experimentally.
- Its chemistry is more uncertain than simple periodic-table extrapolation suggests.
- A successful experiment would likely identify it from decay chains rather than direct chemical separation.
- All ordinary material properties listed for it in informal sources are predictions or guesses.
画像
性質
物理的性質
データなし
化学的性質
- 電子親和力
- 0.5 eV
- 電子配置
- [Og] 5g⁷ 8s²
熱力学的性質
データなし
原子核
- 陽子数
- 127 全元素の陽子数を比較 →
- 既知の同位体
- 0 全元素の既知の同位体を比較 →
- 安定同位体
- 0 全元素の安定同位体を比較 →
- 天然での存在
- 未観測
存在度
データなし
安全性
- 放射性
- はい
結晶構造
データなし
電子構造
- 各電子殻の電子数
- 2, 8, 18, 32, 39, 18, 8, 2 全元素の各電子殻の電子数を比較 →
識別子
- CAS登録番号
- 54576-78-2 全元素のCAS登録番号を比較 →
電子配置 予測値
——このイオンの電子配置データはありません。
原子モデル
同位体によって中性子数、質量、安定性は変わりますが、中性原子の電子配置は変わりません。
データなし
模式的な原子モデルです。実際の縮尺とは異なります。
原子の指紋
発光／吸収スペクトル
同位体分布
安定同位体はありません。
| 質量数 | 原子質量（u） | 天然存在比 | 半減期 |
|---|
相／状態
相・状態のデータはありません
データなし
相・状態のデータはありません