2021
DOI: 10.1134/s1070363221020134
|View full text |Cite
|
Sign up to set email alerts
|

Quantum Chemical Study of X@BikPbm, BikPbm∙X, X@SbkSnm, and SbkSnm∙X Clusters

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
2

Citation Types

0
7
0

Year Published

2022
2022
2023
2023

Publication Types

Select...
4

Relationship

1
3

Authors

Journals

citations
Cited by 4 publications
(7 citation statements)
references
References 43 publications
0
7
0
Order By: Relevance
“…If n i = 1, then the spinor i=bold-italicρtruêi describes occupied natural localized one‐electron state; if n i ≈ 1 or n i ≈ 0, then the deviation from naturalness or from localization is measured by a dispersion (4) [32, 33]. υigoodbreak=trueρ̂iini2goodbreak=ibold-italicρtruêni2igoodbreak=ibold-italicρtruê2iitrueρ̂i2goodbreak=()1ni0.25emni Two localized spinors │ i › = bold-italicρtruê│ i › and │ i ′ › = bold-italicρtruê│ i ′ › with maximal populations n i ≈ n i ′ ≈ 1 (and with minimal dispersions υ i ≈ υ i ′ ≈ 0) describes the lone or binding electron pair, if the time reversal operator [34] T = ‐ i ′σ y C transforms one spinor into the other: i=Ti;i=Ti The oxidation number Ξ X of an atom or atomic group X in the [X@Ω] ξ cluster [16] we associate with the cluster charge ξ, the populations of one‐electron states localized in the shell Ω, and the atomic core charges Z A by new formula (): normalΞnormalX=ξ+bold∑ωΩEntirenω+εbold∑AΩZnormalA For the parameter ε , we take th...…”
Section: Computational Detailsmentioning
confidence: 99%
See 4 more Smart Citations
“…If n i = 1, then the spinor i=bold-italicρtruêi describes occupied natural localized one‐electron state; if n i ≈ 1 or n i ≈ 0, then the deviation from naturalness or from localization is measured by a dispersion (4) [32, 33]. υigoodbreak=trueρ̂iini2goodbreak=ibold-italicρtruêni2igoodbreak=ibold-italicρtruê2iitrueρ̂i2goodbreak=()1ni0.25emni Two localized spinors │ i › = bold-italicρtruê│ i › and │ i ′ › = bold-italicρtruê│ i ′ › with maximal populations n i ≈ n i ′ ≈ 1 (and with minimal dispersions υ i ≈ υ i ′ ≈ 0) describes the lone or binding electron pair, if the time reversal operator [34] T = ‐ i ′σ y C transforms one spinor into the other: i=Ti;i=Ti The oxidation number Ξ X of an atom or atomic group X in the [X@Ω] ξ cluster [16] we associate with the cluster charge ξ, the populations of one‐electron states localized in the shell Ω, and the atomic core charges Z A by new formula (): normalΞnormalX=ξ+bold∑ωΩEntirenω+εbold∑AΩZnormalA For the parameter ε , we take th...…”
Section: Computational Detailsmentioning
confidence: 99%
“… υigoodbreak=trueρ̂iini2goodbreak=ibold-italicρtruêni2igoodbreak=ibold-italicρtruê2iitrueρ̂i2goodbreak=()1ni0.25emni Two localized spinors │ i › = bold-italicρtruê│ i › and │ i ′ › = bold-italicρtruê│ i ′ › with maximal populations n i ≈ n i ′ ≈ 1 (and with minimal dispersions υ i ≈ υ i ′ ≈ 0) describes the lone or binding electron pair, if the time reversal operator [34] T = ‐ i ′σ y C transforms one spinor into the other: i=Ti;i=Ti The oxidation number Ξ X of an atom or atomic group X in the [X@Ω] ξ cluster [16] we associate with the cluster charge ξ, the populations of one‐electron states localized in the shell Ω, and the atomic core charges Z A by new formula (): normalΞnormalX=ξ+bold∑ωΩEntirenω+εbold∑AΩZnormalA For the parameter ε , we take the value 0.15, that is, we refer all the states with populations 0.85 ≤ n ω ≤ 1.00 to the localized ones. We borrowed the letter designation Ξ X for the oxidation number [35], but abandoned the formula proposed in it, which for X = Hg, Cd, Yb, Sr, and Ba in X@Pb 12 clusters gave negative oxidation numbers instead of the positive integer values Ξ X = +2 [16]. The oxidation number of an atom is usually understood as ...…”
Section: Computational Detailsmentioning
confidence: 99%
See 3 more Smart Citations