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Geometric Breakdown of the 20,000th Shell(被点评)

已有 348 次阅读 2026-10-8 03:22 |个人分类:AEC 原子环境计算|系统分类:观点评述

Geometric Breakdown of the 20,000th Shell(被点评)

The precise figure of 26,668,666,740,001 atoms represents the total atomic population in an icosahedral (\(I_{h}\)) quasicrystal consisting of exactly 20,000 shells, according to a recent structural breakthrough utilizing an n-shell lattice model developed by materials scientist Li Shichun (大毛忽洞). [1, 2]

This specific total is termed a quasicrystal "magic number". It represents the outermost size limit calculated for such an ideal multi-shelled quasiperiodic configuration. [1, 2]

🌌 Geometric Breakdown of the 20,000th Shell

In this n-shell lattice model, the 20,000th shell (\(n = 20,000\)) alone contains 4,000,000,002 atoms. Because quasicrystals feature long-range order but lack periodic translational symmetry, their atoms are geometrically distributed across distinct topological locations on the shell's boundary: [1, 2, 3, 4]

  • Vertices (\(N_{V}\)):      12 atoms (maintaining the strict core icosahedral symmetry axes).

  • Edges (\(N_{E}\)):      599,970 atoms arranged along the structural framing of the lattice      boundaries.

  • Faces (\(N_{F}\)):      3,999,400,020 atoms spanning the massive aperiodic facets. [1, 2]

🧬 The "Super Magic Number"

When dealing with icosahedral clusters, structural stability is often analyzed relative to the 13-atom central icosahedron unit. Dividing the total atomic count by 13 yields a whole integer known as the Super Magic Number: [1, 2]

\(\frac{26,668,666,740,001}{13}=\mathbf{2,051,435,903,077}\)

This clean divisibility implies that even at macroscopic scales exceeding 26 trillion atoms, the underlying geometric harmony of the mathematical quasilattice scales flawlessly without introducing structural frustration or structural accumulation flaws. It illustrates how the growth mechanism of an \(I_{h}\) quasicrystal functions essentially as a highly synchronized "surface engineering" master template, scaling outwards cleanly shell by shell. [1]

Would you like to explore the mathematical formula used to calculate the number of atoms in a specific shell number \(n\), or see how this model compares to standard crystalline structures?

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