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Related Concept Videos

Metallic Solids02:37

Metallic Solids

Metallic solids such as crystals of copper, aluminum, and iron are formed by metal atoms. The structure of metallic crystals is often described as a uniform distribution of atomic nuclei within a “sea” of delocalized electrons. The atoms within such a metallic solid are held together by a unique force known as metallic bonding that gives rise to many useful and varied bulk properties.
All metallic solids exhibit high thermal and electrical conductivity, metallic luster, and malleability. Many...
Network Covalent Solids02:18

Network Covalent Solids

Network covalent solids contain a three-dimensional network of covalently bonded atoms as found in the crystal structures of nonmetals like diamond, graphite, silicon, and some covalent compounds, such as silicon dioxide (sand) and silicon carbide (carborundum, the abrasive on sandpaper). Many minerals have networks of covalent bonds.
To break or to melt a covalent network solid, covalent bonds must be broken. Because covalent bonds are relatively strong, covalent network solids are typically...
Lattice Centering and Coordination Number02:33

Lattice Centering and Coordination Number

The structure of a crystalline solid, whether a metal or not, is best described by considering its simplest repeating unit, which is referred to as its unit cell. The unit cell consists of lattice points that represent the locations of atoms or ions. The entire structure then consists of this unit cell repeating in three dimensions. The three different types of unit cells present in the cubic lattice are illustrated in Figure 1.
Types of Unit Cells
Imagine taking a large number of identical...
Structures of Solids02:22

Structures of Solids

Solids in which the atoms, ions, or molecules are arranged in a definite repeating pattern are known as crystalline solids. Metals and ionic compounds typically form ordered, crystalline solids. A crystalline solid has a precise melting temperature because each atom or molecule of the same type is held in place with the same forces or energy. Amorphous solids or non-crystalline solids (or, sometimes, glasses) which lack an ordered internal structure and are randomly arranged. Substances that...

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Fabrication of Three-Dimensional Graphene-Based Polyhedrons via Origami-Like Self-Folding
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Corrugation-Stabilized Layers and Stacking-Selected Ground State in Layered Graphitic C3N4.

JianJia Chen1, Yujie Liao2, Jianxin Zhong3,4

  • 1School of Physics and Optoelectronics, Xiangtan University, Xiangtan 411105, China.

The Journal of Physical Chemistry Letters
|May 18, 2026
PubMed
Summary
This summary is machine-generated.

Graphitic carbon nitride (C₃N₄) bulk structure was resolved by exploring intralayer corrugation and interlayer stacking. The P3̅c1 phase, stabilized by stacking, is identified as the lowest-energy graphitic C₃N₄ structure.

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Area of Science:

  • Materials Science
  • Computational Chemistry
  • Solid State Physics

Background:

  • Graphitic carbon nitride (C₃N₄) displays structural polymorphism due to flexible heptazine networks.
  • Corrugated monolayers are favored over planar sheets, but the bulk ground state of C₃N₄ remains uncertain due to unexplored interlayer stacking effects.

Purpose of the Study:

  • To systematically investigate the intralayer corrugation and interlayer stacking effects on the bulk ground state of graphitic C₃N₄.
  • To identify the most stable crystalline phase of graphitic C₃N₄.

Main Methods:

  • Performed a comprehensive structural search combining intralayer corrugation and interlayer stacking within an NX-network framework.
  • Utilized first-principles optimization for approximately one hundred candidate structures.
  • Conducted phonon calculations and simulated X-ray diffraction for stability and characterization.

Main Results:

  • Layer corrugation is the primary stabilization factor, with interlayer stacking providing additional energy gains.
  • Stacking of the P3₂1 monolayer leads to the P3̅c1 phase, which is energetically more favorable than the commonly assumed Pbca structure.
  • Phonon calculations confirmed the dynamic stability of the P3̅c1 phase.

Conclusions:

  • A two-step stabilization mechanism involving corrugation and stacking governs the bulk structure of graphitic C₃N₄.
  • The P3̅c1 phase is identified as a strong candidate for the lowest-energy bulk graphitic C₃N₄.
  • Simulated X-ray diffraction patterns can distinguish the P3̅c1 phase from the Pbca structure.