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Related Concept Videos

Ionic Crystal Structures02:42

Ionic Crystal Structures

Ionic crystals consist of two or more different kinds of ions that usually have different sizes. The packing of these ions into a crystal structure is more complex than the packing of metal atoms that are the same size.
Most monatomic ions behave as charged spheres, and their attraction for ions of opposite charge is the same in every direction. Consequently, stable structures for ionic compounds result (1) when ions of one charge are surrounded by as many ions as possible of the opposite...
Crystal Field Theory - Octahedral Complexes02:58

Crystal Field Theory - Octahedral Complexes

Crystal Field Theory
To explain the observed behavior of transition metal complexes (such as colors), a model involving electrostatic interactions between the electrons from the ligands and the electrons in the unhybridized d orbitals of the central metal atom has been developed. This electrostatic model is crystal field theory (CFT). It helps to understand, interpret, and predict the colors, magnetic behavior, and some structures of coordination compounds of transition metals.
CFT focuses on...
Crystal Field Theory - Tetrahedral and Square Planar Complexes02:46

Crystal Field Theory - Tetrahedral and Square Planar Complexes

Tetrahedral Complexes
Crystal field theory (CFT) is applicable to molecules in geometries other than octahedral. In octahedral complexes, the lobes of the dx2−y2 and dz2 orbitals point directly at the ligands. For tetrahedral complexes, the d orbitals remain in place, but with only four ligands located between the axes. None of the orbitals points directly at the tetrahedral ligands. However, the dx2−y2 and dz2 orbitals (along the Cartesian axes) overlap with the ligands less than the dxy,...
Imperfections in Crystal Structure: Point, Line and Plane Defects01:25

Imperfections in Crystal Structure: Point, Line and Plane Defects

A perfect crystal, in theory, has a uniform structure with the same unit cell and lattice points throughout. However, any deviation from this periodic arrangement is known as an imperfection or defect. These defects can be categorized into three types: point, line, and plane defects.Point defects occur when there is a deviation from the ideal due to missing atoms, displaced atoms, or additional atoms. These imperfections might occur due to imperfect packing during crystallization or because of...
Imperfections in Crystal Structure: Stoichiometric Point Defects01:26

Imperfections in Crystal Structure: Stoichiometric Point Defects

Schottky defects arise when some lattice points in a crystal, such as those in NaCl, remain unoccupied, creating lattice vacancies without disturbing the overall electrical neutrality of the crystal. This defect is common in ionic crystals where the positive and negative ions are similar in size, as seen in sodium chloride and cesium chloride. The presence of Schottky defects enables the crystal to conduct electricity to a small extent through an ionic mechanism. Electric fields cause nearby...
Imperfections in Crystal Structure: Non-Stoichiometric Defects01:29

Imperfections in Crystal Structure: Non-Stoichiometric Defects

Non-stoichiometric defects refer to a type of defect in the crystal structure of a compound where the ratio of its constituent elements deviates from the ideal stoichiometric ratio. There are two main types of non-stoichiometric defects: metal excess defects and metal deficiency defects.Metal excess defects occur when there is a slight surplus of metal ions than what is required by the stoichiometric ratio of the compound. For example, heating a sodium chloride crystal in sodium vapor results...

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Related Experiment Video

Updated: May 9, 2026

Influence of Hybrid Perovskite Fabrication Methods on Film Formation, Electronic Structure, and Solar Cell Performance
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Influence of Hybrid Perovskite Fabrication Methods on Film Formation, Electronic Structure, and Solar Cell Performance

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Tuning the Quantum-Well Structure of Single-Crystal Layered Perovskite Heterostructures.

Arundhati P Deshmukh1, Yinan Chen2, Jamie L Cleron1

  • 1Department of Chemistry, Stanford University, Stanford, California 94305, United States.

Journal of the American Chemical Society
|October 24, 2025
PubMed
Summary

We synthesized new layered perovskite heterostructures with tunable electronic properties. These materials exhibit distinct quantum-well structures, enabling control over exciton behavior for advanced optoelectronic applications.

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Low Pressure Vapor-assisted Solution Process for Tunable Band Gap Pinhole-free Methylammonium Lead Halide Perovskite Films
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Facile Synthesis of Colloidal Lead Halide Perovskite Nanoplatelets via Ligand-Assisted Reprecipitation
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Low Pressure Vapor-assisted Solution Process for Tunable Band Gap Pinhole-free Methylammonium Lead Halide Perovskite Films
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Facile Synthesis of Colloidal Lead Halide Perovskite Nanoplatelets via Ligand-Assisted Reprecipitation
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Area of Science:

  • Materials Science
  • Solid-State Chemistry
  • Crystallography

Background:

  • Layered perovskite heterostructures offer a scalable route to emergent properties.
  • Mechanically stacked monolayers have shown promising emergent properties.

Purpose of the Study:

  • To synthesize and characterize novel single-crystal layered perovskite heterostructures.
  • To investigate the influence of structural variations on electronic and optical properties.
  • To explore the tunability of quantum-well structures and exciton behavior.

Main Methods:

  • Single-crystal synthesis of M 2(PbCl 2)(AMCHC) 2(PbCl 4) ·2H 2O (1_M) heterostructures.
  • X-ray crystallography to determine crystal structure (chiral, polar space group C2).
  • Computational methods (band structure calculations) to analyze electronic properties and quantum-well structures.

Main Results:

  • Two new heterostructures (1_Na and 1_Li) were synthesized, featuring alternating perovskite and intergrowth layers.
  • Both heterostructures exhibit wide bandgaps, distinct excitonic features, and strong second harmonic generation.
  • 1_Na displays a Type-I quantum-well structure with intralayer excitons, while 1_Li shows a Type-II structure with interlayer excitons.

Conclusions:

  • The band alignment and exciton localization can be tuned by altering alkali metal cations and water molecule orientation.
  • These findings provide a pathway to control band alignment in self-assembled bulk perovskite heterostructures.
  • The synthesized materials hold potential for applications in optoelectronics and nonlinear optics.