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Related Concept Videos

Ionic Crystal Structures02:42

Ionic Crystal Structures

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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...
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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.
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Coordination compounds and complexes exhibit different colors, geometries, and magnetic behavior, depending on the metal atom/ion and ligands from which they are composed. In an attempt to explain the bonding and structure of coordination complexes, Linus Pauling proposed the valence bond theory, or VBT, using the concepts of hybridization and the overlapping of the atomic orbitals. According to VBT, the central metal atom or ion (Lewis acid) hybridizes to provide empty orbitals of suitable...
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Radicals: Electronic Structure and Geometry01:07

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This lesson delves into the geometry of a radical, which is influenced by the electronic structure of the molecule. The principle is similar to that of a lone pair, where the unpaired electron influences the geometry at the radical center.
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For any given polymer, the weight average molecular weight (Mw) is higher than, if not equal to, the number average molecular weight (Mn). The only situation in which the weight average molecular weight and the number average molecular weight are equal is when a polymer consists only of chains with equal molecular weight. However, this never happens in a synthetic polymer, since it is difficult to control the polymerization process up to a molecular level with accuracy to a hundred percent.
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Intrinsic semiconductors are highly pure materials with no impurities. At absolute zero, these semiconductors behave as perfect insulators because all the valence electrons are bound, and the conduction band is empty, disallowing electrical conduction. The Fermi level is a concept used to describe the probability of occupancy of energy levels by electrons at thermal equilibrium. In intrinsic semiconductors, the Fermi level is positioned at the midpoint of the energy gap at absolute zero. When...
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Updated: May 3, 2026

Characterization of Nanocrystal Size Distribution using Raman Spectroscopy with a Multi-particle Phonon Confinement Model
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Characterization of Nanocrystal Size Distribution using Raman Spectroscopy with a Multi-particle Phonon Confinement Model

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Polytype distribution in circumstellar silicon carbide.

T L Daulton1, T J Bernatowicz, R S Lewis

  • 1Materials Science Division, Argonne National Laboratory, Argonne IL, 60439-4838, USA. tdaulton@nrlssc.navy.mil

Science (New York, N.Y.)
|June 8, 2002
PubMed
Summary
This summary is machine-generated.

Astronomical infrared spectra of silicon carbide (SiC) are controversial. Direct analysis of presolar SiC from meteorites reveals only two common polytypes, simplifying previous models.

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Area of Science:

  • * Astrochemistry and materials science.
  • * Characterization of presolar grains.
  • * Stellar evolution and nucleosynthesis.

Background:

  • * The crystallographic structure of circumstellar silicon carbide (SiC) is debated, with astronomical infrared spectra suggesting a complex mixture of polytypes.
  • * Previous studies relied on indirect spectral analysis, leading to uncertainty about the actual SiC structures formed in stellar outflows.

Purpose of the Study:

  • * To directly determine the polytype distribution of circumstellar silicon carbide (SiC).
  • * To resolve the controversy surrounding SiC crystallographic classes inferred from astronomical data.
  • * To understand the formation conditions of SiC in stellar environments.

Main Methods:

  • * Direct structural analysis using transmission electron microscopy (TEM).
  • * Examination of presolar silicon carbide (SiC) grains extracted from the Murchison carbonaceous meteorite.
  • * Identification and quantification of SiC polytypes present in the samples.

Main Results:

  • * Only two SiC polytypes were identified: cubic 3C and hexagonal 2H.
  • * Intergrowths of these two polytypes were also observed.
  • * The observed structural simplicity contrasts with the wide variety of polytypes suggested by spectral analyses.

Conclusions:

  • * The limited polytype distribution is attributed to low pressures in circumstellar outflows.
  • * Low condensation temperatures of silicon carbide in these environments favor the formation of only 3C and 2H polytypes.
  • * This finding simplifies our understanding of SiC formation in evolved stars.