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Related Concept Videos

Metallic Solids02:37

Metallic Solids

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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.
All metallic solids exhibit high thermal and electrical conductivity, metallic luster, and malleability....
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Structures of Solids02:22

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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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Network Covalent Solids02:18

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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.
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Molecular and Ionic Solids02:54

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Crystalline solids are divided into four types: molecular, ionic, metallic, and covalent network based on the type of constituent units and their interparticle interactions.
Molecular Solids
Molecular crystalline solids, such as ice, sucrose (table sugar), and iodine, are solids that are composed of neutral molecules as their constituent units. These molecules are held together by weak intermolecular forces such as London dispersion forces, dipole-dipole interactions, or hydrogen bonds, which...
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Particles in a solid are tightly packed together (fixed shape) and often arranged in a regular pattern; in a liquid, they are close together with no regular arrangement (no fixed shape); in a gas, they are far apart with no regular arrangement (no fixed shape). Particles in a solid vibrate about fixed positions (cannot flow) and do not generally move in relation to one another; in a liquid, they move past each other (can flow) but remain in essentially constant contact; in a gas, they move...
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Volumes of irregularly shaped objects can be systematically determined using the concept of solids of revolution. This approach begins with a region defined by a curve in a two-dimensional plane. When this region is rotated about a fixed line, known as the axis of revolution, it generates a three-dimensional object with rotational symmetry. Such objects frequently arise in mathematical modeling, physics, and engineering applications.When the region being rotated lies directly against the axis...
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Introduction to Solid Supported Membrane Based Electrophysiology
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Eigenstate versus Zeeman-based approaches to the solid effect.

Inés Rodríguez-Arias1, Alberto Rosso1, Andrea De Luca2

  • 1LPTMS, CNRS, University of Paris-Sud, Université Paris-Saclay, 91405 Orsay, France.

Magnetic Resonance in Chemistry : MRC
|February 21, 2018
PubMed
Summary
This summary is machine-generated.

The solid effect enhances nuclear polarization through electron-nuclear spin interactions. This study reveals the Zeeman approach underestimates polarization due to leakage transitions, unlike the eigenstate method.

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Area of Science:

  • Quantum mechanics
  • Solid-state physics
  • Spin physics

Background:

  • The solid effect is a key mechanism for dynamic nuclear polarization.
  • It relies on polarization exchange between electron and nuclear spins via hyperfine interaction.
  • Theoretical analysis is complex due to lattice contact and microwave irradiation.

Purpose of the Study:

  • To analyze and compare two perturbation schemes for the solid effect: Zeeman and eigenstate-based approaches.
  • To derive an effective Liouville equation for the spin system's density matrix.
  • To understand the discrepancy in nuclear polarization predictions between the two schemes.

Main Methods:

  • Derivation of an effective Liouville equation from first principles for both perturbation schemes.
  • Numerical study of nuclear polarization behavior for varying hyperfine coupling values.
  • Projection onto the diagonal part of the spin-system density matrix to analyze discrepancies.

Main Results:

  • The Zeeman-based approach generally underestimates nuclear polarization compared to the eigenstate-based approach.
  • Parasite leakage transitions were identified as the cause of the underestimation in the Zeeman basis.
  • The study provides a detailed theoretical framework for understanding dynamic nuclear polarization.

Conclusions:

  • The eigenstate-based approach provides a more accurate description of dynamic nuclear polarization via the solid effect.
  • The Zeeman approach's limitations stem from unaddressed leakage transitions.
  • Accurate theoretical modeling is crucial for optimizing dynamic nuclear polarization techniques.