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Related Concept Videos

Structures of Solids02:22

Structures of Solids

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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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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.
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Spin–Spin Coupling Constant: Overview01:08

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In bromoethane, the three methyl protons are coupled to the two methylene protons that are three bonds away. In accordance with the n+1 rule, the signal from the methyl protons is split into three peaks with 1:2:1 relative intensities. The methylene protons appear as a quartet, with the relative intensities of 1:3:3:1.
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NMR Spectroscopy: Spin–Spin Coupling01:08

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The spin state of an NMR-active nucleus can have a slight effect on its immediate electronic environment. This effect propagates through the intervening bonds and affects the electronic environments of NMR-active nuclei up to three bonds away; occasionally, even farther. This phenomenon is called spin–spin coupling or J-coupling. Coupling interactions are mutual and result in small changes in the absorption frequencies of both nuclei involved. While nuclei of the same element are involved...
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Spin–Spin Coupling: One-Bond Coupling01:17

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Coupling interactions are strongest between NMR-active nuclei bonded to each other, where spin information can be transmitted directly through the pair of bonding electrons. While nuclei polarize their electrons to the opposite spins, the bonding electron pair has opposite spins. Configurations with antiparallel nuclear spins are expected to be lower in energy. When coupling makes antiparallel states more favorable, J is considered to have a positive value. The one-bond coupling constant, 1J,...
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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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Experimental Methods for Spin- and Angle-Resolved Photoemission Spectroscopy Combined with Polarization-Variable Laser
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Three-spin solid effect and the spin diffusion barrier in amorphous solids.

Kong Ooi Tan1, Michael Mardini1, Chen Yang1

  • 1Francis Bitter Magnet Laboratory and Department of Chemistry, Massachusetts Institute of Technology, Cambridge, MA 02139, USA.

Science Advances
|July 31, 2019
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Summary
This summary is machine-generated.

Dynamic nuclear polarization (DNP) enhances NMR signals. This study reveals how electron polarization transfers to nearby nuclei, identifying protons on the trityl radical as key for initial transfer.

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Area of Science:

  • Solid-state Nuclear Magnetic Resonance (NMR) spectroscopy
  • Electron Paramagnetic Resonance (EPR) spectroscopy
  • Dynamic Nuclear Polarization (DNP)

Background:

  • Dynamic nuclear polarization (DNP) significantly amplifies Nuclear Magnetic Resonance (NMR) signals.
  • The precise mechanisms and spatial localization of electron polarization transfer to surrounding nuclei in DNP remain incompletely understood.
  • Understanding these processes is crucial for advancing applications in chemistry, biology, and physics.

Purpose of the Study:

  • To elucidate the detailed mechanism of electron polarization transfer in DNP.
  • To determine the spatial proximity of nuclei involved in polarization transfer relative to the polarizing agent.
  • To quantify the extent of the spin diffusion barrier around the polarizing agent.

Main Methods:

  • Theoretical analysis of the three-spin solid effect, sensitive to electron-nuclear distances.
  • Experimental determination of electron-nuclear distances using the sensitivity of the solid effect.
  • Proton Electron Nuclear Double Resonance (1H ENDOR) experiments to track polarization transfer pathways.

Main Results:

  • The three-spin solid effect analysis revealed high sensitivity to electron-nuclear distances.
  • The spin diffusion barrier around the trityl radical in a glycerol-water matrix was determined to be less than 6 Å.
  • Protons on the trityl molecule itself were identified as the primary sites for initial polarization transfer.

Conclusions:

  • The study precisely maps the initial steps of DNP polarization transfer.
  • The findings indicate that polarization is first transferred to protons on the trityl radical.
  • Subsequent polarization transfer to surrounding glycerol molecules occurs through molecules in close contact with the trityl radical.