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Related Concept Videos

Valence Bond Theory02:42

Valence Bond Theory

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...
Valence Bond Theory02:45

Valence Bond Theory

Overview of Valence Bond Theory
Spin–Spin Coupling: One-Bond Coupling01:17

Spin–Spin Coupling: One-Bond Coupling

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,...
Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)01:20

Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)

Two NMR-active nuclei bonded to a central atom can be involved in geminal or two-bond coupling. Geminal coupling is commonly seen between diastereotopic protons in chiral molecules and unsymmetrical alkenes, among others.
The central atom need not be NMR-active because its electrons are affected by the electron polarization of the spin-active atoms. However, spin information is transmitted less effectively than in one-bond coupling, and 2J values are usually weaker than 1J values. The energy of...
Atomic Nuclei: Nuclear Spin State Overview01:03

Atomic Nuclei: Nuclear Spin State Overview

NMR-active nuclei have energy levels called 'spin states' that are associated with the orientations of their nuclear magnetic moments. In the absence of a magnetic field, the nuclear magnetic moments are randomly oriented, and the spin states are degenerate. When an external magnetic field is applied, the spin states have only 2 + 1 orientations available to them. A proton with = ½ has two available orientations. Similarly, for a quadrupolar nucleus with a nuclear spin value of one, the...
Spin–Spin Coupling: Three-Bond Coupling (Vicinal Coupling)01:22

Spin–Spin Coupling: Three-Bond Coupling (Vicinal Coupling)

Vicinal or three-bond coupling is commonly observed between protons attached to adjacent carbons. Here, nuclear spin information is primarily transferred via electron spin interactions between adjacent C‑H bond orbitals. This generally favors the antiparallel arrangement of spins, so 3J values are usually positive.
The extent of coupling depends on the C‑C bond length, the two H‑C‑C angles, any electron-withdrawing substituents, and the dihedral angle between the involved orbitals. The...

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Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope
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Spin reorientation in TlFe1.6Se2 with complete vacancy ordering.

Andrew F May1, Michael A McGuire, Huibo Cao

  • 1Materials Science and Technology Division, Oak Ridge National Laboratory, Tennessee 37831, USA.

Physical Review Letters
|September 26, 2012
PubMed
Summary

Vacancy ordering in TlFe(1.6)Se(2) influences magnetism, revealing a true ground state with in-plane magnetic moments. This contrasts with disordered regions, suggesting coupled effects in superconducting analogues.

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Area of Science:

  • Condensed Matter Physics
  • Materials Science
  • Solid State Chemistry

Background:

  • Investigating the interplay between crystal structure and magnetic properties is crucial for understanding novel materials.
  • TlFe(1.6)Se(2) exhibits complex magnetic behavior influenced by vacancy ordering.

Purpose of the Study:

  • To elucidate the relationship between vacancy ordering and the magnetic ground state in TlFe(1.6)Se(2).
  • To clarify the magnetic moment orientation in homogeneous versus partially disordered crystals.

Main Methods:

  • Single crystal neutron diffraction
  • Nuclear forward scattering
  • Transmission electron microscopy

Main Results:

  • Homogeneous TlFe(1.6)Se(2) crystals display Fe magnetic moments aligned in the ab plane below 100 K.
  • Partially disordered crystals show competing magnetic moment orientations (c-axis vs. ab plane).
  • Properties of disordered TlFe(1.6)Se(2) are not solely from ordered or disordered regions.

Conclusions:

  • The true ground state of TlFe(1.6)Se(2) is characterized by in-plane magnetic ordering.
  • Phase separation in intercalated iron selenides may involve coupling between ordered and disordered regions.
  • This coupling could be significant for understanding superconducting analogues.