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Valence Bond Theory02:42

Valence Bond Theory

10.4K
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...
10.4K
Colors and Magnetism03:02

Colors and Magnetism

13.2K
Color in Coordination Complexes
When atoms or molecules absorb light at the proper frequency, their electrons are excited to higher-energy orbitals. For many main group atoms and molecules, the absorbed photons are in the ultraviolet range of the electromagnetic spectrum, which cannot be detected by the human eye. For coordination compounds, the energy difference between the d orbitals often allows photons in the visible range to be absorbed and emitted, which is seen as colors by the human...
13.2K
Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)01:20

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

1.4K
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...
1.4K
Spin–Spin Coupling: One-Bond Coupling01:17

Spin–Spin Coupling: One-Bond Coupling

1.2K
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,...
1.2K
Spin–Spin Coupling: Three-Bond Coupling (Vicinal Coupling)01:22

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

1.3K
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...
1.3K
Crystal Field Theory - Tetrahedral and Square Planar Complexes02:46

Crystal Field Theory - Tetrahedral and Square Planar Complexes

46.7K
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,...
46.7K

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Related Experiment Video

Updated: Dec 2, 2025

Fabricating van der Waals Heterostructures with Precise Rotational Alignment
09:25

Fabricating van der Waals Heterostructures with Precise Rotational Alignment

Published on: July 5, 2019

9.9K

Gate-controlled spin-valley-layer locking in bilayer transition-metal dichalcogenides.

H Khani1, S Piri Pishekloo

  • 1Department of Physics, Kharazmi University, 31979-37551, Tehran, Iran. hoseinkhani01@gmail.com.

Nanoscale
|November 4, 2020
PubMed
Summary

Researchers demonstrate an electrically controllable platform in bilayer transition metal dichalcogenides (TMDs) for advanced logic devices. This platform enables precise control over electron spin, valley, and layer pseudospin for high-performance electronics.

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Ohmic Contact Fabrication Using a Focused-ion Beam Technique and Electrical Characterization for Layer Semiconductor Nanostructures
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Area of Science:

  • Condensed Matter Physics
  • Materials Science
  • Nanotechnology

Background:

  • Electron internal degrees of freedom are crucial for high-performance electronic devices.
  • Bilayer transition metal dichalcogenides (TMDs) exhibit interplay between spin-orbit and interlayer couplings.
  • Pseudospintronics offers a new paradigm for electronic device design.

Purpose of the Study:

  • To investigate the transport of spin, valley, and layer pseudospin in AB-stacked bilayer TMDs.
  • To demonstrate an electrically controllable platform for multifunctional and ultra-high-speed logic devices.
  • To determine conditions for excellent spin, valley, and layer polarizations.

Main Methods:

  • Theoretical study of electron transport through a magnetoelectric barrier in bilayer TMDs.
  • Analysis of spin, valley, and layer pseudospin transport under electric and magnetic fields.
  • Investigation of gate-controlled polarization inversion.

Main Results:

  • Achieved perfect spin and valley polarizations and good layer localization over a large Fermi energy range.
  • Demonstrated electrical control for inverting spin, valley, and layer polarizations using gate potentials.
  • Identified conditions for excellent polarizations in terms of adjustable system parameters.
  • Showed that a single electric barrier acts as a bipolar pseudospin semiconductor.

Conclusions:

  • An electrically controllable platform for multifunctional pseudospintronic devices based on bilayer TMDs has been demonstrated.
  • The findings pave the way for novel 2D material-based pseudospintronic applications.
  • Precise control over electron spin, valley, and layer pseudospin is achievable.