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Quantum Numbers02:43

Quantum Numbers

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It is said that the energy of an electron in an atom is quantized; that is, it can be equal only to certain specific values and can jump from one energy level to another but not transition smoothly or stay between these levels.
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Crystal Field Theory - Octahedral Complexes02:58

Crystal Field Theory - Octahedral Complexes

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Crystal Field Theory
To explain the observed behavior of transition metal complexes (such as colors), a model involving electrostatic interactions between the electrons from the ligands and the electrons in the unhybridized d orbitals of the central metal atom has been developed. This electrostatic model is crystal field theory (CFT). It helps to understand, interpret, and predict the colors, magnetic behavior, and some structures of coordination compounds of transition metals.
CFT focuses on...
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Crystal Field Theory - Tetrahedral and Square Planar Complexes02:46

Crystal Field Theory - Tetrahedral and Square Planar Complexes

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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,...
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Predicting Molecular Geometry02:27

Predicting Molecular Geometry

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VSEPR Theory for Determination of Electron Pair Geometries
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Coordination Number and Geometry02:57

Coordination Number and Geometry

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For transition metal complexes, the coordination number determines the geometry around the central metal ion. Table 1 compares coordination numbers to molecular geometry. The most common structures of the complexes in coordination compounds are octahedral, tetrahedral, and square planar.
19.1K
The Quantum-Mechanical Model of an Atom02:45

The Quantum-Mechanical Model of an Atom

59.0K
Shortly after de Broglie published his ideas that the electron in a hydrogen atom could be better thought of as being a circular standing wave instead of a particle moving in quantized circular orbits, Erwin Schrödinger extended de Broglie’s work by deriving what is now known as the Schrödinger equation. When Schrödinger applied his equation to hydrogen-like atoms, he was able to reproduce Bohr’s expression for the energy and, thus, the Rydberg formula governing hydrogen spectra.
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Related Experiment Video

Updated: Feb 7, 2026

Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
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What Spatial Geometries do (2+1)-Dimensional Quantum Field Theory Vacua Prefer?

Sebastian Fischetti1, Lucas Wallis1, Toby Wiseman1

  • 1Theoretical Physics Group, Blackett Laboratory, Imperial College, London SW7 2AZ, United Kingdom.

Physical Review Letters
|July 14, 2018
PubMed
Summary

Relativistic quantum field theories in (2+1) dimensions favor crumpled spaces due to negative vacuum free energy. This quantum effect is significant for graphene, even at room temperature, influencing material configurations.

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Area of Science:

  • Theoretical Physics
  • Quantum Field Theory
  • Condensed Matter Physics

Background:

  • Investigating vacuum free energy in relativistic (2+1)-dimensional quantum field theories (QFTs).
  • Analyzing the influence of temperature and spatial geometry on vacuum energy.
  • Considering free scalar and Dirac fields on perturbed flat space.

Purpose of the Study:

  • To determine the vacuum free energy as a function of temperature and spatial geometry.
  • To understand the energetic preference of QFTs for specific spatial configurations.
  • To assess the relevance of vacuum energy effects in materials like graphene.

Main Methods:

  • Calculated vacuum free energy for free scalar and Dirac fields.
  • Examined arbitrary perturbations of flat space in (2+1) dimensions.
  • Analyzed the leading-order contribution to the free energy difference from flat space.

Main Results:

  • The free energy difference from flat space is finite and negative.
  • Relativistic (2+1)-dimensional QFTs energetically favor crumpled spaces.
  • This effect holds true for both quantum (zero temperature) and thermal (high temperature) contributions.

Conclusions:

  • Free (2+1)-dimensional QFTs consistently favor crumpled spatial geometries.
  • The vacuum energy effect is non-negligible for relativistic Dirac fields in materials like graphene.
  • This quantum effect must be considered for accurate analysis of graphene's equilibrium configuration.