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Related Concept Videos

Hydrogen Bonds01:04

Hydrogen Bonds

A hydrogen bond is formed when a weakly positive hydrogen atom already bonded to one electronegative atom (for example, the oxygen in the water molecule) is attracted to another electronegative atom from another polar molecule, such as water (H2O), hydrogen fluoride (HF), or ammonia (NH3). The huge electronegativity difference between the H atom (2.1) and the atom to which it is bonded (4.0 for an F atom, 3.5 for an O atom, or 3.0 for an N atom), combined with the very small size of an H atom...
Hydrogen Bonds00:26

Hydrogen Bonds

Hydrogen bonds are weak attractions between atoms that have formed other chemical bonds. One of these atoms is electronegative, like oxygen, and has a partial negative charge. The other is a hydrogen atom that has bonded with another electronegative atom and has a partial positive charge.
Hydrogen Bonds Control the World!
Because hydrogen has very weak electronegativity when it binds with a strongly electronegative atom, such as oxygen or nitrogen, electrons in the bond are unequally shared.
Molecular Orbital Theory II03:51

Molecular Orbital Theory II

Molecular Orbital Energy Diagrams
Valence Bond Theory02:45

Valence Bond Theory

Overview of Valence Bond Theory
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...
Lewis Structures of Molecular Compounds and Polyatomic Ions02:54

Lewis Structures of Molecular Compounds and Polyatomic Ions

To draw Lewis structures for complicated molecules and molecular ions, it is helpful to follow a step-by-step procedure as outlined:

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Related Experiment Video

Updated: May 30, 2026

Quantification of Hydrogen Concentrations in Surface and Interface Layers and Bulk Materials through Depth Profiling with Nuclear Reaction Analysis
14:11

Quantification of Hydrogen Concentrations in Surface and Interface Layers and Bulk Materials through Depth Profiling with Nuclear Reaction Analysis

Published on: March 29, 2016

g factor of hydrogenlike ²⁸Si¹³⁺.

S Sturm1, A Wagner, B Schabinger

  • 1Max-Planck-Institut für Kernphysik, Saupfercheckweg 1, 69117 Heidelberg, Germany.

Physical Review Letters
|July 30, 2011
PubMed
Summary

Scientists measured the electron g factor in silicon-28 ions using a Penning trap. The experimental value precisely matches theoretical predictions, validating quantum electrodynamics calculations for bound states.

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Last Updated: May 30, 2026

Quantification of Hydrogen Concentrations in Surface and Interface Layers and Bulk Materials through Depth Profiling with Nuclear Reaction Analysis
14:11

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Synthesis of Nine-atom Deltahedral Zintl Ions of Germanium and their Functionalization with Organic Groups

Published on: February 11, 2012

Area of Science:

  • Atomic Physics
  • Quantum Electrodynamics
  • High-Precision Measurements

Background:

  • The electron g factor is a fundamental constant in quantum mechanics.
  • Bound-state quantum electrodynamics (QED) calculations are crucial for understanding atomic properties.

Purpose of the Study:

  • To experimentally determine the g factor of an electron bound in hydrogenlike ²⁸Si¹³⁺.
  • To test the accuracy of advanced QED calculations in a strong electromagnetic field.

Main Methods:

  • Confining a single hydrogenlike ²⁸Si¹³⁺ ion in a cylindrical Penning trap.
  • Measuring the ratio of the ion's cyclotron frequency to its spin flip frequency.

Main Results:

  • The experimental g factor was determined to be 1.995 348 958 7(5)(3)(8).
  • This value shows excellent agreement with the theoretical prediction of 1.995 348 958 0(17).

Conclusions:

  • The precise agreement validates state-of-the-art QED calculations, including two-loop contributions.
  • This experiment serves as a stringent test of bound-state QED theory.