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Related Concept Videos

The Quantum-Mechanical Model of an Atom02:45

The Quantum-Mechanical Model of an Atom

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. Schrödinger...
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The word "gas" comes from the Flemish word meaning "chaos," first used to describe vapors by the chemist J. B. van Helmont. Consider a container filled with gas, with a continuous and random motion of molecules. During collisions, the velocity component parallel to the wall is unchanged, and the component perpendicular to the wall reverses direction but does not change in magnitude. If the molecule’s velocity changes in the x-direction, then its momentum is changed. During the short time of the...
π Electron Effects on Chemical Shift: Overview01:27

π Electron Effects on Chemical Shift: Overview

An applied magnetic field causes loosely bound π-electrons in organic molecules to circulate, producing a local or induced diamagnetic field over a large spatial volume. As the molecules tumble in solution, the field generated by π-electrons in spherical substituents results in a zero net field. However, the net field generated by π-electrons in non-spherical substituents is not zero. The effect of this induced field depends on the orientation of the molecule with respect to B0, resulting in...
Fermi Level Dynamics01:12

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The vacuum level denotes the energy threshold required for an electron to escape from a material surface. It is usually positioned above the conduction band of a semiconductor and acts as a benchmark for comparing electron energies within various materials.
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Related Experiment Video

Updated: May 23, 2026

Generation and Coherent Control of Pulsed Quantum Frequency Combs
06:42

Generation and Coherent Control of Pulsed Quantum Frequency Combs

Published on: June 8, 2018

From molecular control to quantum technology with the dynamic Stark effect.

Philip J Bustard1, Guorong Wu, Rune Lausten

  • 1Steacie Institute for Molecular Sciences, National Research Council of Canada, 100 Sussex Drive, Ottawa, Ontario, K1A 0R6, Canada.

Faraday Discussions
|March 29, 2012
PubMed
Summary

The non-resonant dynamic Stark effect precisely controls ultrafast processes in matter. This method manipulates molecular dynamics, chemical reactions, and quantum light states for advanced applications.

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Area of Science:

  • Atomic, Molecular, and Optical Physics
  • Quantum Optics
  • Physical Chemistry

Background:

  • The non-resonant dynamic Stark effect offers precise control over ultrafast phenomena.
  • Understanding this effect is key to manipulating quantum systems.

Purpose of the Study:

  • To elucidate the physics of the non-resonant dynamic Stark effect.
  • To demonstrate its broad applicability in controlling diverse physical and chemical processes.

Main Methods:

  • Theoretical discussion of the non-resonant dynamic Stark effect.
  • Demonstration of control in various atomic, molecular, and solid-state systems.

Main Results:

  • The non-resonant dynamic Stark effect provides exquisite precision in manipulating ultrafast processes.
  • Successful control demonstrated in molecular rotation, chemical reactions, and quantum state preparation.
  • Applications include suppression of vacuum fluctuations and dynamic bandwidth generation for quantum light storage.

Conclusions:

  • The non-resonant dynamic Stark effect is a versatile and powerful tool for controlling ultrafast dynamics.
  • Its applications span fundamental physics, chemistry, and quantum information science.