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Related Concept Videos

¹H NMR: Long-Range Coupling01:27

¹H NMR: Long-Range Coupling

The coupling interactions of nuclei across four or more bonds are usually weak, with J values less than 1 Hz. While these are usually not observed in spectra, the presence of multiple bonds along the coupling pathway can result in observable long-range coupling.
In alkenes, spin information is communicated via σ–π overlap, as seen in allylic (four-bond) and homoallylic (five-bond) couplings. These coupling interactions are stronger when the σ bond is parallel to the alkene π orbitals.
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...
The de Broglie Wavelength02:32

The de Broglie Wavelength

In the macroscopic world, objects that are large enough to be seen by the naked eye follow the rules of classical physics. A billiard ball moving on a table will behave like a particle; it will continue traveling in a straight line unless it collides with another ball, or it is acted on by some other force, such as friction. The ball has a well-defined position and velocity or well-defined momentum, p = mv, which is defined by mass m and velocity v at any given moment. This is the typical...
¹H NMR: Interpreting Distorted and Overlapping Signals01:02

¹H NMR: Interpreting Distorted and Overlapping Signals

Spin systems where the difference in chemical shifts of the coupled nuclei is greater than ten times J are called first-order spin systems. These nuclei are weakly coupled, and their chemical shifts and coupling constant can generally be estimated from the well-separated signals in the spectrum.
As Δν decreases and the signals move closer, the doublets appear increasingly distorted. The intensities of the inner lines increase at the cost of those of the outer lines as the signals are slanted or...
Electromagnetic Waves in Matter01:30

Electromagnetic Waves in Matter

Electromagnetic waves can travel in the vacuum as well as in matter. For example light, which is an electromagnetic wave, can travel through air, water, or glass.
Consider the electromagnetic wave passing through a dielectric medium. In such a case, Maxwell's equations get modified. In Ampere's law, ε0 , the dielectric permittivity of free space is replaced with ε, the permittivity of dielectric. Also, the vacuum permeability μ0 is replaced by the permeability of the medium, μ.
Furthermore, the...
NMR Spectroscopy: Spin–Spin Coupling01:08

NMR Spectroscopy: Spin–Spin Coupling

The spin state of an NMR-active nucleus can have a slight effect on its immediate electronic environment. This effect propagates through the intervening bonds and affects the electronic environments of NMR-active nuclei up to three bonds away; occasionally, even farther. This phenomenon is called spin–spin coupling or J-coupling. Coupling interactions are mutual and result in small changes in the absorption frequencies of both nuclei involved. While nuclei of the same element are involved in...

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Related Experiment Video

Updated: Jun 3, 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

Coherent electron-phonon coupling in tailored quantum systems.

P Roulleau1, S Baer, T Choi

  • 1Solid State Physics Laboratory, ETH Zurich, 8093 Zurich, Switzerland. roulleau@phys.ethz.ch

Nature Communications
|March 17, 2011
PubMed
Summary
This summary is machine-generated.

Electron-phonon coupling causes decoherence in nanostructures. We observed current oscillations in double quantum dots due to acoustic phonon interference, which diminish with increasing temperature.

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Last Updated: Jun 3, 2026

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High Resolution Phonon-assisted Quasi-resonance Fluorescence Spectroscopy
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Resonance Fluorescence of an InGaAs Quantum Dot in a Planar Cavity Using Orthogonal Excitation and Detection
12:57

Resonance Fluorescence of an InGaAs Quantum Dot in a Planar Cavity Using Orthogonal Excitation and Detection

Published on: October 13, 2017

Area of Science:

  • Quantum physics
  • Condensed matter physics
  • Nanotechnology

Background:

  • Decoherence, arising from system-environment coupling, hinders coherent manipulation of quantum states.
  • Understanding decoherence sources is vital for quantum technologies utilizing nanostructures.

Purpose of the Study:

  • Investigate the impact of electron-phonon coupling on decoherence in graphene and InAs nanowire double quantum dots (DQDs).
  • Identify the mechanisms behind observed current oscillations in DQDs.

Main Methods:

  • Electrical transport measurements on graphene and InAs nanowire DQDs.
  • Analysis of DQD current as a function of energy detuning.
  • Temperature-dependent measurements to probe decoherence effects.

Main Results:

  • Observed current oscillations periodic in energy detuning in both graphene and InAs nanowire DQDs.
  • Oscillations were more pronounced in the InAs nanowire compared to graphene.
  • The oscillations disappeared at elevated temperatures.

Conclusions:

  • The observed oscillations are attributed to interference between inelastic decay paths involving acoustic phonons.
  • This electron-phonon coupling mechanism explains the temperature dependence of the oscillations.
  • The findings provide insights into decoherence in nanostructure-based quantum systems.