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Standing Waves in a Cavity01:28

Standing Waves in a Cavity

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A household microwave and lasers are examples of standing electromagnetic waves in a cavity. When two conducting metal plates are placed parallel at the nodal planes, it creates a cavity where standing waves are formed. The cavity between the two planes is analogous to a stretched string held at the points x = 0 and x = L. Here, the distance 'L' between the two planes must be an integer multiple of half of the wavelength. The wavelengths that satisfy this condition are given by:
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Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)01:20

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

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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...
1.0K
¹H NMR: Long-Range Coupling01:27

¹H NMR: Long-Range Coupling

1.7K
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...
1.7K
Spin–Spin Coupling: Three-Bond Coupling (Vicinal Coupling)01:22

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

1.1K
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...
1.1K
The Quantum-Mechanical Model of an Atom02:45

The Quantum-Mechanical Model of an Atom

42.3K
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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Spin–Spin Coupling Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

919
In bromoethane, the three methyl protons are coupled to the two methylene protons that are three bonds away. In accordance with the n+1 rule, the signal from the methyl protons is split into three peaks with 1:2:1 relative intensities. The methylene protons appear as a quartet, with the relative intensities of 1:3:3:1.
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must...
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Related Experiment Video

Updated: Jun 30, 2025

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

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Photonic Which-Path Entangler Based on Longitudinal Cavity-Qubit Coupling.

Z M McIntyre1, W A Coish1

  • 1Department of Physics, McGill University, 3600 rue University, Montreal, Québec H3A 2T8, Canada.

Physical Review Letters
|March 15, 2024
PubMed
Summary
This summary is machine-generated.

Researchers demonstrate a new method for creating qubit-which-path (QWP) entangled states using modulated cavity-qubit coupling. This technique enables entanglement distribution in quantum networks without requiring single-photon sources or detectors.

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Area of Science:

  • Quantum optics
  • Quantum information science
  • Cavity quantum electrodynamics

Background:

  • Quantum entanglement is a fundamental resource for quantum information processing.
  • Distributing entanglement over long distances is crucial for quantum networks.
  • Current methods often rely on fragile single-photon states and detectors.

Purpose of the Study:

  • To introduce a novel method for generating qubit-which-path (QWP) entangled states.
  • To demonstrate the potential of QWP states for generating multipartite entanglement.
  • To enable entanglement distribution in quantum networks without single-photon components.

Main Methods:

  • Utilizing modulated longitudinal cavity-qubit coupling.
  • Controlling the path of a multiphoton coherent-state wave packet.
  • Conditioning the wave packet's path on the qubit's state.

Main Results:

  • Successfully generated qubit-which-path (QWP) entangled states.
  • Showcased the ability of QWP states to generate long-range multipartite entanglement.
  • Established a pathway for entanglement distribution in quantum networks.

Conclusions:

  • Modulated cavity-qubit coupling offers a robust method for generating QWP entanglement.
  • This approach bypasses the need for single-photon sources and detectors in quantum networks.
  • The generated QWP states are a promising resource for scalable quantum communication.