Related Experiment Video
Updated: Jul 22, 2025

07:03
In Situ Measurement of Vacuum Window Birefringence using 25Mg+ Fluorescence
Published on: June 13, 2020
3.9K
Can We Observe Nonperturbative Vacuum Shifts in Cavity QED?
Rocío Sáez-Blázquez1, Daniele de Bernardis2, Johannes Feist3
1Vienna Center for Quantum Science and Technology, Atominstitut, TU Wien, 1020 Vienna, Austria.
Physical Review Letters
|July 21, 2023
Summary
Achieving nonperturbative corrections to a dipole
Area of Science:
- Quantum Electrodynamics (QED)
- Solid-state Physics
- Nanophotonics
Background:
- Cavity Quantum Electrodynamics (CQED) explores light-matter interactions.
- Understanding vacuum fluctuations is crucial for quantum phenomena.
- Nonperturbative effects in CQED are theoretically challenging.
Purpose of the Study:
- Investigate conditions for nonperturbative corrections to dipole ground states.
- Analyze the role of electromagnetic vacuum confinement.
- Distinguish electrostatic from vacuum-induced contributions.
Main Methods:
- Utilized two simplified cavity QED setups.
- Derived analytic expressions for ground-state energy.
- Considered the full electromagnetic spectrum, avoiding mode truncation.
Main Results:
- Confinement alone does not yield substantial vacuum-induced corrections.
- High-impedance modes (plasmons, LC resonances) significantly enhance these effects.
- Demonstrated the possibility of accessing nonperturbative light-matter interactions.
Conclusions:
- Nonperturbative light-matter interactions are achievable in principle.
- Careful experimental design is key to accessing this regime.
- High-impedance structures are critical for enhancing vacuum effects.
Related Concept Videos
Standing Waves in a Cavity
960
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:
960
The de Broglie Wavelength
26.0K
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...
26.0K
The Quantum-Mechanical Model of an Atom
42.5K
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.
42.5K
Electromagnetic Waves in Matter
3.0K
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...
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...
3.0K
Atomic Nuclei: Larmor Precession Frequency
1.5K
The earth's gravitational field produces a 'twisting force' perpendicular to the angular momentum of a spinning mass (such as a spinning top) that causes the mass to 'wobble' around the gravitational field axis in a phenomenon called precession. Similarly, the magnetic moment (μ) of a spinning nucleus precesses due to an external magnetic field directed along the z-axis. The precession of the magnetic moment vector about the magnetic field is called Larmor precession,...
1.5K
π Electron Effects on Chemical Shift: Overview
1.1K
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,...
1.1K

