Related Experiment Video
Updated: Mar 15, 2026

09:23
Quantum State Engineering of Light with Continuous-wave Optical Parametric Oscillators
Published on: May 30, 2014
15.1K
Quantum-beat based dissipation for spin squeezing and light entanglement.
Optics Express
|August 25, 2016
Summary
Engineered dissipation enhances spin squeezing and light entanglement in a quantum beat system. This method controls atom-field interactions to achieve near-perfect two-mode squeezing and entanglement for bright fields and dressed spins.
Area of Science:
- Quantum optics
- Atomic physics
- Quantum information science
Background:
- Quantum beat systems offer a platform for studying light-matter interactions.
- Spin squeezing and entanglement are crucial resources for quantum technologies.
- Controlling dissipation is key to preserving quantum states.
Purpose of the Study:
- To demonstrate engineered dissipation for enhancing spin squeezing and light entanglement.
- To investigate the role of atomic coherence in controlling dissipation.
- To achieve near-perfect two-mode squeezing and entanglement in a V-configuration atomic system.
Main Methods:
- Utilizing a quantum beat system with two bright fields interacting with three-level atoms.
- Employing atom-field nonlinear interactions controlled by atomic coherence.
- Performing physical analysis and numerical verification using dressed atomic states.
Main Results:
- Engineered dissipation induces significant spin squeezing and light entanglement.
- Near-perfect two-mode squeezing and entanglement achieved for both bright fields and dressed spins.
- Excited-state spin squeezing approaches 40% below the standard quantum limit.
Conclusions:
- Engineered dissipation is a viable method for generating quantum correlations in atomic systems.
- The control of atomic coherence is essential for effective dissipation engineering.
- This work provides a pathway for creating robust entangled states for quantum information processing.
Related Concept Videos
Spin–Spin Coupling Constant: Overview
1.6K
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...
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...
1.6K
The de Broglie Wavelength
34.2K
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...
34.2K
Atomic Nuclei: Nuclear Relaxation Processes
1.3K
In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis, the precessing magnetic moments are randomly oriented around the z-axis.
1.3K
NMR Spectroscopy: Spin–Spin Coupling
3.6K
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...
3.6K
Atomic Nuclei: Nuclear Spin State Overview
2.2K
NMR-active nuclei have energy levels called 'spin states' that are associated with the orientations of their nuclear magnetic moments. In the absence of a magnetic field, the nuclear magnetic moments are randomly oriented, and the spin states are degenerate. When an external magnetic field is applied, the spin states have only 2 + 1 orientations available to them. A proton with = ½ has two available orientations. Similarly, for a quadrupolar nucleus with a nuclear spin value of one, the...
2.2K
¹H NMR: Interpreting Distorted and Overlapping Signals
1.7K
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...
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...
1.7K

