Related Experiment Video
Updated: Aug 8, 2026

09:23
Quantum State Engineering of Light with Continuous-wave Optical Parametric Oscillators
Published on: May 30, 2014
Atomic quantum state teleportation and swapping
1Department of Physics and Astronomy, University of Rochester, Rochester, New York 14627, USA.
Physical Review Letters
|January 3, 2001
Summary
New protocols enable quantum state teleportation and swapping between atoms and photons using Einstein-Podolsky-Rosen light. These methods are feasible for continuous quantum variables and macroscopic atomic samples.
Area of Science:
- Quantum Information Science
- Atomic Physics
- Quantum Optics
Background:
- Quantum state teleportation and swapping are fundamental quantum information tasks.
- Utilizing continuous quantum variables offers advantages for macroscopic systems.
- Einstein-Podolsky-Rosen (EPR) light provides a resource for quantum correlations.
Purpose of the Study:
- To propose novel protocols for quantum state teleportation and swapping.
- To extend these protocols to both atom-photon and atom-atom entanglement.
- To investigate the feasibility of these protocols for macroscopic atomic ensembles.
Main Methods:
- Development of theoretical protocols leveraging EPR light.
- Application to polarization quantum states of multiphoton light pulses.
- Consideration of macroscopic atomic samples with continuous quantum variables.
Main Results:
- Proposed protocols for atom-photon and atom-atom quantum state teleportation and swapping.
- Demonstrated applicability to continuous quantum variables and macroscopic atomic samples.
- Showcased the sufficiency of simple free-space interaction between polarized light and atomic ensembles.
Conclusions:
- The proposed protocols offer a viable route for quantum information processing with macroscopic atomic systems.
- Experimental realization using gas samples of atoms is feasible.
- These advancements contribute to the development of robust quantum technologies.
Related Concept Videos
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...
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 Pauli Exclusion Principle
The arrangement of electrons in the orbitals of an atom is called its electron configuration. We describe an electron configuration with a symbol that contains three pieces of information:
Hybridization of Atomic Orbitals II
sp3d and sp3d 2 Hybridization
Atomic Nuclei: Nuclear Spin State Overview
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...
Deactivation Processes: Jablonski Diagram
Luminescence, the emission of light by a substance that has absorbed energy, is a process that involves the interaction of molecules with light. The energy-level diagram, or Jablonski diagram, is a graphical representation of these interactions, illustrating the various states and transitions a molecule can undergo. In a typical Jablonski diagram, the lowest horizontal line represents the ground-state energy of the molecule, which is usually a singlet state. This state represents the energies...

