Related Experiment Video
Updated: Jul 3, 2026

10:00
Gradient Echo Quantum Memory in Warm Atomic Vapor
Published on: November 11, 2013
Storing images in warm atomic vapor.
M Shuker1, O Firstenberg, R Pugatch
1Department of Physics, Technion-Israel Institute of Technology, Haifa 32000, Israel.
Physical Review Letters
|July 23, 2008
Summary
Scientists stored 2D images in atomic vapor for 30 microseconds using electromagnetically induced transparency. Atom diffusion limited storage, but a phase-shift technique improved image visibility.
Area of Science:
- Quantum optics
- Atomic physics
- Optical information storage
Background:
- Coherent light storage in atomic media is crucial for quantum technologies.
- Electromagnetically induced transparency (EIT) enables light manipulation in atomic systems.
Purpose of the Study:
- To store arbitrary 2D images in warm atomic vapor.
- To investigate the limitations and potential improvements for optical image storage in atomic media.
Main Methods:
- Utilized electromagnetically induced transparency (EIT) in warm atomic vapor.
- Stored 2D optical images, preserving both intensity and phase information.
- Employed a phase-shift lithography-analogous technique to mitigate atomic diffusion effects.
Main Results:
- Successfully stored and retrieved 2D images with fidelity for up to 30 microseconds.
- Identified atomic diffusion as the primary limitation for storage resolution and duration.
- Demonstrated that the phase-shift technique enhances reconstructed image visibility.
Conclusions:
- EIT provides a viable method for reversible optical image storage in atomic ensembles.
- Atomic diffusion is a key challenge to overcome for longer storage times and higher resolution.
- Advanced techniques can improve the quality of stored and retrieved optical information.
Related Concept Videos
Atomic Spectroscopy: Effects of Temperature
Atomization, converting samples into gas-phase atoms and ions, is essential for atomic spectroscopy. The flame temperature required for atomization affects the efficiency of the atomic spectroscopic methods by increasing the atomization efficiency and the relative population of the excited and ground states.
At thermal equilibrium, the relative populations of excited and ground state atoms can be estimated using the Maxwell–Boltzmann distribution. For example, an increase in temperature from...
At thermal equilibrium, the relative populations of excited and ground state atoms can be estimated using the Maxwell–Boltzmann distribution. For example, an increase in temperature from...
Preparation of Samples for Electron Microscopy
To be visualized by an electron microscope, either transmission or scanning, biological samples need to be fixed (stabilized) so the electron beam does not destroy them and dried thoroughly (desiccated/dehydrated) so the vacuum does not affect them. Fixation needs to be done as quickly as possible because the sample properties will start changing as soon as it is removed from its natural environment. For example, in a tissue sample, the oxygen levels begin decreasing, causing an altered...
Atomic Absorption Spectroscopy: Atomization Methods
Atomic Absorption Spectroscopy (AAS) atomizes samples through flame atomization or electrothermal atomization. Flame atomization typically involves a nebulizer and spray chamber assembly to combine the sample with a fuel–oxidant mixture, creating a fine aerosol mist that enters a burner. Typically, the fuel and oxidant are combined in an approximately stoichiometric ratio. However, for atoms that are easily oxidized, a fuel-rich mixture may be more advantageous. Only about 5% of the aerosol...
Vaporization
The physical form of a substance changes by changing its temperature. For example, raising the temperature of a liquid causes the liquid to vaporize (convert into vapor). The process is called vaporization—a surface phenomenon. For vaporization to occur, kinetic energy must be greater than the intermolecular forces that keep molecules bonded. The amount of energy needed to vaporize a quantity of liquid at a given pressure and a constant temperature is called the heat of vaporization. When...
Atomic Nuclei: Nuclear Relaxation Processes
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. This...
Atomic Nuclei: Types of Nuclear Relaxation
Nuclear relaxation restores the equilibrium population imbalance and can occur via spin–lattice or spin–spin mechanisms, which are first-order exponential decay processes.
In spin–lattice or longitudinal relaxation, the excited spins exchange energy with the surrounding lattice as they return to the lower energy level. Among several mechanisms that contribute to spin–lattice relaxation, magnetic dipolar interactions are significant. Here, the excited nucleus transfers energy to a nearby...
In spin–lattice or longitudinal relaxation, the excited spins exchange energy with the surrounding lattice as they return to the lower energy level. Among several mechanisms that contribute to spin–lattice relaxation, magnetic dipolar interactions are significant. Here, the excited nucleus transfers energy to a nearby...

