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Related Concept Videos

Atomic Nuclei: Nuclear Relaxation Processes01:23

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: Nuclear Spin State Overview01:03

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...
Atomic Nuclei: Types of Nuclear Relaxation01:28

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...
Atomic Nuclei: Nuclear Spin State Population Distribution01:14

Atomic Nuclei: Nuclear Spin State Population Distribution

Near absolute zero temperatures, in the presence of a magnetic field, the majority of nuclei prefer the lower energy spin-up state to the higher energy spin-down state. As temperatures increase, the energy from thermal collisions distributes the spins more equally between the two states. The Boltzmann distribution equation gives the ratio of the number of spins predicted in the spin −½ (N−) and spin +½ (N+) states.
Atomic Emission Spectroscopy: Interference01:30

Atomic Emission Spectroscopy: Interference

In atomic emission spectroscopy (AES), high-temperature atomizers excite a broad range of elements and molecules that generate complex emissions from sources such as oxides, hydroxides, and flame combustion products in the flame or plasma. Several strategies can be employed to minimize spectral interferences caused by overlapping emission lines or bands. These include increasing instrument resolution, choosing alternative emission lines, optimally placing the detector in low-background regions,...
Atomic Nuclei: Nuclear Spin01:08

Atomic Nuclei: Nuclear Spin

All atomic particles possess an intrinsic angular momentum, or 'spin'. Electrons, protons, and neutrons each have a spin value of ½, although protons and neutrons in nuclei may have higher half-integer spins owing to energetic factors.
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Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving
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Published on: March 30, 2017

Feedback control of trapped coherent atomic ensembles.

T Vanderbruggen1, R Kohlhaas, A Bertoldi

  • 1Laboratoire Charles Fabry, Institut d'Optique, CNRS, Université Paris-Sud, 2 avenue Augustin Fresnel, 91127 Palaiseau, France.

Physical Review Letters
|June 11, 2013
PubMed
Summary

We developed a feedback control system using weak optical measurements and microwave manipulations to protect atomic ensembles from decoherence. This method enhances the stability of superposition states for applications like atomic sensors.

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Area of Science:

  • Quantum optics
  • Atomic physics
  • Quantum control

Background:

  • Coherent atomic ensembles are sensitive to collective noise, leading to decoherence.
  • Protecting quantum states is crucial for quantum technologies and precision measurements.

Purpose of the Study:

  • To demonstrate feedback control for maintaining the internal states of trapped atomic ensembles.
  • To protect superposition states against collective decoherence using a novel feedback scheme.

Main Methods:

  • Utilizing weak optical measurements with minimal backaction.
  • Implementing coherent microwave manipulations for state correction.
  • Analyzing feedback efficiency using a binary noise model and characterizing the probe's trade-offs.

Main Results:

  • Successfully controlled internal states of trapped coherent atomic ensembles.
  • Demonstrated protection of superposition states against collective noise.
  • Showcased correction of general collective noise types.

Conclusions:

  • The developed feedback scheme effectively combats decoherence in atomic ensembles.
  • This technique advances the operation of atomic interferometers beyond the Ramsey scheme.
  • The method paves the way for the development of more sensitive atomic sensors.