Jove
Visualize
Contact Us
JoVE
x logofacebook logolinkedin logoyoutube logo
ABOUT JoVE
OverviewLeadershipBlogJoVE Help Center
AUTHORS
Publishing ProcessEditorial BoardScope & PoliciesPeer ReviewFAQSubmit
LIBRARIANS
TestimonialsSubscriptionsAccessResourcesLibrary Advisory BoardFAQ
RESEARCH
JoVE JournalMethods CollectionsJoVE Encyclopedia of ExperimentsArchive
EDUCATION
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab ManualFaculty Resource CenterFaculty Site
Terms & Conditions of Use
Privacy Policy
Policies

Related Concept Videos

Atomic Nuclei: Types of Nuclear Relaxation01:28

Atomic Nuclei: Types of Nuclear Relaxation

1.1K
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...
1.1K
Atomic Nuclei: Nuclear Relaxation Processes01:23

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
Van der Waals Interactions01:24

Van der Waals Interactions

72.9K
Atoms and molecules interact with each other through intermolecular forces. These electrostatic forces arise from attractive or repulsive interactions between particles with permanent, partial, or temporary charges. The intermolecular forces between neutral atoms and molecules are ion–dipole, dipole–dipole, and dispersion forces, collectively known as van der Waals forces.
72.9K
Atomic Nuclei: Nuclear Spin State Population Distribution01:14

Atomic Nuclei: Nuclear Spin State Population Distribution

2.5K
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.
2.5K
Atomic Absorption Spectroscopy: Interference01:25

Atomic Absorption Spectroscopy: Interference

2.3K
Interference leads to systematic error in atomic absorption (AA) measurements by enhancing or diminishing the analytical signal or the background. These interferences can be grouped into three main categories: spectral interference, chemical interference, and physical interference.
Spectral interference occurs when signals from other elements or molecules overlap with the analyte signal, falsely elevating or masking the analyte's absorbance. This interference can be corrected using Zeeman,...
2.3K
Deactivation Processes: Jablonski Diagram01:25

Deactivation Processes: Jablonski Diagram

2.1K
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...
2.1K

You might also read

Related Articles

Articles linked to this work by shared authors, journal, and citation graph.

Sort by
Same author

Quench Instabilities of a Strongly Interacting Quantum Gas in an Optical Cavity.

Physical review letters·2026
Same author

Fully Collective Superradiant Lasing with Vanishing Sensitivity to Cavity Length Vibrations.

Physical review letters·2026
Same author

Decoherence Cancellation through Noise Interference.

Physical review letters·2026
Same author

From Light-Cone to Supersonic Propagation of Correlations by Competing Short- and Long-Range Couplings.

Physical review letters·2025
Same author

Causality, localization, and universality of monitored quantum walks with long-range hopping.

Physical review. E·2025
Same author

Stability and decay of subradiant patterns in a quantum gas with photon-mediated interactions.

Science advances·2025

Related Experiment Video

Updated: Mar 15, 2026

Gradient Echo Quantum Memory in Warm Atomic Vapor
10:00

Gradient Echo Quantum Memory in Warm Atomic Vapor

Published on: November 11, 2013

13.3K

Dissipation-Assisted Prethermalization in Long-Range Interacting Atomic Ensembles.

Stefan Schütz1, Simon B Jäger1, Giovanna Morigi1

  • 1Theoretische Physik, Universität des Saarlandes, D-66123 Saarbrücken, Germany.

Physical Review Letters
|September 3, 2016
PubMed
Summary
This summary is machine-generated.

We found that dissipation significantly extends prethermalization in driven-dissipative atomic systems. This effect, driven by momentum-position correlations, slows down thermalization in long-range interacting many-body systems.

More Related Videos

Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving
11:21

Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving

Published on: March 30, 2017

7.9K
Non-equilibrium Microwave Plasma for Efficient High Temperature Chemistry
07:17

Non-equilibrium Microwave Plasma for Efficient High Temperature Chemistry

Published on: August 1, 2017

13.3K

Related Experiment Videos

Last Updated: Mar 15, 2026

Gradient Echo Quantum Memory in Warm Atomic Vapor
10:00

Gradient Echo Quantum Memory in Warm Atomic Vapor

Published on: November 11, 2013

13.3K
Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving
11:21

Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving

Published on: March 30, 2017

7.9K
Non-equilibrium Microwave Plasma for Efficient High Temperature Chemistry
07:17

Non-equilibrium Microwave Plasma for Efficient High Temperature Chemistry

Published on: August 1, 2017

13.3K

Area of Science:

  • Atomic physics
  • Quantum optics
  • Condensed matter theory

Background:

  • Driven-dissipative systems exhibit complex phase transitions.
  • Long-range interactions and cavity mediation are crucial in atomic ensembles.
  • Understanding relaxation dynamics after a quantum quench is key.

Purpose of the Study:

  • To theoretically characterize semiclassical dynamics after a quench across a driven-dissipative phase transition.
  • To investigate the role of coherent and dissipative long-range forces.
  • To explore the impact of dissipation on prethermalization and thermalization timescales.

Main Methods:

  • Semiclassical dynamics simulation.
  • Theoretical analysis of driven-dissipative systems.
  • Investigation of long-range interacting many-body systems.

Main Results:

  • A long prethermalizing behavior dominated first by coherent forces, then by their interplay with dissipation.
  • Dissipation-assisted prethermalization is orders of magnitude longer than coherent dynamics.
  • Creation of non-mean-field momentum-position correlations.

Conclusions:

  • Dissipation substantially slows down thermalization in long-range interacting systems.
  • Cavity cooling into self-organized phases may require longer experimental timescales.
  • Noise and dissipation play a critical role in the dynamics of many-body systems.