Related Experiment Video
Updated: Feb 10, 2026

10:00
Gradient Echo Quantum Memory in Warm Atomic Vapor
Published on: November 11, 2013
13.2K
Detailed Balance of Thermalization Dynamics in Rydberg-Atom Quantum Simulators.
Hyosub Kim1, YeJe Park1, Kyungtae Kim1
1Department of Physics, KAIST, Daejeon 34141, Korea.
Physical Review Letters
|May 19, 2018
Summary
Researchers demonstrate that thermalization in isolated quantum systems follows a master equation. This finding, observed in quantum Ising-like models, shows detailed balance without external baths or randomness.
Area of Science:
- Quantum physics
- Statistical mechanics
- Complex systems
Background:
- Large complex systems often follow master equations for equilibrium dynamics.
- Understanding thermalization in isolated quantum systems is a key challenge.
Purpose of the Study:
- To investigate if thermalization of isolated many-body quantum states can be described by a master equation.
- To experimentally demonstrate detailed balance in quantum thermalization dynamics.
Main Methods:
- Utilized a quantum simulator with defect-free single-atom tweezers and Rydberg-atom interactions.
- Implemented sudden quench dynamics in quantum Ising-like models.
- Experimentally constructed a master equation by monitoring prequench state occupation probabilities and applying detailed balance.
Main Results:
- Observed that the saturation of local observables, a signature of thermalization, obeys a master equation.
- Demonstrated detailed balance in the thermalization dynamics of an isolated quantum system.
- Results align with theoretical predictions.
Conclusions:
- Thermalization in isolated quantum many-body systems can be accurately described by a master equation.
- Detailed balance can be achieved in quantum systems without coupling to external baths or invoking randomness.
- The study provides experimental evidence for fundamental principles of quantum statistical mechanics.
Related Concept Videos
The Quantum-Mechanical Model of an Atom
59.5K
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.
59.5K
Quantum Numbers
52.1K
It is said that the energy of an electron in an atom is quantized; that is, it can be equal only to certain specific values and can jump from one energy level to another but not transition smoothly or stay between these levels.
52.1K
Atomic Orbitals
44.9K
An atomic orbital represents the three-dimensional regions in an atom where an electron has the highest probability to reside. The radial distribution function indicates the total probability of finding an electron within the thin shell at a distance r from the nucleus. The atomic orbitals have distinct shapes which are determined by l, the angular momentum quantum number. The orbitals are often drawn with a boundary surface, enclosing densest regions of the cloud.
44.9K
Balancing Redox Equations
62.3K
Electrochemistry is the science involved in the interconversion of electrical and chemical reactions. Such reactions are called reduction-oxidation, or redox reactions. These important reactions are defined by changes in oxidation states for one or more reactant elements and include a subset of reactions involving the transfer of electrons between reactant species. Electrochemistry as a field has evolved to yield sufficient insights on the fundamental principles of redox chemistry and multiple...
62.3K
Atomic Radii and Effective Nuclear Charge
62.3K
The elements in groups of the periodic table exhibit similar chemical behavior. This similarity occurs because the members of a group have the same number and distribution of electrons in their valence shells.
62.3K
Atomic Structure
211.1K
Overview
211.1K

