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

The Quantum-Mechanical Model of an Atom02:45

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...
First Law: Particles in One-dimensional Equilibrium01:10

First Law: Particles in One-dimensional Equilibrium

Newton's first law of motion states that a body at rest remains at rest, or if in motion, remains in motion at constant velocity, unless acted on by a net external force. It also states that there must be a cause for any change in velocity (a change in either magnitude or direction) to occur. This cause is a net external force. For example, consider what happens to an object sliding along a rough horizontal surface. The object quickly grinds to a halt, due to the net force of friction. If we...
Free Energy Changes for Nonstandard States03:25

Free Energy Changes for Nonstandard States

The free energy change for a process taking place with reactants and products present under nonstandard conditions (pressures other than 1 bar; concentrations other than 1 M) is related to the standard free energy change according to this equation:
First Law: Particles in Two-dimensional Equilibrium01:18

First Law: Particles in Two-dimensional Equilibrium

Recall that a particle in equilibrium is one for which the external forces are balanced. Static equilibrium involves objects at rest, and dynamic equilibrium involves objects in motion without acceleration; but it is important to remember that these conditions are relative. For instance, an object may be at rest when viewed from one frame of reference, but that same object would appear to be in motion when viewed by someone moving at a constant velocity.
Newton's first law tells us about the...
Entropy Change in Reversible Processes01:10

Entropy Change in Reversible Processes

In the Carnot engine, which achieves the maximum efficiency between two reservoirs of fixed temperatures, the total change in entropy is zero. The observation can be generalized by considering any reversible cyclic process consisting of many Carnot cycles. Thus, it can be stated that the total entropy change of any ideal reversible cycle is zero.
The statement can be further generalized to prove that entropy is a state function. Take a cyclic process between any two points on a p-V diagram.
Fermi Level Dynamics01:12

Fermi Level Dynamics

The vacuum level denotes the energy threshold required for an electron to escape from a material surface. It is usually positioned above the conduction band of a semiconductor and acts as a benchmark for comparing electron energies within various materials.
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...

You might also read

Related Articles

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

Sort by
Same author

A universal constraint for relaxation rates for quantum Markov generators: complete positivity and beyond<sup></sup>.

Reports on progress in physics. Physical Society (Great Britain)·2025
Same author

A mirrored pair of optimal non-decomposable entanglement witnesses for two qudits does exist.

Scientific reports·2025
Same author

A class of entanglement witnesses and a realignment-like criterion.

Scientific reports·2025
Same author

On the structure of mirrored operators obtained from optimal entanglement witnesses.

Scientific reports·2023
Same author

On Markovianity and classicality in multilevel spin-boson models.

Scientific reports·2023
Same author

Strongly coupled quantum Otto cycle with single qubit bath.

Physical review. E·2023

Related Experiment Video

Updated: Jun 14, 2026

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids
11:03

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids

Published on: December 4, 2017

Non-Markovian quantum dynamics: local versus nonlocal.

Dariusz Chruściński1, Andrzej Kossakowski

  • 1Institute of Physics, Nicolaus Copernicus University, Grudziadzka 5/7, 87-100 Toruń, Poland.

Physical Review Letters
|April 7, 2010
PubMed
Summary

We analyze non-Markovian evolution in open quantum systems. Our findings show that dynamics can be described by either nonlocal or local equations, revealing key aspects of quantum memory effects.

Area of Science:

  • Quantum Physics
  • Quantum Information Science

Background:

  • Open quantum systems exhibit complex dynamics.
  • Non-Markovian evolution is crucial for understanding quantum information processing.

Purpose of the Study:

  • To analyze the non-Markovian evolution of open quantum systems.
  • To explore complementary descriptions of quantum dynamics.

Main Methods:

  • Analysis of dynamical maps.
  • Development of nonlocal master equations with memory kernels.
  • Formulation of time-local equations.

Main Results:

  • Any dynamical map can be described by nonlocal or time-local equations.
  • These descriptions are complementary, with complexity shifting between them.

More Related Videos

Quantum State Engineering of Light with Continuous-wave Optical Parametric Oscillators
09:23

Quantum State Engineering of Light with Continuous-wave Optical Parametric Oscillators

Published on: May 30, 2014

Related Experiment Videos

Last Updated: Jun 14, 2026

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids
11:03

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids

Published on: December 4, 2017

Quantum State Engineering of Light with Continuous-wave Optical Parametric Oscillators
09:23

Quantum State Engineering of Light with Continuous-wave Optical Parametric Oscillators

Published on: May 30, 2014

  • The time-local generator retains memory of the initial time, defining non-Markovianity.
  • Singularities in the generator can lead to phenomena like coherence revival and entanglement dynamics.
  • Conclusions:

    • Non-Markovian quantum dynamics can be equivalently described by nonlocal or time-local formalisms.
    • The time-local approach inherently captures memory effects essential for non-Markovianity.
    • Generator singularities in the local description are linked to observable quantum phenomena.