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 de Broglie Wavelength02:32

The de Broglie Wavelength

34.8K
In the macroscopic world, objects that are large enough to be seen by the naked eye follow the rules of classical physics. A billiard ball moving on a table will behave like a particle; it will continue traveling in a straight line unless it collides with another ball, or it is acted on by some other force, such as friction. The ball has a well-defined position and velocity or well-defined momentum, p = mv, which is defined by mass m and velocity v at any given moment. This is the typical...
34.8K
The Uncertainty Principle04:08

The Uncertainty Principle

34.9K
Werner Heisenberg considered the limits of how accurately one can measure properties of an electron or other microscopic particles. He determined that there is a fundamental limit to how accurately one can measure both a particle’s position and its momentum simultaneously. The more accurate the measurement of the momentum of a particle is known, the less accurate the position at that time is known and vice versa. This is what is now called the Heisenberg uncertainty principle. He...
34.9K
Atomic Nuclei: Nuclear Spin State Population Distribution01:14

Atomic Nuclei: Nuclear Spin State Population Distribution

2.6K
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.
2.6K
The Quantum-Mechanical Model of an Atom02:45

The Quantum-Mechanical Model of an Atom

62.0K
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...
62.0K
Basic Postulates of Kinetic Molecular Theory: Particle Size, Energy, and Collision02:43

Basic Postulates of Kinetic Molecular Theory: Particle Size, Energy, and Collision

39.3K
The ideal-gas equation, which is empirical, describes the behavior of gases by establishing relationships between their macroscopic properties. For example, Charles’ law states that volume and temperature are directly related. Gases, therefore, expand when heated at constant pressure. Although gas laws explain how the macroscopic properties change relative to one another, it does not explain the rationale behind it.
39.3K
The Bohr Model02:18

The Bohr Model

84.3K
Following the work of Ernest Rutherford and his colleagues in the early twentieth century, the picture of atoms consisting of tiny dense nuclei surrounded by lighter and even tinier electrons continually moving about the nucleus was well established. This picture was called the planetary model since it pictured the atom as a miniature “solar system” with the electrons orbiting the nucleus like planets orbiting the sun. The simplest atom is hydrogen, consisting of a single proton as...
84.3K

You might also read

Related Articles

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

Sort by
Same author

Experimental observation of counter-intuitive features of photonic bunching.

Light, science & applications·2026
Same author

High-efficiency free-space optical communication link with refractive adaptive optics.

Optics express·2026
Same author

Multiparameter quantum-enhanced adaptive metrology with squeezed light.

Nature communications·2026
Same author

Experimental data reuploading with provable enhanced learning capabilities.

Science advances·2026
Same author

Multiphoton Quantum Simulation of the Generalized Hopfield Memory Model.

Physical review letters·2026
Same author

Amplitude- and Phase-Programmable Dual-Color Photonic Chip for High-Contrast Structured Illumination Microscopy.

ACS photonics·2026

Related Experiment Video

Updated: Apr 16, 2026

Measurement of Quantum Interference in a Silicon Ring Resonator Photon Source
12:19

Measurement of Quantum Interference in a Silicon Ring Resonator Photon Source

Published on: April 4, 2017

9.0K

Particle statistics affects quantum decay and Fano interference.

Andrea Crespi1, Linda Sansoni2, Giuseppe Della Valle1,3

  • 1Istituto di Fotonica e Nanotecnologie, Consiglio Nazionale delle Ricerche, Piazza Leonardo da Vinci 32, I-20133 Milano, Italy.

Physical Review Letters
|March 21, 2015
PubMed
Summary
This summary is machine-generated.

Particle statistics significantly influence quantum decay. Bosons exhibit fractional decay due to bound states in the continuum, while fermions experience complete decay because of the Pauli exclusion principle.

More Related Videos

Measurement of Coherence Decay in GaMnAs Using Femtosecond Four-wave Mixing
15:58

Measurement of Coherence Decay in GaMnAs Using Femtosecond Four-wave Mixing

Published on: December 3, 2013

6.2K
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

15.2K

Related Experiment Videos

Last Updated: Apr 16, 2026

Measurement of Quantum Interference in a Silicon Ring Resonator Photon Source
12:19

Measurement of Quantum Interference in a Silicon Ring Resonator Photon Source

Published on: April 4, 2017

9.0K
Measurement of Coherence Decay in GaMnAs Using Femtosecond Four-wave Mixing
15:58

Measurement of Coherence Decay in GaMnAs Using Femtosecond Four-wave Mixing

Published on: December 3, 2013

6.2K
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

15.2K

Area of Science:

  • Quantum mechanics
  • Quantum optics
  • Many-body physics

Background:

  • Quantum mechanical decay, Fano interference, and bound states in the continuum are fundamental phenomena across physics.
  • Understanding multiparticle quantum decay is crucial for various quantum technologies.

Purpose of the Study:

  • To experimentally investigate the influence of particle statistics on quantum mechanical decay in a multiparticle system.
  • To simulate quantum decay in a two-photon system within a Fano-Anderson model.

Main Methods:

  • Propagation of two-photon states in engineered photonic lattices.
  • Simulation of quantum decay for two non-interacting particles in a multilevel Fano-Anderson model.
  • Experimental observation of decay dynamics for bosonic and fermionic particles.

Main Results:

  • Fractional quantum mechanical decay was observed for bosonic particles when a bound state in the continuum was present.
  • Complete quantum mechanical decay was observed for fermionic particles under identical conditions.
  • The Pauli exclusion principle was identified as the cause for complete decay in fermions, preventing occupation of the bound state.

Conclusions:

  • Particle statistics profoundly affect quantum mechanical decay in multiparticle systems.
  • The presence of a bound state in the continuum, combined with particle statistics, can tune decay from fractional to complete.
  • Experimental findings highlight the role of quantum statistics in controlling quantum decay processes.