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

Poisson's And Laplace's Equation01:25

Poisson's And Laplace's Equation

4.1K
The electric potential of the system can be calculated by relating it to the electric charge densities that give rise to the electric potential. The differential form of Gauss's law expresses the electric field's divergence in terms of the electric charge density.
4.1K
Exponential Fourier series01:24

Exponential Fourier series

629
In audio signal processing, the exponential Fourier series plays a crucial role in sound synthesis, allowing complex sounds to be broken down into simpler sinusoidal components. This decomposition process is fundamental in analyzing and reconstructing musical notes and other audio signals. The exponential Fourier series expresses periodic signals as the sum of complex exponentials at both positive and negative harmonic frequencies, providing a powerful tool for signal analysis.
Euler's identity...
629
Random Variables01:09

Random Variables

17.2K
A random variable is a single numerical value that indicates the outcome of a procedure. The concept of random variables is fundamental to the probability theory and was introduced by a Russian mathematician, Pafnuty Chebyshev, in the mid-nineteenth century.
Uppercase letters such as X or Y denote a random variable. Lowercase letters like x or y denote the value of a random variable. If X is a random variable, then X is written in words, and x is given as a number.
For example, let X = the...
17.2K
Propagation of Uncertainty from Random Error00:59

Propagation of Uncertainty from Random Error

1.6K
An experiment often consists of more than a single step. In this case, measurements at each step give rise to uncertainty. Because the measurements occur in successive steps, the uncertainty in one step necessarily contributes to that in the subsequent step. As we perform statistical analysis on these types of experiments, we must learn to account for the propagation of uncertainty from one step to the next. The propagation of uncertainty depends on the type of arithmetic operation performed on...
1.6K
Fermi Level Dynamics01:12

Fermi Level Dynamics

629
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...
629
Entropy Change in Reversible Processes01:10

Entropy Change in Reversible Processes

3.2K
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.
3.2K

You might also read

Related Articles

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

Sort by
Same author

Controlled Growth of Rare-Earth-Doped TiO<sub>2</sub> Thin Films on III-V Semiconductors for Hybrid Quantum Photonic Interfaces.

ACS applied optical materials·2026
Same author

Optimization of iterative wavefront shaping algorithms for quantum light.

Optics letters·2026
Same author

Engineering Nanohole-Etched Quantum Dots for Telecom-Band Single-Photon Generation.

ACS nano·2026
Same author

Controlling the degree of entanglement in downconversion by targeted birth zone activation.

Optics express·2025
Same author

Feature engineering driven estimation of <i>C</i><sub><i>n</i></sub><sup>2</sup> from deformed optical signals using neural networks.

Journal of the Optical Society of America. A, Optics, image science, and vision·2025
Same author

Controlling the transmission of broadband light through scattering media using a digital micromirror device.

Optics letters·2023

Related Experiment Videos

Exponentially tempered Lévy sums in random lasers.

Ravitej Uppu1, Sushil Mujumdar1

  • 1Nano-optics and Mesoscopic Optics Laboratory, Tata Institute of Fundamental Research, 1, Homi Bhabha Road, Mumbai 400 005, India.

Physical Review Letters
|May 23, 2015
PubMed
Summary

Truncated Lévy flights, a process limiting extreme fluctuations, are perfectly manifested in coherent random lasers. This explains the statistical behavior of nonresonant random lasers, validated by rigorous parameter estimation.

Related Experiment Videos

Area of Science:

  • Physics
  • Nonlinear Dynamics
  • Statistical Mechanics

Background:

  • Lévy fluctuations present mathematical challenges due to diverging moments.
  • Truncated Lévy flights address these infinities by restricting fluctuation magnitudes.
  • Understanding random laser behavior is crucial for developing novel light sources.

Purpose of the Study:

  • To demonstrate the occurrence of truncated Lévy flights in coherent random lasers.
  • To establish truncated Lévy flights as the underlying explanation for nonresonant random laser statistics.
  • To perform rigorous parameter estimation for truncated Lévy flight models in random lasers.

Main Methods:

  • Modeling random laser intensity using exponentially tempered Lévy sums.
  • Implementing rigorous parameter estimation for summand variables, truncation, and power-law exponents.
  • Comparing theoretical models with experimental data on fluctuation behavior.

Main Results:

  • A perfect manifestation of truncated Lévy flights was observed in coherent random lasers.
  • The truncated Lévy flight model accurately explains the complete statistical behavior of nonresonant random lasers.
  • Parameter estimation showed excellent agreement between computed and experimentally observed fluctuation behaviors.

Conclusions:

  • Truncated Lévy flights provide a unified explanation for random laser statistical properties.
  • The study validates the application of truncated Lévy flight models in physical systems.
  • This research bridges theoretical concepts in stochastic processes with experimental observations in random lasers.