Related Experiment Video
Updated: Feb 15, 2026

08:48
Demonstration of Spin-Multiplexed and Direction-Multiplexed All-Dielectric Visible Metaholograms
Published on: September 25, 2020
6.3K
Finite connected components in infinite directed and multiplex networks with arbitrary degree distributions
1Van 't Hoff Institute for Molecular Sciences, University of Amsterdam, PO Box 94214, 1090 GE Amsterdam, Netherlands.
Physical Review. E
|January 20, 2018
Summary
This study provides exact formulas for component sizes in directed and multiplex networks. These findings reveal critical exponents governing network behavior, offering new insights into complex systems.
Area of Science:
- Network Science
- Statistical Physics
- Complex Systems
Background:
- Understanding the structure of complex networks is crucial in various scientific fields.
- Existing models often simplify network topology, limiting applicability to real-world systems.
- Characterizing connected components in generalized network models remains an active research area.
Purpose of the Study:
- To derive exact expressions for the size distributions of weakly and multilayer connected components.
- To analyze these distributions in two generalized network models: directed and multiplex networks.
- To investigate the critical behavior and exponents of these size distributions.
Main Methods:
- Development of exact analytical expressions for component size distributions.
- Application of the configuration model generalizations for directed and multiplex networks.
- Asymptotic analysis to determine critical exponents under specific conditions.
Main Results:
- Derived computable, polynomial-time expressions for size distributions.
- Identified specific critical exponents (-3/2) for two-layer connected components in multiplex networks.
- Revealed two critical exponents (-1/2 and -3/2) for weakly connected components in directed networks.
Conclusions:
- The derived expressions provide a precise framework for analyzing network components.
- The findings offer quantitative insights into the phase transitions and critical phenomena in these network types.
- This work advances the theoretical understanding of complex network structures and their properties.
Related Concept Videos
One-Degree-of-Freedom System
869
In mechanical engineering, one-degree-of-freedom systems form the basis of a wide range of electrical and mechanical components. Using these models, engineers can predict the behavior of various parts in a larger system, which gives them insight into how different forces interact with each other.
A one-degree-of-freedom system is defined by an independent variable that determines its state and behavior. One example of a one-degree-of-freedom system is a simple harmonic oscillator, such as a...
A one-degree-of-freedom system is defined by an independent variable that determines its state and behavior. One example of a one-degree-of-freedom system is a simple harmonic oscillator, such as a...
869
Degrees of Freedom
7.3K
The degree of freedom for a particular statistical calculation is the number of values that are free to vary. Thus, the minimum number of independent numbers can specify a particular statistic. The degrees of freedom differ greatly depending on known and uncalculated statistical components.
For example, suppose there are three unknown numbers whose mean is 10; although we can freely assign values to the first and second numbers, the value of the last number can not be arbitrarily assigned.
For example, suppose there are three unknown numbers whose mean is 10; although we can freely assign values to the first and second numbers, the value of the last number can not be arbitrarily assigned.
7.3K
Degrees of Freedom
10.4K
The degree of freedom for a particular statistical calculation is the number of values that are free to vary. As a result, the minimum number of independent numbers can specify a particular statistic. The degrees of freedom differ greatly depending on known and uncalculated statistical components.
For example, suppose there are three unknown numbers whose mean is 10; although we can freely assign values to the first and second numbers, the value of the last number can not be arbitrarily...
For example, suppose there are three unknown numbers whose mean is 10; although we can freely assign values to the first and second numbers, the value of the last number can not be arbitrarily...
10.4K
Improper Integrals: Infinite Intervals
118
An integral is classified as improper due to an infinite interval when at least one of its limits of integration extends to positive or negative infinity. In such cases, the region under the curve is unbounded, and standard techniques for evaluating definite integrals are not directly applicable. Instead, the improper integral is defined through a limiting process that allows one to determine whether the accumulated area remains finite despite the infinite domain.Application to Exponential...
118
Protein Networks
4.6K
An organism can have thousands of different proteins, and these proteins must cooperate to ensure the health of an organism. Proteins bind to other proteins and form complexes to carry out their functions. Many proteins interact with multiple other proteins creating a complex network of protein interactions.
These interactions can be represented through maps depicting protein-protein interaction networks, represented as nodes and edges. Nodes are circles that are representative of a protein,...
These interactions can be represented through maps depicting protein-protein interaction networks, represented as nodes and edges. Nodes are circles that are representative of a protein,...
4.6K
Degree of Unsaturation
10.8K
The degree of unsaturation (U), or index of hydrogen deficiency (IHD), is defined as the difference in the number of pairs of hydrogen atoms between the compound and the acyclic alkane with the same number of carbon atoms. Each double bond or ring costs two hydrogen atoms compared to a saturated analog and results in one degree of unsaturation.
The degree of unsaturation for hydrocarbons is U = (2C + 2 − H) / 2, where C is the number of carbon atoms and H is the number of hydrogen atoms.
The degree of unsaturation for hydrocarbons is U = (2C + 2 − H) / 2, where C is the number of carbon atoms and H is the number of hydrogen atoms.
10.8K

