The minimum regret path problem on stochastic fuzzy time-varying networks

Wei Huang1, Zhilei Xu1, Liehuang Zhu1

  • 1School of Cyberspace Science and Technology, Beijing Institute of Technology, 100081 Beijing, China.

Insights

We introduce a stochastic fuzzy time-varying minimum regret path problem and propose a novel random fuzzy delay neural network (RFDNN) to solve it efficiently. The RFDNN demonstrates superior performance in finding minimum regret paths in complex networks.

Area of Science:

  • Operations Research
  • Artificial Intelligence
  • Network Science

Background:

  • Stochastic fuzzy time-varying networks present challenges for pathfinding due to uncertainty and dynamic edge weights.
  • Existing shortest path algorithms may not adequately address the 'minimum regret' criterion in such complex environments.

Purpose of the Study:

  • To introduce and define the stochastic fuzzy time-varying minimum regret path problem (SFTMRP).
  • To develop a novel, training-free neural network approach for solving the SFTMRP.

Main Methods:

  • The proposed Random Fuzzy Delay Neural Network (RFDNN) utilizes specialized neurons with six distinct layers.
  • Information exchange within the RFDNN involves shortest path and maximum probability solution signals.
  • Theoretical analysis covers time-complexity and correctness, validated by numerical examples.

Main Results:

  • The RFDNN effectively addresses the SFTMRP by finding paths with minimal regret.
  • Experimental results on stochastic fuzzy time-varying road networks show significant performance improvements over existing methods.
  • The algorithm's efficiency was tested on networks with 1000-5000 nodes.

Conclusions:

  • The RFDNN is a viable and efficient method for solving the SFTMRP.
  • This approach offers a significant advancement in finding optimal paths in uncertain, dynamic network conditions.

Related Concept Videos

Propagation of Uncertainty from Random Error00:59

Propagation of Uncertainty from Random Error

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...
1.1K
Propagation of Uncertainty from Systematic Error01:10

Propagation of Uncertainty from Systematic Error

The atomic mass of an element varies due to the relative ratio of its isotopes. A sample's relative proportion of oxygen isotopes influences its average atomic mass. For instance, if we were to measure the atomic mass of oxygen from a sample, the mass would be a weighted average of the isotopic masses of oxygen in that sample. Since a single sample is not likely to perfectly reflect the true atomic mass of oxygen for all the molecules of oxygen on Earth, the mass we obtain from this...
874
Woodward–Hoffmann Selection Rules and Microscopic Reversibility01:34

Woodward–Hoffmann Selection Rules and Microscopic Reversibility

Electrocyclic reactions, cycloadditions, and sigmatropic rearrangements are concerted pericyclic reactions that proceed via a cyclic transition state. These reactions are stereospecific and regioselective. The stereochemistry of the products depends on the symmetry characteristics of the interacting orbitals and the reaction conditions. Accordingly, pericyclic reactions are classified as either symmetry-allowed or symmetry-forbidden. Woodward and Hoffmann presented the selection criteria for...
3.3K
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.
2.7K
Parameters Affecting Nonlinear Elimination: Zero-Order Input, First-Order Absorption and Two-Compartment Model01:13

Parameters Affecting Nonlinear Elimination: Zero-Order Input, First-Order Absorption and Two-Compartment Model

Drugs administered through various routes can lead to nonlinear elimination, resulting in complex pharmacokinetic behaviors crucial to understanding efficacious drug dosing.
When a drug is administered through a constant intravenous infusion and eliminated via nonlinear pharmacokinetics, it follows zero-order input. For example, oral drugs undergo first-order absorption upon administration and are eliminated through nonlinear pharmacokinetics.
In the case of subcutaneously administered drugs,...
125
Linear time-invariant Systems01:23

Linear time-invariant Systems

A system is linear if it displays the characteristics of homogeneity and additivity, together termed the superposition property. This principle is fundamental in all linear systems. Linear time-invariant (LTI) systems include systems with linear elements and constant parameters.
The input-output behavior of an LTI system can be fully defined by its response to an impulsive excitation at its input. Once this impulse response is known, the system's reaction to any other input can be...
392