Related Experiment Videos
Absorbing state dynamics of stochastic gradient descent
Guanming Zhang1,2, Stefano Martiniani1,2,3,4
1New York University, Center for Soft Matter Research, Department of Physics, New York 10003, USA.
Physical Review. E
|July 24, 2026
Summary
Stochastic gradient descent (SGD) in machine learning mirrors particle dynamics, revealing connections to statistical physics. This study links SGD to biased random organization models, showing equivalence in certain limits and offering insights into generalization.
Area of Science:
- Statistical Physics
- Machine Learning
- Stochastic Optimization
Background:
- Stochastic gradient descent (SGD) is a cornerstone of machine learning and stochastic optimization.
- Understanding SGD's behavior is crucial for advancing AI and complex system modeling.
- Existing frameworks often lack direct links to physical processes.
Purpose of the Study:
- To investigate Stochastic Gradient Descent (SGD) through the framework of particle dynamics.
- To establish a connection between SGD and models from nonequilibrium statistical physics.
- To analyze the phase transition behavior of SGD in a simplified physical model.
Main Methods:
- Developed a minimal physical model of spherical particles undergoing SGD to minimize energy.
- Employed the biased random organization (BRO) model, a nonequilibrium absorbing state model, to describe SGD dynamics.
- Analyzed particle interactions, noise mechanisms, and critical phenomena near phase transitions.
Main Results:
- SGD dynamics were shown to be approximable by particles with linear repulsive interactions under anisotropic noise.
- In the small learning rate limit, SGD and BRO dynamics for repulsive particles become equivalent, converging to a critical packing fraction (ϕ_{c}≈0.64).
- Both models exhibit critical behavior consistent with the Manna universality class.
Conclusions:
- SGD's behavior can be effectively described using concepts from nonequilibrium statistical physics, specifically BRO dynamics.
- The equivalence between SGD and BRO near criticality provides a novel physical interpretation of optimization processes.
- SGD's tendency to favor flatter energy landscapes, observed above the transition, correlates with improved generalization in neural network training.
Related Concept Videos
Reaction Mechanisms: The Steady-State Approximation
The steady-state approximation, also referred to as the quasi-steady-state approximation to differentiate it from a true steady state, is a widely used method for simplifying calculations in complex reaction mechanisms. This approach is particularly useful when dealing with multi-step reactions that involve reverse reactions or several steps, which can significantly increase mathematical complexity and make the reactions nearly unsolvable analytically.The steady-state approximation operates on...
State Function, Exact and Inexact Differentials
A state function is a thermodynamic property that depends solely on the current state of a system, irrespective of its history or how it arrived at that state. These functions are represented by capital letters, such as U, H, and S, which stand for internal energy, enthalpy, and entropy, respectively.For instance, the value of internal energy depends on the system's state variables and remains unaffected by the process path. This means that whether the system underwent a linear process or a...
Maximizing the Directional Derivative
The directional derivative is a central concept in multivariable calculus that describes how a function changes at a given point when moving in a specified direction. This direction is represented by a unit vector, ensuring that only the orientation influences the rate of change. By varying the direction, different rates of change can be observed, demonstrating that the directional derivative depends strongly on the chosen direction.The directional derivative is computed using the gradient...
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.
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.
The Entropy as a State Function
Consider an arbitrary process that moves between two specific states (A and B) in a cyclic manner. This process is reversible and broken down into smaller parts that each follow a Carnot cycle. A Carnot cycle has two isothermal (constant temperature) processes. During these processes, the ratio of the amount of heat transferred to their respective temperature remains constant. The other two processes in the Carnot cycle are also reversible but adiabatic, which means they occur without any heat...
State Space Representation
The frequency-domain technique, commonly used in analyzing and designing feedback control systems, is effective for linear, time-invariant systems. However, it falls short when dealing with nonlinear, time-varying, and multiple-input multiple-output systems. The time-domain or state-space approach addresses these limitations by utilizing state variables to construct simultaneous, first-order differential equations, known as state equations, for an nth-order system.
Consider an RLC circuit, a...
Consider an RLC circuit, a...