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Work statistics of sudden quantum quenches: A random matrix theory perspective on Gaussianity and its deviations

This paper demonstrates that the work distribution for sudden quantum quenches in translation-invariant quadratic fermionic chains can be mapped to the statistics of traces of Haar unitary matrices, yielding a Gaussian distribution via multivariate central limit theorems while also characterizing the specific conditions—such as long-range interactions or Fisher-Hartwig singularities—that lead to non-Gaussian deviations.

Original authors: Miguel Tierz

Published 2026-10-15
📖 6 min read🧠 Deep dive

Original authors: Miguel Tierz

Original paper licensed under CC BY 4.0 (http://creativecommons.org/licenses/by/4.0/). ✨ This is an AI-generated explanation of the paper below. It is not written or endorsed by the authors. For technical accuracy, refer to the original paper. Read full disclaimer

In the world of physics, energy is rarely a static number; it is a story of change. When a system is pushed out of balance, it absorbs or releases energy, and scientists call this exchange "work." In the classical world, we can track this energy like a bank account, knowing exactly how much was spent and how much remains. But in the quantum realm, where particles exist in a haze of probabilities, the concept of work becomes slippery. It is not a single, fixed value that can be measured at a glance. Instead, it is a fluctuating quantity, a random variable that changes every time an experiment is run. To understand the behavior of these quantum systems, researchers must look not just at the average amount of energy transferred, but at the entire landscape of possibilities: how often the system takes a little energy, how often it takes a lot, and how the shape of these fluctuations reveals the hidden rules of the material.

This is the territory explored by Miguel Tierz in a new study focusing on "sudden quenches." Imagine a quantum system sitting quietly in its lowest energy state, and then, in an instant, the rules of the game are changed. Perhaps the magnetic field holding the atoms in place is switched off, or the strength of the bonds between them is altered. The system is suddenly forced to evolve under these new conditions. This abrupt change is the quench. The question Tierz tackles is simple yet profound: when this happens, what is the statistical pattern of the work done on the system? Does the energy transfer follow a predictable, bell-shaped curve, or does it behave in wilder, more unpredictable ways?

The answer, the research shows, depends entirely on the nature of the connections between the particles in the system. Tierz discovered that for a vast class of quantum materials, specifically those where particles interact only with their immediate neighbors in a regular pattern, the work distribution is remarkably orderly. It forms a perfect bell curve, known as a Gaussian distribution. This means that while the exact amount of work varies from one experiment to the next, the variations are well-behaved and centered around a specific average. The researchers found that this order emerges because the quantum system, when viewed through the lens of random matrix theory, behaves like a collection of independent, random waves. Just as the average of many coin flips settles into a predictable pattern, the sum of these quantum fluctuations settles into a smooth, Gaussian shape. The size of the fluctuations is determined by the strength of the interactions between the particles, a relationship that can be calculated precisely from the system's design.

However, the story changes when the connections between particles become long-range or when the system is pushed to the edge of a phase transition. The study reveals that the neat bell curve is not a universal law; it is a fragile state that breaks down under specific conditions. If the particles interact with neighbors far away from them, or if the strength of these interactions fades very slowly with distance, the work distribution develops heavy, non-Gaussian tails. In these scenarios, extreme events—where the system absorbs or releases a massive amount of energy—become much more likely than the standard bell curve would predict. Similarly, if the quench pushes the system across a critical point, a threshold where the material's fundamental nature changes, the distribution develops sharp, structured irregularities. These deviations are not random noise; they are signatures of deep physical phenomena, such as the emergence of new types of order or the breakdown of standard statistical rules.

To reach these conclusions, Tierz employed a powerful mathematical trick that translates the complex problem of quantum work into the language of random matrices. Instead of tracking the chaotic motion of billions of particles, the problem is mapped onto the properties of a special kind of random matrix, a mathematical object where the entries are chosen from a uniform distribution. In this new language, the work done on the system corresponds to the sum of the traces of powers of these matrices. This transformation is crucial because it allows the use of rigorous statistical tools that have been developed over decades to understand how these random matrices behave. The research confirms that for systems with short-range interactions, the mathematical conditions for a Gaussian distribution are always met, guaranteeing the bell curve. But when the interactions are long-range or the system is critical, these conditions fail, and the distribution reveals its true, more complex character.

The implications of this work extend beyond abstract theory. The shape of the work distribution tells us how difficult it is to predict the behavior of a quantum system and how efficiently it can be controlled. In the Gaussian regime, the system is predictable, and the energy costs are well-defined. But in the non-Gaussian regimes, rare, extreme events dominate the statistics, making the system much harder to manage and its energy costs much more volatile. This distinction is vital for the development of quantum technologies, where controlling energy flow is essential. The study also draws a surprising parallel to another area of quantum physics: entanglement. The same mathematical features that cause the work distribution to become non-Gaussian are also responsible for unusual patterns in how quantum particles become linked to one another. This suggests that by measuring the fluctuations of work, scientists might be able to detect these deep quantum correlations without needing to measure the particles directly.

Ultimately, this research provides a clear map for when quantum systems behave simply and when they behave wildly. It shows that the familiar bell curve of statistics is not the default state of the quantum world, but a special case that arises only when interactions are local and well-behaved. When the connections stretch too far or the system teeters on the edge of change, the rules shift, and the work distribution reveals a richer, more complex landscape. By identifying the precise conditions that lead to these deviations, the study offers a new way to diagnose the health and complexity of quantum materials, turning the measurement of energy fluctuations into a powerful tool for exploring the frontiers of quantum matter.

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