Quantum ‘birthmarks’ hold lasting traces of a system’s past

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Phys.org • October 11, 2026

Researchers at Harvard University and other institutions have introduced the concept of "quantum birthmarks," which are statistical traces of a system’s initial state and early evolution that persist even in chaotic environments. While classical systems typically forget their starting conditions over time due to ergodicity, isolated quantum systems can retain this memory through coherence effects. Joonas Keski-Rahkonen, the senior author, explained that unlike classical chaos which resets a system to a blank state, quantum systems cannot fully hide their history. This phenomenon manifests as a lasting preference for revisiting specific paths, even when those paths appear random from a classical perspective.

The team developed a theoretical framework splitting this effect into two parts: a universal memory factor present in any evolving quantum state, and a revival factor linked to early-time recurrences known as quantum scars. They demonstrated mathematically that these traces limit a system’s ability to explore all possible configurations completely. Keski-Rahkonen described this as a "maximum exploration principle," noting that if a system has not fully explored its available phase space by a specific time, it will never do so. This contrasts sharply with classical ergodic systems, which can continue exploring new regions without such quantum limitations.

To test their theory, the researchers performed computer calculations on a particle confined within a stadium-shaped enclosure. The results showed that long-term probability patterns retained distinct traces of the particle’s starting state and motion, with quantum scars strengthening the birthmark effect. This study establishes a generic constraint on quantum ergodicity, suggesting that the assumption underlying thermodynamics may need rethinking regarding how quantum systems thermalize. The framework aims to unify various known types of quantum scarring under a single phenomenon applicable to any generic nonstationary quantum state associated with a classical trajectory.

Source: Phys.org • October 11, 2026

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