Quantum Chaos, Unthermalizable States And Really Tiny Balloons

When a hypothetical, quantum-scale balloon is popped in a vacuum, do the particles inside spread out as predicted by classical mechanics or do something else, since matter at the infinitesimally small quantum scale is both a wave and a particle, and its location cannot be fixed precisely because measurement alters the system? The question is deceptively complex, since quantum particles do not look or act like air molecules in a real balloon. Theoretical physicists at the University of Southern California have an answer Heisenberg would be proud of. Quantum-scale chaos exists … sort of.

When a hypothetical, quantum-scale balloon is popped in a vacuum, do the particles inside spread out as predicted by classical mechanics or do something else, since matter at the infinitesimally small quantum scale is both a wave and a particle, and its location cannot be fixed precisely because measurement alters the system?

The question is deceptively complex, since quantum particles do not look or act like air molecules in a real balloon. Theoretical physicists at the University of Southern California have an answer Heisenberg would be proud of.

Quantum-scale chaos exists … sort of.

Writing in Nature, senior author Maxim Olshanii reported that when an observer attempts to measure the energies of particles coming out of a quantum balloon, the interference caused by the attempt throws the system into a final, “relaxed” state analogous to the chaotic scattering of air molecules.

The result is the same for any starting arrangement of particles, Olshanii added, since the act of measuring wipes out the differences between varying initial states.

“It’s enough to know the properties of a single stationary state of definite energy of the system to predict the properties of the thermal equilibrium (the end state),” Olshanii said.

The measurement – which must involve interaction between observer and observed, such as light traveling between the two – disrupts the “coherent” state of the system, Olshanii said.

In mathematical terms, the resulting interference reveals the final state, which had been hidden in the equations describing the initial state of the system.

“The thermal equilibrium is already encoded in an initial state,” Olshanii said. “You can see some signatures for the future equilibrium. They were already there but more masked by quantum coherences.”

The finding holds implications for the emerging fields of quantum computing and quantum information theory, said Paolo Zanardi, an associate professor of physics studying quantum information at USC. In Zanardi’s world, researchers want to prevent coherent systems from falling into the chaos of thermal equilibrium.

“Finding such ‘unthermalizable’ states of matter and manipulating them is exactly one of those things that quantum information/computation folks like me would love to do,” Zanardi wrote. “Such states would be immune from ‘decoherence’ (loss of quantum coherence induced by the coupling with environment) that’s still the most serious, both conceptually and practically, obstacle between us and viable quantum information processing.”

Zanardi and a collaborator introduced the notion of “decoherence-free” quantum states in 1997. Researchers such as Zanardi and Daniel Lidar, associate professor of chemistry, among others, have helped make USC a major center for the study of quantum computing.

Olshanii and his co-authors, postdoctoral researchers Marcos Rigol and Vanja Dunjko, developed their theory of quantum thermal equilibrium at USC and completed their work at the University of Massachusetts Boston.

Their research was funded by the National Science Foundation and the Office of Naval Resarch.

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