ഹൈബ്രിഡ് ക്വാണ്ടം കമ്പ്യൂട്ടർ ഉപയോഗിച്ച് അഹരോനോവ്-ബോം പ്രഭാവം പുതിയ രീതിയിൽ നിരീക്ഷിച്ചു

Physicists in the Department of Physics at the University of Oxford have used a hybrid quantum computer, made up of qubits and quantum oscillators, to observe the Aharonov–Bohm effect in a quantum simulation. The effect is a quantum phenomenon in which a particle can acquire a measurable phase by traveling around a magnetic flux, even though it never passes through a region where a magnetic field is present.

The result demonstrates how hybrid quantum systems can be used to simulate interactions between matter and gauge fields that become increasingly difficult to model on classical computers. The paper has been published in Nature Physics.

A phase without crossing the field

In classical, everyday physics, the motion of a charged particle is determined locally by the electric and magnetic fields it encounters. Quantum mechanics allows a more subtle effect. In 1959, physicists Yakir Aharonov and David Bohm predicted that a charged particle traveling around, rather than through, a region containing a magnetic field would still pick up a measurable trace of that field's presence. This became known as the Aharonov–Bohm effect, and it was later confirmed in experiments with real electrons.

Physicists are now interested in seeing the effect emerge in a different setting: lattice gauge theories. These are mathematical frameworks used to describe interactions between matter and gauge fields, including important models in particle and high-energy physics. In a lattice gauge theory, matter sits at the points of a grid, and the fields live on the links connecting those points.

The difficulty is that as these systems grow, their behavior becomes increasingly difficult to calculate on a classical computer. Quantum computers, which operate according to the same quantum rules the theories describe, offer another approach: Rather than solving the full dynamics on a classical computer, researchers build a physical system that behaves in the same way and observe what it does. This is known as quantum simulation.

Matter and fields share trapped ions

Beginning in 2022, lead author Dr. Sebastian Saner, Dr. Oana Bazavan and colleagues in Oxford, working with Dr. Alejandro Bermudez from the Instituto de Física Teórica in Madrid, developed an experiment to simulate lattice gauge theories using a hybrid quantum system. Their experiment used two kinds of components, each playing a different physical role.

Qubits—quantum bits, encoded in the internal states of trapped ions—represented the gauge fields, while quantum oscillators—the vibrations of those same ions—represented the matter. Using this encoding, the team built a loop, the elementary building block of the theory, from two oscillators representing matter at two points, connected by two qubits representing the fields between them.

The team then prepared the two qubits in an entangled quantum state, in which their properties are linked in a way that has no classical equivalent. In the language of the lattice gauge theory, this corresponds to a magnetic flux piercing the loop. Producing such a flux in the conventional way, as a fixed background, would have required an interaction the hardware could not provide, so encoding it in the qubits began as a practical workaround.

"For us, the exciting step was to encode the magnetic flux in a gauge field that was itself dynamical," says Saner. "Rather than having matter evolve in a fixed background, the matter and gauge field become part of the same quantum dynamics." What began as a workaround turned out to be the more interesting route.

Magnetic flux brings tunneling to a halt

The researchers then watched a matter particle tunnel around the loop. With no flux present, it tunneled freely. With the flux present, the two paths around the loop interfered destructively, suppressing the tunneling completely and leaving the system frozen in its starting state. The result was an experimental demonstration of the Aharonov–Bohm effect in a dynamical setting within a lattice gauge theory.