A hybrid trapped-ion system reproduced the Aharonov–Bohm effect with a changing, entangled gauge field, offering a new way to study interactions that challenge classical computers.
A particle can respond to a magnetic field it never crosses. In a new quantum simulation, researchers at the University of Oxford reproduced this counterintuitive effect using a hybrid system built from trapped ions—and made the magnetic flux part of the system’s own quantum dynamics.
The experiment demonstrates a route to studying fundamental interactions that can become difficult to calculate on conventional computers. It does not amount to a large-scale or fault-tolerant quantum computer. Rather, it shows how a carefully constructed quantum system can imitate a specific physical process and let researchers observe its behavior.
The effect, named for physicists Yakir Aharonov and David Bohm, was predicted in 1959 and later confirmed in experiments with real electrons. In everyday classical physics, a charged particle’s motion is shaped by electric and magnetic fields where it travels. Quantum mechanics permits a subtler influence: a particle that travels around a region containing magnetic flux can acquire a measurable phase, even without passing through the magnetic field itself.
Oxford’s team recreated the principle in a lattice gauge theory, a framework used to describe interactions between matter and fields in areas including particle physics. In the team’s model, matter occupies points on a grid and gauge fields connect those points. For its elementary loop, two vibrational modes represented matter at two locations, while two qubits represented the fields linking them.
The qubits were encoded in the internal states of trapped ions; the ions’ vibrations served as quantum oscillators. The researchers combined digital and analogue techniques to prepare the state, evolve the system while maintaining gauge-invariant dynamics, and measure the outcome.
The central result was not simply a simulated magnetic field imposed from outside. The team encoded flux in an entangled state of the qubits, making the gauge field itself dynamic. As Oxford researcher Sebastian Saner described it, matter and the gauge field became part of the same quantum dynamics.
Researchers then followed a matter excitation as it could tunnel along two routes around the loop. Without flux, tunnelling proceeded. With the encoded flux, the two routes interfered destructively: their contributions canceled, suppressing tunnelling and leaving the excitation in its starting state. That halt supplied the signature of the Aharonov–Bohm effect in this simulated, dynamical setting.
The distinction matters. A fixed background flux would have required an interaction the hardware could not provide. Encoding the flux in the qubits began as a practical workaround, but gave the researchers a way to explore the coupled behavior of matter and gauge fields rather than treating one as an unchanging backdrop.
The work, published in Nature Physics, sits within a broader effort to use quantum devices as simulators of quantum theories. As the systems described by lattice gauge theories grow, their possible behaviors become harder to reproduce through classical calculation. A quantum simulator does not solve every such problem automatically; it must be built and controlled for the physics under study. This experiment shows one way to do that on a small scale.
A separate study published alongside the Oxford result, led by Norbert Linke’s group at the University of Maryland, used a hybrid quantum system to simulate the Yukawa potential, an interaction relevant to nuclear and particle physics. The groups developed their approaches independently and coordinated their submissions, according to the research account.
The Oxford paper presents its architecture as a possible route toward scalable quantum simulations of lattice gauge theories in higher dimensions. That is a research direction, not a capability demonstrated in this experiment. The next challenge will be extending the simulated systems while preserving the delicate quantum behavior that makes them useful—and testing whether the approach can illuminate more complex interactions that remain out of reach for classical methods.

