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Heavy-quark spin precession as a magnetic field chronometer

This paper proposes that the Larmor spin precession of polarized heavy quarks (charm and bottom) in the strong magnetic fields of relativistic heavy-ion collisions generates measurable charge-dependent polarization splittings in their hadronic decay products, offering a novel quantitative probe to determine the lifetime and profile of these magnetic fields.

Original authors: Dushmanta Sahu, Captain R. Singh

Published 2026-09-22
📖 4 min read🧠 Deep dive

Original authors: Dushmanta Sahu, Captain R. Singh

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 most violent collisions ever created by human hands, where atomic nuclei smash together at nearly the speed of light, nature briefly recreates conditions that existed just moments after the Big Bang. These collisions generate a state of matter called the quark-gluon plasma, a super-hot soup where the building blocks of protons and neutrons roam freely. But these collisions also produce something even more extreme: the strongest magnetic fields in the known universe. For decades, physicists have known these fields exist, but a stubborn mystery has remained: how long do they last? Do they vanish in a flash as the colliding particles fly apart, or does the hot, electrically conducting plasma keep them alive for a significant time? Solving this puzzle is crucial because the duration of this magnetic field influences how the plasma behaves, how particles move, and how the fundamental forces of nature operate in these extreme environments.

A new study proposes a clever way to time this fleeting magnetic field by watching how heavy particles spin. The researchers focused on two types of heavy quarks, known as charm and bottom, which are produced in the very first split-second of a collision. Unlike lighter particles that are constantly bumped and scrambled by the hot plasma, these heavy quarks are massive and stable enough to preserve their initial spin orientation as they travel through the medium. The team suggested that if a magnetic field persists, it acts like a cosmic compass, causing the spin of these charged particles to slowly rotate, or precess, as they move. Because charm quarks and bottom quarks carry opposite electric charges, they would rotate in opposite directions if a magnetic field were present. By measuring the difference in the final spin direction of particles made from these quarks, scientists could effectively read the history of the magnetic field's strength and duration.

To test this idea, the researchers built a detailed simulation of a heavy-ion collision, modeling the expansion of the quark-gluon plasma and the evolution of the magnetic field over time. They explored three different scenarios for how the field might behave: one where it dies away almost instantly in a vacuum, another where it fades exponentially, and a third where the plasma's electrical conductivity helps sustain the field for a longer period. They tracked the journey of polarized charm and bottom quarks through these environments, calculating exactly how much their spins would rotate before the plasma cooled down enough for them to form new particles. The results showed that for realistic magnetic field strengths, the accumulated rotation is large enough to be measured. Specifically, the charm quarks, being lighter than bottom quarks, develop a much larger rotation angle, making them particularly sensitive to the field's presence.

The study found that if the magnetic field lasts for several units of time known as femtoseconds, the difference in spin between the matter particles and their antimatter counterparts becomes distinct and measurable. This difference, known as a charge-dependent polarization splitting, serves as a unique signature. Because the rotation depends directly on the total time the field exists, observing this splitting would provide direct evidence that the magnetic field survived long enough to influence the heavy quarks. Conversely, if no such difference is found, it would suggest the field vanished almost immediately. The researchers noted that this method offers a cleaner way to study the field than looking at lighter particles, which are easily confused by other effects like the swirling motion of the plasma itself.

The findings suggest that heavy-flavor polarization, especially in the charm sector, acts as a reliable clock for the magnetic field's life. The simulations indicate that the effect is strong enough to be detected in current experiments at the Large Hadron Collider. By comparing the spin directions of particles like the Lambda-c and its antimatter partner, physicists could finally pin down how long these extreme magnetic fields endure. This approach transforms the heavy quark from a passive passenger into an active recorder of the collision's electromagnetic history, offering a new and precise tool to understand the dynamics of the quark-gluon plasma. The authors conclude that future measurements of these heavy particles will provide a direct window into the space-time evolution of the strongest magnetic fields in nature.

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