Bulletin of the American Physical Society
56th Annual Meeting of the APS Division of Atomic, Molecular and Optical Physics
Monday–Friday, June 16–20, 2025; Portland, Oregon
Session B08: Quantum Simulation I
10:45 AM–12:21 PM,
Tuesday, June 17, 2025
Oregon Convention Center
Room: E145-146
Chair: Michael Peper, Princeton University
Abstract: B08.00004 : Quantum simulation with circular Rydberg atoms of Strontium
11:21 AM–11:33 AM
Presenter:
Baptiste Muraz
(Collège de France)
Authors:
Baptiste Muraz
(Collège de France)
Mathis Pépin
(Collège de France)
Clara Weser
(Collège de France)
Brice Bakkali-Hassani
(Collège de France)
Jean-Michel Raimond
(Laboratoire Kastler-Brossel)
Michel Brune
(Collège de France)
Sebastien Gleyzes
(Collège de France)
In our group, we are working with circular Rydberg states, characterized by maximum angular momentum (l = m = n-1). Unlike low-l Rydberg states, which have lifetimes of about 100 µs, circular states can survive for several milliseconds when placed in a cryogenic environment where blackbody radiation is suppressed. This extended lifetime could allow us to explore dynamics that are inaccessible with conventional Rydberg states.
To study these long-time dynamics, circular atoms must be trapped during the simulation. The nearly free electron in the Rydberg state is affected by the ponderomotive potential of the trapping light, which is repulsive. While blue-detuned traps with specialized geometries can trap these states, they require significant laser power, which is not ideal for scaling purposes. An alternative approach is to use alkaline-earth like species and take advantage of the polarizability of the ionic core to trap the Rydberg atom.
This is why we have built a cryogenic (4K) experimental setup to trap strontium atoms in an optical tweezer array and excite them to circular Rydberg states where they will be trapped for millisecond. Once the atoms are trapped, we will demonstrate that the fast transition of the Sr+ ionic core make it possible to image the Rydberg states directly whithout having to transfer them back to the ground state.
Furthermore, the electric quadrupole interaction between the Rydberg electron and the ionic core induces an energy shift in the bare ion's energy levels, which depends on the Rydberg state. By resolving this shift, it is then possible to implement shelving technique or apply phase shifts to specific Rydberg states using lasers.
This opens the way to perform non-destructive measurements or gate operations.
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