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Microwave Dressed Potentials: a coherence control method for an atomic Sagnac Interferometer

Morrison, Rhys Jordan

Published Dec 12, 2025• 0 citations
OpenAlex

Abstract

The process of atomic interferometry relies heavily on the underlying atomic manipulation methods that have been developed over the past few decades. The ability to manipulate the internal state dynamics of atoms, and precisely control their time-space co-ordinates both lend themselves to the improvement of the sensitivities of these devices, allowing for more precise measurements, and more in-depth exploration of the physical world. In this thesis the design of a state-dependent fully trapped interferometric transport is presented, wherein atoms are fully magnetically trapped for the entire duration of an interferometric sequence. Through use of Radio-Frequency dressed potentials, we are able to create a trapping system that is both robust, and able to create state-dependent trap that can be dynamically moved to create the mechanical basis for an interferometer. We also investigate the coherence time of a superposition of hyperfine states loaded into the interferometer, necessary for a Ramsey-Borde sequence, and find it is significantly lower than what would be required to perform interferometry. We then present how this lack in coherence time is due to a mismatch in trapping potentials that arises due to a slight discrepancy between gyromagnetic ratios in the two superpositional states. This mismatch broadens the transition linewidth, leading to a reduction in superposition coherence time. Finally, we lay out the theoretical groundwork, and experimental progress, in realising Microwave-Dressed potentials, which utilise the AC-Stark shift to adiabatically shift the trapping potentials of the atoms, reducing the mismatch and thus increasing the coherence time of the superposition.

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The process of atomic interferometry relies heavily on the underlying atomic manipulation methods that have been developed over the past few decades. The ability to manipulate the internal state dynamics of atoms, and precisely control their time-space co-ordinates both lend themselves to the improvement of the sensitivities of these devices, allowing for more precise measurements, and more in-depth exploration of the physical world. In this thesis the design of a state-dependent fully trapped interferometric transport is presented, wherein atoms are fully magnetically trapped for the entire duration of an interferometric sequence. Through use of Radio-Frequency dressed potentials, we are able to create a trapping system that is both robust, and able to create state-dependent trap that can be dynamically moved to create the mechanical basis for an interferometer. We also investigate the coherence time of a superposition of hyperfine states loaded into the interferometer, necessary for a Ramsey-Borde sequence, and find it is significantly lower than what would be required to perform interferometry. We then present how this lack in coherence time is due to a mismatch in trapping potentials that arises due to a slight discrepancy between gyromagnetic ratios in the two superpositional states. This mismatch broadens the transition linewidth, leading to a reduction in superposition coherence time. Finally, we lay out the theoretical groundwork, and experimental progress, in realising Microwave-Dressed potentials, which utilise the AC-Stark shift to adiabatically shift the trapping potentials of the atoms, reducing the mismatch and thus increasing the coherence time of the superposition.
The manipulation of ultracold atoms in radio-frequency (RF)-dressed potentials offers unique advantages over static magnetic traps, such as the ability to create more complex potential landscapes, better control of atomic states, and increased robustness to environmental noise. Among the accessible geometries, ring traps are particularly promising for atomic Sagnac interferometers, which can be used to measure rotational motion with high sensitivity. Here, the authors demonstrate the state-dependent transport of atoms in an RF-dressed ring trap on an atom chip. By exploiting the polarization-dependent coupling of RF fields to different atomic hyperfine states, the authors achieve controlled transport of atoms in opposite directions. This approach targets the development of compact, high-precision devices for applications in inertial navigation and rotation sensing.
This thesis describes the experimental realisation of state-dependent traps employing RF-dressed adiabatic potentials. Rb-87 atoms have been successfully confined to chip-based atom traps that can independently address atomic ground states defined by the total angular momentum, F. The ring-shaped trap can be used as a Sagnac interferometer to measure rotation with respect to the inertial frame of reference. The results of spatially dependent radio frequency field polarisation control in this trap resulted in counterpropagating motion of the atoms in the F = 1 and F = 2 states.
This thesis presents the experimental scheme for a guided cold atom Sagnac interferometer. Although atom interferometers have become an established method for precision measurements, a feasible clock-scheme based on fully guided atoms has yet to be realised. Radio frequency potentials, generated by a chip, provide a means to create a compact, fully controllable guided atom interferometer. The experimental infrastructure for a rubidium cold atom system is built and characterised. A chip-based atomic clock scheme is presented, utilising state-dependent guiding around a ring shaped trap. The chip design to form the trap and operate the interferometer is presented, and a vacuum compatible PCB has been designed and commercially manufactured to provide atomic transport and compression towards an atom chip. This project is part of the larger MatterWave project. In collaboration with Birmingham and Crete, the Matterwave project aims to develop ultra-sensitive matter-wave interferometry for compact devices.
Sagnac interferometers with massive particles promise unique advantages in achieving high-precision measurements of rotation rates over their optical counterparts. Recent proposals and experiments are exploring nonballistic Sagnac interferometers where trapped atoms are transported along a closed path. This is achieved by using superpositions of internal quantum states and their control with state-dependent potentials. We address emergent questions regarding the dynamical behavior of Bose-Einstein condensates in such an interferometer and its impact on rotation sensitivity. We investigate complex dependencies on atomic interactions as well as trap geometries, rotation rates, and speed of operation. We find that temporal transport profiles obtained from a simple optimization strategy for noninteracting particles remain surprisingly robust also in the presence of interactions over a large range of realistic parameters. High sensitivities can be achieved for short interrogation times far from the adiabatic regime. This highlights a route to building fast and robust guided-ring Sagnac interferometers with fully trapped atoms.
Adiabatic dressed state potentials are created when magnetic substates of trapped atoms are coupled by a radio-frequency field. We discuss their theoretical foundations and point out fundamental advantages over potentials purely based on static fields. The enhanced flexibility enables one to implement numerous configurations, including double wells, Mach-Zehnder, and Sagnac interferometers which even allows for internal state-dependent atom manipulation. These can be realized using simple and highly integrated wire geometries on atom chips.
The spectacular progress in the field of ultracold quantum gases is intimately connected with the availability of sophisticated techniques for quantum-level control of internal states, motional states, and collisional interactions. Atom chips provide such control in compact, robust, and scalable setups, which makes them attractive for both applications and fundamental studies. In this thesis I report on experiments that use a new method for coherent manipulation of ultracold atoms. The method is based on microwave near-fields, provided by a waveguide structure that is fully integrated on an atom chip. We generate microwave near-field potentials that combine the versatility of optical traps with the robustness and tailorability of static magnetic microtraps. These potentials depend on the internal atomic state, and we use them for state-selective splitting of Rb Bose-Einstein condensates. We show for the first time combined coherent manipulation of internal and motional states on an atom chip, realizing a trapped-atom interferometer with internal state labeling of the interferometer paths. Moreover, we use microwave near-field potentials for the preparation of spin-squeezed states for quantum-enhanced metrology through controlling state-dependent collisional interactions. In addition, very promising proposals exist for the implementation of a quantum phase gate using these potentials. Measuring microwave fields is important for engineering of microwave devices as well as in science, e.g. to characterize the field homogeneity in the interaction regions of an atomic clock. We develop a novel technique that uses clouds of uncondensed ultracold atoms as sensitive, tunable and non-invasive probes for microwave field imaging with micrometer spatial resolution. The microwave magnetic field components drive Rabi oscillations on atomic hyperfine transitions whose frequency can be tuned with a static magnetic field. Readout is accomplished using state-selective absorption imaging. Quantitative data extraction is simple and it is possible to reconstruct the amplitudes and phases of the different microwave magnetic field components. While we demonstrate 2D imaging, an extension to 3D imaging is straightforward. We use the method to determine the microwave near-field distribution around the on-chip waveguide and reconstruct the corresponding current distribution. For our experimental parameters, the method provides a microwave magnetic field sensitivity of 0.2 mG, which can even be improved further with variants discussed. The experiments presented in this thesis open the path for the realization of portable quantum-enhanced interferometer devices, the implementation of a quantum phase gate as well as for a new generation of microwave field sensors.