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Bulletin of the American Physical Society

A quantum gas microscope for highly dipolar atoms

Susannah M. Dickerson, Anne Hébert, Aaron Krahn, Gregory Phelps, Markus Greiner

Published Jun 7, 2017• 0 citations
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Quantum gas microscopy is an exciting platform for the study ofin situatom-atom interactions.Erbium, a dipolar atom, presents an opportunity to extend previous quantum gas microscopy ex-periments to more complex systems influenced by long-range, anisotropic interactions. In this the-sis, I present progress towards a quantum gas microscope of erbium atoms, including details on thedesign of a novel accordion lattice system. This system will allow us to dynamically tune the spac-ing of both the vertical and horizontal optical lattices confining the atoms. In addition, I present onthe sub-second generation of erbium Bose-Einstein condensates, made possible by implementing atwo-stage magneto-optical trap and a crossed optical dipole trap with a tunable geometry.

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Quantum gas microscopes are versatile and powerful tools for fundamental science as well as promising candidates for enticing applications such as in quantum simulation or quantum computation. Here we present a quantum gas microscopy setup for experiments with highly magnetic atoms of the lanthanoid elements erbium and dysprosium. Our setup features a non-magnetic, non-conducting, large-working-distance, high-numerical-aperture, in-vacuum microscope objective, mounted inside a glue-free quartz glass cell. The quartz glass cell is enclosed by a compact multi-shell ferromagnetic shield that passively suppresses external magnetic field noise by a factor of more than a thousand. Our setup will enable direct manipulation and probing of the rich quantum many-body physics of dipolar atoms in optical lattices, and bears the potential to put exciting theory proposals - including exotic magnetic phases and quantum phase transitions - to an experimental test.

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Erbium quantum gas microscope

Aaron Krahn

Quantum gas microscopy of dipolar atoms is a promising opportunity to expand upon previous quantum simulations of neutral atoms in optical lattices. Erbium atoms interact via the long-range magnetic dipole-dipole interaction, which leads to a variety of new many-body effects and strongly correlated phases that are currently unexplored in microscopes with only short-range interactions. In this thesis I will detail progress toward the construction of an erbium quantum gas microscope as well as the techniques we implemented to produce a Bose-Einstein condensate of $8\times10^4$ atoms in under a second. These include the installation of a dual-stage magneto-optical trap, a stroboscopic optical dipole trap, as well as a tunable crossed optical dipole trap that allows for efficient evaporation of both bosonic and fermionic isotopes. I will also discuss the frequency stabilization systems we have implemented to produce laser linewidths of less than $1$ kHz for near-resonant laser cooling on narrow transitions and a custom, high NA reflective objective to be used as part of a high resolution imaging system. Finally, I will discuss the noise properties of charge-coupled devices and the photon counting techniques that are needed for having high fidelities while using fast imaging schemes.

•Jan 20, 2021•1 citation
Quantum gas microscopy is an exciting platform for the study ofin situatom-atom interactions.Erbium, a dipolar atom, presents an opportunity to extend previous quantum gas microscopy ex-periments to more complex systems influenced by long-range, anisotropic interactions. In this the-sis, I present progress towards a quantum gas microscope of erbium atoms, including details on thedesign of a novel accordion lattice system. This system will allow us to dynamically tune the spac-ing of both the vertical and horizontal optical lattices confining the atoms. In addition, I present onthe sub-second generation of erbium Bose-Einstein condensates, made possible by implementing atwo-stage magneto-optical trap and a crossed optical dipole trap with a tunable geometry.
Quantum gas microscopes are versatile and powerful tools for fundamental science as well as promising candidates for enticing applications such as in quantum simulation or quantum computation. Here we present a quantum gas microscopy setup for experiments with highly magnetic atoms of the lanthanoid elements erbium and dysprosium. Our setup features a non-magnetic, non-conducting, large-working-distance, high-numerical-aperture, in-vacuum microscope objective, mounted inside a glue-free quartz glass cell. The quartz glass cell is enclosed by a compact multi-shell ferromagnetic shield that passively suppresses external magnetic field noise by a factor of more than a thousand. Our setup will enable direct manipulation and probing of the rich quantum many-body physics of dipolar atoms in optical lattices, and bears the potential to put exciting theory proposals - including exotic magnetic phases and quantum phase transitions - to an experimental test.
Quantum gas microscopy of dipolar atoms is a promising opportunity to expand upon previous quantum simulations of neutral atoms in optical lattices. Erbium atoms interact via the long-range magnetic dipole-dipole interaction, which leads to a variety of new many-body effects and strongly correlated phases that are currently unexplored in microscopes with only short-range interactions. In this thesis I will detail progress toward the construction of an erbium quantum gas microscope as well as the techniques we implemented to produce a Bose-Einstein condensate of 8×1048\times10^48×104 atoms in under a second. These include the installation of a dual-stage magneto-optical trap, a stroboscopic optical dipole trap, as well as a tunable crossed optical dipole trap that allows for efficient evaporation of both bosonic and fermionic isotopes. I will also discuss the frequency stabilization systems we have implemented to produce laser linewidths of less than 111 kHz for near-resonant laser cooling on narrow transitions and a custom, high NA reflective objective to be used as part of a high resolution imaging system. Finally, I will discuss the noise properties of charge-coupled devices and the photon counting techniques that are needed for having high fidelities while using fast imaging schemes.