Optical magnetism and wavefront control by arrays of strontium atoms
By analyzing the parameters of electronic transitions, we show how bosonic Sr atoms in planar optical lattices can be engineered to exhibit optical magnetism and other higher-order electromagnetic multipoles that can be harnessed for wavefront control of incident light. Resonant λ≃2.6μm light for th...
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sg-ntu-dr.10356-1646082023-02-28T20:11:32Z Optical magnetism and wavefront control by arrays of strontium atoms Ballantine, K. E. Wilkowski, David Ruostekoski, J. School of Physical and Mathematical Sciences Nanyang Quantum Hub MajuLab, International Joint Research Unit IRL 3654, CNRS Science::Physics Electromagnetics Optical Magnetisms By analyzing the parameters of electronic transitions, we show how bosonic Sr atoms in planar optical lattices can be engineered to exhibit optical magnetism and other higher-order electromagnetic multipoles that can be harnessed for wavefront control of incident light. Resonant λ≃2.6μm light for the ³D₁ →³P₀ transition mediates cooperative interactions between the atoms while the atoms are trapped in a deeply subwavelength optical lattice. The atoms then exhibit collective excitation eigenmodes, e.g., with a strong cooperative magnetic response at optical frequencies, despite individual atoms having negligible coupling to the magnetic component of light. We provide a detailed scheme to utilize excitations of such cooperative modes consisting of arrays of electromagnetic multipoles to form an atomic Huygens' surface, with complete 2π phase control of transmitted light and almost no reflection, allowing nearly arbitrary wavefront shaping. In the numerical examples, this is achieved by controlling the atomic level shifts of Sr with off-resonant ³PJ→³D₁ transitions, which results in a simultaneous excitation of arrays of electric dipoles and electric quadrupoles or magnetic dipoles. We demonstrate the wavefront engineering for a Sr array by realizing the steering of an incident beam and generation of a baby-Skyrmion texture in the transmitted light via a topologically nontrivial transition of a Gaussian beam to a Poincaré beam, which contains all possible polarizations in a single cross-section. Ministry of Education (MOE) Published version K.E.B. and J.R. acknowledge financial support from the United Kingdom Engineering and Physical Sciences Research Council (EPSRC) (Grants No. EP/S002952/1, No. EP/P026133/1, and No. EP/W005638/1). D.W. acknowledges the Singapore Ministry of Education and the Centre for Quantum Technologies (CQT/MoE Grant No. R-710-002- 016-271). 2023-02-06T06:52:56Z 2023-02-06T06:52:56Z 2022 Journal Article Ballantine, K. E., Wilkowski, D. & Ruostekoski, J. (2022). Optical magnetism and wavefront control by arrays of strontium atoms. Physical Review Research, 4(3). https://dx.doi.org/10.1103/PhysRevResearch.4.033242 2643-1564 https://hdl.handle.net/10356/164608 10.1103/PhysRevResearch.4.033242 2-s2.0-85139235276 3 4 en R-710-002-016-271 Physical Review Research © The Authors. Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article’s title, journal citation, and DOI. application/pdf |
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Science::Physics Electromagnetics Optical Magnetisms Ballantine, K. E. Wilkowski, David Ruostekoski, J. Optical magnetism and wavefront control by arrays of strontium atoms |
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By analyzing the parameters of electronic transitions, we show how bosonic Sr atoms in planar optical lattices can be engineered to exhibit optical magnetism and other higher-order electromagnetic multipoles that can be harnessed for wavefront control of incident light. Resonant λ≃2.6μm light for the ³D₁ →³P₀ transition mediates cooperative interactions between the atoms while the atoms are trapped in a deeply subwavelength optical lattice. The atoms then exhibit collective excitation eigenmodes, e.g., with a strong cooperative magnetic response at optical frequencies, despite individual atoms having negligible coupling to the magnetic component of light. We provide a detailed scheme to utilize excitations of such cooperative modes consisting of arrays of electromagnetic multipoles to form an atomic Huygens' surface, with complete 2π phase control of transmitted light and almost no reflection, allowing nearly arbitrary wavefront shaping. In the numerical examples, this is achieved by controlling the atomic level shifts of Sr with off-resonant ³PJ→³D₁ transitions, which results in a simultaneous excitation of arrays of electric dipoles and electric quadrupoles or magnetic dipoles. We demonstrate the wavefront engineering for a Sr array by realizing the steering of an incident beam and generation of a baby-Skyrmion texture in the transmitted light via a topologically nontrivial transition of a Gaussian beam to a Poincaré beam, which contains all possible polarizations in a single cross-section. |
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School of Physical and Mathematical Sciences |
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School of Physical and Mathematical Sciences Ballantine, K. E. Wilkowski, David Ruostekoski, J. |
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Article |
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Ballantine, K. E. Wilkowski, David Ruostekoski, J. |
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Ballantine, K. E. |
title |
Optical magnetism and wavefront control by arrays of strontium atoms |
title_short |
Optical magnetism and wavefront control by arrays of strontium atoms |
title_full |
Optical magnetism and wavefront control by arrays of strontium atoms |
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Optical magnetism and wavefront control by arrays of strontium atoms |
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Optical magnetism and wavefront control by arrays of strontium atoms |
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optical magnetism and wavefront control by arrays of strontium atoms |
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2023 |
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https://hdl.handle.net/10356/164608 |
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