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Increasing the scalability of atom arrays with magic wavelength tweezers

Mohammad Mujahid Aliyu, Luheng Zhao, Xiu Quan Quek, Krishna Chaitanya Yellapragada, Huanqian Loh

Published May 31, 2021• 1 citation
OpenAlex

Abstract

We report the use of magic wavelength tweezers to trap and image single atoms on the D1 transition with 80.0(6)% efficiency. Such magic wavelengths for the D1 transition have been predicted for the alkali atoms but are not yet demonstrated to date. Here, we confirm a D1 magic wavelength that is predicted to lie at 615.87 nm for $^{23}$Na, which we then use to trap and image individual atoms without having to modulate the trapping and imaging light intensities. We further demonstrate that the mean loading efficiency remains as high as 74.2(7)% for a 1D array of eight atoms. Leveraging on our high loading probabilities and the absence of trap intensity modulation, we achieve an order-of-magnitude reduction on the tweezer laser power requirements and a corresponding increase in the scalability of atom arrays. The methods reported here are applicable to a wide variety of atoms, including those that can be manipulated with different Feshbach resonances or assembled into dipolar molecules.

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D1 magic wavelength tweezers for scaling atom arrays

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Efficient trapping and detection of single atoms in optical tweezers are important for realizing atom arrays, a promising platform for quantum simulation and quantum information processing. However, the scaling up of atom arrays can be impeded by detrimental light shifts induced by the tweezer trap, making it challenging to cool and image single atoms. Here, we report an order-of-magnitude increase in the scalability of $^{23}\mathrm{Na}$ atom arrays by using ${D}_{1}$ magic wavelength tweezers to reduce the required tweezer power per trap. ${D}_{1}$ magic wavelengths have been previously predicted to exist for all the alkali atoms but are not yet observed to date. We first experimentally confirm a ${D}_{1}$ magic wavelength that is predicted to lie at 615.87 nm, which we then use to trap and image single atoms without having to modulate the trapping and imaging light intensities. We further demonstrate that the mean loading efficiency remains as high as 80.0(6)% for a single trap and 74.2(7)% for a one-dimensional array of eight atoms. The methods reported here are applicable to all the alkalis, including those that are attractive candidates for dipolar molecule assembly, Rydberg dressing, or are fermionic in nature.

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Neutral-atom arrays offer a promising path for quantum simulation, yet the potential of fermionic $^{40}$K remains largely constrained by state-dependent light shifts that degrade cooling and detection fidelities. This problem can be resolved by working at a magic wavelength, where the differential light shift vanishes. We report the first experimental determination of the magic wavelength for the D1 transition in fermionic $^{40}$K at 1227.54(4) nm. Using in-trap loss spectroscopy in a wavelength-tunable optical tweezer, we map the differential AC Stark shift across a range of trapping powers and wavelengths. By converting these shifts to differential scalar polarizabilities, we find excellent agreement with relativistic all-order calculations. Benchmark measurements at 1064.49 nm further quantify the intensity-sampling systematics inherent to standard trapping wavelengths, contrasting with the ``mechanically clean'' environment provided by the magic condition. Our results provide an important step toward high-fidelity in-trap D1 cooling, fluorescence imaging, and light-assisted loading, establishing a robust path toward scaling fermionic neutral-atom arrays for quantum information science.

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Direct Generation of an Array with 78400 Optical Tweezers Using a Single Metasurface

Yuqing Wang, Yuxuan Liao, Tao Zhang +9 more

Scalability remains a major challenge in building practical fault-tolerant quantum computers. Currently, the largest number of qubits achieved across leading quantum platforms ranges from hundreds to thousands. In atom arrays, scalability is primarily constrained by the capacity to generate large numbers of optical tweezers, and conventional techniques using acousto-optic deflectors or spatial light modulators struggle to produce arrays much beyond $\sim 10,000$ tweezers. Moreover, these methods require additional microscope objectives to focus the light into micrometer-sized spots, which further complicates system integration and scalability. Here, we demonstrate the experimental generation of an optical tweezer array containing $280\times 280$ spots using a metasurface, nearly an order of magnitude more than most existing systems. The metasurface leverages a large number of subwavelength phase-control pixels to engineer the wavefront of the incident light, enabling both large-scale tweezer generation and direct focusing into micron-scale spots without the need for a microscope. This result shifts the scalability bottleneck for atom arrays from the tweezer generation hardware to the available laser power. Furthermore, the array shows excellent intensity uniformity exceeding $90\%$, making it suitable for homogeneous single-atom loading and paving the way for trapping arrays of more than $10,000$ atoms in the near future.

cond-mat.quant-gasCross-listedarXiv:2512.08222•Chinese Physics Letters•Dec 10, 2025•3 citations
We report the use of magic wavelength tweezers to trap and image single atoms on the D1 transition with 80.0(6)% efficiency. Such magic wavelengths for the D1 transition have been predicted for the alkali atoms but are not yet demonstrated to date. Here, we confirm a D1 magic wavelength that is predicted to lie at 615.87 nm for 23^{23}23Na, which we then use to trap and image individual atoms without having to modulate the trapping and imaging light intensities. We further demonstrate that the mean loading efficiency remains as high as 74.2(7)% for a 1D array of eight atoms. Leveraging on our high loading probabilities and the absence of trap intensity modulation, we achieve an order-of-magnitude reduction on the tweezer laser power requirements and a corresponding increase in the scalability of atom arrays. The methods reported here are applicable to a wide variety of atoms, including those that can be manipulated with different Feshbach resonances or assembled into dipolar molecules.
Efficient trapping and detection of single atoms in optical tweezers are important for realizing atom arrays, a promising platform for quantum simulation and quantum information processing. However, the scaling up of atom arrays can be impeded by detrimental light shifts induced by the tweezer trap, making it challenging to cool and image single atoms. Here, we report an order-of-magnitude increase in the scalability of 23Na^{23}\mathrm{Na}23Na atom arrays by using D1{D}_{1}D1​ magic wavelength tweezers to reduce the required tweezer power per trap. D1{D}_{1}D1​ magic wavelengths have been previously predicted to exist for all the alkali atoms but are not yet observed to date. We first experimentally confirm a D1{D}_{1}D1​ magic wavelength that is predicted to lie at 615.87 nm, which we then use to trap and image single atoms without having to modulate the trapping and imaging light intensities. We further demonstrate that the mean loading efficiency remains as high as 80.0(6)% for a single trap and 74.2(7)% for a one-dimensional array of eight atoms. The methods reported here are applicable to all the alkalis, including those that are attractive candidates for dipolar molecule assembly, Rydberg dressing, or are fermionic in nature.
Experimental Determination of the D1D1D1 Magic Wavelength for 40^{40}40K
Neutral-atom arrays offer a promising path for quantum simulation, yet the potential of fermionic 40^{40}40K remains largely constrained by state-dependent light shifts that degrade cooling and detection fidelities. This problem can be resolved by working at a magic wavelength, where the differential light shift vanishes. We report the first experimental determination of the magic wavelength for the D1 transition in fermionic 40^{40}40K at 1227.54(4) nm. Using in-trap loss spectroscopy in a wavelength-tunable optical tweezer, we map the differential AC Stark shift across a range of trapping powers and wavelengths. By converting these shifts to differential scalar polarizabilities, we find excellent agreement with relativistic all-order calculations. Benchmark measurements at 1064.49 nm further quantify the intensity-sampling systematics inherent to standard trapping wavelengths, contrasting with the ``mechanically clean'' environment provided by the magic condition. Our results provide an important step toward high-fidelity in-trap D1 cooling, fluorescence imaging, and light-assisted loading, establishing a robust path toward scaling fermionic neutral-atom arrays for quantum information science.
We present the first successful trapping of single erbium atoms in an array of optical tweezers. Using a single narrow-line optical transition, we achieve deep cooling for direct tweezer loading, pairwise ejection, and continuous imaging without additional recoil suppression techniques. Our tweezer wavelength choice enables us to reach the magic trapping condition by tuning the ellipticity of the trapping light. Additionally, we implement an ultrafast high-fidelity fluorescence imaging scheme using a broad transition, allowing time-resolved study of the tweezer population dynamics from many to single atoms during light-assisted collisions. In particular, we extract a pair-ejection rate that qualitatively agrees with the semiclassical predictions by the Gallagher-Pritchard model. This Letter represents a promising starting point for the exploration of erbium as a powerful resource for quantum simulation in optical tweezers.
We report the preparation and observation of single atoms of dysprosium in arrays of optical tweezers with a wavelength of 532 nm, imaged on the intercombination line at 626 nm. We use the anisotropic light shift specific to lanthanides and in particular a large difference in tensor and vector polarizabilities between the ground and excited states to tune the differential light shift and produce tweezers in near-magic or magic polarization. This allows us to find a regime where single atoms can be trapped and imaged. Using the tweezer array toolbox to manipulate lanthanides will open new research directions for quantum physics studies by taking advantage of their rich spectrum, large spin, and magnetic dipole moment.
Subwavelength atomic tweezer arrays, in which atoms can be positioned at distances smaller than their emission wavelength, have been proposed as a versatile platform to study collective emission phenomena, such as superradiance and subradiance. Experimentally, the realization of such arrays has been a challenge as typical emission wavelengths in the visible or near-infrared are short compared to typical tweezer spacings in the micrometer range. Here, we use 88^{88}88Sr atoms in optical tweezer arrays to access a mid-infrared transition at 2,923 nm (5s5p 3P2→ 5s4d 3D35s5p\:^{3}P_{2} \rightarrow\, 5s4d\:^{3}D_{3}5s5p3P2​→5s4d3D3​). We identify a magic trapping wavelength at 597.14(3) nm and demonstrate single-atom preparation and imaging with high fidelity. In addition, using 2,923 nm light, we demonstrate resolved-sideband cooling of tweezer-trapped strontium. Beyond enabling studies of collective emission phenomena in flexible arrangements of atoms, our platform opens novel opportunities for dipolar many-body physics and enhanced control over Rydberg dynamics and the strontium fine-structure qubit.
Scalability remains a major challenge in building practical fault-tolerant quantum computers. Currently, the largest number of qubits achieved across leading quantum platforms ranges from hundreds to thousands. In atom arrays, scalability is primarily constrained by the capacity to generate large numbers of optical tweezers, and conventional techniques using acousto-optic deflectors or spatial light modulators struggle to produce arrays much beyond ∼10,000\sim 10,000∼10,000 tweezers. Moreover, these methods require additional microscope objectives to focus the light into micrometer-sized spots, which further complicates system integration and scalability. Here, we demonstrate the experimental generation of an optical tweezer array containing 280×280280\times 280280×280 spots using a metasurface, nearly an order of magnitude more than most existing systems. The metasurface leverages a large number of subwavelength phase-control pixels to engineer the wavefront of the incident light, enabling both large-scale tweezer generation and direct focusing into micron-scale spots without the need for a microscope. This result shifts the scalability bottleneck for atom arrays from the tweezer generation hardware to the available laser power. Furthermore, the array shows excellent intensity uniformity exceeding 90%90\%90%, making it suitable for homogeneous single-atom loading and paving the way for trapping arrays of more than 10,00010,00010,000 atoms in the near future.