Pith. sign in

REVIEW 5 minor 36 references

A versatile laser-machined rf trap for arrays of 100+ ions

T0 review · 0 major / 5 minor · reviewed 2026-08-02 · deepseek-v4-flash

Challenge this review Re-run · record.json Download PDF Read on arXiv ↗

Pith's one-line read A single rf trap made from laser-machined fused-silica wafers confines more than 100 ions in flat two-dimensional arrays, together with several distinct one-dimensional ion configurations, using only ten independently biased electrodes.

desk verdict A practical, well-characterized stacked-wafer trap that delivers >100-ion 2D crystals; the core claims hold, with a few unsupported side numbers that deserve tightening. read the letter →

arxiv 2607.13342 v1 pith:MOCRKDCP submitted 2026-07-15 quant-ph

Frank G. Schroer , Ilyoung Jung , Thomas W. Burkle , Jack B. Lyons , Joseph W. Van Vlack , Joseph Ezuma , Philip Richerme This is my paper
classification quant-ph
keywords iontrap2Dcrystalsquantumsimulationselectivelaseretchingstacked-wafermicromotioncompensationsecularfrequenciesCoulomb
verification ladder T0 review T1 audit T2 compute T3 formal

The pith

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The reading

The paper aims to establish that a macroscopic rf trap assembled from laser-etched fused-silica wafers can serve as a flexible quantum-simulation platform for large ion crystals. It demonstrates trapping of up to 154 ions in lateral two-dimensional arrays, as well as long one-dimensional chains, near-uniformly spaced strings, and split-well double chains, all shaped by ten independently biased dc electrodes. The small ion-electrode distance gives radial secular frequencies above 2π×3.5 MHz at only 165 V, while the measured heating rate is 257±41 quanta/s. If the approach works as claimed, it offers a low-cost and easily assembled route to large, reconfigurable ion arrays without monolithic microfabrication.

What carries the argument

The load-bearing component is the stacked-wafer geometry: two outer dc electrode layers and a central rf layer, separated by spacer wafers, with features defined by selective laser etching to 1–3 µm tolerances. The ten independently biased electrodes (endcaps, midcaps, and center electrodes) shape the axial potential, which is what allows the different crystal configurations. The 100 µm ion-electrode distance provides high radial confinement, and rotating the principal axes with dc voltages aligns the probe-beam wavevector with one radial mode, suppressing micromotion-driven heating in two-dimensional crystals.

What would settle it

Run the published finite-element model for the N=54 voltage set and check whether the observed rectangular interior lattice is a predicted equilibrium; if no voltage set reproduces it, the claim that it is a stable trapping configuration is unsupported. Alternatively, operate the same trap under cryogenic vacuum and see whether crystals beyond roughly 200 ions remain stable; if they melt or heat from rf-induced effects rather than background collisions, the N≈1,000 scaling estimate fails.

Watch

Extended reading notes

Core claim

The central discovery is that a five-layer stacked-wafer rf trap, with electrodes patterned by selective laser etching, provides enough precision and electrode flexibility to support large two-dimensional Coulomb crystals and multiple one-dimensional geometries in a single device. Ten grounded and ten independently biased dc electrodes shape the axial potential: weak axial confinement gives long harmonic chains, raised center-electrode voltages produce near-uniform spacing, and further increases create a symmetric double well. Raising the endcap voltages makes the axial and one radial confinement comparable, so ions self-assemble into lateral two-dimensional crystals; the largest demonstrate

Load-bearing premise

The estimate that nearly 1,000 ions can be confined assumes that background-gas collisions and off-axis micromotion are the only practical limits; if the electrode geometry introduces extra anharmonicity or rf heating for large crystals, that scaling estimate fails.

Editorial extensions

If this is right

  • Groups can build a versatile ion-trap quantum simulator from commercially laser-machined parts and the published design files, without monolithic fabrication.
  • The demonstrated 154-ion two-dimensional arrays and near-uniform one-dimensional chains offer starting points for quantum simulation experiments needing large, regularly spaced qubit registers.
  • The measured 257 quanta/s heating rate, below comparable room-temperature laser-machined traps, suggests the design can support coherent operations without cryogenic equipment.
  • The voltage-controlled principal-axis rotation provides a general method to suppress micromotion coupling in lateral two-dimensional crystals.
  • With improved vacuum, the paper estimates that nearly 1,000 ions could be confined in the same two-dimensional geometry.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • The N=54 rectangular interior lattice, reported without a supporting simulation, may indicate a new class of finite 2D Coulomb crystal structures; running the published model for that voltage set would show whether it is a true equilibrium or a metastable configuration.
  • The same stacked-wafer construction could be adapted to other laser-machinable substrates such as alumina, sapphire, or diamond, potentially improving thermal conductivity or reducing charging.
  • A natural testable extension is to measure heating rate and crystal stability as a function of ion number; the paper's assumption that background pressure is the main limit predicts that cryogenic vacuum should sharply extend the stable array size.
  • The estimated 20 Hz inter-well coupling in the split-well configuration suggests a tunable platform for studying weak-link quantum systems, though the paper does not investigate that direction.
Share X Bluesky LinkedIn Reddit HN

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, and a circularity audit.

Referee Report

0 major / 5 minor

Summary. The paper introduces a laser-machined stacked-wafer Paul trap for trapped-ion quantum simulation. The design uses ten independently biased dc electrodes on fused-silica substrates, enabling flexible shaping of the axial potential and radial confinement. The authors characterize the trap by measuring radial secular frequencies above 2π×3.5 MHz at low rf amplitudes, demonstrating micromotion compensation, rotating the principal axes, and measuring a heating rate of 257±41 quanta/s. They trap 1D chains (harmonic, uniformly spaced, double-well) and lateral 2D crystals containing up to 154 ions, and they estimate that nearly 1,000 ions could be confined under cryogenic vacuum. The manuscript includes CAD models, parts lists, and datasets.

Significance. The paper is a strong experimental contribution: the fabrication approach is accessible and low-cost, the open-data/CAD policy is exemplary, and the quantitative characterization in Figs. 2–4 directly supports the central claims. The demonstration of >100-ion lateral 2D crystals in a macroscopic, easy-to-assemble trap is important for the quantum simulation community. Several side claims are not supported by derivations or models — e.g., the "theoretical minimum" spacing variation, the 20 Hz inter-well coupling, and the unpredicted rectangular lattice — but these do not affect the main results and can be addressed with local revisions.

minor comments (5)
  1. [Results, Ion Trapping and Manipulation, Fig. 5(b)] The claim that the measured ~4% spacing variation is "consistent with the theoretical minimum for a trap with 10 static electrodes" is stated without derivation or citation. Please provide a quantitative argument for this bound, or soften the statement to "comparable to the expected limit for our electrode geometry."
  2. [Results, Ion Trapping and Manipulation, Fig. 5(c)] The "20 Hz inter-well coupling strength" estimate is not defined. Specify the model used (e.g., normal-mode splitting, tunneling rate) and the parameters (ion spacing, barrier height, well curvature) that yield 20 Hz.
  3. [Results, Ion Trapping and Manipulation, Fig. 7(c)] The claim that the N=54 crystal exhibits "a rectangular lattice in the interior... which has not been previously predicted in the literature" is a strong novelty claim. Without a structural model or explicit comparison to known phase diagrams, please provide a reference or rephrase to avoid overclaiming.
  4. [Discussion] The N≈1000 estimate assumes that background pressure and off-axis micromotion are the only practical limits. The text already conditions this on cryogenic vacuum and symmetric lattices; please also explicitly acknowledge that anharmonicity and rf heating may alter the limit at large ion numbers.
  5. [Data Availability and References] The data DOI is a placeholder (10.XXXX); please provide the resolved DOI. Additionally, there are small typographical errors (e.g., "Hammamatsu" → "Hamamatsu" in Methods; ref. 22 "Schifffer" → "Schiffer"; inconsistent notation for the 2S1/2 electronic state).

Circularity Check

0 steps flagged · score 1.0 of 10

No significant circularity: central claims are directly experimentally demonstrated, and the few extrapolations are clearly labeled estimates.

full rationale

The paper's central claims—trapping 1D chains, uniformly spaced and split-well configurations, lateral 2D arrays up to N=154 ions, radial frequencies above 2π×3.5 MHz, micromotion compensation, principal-axis rotation, and heating rate—are supported by direct measurements: sideband fits in Fig. 2, micromotion modulation-index data in Fig. 3, principal-axis suppression in Fig. 4, and fluorescence images in Figs. 5–7. Eq. 3 is a standard Paul-trap pseudopotential expression fitted to observed secular-frequency versus rf-voltage data in Fig. 2; it is a characterization model, not a source of the demonstrated ion crystals or ion numbers. The FEM predictions in Fig. 1 are parameter-free geometry-and-voltage calculations whose outputs are then compared with experiment; that is a normal theory-experiment loop, not circularity. The N≈1000 estimate in the Discussion is explicitly conditional ('It is likely that realizing these very large ion numbers in practice will require cryogenic-level vacuum pressures, highly symmetric ion lattices, and minimal cross-coupling...') and is presented as an extrapolation, not as evidence for the central result. The only self-citation (ref. 54, Kyprianidis/Rasmusson/Richerme) provides background motivation about uniform spacing and double-well applications; it is not load-bearing for any derived quantity. No equation reduces to its own input, and no fitted parameter is renamed as a prediction. The novel rectangular-lattice observation lacks a supporting model, but that is a completeness limitation, not a circular step.

Assumptions & free parameters 2 free parameters · 3 assumptions · 0 invented entities

The central claim is an engineered device, so no new physical entities are introduced. The main inputs are fitted geometric factors and empirically chosen voltages. The paper does not postulate new forces, particles, or conserved quantities.

free parameters (2)
  • Geometric factors κ, γ, ζ in Eq. 3 = Not given explicitly; obtained by fitting Eq. 3 to measured secular frequencies in Fig. 2.
    These dimensionless coefficients describe the electrode geometry and radial asymmetry. They are fitted to calibration data, not predicted a priori, and are used to characterize the trap rather than to derive a new physical effect.
  • Voltage sets for each crystal configuration = e.g., {225, 1.5, 0, 0} V for 31-ion chain; {176, 4.425, -4, 1.88} V for uniform 13-ion chain; {152, 15, 3, 5} V for 2D a
    The voltages that produce each geometry are chosen with FEM guidance and empirical adjustment, not derived from a first-principles optimization. They are experimental settings, but they are essential inputs for achieving the demonstrated configurations.
assumptions (3)
  • domain assumption Pseudopotential approximation
    Used to derive Eq. 3 and interpret secular frequencies; valid for small Mathieu q parameters, but large 2D crystals with significant micromotion may deviate.
  • domain assumption FEM simulations accurately model the trap potentials
    Electrode potentials and ion equilibrium positions are computed using FEM with assumed tolerances of 1-3 µm; real fabrication imperfections and charging may modify the fields.
  • standard math Laplace's equation for DC potentials (γ+ζ=2)
    Assumed in Eq. 2 for the harmonic expansion of the DC potential; standard for electrostatic potentials in free space.

how reviews work

0 comments
Cite this review

Pith. "Pith review of A versatile laser-machined rf trap for arrays of 100+ ions." pith.science (2026). https://pith.science/paper/MOCRKDCP

@misc{pith2026260713342,
  author       = {Pith},
  title        = {Pith review of: A versatile laser-machined rf trap for arrays of 100+ ions},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/MOCRKDCP}},
  note         = {Machine review of arXiv:2607.13342}
}
read the original abstract

Large ion crystals in diverse geometries are a key resource for quantum simulation experiments. In this work, we introduce a macroscopic rf trap that supports a wide variety of one-dimensional ion configurations as well as lateral two-dimensional crystals with more than 100 ions. Our design is based on precision-machined fused silica wafers that are stacked to form the trap structure. Ten independently biased electrodes provide flexible control over the axial potential, enabling long one-dimensional crystals, isospaced ion strings, split-well chains, and two-dimensional arrays with tunable aspect ratios. We present the design and fabrication process for this trap and demonstrate the ability to tune the radial secular frequencies, detect and compensate micromotion, rotate the principal axes, and characterize trapped ion heating rates. All trap design and documentation files are freely available alongside this work, to facilitate adoption and further development within the ion trap community.

Figures

Figures reproduced from arXiv: 2607.13342 by the authors.

Figure 1
Figure 1. (a) Exploded CAD assembly showing the trap substrates, mounting system, and electrical connections. (b) Picture of the mounted substrates and electrical connections; (c) Schematic of the central trapping region, showing the electrode geometry and coordinate axes. Voltages are applied to endcap (END), midcap (MID), and center (CTR) electrodes, which alternate with grounded (GND) electrodes. Simulated electrical poten… view at source ↗
Figure 2
Figure 2. The radial secular frequencies in the y and z directions show an approximately linear dependence on the applied rf voltage. Solid lines are fits of Eq. 3 to the measured data. The inset shows a typical Raman-driven red sideband scan, from which the radial secular frequencies are extracted. We characterize our radial trap frequencies ωy and ωz as a function of applied rf voltage V0 by probing the secular motional sid… view at source ↗
Figure 3
Figure 3. Micromotion modulation index β measured along the z direction, as a function of displacement voltage applied along the (a) x, (b) y, and (c) z trap axes. Zero displacement corresponds to the trap voltages that minimize the observed micromotion. Displacements are applied by asymmetrically biasing electrodes on opposite sides of the trap. Solid lines are fits to the data that include contributions from both intrinsic … view at source ↗
Figures from the paper (4 more)
Figure 4
Figure 4. Figure 4: (a) Simulated trap potentials when the radial principal axes have been rotated to align with the trap coordinate axes. Under these conditions, the wavevector difference ∆⃗k of our Raman beams couples only to the ωz mode. (b) When the principal axes are rotated, the ωz …
Figure 5
Figure 5. Figure 5: Ions trapped in different 1D configurations. (a) A 31-ion chain is trapped by keeping the axial confinement weak relative to the radial confinement. (b) Increasing the center electrode voltage produces a chain with near-uniform spacing. (c) Continuing to increase the c…
Figure 6
Figure 6. Figure 6: Ions trapped in near-circular 2D arrays. Crystals of (a) 3 ions, (b) 7 ions, (c) 17 ions, and (d) 19 ions self-assemble into a minimum-energy configuration when a slight frequency difference breaks the rotational symmetry of the trapping potential. When the potential s…
Figure 7
Figure 7. Figure 7: Ions trapped in lateral 2D arrays with large aspect ratio. Crystals of (a) 37 ions, (b) 49 ions, (c) 54 ions, and (d) 154 ions self-assemble into a variety of different lattice structures that depend sensitively on ion number and trap frequencies. Crystals in panels (a…

Discussion (0). Sign in to comment.

Reference graph

Works this paper leans on

36 extracted references · 1 canonical work pages

  1. [2]

    D., Boyd, M

    Ludlow, A. D., Boyd, M. M., Ye, J., Peik, E. & Schmidt, P. O. Optical atomic clocks.Rev. Mod. Phys.87, 637–701 (2015)

    2015

  2. [3]

    J.et al.Experimental issues in coherent quantum-state manipulation of trapped atomic ions.J

    Wineland, D. J.et al.Experimental issues in coherent quantum-state manipulation of trapped atomic ions.J. research Natl. Inst. Standards Technol.103, 259 (1998)

    1998

  3. [4]

    Monroe, C.et al.Programmable quantum simulations of spin systems with trapped ions.Rev. Mod. Phys.93, 025001 (2021). 5.Siverns, J. D. & Quraishi, Q. Ion trap architectures and new directions.Quantum Inf. Process.16, 314 (2017). 6.Maunz, P. High optical access trap 2.0.Tech. Rep. SAND2016-0796R(2016). 7.Revelle, M. C. Phoenix and peregrine ion traps.arXiv ...

    arXiv 2021

  4. [11]

    W., Norton, B

    Streed, E. W., Norton, B. G., Jechow, A., Weinhold, T. J. & Kielpinski, D. Imaging of trapped ions with a microfabricated optic for quantum information processing.Phys. Rev. Lett.106, 010502 (2011)

    2011

  5. [12]

    Phys.13, 103005 (2011)

    True Merrill, J.et al.Demonstration of integrated microscale optics in surface-electrode ion traps.New J. Phys.13, 103005 (2011). 13.Mehta, K. K.et al.Integrated optical multi-ion quantum logic.Nature586, 533–537 (2020). 14.Ivory, M.et al.Integrated optical addressing of a trapped ytterbium ion.Phys. Rev. X11, 041033 (2021)

    2011

  6. [15]

    M.et al.Integrated-photonics-based systems for polarization-gradient cooling of trapped ions.Light

    Corsetti, S. M.et al.Integrated-photonics-based systems for polarization-gradient cooling of trapped ions.Light. Sci. & Appl.15, 57 (2026). 16.Ospelkaus, C.et al.Microwave quantum logic gates for trapped ions.Nature476, 181–184 (2011). 17.Allcock, D.et al.A microfabricated ion trap with integrated microwave circuitry.Appl. Phys. Lett.102(2013)

    2026

  7. [18]

    M.et al.Spatially uniform single-qubit gate operations with near-field microwaves and composite pulse compensation.New J

    Shappert, C. M.et al.Spatially uniform single-qubit gate operations with near-field microwaves and composite pulse compensation.New J. Phys.15, 083053 (2013). 19.Lekitsch, B.et al.Blueprint for a microwave trapped ion quantum computer.Sci. Adv.3, e1601540 (2017)

    2013

  8. [20]

    Hughes, A.et al.Trapped-ion two-qubit gates with> 99.99% fidelity without ground-state cooling.arXiv preprint arXiv:2510.17286(2025)

    arXiv 2025

Show all 36 references
  1. [21]

    Bowers, C.et al.Robust two-qubit geometric phase gates using amplitude and frequency ramping.arXiv preprint arXiv:2511.14364(2025)

    2025

  2. [22]

    Drewsen, M., Brodersen, C., Hornekær, L., Hangst, J. S. & Schifffer, J. Large ion crystals in a linear paul trap.Phys. Rev. Lett.81, 2878 (1998). 23.Olmschenk, S.et al.Manipulation and detection of a trapped yb+ hyperfine qubit.Phys. Rev. A76, 052314 (2007)

    1998

  3. [24]

    & Ozeri, R

    Shapira, Y ., Markov, J., Akerman, N., Stern, A. & Ozeri, R. Programmable quantum simulations on a trapped-ion quantum computer with a global drive.Phys. Rev. Lett.134, 010602 (2025)

    2025

  4. [25]

    Gulde, S.Experimental realization of quantum gates and the deutsch-jozsa algorithm with trapped calcium ions. Ph.D. thesis, Universität Innsbruck (2003)

    2003

  5. [26]

    T., Porras, D

    Friedenauer, A., Schmitz, H., Glueckert, J. T., Porras, D. & Schätz, T. Simulating a quantum magnet with trapped ions. Nat. Phys.4, 757–761 (2008)

    2008

  6. [27]

    J.et al.Versatile ytterbium ion trap experiment for operation of scalable ion-trap chips with motional heating and transition-frequency measurements.Phys

    McLoughlin, J. J.et al.Versatile ytterbium ion trap experiment for operation of scalable ion-trap chips with motional heating and transition-frequency measurements.Phys. Rev. A83, 013406 (2011)

    2011

  7. [28]

    communications4, 2290 (2013)

    Ulm, S.et al.Observation of the kibble–zurek scaling law for defect formation in ion crystals.Nat. communications4, 2290 (2013). 29.Jurcevic, P.et al.Quasiparticle engineering and entanglement propagation in a quantum many-body system.Nature511, 202–205 (2014). 10/12

    2013

  8. [30]

    31.Xie, Y .et al.An open-endcap blade trap for radial-2d ion crystals.Quantum Sci

    Debnath, S.et al.Demonstration of a small programmable quantum computer with atomic qubits.Nature536, 63–66 (2016). 31.Xie, Y .et al.An open-endcap blade trap for radial-2d ion crystals.Quantum Sci. & Technol.6, 044009 (2021)

    2016

  9. [32]

    C., Hulet, R

    Bergquist, J. C., Hulet, R. G., Itano, W. M. & Wineland, D. J. Observation of quantum jumps in a single atom.Phys. Rev. Lett.57, 1699 (1986)

    1986

  10. [33]

    Yoshimura, B., Stork, M., Dadic, D., Campbell, W. C. & Freericks, J. K. Creation of two-dimensional coulomb crystals of ions in oblate paul traps for quantum simulations.EPJ Quantum Technol.2, 2 (2015)

    2015

  11. [34]

    & Peik, E

    Huntemann, N., Sanner, C., Lipphardt, B., Tamm, C. & Peik, E. Single-ion atomic clock with 3 × 10-18 systematic uncertainty.Phys. Rev. Lett.116, 063001 (2016)

    2016

  12. [35]

    K., Kato, A., Hasanzadeh, A

    Ivory, M. K., Kato, A., Hasanzadeh, A. & Blinov, B. B. A paul trap with sectored ring electrodes for experiments with two-dimensional ion crystals.Rev. Sci. Instruments91(2020)

    2020

  13. [36]

    V ., Kato, A

    Pashinsky, B. V ., Kato, A. & Blinov, B. B. Structural transitions and melting of two-dimensional ion crystals in rf traps. Entropy27, 325 (2025)

    2025

  14. [37]

    J.Advanced ion trap development and ultrafast laser-ion interactions

    Madsen, M. J.Advanced ion trap development and ultrafast laser-ion interactions. Ph.D. thesis, University of Michigan (2006)

    2006

  15. [38]

    & Mehlstäubler, T

    Pyka, K., Herschbach, N., Keller, J. & Mehlstäubler, T. E. A high-precision segmented paul trap with minimized micromotion for an optical multiple-ion clock.Appl. Phys. B114, 231–241 (2014)

    2014

  16. [39]

    M.et al.Al+ 27 quantum-logic clock with a systematic uncertainty below 10-18.Phys

    Brewer, S. M.et al.Al+ 27 quantum-logic clock with a systematic uncertainty below 10-18.Phys. Rev. Lett.123, 033201 (2019)

    2019

  17. [40]

    & Home, J

    Ragg, S., Decaroli, C., Lutz, T. & Home, J. P. Segmented ion-trap fabrication using high precision stacked wafers.Rev. Sci. Instruments90(2019). 41.Jordan, E.et al.Scalable chip-based 3d ion traps.Quantum Sci. Technol.10, 045005 (2025)

    2019

  18. [42]

    Quantum Technol.3, 2000068 (2020)

    Wang, Y .et al.Coherently manipulated 2d ion crystal in a monolithic paul trap.Adv. Quantum Technol.3, 2000068 (2020)

    2020

  19. [43]

    Kiesenhofer, D.et al.Controlling two-dimensional coulomb crystals of more than 100 ions in a monolithic radio-frequency trap.PRX Quantum4, 020317 (2023)

    2023

  20. [44]

    Guo, S.-A.et al.A site-resolved two-dimensional quantum simulator with hundreds of trapped ions.Nature630, 613–618 (2024)

    2024

  21. [45]

    Menon, A.et al.Monolithic segmented 3d ion trap for quantum technology applications.arXiv preprint arXiv:2603.16048 (2026)

    2026

  22. [46]

    G.et al.Dataset for ‘A versatile laser-cut trap for arrays of 100+ ions’

    Schroer, F. G.et al.Dataset for ‘A versatile laser-cut trap for arrays of 100+ ions’. Indiana University DataCORE, DOI: 10.XXXX (2026). 47.D’Onofrio, M.et al.Radial two-dimensional ion crystals in a linear paul trap.Phys. Rev. Lett.127, 020503 (2021)

    2026

  23. [48]

    & Duan, L.-M

    Wang, S.-T. & Duan, L.-M. Quantum computation under micromotion in a planar ion crystal.Sci. reports5, 8555 (2015). 49.Campbell, W. C.et al.Ultrafast gates for single atomic qubits.Phys. Rev. Lett.105, 090502 (2010)

    2015

  24. [50]

    & Hensinger, W

    Siverns, J., Simkins, L., Weidt, S. & Hensinger, W. On the application of radio frequency voltages to ion traps via helical resonators.Appl. Phys. B107, 921–934 (2012)

    2012

  25. [51]

    L., Burgermeister, T

    Keller, J., Partner, H. L., Burgermeister, T. & Mehlstäubler, T. Precise determination of micromotion for trapped-ion optical clocks.J. Appl. Phys.118(2015). 52.Dubin, D. H. Theory of structural phase transitions in a trapped coulomb crystal.Phys. Rev. Lett.71, 2753 (1993). 53...

    2015

  26. [54]

    & Richerme, P

    Kyprianidis, A., Rasmusson, A. & Richerme, P. Interaction graph engineering in trapped-ion quantum simulators with global drives.New J. Phys.26, 023033 (2024)

    2024

  27. [55]

    Technol.4, 014004 (2019)

    Pagano, G.et al.Cryogenic trapped-ion system for large scale quantum simulation.Quantum Sci. Technol.4, 014004 (2019)

    2019

  28. [56]

    A., Dugan, M

    Bellouard, Y ., Said, A. A., Dugan, M. & Bado, P. Monolithic integration in fused silica: When fluidics, mechanics and optics meet in a single substrate.2009 Int. Symp. on Optomechatronic Technol.445–450 (2009). 57.Johnson, K. G.et al.Active stabilization of ion trap radiofreq...

    2009 doi

Pith tools

Reviewed August 2, 2026 · model on record in the stance chip above.