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2025-129
Response Deadline
May 16, 2026, 6:00 PM(PDT)30 days
Eligibility
Contract Type
Special Notice
Opportunity:
Lawrence Livermore National Laboratory (LLNL), operated by the Lawrence Livermore National Security (LLNS), LLC under contract no. DE-AC52-07NA27344 (Contract 44) with the U.S. Department of Energy (DOE), is offering the opportunity to enter into a collaboration to further develop and commercialize its nobel-ice-modulated superconducting circuit.
Background:
Superconducting resonators and qubits must hit target frequencies with ± kHz precision, yet lithography, thin-film variation and unknown surface adsorbates routinely scatter them by >100 MHz—forcing designers to leave wide spacing between elements, accept low wafer yield, or add lossy, noisy tuning hardware. Today’s state-of-the-art fixes are: (1) embedded SQUID loops flux-biased through extra control lines—effective but limited in range and plagued by 1/f flux noise and wiring overhead; (2) ex-situ trims such as laser annealing of Josephson junctions (LASIQ, 2022) or Alternating-Bias Assisted Anneal (ABAA, 2024)—which shrink spread at room temperature but drift back during cryogenic cooldown; and (3) geometric over-etch / dielectric varactors for MKIDs—adding fabrication steps and introducing loss. None of these approaches simultaneously offer large tuning range, zero added dissipation, minimal complexity, and the ability to correct shifts after the device reaches its 10 mK operating temperature. A gap therefore remains for a passive, cryogenic, loss-free post-fabrication tuning method that can collapse frequency scatter without compromising coherence or scaling economics—a gap the neon-ice heater technology directly targets
Description:
A neon-filled, hermetic package lets a thin film of solid neon coat a superconducting-resonator chip at millikelvin temperatures. Simple on-chip heaters briefly raise local spots to ≈25 K, causing the neon ice there to sublimate and redeposit elsewhere; thinning or thickening this ultra-low-loss dielectric shifts each resonator (or qubit) frequency with kHz precision over a MHz–GHz range. After tuning, heaters turn off, leaving a passive, loss-free device. Unlike SQUID flux lines (added noise), ex-situ laser or galvanic anneals (drift on cooldown), and dielectric varactors (extra loss), this method corrects frequency scatter in situ without new materials, masks, or steady control lines—turning a yield-limiting fabrication tolerance into a quick software trim inside the fridge.
Advantages/Benefits:
The neon-ice trimming platform beats every existing tuner on four fronts: Accuracy & range — kHz-level resolution across MHz-to-GHz spans at 10 mK, whereas SQUID loops or laser anneals top out at tens of MHz; Zero added loss — inert neon and superconducting heaters leave the resonator Q unchanged, unlike flux lines (1/f noise) or dielectric varactors (tan δ penalties); Simplicity — heaters pattern in the same mask set, no extra materials, masks, or bias wiring once tuning is done; Post-cooldown adjustability — corrects the 0.2 % drifts that cripple ex-situ trims. Those advantages translate into hard economic value: looser lithography specs, far higher wafer yield, and denser qubit/MKID packing, which together slash cost per qubit or pixel while boosting gate fidelity and sensor resolution. Because the method is geometry-agnostic, it unifies frequency control across multi-interleave (multi-IL) chip architectures—letting stacked or chiplet layers share a single, passive tuning scheme rather than bespoke flux or dielectric elements—simplifying the overall system and accelerating adoption by quantum-processor and cryogenic-sensor manufacturers.
Potential Applications:
Potential applications span the full cryogenic-electronics landscape: superconducting quantum-processor makers (IBM, Google, Rigetti, AWS, etc.) can use neon-ice trimming to lift qubit yield, gate fidelity and layout density, while commercial wafer foundries (e.g., IMEC, GlobalFoundries’ Cryo-CMOS lines) could offer a “neon-tuned” option that relaxes lithography tolerances yet still bins devices into tight frequency windows. The same capability unlocks denser, higher-resolution Microwave Kinetic-Inductance Detector (MKID) arrays for ground-based or space infrared/sub-millimeter telescopes, and provides a passive, vibration-tolerant tuning method for satellite IR imagers, Earth-observation payloads and missile-warning sensors. In fundamental physics, high-Q resonator combs used in axion and dark-matter haloscope experiments can sweep wider frequency bands without sacrificing quality factor, accelerating search rates. Beyond these headline markets, precise cryogenic frequency control benefits superconducting parametric amplifiers, RF filter banks and ultra-wideband spectrum analyzers, while fridge vendors can monetize “neon-ready” retrofit kits and heater-control electronics for the growing base of quantum-research cryostat.
Development Status:
Current stage of technology development: TRL ☒ 0-2 ☐ 3-5 ☐ 5-9
LLNL has filed for patent protection on this invention.
LLNL is seeking industry partners with a demonstrated ability to bring such inventions to the market. Moving critical technology beyond the Laboratory to the commercial world helps our licensees gain a competitive edge in the marketplace. All licensing activities are conducted under policies relating to the strict nondisclosure of company proprietary information.
Please visit the IPO website at https://ipo.llnl.gov/resources for more information on working with LLNL and the industrial partnering and technology transfer process.
Note: THIS IS NOT A PROCUREMENT. Companies interested in commercializing LLNL's nobel-ice-modulated superconducting circuit should provide an electronic OR written statement of interest, which includes the following:
Please provide a complete electronic OR written statement to ensure consideration of your interest in LLNL's nobel-ice-modulated superconducting circuit.
The subject heading in an email response should include the Notice ID and/or the title of LLNL’s Technology/Business Opportunity and directed to the Primary and Secondary Point of Contacts listed below.
Written responses should be directed to:
Lawrence Livermore National Laboratory
Innovation and Partnerships Office
P.O. Box 808, L-779
Livermore, CA 94551-0808
Attention: 2025-129
DEPARTMENT OF ENERGY
DEPARTMENT OF ENERGY
LLNS – DOE CONTRACTOR
LLNS – DOE CONTRACTOR
7000 East Avenue
Livermore, CA, 94551
NAICS
Semiconductor and Related Device Manufacturing