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Low-Loss, High-Coherence Airbridge Interconnects Fabricated by Single-Step Lithography

Jibang Fu, Bo Ren, Jiandong Ouyang, Cong Li, Kechengqi Zhu, Yonggang Che, Xiang Fu, Shichuan Xue, Zhaohua Yang, Mingtang Deng, Junjie Wu

Abstract

Airbridges are essential for creating high-performance, low-parasitic interconnects in integrated circuits and quantum devices. Conventional multi-step fabrication methods hinder miniaturization and introduce process-related defects. We report a simplified process for fabricating nanoscale airbridges using only a single electron-beam lithography step. By optimizing a multilayer resist stack with a triple-exposure-dose scheme and a thermal reflow step, we achieve smooth, suspended metallic bridges with sub-200-nm features that exhibit robust mechanical stability. Fabricated within a gradiometric SQUID design for superconducting transmon qubits, these airbridges introduce no measurable additional loss in the relaxation time $T_1$, while enabling a 2.5-fold enhancement of the dephasing time $T_2^*$. This efficient method offers a practical route toward integrating high-performance three-dimensional interconnects in advanced quantum and nano-electronic devices.

Low-Loss, High-Coherence Airbridge Interconnects Fabricated by Single-Step Lithography

Abstract

Airbridges are essential for creating high-performance, low-parasitic interconnects in integrated circuits and quantum devices. Conventional multi-step fabrication methods hinder miniaturization and introduce process-related defects. We report a simplified process for fabricating nanoscale airbridges using only a single electron-beam lithography step. By optimizing a multilayer resist stack with a triple-exposure-dose scheme and a thermal reflow step, we achieve smooth, suspended metallic bridges with sub-200-nm features that exhibit robust mechanical stability. Fabricated within a gradiometric SQUID design for superconducting transmon qubits, these airbridges introduce no measurable additional loss in the relaxation time , while enabling a 2.5-fold enhancement of the dephasing time . This efficient method offers a practical route toward integrating high-performance three-dimensional interconnects in advanced quantum and nano-electronic devices.
Paper Structure (6 sections, 4 figures, 1 table)

This paper contains 6 sections, 4 figures, 1 table.

Figures (4)

  • Figure 1: Schematic of the single-lithography airbridge (SL-airbridge) fabrication process. a, Deposition, patterning, and etching of a 100-nm-thick Al base wire. b, Spin-coating of a multilayer electron-beam resist stack. c, Patterning via EBL using three distinct exposure doses. d, Thermal reflow of the developed resist stack on a hotplate. e, Ion milling of the base metal contact areas followed by electron-beam evaporation of the bridge metal (150 nm Al). f, Lift-off and ultrasonic cleaning. g, Top-view scanning electron microscopy (SEM) image of a fabricated nanoscale airbridge. h, Side-view SEM image of an airbridge taken at an 85° stage tilt.
  • Figure 2: Control experiments of reflow and triple-dose exposure scheme. Comparison of SL-airbridges fabricated a without and b with the thermal reflow step and comparison of SL-airbridges fabricated c with a double-dose exposure scheme and d with the optimized triple-dose exposure scheme.
  • Figure 3: Ultrasonic treatment tests of SL-airbridges.a, Optical images of a subset of the 60 test samples. b, Layout of a single test sample with four contact pads. c, Intact SL-airbridge after low-power ultrasonic treatment for 20 s. d, Damaged SL-airbridge after high-power ultrasonic treatment for 20 s.
  • Figure 4: Enhanced qubit coherence with SL-airbridge interconnects.a, False-color SEM image of an 8-mon qubit with an SL-airbridge (blue) connecting the two loops of the gradiometric SQUID. Inset shows a side-view SEM image at a 75° tilt. b, Highest measured $T_1$ for qubit $Q_{1}$ (8-mon with SL-airbridge). c, Highest measured $T_2^*$ for $Q_{1}$. d, Highest measured $T_1$ for qubit $Q_{4}$ (X-mon). e, Highest measured $T_2^*$ for $Q_{4}$. f, False-color SEM image of an 8-mon qubit with a dielectric (SiO$_2$, red) crossover. g, Highest measured $T_1$ for qubit $Q_{6}$ (8-mon with dielectric crossover). h, Highest measured $T_2^*$ for $Q_{6}$.