
Scientists have demonstrated a CMOS‑compatible process for fabricating tantalum nitride (TaN) nanowires and TaN/copper bilayer nanowires on 300 mm silicon wafers. Integrating a copper heatsink increased the Skocpol‑Beasley‑Tinkham β parameter and effective interfacial heat‑transfer efficiency by roughly 100‑fold, yielding near‑unity critical‑to‑retrapping current ratios. The devices showed less than 5 % variation in key dimensions and superconducting metrics across the wafer, confirming high uniformity. These results pave the way for fast, large‑area superconducting nanowire single‑photon detector (SNSPD) arrays for quantum computing and other advanced applications.
Superconducting nanowire single‑photon detectors have become the gold standard for ultra‑low‑noise optical sensing, yet their performance is limited by the time required for the nanowire to cool after a photon‑induced hotspot. Conventional TaN nanowires rely on intrinsic phonon cooling, which can lead to microsecond‑scale reset times and constrain array density. By embedding a thin copper layer directly beneath the superconducting filament, researchers create an efficient thermal conduit that rapidly extracts heat to the substrate, addressing one of the most persistent bottlenecks in SNSPD technology.
The experimental data reveal a roughly 100‑fold increase in the Skocpol‑Beasley‑Tinkham slope parameter β, a metric that directly reflects interfacial heat‑transfer efficiency. Simultaneously, the critical‑to‑retrapping current ratio approaches unity, indicating that the copper heatsink does not degrade the superconducting margin. Uniformity measurements across a full 300 mm wafer show less than 5 % variation in critical dimensions, resistance, and critical temperature, confirming that the process is compatible with standard CMOS lines. This combination of thermal performance and manufacturing scalability is unprecedented for SNSPDs.
With fast reset times now attainable, large‑area detector arrays can be fabricated without sacrificing sensitivity, opening new possibilities in photonic quantum computing, deep‑space cosmology instruments, and neuromorphic sensing platforms. The wafer‑scale approach also reduces per‑device cost, making high‑performance quantum photonics more accessible to research labs and commercial ventures. Ongoing work will explore geometry tuning and alternative metal heatsinks to push β even higher, while preserving the 4.1 K critical temperature of TaN. The integration of copper‑based thermal management thus marks a pivotal step toward mass‑produced, high‑speed quantum detectors.
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