Superconducting Qubits

last updated 2026-05-04 · +19 sources in last 30d

Physics / mechanism

Superconducting qubits exploit Josephson junctions — tunnel junctions between two superconductors separated by a thin insulator — to create artificial two-level quantum systems. Below ~20 mK, Cooper-pair tunnelling produces nonlinear inductance, making energy levels anharmonic and addressable at microwave frequencies (4–8 GHz). Key qubit types: transmon (dominant; anharmonicity ~200–300 MHz), fluxonium (longer T1, up to ~1 ms demonstrated). Gate fidelities: single-qubit >99.9%, two-qubit ~99.5% (IBM Heron, Google Willow, 2024). Coherence times T1/T2 now routinely 100–500 µs on best devices. Scaling bottleneck is cryogenic wiring fan-out and materials-limited coherence (TLS defects at interfaces, substrate, and junction oxide).

Competitive landscape

The primary qubit modality competitors are trapped ions (higher fidelity, slower gates, room-temperature laser control), photonic qubits (room-temp, hard to make deterministic gates), neutral atoms (fast reconfigurable arrays, early-stage error correction), and spin qubits in silicon (CMOS-compatible, short coherence currently). Superconducting qubits lead on gate speed (~10–100 ns) and ecosystem maturity.

ModalityGate speedCoherenceCMOS integration
Superconducting~10–100 ns100–500 µsPartial (via fab)
Trapped ion~1–10 µsSecondsNo
Spin (Si)~1–100 ns~1 msHigh potential

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