Quantum-limited cryogenic amplifiers are the first active stage of the superconducting qubit readout chain. They amplify the ~10-photon-level readout signal to levels detectable by room-temperature electronics while adding the minimum noise allowed by quantum mechanics (). Without them, readout fidelity is limited to ~90%; with them, >99.9% single-shot fidelity is routinely achieved.
Figure

Description
Types
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Josephson Parametric Amplifier (JPA): Single-mode resonant amplifier using a Josephson junction’s nonlinearity. Narrow bandwidth (~10 MHz) but truly quantum-limited. Workhorse for single-qubit readout.
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Josephson Traveling-Wave Parametric Amplifier (JTWPA): Broadband (~4 GHz) amplifier using thousands of Josephson junctions in a transmission line. Enables frequency-multiplexed readout of many qubits simultaneously. Critical for scaling.
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HEMT (High Electron Mobility Transistor): Semiconductor amplifier at 4K stage. Higher noise (~20× quantum limit) but robust, broadband, and commercially available. Used as second-stage amplification.
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Kinetic Inductance Amplifiers (KIT): Uses the nonlinear kinetic inductance of superconducting thin films. Potentially simpler fabrication than JTWPA with comparable bandwidth.
Readout chain
Typical signal flow: qubit → readout resonator → circulator → JPA/JTWPA (20 mK) → HEMT (4K) → room-temperature ADC. The quantum-limited first stage sets the ultimate readout fidelity.
Hamiltonian
Josephson parametric amplifier (degenerate mode):
where is the Kerr nonlinearity from the Josephson junction and is the pump strength. Near-quantum-limited amplification occurs when the pump drives parametric gain: .
Performance Metrics
| Metric | Value | Notes | Fidelity reference |
|---|---|---|---|
| JPA added noise | ~0.5 photons | At quantum limit | macklin-2015-jtwpa |
| JTWPA bandwidth | ~4 GHz | 4–8 GHz typical | macklin-2015-jtwpa |
| JTWPA gain | ~20 dB | Sufficient for HEMT cascade | macklin-2015-jtwpa |
| Readout fidelity enabled | >99.9% | Single-shot, with JPA/JTWPA | macklin-2015-jtwpa |