Quantum Computing and Quantum RF Cryogenic Microwave Engineering Informational

How do I design a microwave diplexer for multiplexed qubit readout?

A microwave diplexer for multiplexed qubit readout combines or separates readout signals from qubits at different frequencies, enabling multiple qubits to share a single readout line and amplifier chain. In frequency-multiplexed readout, each qubit is coupled to a readout resonator at a unique frequency (typically spaced 50-200 MHz apart within a 4-8 GHz band). The diplexer (or multiplexer for >2 channels) routes specific frequency bands to different qubits or combines signals from multiple resonators onto a single output line. Design considerations: (1) Channel frequencies are set by the readout resonator design, typically fixed on-chip. The multiplexer must match these frequencies with minimal insertion loss (<0.5 dB) in each passband. (2) Isolation between channels (>20 dB) prevents readout tone leakage from one qubit's resonator exciting another qubit. (3) The multiplexer must operate at millikelvin temperatures, requiring superconducting or very-low-loss normal-metal construction. (4) Power handling is not a concern (readout signals are at the single-photon level, <-100 dBm). Common implementations: on-chip multiplexers using coupled CPW resonators fabricated alongside the qubits (most compact, lowest loss), PCB-based multiplexers using microstrip filters on low-loss substrates (more flexible for prototyping), and Purcell filter networks that simultaneously provide frequency multiplexing and qubit protection from T1 decay through the readout port. Current systems multiplex 5-16 qubits per readout line, with research targeting 50+ qubits per line using kinetic-inductance-based multiplexers.
Category: Quantum Computing and Quantum RF
Updated: April 2026
Product Tie-In: Cryogenic Components, Attenuators, Circulators, Cables

Multiplexed Qubit Readout Design

Frequency multiplexing of qubit readout is the primary strategy for reducing the number of readout cables and amplifiers in large-scale quantum computers. Without multiplexing, each qubit requires its own output line, circulator chain, and amplifier, creating an unsustainable scaling burden.

Common Questions

Frequently Asked Questions

How many qubits can share one readout line?

Current systems: 5-16 qubits per readout line (Google: 8, IBM: 5-8, Rigetti: 8-16). Practical limits: frequency space (4-8 GHz band divided by 50-200 MHz spacing = 20-80 channels), readout resonator Q (determines minimum spacing without channel overlap), amplifier bandwidth (JPA: ~20 MHz supports 1-3 channels; TWPA: ~4 GHz supports 20-80 channels), and room-temperature electronics (need one DAC/ADC channel per qubit readout frequency). Research demonstrations have shown up to 50+ multiplexed readout resonators in a single band using kinetic inductance detectors, but maintaining qubit readout fidelity with that density has not been fully demonstrated.

What insertion loss is acceptable for the multiplexer?

On the output (readout) side: every dB of multiplexer insertion loss directly degrades readout SNR. Target <0.5 dB. On-chip multiplexers using superconducting CPW resonators achieve insertion loss of 0.1-0.3 dB per channel. PCB-based external multiplexers add 0.5-2 dB due to connector transitions and normal-metal conductor losses. On the input (drive) side: insertion loss is less critical because the signal power can be increased at the source. However, multiplexer loss at the MC stage generates thermal noise at ~20 mK, which is negligible (n_th = 0.083 at 5 GHz), so even 3-5 dB of loss is acceptable if the room-temperature electronics can compensate.

Does multiplexing affect readout fidelity?

Multiplexing can slightly reduce readout fidelity compared to dedicated per-qubit readout through several mechanisms: (1) Residual crosstalk between channels (a strong readout signal from qubit A leaking into qubit B's measurement). With 200 MHz spacing and Q_c = 2000: crosstalk < -30 dB, contributing <0.1% measurement error. (2) Amplifier dynamic range: the TWPA/JPA must simultaneously amplify N readout signals. The total power (N × per-channel power) must remain below the amplifier P1dB. For N = 16 and per-channel power of -130 dBm at the amplifier: total = -130 + 12 = -118 dBm, well below the JPA P1dB of -100 dBm. (3) Room-temperature demodulation errors: imperfect digital filtering between closely-spaced channels. These effects are manageable with careful design and are far outweighed by the cabling and thermal benefits of multiplexing.

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