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arXiv:2603.13653

Quantum dial

Aashish Sah, Suman Kundu, Priyank Singh, Eemeli Forsbom, Vasilii Vadimov, Mikko Möttönen

quant-phSubmitted Mar 13, 2026• Announced Mar 17, 2026• 0 citations
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Abstract

Accurate control of quantum degrees of freedom is promising for sensing, communication, and computing, but building a useful quantum computer faces a central isolation-and-control challenge: qubits must remain well isolated from their environment to preserve coherence, yet also be coupled strongly enough for control, readout, and reset. Existing approaches address this challenge only partially, using separate reset elements, drive schemes, and Purcell filters, often with added complexity and tradeoffs such as heating and crosstalk. Here we introduce and demonstrate a first-generation quantum dial: a device that on demand mediates the coupling of a qubit to selected auxiliary degrees of freedom. Our implementation uses a band-stop filter between a high-coherence transmon qubit and a broadband transmission line, enabling the coupling strength to be tuned by several orders of magnitude on nanosecond timescales without significant Stark shift. In the reset configuration, we reduce the qubit energy relaxation time T1 from >150 $μ$s to about 200 ns and demonstrate reset independent of the initial state. In the control configuration, we obtain 99.99% idle fidelity and 99.9% gate fidelities for 40 ns pulses at about -110 dBm. The same device also enables thermometry of the qubit environment, reaching a noise-equivalent temperature of 0.6 mK/$\sqrt{Hz}$ at 60 mK and approaching the Cramér-Rao bound at higher temperatures. The quantum dial thus offers fast, on-demand switching between isolation and strong coupling, with potential to reduce noise and errors in future quantum processors.

Comments
Main text (25 pages, 6 figures), Supplementary material (33 pages, 22 figures, 3 tables)

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Accurate control of quantum degrees of freedom is promising for sensing, communication, and computing, but building a useful quantum computer faces a central isolation-and-control challenge: qubits must remain well isolated from their environment to preserve coherence, yet also be coupled strongly enough for control, readout, and reset. Existing approaches address this challenge only partially, using separate reset elements, drive schemes, and Purcell filters, often with added complexity and tradeoffs such as heating and crosstalk. Here we introduce and demonstrate a first-generation quantum dial: a device that on demand mediates the coupling of a qubit to selected auxiliary degrees of freedom. Our implementation uses a band-stop filter between a high-coherence transmon qubit and a broadband transmission line, enabling the coupling strength to be tuned by several orders of magnitude on nanosecond timescales without significant Stark shift. In the reset configuration, we reduce the qubit energy relaxation time T1 from >150 μμμs to about 200 ns and demonstrate reset independent of the initial state. In the control configuration, we obtain 99.99% idle fidelity and 99.9% gate fidelities for 40 ns pulses at about -110 dBm. The same device also enables thermometry of the qubit environment, reaching a noise-equivalent temperature of 0.6 mK/Hz\sqrt{Hz}Hz​ at 60 mK and approaching the Cramér-Rao bound at higher temperatures. The quantum dial thus offers fast, on-demand switching between isolation and strong coupling, with potential to reduce noise and errors in future quantum processors.
Rapid reset and readout of qubit states are essential for quantum error correction, yet accelerating these operations through stronger coupling to a dissipative environment inevitably increases qubit decay via the Purcell effect. Here we present a broadband Purcell filter that decouples the reset and readout paths, enabling both operations to be independently optimized without compromising qubit coherence. The filter employs two engineered notches - an intrinsic notch and a bandstop notch - to provide broadband Purcell protection, together with an additional reset stub that creates a reset mode below the protected band. To enable fast reset while suppressing filter-mediated interactions between qubits, we couple each qubit to a dedicated reset resonator. We experimentally demonstrate Purcell-limited relaxation times exceeding 1 ms across a 1.2 GHz bandwidth, simultaneously with 500 ns readout without a Josephson parametric amplifier and 100 ns reset with 99.6% efficiency. The reset resonator is designed with a deliberate kappa-chi mismatch, which suppresses photon-shot-noise-induced dephasing by a factor of 70 compared to the readout resonator. Our work provides a scalable hardware solution that resolves the traditional trade-off between fast qubit operations and qubit protection, advancing the prospects for fault-tolerant quantum computing.
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Quantum error correction imposes stringent requirements on the underlying hardware: all core operations of a quantum processor – single-qubit gates, two-qubit entangling gates, qubit readout, and qubit reset – must operate well below the error thresholds of leading codes. While such thresholds have already been crossed in several platforms, the associated overhead in physical qubits and circuit depth remains extremely sensitive to the physical error rate. This thesis investigates how far a superconducting platform based on transmon qubits can be pushed toward its physical limits, and how architectural and control choices can be optimized to reduce the overhead required for fault-tolerant quantum computation. First, we develop and characterize tunable-coupler architectures that enable fast, high-fidelity controlled-Z (CZ) gates. A long-distance coupler increases the qubit-qubit separation, freeing chip area for additional on-chip components, while still achieving CZ fidelities above 99.8%. Building on this, we optimize the qubit-coupler coupling to simultaneously support high-performance single- and two-qubit gates. We achieve simultaneous single- and two-qubit gate fidelities exceeding 99.9% on the same chip using a CZ calibration experiment based on our phase-averaged leakage error amplification (PALEA) protocol. PALEA coherently amplifies small over- and under-rotations of the diabatic CZ gate, making calibration errors easier to detect and correct. Second, we address single-qubit gates. Using spectrally engineered FAST-DRAG and higherderivative DRAG pulses, we demonstrate sub-8 ns gates with errors of order 10!" and strongly suppressed leakage. Third, we address readout by combining shelving to a higher qubit level with Purcell-filtered resonators and quantum-limited amplification, achieving readout errors below 10!#. Beyond the transmon workhorse, we explore the unimon qubit, which combines large anharmonicity with reduced charge sensitivity, and investigate a quantum circuit refrigerator as an integrated resource for fast, unconditional qubit reset via engineered dissipation. Finally, we demonstrate a cryogenic microwave link between two dilution refrigerators, enabling remote state transfer and entanglement over a five-meter distance and illustrating a path toward modular and distributed superconducting quantum processors. Together, these results show that with careful co-design of device layout, coupling topology, pulse shaping, and calibration protocols, all core operations – except qubit reset – of a superconducting quantum processor can be operated in the 10!#–10!" error regime within a coherent hardware and control stack, substantially lowering the resource overhead required for future fault-tolerant architectures.
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The ability to fast reset a qubit state is crucial for quantum information processing. However, to actively reset a qubit requires engineering a pathway to interact with a dissipative bath, which often comes at the cost of reduced qubit protection from the environment. Here, we present a multipurpose architecture that enables fast reset and protection of superconducting qubits during control and readout. In our design, two on-chip diplexers are connected by two transmission lines. The high-pass branch provides a flat passband for convenient allocation of readout resonators above the qubit frequencies, which is preferred for reducing measurement-induced state transitions. In the low-pass branch, we leverage a standing-wave mode below the maximum qubit frequency for a rapid reset. The qubits are located in the common stopband to inhibit dissipation during coherent operations. We demonstrate resetting a transmon qubit from its first excited state to the ground state in 100 ns, achieving a residual population of 2.7%. The reset time may be further shortened to 27 ns by exploiting the coherent population inversion effect. We further extend the technique to resetting the qubit from its second excited state. Our approach promises scalable implementation of fast reset and qubit protection during control and readout, adding to the toolbox of dissipation engineering.