Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Multi_Stage_Cryogenic_Architecture_with_Programmable_Dissipation

Walter Ayala

Published Sep 24, 2026• 0 citations
Publisher

Abstract

This work presents a theoretical, engineering, and experimental framework for a multi-stagecryogenic architecture with programmable thermal conductance. The objective is to inves-tigate whether dynamically controlled thermal links can modify the low-frequency thermalenvironment experienced by a superconducting quantum device without introducing compen-sating noise or instability.The architecture is represented as a lumped thermal network containing nodes with heat ca-pacities, thermal conductances, external heat loads, and stochastic heat-current sources. Thisformulation replaces a single-stage temperature-noise expression with a matrix description ofthermal fluctuations and transfer functions. For a linear network, the temperature fluctuationspectrum is obtained from the thermal susceptibility matrix and the spectral-density matrixof the dissipative heat-current sources.A central methodological distinction is made between (i) mean temperature, (ii) tempera-ture fluctuations, (iii) electromagnetic noise, (iv) mechanical/vibrational noise, and (v) qubitdecoherence. These quantities are not assumed to be equivalent.The programmable element is modeled as a controllable thermal conductance Gi(u, t).Its effect is evaluated together with the noise associated with the control mechanism, pos-sible electromagnetic coupling, mechanical coupling, and transient thermal response. Theexperimental protocol therefore contains matched passive and programmable conditions, ran-domized measurement order, independent calibration, thermal settling criteria, control-bandmeasurements, and reproducibility across cooldowns.The primary endpoint is a pre-registered, band-limited reduction in the temperature-noisepower spectral density at the quantum device stage. Secondary endpoints include integratedtemperature variance, qubit T1, qubit T∗2, and randomized-benchmarking metrics. The pro-posal does not assume that any secondary endpoint must improve.The framework is explicitly falsifiable. A programmable architecture can fail to provide anet benefit if it produces additional noise, thermal gradients, control instability, electromag-netic interference, mechanical coupling, excessive settling time, or no reproducible reductionin the predefined thermal-noise metric.

DOI
10.5281/zenodo.22942199

Related papers

Quantum_Control_System_with_Active_Thermal_Compensation

Walter Ayala

This document develops a theoretical, technical, and experimental framework for activethermal compensation of quantum-control pulses in superconducting qubits. The centralproposal is to measure a temperature-related control variable and use that information toadapt the microwave control amplitude so that the realized gate rotation is less sensitive toslow or reproducible thermal variations.Version 2.0 makes an important distinction between established physical relations andphenomenological assumptions. In particular, no universal linear dependence of the Rabifrequency on temperature is assumed. Instead, the temperature-to-control response is rep-resented by experimentally identifiable transfer functions and local calibration coefficients.Possible microscopic contributions from quasiparticles, thermal photons, two-level systems,dielectric loss, and other environmental channels are treated as candidate mechanisms ratherthan as a universal additive law.The control problem is formulated using a driven two-level Hamiltonian with both am-plitude and detuning errors. A thermal sensitivity coefficient is introduced through theexperimentally measurable derivative of the effective Rabi frequency with respect to tem-perature. The compensation law is derived from this measured response. Finite sensor andactuator bandwidth are incorporated through a causal filter and an explicit latency term.The experimental protocol combines Rabi calibration, thermal characterization, random-ized benchmarking, interleaved randomized benchmarking, and independent measurementsof T1 and T∗2. The primary experimental question is whether active thermal compensationproduces a statistically and experimentally resolvable reduction of gate error under controlledthermal perturbations.The proposal does not assume a predetermined improvement in fidelity, and it does notassume that amplitude compensation automatically suppresses all thermal decoherence. Allnumerical coefficients introduced in this document are design parameters or initial experi-mental ranges unless explicitly identified as measured quantities. No experimental result isclaimed.

•Sep 20, 2026•0 citations

Error_Correction_Protocols_with _Thermal_Information

Walter Ayala

This work proposes an experimentally falsifiable framework for incorporating real-timethermal information into quantum error correction for superconducting qubits. The centralidea is not to assume a universal thermal error law, but to determine experimentally whetherlocal temperature, thermal gradients, and related thermal observables contain predictive in-formation about physical error probabilities.Version 3.1 replaces the previous additive phenomenological error expression with a boundedstatistical model based on conditional error probabilities. For each physical error channel a,the model has the generic formp(a)i(t) = logit−1[︂β(a)0 + β(a)TδTi(t) + β(a)∇T Gi(t) + β(a)τδτ (t) + β(a)·xi(t)]︂,where Gi represents a normalized local temperature-gradient observable and xi containsoptional control variables. A physically motivated thermal occupation term may be includedas a covariate, but it is not imposed as the complete error model.Three operating modes are compared:1. Mode A: fixed-rate baseline decoder;2. Mode B: thermal-information-aware decoder with fixed cycle duration;3. Mode C: thermal-information-aware decoder with bounded adaptive cycle duration.The primary endpoint is the logical error-rate ratio between Mode B and Mode A undermatched experimental conditions. The secondary endpoint compares Mode C with Mode B.The protocol incorporates calibration, cross-validation, pre-registration of the primaryendpoint, paired experimental blocks, bootstrap confidence intervals, multiple-comparisoncontrol, systematic-error analysis, placebo tests, latency characterization, and independentcooldown reproducibility.No experimental result is claimed.

•Sep 24, 2026•0 citations

Thermal_Diagnostic_System_by_Quantum_Tomography

Walter Ayala

This version develops a rigorous experimental framework for spatial thermal diagnosticsusing superconducting qubits as distributed sensing elements. The central methodologicalchange relative to a simple frequency-to-temperature conversion is the introduction of anexplicit measurement model separating thermal and non-thermal contributions to the observedqubit-frequency shift.For sensor i,δωobsi = δωthi + δωfluxi + δωqpi + δωTLSi + δωroi + δωotheri.Only after characterization of these contributions is a temperature estimate formed. Thelocal thermal response is represented by a calibrated coefficientαi(T0) = ∂ωq,i∂T⃓⃓⃓⃓T0,with explicit uncertainty and possible nonlinear correction.The spatial inverse problem is formulated through a response matrix, a point-spreadfunction (PSF), and regularized reconstruction. Spatial resolution is therefore not identifiedsimply with sensor spacing.The protocol introduces independent reference thermometry, blocked test data, blind lo-calized thermal perturbations, cross-validation, uncertainty propagation, hierarchical analysisacross cooldowns, and predefined falsification criteria. The primary endpoint is the inde-pendently evaluated reconstruction error of the thermal field. Secondary endpoints includeeffective spatial resolution, temperature resolution, localized perturbation detection, calibrationstability, and cross-cooldown reproducibility.The proposal remains exploratory and falsifiable. It does not claim experimental validation,universal thermometry, or superiority over conventional thermal sensors.

•Sep 24, 2026•0 citations

Inherent Thermal-Noise Problem in Addressing Qubits

Slawomir Simbierowicz, Massimo Borrelli, V. Yu. Monarkha +2 more

Qubit-specific measurement in a superconducting quantum processor requires physical interconnects that traverse 4 orders of magnitude in temperature from 293 K to 10 mK. Although the quantum processor can be thermalized and shielded from electromagnetic noise, the interconnects themselves introduce an unavoidable remote heat bath that causes decoherence of quantum states. In the present work, we report quantitative and device-independent measurements of the power radiated to the quantum processor from its control lines. Our results have been obtained using a calibrated bolometer that operates within a millikelvin environment with time-resolved measurement capability. In the limit of zero applied power, the noise power emitted to the quantum processor is equivalent to that of a blackbody with temperature 63–71 mK for the prototypical drive lines in the study. Experimentally, we increase the applied power of a simulated control signal to map out the resulting temperature rise and thermal time constant of five prototypical drive-line varieties. We input the data to an open quantum system model to demonstrate the trade-off between dissipated signal power, transmon-qubit lifetime, pure dephasing, gate fidelity, and the implied decoherence rates due to self-heating during microwave operations. Beyond explaining dephasing rates observed in the literature, our work sets the stage for accurate noise modeling in novel quantum computer interfacing methods due to our device-agnostic approach. Published by the American Physical Society 2024

PRX Quantum•Jul 2, 2024•16 citations

Cryogenic electronics for quantum engineering

Loïck Le Guevel

Thousands to millions of sensitive signals will need to be conveyed through all the temperature stages of a dilution fridge to operate future large-scale quantum processors made of many quantum bits. The exploding number of heat-conductive coaxial cables will overwhelm the fridge cooling capabilities, detrimental to the quantum core. Moving the control electronics down to cryogenic temperatures allows the use of already-available superconducting cables, alleviating heat conduction between low-temperature stages, and appears as a clear path towards scalability in the number of operating qubits.This Ph.D. work aimed to explore the use of the industrial CMOS 28nm Fully-Depleted Silicon-On-Insulator (FD-SOI) technology at cryogenic temperatures for quantum computing applications. Our first objective is to extend the sparse existing knowledge about the FD-SOI 28nm transistors at cryogenic temperatures for practical aspects of circuit design and later for developments of compact models.To speed-up the characterization of single devices with the inherent hour-long cooling cycles, we designed an integrated circuit multiplexing a thousand of transistors for different geometries and gate-stack flavors for low-frequency measurement of the current-voltage characteristics and pair-matching analysis from 300 down to 0.1K. We discuss and analyze the evolution trends with varying geometry at different temperatures for important quantities in circuit design, such as the transconductance, the conductance, and the transconductance over drain current ratio of individual transistors.Secondly, we explore the low-temperature co-integration and the full on-chip integration of semiconductor quantum devices with classical electronics aimed at specific measurements down to the millikelvin range.We first focus on the sub-nanoampere current measurement of quantum dot devices by designing and characterizing a low-power transimpedance amplifier (TIA). The high-gain amplifier is successfully applied to measure the current across single- and double quantum-dot devices, respectively wire-bonded a few mm away or on-chip integrated a few micrometers-away. To further leverage the integration into the same substrate, we connected GHz-range voltage-controlled oscillators to one of the gates of the double dot in an attempt to observe discrete charge pumping in a fully-integrated device.Lastly, we tackled the measurement of the gate capacitance of single quantum devices by proposing a new measurement scheme making use of the cryogenic electronics capabilities as an alternative to the well-known reflectometry. By integrating a voltage-controlled current excitation and a voltage-sensing amplifier in the 200 MHz range, both in close proximity to the quantum device connected to an LC tank, the read-out circuitry of a variation in the device capacitance becomes a purely lumped-element system with impedance measurement of the resonant circuit without any wave propagation like in reflectometry. This approach increases simplicity and compactness of the measurement set-up. We even replace the bulky passive inductor used in reflectometry by an active inductor made of transistors and capacitors, offering improved scalability with a 3-orders of magnitude lower area for the same inductance. The resulting circuit successfully measured aF-capacitance variations of nanometric transistors at 4.2K revealing oscillatory quantum effects in the gate capacitance as a function of the gate and back-gate voltages.At the end of this dissertation, a picture is given with the challenges laying ahead related to circuit architecture and design for the ultimate goal of entering into the era of large-scale quantum processing.

•Jan 13, 2023•0 citations

Cryogenic thermal modeling of microwave high density signaling

Naomi Raicu, Tom Hogan, Xian Wu +4 more

Abstract Superconducting quantum computers require microwave control lines running from room temperature to the mixing chamber of a dilution refrigerator. Adding more lines without preliminary thermal modeling to make predictions risks overwhelming the cooling power at each thermal stage. In this paper, we investigate the thermal load of SC-086/50-SCN-CN semi-rigid coaxial cable, which is commonly used for the control and readout lines of a superconducting quantum computer, as we increase the number of lines to a quantum processor. We investigate the makeup of the coaxial cables, verify the materials and dimensions, and experimentally measure the total thermal conductivity of a single cable as a function of the temperature from cryogenic to room temperature values. We also measure the cryogenic DC electrical resistance of the inner conductor as a function of temperature, allowing for the calculation of active thermal loads due to Ohmic heating. Fitting this data produces a numerical thermal conductivity function used to calculate the static heat loads due to thermal transfer within the wires resulting from a temperature gradient. The resistivity data is used to calculate active heat loads, and we use these fits in a cryogenic model of a superconducting quantum processor in a typical Bluefors XLD1000-SL dilution refrigerator, investigating how the thermal load increases with processor sizes ranging from 100 to 225 qubits. We conclude that the theoretical upper limit of the described architecture is approximately 200 qubits. However, including an engineering margin in the cooling power and the available space for microwave readout circuitry at the mixing chamber, the practical limit is approximately 140 qubits.

arXiv:2502.01945•EPJ Quantum Technology•Oct 30, 2025•8 citations
This work presents a theoretical, engineering, and experimental framework for a multi-stagecryogenic architecture with programmable thermal conductance. The objective is to inves-tigate whether dynamically controlled thermal links can modify the low-frequency thermalenvironment experienced by a superconducting quantum device without introducing compen-sating noise or instability.The architecture is represented as a lumped thermal network containing nodes with heat ca-pacities, thermal conductances, external heat loads, and stochastic heat-current sources. Thisformulation replaces a single-stage temperature-noise expression with a matrix description ofthermal fluctuations and transfer functions. For a linear network, the temperature fluctuationspectrum is obtained from the thermal susceptibility matrix and the spectral-density matrixof the dissipative heat-current sources.A central methodological distinction is made between (i) mean temperature, (ii) tempera-ture fluctuations, (iii) electromagnetic noise, (iv) mechanical/vibrational noise, and (v) qubitdecoherence. These quantities are not assumed to be equivalent.The programmable element is modeled as a controllable thermal conductance Gi(u, t).Its effect is evaluated together with the noise associated with the control mechanism, pos-sible electromagnetic coupling, mechanical coupling, and transient thermal response. Theexperimental protocol therefore contains matched passive and programmable conditions, ran-domized measurement order, independent calibration, thermal settling criteria, control-bandmeasurements, and reproducibility across cooldowns.The primary endpoint is a pre-registered, band-limited reduction in the temperature-noisepower spectral density at the quantum device stage. Secondary endpoints include integratedtemperature variance, qubit T1, qubit T∗2, and randomized-benchmarking metrics. The pro-posal does not assume that any secondary endpoint must improve.The framework is explicitly falsifiable. A programmable architecture can fail to provide anet benefit if it produces additional noise, thermal gradients, control instability, electromag-netic interference, mechanical coupling, excessive settling time, or no reproducible reductionin the predefined thermal-noise metric.
This document develops a theoretical, technical, and experimental framework for activethermal compensation of quantum-control pulses in superconducting qubits. The centralproposal is to measure a temperature-related control variable and use that information toadapt the microwave control amplitude so that the realized gate rotation is less sensitive toslow or reproducible thermal variations.Version 2.0 makes an important distinction between established physical relations andphenomenological assumptions. In particular, no universal linear dependence of the Rabifrequency on temperature is assumed. Instead, the temperature-to-control response is rep-resented by experimentally identifiable transfer functions and local calibration coefficients.Possible microscopic contributions from quasiparticles, thermal photons, two-level systems,dielectric loss, and other environmental channels are treated as candidate mechanisms ratherthan as a universal additive law.The control problem is formulated using a driven two-level Hamiltonian with both am-plitude and detuning errors. A thermal sensitivity coefficient is introduced through theexperimentally measurable derivative of the effective Rabi frequency with respect to tem-perature. The compensation law is derived from this measured response. Finite sensor andactuator bandwidth are incorporated through a causal filter and an explicit latency term.The experimental protocol combines Rabi calibration, thermal characterization, random-ized benchmarking, interleaved randomized benchmarking, and independent measurementsof T1 and T∗2. The primary experimental question is whether active thermal compensationproduces a statistically and experimentally resolvable reduction of gate error under controlledthermal perturbations.The proposal does not assume a predetermined improvement in fidelity, and it does notassume that amplitude compensation automatically suppresses all thermal decoherence. Allnumerical coefficients introduced in this document are design parameters or initial experi-mental ranges unless explicitly identified as measured quantities. No experimental result isclaimed.
This work proposes an experimentally falsifiable framework for incorporating real-timethermal information into quantum error correction for superconducting qubits. The centralidea is not to assume a universal thermal error law, but to determine experimentally whetherlocal temperature, thermal gradients, and related thermal observables contain predictive in-formation about physical error probabilities.Version 3.1 replaces the previous additive phenomenological error expression with a boundedstatistical model based on conditional error probabilities. For each physical error channel a,the model has the generic formp(a)i(t) = logit−1[︂β(a)0 + β(a)TδTi(t) + β(a)∇T Gi(t) + β(a)τδτ (t) + β(a)·xi(t)]︂,where Gi represents a normalized local temperature-gradient observable and xi containsoptional control variables. A physically motivated thermal occupation term may be includedas a covariate, but it is not imposed as the complete error model.Three operating modes are compared:1. Mode A: fixed-rate baseline decoder;2. Mode B: thermal-information-aware decoder with fixed cycle duration;3. Mode C: thermal-information-aware decoder with bounded adaptive cycle duration.The primary endpoint is the logical error-rate ratio between Mode B and Mode A undermatched experimental conditions. The secondary endpoint compares Mode C with Mode B.The protocol incorporates calibration, cross-validation, pre-registration of the primaryendpoint, paired experimental blocks, bootstrap confidence intervals, multiple-comparisoncontrol, systematic-error analysis, placebo tests, latency characterization, and independentcooldown reproducibility.No experimental result is claimed.
This version develops a rigorous experimental framework for spatial thermal diagnosticsusing superconducting qubits as distributed sensing elements. The central methodologicalchange relative to a simple frequency-to-temperature conversion is the introduction of anexplicit measurement model separating thermal and non-thermal contributions to the observedqubit-frequency shift.For sensor i,δωobsi = δωthi + δωfluxi + δωqpi + δωTLSi + δωroi + δωotheri.Only after characterization of these contributions is a temperature estimate formed. Thelocal thermal response is represented by a calibrated coefficientαi(T0) = ∂ωq,i∂T⃓⃓⃓⃓T0,with explicit uncertainty and possible nonlinear correction.The spatial inverse problem is formulated through a response matrix, a point-spreadfunction (PSF), and regularized reconstruction. Spatial resolution is therefore not identifiedsimply with sensor spacing.The protocol introduces independent reference thermometry, blocked test data, blind lo-calized thermal perturbations, cross-validation, uncertainty propagation, hierarchical analysisacross cooldowns, and predefined falsification criteria. The primary endpoint is the inde-pendently evaluated reconstruction error of the thermal field. Secondary endpoints includeeffective spatial resolution, temperature resolution, localized perturbation detection, calibrationstability, and cross-cooldown reproducibility.The proposal remains exploratory and falsifiable. It does not claim experimental validation,universal thermometry, or superiority over conventional thermal sensors.
Qubit-specific measurement in a superconducting quantum processor requires physical interconnects that traverse 4 orders of magnitude in temperature from 293 K to 10 mK. Although the quantum processor can be thermalized and shielded from electromagnetic noise, the interconnects themselves introduce an unavoidable remote heat bath that causes decoherence of quantum states. In the present work, we report quantitative and device-independent measurements of the power radiated to the quantum processor from its control lines. Our results have been obtained using a calibrated bolometer that operates within a millikelvin environment with time-resolved measurement capability. In the limit of zero applied power, the noise power emitted to the quantum processor is equivalent to that of a blackbody with temperature 63–71 mK for the prototypical drive lines in the study. Experimentally, we increase the applied power of a simulated control signal to map out the resulting temperature rise and thermal time constant of five prototypical drive-line varieties. We input the data to an open quantum system model to demonstrate the trade-off between dissipated signal power, transmon-qubit lifetime, pure dephasing, gate fidelity, and the implied decoherence rates due to self-heating during microwave operations. Beyond explaining dephasing rates observed in the literature, our work sets the stage for accurate noise modeling in novel quantum computer interfacing methods due to our device-agnostic approach. Published by the American Physical Society 2024
Thousands to millions of sensitive signals will need to be conveyed through all the temperature stages of a dilution fridge to operate future large-scale quantum processors made of many quantum bits. The exploding number of heat-conductive coaxial cables will overwhelm the fridge cooling capabilities, detrimental to the quantum core. Moving the control electronics down to cryogenic temperatures allows the use of already-available superconducting cables, alleviating heat conduction between low-temperature stages, and appears as a clear path towards scalability in the number of operating qubits.This Ph.D. work aimed to explore the use of the industrial CMOS 28nm Fully-Depleted Silicon-On-Insulator (FD-SOI) technology at cryogenic temperatures for quantum computing applications. Our first objective is to extend the sparse existing knowledge about the FD-SOI 28nm transistors at cryogenic temperatures for practical aspects of circuit design and later for developments of compact models.To speed-up the characterization of single devices with the inherent hour-long cooling cycles, we designed an integrated circuit multiplexing a thousand of transistors for different geometries and gate-stack flavors for low-frequency measurement of the current-voltage characteristics and pair-matching analysis from 300 down to 0.1K. We discuss and analyze the evolution trends with varying geometry at different temperatures for important quantities in circuit design, such as the transconductance, the conductance, and the transconductance over drain current ratio of individual transistors.Secondly, we explore the low-temperature co-integration and the full on-chip integration of semiconductor quantum devices with classical electronics aimed at specific measurements down to the millikelvin range.We first focus on the sub-nanoampere current measurement of quantum dot devices by designing and characterizing a low-power transimpedance amplifier (TIA). The high-gain amplifier is successfully applied to measure the current across single- and double quantum-dot devices, respectively wire-bonded a few mm away or on-chip integrated a few micrometers-away. To further leverage the integration into the same substrate, we connected GHz-range voltage-controlled oscillators to one of the gates of the double dot in an attempt to observe discrete charge pumping in a fully-integrated device.Lastly, we tackled the measurement of the gate capacitance of single quantum devices by proposing a new measurement scheme making use of the cryogenic electronics capabilities as an alternative to the well-known reflectometry. By integrating a voltage-controlled current excitation and a voltage-sensing amplifier in the 200 MHz range, both in close proximity to the quantum device connected to an LC tank, the read-out circuitry of a variation in the device capacitance becomes a purely lumped-element system with impedance measurement of the resonant circuit without any wave propagation like in reflectometry. This approach increases simplicity and compactness of the measurement set-up. We even replace the bulky passive inductor used in reflectometry by an active inductor made of transistors and capacitors, offering improved scalability with a 3-orders of magnitude lower area for the same inductance. The resulting circuit successfully measured aF-capacitance variations of nanometric transistors at 4.2K revealing oscillatory quantum effects in the gate capacitance as a function of the gate and back-gate voltages.At the end of this dissertation, a picture is given with the challenges laying ahead related to circuit architecture and design for the ultimate goal of entering into the era of large-scale quantum processing.
Abstract Superconducting quantum computers require microwave control lines running from room temperature to the mixing chamber of a dilution refrigerator. Adding more lines without preliminary thermal modeling to make predictions risks overwhelming the cooling power at each thermal stage. In this paper, we investigate the thermal load of SC-086/50-SCN-CN semi-rigid coaxial cable, which is commonly used for the control and readout lines of a superconducting quantum computer, as we increase the number of lines to a quantum processor. We investigate the makeup of the coaxial cables, verify the materials and dimensions, and experimentally measure the total thermal conductivity of a single cable as a function of the temperature from cryogenic to room temperature values. We also measure the cryogenic DC electrical resistance of the inner conductor as a function of temperature, allowing for the calculation of active thermal loads due to Ohmic heating. Fitting this data produces a numerical thermal conductivity function used to calculate the static heat loads due to thermal transfer within the wires resulting from a temperature gradient. The resistivity data is used to calculate active heat loads, and we use these fits in a cryogenic model of a superconducting quantum processor in a typical Bluefors XLD1000-SL dilution refrigerator, investigating how the thermal load increases with processor sizes ranging from 100 to 225 qubits. We conclude that the theoretical upper limit of the described architecture is approximately 200 qubits. However, including an engineering margin in the cooling power and the available space for microwave readout circuitry at the mixing chamber, the practical limit is approximately 140 qubits.