Michael L. W. Thewalt
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
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Research Interests
Michael L. W. Thewalt has a total of 409 co-authors. Here are the top co-authors by number of shared publications:
H. Riemann
Leibniz-Institut für Kristallzüchtung, Berlin 12489, Germany
22 shared publicationsA. Yang
Simon Fraser University 1 Department of Physics Burnaby, British Columbia V5A 1S6, Canada
20 shared publicationsM. Steger
Department of Physics, Simon Fraser University, Burnaby, BC, Canada
20 shared publicationsN. V. Abrosimov
Leibniz-Institut für Kristallzüchtung, Berlin 12489, Germany
20 shared publicationsS. P. Watkins
Department of Physics, Simon Fraser University, Burnaby, British Columbia, Canada
20 shared publicationsP. Becker
Physikalisch-Technische Bundestanstalt Braunschweig, Braunschweig 38116, Germany
17 shared publications
Latest Publications
- Open Access
- 17 February 2026
- Published by American Physical Society (APS) in Physical Review B
- Vol. 113 (7)
Strained donor-bound excitons in Si 28
We present a comprehensive experimental study of the neutral donor to donor-bound exciton transition ( D 0 → D 0 X ) in isotopically enriched Si 28 , focusing on the group V donors P, As, and Sb under finely tuned uniaxial stress along the [100] and [110] crystal axes and magnetic fields from 3.5 mT to 1.7 T. From these measurements, donor-specific deformation potentials are extracted. The uniaxial electron deformation potential Ξ u is found to be significantly larger than values reported for other states or transitions in silicon and shows clear dependence on the donor species, indicating an increased sensitivity of the D 0 X state to strain and central-cell effects. We also observe a magnetic field dependence of the hole shear deformation potential d , suggesting a more complex strain coupling mechanism than captured by standard theory. Diamagnetic shift parameters determined from Zeeman spectra show good agreement with earlier measurements. Our results provide a refined parameter set critical for the design of silicon quantum devices based on D 0 X transitions.
- 17 February 2026
- Published by American Physical Society (APS) in Physical Review B
- Vol. 113 (7)
Open AccessStrained donor-bound excitons in Si 28
We present a comprehensive experimental study of the neutral donor to donor-bound exciton transition ( D 0 → D 0 X ) in isotopically enriched Si 28 , focusing on the group V donors P, As, and Sb under finely tuned uniaxial stress along the [100] and [110] crystal axes and magnetic fields from 3.5 mT to 1.7 T. From these measurements, donor-specific deformation potentials are extracted. The uniaxial electron deformation potential Ξ u is found to be significantly larger than values reported for other states or transitions in silicon and shows clear dependence on the donor species, indicating an increased sensitivity of the D 0 X state to strain and central-cell effects. We also observe a magnetic field dependence of the hole shear deformation potential d , suggesting a more complex strain coupling mechanism than captured by standard theory. Diamagnetic shift parameters determined from Zeeman spectra show good agreement with earlier measurements. Our results provide a refined parameter set critical for the design of silicon quantum devices based on D 0 X transitions.
- 4 February 2026
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 136 (5) , 053602
Giant Isotope Effect on the Excited-State Lifetime and Emission Efficiency of the Silicon T Center
Efficient single-photon emitters are desirable for quantum technologies including quantum networks and photonic quantum computers. We investigate the T center, a telecommunications-band emitter in silicon, and find a strong isotope dependence of its excited-state lifetime. In particular, the lifetime of the deuterium T center is over five times longer than the common protium variant. We measure an isotope-dependent shift of the local vibrational carbon-hydrogen stretch mode energy and show through explicit first-principles calculations that the dramatic lifetime difference is consistent with strong suppression of nonradiative decay due to the reduced energy of this mode for deuterium T centers. Our results imply that the deuterium T center approaches unit quantum efficiency, enabling more efficient single-photon sources and quantum memories and improved readout of the T center electron spin.
- 4 February 2026
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 136 (5) , 053602
Giant Isotope Effect on the Excited-State Lifetime and Emission Efficiency of the Silicon T Center
Efficient single-photon emitters are desirable for quantum technologies including quantum networks and photonic quantum computers. We investigate the T center, a telecommunications-band emitter in silicon, and find a strong isotope dependence of its excited-state lifetime. In particular, the lifetime of the deuterium T center is over five times longer than the common protium variant. We measure an isotope-dependent shift of the local vibrational carbon-hydrogen stretch mode energy and show through explicit first-principles calculations that the dramatic lifetime difference is consistent with strong suppression of nonradiative decay due to the reduced energy of this mode for deuterium T centers. Our results imply that the deuterium T center approaches unit quantum efficiency, enabling more efficient single-photon sources and quantum memories and improved readout of the T center electron spin.
- 13 January 2026
- Published by American Physical Society (APS) in Physical Review B
- Vol. 113 (3)
Silicon T -center hyperfine structure and memory protection schemes
- 13 January 2026
- Published by American Physical Society (APS) in Physical Review B
- Vol. 113 (3)
Silicon T -center hyperfine structure and memory protection schemes
- Open Access
- 16 September 2025
- Published by American Physical Society (APS) in PRX Quantum
- Vol. 6 (3)
Laser-Induced Spectral Diffusion and Excited-State Mixing of Silicon T Centers
To find practical application as photon sources for entangled optical-resource states or as spin-photon interfaces in entangled networks, semiconductor emitters must produce indistinguishable photons with high efficiency and spectral stability. Nanophotonic cavity integration increases efficiency and bandwidth but it also introduces environmental charge instability and spectral diffusion. Among various candidates, silicon color centers have emerged as compelling platforms for integrated-emitter quantum technologies. Here, we investigate the dynamics of spectral wandering in nanophotonics-coupled individual silicon T centers using spectral correlation measurements. We observe that spectral fluctuations are driven predominantly by the near-infrared excitation laser, consistent with a power-dependent Ornstein-Uhlenbeck process, and we show that the spectrum is stable for up to 1.5 ms in the dark. We demonstrate a factor-of- 35 narrowing of the emitter linewidth to 110 MHz using a resonance-check scheme and discuss the advantage for pairwise entanglement rates and optical-resource-state generators. Finally, we report laser-induced spin mixing in the excited state and discuss potential mechanisms common to both phenomena. These effects must be considered in calibrating T-center devices for high-performance entanglement generation.
- 16 September 2025
- Published by American Physical Society (APS) in PRX Quantum
- Vol. 6 (3)
Open AccessLaser-Induced Spectral Diffusion and Excited-State Mixing of Silicon T Centers
To find practical application as photon sources for entangled optical-resource states or as spin-photon interfaces in entangled networks, semiconductor emitters must produce indistinguishable photons with high efficiency and spectral stability. Nanophotonic cavity integration increases efficiency and bandwidth but it also introduces environmental charge instability and spectral diffusion. Among various candidates, silicon color centers have emerged as compelling platforms for integrated-emitter quantum technologies. Here, we investigate the dynamics of spectral wandering in nanophotonics-coupled individual silicon T centers using spectral correlation measurements. We observe that spectral fluctuations are driven predominantly by the near-infrared excitation laser, consistent with a power-dependent Ornstein-Uhlenbeck process, and we show that the spectrum is stable for up to 1.5 ms in the dark. We demonstrate a factor-of- 35 narrowing of the emitter linewidth to 110 MHz using a resonance-check scheme and discuss the advantage for pairwise entanglement rates and optical-resource-state generators. Finally, we report laser-induced spin mixing in the excited state and discuss potential mechanisms common to both phenomena. These effects must be considered in calibrating T-center devices for high-performance entanglement generation.
- 11 September 2025
- Published by Springer Nature in Nature Photonics
- Vol. 19 (10) , 1132-1137
Electrically triggered spin–photon devices in silicon
- 11 September 2025
- Published by Springer Nature in Nature Photonics
- Vol. 19 (10) , 1132-1137
Electrically triggered spin–photon devices in silicon
- Open Access
Electrically-triggered spin-photon devices in silicon
Quantum networking and computing technologies demand scalable hardware with high-speed control for large systems of quantum devices. Solid-state platforms have emerged as promising candidates, offering scalable fabrication for a wide range of qubits. Architectures based on spin-photon interfaces allow for highly-connected quantum networks over photonic links, enabling entanglement distribution for quantum networking and distributed quantum computing protocols. With the potential to address these demands, optically-active spin defects in silicon are one proposed platform for building quantum technologies. Here, we electrically excite the silicon T centre in integrated optoelectronic devices that combine nanophotonic waveguides and cavities with p-i-n diodes. We observe single-photon electroluminescence from a cavity-coupled T centre with $g^{(2)}(0)=0.05(2)$. Further, we use the electrically-triggered emission to herald the electron spin state, initializing it with $92(8)\%$ fidelity. This shows, for the first time, electrically-injected single-photon emission from a silicon colour centre and a new method of electrically-triggered spin initialization. These findings present a new telecommunications band light source for silicon and a highly parallel control method for T centre quantum processors, advancing the T centre as a versatile defect for scalable quantum technologies.Open AccessElectrically-triggered spin-photon devices in silicon
Quantum networking and computing technologies demand scalable hardware with high-speed control for large systems of quantum devices. Solid-state platforms have emerged as promising candidates, offering scalable fabrication for a wide range of qubits. Architectures based on spin-photon interfaces allow for highly-connected quantum networks over photonic links, enabling entanglement distribution for quantum networking and distributed quantum computing protocols. With the potential to address these demands, optically-active spin defects in silicon are one proposed platform for building quantum technologies. Here, we electrically excite the silicon T centre in integrated optoelectronic devices that combine nanophotonic waveguides and cavities with p-i-n diodes. We observe single-photon electroluminescence from a cavity-coupled T centre with $g^{(2)}(0)=0.05(2)$. Further, we use the electrically-triggered emission to herald the electron spin state, initializing it with $92(8)\%$ fidelity. This shows, for the first time, electrically-injected single-photon emission from a silicon colour centre and a new method of electrically-triggered spin initialization. These findings present a new telecommunications band light source for silicon and a highly parallel control method for T centre quantum processors, advancing the T centre as a versatile defect for scalable quantum technologies. - 3 December 2024
- Published by American Physical Society (APS) in Physical Review Applied
- Vol. 22 (6)
Optical-transition parameters of the silicon center- 3 December 2024
- Published by American Physical Society (APS) in Physical Review Applied
- Vol. 22 (6)
Optical-transition parameters of the silicon center- 10 September 2024
- Published by American Physical Society (APS) in Physical Review B
- Vol. 110 (12) , 125414
Impact of electrostatic crosstalk on spin qubits in dense CMOS quantum dot arrays
Current complementary metal-oxide semiconductor (CMOS) quantum processors employ dense gate arrays to define quantum dots, making them susceptible to crosstalk from capacitive coupling between the dots and the neighboring gates. Small but sizable spin-orbit interactions can transfer this electrostatic crosstalk to the spin factors, creating a dependence of the Larmor frequency on the electric field generated by gate electrodes positioned tens of nanometers apart. We study the Stark shift from tens of CMOS spin qubits measured in nine devices and develop a theoretical framework that explains how electric fields couple to the spin of the electrons in increasingly complex arrays. This includes electric fluctuations that limit qubit coherence times . The results will aid in the design of robust strategies to scale CMOS quantum technology.- 10 September 2024
- Published by American Physical Society (APS) in Physical Review B
- Vol. 110 (12) , 125414
Impact of electrostatic crosstalk on spin qubits in dense CMOS quantum dot arrays
Current complementary metal-oxide semiconductor (CMOS) quantum processors employ dense gate arrays to define quantum dots, making them susceptible to crosstalk from capacitive coupling between the dots and the neighboring gates. Small but sizable spin-orbit interactions can transfer this electrostatic crosstalk to the spin factors, creating a dependence of the Larmor frequency on the electric field generated by gate electrodes positioned tens of nanometers apart. We study the Stark shift from tens of CMOS spin qubits measured in nine devices and develop a theoretical framework that explains how electric fields couple to the spin of the electrons in increasingly complex arrays. This includes electric fluctuations that limit qubit coherence times . The results will aid in the design of robust strategies to scale CMOS quantum technology.- Open Access
Room temperature quantum bit storage exceeding 39 minutes using ionized donors in 28-silicon
Quantum memories capable of storing and retrieving coherent information for extended times at room temperature would enable a host of new technologies. Electron and nuclear spin qubits using shallow neutral donors in semiconductors have been studied extensively but are limited to low temperatures ($\le$10 K); however, the nuclear spins of ionized donors have potential for high temperature operation. We use optical methods and dynamical decoupling to realize this potential for an ensemble of 31P donors in isotopically purified 28Si and observe a room temperature coherence time of over 39 minutes. We further show that a coherent spin superposition can be cycled from 4.2 K to room temperature and back, and report a cryogenic coherence time of 3 hours in the same system.
Open AccessRoom temperature quantum bit storage exceeding 39 minutes using ionized donors in 28-silicon
Quantum memories capable of storing and retrieving coherent information for extended times at room temperature would enable a host of new technologies. Electron and nuclear spin qubits using shallow neutral donors in semiconductors have been studied extensively but are limited to low temperatures ($\le$10 K); however, the nuclear spins of ionized donors have potential for high temperature operation. We use optical methods and dynamical decoupling to realize this potential for an ensemble of 31P donors in isotopically purified 28Si and observe a room temperature coherence time of over 39 minutes. We further show that a coherent spin superposition can be cycled from 4.2 K to room temperature and back, and report a cryogenic coherence time of 3 hours in the same system.
- Open Access
On-demand electrical control of spin qubits
Once called a "classically non-describable two-valuedness" by Pauli , the electron spin is a natural resource for long-lived quantum information since it is mostly impervious to electric fluctuations and can be replicated in large arrays using silicon quantum dots, which offer high-fidelity control. Paradoxically, one of the most convenient control strategies is the integration of nanoscale magnets to artificially enhance the coupling between spins and electric field, which in turn hampers the spin's noise immunity and adds architectural complexity. Here we demonstrate a technique that enables a \emph{switchable} interaction between spins and orbital motion of electrons in silicon quantum dots, without the presence of a micromagnet. The naturally weak effects of the relativistic spin-orbit interaction in silicon are enhanced by more than three orders of magnitude by controlling the energy quantisation of electrons in the nanostructure, enhancing the orbital motion. Fast electrical control is demonstrated in multiple devices and electronic configurations, highlighting the utility of the technique. Using the electrical drive we achieve coherence time $T_{2,{\rm Hahn}}\approx50 \mu$s, fast single-qubit gates with ${T_{\pi/2}=3}$ ns and gate fidelities of 99.93 % probed by randomised benchmarking. The higher gate speeds and better compatibility with CMOS manufacturing enabled by on-demand electric control improve the prospects for realising scalable silicon quantum processors.Open AccessOn-demand electrical control of spin qubits
Once called a "classically non-describable two-valuedness" by Pauli , the electron spin is a natural resource for long-lived quantum information since it is mostly impervious to electric fluctuations and can be replicated in large arrays using silicon quantum dots, which offer high-fidelity control. Paradoxically, one of the most convenient control strategies is the integration of nanoscale magnets to artificially enhance the coupling between spins and electric field, which in turn hampers the spin's noise immunity and adds architectural complexity. Here we demonstrate a technique that enables a \emph{switchable} interaction between spins and orbital motion of electrons in silicon quantum dots, without the presence of a micromagnet. The naturally weak effects of the relativistic spin-orbit interaction in silicon are enhanced by more than three orders of magnitude by controlling the energy quantisation of electrons in the nanostructure, enhancing the orbital motion. Fast electrical control is demonstrated in multiple devices and electronic configurations, highlighting the utility of the technique. Using the electrical drive we achieve coherence time $T_{2,{\rm Hahn}}\approx50 \mu$s, fast single-qubit gates with ${T_{\pi/2}=3}$ ns and gate fidelities of 99.93 % probed by randomised benchmarking. The higher gate speeds and better compatibility with CMOS manufacturing enabled by on-demand electric control improve the prospects for realising scalable silicon quantum processors.