Mark A. Eriksson
Wisconsin Alumni Research Foundation
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Publication
Featured researches published by Mark A. Eriksson.
Nature Nanotechnology | 2015
D. H. Kim; D. R. Ward; C. B. Simmons; John King Gamble; Robin Blume-Kohout; Erik Nielsen; D. E. Savage; Max G. Lagally; Mark Friesen; S. N. Coppersmith; Mark A. Eriksson
An intuitive realization of a qubit is an electron charge at two well-defined positions of a double quantum dot. This qubit is simple and has the potential for high-speed operation because of its strong coupling to electric fields. However, charge noise also couples strongly to this qubit, resulting in rapid dephasing at all but one special operating point called the sweet spot. In previous studies d.c. voltage pulses have been used to manipulate semiconductor charge qubits but did not achieve high-fidelity control, because d.c. gating requires excursions away from the sweet spot. Here, by using resonant a.c. microwave driving we achieve fast (greater than gigahertz) and universal single qubit rotations of a semiconductor charge qubit. The Z-axis rotations of the qubit are well protected at the sweet spot, and we demonstrate the same protection for rotations about arbitrary axes in the X-Y plane of the qubit Bloch sphere. We characterize the qubit operation using two tomographic approaches: standard process tomography and gate set tomography. Both methods consistently yield process fidelities greater than 86% with respect to a universal set of unitary single-qubit operations.
Physical Review B | 2017
Pasquale Scarlino; Erika Kawakami; Thibaut Jullien; D. R. Ward; D. E. Savage; Max G. Lagally; Mark Friesen; S. N. Coppersmith; Mark A. Eriksson; L. M. K. Vandersypen
The valley degree of freedom is intrinsic to spin qubits in Si/SiGe quantum dots. It has been viewed alternately as a hazard, especially when the lowest valley-orbit splitting is small compared to the thermal energy, or as an asset, most prominently in proposals to use the valley degree of freedom itself as a qubit. Here we present experiments in which microwave electric field driving induces transitions between both valley-orbit and spin states. We show that this system is highly nonlinear and can be understood through the use of dressed photon-orbital states, enabling a unified understanding of the six microwave resonance lines we observe. Some of these resonances are inter-valley spin transitions that arise from a non-adiabatic process in which both the valley and the spin degree of freedom are excited simultaneously. For these transitions, involving a change in valley-orbit state, we find a tenfold increase in sensitivity to electric fields and electrical noise compared to pure spin transitions, strongly reducing the phase coherence when changes in valley-orbit index are incurred. In contrast to this non-adiabatic transition, the pure spin transitions, whether arising from harmonic or subharmonic generation, are shown to be adiabatic in the orbital sector. The non-linearity of the system is most strikingly manifest in the observation of a dynamical anti-crossing between a spin-flip, inter-valley transition and a three-photon transition enabled by the strong nonlinearity we find in this seemly simple system.
Bulletin of the American Physical Society | 2015
Clement Wong; Mark A. Eriksson; S. N. Coppersmith; Mark Friesen
We propose an optimal set of quantum gates for a singlet-triplet qubit in a double quantum dot with two electrons utilizing the
Physical Review B | 2017
Zhenyi Qi; Xian Wu; D. R. Ward; Jonathan Prance; D. H. Kim; John King Gamble; R. T. Mohr; Zhan Shi; D. E. Savage; Max G. Lagally; Mark A. Eriksson; Mark Friesen; S. N. Coppersmith; Maxim Vavilov
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optical fiber communication conference | 2001
Mark Friesen; Paul P. Rugheimer; D. E. Savage; Max G. Lagally; Daniel W. Weide; Robert Joynt; Mark A. Eriksson
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Archive | 2005
Todd Robert Narkis; Matt S. Marcus; Max G. Lagally; Mark A. Eriksson
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Archive | 2008
Hao-Chih Yuan; Guogong Wang; Mark A. Eriksson; Paul G. Evans; Max G. Lagally; Zhenqiang Ma
subspace. Qubit rotations are driven by the applied magnetic field and an orthogonal field gradient provided by a micromagnet. We optimize the fidelity of this qubit as a function of magnetic fields, taking advantage of sweet spots where the rotation frequencies are independent of the energy level detuning, providing protection against charge noise. We simulate gate operations and qubit rotations in the presence of quasistatic noise from charge and nuclear spins as well as leakage to nonqubit states, and predict that in silicon quantum dots gate fidelities greater than
Archive | 2014
Mark A. Eriksson; John King Gamble; Daniel R. Ward; S. N. Coppersmith; Mark Friesen
99%
arXiv: Materials Science | 2004
James L. Truitt; Keith A. Slinker; K. L. M. Lewis; D. E. Savage; Charles Tahan; Levente J. Klein; Robert Joynt; Max G. Lagally; D.W. van der Weide; S. N. Coppersmith; Mark A. Eriksson; Alexei M. Tyryshkin; Jack O. Chu; P. M. Mooney
can be achieved for two nearly-orthogonal rotation axes.
Archive | 2001
Mark Friesen; Mark A. Eriksson; Robert Joynt; Max G. Lagally; Daniel W. van der Weide; Paul P. Rugheimer; D. E. Savage
We study the dynamics of a pulse-gated semiconductor double quantum dot qubit. In our experiments, the qubit coherence times are relatively long, but the visibility of the quantum oscillations is low. We show that these observations are consistent with a theory that incorporates decoherence arising from charge noise that gives rise to detuning fluctuations of the double dot. Because effects from charge noise are largest near the singlet-triplet avoided level crossing, the visibility of the oscillations are low when the singlet-triplet avoided level crossing occurs in the vicinity of the charge degeneracy point crossed during the manipulation, but there is only modest dephasing at the large detuning value at which the quantum phase accumulates. This theory agrees well with experimental data and predicts that the visibility can be increased greatly by appropriate tuning of the interdot tunneling rate.