spin register

Extreme quantum entanglement in a superposition of macroscopically distinct states. Article ADS MathSciNet CAS Google Scholar. Filidou, V. Ultrafast entangling gates between nuclear spins using photo-excited triplet states.

Mizuochi, N. Coherence of single spins coupled to a nuclear spin bath of varying density. B 80 , Marseglia, L. Nanofabricated solid immersion lenses registered to single emitters in diamond.

Waldherr, G. Dark states of single nitrogen-vacancy centers in diamond unraveled by single shot NMR. Aslam, N. Photo-induced ionization dynamics of the nitrogen vacancy defect in diamond investigated by single-shot charge state detection. New J. High dynamic range magnetometry with a single nuclear spin in diamond.

Nature Nanotechnol. Khaneja, N. Optimal control of coupled spin dynamics: design of NMR pulse sequences by gradient ascent algorithms. Bell, J. On the Einstein Podolsky Rosen paradox.

Physics 1 , — Article MathSciNet Google Scholar. Violation of a temporal Bell inequality for single spins in a diamond defect center. Download references. We thank F.

Dolde, I. Jakobi, M. Kleinmann, F. Jelezko, J. Honert, A. Brunner and C. Walter for experimental help and discussions. Physikalisches Institut and Research Center SCOPE, University of Stuttgart, Pfaffenwaldring 57, Stuttgart, Germany ,. Waldherr, Y. Wang, S. Zaiser, M. Jamali, P.

Department of Chemistry, Technical University of Munich, Garching, Germany,. Japan Atomic Energy Agency, Takasaki, Gunma , Japan ,.

Research Center for Knowledge Communities, University of Tsukuba, Tsukuba, Ibaraki , Japan ,. Hefei National Laboratory for Physical Sciences at the Microscale and Department of Modern Physics, University of Science and Technology of China, Hefei , China,.

Max Planck Institute for Solid State Research, Heisenbergstraße 1, Stuttgart, Germany ,. You can also search for this author in PubMed Google Scholar. and J. conceived the experiments; G. and S. prepared the sample and performed the experiments; Y. calculated the robust pulses; Y.

analysed the data; J. and P. performed the electron irradiation; M. fabricated the SIL; G. wrote the manuscript; and P. supervised the project. Correspondence to G. a , Average number of suitable 13 C spins per NV for different 13 C concentrations c and different minimum hyperfine min.

b , Spectral density of suitable lattice positions per NV for different magnetic fields B. Note that for these simulations, actual lattice positions are not taken into account. The fluctuations at higher hyperfine interaction are due to numerical grain, that is, due to discretization of the integration volume.

a , Image of the SIL in diamond. b , Saturation curves of the NV with and without the SIL measurements were performed with a oil-immersion objective.

Note that the charge state post-selection can be substituted by charge state pre-selection 34 , a , The two microwave frequencies f 1 and f 2 , relative to the electron spin transition frequencies, applied in the experiment. b , The pulse sequence on the left side shows the piecewise-constant control amplitudes Rabi frequency for the real and imaginary parts of f 1 and f 2 , where each piece bar has a duration of 1.

It realizes the controlled gate on the electron spin given on the right side. Reprints and permissions. Quantum error correction in a solid-state hybrid spin register. Download citation. Received : 02 September Accepted : 27 November Published : 12 February Issue Date : 13 February Anyone you share the following link with will be able to read this content:.

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Authors: C. Bradley , J. Randall , M. Abobeih , R. Berrevoets , M. Degen , M. Bakker , M. Markham , D. Twitchen , T. Download a PDF of the paper titled A qubit solid-state spin register with quantum memory up to one minute, by C.

Bradley and 8 other authors. Subjects: Quantum Physics quant-ph ; Mesoscale and Nanoscale Physics cond-mat. mes-hall Cite as: arXiv Focus to learn more DOI s linking to related resources.

Submission history From: Conor Bradley [ view email ] [v1] Mon, 6 May UTC 8, KB [v2] Thu, 9 May UTC 8, KB. Full-text links: Access Paper: Download a PDF of the paper titled A qubit solid-state spin register with quantum memory up to one minute, by C.

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Our experiments demonstrate a fully functional hybrid spin register. We have combined optimal-control-based error avoidance with error Detailed product information can be found using SPIN, Partial Product/Trustee Name. Click on the results to see more information about the specific product The generation of a register of highly coherent, but independent, qubits is a prerequisite to performing universal quantum computation

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What is Quantum Mechanical Spin?

Spin register - Post completion SPIN for paediatricians on the GMC specialist register - This is additional training or experience, which you complete Our experiments demonstrate a fully functional hybrid spin register. We have combined optimal-control-based error avoidance with error Detailed product information can be found using SPIN, Partial Product/Trustee Name. Click on the results to see more information about the specific product The generation of a register of highly coherent, but independent, qubits is a prerequisite to performing universal quantum computation

Recent experiments have demonstrated long coherence times, high-fidelity operations, and long-range entanglement. However, control has so far been limited to a few qubits, with entangled states of three spins demonstrated.

Realizing larger multiqubit registers is challenging due to the need for quantum gates that avoid cross talk and protect the coherence of the complete register. In this paper, we present novel decoherence-protected gates that combine dynamical decoupling of an electron spin with selective phase-controlled driving of nuclear spins.

We use these gates to realize a ten-qubit quantum register consisting of the electron spin of a nitrogen-vacancy center and nine nuclear spins in diamond. We show that the register is fully connected by generating entanglement between all 45 possible qubit pairs and realize genuine multipartite entangled states with up to seven qubits.

Finally, we investigate the register as a multiqubit memory. We demonstrate the protection of an arbitrary single-qubit state for over 75 s—the longest reported for a single solid-state qubit—and show that two-qubit entanglement can be preserved for over 10 s.

Our results enable the control of large quantum registers with long coherence times and therefore open the door to advanced quantum algorithms and quantum networks with solid-state spin qubits.

Published by the American Physical Society under the terms of the Creative Commons Attribution 4. A ten-qubit system based on spins in impure diamond achieves coherence times of over a minute.

Abobeih 1,2 , R. Berrevoets 1,2 , M. Degen 1,2 , M. Bakker 1,2 , M. Markham 3 , D. Twitchen 3 , and T. Box , GA Delft, Netherlands 2 Kavli Institute of Nanoscience Delft, Delft University of Technology, P. Box , GA Delft, Netherlands 3 Element Six, Fermi Avenue, Harwell Oxford, Didcot, Oxfordshire, OX11 0QR, United Kingdom.

The computational power of quantum networks is expected to far exceed that of classical technologies. Among the most promising quantum bits qubits for such networks are the spins of individual particles in solids, such as electrons and nuclei. Elementary control of such qubits and links within quantum networks have been demonstrated, but the largest entangled quantum states reported to date have contained just three spins.

Larger quantum registers are essential to realizing advanced computational power. However, controlling individual spins within complex and strongly interacting spin systems is a significant challenge.

In this study, we demonstrate a fully controllable ten-qubit register. Working at 3. We show that the system is fully connected by generating entangled states between all 45 possible spin pairs, and we prepare genuine seven-spin entanglement.

The spins that we study are excellent quantum memories that can store quantum states for up to one minute, the longest coherence time reported for solid-state spin qubits. We expect that our methods can also be applied to other spin platforms in diamond, silicon, and silicon carbide.

Our findings pave the way for advanced quantum algorithms and large multiqubit quantum networks based on tens of solid-state spin qubits. Illustration of the ten-qubit register developed in this work.

The electron spin of a single NV center in diamond acts as a central qubit and is connected by two-qubit gates to the intrinsic N 14 nuclear spin and a further eight C 13 nuclear spins surrounding the NV center.

a Illustration of the pulse sequence employed to realize a DDrf gate. Dynamical decoupling pulses on the electron spin purple are interleaved with rf pulses yellow , which selectively drive a single nuclear spin.

b Illustration showing that the initial state of the electron spin determines which rf pulses are resonant with the nuclear spin. The phase of each rf pulse is adapted to create the desired nuclear spin evolution, accounting for periods of free precession according to Eq.

The final state vectors are antiparallel along the equator; therefore, the gate is a maximally entangling two-qubit gate.

d Top-down view of c. a Nuclear spin spectroscopy. The electron spin is then measured along a basis in the equatorial plane defined by angle φ see inset. By fitting the amplitude, we distinguish such deterministic phase shifts from loss of coherence due to entangling interactions. The signals due to interaction with the eight C 13 spins used in this work are labeled.

The dashed gray line indicates the C 13 Larmor frequency ω L. A detailed analysis of the spectrum is given in the Supplemental Material [ 53 ]. b , c Example phase sweeps for two data points highlighted in red b and orange c in a.

Solid lines are fits to f φ. a Experimental sequence to prepare an electron-nuclear Bell state and determine the expectation value of the two-qubit operator Z X. A series of single- and two-qubit gates are used to initialize the nuclear spin [ 16, 37 ].

A measurement of the electron spin in the Z basis is followed by an X -basis measurement of the nuclear spin through the electron spin. These measurements are separated by a nuclear spin echo, which is implemented to mitigate dephasing of the nuclear spin.

The entire sequence is applied with and without an additional electron π pulse dashed box before the first electron readout in order to reconstruct the electron state while ensuring that the measurement does not disturb the nuclear spin state [ 16, 42 ].

b Density matrix of the electron-nuclear state after applying the sequence shown in a to qubit C1, reconstructed with state tomography. We correct for infidelities in the readout sequence characterized in separate measurements [ 53 ].

We use error function pulse envelopes with a 7. a Experimental sequence for the preparation of a nuclear-nuclear Bell state and measurement of the two-qubit operator Z Z.

Measurement of the two-qubit correlations between the nuclear spins is then performed through the electron spin. Spin echoes dashed boxes built into the measurement sequence protect the nuclear spins from dephasing errors. Blue purple bars show the experimental ideal expectation values for each operator.

The nuclear-nuclear correlations are well preserved after a nondestructive measurement of the electron spin in the X basis. Measured Bell state fidelities for all pairs of qubits in the ten-qubit register.

Genuine entanglement is confirmed in all cases, as witnessed by a fidelity exceeding 0. Qubits C1, C7, C8, and N 14 are controlled using DDrf gates Sec. Qubits C2, C3, C4, C5, and C6 are controlled using the methods described in Taminiau et al. The measurement sequence is broken down into basis rotations BR 1,2 , an electron readout RO , nuclear spin echoes echo 1,2 , and a multiqubit readout of the nuclear spins.

All operations are applied sequentially in the same way as shown in Fig. b , c Bar plots showing the measured expectation values nonzero terms of the ideal state only after preparing the five-spin b and seven-spin c GHZ states. The colors indicate the number of qubits involved, i.

Gray bars show the ideal expectation values. Quantum Physics. Authors: C. Bradley , J. Randall , M. Abobeih , R. Berrevoets , M. Degen , M. Bakker , M.

Markham , D. Twitchen , T. Download a PDF of the paper titled A qubit solid-state spin register with quantum memory up to one minute, by C.

Bradley and 8 other authors. Subjects: Quantum Physics quant-ph ; Mesoscale and Nanoscale Physics cond-mat. mes-hall Cite as: arXiv Focus to learn more DOI s linking to related resources.

Submission history From: Conor Bradley [ view email ] [v1] Mon, 6 May UTC 8, KB [v2] Thu, 9 May UTC 8, KB. Full-text links: Access Paper: Download a PDF of the paper titled A qubit solid-state spin register with quantum memory up to one minute, by C. view license. new recent Change to browse by: cond-mat cond-mat.

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The electron spin of registsr single NV cbtf in diamond acts as spin register regisetr qubit spin register is connected by two-qubit spin register to regiser intrinsic N spin register nuclear spin and a spin register eight Genie casino 13 nuclear spins surrounding the NV center. In particular, we trap individual 87 Sr atoms in an array of optical tweezers, prepare a uniformly filled register of spin-polarized atoms, then individually manipulate, and read out the spin state of the qubits. Jamali, P. CORE Recommender What is CORE? Retrospective experience is not accepted to count towards post completion SPIN modules in diabetes and applications must be prospective. REGISTER FOR SPIN. Download a PDF of the paper titled A qubit solid-state spin register with quantum memory up to one minute, by C. We use these gates to realize a ten-qubit quantum register consisting of the electron spin of a nitrogen-vacancy center and nine nuclear spins in diamond. Copy to clipboard. a Experimental sequence to prepare an electron-nuclear Bell state and determine the expectation value of the two-qubit operator Z X. Abstract Error correction is important in classical and quantum computation. Our experiments demonstrate a fully functional hybrid spin register. We have combined optimal-control-based error avoidance with error Detailed product information can be found using SPIN, Partial Product/Trustee Name. Click on the results to see more information about the specific product The generation of a register of highly coherent, but independent, qubits is a prerequisite to performing universal quantum computation Product registration is vitally important to record your ownership of this product. By trusting us with your contact data, you will greatly assist us in SPIN is a database on the use of Substances in Products in the Nordic Countries. It is a public accessible database, which can be used free of charge. You can Published 11 September A ten-qubit system based on spins in impure diamond achieves coherence times of over a minute. See more Register for an account where you will be able to customise your profile and set up job alert preferences Any player can be registered by completing the on-line registration form and paying on-line. Nations will be automatically notified of all player registrations Post completion SPIN for paediatricians on the GMC specialist register - This is additional training or experience, which you complete spin register
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Spin register - Post completion SPIN for paediatricians on the GMC specialist register - This is additional training or experience, which you complete Our experiments demonstrate a fully functional hybrid spin register. We have combined optimal-control-based error avoidance with error Detailed product information can be found using SPIN, Partial Product/Trustee Name. Click on the results to see more information about the specific product The generation of a register of highly coherent, but independent, qubits is a prerequisite to performing universal quantum computation

We correct for infidelities in the readout sequence characterized in separate measurements [ 53 ]. We use error function pulse envelopes with a 7. a Experimental sequence for the preparation of a nuclear-nuclear Bell state and measurement of the two-qubit operator Z Z.

Measurement of the two-qubit correlations between the nuclear spins is then performed through the electron spin. Spin echoes dashed boxes built into the measurement sequence protect the nuclear spins from dephasing errors. Blue purple bars show the experimental ideal expectation values for each operator.

The nuclear-nuclear correlations are well preserved after a nondestructive measurement of the electron spin in the X basis. Measured Bell state fidelities for all pairs of qubits in the ten-qubit register.

Genuine entanglement is confirmed in all cases, as witnessed by a fidelity exceeding 0. Qubits C1, C7, C8, and N 14 are controlled using DDrf gates Sec.

Qubits C2, C3, C4, C5, and C6 are controlled using the methods described in Taminiau et al. The measurement sequence is broken down into basis rotations BR 1,2 , an electron readout RO , nuclear spin echoes echo 1,2 , and a multiqubit readout of the nuclear spins.

All operations are applied sequentially in the same way as shown in Fig. b , c Bar plots showing the measured expectation values nonzero terms of the ideal state only after preparing the five-spin b and seven-spin c GHZ states. The colors indicate the number of qubits involved, i.

Gray bars show the ideal expectation values. See the Supplemental Material [ 53 ] for the operator corresponding to each bar. The fidelity with the target state is 0. d Plot of GHZ state fidelity against the number of constituent qubits.

A value above 0. The blue points are the measured data, while the green points are theoretical predictions assuming a simple depolarizing noise model whose parameters are extracted from single- and two-qubit experiments.

Numerical values are given in the Supplemental Material [ 53 ]. a Dynamical decoupling for spin C5. B , T , and n are fit parameters which account for the decay of the fidelity due to interactions with the nuclear spin bath, external noise, and pulse errors.

b Dynamical decoupling of the N 14 spin. Solid lines are fits to f t , but with A as a free parameter to account for the observed decrease in the Z Z correlations at large pulse numbers, likely due to pulse errors.

With decoupling pulses, genuine two-qubit entanglement is witnessed at times up to In addition, interpolation of the fit yields For pair 1, the fitted decay times T are 0.

For pair 2, the equivalent values are 0. It is not necessary to obtain permission to reuse this article or its components as it is available under the terms of the Creative Commons Attribution 4. This license permits unrestricted use, distribution, and reproduction in any medium, provided attribution to the author s and the published article's title, journal citation, and DOI are maintained.

Please note that some figures may have been included with permission from other third parties. It is your responsibility to obtain the proper permission from the rights holder directly for these figures. Physical Review X Highlights Recent Subjects Accepted Collections Authors Referees Search Press About Editorial Team.

Featured in Physics Open Access. A Ten-Qubit Solid-State Spin Register with Quantum Memory up to One Minute C. Bradley, J. Randall, M. Abobeih, R. Berrevoets, M. Degen, M. Bakker, M. Markham, D. Twitchen, and T. Please input your request in additional information of Step 2.

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