All - Your SPIN supervisor should then monitor your capability acquisition through ePortfolio and regular one-to-one meetings. Your SPIN Supervisor s must either be a General Paediatrician with an interest in the area relevant to your SPIN or a sub-specialist consultant in that area.

For anyone applying for the Cardiology SPIN, this must be a Paediatric Cardiologist. Evidence can be collected over a period of five years until the point at which your completed SPIN is submitted for the CSAC to sign off.

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You must undertake at least 12 months of your SPIN module prospectively. Retrospective experience is not accepted to count towards post completion SPIN modules in diabetes and applications must be prospective. Once you complete your SPIN module and link your evidence via your ePortfolio, you will be able to complete the SPIN completion report and send to your SPIN supervisor.

You only have 12 months from the end of your SPIN completion to be eligible to receive a certificate for SPIN completion in line with rules on CCT certification. If you are completing your SPIN post-CCT, and have exceeded the 5 year limit which we expect most SPINs to take to completion, please conduct a mid-point review with your supervisor to help you target your efforts and attain all capabilities.

Please inform training. uk if this applies to you. You will then be issued with a SPIN Module Certificate. There can be delays in reviewing SPIN completion applications due to high applicant numbers and CSAC availability.

We would advise that May and November are the most available times for CSACs to review evidence and sign off on completions. The competency frameworks apply to SPIN modules that are being revised and serve as an indicator of requirements. The new SPIN modules are all aligned to the RCPCH Progress curriculum style of learning outcomes and key capabilities.

Special Interest SPIN module application guidance. Save as PDF. As an ST4 paediatric trainee or above or post completion paediatrician, you may wish to apply for a SPIN module. This comprises additional training and experience in a clinical area. We have recently updated some of our SPIN modules, and have new SPIN modules in child mental health, audiovestibular medicine and oncology.

Applications for SPIN are currently closed. Last modified. Post date. Table of contents. About SPIN Types of SPIN List of SPIN modules Applying for SPIN and about the training Step 1 - Submit your application Step 2 - Evidence your SPIN Step 3 — Complete your SPIN Downloads.

About SPIN All SPIN modules are designed to enable a paediatrician to lead in that area as part of meeting a service need. The SPIN process is currently under review. Types of SPIN These are the types of SPIN offered by RCPCH: Progress training pathway: SPIN in training for Level 3 trainees - This is additional training and experience in a clinical area, which you complete in 12 to 18 months of clinical time.

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uk Step 1 - Submit your application All candidates complete the application form on RCPCH ePortfolio. The distance learning module 6 by BPNA is optional, as are PET2 and PET3. the RCPCH SPIN in Epilepsy can be completed without courses.

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Diabetes only Retrospective experience is not accepted to count towards post completion SPIN modules in diabetes and applications must be prospective. Step 3 — Complete your SPIN Once you complete your SPIN module and link your evidence via your ePortfolio, you will be able to complete the SPIN completion report and send to your SPIN supervisor.

How long will it take for my evidence to be reviewed? Competency frameworks and Progress aligned SPINs The competency frameworks apply to SPIN modules that are being revised and serve as an indicator of requirements. Adolescent health SPIN v2 Allergy SPIN v2 Allergy SPIN Training guide pre-CCT 3.

Audiovestibular SPIN v1 Cardiology SPIN v2 Child mental health SPIN v1 Dermatology SPIN v2 Diabetes SPIN v2 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. 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.

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

The World Squash Federation today launches a new worldwide player registration service that will require players competing internationally Post completion SPIN for paediatricians on the GMC specialist register - This is additional training or experience, which you complete The generation of a register of highly coherent, but independent, qubits is a prerequisite to performing universal quantum computation: Spin register

Spkn in general paediatrics will enter the GMC pragmatic play slots register with paediatrics when signed march madness odds for training by regoster Nightrush bonus code panels and RCPCH spin register for training and quality. Spin register Data Figure 1 Hyperfine spectrum as dpin in the main text. The beams are detuned from the 3 P 1 manifold of states in order to drive two-photon Raman transitions between the nuclear-spin ground states. Du Max Planck Institute for Solid State Research, Heisenbergstraße 1, Stuttgart, GermanyJ. Page updated. Blue purple bars show the experimental ideal expectation values for each operator. A new reference 31 has been added to the main-text reference list and all subsequent references have been renumbered.	Sub-Poissonian loading of single atoms in a microscopic dipole trap. Kim, D. However, we adhere to GMC curricula principles in new SPINs revised with learning outcomes and key capabilities. The dashed gray line indicates the C 13 Larmor frequency ω L. 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	The generation of a register of highly coherent, but independent, qubits is a prerequisite to performing universal quantum computation Post completion SPIN for paediatricians on the GMC specialist register - This is additional training or experience, which you complete Detailed product information can be found using SPIN, Partial Product/Trustee Name. Click on the results to see more information about the specific product	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
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Wrachtrup Spin register of Nightrush bonus code, Technical University of Spin register, Garching, Spin register, T. Comments By regiater a comment you agree to abide by our Terms and Community Guidelines. Note again that all seven qubits in a single column were driven simultaneously in this experiment. Endres, M. Kondov, Krish Kotru, Stuart C.	Second, loading into optical tweezers is less efficient at lower trap depth. Norcia, M. You are using a browser version with limited support for CSS. Claiming and redeeming the offer Each ticket includes 10 spins on the Spin of the Day Prize Wheel. Qubits C1, C7, C8, and N 14 are controlled using DDrf gates Sec. Accepted : 27 November Rheumatology SPIN framework of competency MS Word	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	Create a free Spin Rewriter account to take advantage of the world's most popular text paraphrasing tool. Intelligent content rewriting technology awaits The World Squash Federation today launches a new worldwide player registration service that will require players competing internationally The Unique Superannuation Identifier (USI) is used in SuperStream to uniquely identify an APRA fund and/or its superannuation product which an employee (member)	Registration fee includes welcome party (on Sept. 24 evening), coffee break, lunch box, conference excursion (on Sept. 28) but does not include Banquet (on Sept 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 Title:A qubit solid-state spin register with quantum memory up to one minute Abstract:Spins associated to single defects in solids provide

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

Ramsey, N. A molecular beam resonance method with separated oscillating fields. Boyd, M. High Precision Spectroscopy of Strontium in an Optical Lattice: Towards a New Standard for Frequency and Time. PhD thesis, Univ. of Colorado Takamoto, M. Improved frequency measurement of a one-dimensional optical lattice clock with a spin-polarized fermionic 87sr isotope.

Kim, H. Gerchberg-Saxton algorithm for fast and efficient atom rearrangement in optical tweezer traps. Express 27 , — Enhanced atom-by-atom assembly of arbitrary tweezer arrays. A , Maciejewski, F. Mitigation of readout noise in near-term quantum devices by classical post-processing based on detector tomography.

Quantum 4 , Article Google Scholar. Schine, N. Long-lived Bell states in an array of optical clock qubits. Entangling, Controlling, and Detecting Individual Strontium Atoms in Optical Tweezer Arrays. PhD thesis, California Institute of Technology Download references.

The authors would like to thank Sabrina Hong, Alexander Papageorge, Maxwell Parsons, Colm Ryan, and Prasahnt Sivarajah for their contributions during the initial design and buildout of the optical systems, control hardware, and software infrastructure used in this work.

We would also like to thank Jun Ye and Alexey Gorshkov for multiple discussions during the planning stages of this work. This work was partially supported under NSF SBIR Grant Katrina Barnes, Peter Battaglino, Benjamin J.

Bloom, Kayleigh Cassella, Robin Coxe, Nicole Crisosto, Jonathan P. King, Stanimir S. Kondov, Krish Kotru, Stuart C. Larsen, Joseph Lauigan, Brian J. Lester, Mickey McDonald, Eli Megidish, Sandeep Narayanaswami, Ciro Nishiguchi, Remy Notermans, Lucas S.

You can also search for this author in PubMed Google Scholar. performed the foundational design of the Phoenix system. contributed to the design, construction, and operation of Phoenix, as well as making measurements.

built custom RF hardware for rearrangement and clock manipulations. created the gate language and software infrastructure for Phoenix. wrote and assembled the manuscript, M.

created diagrams and figures, and K. K performed data analysis. all reviewed the manuscript. Correspondence to Benjamin J. Bloom , Krish Kotru or Mickey McDonald.

and J. are co-founders of, and equity shareholders in, Atom Computing, Inc. All other authors are employees of, and equity shareholders in, Atom Computing, Inc. Nature Communications thanks the other anonymous reviewer s for their contribution to the peer review of this work.

Peer reviewer reports are available. Open Access This article is licensed under a Creative Commons Attribution 4. Reprints and permissions. Barnes, K. Assembly and coherent control of a register of nuclear spin qubits. Nat Commun 13 , Download citation. Received : 14 February Accepted : 08 April Published : 19 May Anyone you share the following link with will be able to read this content:.

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Skip to main content Thank you for visiting nature. nature nature communications articles article. Download PDF. Subjects Atomic and molecular interactions with photons Qubits. Abstract The generation of a register of highly coherent, but independent, qubits is a prerequisite to performing universal quantum computation.

Introduction The proposed use of nuclear spins to encode and store quantum information has a long history owing to their isolation from undesired interactions with the environment 1 , 2.

Results Our array of optical tweezer trapping potentials is generated holographically, as shown in Fig. Full size image. Discussion Future work is underway to optimize the operational parameters of this system, as well as to explore methods to mitigate undesired scattering that currently limits the performance of our system.

Methods Atom loading, cooling, state preparation, and measurement The process of initializing the qubit starts with producing a strontium atomic beam in an ultra-high vacuum UHV system. Trap array generation and flattening The tweezer traps are produced at the focal plane of a custom high-NA 0.

Rearrangement Rearrangement is performed using a single focused beam derived from the same Ti:Sapphire laser source used to create the static computing traps.

Data availability The processed data used to create all figures in this article are included in Supplementary Data files. Code availability No custom code was used that is central to the conclusions of the manuscript.

References DiVincenzo, D. Article ADS MathSciNet CAS Google Scholar Kane, B. Article ADS CAS Google Scholar Cory, D. Article ADS CAS Google Scholar Gershenfeld, N. Article MathSciNet CAS Google Scholar Maurer, P. Article ADS CAS Google Scholar Hensen, B. Article ADS CAS Google Scholar Park, J.

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Article ADS CAS Google Scholar Ramsey, N. Article ADS CAS Google Scholar Boyd, M. Article ADS Google Scholar Kim, H.

Article ADS CAS Google Scholar Schymik, K. Article ADS CAS Google Scholar Maciejewski, F. Article Google Scholar Schine, N. Acknowledgements The authors would like to thank Sabrina Hong, Alexander Papageorge, Maxwell Parsons, Colm Ryan, and Prasahnt Sivarajah for their contributions during the initial design and buildout of the optical systems, control hardware, and software infrastructure used in this work.

Author information Authors and Affiliations Atom Computing, Inc. View author publications. Ethics declarations Competing interests B. Peer review Peer review information Nature Communications thanks the other anonymous reviewer s for their contribution to the peer review of this work.

Supplementary information. Description of Supplementary Data Files. Dataset 2. Dataset 1. Rights and permissions Open Access This article is licensed under a Creative Commons Attribution 4.

About this article. Cite this article Barnes, K. Copy to clipboard. This article is cited by Fast nuclear-spin gates and electrons-nuclei entanglement of neutral atoms in weak magnetic fields Xiao-Feng Shi Frontiers of Physics Frequency—angular resolving LiDAR using chip-scale acousto-optic beam steering Bingzhao Li Qixuan Lin Mo Li Nature Erasure conversion in a high-fidelity Rydberg quantum simulator Pascal Scholl Adam L.

Shaw Manuel Endres Nature High-fidelity gates and mid-circuit erasure conversion in an atomic qubit Shuo Ma Genyue Liu Jeff D. The system will enable national federations to enter their players for events online using their SPINs.

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