Quantum Computing in the UK Today Dr Rupesh Srivastava, User Engagement May 2021
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Quantum Computing in the UK today Dr Rupesh Srivastava, User Engagement May 2021 For BCS Berkshire For BCS Berkshire Members What we’ll cover 1. What is Quantum Computing and why the excitement? 2. The status and outlook for Quantum Computing & Simulation 3. The UK QT Programme 4. How to engage with Quantum Computing Question: When will Quantum Computing make an impact? For BCS Berkshire Members “Quantum information is a radical departure in information technology, more fundamentally different from current technology than the digital computer is from the abacus.” W. D. Phillips Nobel Laureate 1997 Saunpan Abacus Modern Laptop Computer A recent history of science and computation For BCS Berkshire Members 19th 20th 21st Quantum 2.0 ENIAC Babbage Difference Engine Colossus at Bletchley Park Summit Supercomputer QCS Hub Research For BCS Berkshire Members Classical Physics influences the design of the latest chips Some components may use quantum principles in their operation – but the chip does not use quantum for computation 32-core AMD Epyc (2017) 19,200,000,000 transistors (14 nm) BREAKING NEWS 2021 For BCS Berkshire Members Why build a quantum computer? The first question is, What kind of computer are we going to use to simulate physics? But the physical world is quantum mechanical, and therefore the proper problem is the simulation of quantum physics. Can you do it with a new kind of computer, a Richard Feynman quantum computer? Nobel laureate … It’s not a Turing machine, but a machine of a different kind. For BCS Berkshire Members Why build a quantum computer? Opportunity New era of discoveries Motivation Moore’s Law can’t continue forever Timing Because now we can!* * 40 years later For BCS Berkshire Members Timing – is key Theory Experiment You need a happy confluence of theory, experiment and engineering Engineering For BCS Berkshire Members Timing – what about now? Theory Experiment It’s just possible to engineer a quantum computer Engineering For BCS Berkshire Members Quantum Computing and Qubits Use and manipulate phenomena of quantum physics • Superposition: • Qubits being in multiple states at the same time, e.g. ‘0’ and ‘1’ • Entanglement: • Grouped behaviour of multiple ‘qubits’ • Interference • Utilising wave properties to amplify the “right” answers and (Source: Blackett Review, 2017) cancel out the “wrong” ones For BCS Berkshire Members Quantum Computing and Qubits In order to simulate N qubits requires 2N classical bits N 2N Comment 3 8 easy! 6 20 ~1x10 laptop 15 50 ~1x10 supercomputer 90 (Source: Blackett Review, 2017) 300 ~2x10 > atoms in known universe For BCS Berkshire Members Illustrating superposition with light A ‘photon’ is a particle of light 1 0 Which path? Quantum physics says that even a single photon can pass through both slits A single photon encodes a “qubit” – a superposition of “0” + “1” For BCS Berkshire Members Why the excitement? • A Quantum Computer’s power doubles with every qubit added • Speedups beyond the capability of future digital computing • Able to solve ‘hard problems’ • Able to mimic real world quantum systems • Expected high impact on most industry sectors, national economies, national security and research and discovery • Estimated impact, $450-800bn operating income/yr* *(Source: Where will Quantum Computer Create Value – And When?, BCG, 2019) Source: The Business Potential of Quantum Computing, BCG @ Q2B, Dec 2019 For BCS Berkshire Members A variety of application areas… starting with M • Medicine • Machine Learning • Materials • Mobility • Molecules • Manufacturing • Modelling & Simulation • Mass Communication • Money Markets • Mysteries of the universe For BCS Berkshire Members Application areas (cont’) (Source: The Business Potential of Quantum Computing, BCG, 2019) For BCS Berkshire Members A variety of ways to build quantum computers Superconducting Solid Cold Nano Ion-traps Photonics circuits state atoms wires Oxford Quantum Oxford Ionics Duality Photonics Quantum Motions Cold Quanta Microsoft Circuits Universal Quantum ORCA Computing Intel Atom Computing IBM IonQ PsiQuantum Quantum Brilliance Pasqal Google Atos Xanadu Rigetti Honeywell QuiX Intel Alibaba MATERIALS IN SUPERCONDUCTING QUANTUM BITS box (a charge qubit) by Nakamura and co-workers 8 9 MATERIALS IN SUPERCONDUCTINGin 1999. In QUANTUM 2002, Vion BITS et al. developed the Trapped-ion qubitsTrapped for -quantumion qubits for computing quantum computingquantronium qubit (a modifi ed charge qubit) with a T2 coherence time of hundreds of nanoseconds David Lucas, NQIT OxfordFor BCS Berkshire Members David Lucas, NQIT Oxford based on the concept of design and operation Quantum computing: some qubit technologies at fi rst-order noise-insensitive bias points. Example ion traps: box (a charge qubit)Burkard by Nakamura et al. and 1 0 co-workerselucidated the importance Example ion traps: 1mm in 1999. 8 In 2002,of Vion symmetry et al. 9 indeveloped qubit designs, the which in con- Superconducting Superconducting1mmIons circuits Diamond quantronium qubit (ajunction modifi ed with charge Bertet qubit) et al. with brought persistent- current fl ux qubit coherence times into the a T2 coherence time of hundreds of nanoseconds 1 1 IBM based on the conceptfew ofmicroseconds design and operation range. In 2005–2006, 12 13 at fi rst-order noise-insensitiveIthier et al. and bias Yoshihara points. et al. extensively measured the noise properties of quantro- Burkard et al. 1 0 elucidated the importance 5mm Microfabricated surface traps with nium and fl ux qubits, respectively, to better integrated microwaveof circuitry symmetry in qubit designs, which in con- Superconducting circuitsMacroscopicMacroscopic ion trap understand the sources of decoherence. The Oxford junction with Bertet et al. brought persistent- 5mm “blade”Microfabricated trap surface traps with ~1 cm“transmon” qubit developed by Schoelkopf integrated microwave circuitry current fl ux qubitand coherence co-workers times signifi into cantlythe reduced the IBM Macroscopic ion trap Key features: few microseconds range. 1 1 In 2005–2006, • Electric circuits made from charge sensitivity+ of the Cooper pair box • room temperature operations Ithier et al. 12 and Yoshiharasingle Ca etion al. 13 extensively superconducting materials• high -vacuum 9-qubit “memory register” by adding a shunt interdigitated capacitor, • 10μm – 100μm feature sizes measured the noisewhich properties would later of quantro-bring microsecond times • Fabricated using semiconductor Key features: • optical (laser) and electronic control nium and fl ux qubits,to the respectively, cavity-QED (quantumto better electrodynamic) industry cleanroom techniques + • room temperature operations understandsingle the Ca sourcesionarchitecture. of decoherence. 14 , 15 An MIT/NEC The group increased Oxford • high-vacuum 9-qubit “memory register” “transmon” qubit Tdeveloped above 20 µby s withSchoelkopf a persistent-current fl ux • Operated at very low Microfabricatedtemperature 9 qubit 2 • 10μm – 100μm feature sizes and co-workers qubitsignifi incantly a 2D reduced geometry the using dynamical to make them quantum “chip” trap “memory register” • Electric circuits made• optical from (laser) and electronic control charge sensitivitydecoupling of the Cooper sequences, pair 1 6box and the 3D-cavity superconducting •materialsControlled using microwaves by adding a shuntapproach interdigitated developed capacitor, at Yale 1 7 and now used Oliver & Welander ~ 2 nm Figure 1. Superconducting qubits and their coherence. (a) The three fundamentalwhich would laterby bring several microsecond groups has timesfurther increased this • Fabricated using •semiconductorIn ~20 years of development, MRS Bulletin 2013 coherencesuperconducting has improved qubit modalities: >1000x charge, f ux, and phase. Each includes oneto theor more cavity-QED time (quantum to around electrodynamic) 100 µ s. 1 8 More recently, improve- industry cleanroom techniquesJosephson junctions (shown in red). Illustration by Corey Reed, adapted from Reference 3. architecture. 14 , 15 Anments MIT/NEC in substrate group increasedpreparation and materials (b) The Josephson junction acts as both an inductor, L J , and capacitor, CJ . External inductors Superconducting Circuits for Quantum Computing — Peter Leek choices, addressing issues elucidated by the 3D • Operated at very low temperatureand capacitors, Lext and Cext , can be added to modify the qubit’s potentialT 2energy above 20 µ s with a persistent-current fl ux to make them quantumlandscape and reduce sensitivity to noise. (c) Because the Josephson junctionqubit inductance in a 2D geometrygeometries, using have dynamicalled to improved coherence is nonlinear, the qubit potential is anharmonic. The qubit comprises the two-lowest states 1 9 , 2 0 of 2D 1 6 geometries. T h i s fi ve-orders-of- and is addressed at a unique frequency, f01 . (d) 15 years of progress in qubit coherdecouplingence times, sequences, and the 3D-cavity • Controlled using microwavesreminiscent of Moore’s Law for semiconductor electronics. On average, the doublingapproach rate for developed magnitude at Yale improvement 1 7 and now used in the primary single- coherence times in superconducting qubitsOliver is about & Welanderonce per year. Improvements have been qubit metric can be justly termed a “Moore’s • In ~20 Figure years 1. Superconducting of development,driven qubits by both and new their device coherence. designs (a)and The materials three fundamentaladvances. Qubit modalitiesby represented several groups has further increased this MRS