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Make it stand out Whatever it is, the way you tell your story online can make all the difference. https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1594824914512-RICS1MK3EA3SBVFOA6O6/synthesis.jpg Workshop Quantum Computer Systems: Research for Noisy Intermediate-Scale Quantum Computers, by Ding and Chong. https://www.epiqc.cs.uchicago.edu/education-overview daily 0.75 2021-11-30 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1516487974006-9803ZEOLJYX428CMWYJK/20131205_Core_1050.jpg Overview https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1516484051534-8KTN9ZZ79Q0T7CGWZZ6J/20150228_FEMMES-Camp_9730+%281%29.JPG Overview https://www.epiqc.cs.uchicago.edu/home daily 1.0 2022-11-10 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1516050943359-MOTJDWNURJ6YAYK81134/image-asset.jpeg EPiQC https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1523892735548-ISJZASIX4OON1FFJXETI/image-asset.jpeg EPiQC An NSF Expedition in Computing ENABLING PRACTICAL-SCALE QUANTUM COMPUTING https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1549431040057-GNC6J3FM0SJE11Z3JO5Q/Zines.png EPiQC EPiQC Zines Explain Quantum Computing Read More https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1527026917820-4EZ2BMCOE1ATVIW1UJHI/20180517-0000.jpg EPiQC Diana Franklin Testifies before Congress Read More https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1531268498946-D9EFD8TMXFPGI4M1HDW9/ISCA.2018.IMG_0245.jpg EPiQC Quantum Computing Tutorials Read More https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1585326729879-68AXFVPEPY1QIB8RC2VN/two_qubit_pauli_graph-web.png EPiQC - IBM Q Best Paper Award for VQE Research IBM Q Best Paper Award for VQE Research Read More https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1587047818072-RISINDG5SDMTFSNIWQ4P/students.soar.001.jpeg EPiQC - EPiQC Students Soar EPiQC Students Soar Read More https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1587414231062-7QWCBTX8TO7G7135MIT7/super.tech.logo.png EPiQC EPiQC-Related Startup acquired by ColdQuanta read more https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1622826332131-67B7L4GOAMV8LU96JB2G/vlq-fig8-1000.png EPiQC - Three EPIQC Papers Chosen by IEEE MICRO for Annual Top Picks Award Three EPIQC Papers Chosen by IEEE MICRO for Annual Top Picks Award Read More https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1625090457000-QU818J86B1OE84EF764D/smith-head.jpeg EPiQC EPiQC postdoc Kate Smith wins Kenneth C. Smith Early Career Award in Microelectronics Kate Smith received the Kenneth C. Smith Early Career Award in Microelectronics from the IEEE Computer Society, Technical Committee on Multiple-Valued Logic (IEEE TC MVL). read more https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1633969226333-XTZKFE8YQQMAFCDSLK5B/yongshan-ding-2020.jpg EPiQC EPiQC Alum Yongshan Ding Joins Yale Faculty Read More https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1634920013726-XRGOP59HCSUKVM4QTS91/CQE21.png EPiQC - EPiQC Research Receives Best Paper Award at IEEE Quantum Week EPiQC Research Receives Best Paper Award at IEEE Quantum Week Read More https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1646093856422-AU29MPVAFNAW4L84JQOA/SupermarQ_SSb-R00a_Mil-1024x440.jpg EPiQC - SupermarQ Super.tech/EPiQC Research Informs New Suite of Benchmarks for Quantum Computers - HPCA Best Paper Award Winner read more https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1646096104232-E73H3PRLAENH4L2LNJ83/sfq-graphic_900x600.png EPiQC - qce award 2021 In-Fridge Controller Could Scale Up Quantum Computers, Award-Winning EPiQC Research Finds read more https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1670511030922-VRFKD6D5YULSGHQUEO0R/Franklin_preferred_head.jpeg EPiQC - Franklin Distinguished Member ACM Franklin named a Distinguished Member by ACM read more https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1670600205232-2NCHEARG6SVMR2S8K0O2/Chong.5X0A0229-smaller-1024x683.jpg EPiQC - Chong IEEE Fellow Professor Fred Chong Named IEEE Fellow read more https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1516056430251-0FG44K1WX2U084WMM7DF/20170923_Drone_0075+%283%29.jpg EPiQC https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1516056481182-3N6H42K8BAFX4W6Y9ZY9/FHYMKH.jpg EPiQC https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1516056507525-KQFH1ULRD0G47VMZJ74K/KG56R9.jpg EPiQC https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1516036669526-QET7TY07BA28R7DP1AI6/20160603_UnCommonCoreChong_5071+%281%29.JPG EPiQC https://www.epiqc.cs.uchicago.edu/people daily 0.75 2026-03-17 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1515789011400-GBQ93KDBFPUBI55AO9FH/Chong-whiteboard2-small.jpg People Fred Chong, PI https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1631722231782-OO6AIJG7ILU55FOU7M6U/Dangwal.Siddharth.jpg People - Make it stand out Siddharth Dangwal https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/6bea208a-a2b1-4097-9857-3db7b61c2019/Kamen.Andrew.jpg People - Make it stand out Andrew Kamen https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/5d9a675e-e968-436a-bef4-3fe5e03297db/morrell2025.jpg People - Make it stand out Zachary Morrell https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1612882301674-57WRJHZEFLDLVE5CA8XC/Nottingham.Natalia.jpg People Natalia Nottingham https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/052ec36f-4f12-4869-b48d-d8681caaa9d7/TinaOberoi.jpeg People - Make it stand out Tina Oberoi https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/ebb97f23-7674-486a-9320-b8936842ec35/ArielleSanford.jpeg People - Make it stand out Arielle Sanford https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/51d58379-061e-4daa-bffa-029c6cc0b323/DhirpalShah.jpeg People - Make it stand out Dhirpal Shah https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/51200c13-cc4f-4be0-8a0a-3fbe93681879/DelaneySmith.jpeg People - Make it stand out Delaney Smith https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/0c5ef69f-c4f3-4b0d-8b19-f03583ef14b3/JamesSud.webp People - Make it stand out James Sud 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Yunong Shi, Quantum Research Scientist, Amazon Web Services (AWS) https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1631722440751-HCTWXCEHXEQ1I2W9G24U/Seifert.jpg People - Make it stand out Lennart Maximilian Seifert, UChicago https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1527681398776-QUZSLRKLSCMUF7Y84MS7/Wu.Xin-Chuan%28Ryan%29.jpg People Xin-Chuan (Ryan) Wu, Intel Research Quantum Group https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1543442507111-HLEVL6GH9E8MH0ASEQ08/image-asset.jpeg People Emma Dasgupta https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1579625765005-G75W35N69R93EZSPQ2UG/DeVoe.Maddie.JPG People Maddie DeVoe https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1527681414344-0IVQ9F1P9M9WKYFPTVGN/Fensterstock.Matthew.2.png People Matthew Fensterstock 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Computers https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1568127856168-QG3DOH1WR594AQX9CVM9/5.png Trapped Ion Quantum Computers https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1568127856139-T06TR4ED4PS8ZV010WWV/6.png Trapped Ion Quantum Computers https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1568127856257-RM1XJ67FGLG1ZLTEOKZH/7.png Trapped Ion Quantum Computers https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1568127856402-SWKATF5M1H7L8TSW3Y7L/8.png Trapped Ion Quantum Computers https://www.epiqc.cs.uchicago.edu/superconducting-qcs daily 0.75 2023-05-15 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1568127591441-K51S51RQAM7G4RCVNXGU/1.png Superconducting Quantum Computers https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1568127591367-2DHLME2R86LRX29KAGQ5/2.png Superconducting Quantum Computers 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https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1568899365028-2A3PLKLJYF1RU6ST3H0R/noun_presentation_65423.png ASTC2019 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1568411679865-998ZA8DHUI719PNW1DUB/QC.P1010659.jpg ASTC2019 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1568411195425-W850CSXUSFQNLDC7HK7S/DesignIO_ConnectedWorlds_08.jpg ASTC2019 - NYSci Connected Worlds https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1568657663607-4R440ZPHD34MOV629Q79/astro_con.png ASTC2019 https://www.epiqc.cs.uchicago.edu/activities daily 0.75 2021-09-09 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1631202184264-1JEY4HHFK1GX7F1WWYR0/Reversibility-Exploring.png QC Activity Registration https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1631202281147-H2EZU5YBOG88R3RQPWPQ/Measurement-JellyBeans.png QC Activity Registration 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https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1631204057838-NO6GFTQNB20EQKXHGMM4/Measurement-JellyBeans.png QC Activities for Informal Educators - Download Materials https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1631204096041-60ZGE7YI7KUSFALX1Y6L/ExponentialGrowth.png QC Activities for Informal Educators - Download Materials https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1631204129404-B4TVZN7YZT9JCFC0PPTA/PlinkoProbability.png QC Activities for Informal Educators - Download Materials - Make it stand out Whatever it is, the way you tell your story online can make all the difference. https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/6aa5b9c7-f8d8-48db-a34d-ddb42e1ef59c/Thaumatrope+COVER.png QC Activities for Informal Educators - Download Materials - Make it stand out Whatever it is, the way you tell your story online can make all the difference. https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/c7ba1d71-8ce2-4602-adfb-5f9fda70c85c/MorseCodeCover.png QC Activities for Informal Educators - Download Materials https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/6a1a6021-4d60-467e-a20e-cae52753746e/SuperpositionWithCardsCover.png QC Activities for Informal Educators - Download Materials - Make it stand out Whatever it is, the way you tell your story online can make all the difference. https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/a06b6214-32ff-44bb-bb93-462487beb430/CardTrickCOVER.png QC Activities for Informal Educators - Download Materials - Make it stand out Whatever it is, the way you tell your story online can make all the difference. https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/b781284b-dea0-4479-8580-189e85049cfe/QuantumGuessWhoCOVER.png QC Activities for Informal Educators - Download Materials - Make it stand out Whatever it is, the way you tell your story online can make all the difference. https://www.epiqc.cs.uchicago.edu/epiqc-videos daily 0.75 2019-09-17 https://www.epiqc.cs.uchicago.edu/optimized-magic-state-distillation-architectures daily 0.75 2019-12-02 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1572289854576-TVR2X4FT8OQ79HRWYMGZ/Holmes.block_pic.png Optimized Magic-State Distillation Architectures Depiction of the Bravyi-Haah magic state distillation protocol https://www.epiqc.cs.uchicago.edu/fault-tolerant-gkp-state-preparation daily 0.75 2019-10-21 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1571688093927-UTTATX162432OC8ISSC1/gkp.Shi..gif Fault-tolerant GKP state preparation Output State https://www.epiqc.cs.uchicago.edu/formal-constraint-based-compilation daily 0.75 2019-10-21 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1571689316207-6XIFUD982W5F0297XP6G/Formal+Constraint-based+Compilation.png Formal Constraint-based Compilation Overview of the compilation process. https://www.epiqc.cs.uchicago.edu/quantum-circuit-simulation-using-data-compression daily 0.75 2019-12-02 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1575305906706-WAWV4QT96JBCUHTYFWBO/sim_design.png Quantum Circuit Simulation Using Data Compression Simulation Overview https://www.epiqc.cs.uchicago.edu/partial-compilation daily 0.75 2020-01-14 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1579029557286-TP0KOW6XKA57ZRAI5W8Q/Gokhale.PartialCompilation.png Partial Compilation Representative variational circuit, decomposed into gates https://www.epiqc.cs.uchicago.edu/crosstalk-mitigation-in-software daily 0.75 2020-12-04 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1579626499143-DR6S5G642CZJHKT8ZH21/Murali.Crosstalk+Mitigation+in+Software.png Crosstalk Mitigation in Software Our Crosstalk Mitigation System https://www.epiqc.cs.uchicago.edu/leakage-with-subsystem-codes daily 0.75 2020-12-04 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1579707420726-9577IIR1QF531TUFDWS8/subsystemcode.jpg Leakage with Subsystem Codes Subsystem surface code used to handle leakage https://www.epiqc.cs.uchicago.edu/2d-compass-codes daily 0.75 2020-12-04 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1579705740490-4FMRLPL618TEVM644SCG/2dccdecoder.png 2D Compass Codes Decoder graph for an example compass code https://www.epiqc.cs.uchicago.edu/mixed-qubit-leakage-reduction daily 0.75 2020-12-04 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1579709442981-TXZ7E5O1V61GJNVNTKSD/mixedqubits.png Mixed Qubit Leakage Reduction Performance of surface codes for Zeeman qubits, hyperfine qubits, and a mixed approach https://www.epiqc.cs.uchicago.edu/lossy-compression-use-cases daily 0.75 2020-12-04 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1580401917542-FMRFR3E4Y2NKIN6Z4C48/Lossy.compression.HPC.jpg Lossy Compression Use Cases Comparison of rate–distortion based on different lossy compression strategies https://www.epiqc.cs.uchicago.edu/adaptive-quantum-simulated-annealing daily 0.75 2020-12-04 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1580835372797-2IZ73ZG6C2GXQV2DTW3R/Harrow.Q.Simulated.Annealing.png Adaptive Quantum Simulated Annealing https://www.epiqc.cs.uchicago.edu/pauli-exclusion-principle-verification daily 0.75 2020-12-04 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1581034120669-9ZP17C045GOM6D3B0T9A/Pauli.Exclusion.Schuster.png Pauli Exclusion Principle Verification Measured orbital occupations verify generalized Pauli principle. https://www.epiqc.cs.uchicago.edu/nisq-boosting-qc-power daily 0.75 2021-01-25 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1591112554095-ZV4S7JSVEB8TH6TTN8UV/NISQ%2B_Holmes.png NISQ+: Boosting QC Power Decoder Microarchitecture https://www.epiqc.cs.uchicago.edu/extended-frontier-with-qutrits daily 0.75 2021-08-10 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1628615844016-G57AJLFZRJ7P23FPAG1A/Logo-IEEE.jpg Extended Frontier with Qutrits - Top Pick https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1599246970206-PO3OJCTIME86TF6U1LB3/frontier.png Extended Frontier with Qutrits The frontier of a quantum computer is the line where every machine qubit is used as a data qubit. https://www.epiqc.cs.uchicago.edu/quantum-for-grid-security daily 0.75 2020-12-04 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1599247714453-GN1V9LD8E433UW6ON3PT/GridSecurityImage.png Quantum for Grid Security Upper bound on quantum advantage for grid contingency analysis https://www.epiqc.cs.uchicago.edu/compiling-to-modular-architectures daily 0.75 2020-12-04 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1599658166659-GWWHUR2FH8MRCJNOPUJR/circuit-partitioning.jpg Compiling to Modular Architectures Non-local communication overhead in circuits mapped to cluster-based machines. Our new mapping scheme FGP-rOEE (Fine Grained Partitioning, with relaxed Overall Extreme Exchange partitioner) provides reduces the number of operations added for non-local communication on benchmarks. https://www.epiqc.cs.uchicago.edu/openpulse-compilation daily 0.75 2021-01-27 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1606948289322-3WRRJ19MUT0S3ZBNP9IL/compilation_flow+%282%29.png OpenPulse Compilation Like classical programs, quantum programs undergo a compilation process from high-level programming language to assembly. However, unlike the classical setting, quantum hardware is controlled via analog pulses. In our work, we optimize the underlying pulse schedule by augmenting the set basis gates to match hardware. Our compiler automatically optimizes user code, which therefore remains hardware-agnostic. https://www.epiqc.cs.uchicago.edu/systematic-crosstalk-mitigation daily 0.75 2021-08-16 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1628615954811-V8UQ7XYCKRD5Z7H0IZOC/Logo-IEEE.jpg Systematic Crosstalk Mitigation - Top Pick honorable mention https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1607106459316-ODCA2KL8EO8Y2YISTIG4/sys.crosstalk.mitigation.png Systematic Crosstalk Mitigation Key benefit of our crosstalk mitigation methodology. Our software toolflow reduces crosstalk on tunable qubits via frequency-aware compilation and real-time calibration. As a result, our work achieves the same level protection against crosstalk, but on simpler hardware (tunable qubit, fixed-coupler). https://www.epiqc.cs.uchicago.edu/virtualized-logical-qubits daily 0.75 2021-08-09 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1628546973637-F805DVCD1NMPP18UUL8I/Logo-IEEE.jpg Virtualized Logical Qubits - TOP Pick https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1607108623449-7Z83915DZ0F74N3OQQLI/vlq-fig8-1000.png Virtualized Logical Qubits A 3D view of our virtual logical qubit Compact embedding. Shown at the top is the 2D grid of transmon qubits. Attached below every transmon is a resonant cavity memory. Compact surface code patches are shown stored, one in each mode. This deformed patch can be tiled in 2D. https://www.epiqc.cs.uchicago.edu/exploring-quantum-reversibility-with-young-learners daily 0.75 2021-01-27 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1608320183900-SH7OPBBN42WFUPJOZ3MY/reversibility.png Exploring Quantum Reversibility with Young Learners Everyday examples of reversibility to introduce the concept to young learners. https://www.epiqc.cs.uchicago.edu/on3-vqe daily 0.75 2021-01-27 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1609791691634-9PI4FEFDEOK88922XJJR/VQE_Paper_Image.jpg O(N^3) VQE Pictorial representation of the commutation on each index between two {a†a†aa} JW rectangles. All indices commute except possibly the eight indices with black bars—these indices anticommute when the black bar (X or Y) is vertically aligned with a blue rectangle Z. In this example, there are an even (4) number of anticommuting terms, so the two patterns commute. https://www.epiqc.cs.uchicago.edu/resource-efficient-quantum-computing-by-breaking-abstractions daily 0.75 2021-01-27 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1609795964464-U3YJ2PLM321MOTHCIGKZ/abstraction.jpg Resource-Efficient Quantum Computing by Breaking Abstractions Same abstractions in quantum computing stacks can be mapped to different physical implementations. https://www.epiqc.cs.uchicago.edu/gottesman-types-for-quantum-programs daily 0.75 2021-09-08 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1609794766989-FKPBKAWNER8585DKGCIO/Gottesman.types.png Gottesman Types for Quantum Programs Superdense coding circuit sending classical bits x and y from Alice to Bob and its program annotated with types at each step https://www.epiqc.cs.uchicago.edu/designing-reliable-qccd-systems daily 0.75 2021-09-29 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1609885280597-JO47TLLSZUU5Z8BGNFCC/Designing+Reliable+QCCD+Systems.png Designing Reliable QCCD Systems Superdense coding circuit sending classical bits x and y from Alice to Bob and its program annotated with types at each step https://www.epiqc.cs.uchicago.edu/architecting-nisq-systems daily 0.75 2021-08-09 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1628546599346-47N39TW1IX4K6D7AJ6HH/Logo-IEEE.jpg Architecting NISQ Systems - TOP PICK TOP PICK https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1609885939402-GYGHII8WQR47KU7KFIQQ/image-asset.png Architecting NISQ Systems QC systems considered in the study https://www.epiqc.cs.uchicago.edu/quantum-hoare-type-theory daily 0.75 2021-09-08 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1609887269906-O489QGBAOX67KRYTWGCL/quantum.hoare.theory.png Quantum Hoare Type Theory Superdense coding circuit sending classical bits x and y from Alice to Bob and its program annotated with types at each step https://www.epiqc.cs.uchicago.edu/extended-flag-gadgets daily 0.75 2021-01-27 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1611693183589-RI0LZCOIDD3D6BCUCOBZ/Capture.Debroy.PNG Extended Flag Gadgets Circuits demonstrating flags for multiple cases. In (a.) we show a general flag gadget for a general n-qubit unitary U. In (b.) we show that for a Clifford subcircuit (here shown surrounded by T-gates) this can be simplified to Pauli flags. In (c.) we show how Pauli flags can be used for a circuit with non-Clifford elements. Lastly in (d.) we show how multiple flags can be used to verify a single circuit. https://www.epiqc.cs.uchicago.edu/9-qubit-compass-codes daily 0.75 2021-01-27 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1611773942164-WZGI609NT2OEW5D3HE1P/Capture.9qubitCompas.PNG 9 Qubit Compass Codes Figures showing best performing codes and pseudothresholds for different error models and sets of codes. In (a,b,c) we are comparing codes in the set {Surface-17, Bacon-Shor-13, Shor-6X2Z, Shor-6Z2X}, while in (d,e,f) we restrict our set to only consider codes with a transversal Hadamard gate, {Surface-17, Bacon-Shor-13}. In (a,d) we look at the intersection of overrotation error (parameterized by the two qubit gate error) and T2 dephasing, in (b,e) we look at overrotation and crosstalk, and in (c,f) we look at T2 dephasing and crosstalk with a background overrotation characterized by a Mølmer-Sørensen error rate of 10−4 . The colored regions indicate which code is optimal at those error parameters, with darker shading implying the code is outperforming a physical CNOT. The colored curves are the pseudothreshold curves for which the logical error rate is equal to the physical error rate in Eq. 5 and the black curves are borders between regions in which different codes are preferred. https://www.epiqc.cs.uchicago.edu/union-find-toric-code daily 0.75 2021-01-28 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1611861897751-G8GE646JMJSIMMLDRUDW/medium.Huang.png union-find toric code Figures showing best performing codes and pseudothresholds for different error models and sets of codes. In (a,b,c) we are comparing codes in the set {Surface-17, Bacon-Shor-13, Shor-6X2Z, Shor-6Z2X}, while in (d,e,f) we restrict our set to only consider codes with a transversal Hadamard gate, {Surface-17, Bacon-Shor-13}. In (a,d) we look at the intersection of overrotation error (parameterized by the two qubit gate error) and T2 dephasing, in (b,e) we look at overrotation and crosstalk, and in (c,f) we look at T2 dephasing and crosstalk with a background overrotation characterized by a Mølmer-Sørensen error rate of 10−4 . The colored regions indicate which code is optimal at those error parameters, with darker shading implying the code is outperforming a physical CNOT. The colored curves are the pseudothreshold curves for which the logical error rate is equal to the physical error rate in Eq. 5 and the black curves are borders between regions in which different codes are preferred. https://www.epiqc.cs.uchicago.edu/fault-tolerant-compass-codes daily 0.75 2021-01-28 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1611862768206-O5FA14B6MSMIEPXLZXWJ/fault.tol.fig2.jpg Fault-tolerant compass codes Figures showing best performing codes and pseudothresholds for different error models and sets of codes. In (a,b,c) we are comparing codes in the set {Surface-17, Bacon-Shor-13, Shor-6X2Z, Shor-6Z2X}, while in (d,e,f) we restrict our set to only consider codes with a transversal Hadamard gate, {Surface-17, Bacon-Shor-13}. In (a,d) we look at the intersection of overrotation error (parameterized by the two qubit gate error) and T2 dephasing, in (b,e) we look at overrotation and crosstalk, and in (c,f) we look at T2 dephasing and crosstalk with a background overrotation characterized by a Mølmer-Sørensen error rate of 10−4 . The colored regions indicate which code is optimal at those error parameters, with darker shading implying the code is outperforming a physical CNOT. The colored curves are the pseudothreshold curves for which the logical error rate is equal to the physical error rate in Eq. 5 and the black curves are borders between regions in which different codes are preferred. https://www.epiqc.cs.uchicago.edu/workshop-i2q daily 0.75 2024-07-02 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1519764998877-QB0JJMMB269ZIH9WGU97/ibm-qc.jpg Workshop: I2Q https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/251857d5-3196-484e-b5aa-809be6f1e069/I2q_23.png Workshop: I2Q - Make it stand out Whatever it is, the way you tell your story online can make all the difference. https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1535494469505-BUS2L4HIQLWKL1QCQ0DA/IMG_0256.jpg Workshop: I2Q https://www.epiqc.cs.uchicago.edu/large-circuits-small-computer daily 0.75 2021-02-08 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1612797435762-3WBKUW9BMM5K5OPQB02Z/harrow.bigcirc.small.computers.png Large circuits, small computer Figures showing best performing codes and pseudothresholds for different error models and sets of codes. In (a,b,c) we are comparing codes in the set {Surface-17, Bacon-Shor-13, Shor-6X2Z, Shor-6Z2X}, while in (d,e,f) we restrict our set to only consider codes with a transversal Hadamard gate, {Surface-17, Bacon-Shor-13}. In (a,d) we look at the intersection of overrotation error (parameterized by the two qubit gate error) and T2 dephasing, in (b,e) we look at overrotation and crosstalk, and in (c,f) we look at T2 dephasing and crosstalk with a background overrotation characterized by a Mølmer-Sørensen error rate of 10−4 . The colored regions indicate which code is optimal at those error parameters, with darker shading implying the code is outperforming a physical CNOT. The colored curves are the pseudothreshold curves for which the logical error rate is equal to the physical error rate in Eq. 5 and the black curves are borders between regions in which different codes are preferred. https://www.epiqc.cs.uchicago.edu/fault-tolerant-cluster-states daily 0.75 2021-02-08 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1612815545517-7KM35KM0RUJL5YGUS2V4/crystal_image.Newman.png Fault-Tolerant Cluster States Figures showing best performing codes and pseudothresholds for different error models and sets of codes. In (a,b,c) we are comparing codes in the set {Surface-17, Bacon-Shor-13, Shor-6X2Z, Shor-6Z2X}, while in (d,e,f) we restrict our set to only consider codes with a transversal Hadamard gate, {Surface-17, Bacon-Shor-13}. In (a,d) we look at the intersection of overrotation error (parameterized by the two qubit gate error) and T2 dephasing, in (b,e) we look at overrotation and crosstalk, and in (c,f) we look at T2 dephasing and crosstalk with a background overrotation characterized by a Mølmer-Sørensen error rate of 10−4 . The colored regions indicate which code is optimal at those error parameters, with darker shading implying the code is outperforming a physical CNOT. The colored curves are the pseudothreshold curves for which the logical error rate is equal to the physical error rate in Eq. 5 and the black curves are borders between regions in which different codes are preferred. https://www.epiqc.cs.uchicago.edu/quantum-algorithms-for-jet-clustering daily 0.75 2021-02-10 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1612972034950-K4HVBBW8WWN9UXH3FAG2/jets.partition.png Quantum Algorithms for Jet Clustering Figures showing best performing codes and pseudothresholds for different error models and sets of codes. In (a,b,c) we are comparing codes in the set {Surface-17, Bacon-Shor-13, Shor-6X2Z, Shor-6Z2X}, while in (d,e,f) we restrict our set to only consider codes with a transversal Hadamard gate, {Surface-17, Bacon-Shor-13}. In (a,d) we look at the intersection of overrotation error (parameterized by the two qubit gate error) and T2 dephasing, in (b,e) we look at overrotation and crosstalk, and in (c,f) we look at T2 dephasing and crosstalk with a background overrotation characterized by a Mølmer-Sørensen error rate of 10−4 . The colored regions indicate which code is optimal at those error parameters, with darker shading implying the code is outperforming a physical CNOT. The colored curves are the pseudothreshold curves for which the logical error rate is equal to the physical error rate in Eq. 5 and the black curves are borders between regions in which different codes are preferred. https://www.epiqc.cs.uchicago.edu/adaptive-quantum-simulated-annealing2 daily 0.75 2021-02-10 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1612974044393-S65NERF2UJJPKOR1IQUM/sa.harrow.wei.png Adaptive Quantum Simulated Annealing Figures showing best performing codes and pseudothresholds for different error models and sets of codes. In (a,b,c) we are comparing codes in the set {Surface-17, Bacon-Shor-13, Shor-6X2Z, Shor-6Z2X}, while in (d,e,f) we restrict our set to only consider codes with a transversal Hadamard gate, {Surface-17, Bacon-Shor-13}. In (a,d) we look at the intersection of overrotation error (parameterized by the two qubit gate error) and T2 dephasing, in (b,e) we look at overrotation and crosstalk, and in (c,f) we look at T2 dephasing and crosstalk with a background overrotation characterized by a Mølmer-Sørensen error rate of 10−4 . The colored regions indicate which code is optimal at those error parameters, with darker shading implying the code is outperforming a physical CNOT. The colored curves are the pseudothreshold curves for which the logical error rate is equal to the physical error rate in Eq. 5 and the black curves are borders between regions in which different codes are preferred. https://www.epiqc.cs.uchicago.edu/qubits-needed-for-quantum-supremacy daily 0.75 2021-02-10 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1612976072583-MVIUJ7VXY2B5Z9LARBOF/gapf-distribution.png Qubits Needed for Quantum Supremacy Figures showing best performing codes and pseudothresholds for different error models and sets of codes. In (a,b,c) we are comparing codes in the set {Surface-17, Bacon-Shor-13, Shor-6X2Z, Shor-6Z2X}, while in (d,e,f) we restrict our set to only consider codes with a transversal Hadamard gate, {Surface-17, Bacon-Shor-13}. In (a,d) we look at the intersection of overrotation error (parameterized by the two qubit gate error) and T2 dephasing, in (b,e) we look at overrotation and crosstalk, and in (c,f) we look at T2 dephasing and crosstalk with a background overrotation characterized by a Mølmer-Sørensen error rate of 10−4 . The colored regions indicate which code is optimal at those error parameters, with darker shading implying the code is outperforming a physical CNOT. The colored curves are the pseudothreshold curves for which the logical error rate is equal to the physical error rate in Eq. 5 and the black curves are borders between regions in which different codes are preferred. https://www.epiqc.cs.uchicago.edu/circuit-decompositions-with-qudits daily 0.75 2021-02-11 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1613072887147-0WM06C5FULB5UONKBTGB/Baker.ISMVL.png Circuit Decompositions with Qudits Figures showing best performing codes and pseudothresholds for different error models and sets of codes. In (a,b,c) we are comparing codes in the set {Surface-17, Bacon-Shor-13, Shor-6X2Z, Shor-6Z2X}, while in (d,e,f) we restrict our set to only consider codes with a transversal Hadamard gate, {Surface-17, Bacon-Shor-13}. In (a,d) we look at the intersection of overrotation error (parameterized by the two qubit gate error) and T2 dephasing, in (b,e) we look at overrotation and crosstalk, and in (c,f) we look at T2 dephasing and crosstalk with a background overrotation characterized by a Mølmer-Sørensen error rate of 10−4 . The colored regions indicate which code is optimal at those error parameters, with darker shading implying the code is outperforming a physical CNOT. The colored curves are the pseudothreshold curves for which the logical error rate is equal to the physical error rate in Eq. 5 and the black curves are borders between regions in which different codes are preferred. https://www.epiqc.cs.uchicago.edu/quantum-program-error-analysis daily 0.75 2021-07-12 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1625075492337-1BDOIYYF4PDUTWX9TV7Q/gleipnir-workflow.png Quantum Program Error Analysis Figures showing best performing codes and pseudothresholds for different error models and sets of codes. In (a,b,c) we are comparing codes in the set {Surface-17, Bacon-Shor-13, Shor-6X2Z, Shor-6Z2X}, while in (d,e,f) we restrict our set to only consider codes with a transversal Hadamard gate, {Surface-17, Bacon-Shor-13}. In (a,d) we look at the intersection of overrotation error (parameterized by the two qubit gate error) and T2 dephasing, in (b,e) we look at overrotation and crosstalk, and in (c,f) we look at T2 dephasing and crosstalk with a background overrotation characterized by a Mølmer-Sørensen error rate of 10−4 . The colored regions indicate which code is optimal at those error parameters, with darker shading implying the code is outperforming a physical CNOT. The colored curves are the pseudothreshold curves for which the logical error rate is equal to the physical error rate in Eq. 5 and the black curves are borders between regions in which different codes are preferred. https://www.epiqc.cs.uchicago.edu/type-theoretic-interpretation-of-q daily 0.75 2021-09-29 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1626115130372-EV3XJ3R580F3VURYCGNJ/ttiq.png Type-Theoretic Interpretation of Q# Figures showing best performing codes and pseudothresholds for different error models and sets of codes. In (a,b,c) we are comparing codes in the set {Surface-17, Bacon-Shor-13, Shor-6X2Z, Shor-6Z2X}, while in (d,e,f) we restrict our set to only consider codes with a transversal Hadamard gate, {Surface-17, Bacon-Shor-13}. In (a,d) we look at the intersection of overrotation error (parameterized by the two qubit gate error) and T2 dephasing, in (b,e) we look at overrotation and crosstalk, and in (c,f) we look at T2 dephasing and crosstalk with a background overrotation characterized by a Mølmer-Sørensen error rate of 10−4 . The colored regions indicate which code is optimal at those error parameters, with darker shading implying the code is outperforming a physical CNOT. The colored curves are the pseudothreshold curves for which the logical error rate is equal to the physical error rate in Eq. 5 and the black curves are borders between regions in which different codes are preferred. https://www.epiqc.cs.uchicago.edu/spectral-circuit-mapping daily 0.75 2021-09-29 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1626115629234-KXCEEEHVM25HZZ2H266P/Lin.greedy_spectral_vs_arct_size_qiskit_errorbars.png Spectral Circuit Mapping Figures showing best performing codes and pseudothresholds for different error models and sets of codes. In (a,b,c) we are comparing codes in the set {Surface-17, Bacon-Shor-13, Shor-6X2Z, Shor-6Z2X}, while in (d,e,f) we restrict our set to only consider codes with a transversal Hadamard gate, {Surface-17, Bacon-Shor-13}. In (a,d) we look at the intersection of overrotation error (parameterized by the two qubit gate error) and T2 dephasing, in (b,e) we look at overrotation and crosstalk, and in (c,f) we look at T2 dephasing and crosstalk with a background overrotation characterized by a Mølmer-Sørensen error rate of 10−4 . The colored regions indicate which code is optimal at those error parameters, with darker shading implying the code is outperforming a physical CNOT. The colored curves are the pseudothreshold curves for which the logical error rate is equal to the physical error rate in Eq. 5 and the black curves are borders between regions in which different codes are preferred. https://www.epiqc.cs.uchicago.edu/epr-assistance-suffices daily 0.75 2021-07-12 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1626116055126-HK7KXQQUNBDRAVDMRIQD/EPR-assistance+suffices.png EPR-assistance suffices Figures showing best performing codes and pseudothresholds for different error models and sets of codes. In (a,b,c) we are comparing codes in the set {Surface-17, Bacon-Shor-13, Shor-6X2Z, Shor-6Z2X}, while in (d,e,f) we restrict our set to only consider codes with a transversal Hadamard gate, {Surface-17, Bacon-Shor-13}. In (a,d) we look at the intersection of overrotation error (parameterized by the two qubit gate error) and T2 dephasing, in (b,e) we look at overrotation and crosstalk, and in (c,f) we look at T2 dephasing and crosstalk with a background overrotation characterized by a Mølmer-Sørensen error rate of 10−4 . The colored regions indicate which code is optimal at those error parameters, with darker shading implying the code is outperforming a physical CNOT. The colored curves are the pseudothreshold curves for which the logical error rate is equal to the physical error rate in Eq. 5 and the black curves are borders between regions in which different codes are preferred. https://www.epiqc.cs.uchicago.edu/optimal-control-compiler daily 0.75 2021-08-11 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1556364588390-IM5W9JFLJAH7HXAWDIXT/QAOA_Aggregated.png Optimal Control Compiler Circuit with aggregated instructions https://www.epiqc.cs.uchicago.edu/logical-abstraction-quantum-simulation daily 0.75 2021-09-29 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1628702603358-MH2U8AI42Y60HHBB6R2F/NoisyBN.png Logical Abstraction Quantum Simulation Figures showing best performing codes and pseudothresholds for different error models and sets of codes. In (a,b,c) we are comparing codes in the set {Surface-17, Bacon-Shor-13, Shor-6X2Z, Shor-6Z2X}, while in (d,e,f) we restrict our set to only consider codes with a transversal Hadamard gate, {Surface-17, Bacon-Shor-13}. In (a,d) we look at the intersection of overrotation error (parameterized by the two qubit gate error) and T2 dephasing, in (b,e) we look at overrotation and crosstalk, and in (c,f) we look at T2 dephasing and crosstalk with a background overrotation characterized by a Mølmer-Sørensen error rate of 10−4 . The colored regions indicate which code is optimal at those error parameters, with darker shading implying the code is outperforming a physical CNOT. The colored curves are the pseudothreshold curves for which the logical error rate is equal to the physical error rate in Eq. 5 and the black curves are borders between regions in which different codes are preferred. https://www.epiqc.cs.uchicago.edu/large-circuits-small-computer-1 daily 0.75 2021-08-11 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1612797435762-3WBKUW9BMM5K5OPQB02Z/harrow.bigcirc.small.computers.png Large circuits, small computer Figures showing best performing codes and pseudothresholds for different error models and sets of codes. In (a,b,c) we are comparing codes in the set {Surface-17, Bacon-Shor-13, Shor-6X2Z, Shor-6Z2X}, while in (d,e,f) we restrict our set to only consider codes with a transversal Hadamard gate, {Surface-17, Bacon-Shor-13}. In (a,d) we look at the intersection of overrotation error (parameterized by the two qubit gate error) and T2 dephasing, in (b,e) we look at overrotation and crosstalk, and in (c,f) we look at T2 dephasing and crosstalk with a background overrotation characterized by a Mølmer-Sørensen error rate of 10−4 . The colored regions indicate which code is optimal at those error parameters, with darker shading implying the code is outperforming a physical CNOT. The colored curves are the pseudothreshold curves for which the logical error rate is equal to the physical error rate in Eq. 5 and the black curves are borders between regions in which different codes are preferred. https://www.epiqc.cs.uchicago.edu/designing-reliable-qccd-systems-1 daily 0.75 2021-08-11 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1609885280597-JO47TLLSZUU5Z8BGNFCC/Designing+Reliable+QCCD+Systems.png Designing Reliable QCCD Systems Superdense coding circuit sending classical bits x and y from Alice to Bob and its program annotated with types at each step https://www.epiqc.cs.uchicago.edu/gottesman-types-for-quantum-programs-1 daily 0.75 2021-09-08 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1609794766989-FKPBKAWNER8585DKGCIO/Gottesman.types.png Gottesman Types for Quantum Programs Superdense coding circuit sending classical bits x and y from Alice to Bob and its program annotated with types at each step https://www.epiqc.cs.uchicago.edu/architecting-nisq-systems-1 daily 0.75 2021-08-11 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1628546599346-47N39TW1IX4K6D7AJ6HH/Logo-IEEE.jpg Architecting NISQ Systems - TOP PICK TOP PICK https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1609885939402-GYGHII8WQR47KU7KFIQQ/image-asset.png Architecting NISQ Systems QC systems considered in the study https://www.epiqc.cs.uchicago.edu/exploring-quantum-reversibility-with-young-learners-1 daily 0.75 2021-08-11 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1608320183900-SH7OPBBN42WFUPJOZ3MY/reversibility.png Exploring Quantum Reversibility with Young Learners Everyday examples of reversibility to introduce the concept to young learners. https://www.epiqc.cs.uchicago.edu/virtualized-logical-qubits-1 daily 0.75 2021-08-11 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1628546973637-F805DVCD1NMPP18UUL8I/Logo-IEEE.jpg Virtualized Logical Qubits - TOP Pick https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1607108623449-7Z83915DZ0F74N3OQQLI/vlq-fig8-1000.png Virtualized Logical Qubits A 3D view of our virtual logical qubit Compact embedding. Shown at the top is the 2D grid of transmon qubits. Attached below every transmon is a resonant cavity memory. Compact surface code patches are shown stored, one in each mode. This deformed patch can be tiled in 2D. https://www.epiqc.cs.uchicago.edu/vqe-simultaneous-measurement-1 daily 0.75 2021-08-12 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1628785440376-O01C7LMTU03IN9CYNBPP/ibm.quantum.png VQE Simultaneous Measurement - Best Paper https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1585692964357-O16Q4JJ6JRYIMCMBW4AD/two_qubit_pauli_graph.png VQE Simultaneous Measurement Graph of Pauli strings, with an edge between pairs that can be measured simultaneously. We seek large “cliques” of mutually-connected Pauli strings that can all be measured at once. https://www.epiqc.cs.uchicago.edu/extended-frontier-with-qutrits-2 daily 0.75 2021-08-11 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1628615844016-G57AJLFZRJ7P23FPAG1A/Logo-IEEE.jpg Extended Frontier with Qutrits - Top Pick https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1599246970206-PO3OJCTIME86TF6U1LB3/frontier.png Extended Frontier with Qutrits The frontier of a quantum computer is the line where every machine qubit is used as a data qubit. https://www.epiqc.cs.uchicago.edu/systematic-crosstalk-mitigation-1 daily 0.75 2021-08-11 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1628615954811-V8UQ7XYCKRD5Z7H0IZOC/Logo-IEEE.jpg Systematic Crosstalk Mitigation - Top Pick honorable mention https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1607106459316-ODCA2KL8EO8Y2YISTIG4/sys.crosstalk.mitigation.png Systematic Crosstalk Mitigation Key benefit of our crosstalk mitigation methodology. Our software toolflow reduces crosstalk on tunable qubits via frequency-aware compilation and real-time calibration. As a result, our work achieves the same level protection against crosstalk, but on simpler hardware (tunable qubit, fixed-coupler). https://www.epiqc.cs.uchicago.edu/strategic-quantum-ancilla-reuse-1 daily 0.75 2021-08-11 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1628616111591-D079YJ2Q1M6XKXZF7RTN/Logo-IEEE.jpg Strategic Quantum Ancilla Reuse - Top Pick honorable mention https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1591038764803-H1AXEEWRFCXT7QFGPCG8/SQUARE.jpg Strategic Quantum Ancilla Reuse Uncomputation is performed strategically for a program in the SQUARE compiler framework. https://www.epiqc.cs.uchicago.edu/gradient-based-optimal-control-1 daily 0.75 2021-08-11 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1581033410479-8U1M7ZJL8BMG285F18PS/QAOA_Aggregated.png Gradient-Based Optimal Control Computational graph of a quantum trajectory evolution https://www.epiqc.cs.uchicago.edu/stabilizer-slicing-2 daily 0.75 2021-08-11 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1546960939904-SZ5OTAF1CC1LGZG38NDZ/s17Sliced.png Stabilizer Slicing Logical error rates and quadratic fits with and without stabilizer slicing https://www.epiqc.cs.uchicago.edu/vqe-simultaneous-measurement-qce daily 0.75 2021-08-17 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1628616653420-Y2JI8C09SPWX0809KMTH/Logo-IEEE.jpg VQE Simultaneous Measurement (QCE) - Quantum Computing and Engineering (QCE) Best Paper https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1585692964357-O16Q4JJ6JRYIMCMBW4AD/two_qubit_pauli_graph.png VQE Simultaneous Measurement (QCE) Graph of Pauli strings, with an edge between pairs that can be measured simultaneously. We seek large “cliques” of mutually-connected Pauli strings that can all be measured at once. https://www.epiqc.cs.uchicago.edu/vqe-simultaneous-measurement-qce-1 daily 0.75 2021-08-12 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1628616653420-Y2JI8C09SPWX0809KMTH/Logo-IEEE.jpg VQE Simultaneous Measurement (QCE) - Quantum Computing and Engineering (QCE) Best Paper https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1585692964357-O16Q4JJ6JRYIMCMBW4AD/two_qubit_pauli_graph.png VQE Simultaneous Measurement (QCE) Graph of Pauli strings, with an edge between pairs that can be measured simultaneously. We seek large “cliques” of mutually-connected Pauli strings that can all be measured at once. https://www.epiqc.cs.uchicago.edu/coresets-for-small-qcs daily 0.75 2021-09-29 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1632925148360-XKO1UOR320NORO18DGZ2/corsets.electronics-10-01690-g001.png Coresets for Small QCs Figures showing best performing codes and pseudothresholds for different error models and sets of codes. In (a,b,c) we are comparing codes in the set {Surface-17, Bacon-Shor-13, Shor-6X2Z, Shor-6Z2X}, while in (d,e,f) we restrict our set to only consider codes with a transversal Hadamard gate, {Surface-17, Bacon-Shor-13}. In (a,d) we look at the intersection of overrotation error (parameterized by the two qubit gate error) and T2 dephasing, in (b,e) we look at overrotation and crosstalk, and in (c,f) we look at T2 dephasing and crosstalk with a background overrotation characterized by a Mølmer-Sørensen error rate of 10−4 . The colored regions indicate which code is optimal at those error parameters, with darker shading implying the code is outperforming a physical CNOT. The colored curves are the pseudothreshold curves for which the logical error rate is equal to the physical error rate in Eq. 5 and the black curves are borders between regions in which different codes are preferred. https://www.epiqc.cs.uchicago.edu/batch-robust-two-qubit-gates daily 0.75 2021-09-29 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1632938636144-TLDMY48MS5VXNMGPYU0J/brobust_public.PNG Batch Robust Two-qubit Gates Figures showing best performing codes and pseudothresholds for different error models and sets of codes. In (a,b,c) we are comparing codes in the set {Surface-17, Bacon-Shor-13, Shor-6X2Z, Shor-6Z2X}, while in (d,e,f) we restrict our set to only consider codes with a transversal Hadamard gate, {Surface-17, Bacon-Shor-13}. In (a,d) we look at the intersection of overrotation error (parameterized by the two qubit gate error) and T2 dephasing, in (b,e) we look at overrotation and crosstalk, and in (c,f) we look at T2 dephasing and crosstalk with a background overrotation characterized by a Mølmer-Sørensen error rate of 10−4 . The colored regions indicate which code is optimal at those error parameters, with darker shading implying the code is outperforming a physical CNOT. The colored curves are the pseudothreshold curves for which the logical error rate is equal to the physical error rate in Eq. 5 and the black curves are borders between regions in which different codes are preferred. https://www.epiqc.cs.uchicago.edu/seamless-high-q-microwave-cavities-for-multimode-cqed daily 0.75 2021-09-29 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1632946999758-3BIWY22B8Z563AYLHAW1/seamlesshighqtemp.PNG Seamless High-Q Microwave Cavities for Multimode cQED Figures showing best performing codes and pseudothresholds for different error models and sets of codes. In (a,b,c) we are comparing codes in the set {Surface-17, Bacon-Shor-13, Shor-6X2Z, Shor-6Z2X}, while in (d,e,f) we restrict our set to only consider codes with a transversal Hadamard gate, {Surface-17, Bacon-Shor-13}. In (a,d) we look at the intersection of overrotation error (parameterized by the two qubit gate error) and T2 dephasing, in (b,e) we look at overrotation and crosstalk, and in (c,f) we look at T2 dephasing and crosstalk with a background overrotation characterized by a Mølmer-Sørensen error rate of 10−4 . The colored regions indicate which code is optimal at those error parameters, with darker shading implying the code is outperforming a physical CNOT. The colored curves are the pseudothreshold curves for which the logical error rate is equal to the physical error rate in Eq. 5 and the black curves are borders between regions in which different codes are preferred. https://www.epiqc.cs.uchicago.edu/emerging-technologies daily 0.75 2021-09-30 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1633018866653-JO0LTAT4B5VGT1VFT823/Baker.emergent.tech.png Emerging Technologies Figures showing best performing codes and pseudothresholds for different error models and sets of codes. In (a,b,c) we are comparing codes in the set {Surface-17, Bacon-Shor-13, Shor-6X2Z, Shor-6Z2X}, while in (d,e,f) we restrict our set to only consider codes with a transversal Hadamard gate, {Surface-17, Bacon-Shor-13}. In (a,d) we look at the intersection of overrotation error (parameterized by the two qubit gate error) and T2 dephasing, in (b,e) we look at overrotation and crosstalk, and in (c,f) we look at T2 dephasing and crosstalk with a background overrotation characterized by a Mølmer-Sørensen error rate of 10−4 . The colored regions indicate which code is optimal at those error parameters, with darker shading implying the code is outperforming a physical CNOT. The colored curves are the pseudothreshold curves for which the logical error rate is equal to the physical error rate in Eq. 5 and the black curves are borders between regions in which different codes are preferred. https://www.epiqc.cs.uchicago.edu/qc-systems-text-book daily 0.75 2021-10-04 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1633375330790-D74JNQOXFPLU4UVQKPFH/Untitled.001.jpeg QC Systems Text Book https://www.epiqc.cs.uchicago.edu/longdistance-interactions daily 0.75 2021-11-16 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1633539886682-XTKBHMQR0T05U9A0NKKZ/Baker.long.dist.neutral.png Long-Distance Interactions Figures showing best performing codes and pseudothresholds for different error models and sets of codes. In (a,b,c) we are comparing codes in the set {Surface-17, Bacon-Shor-13, Shor-6X2Z, Shor-6Z2X}, while in (d,e,f) we restrict our set to only consider codes with a transversal Hadamard gate, {Surface-17, Bacon-Shor-13}. In (a,d) we look at the intersection of overrotation error (parameterized by the two qubit gate error) and T2 dephasing, in (b,e) we look at overrotation and crosstalk, and in (c,f) we look at T2 dephasing and crosstalk with a background overrotation characterized by a Mølmer-Sørensen error rate of 10−4 . The colored regions indicate which code is optimal at those error parameters, with darker shading implying the code is outperforming a physical CNOT. The colored curves are the pseudothreshold curves for which the logical error rate is equal to the physical error rate in Eq. 5 and the black curves are borders between regions in which different codes are preferred. https://www.epiqc.cs.uchicago.edu/longdistance-interactions-1 daily 0.75 2021-10-08 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1633706783146-O0ME7EDI72D01OGTHBBW/Universal+Graph-Based+Scheduling+.png Universal Graph-Based Scheduling Figures showing best performing codes and pseudothresholds for different error models and sets of codes. In (a,b,c) we are comparing codes in the set {Surface-17, Bacon-Shor-13, Shor-6X2Z, Shor-6Z2X}, while in (d,e,f) we restrict our set to only consider codes with a transversal Hadamard gate, {Surface-17, Bacon-Shor-13}. In (a,d) we look at the intersection of overrotation error (parameterized by the two qubit gate error) and T2 dephasing, in (b,e) we look at overrotation and crosstalk, and in (c,f) we look at T2 dephasing and crosstalk with a background overrotation characterized by a Mølmer-Sørensen error rate of 10−4 . The colored regions indicate which code is optimal at those error parameters, with darker shading implying the code is outperforming a physical CNOT. The colored curves are the pseudothreshold curves for which the logical error rate is equal to the physical error rate in Eq. 5 and the black curves are borders between regions in which different codes are preferred. https://www.epiqc.cs.uchicago.edu/scalable-quantum-circuit-optimization daily 0.75 2021-10-12 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1633984515903-TL5BYKM5CLHI3WS1FDI5/QGo.png Scalable Quantum Circuit Optimization Figures showing best performing codes and pseudothresholds for different error models and sets of codes. In (a,b,c) we are comparing codes in the set {Surface-17, Bacon-Shor-13, Shor-6X2Z, Shor-6Z2X}, while in (d,e,f) we restrict our set to only consider codes with a transversal Hadamard gate, {Surface-17, Bacon-Shor-13}. In (a,d) we look at the intersection of overrotation error (parameterized by the two qubit gate error) and T2 dephasing, in (b,e) we look at overrotation and crosstalk, and in (c,f) we look at T2 dephasing and crosstalk with a background overrotation characterized by a Mølmer-Sørensen error rate of 10−4 . The colored regions indicate which code is optimal at those error parameters, with darker shading implying the code is outperforming a physical CNOT. The colored curves are the pseudothreshold curves for which the logical error rate is equal to the physical error rate in Eq. 5 and the black curves are borders between regions in which different codes are preferred. https://www.epiqc.cs.uchicago.edu/optimizing-quantum-program-ordering daily 0.75 2022-04-12 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1633985207240-8O6539P2NO1ZUV8U6PAY/tomesh.traveling.sales.arX.png Optimizing Quantum Program Ordering - Make it stand out A summary of the DQS compilation process and the max-commute-tsp ordering strategy https://www.epiqc.cs.uchicago.edu/quantum-cloud-resource-management daily 0.75 2022-01-19 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1634131294746-C4RQIYNDJT1B136C0LMJ/Ravi.QCE_Proposal3.jpg Quantum Cloud Resource Management - Make it stand out Jobs are scheduled onto an appropriate quantum machine by the job scheduler based on a variety of scheduling constraints. https://www.epiqc.cs.uchicago.edu/analyzing-quantum-cloud-characteristics daily 0.75 2022-01-19 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1634132255789-IS5JFDCXX209GT3SUUTA/Ravi.SC21_Overview.jpg Analyzing Quantum Cloud Characteristics - Make it stand out Clients launch quantum programs from their classical computers onto the vendor's quantum cloud wherein the jobs are queued until execution. https://www.epiqc.cs.uchicago.edu/adapting-qaoa-for-unit-commitment daily 0.75 2022-01-19 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/5dcd6164-746a-4ff5-9534-aad932674926/Koretsky.uc+clean.png Adapting QAOA for Unit Commitment - Make it stand out Example 4-unit system https://www.epiqc.cs.uchicago.edu/epiqc-retreat-2021 daily 0.75 2021-10-29 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1634155971685-YHBPW8TWZVTW2L8Y1881/P1010617.YD.jpg EPiQC Retreat 2021 - Make it stand out Whatever it is, the way you tell your story online can make all the difference. https://www.epiqc.cs.uchicago.edu/quantum-fan-out daily 0.75 2022-01-19 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/68570ed1-a626-4338-a258-5c2733334b91/Gokahle.QCE.fanout.png Quantum Fan-out - Make it stand out Device level fan-out allows a NOT to the bottom four targets iff the top control is on. While exclusive activation induces serialization (left), quantum hardware can implement fan-out simultaneously (right) in a single step. https://www.epiqc.cs.uchicago.edu/sfq-based-two-qubit-gates daily 0.75 2022-01-05 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1634826169543-4WB36KA7AR75WRFBQBZG/QCE-virtual-logo-graph-200x200-1.jpg SFQ-based two-qubit gates - Make it stand out QCE21 Best Paper Award https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1634332027655-S3DMLUNAYFTV13QJR46H/sfq_qce.png SFQ-based two-qubit gates - Make it stand out Error comparison between microwave-based CZ gates obtained using Grape code and SFQ-based CZ gates obtained using genetic algorithm. https://www.epiqc.cs.uchicago.edu/edx-courses daily 0.75 2021-10-22 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1634825639413-I96ECA4RH3818AHQ8XI6/edX.logo.png edX Courses - Make it stand out Whatever it is, the way you tell your story online can make all the difference. https://www.epiqc.cs.uchicago.edu/entanglement_ball daily 0.75 2021-10-28 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1635365166481-J05LR78DDJHJ3JNEXOUY/entanglement.ball.jpg Entanglement Ball - Make it stand out Representation of round 1 game play. https://www.epiqc.cs.uchicago.edu/secure-software-leasing daily 0.75 2021-10-28 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1635448711746-LL6IB4FZ1ANXXT01GQZ3/youtube.png Secure Software Leasing - Make it stand out Video from EUROCRYPT 2021 https://www.epiqc.cs.uchicago.edu/quantum-hypothesis-testing daily 0.75 2021-10-28 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1635449413762-XYK7D70PE6SPMMHQG8X9/QHT.Rossi.png Quantum Hypothesis Testing - Make it stand out Simplified illustrations of different models for quantum circuits performing QHT. Depicted are (a) serial adaptive, (b) parallel, and (c) mixed strategies. https://www.epiqc.cs.uchicago.edu/pimc-1d-stoquastic daily 0.75 2021-11-01 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1635780029425-27HMRYI2NK3L8JDOIJW2/PIMC.harrow.png PIMC 1D stoquastic - Make it stand out Our convergence proof for the Quantum Monte Carlo algorithm uses the "canonical paths" method which requires defining a path between any two possible configurations. One step of the path is illustrated here. https://www.epiqc.cs.uchicago.edu/nonlinear-bell-inequalities daily 0.75 2021-11-01 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1635781023847-70X7DWFOG8R66FPPS9QN/entangledBindingSixSinglets.png Nonlinear Bell inequalities - Make it stand out Our Bell inequalities detect entanglement in macroscopic entangled states like the one pictured here. https://www.epiqc.cs.uchicago.edu/people-1 daily 0.75 2021-11-30 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1515789149169-CHYTX9DDMN0ZWIP5EHHD/DianaCropped.jpg EdTeam Diana Franklin, Associate Professor, EPiQC Education PI Lead. UChicago Computer Science & Quantum Computing Education https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1515789041612-7ZJMO93PRH5WTE5AIG1Y/2886-1.jpg EdTeam Danielle Harlow, Professor UCSB STEM Education https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1525296647854-LOSMAQ51DWGW7XLF40S2/RHL.web.250.250.jpg EdTeam Randall H. Landsberg, EPiQC Director of Ed/Outreach UChicago Education https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1527681058701-HMFP7BYPQPMG5JT2BJ5O/image-asset.png EdTeam Jen Palmer, Curriculum Developer UChicago Science & Computer Science Education https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/8db49c78-38af-4761-a963-1c450a4383ed/portraitpicture2+%281%29.jpg EdTeam - Make it stand out Brent Yen, Curriculum Developer, Research Scientist. UChicago Quantum Information, Education https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1578519317513-20XL6XRLC3XVIBQRQI44/smith.kate.JPG EdTeam Kate Smith, Post-Doctoral Scholar UChicago Technology-Aware Programming Environment https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1579882376449-YGD0QNCARUHFJ227ZG4J/Christman.Devon2.png EdTeam Devon Christman, Graduate Student UCSB Science & Computer Science Education https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1633102761080-CK40554FBKU8UT3F6XB7/Liu.Jonathan.JPG EdTeam - Make it stand out Jonathan Liu, Graduate Student. UChicago Computer Science & Theory Education https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1626121950183-3RTLIE1RK2UR16894ZK5/Lee.Irina.jpeg EdTeam - Make it stand out Irina Lee, Undergraduate UChicago Computer Science https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1558382374882-DWJN4F9W44Q6OO2UVMFH/lehman.liz.png EdTeam Liz Lehman, Curriculum Developer UChicago Education https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1576530063739-066SWGK810C9OX7Q3209/Bennett.Matthew.png EdTeam Matthew Bennet, Graduate Student UCSB Education https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1527681230953-56Y83D4DWPSQ0ZV53IA0/image-asset.jpeg EdTeam Jasmine Marckwordt, Graduate Student UCSB Education https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1543442203399-X7DJ4QK5DAQST9J3R9VJ/Muller_Alexandria_Square.jpg EdTeam Alexandria Muller, Graduate Student UCSB Education https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1543442410412-EIQLG8ECWTSSLLUYIYK6/Crowdus.jpg EdTeam Elizabeth Crowdus, Undergraduate UChicago https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1590677035749-34GCKZ5WGYD0QLJ46ZUZ/Goodman.Noah.jpg EdTeam Noah Goodman, Undergraduate UChicago https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1590676841322-H2K51J5FBK90868SLP0K/Jang.Woorin.jpg EdTeam Woorin Jang, Undergraduate UChicago https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1591710193988-FLRLO98Z2PXBLHVUM72R/Klain.Zipporah.png EdTeam Zipporah Klain, Undergraduate UChicago https://www.epiqc.cs.uchicago.edu/hybrid-quantum-circuit-evaluation daily 0.75 2022-01-07 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/77d3cc91-ce18-4163-b1b9-8623768cf965/CutQC.Tomesh.cutting_example.png Hybrid Quantum Circuit Evaluation - Make it stand out Example of cutting a five-qubit circuit into two smaller subcircuits of three qubits each. https://www.epiqc.cs.uchicago.edu/quantum-fan-out2 daily 0.75 2022-01-19 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1634826169543-4WB36KA7AR75WRFBQBZG/QCE-virtual-logo-graph-200x200-1.jpg Quantum Fan-out - Make it stand out QCE21 Best Paper Award https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1634332027655-S3DMLUNAYFTV13QJR46H/sfq_qce.png Quantum Fan-out - Make it stand out Error comparison between microwave-based CZ gates obtained using Grape code and SFQ-based CZ gates obtained using genetic algorithm. https://www.epiqc.cs.uchicago.edu/adaptive-sensing daily 0.75 2022-01-19 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/5be06991-e70f-4572-8926-be9d94dd5f78/Ma.Adaptive.Sensing.schematic.png Adaptive Sensing - Make it stand out Algorithm schematic https://www.epiqc.cs.uchicago.edu/orchestrated-trios daily 0.75 2022-01-26 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/75fade0d-eeb1-44b0-9b99-9993fb675878/trios-web-fig1.png Orchestrated Trios - Make it stand out Example routing from Qiskit (a) vs. Trios (b). Circles represent qubits and arrows (labeled by timestep) show the SWAP gates used by each compiler for a Toffoli gate on qubits 2, 6, and 19. https://www.epiqc.cs.uchicago.edu/between-shor-and-steane daily 0.75 2022-01-31 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/32e6b93f-f994-4047-b79a-35fbc5a59e11/shorandsteane.png Between Shor and Steane - Make it stand out The decoder graphs of the toric code: the syndrome bits are vertices, the data errors are horizontal edges, and the type-I measurement errors are vertical edges. The ancilla blocks when aligned (a) lead to timelike correlations between directed repeated measurements. By offsetting the ancilla blocks (b), the timelike correlations require spacelike errors in order to correlate defects from top to bottom. https://www.epiqc.cs.uchicago.edu/linear-tape-quantum-architecture daily 0.75 2022-04-12 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/104d8bf7-1566-4ec8-9d58-cc47a4a84d82/TILT.Wu.png Linear-Tape Quantum Architecture - Make it stand out A trapped-ion linear-tape quantum computing architecture. https://www.epiqc.cs.uchicago.edu/hierarchical-synthesized-circuit-reoptimization daily 0.75 2022-04-12 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/49841bfe-e6c7-4790-87de-94d178f48631/Hierarchical+Synthesized+Circuit+Reoptimization.Wu.png Hierarchical Synthesized Circuit Reoptimization - Make it stand out An example of hierarchical synthesis for circuit optimization. https://www.epiqc.cs.uchicago.edu/epiqc-retreat-2022 daily 0.75 2022-06-03 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/24d374ea-a8b6-4f70-b29e-2a9646a79a93/UChicago_Aerial-Campus-Skyline.jpg EPiQC Retreat 2022 - Make it stand out Whatever it is, the way you tell your story online can make all the difference. https://www.epiqc.cs.uchicago.edu/systematic-design-of-trapped-ion-qc daily 0.75 2022-11-02 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/d22db3a9-4646-4b00-a690-aec7fad8bd52/Modular.QCCD.Murali.png Systematic Design of Trapped Ion QC - Make it stand out Modular QCCD system https://www.epiqc.cs.uchicago.edu/hidden-inverse-error-cancellation daily 0.75 2022-11-02 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/df81c518-9b94-43be-b5da-331f3f611443/Hidden+Inverse+Error+Cancelation.png Hidden Inverse Error Cancellation - Make it stand out Two-qubit hidden inverse experiment data and simulated final state fidelity https://www.epiqc.cs.uchicago.edu/entanglement-spread daily 0.75 2022-11-03 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/dc39ee03-fd89-426b-a117-519ea785b45f/entanglement.spread.png Entanglement Spread - Make it stand out Entanglement spectrum across a general partition https://www.epiqc.cs.uchicago.edu/variational-error-mitigation daily 0.75 2022-11-04 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/aaf29022-5df4-47ad-aae1-9633077124a4/VAQEM.intro.png Variational Error Mitigation - Make it stand out Traditional VAQ flow (dashed grey arrows) & VAQEM error mitigation (red arrow) https://www.epiqc.cs.uchicago.edu/robust-quantum-circuits-search daily 0.75 2023-01-24 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1777d3ab-6d6f-405b-ae28-3fd704628fc6/Robust+Quantum+Circuits+Search.png+.png Robust Quantum Circuits Search - Make it stand out Noise-adaptive circuit and qubit mapping co-search. A gatesharing SuperCircuit that contains numerous parameter subsets (SubCircuit) is firstly trained. Then we perform an evolutionary search with the quantum noise feedback to find the most robust circuit and qubit mapping. https://www.epiqc.cs.uchicago.edu/ml-for-fidelity-estimation daily 0.75 2023-01-24 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1ead0f9d-21c8-4b4c-8f60-9fc04de3324a/ML.4.fidelity.png ML for Fidelity Estimation - Make it stand out The proposed fidelity prediction framework. The quantum circuit is firstly embedded into a graph in which the nodes are gates and edges are execution orders. The feature vector on each node contains the device noise information, such as gate error rates. The graph is processed by a graph transformer in TorchQuantum to estimate circuit fidelity. https://www.epiqc.cs.uchicago.edu/scalable-quantum-controller daily 0.75 2023-01-24 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/c478edca-3a0d-49eb-9c3f-633cc4350a2f/Scalable+Quantum+Controller.fridge2.png Scalable Quantum Controller - Make it stand out (a) Today’s controller design: controller at room temperature, (b) DigiQ: controller close to quantum chip https://www.epiqc.cs.uchicago.edu/supermarq-scalable-quantum-benchmarking daily 0.75 2023-01-24 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/9e56571a-bc56-48d0-ada5-e40fa17d7184/SupermarQ.png SupermarQ: Scalable Quantum Benchmarking - Make it stand out Hardware-agnostic feature maps of the eight original SupermarQ benchmarks. https://www.epiqc.cs.uchicago.edu/preparation-of-metrological-states daily 0.75 2023-01-24 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/d0e2ab48-b5e4-4e79-9fe0-aa9db5c25ccd/Preparation+of+Metrological+States.png Preparation of Metrological States - Make it stand out Preparation of metrological states by variational ansatz. a Schematic of a dipolar-interacting spin ensemble in a 3D-random configuration. b The quantum circuit consists of three parts: a sequence for generating entanglement (entangler), phase accumulation (Ramsey) and single-qubit readout in the Pz basis. Dipolar interactions during Ramsey interference are eliminated by dynamical decoupling. The measurement outcome is processed on a classical computer and used to determine the next generation for θ. c Gate sequence of each variational layer and the Wigner distributions for a 5-spin state after each gate. d Illustration of an optimization process on a 3-spin system with m = 1. The contour plots show the 2D projection of the multidimensional θ space for fixed ϑ1. The orange points mark the sampling positions in the parameter space. Convergence to the global maximum is reached in the 63rd generation. https://www.epiqc.cs.uchicago.edu/supermarq-scalable-quantum-benchmarking-copy daily 0.75 2023-01-25 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/9e56571a-bc56-48d0-ada5-e40fa17d7184/SupermarQ.png Preparation of Metrological States - Make it stand out Hardware-agnostic feature maps of the eight original SupermarQ benchmarks. https://www.epiqc.cs.uchicago.edu/photonic-qcs daily 0.75 2023-05-09 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1674779528772-9ZTVU6D9Z2KITOQOL3TP/PhotonicQCs_page+1.png Photonic Quantum Computers https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1674779528773-KEJGDUM96RZBNOQQ21BT/PhotonicQCs_page+2.png Photonic Quantum Computers https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1674779529663-NWF81R3LN4TBWBCLWKPT/PhotonicQCs_page+3.png Photonic Quantum Computers https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1674779529744-6BGK81FYVXFKWVLN9MDU/PhotonicQCs_page+4.png Photonic Quantum Computers https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1674779530468-QD813ZLWCEAEWG7ZRIUE/PhotonicQCs_page+5.png Photonic Quantum Computers https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1674779530536-XQIUQAKL119GY06ANDJ3/PhotonicQCs_page+6.png Photonic Quantum Computers https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1674779531313-1J1EGU74IS4DHTXUEYYD/PhotonicQCs_page+7.png Photonic Quantum Computers https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1674779531391-ZDMWSB68XSCALR2G437H/PhotonicQCs_page+8.png Photonic Quantum Computers https://www.epiqc.cs.uchicago.edu/simulation-of-real-time-software daily 0.75 2023-02-02 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/106a548e-50b5-4ba7-a71f-489e188a444c/Simulation+of+real-time+software.png Simulation of real-time software - Make it stand out A schematic overview of the microarchitectural components in the core device. https://www.epiqc.cs.uchicago.edu/modular-real-time-software daily 0.75 2023-02-02 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/e79e77a2-780a-46d4-8e8b-b77bc56915a9/Modular+real-time+software.png Modular real-time software - Make it stand out A schematic overview of the microarchitectural components in the core device. https://www.epiqc.cs.uchicago.edu/time-efficient-qudit-gates daily 0.75 2023-02-02 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/ef0499de-045d-49c9-9015-9203da94c3c8/Seifert.H_4_intro_2.png Time-Efficient Qudit Gates - Make it stand out For quantum optimal control tasks to realize a certain gate or state evolution, truncated control pulses can be used as initial guesses for optimizations of shorter duration. Since they originate from a previous optimization, they already drive the system close to the desired objective. In this figure, the plot on the top shows a high-fidelity pulse being truncated to a shorter duration, and the plot on the bottom is the result of re-optimizing this truncated pulse (achieving the same high fidelity at a shorter duration). https://www.epiqc.cs.uchicago.edu/qunity daily 0.75 2023-02-02 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/4c7b5e10-f8c7-44b9-80b3-ffa54885b517/qunity-features.jpg Qunity - Make it stand out Translating classical language features to the quantum domain. https://www.epiqc.cs.uchicago.edu/boosting-fidelity-of-qaoa-by-skipping-hotspot-nodes daily 0.75 2023-02-16 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/800fb099-32d6-47b5-be48-609d726f1769/frozen.qubit.png Boosting Fidelity of QAOA by Skipping Hotspot Nodes - Make it stand out Frozen Qubit https://www.epiqc.cs.uchicago.edu/ion-trap-crosstalk-cancellation daily 0.75 2023-02-16 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/dc557170-680e-464b-b072-7815f5862239/crosstalk.png Ion Trap Crosstalk Cancellation - Make it stand out (a) Schematic of a five-ion chain with two tightly focused beams addressing ion 1 and ion 2 and the rest of the ions considered to be the spectators impacted by intensity crosstalk. (b) Circuit model of the effect of crosstalk with one spectator qubit. The residual entanglement between each target qubit and the spectator qubit is expressed as the MS interaction X^σϕ. (c) Populations of ion 0 and ion 3 (red and blue, respectively) after applying 21 consecutive XX(π/4) to ion 1 and ion 2. The population of ion 3 varies as the effective crosstalk depends on ϕbeam. The population of ion 0 sees a much smaller excitation, since ion 0’s coupling to the motional modes mostly involved in the MS gate is weaker. The population of ion 3 after crosstalk suppression using the echoing technique is also shown (green). The average population drops from 0.25 to 0.03. https://www.epiqc.cs.uchicago.edu/modular-simulator-for-quantum-circuits daily 0.75 2023-02-16 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/3070618f-6632-420e-878d-dcb25a9c4d55/Modular+Simulator+for+Quantum+Circuitsrb_plot_img.png Modular Simulator for Quantum Circuits - Make it stand out Results from running Direct RB on hardware and in simulation https://www.epiqc.cs.uchicago.edu/let-each-quantum-bit-choose daily 0.75 2023-02-16 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/e0ce4762-dd27-4a53-90fb-cd984b706f61/Lin.weyl_chamber_swap.png Let each quantum bit choose - Make it stand out Gates that are not able to synthesize SWAP in 3 layers, shown in a Weyl chamber. https://www.epiqc.cs.uchicago.edu/advances-in-quantum-computation daily 0.75 2023-02-18 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/e153d25c-e460-42fc-84a0-6e1289da3053/Advances+in+Quantum+Computation.stack.png Advances in Quantum Computation - Make it stand out Abstraction stack of classical/quantum computation https://www.epiqc.cs.uchicago.edu/robust-quantum-optimal-control daily 0.75 2023-02-20 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/236f94d1-eef8-4a9b-97b0-2488e447ff38/Robust+Quantum+Optimal+Control.png Robust Quantum Optimal Control - Make it stand out This work investigated tradeoffs between gate length and robustness to experimental errors for quantum computers. https://www.epiqc.cs.uchicago.edu/hs-qiskit daily 0.75 2024-09-27 https://www.epiqc.cs.uchicago.edu/neutral-atom-qcs daily 0.75 2023-05-09 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1680292247598-17TYP8N0B57CUWJOLVYS/1-COVER.png Neutral Atom Quantum Computers https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1680292247726-B93QG47LIU27M5QB6XHS/2.png Neutral Atom Quantum Computers https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1680292248366-HUZ6OPBPLLC441RD5SRQ/3.png Neutral Atom Quantum Computers https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1680292248457-PHJS8Y2R71EX5HBZ7ZNL/4.png Neutral Atom Quantum Computers https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1680621559188-YMDSU3IADN864XBPJX46/5.png Neutral Atom Quantum Computers https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1680292249293-YF5Y1JYAN5L3JKMG4YD5/6.png Neutral Atom Quantum Computers https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1680292249950-75BT7TR6D13AA3U2HE66/7.png Neutral Atom Quantum Computers https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1680292250057-7U2O3EXF45DK2N37XII5/8-BACK.png Neutral Atom Quantum Computers https://www.epiqc.cs.uchicago.edu/qc-history-jpn daily 0.75 2023-05-15 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1684182108171-HNNQ7YL5IH4Y1M7HOHVO/1-COVER%40300x.png 量子コンピューティングの歴史 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1684182108239-91D1AXNF2QKVQL1IFQM5/2%40300x.png 量子コンピューティングの歴史 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1684182108913-0LNHAC5AHM6UMG5BF6KN/3%40300x.png 量子コンピューティングの歴史 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1684182108985-3FRW5JL02G2BLBVHZSD2/4%40300x.png 量子コンピューティングの歴史 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1684182109637-DXBMYID95OKMEM8CVYO7/5%40300x.png 量子コンピューティングの歴史 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1684182109778-GZWX2O6P8I198LV2JW5R/6%40300x.png 量子コンピューティングの歴史 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1684182110418-U47Y7BBNRKUUXM6KOALM/7%40300x.png 量子コンピューティングの歴史 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1684182110487-J1SMKAS7PXLNRENMHBAQ/8-BACK%40300x.png 量子コンピューティングの歴史 https://www.epiqc.cs.uchicago.edu/1-qubit-jpn daily 0.75 2023-05-15 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1684117610881-CTP3I08Y2Q9T8DXF8VSF/1-COVER%40300x.png 1量子ビット https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1684117610877-WWLSBAAXUZJO2W77CFVQ/2%40300x.png 1量子ビット https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1684117611728-NVKOTJWZTJ9LV3LAQKVA/3%40300x.png 1量子ビット https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1684117611855-LAWUDIN93GS4S9RAFITV/4%40300x.png 1量子ビット https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1684117612411-SJMTFD0QSM7RCO0FG5TY/5%40300x.png 1量子ビット 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https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683815210440-R5C0WNZNHV02862W17QH/1-COVER%40300x.png 指数的な発展を https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683815210623-RC32GQ1ALS15G3GFUIDY/2%40300x.png 指数的な発展を https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683815211240-FCOXOBPYKK3RJYDHLQJI/3%40300x.png 指数的な発展を https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683815211348-AE737IYDV33HI0GM1RSG/4%40300x.png 指数的な発展を https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683815211980-9Z3OD6QDWKZFOYF8M7IW/5%40300x.png 指数的な発展を https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683815212081-L4QPR2BQXQ6DZSS97984/6%40300x.png 指数的な発展を https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683815212882-S8EX5MH0YLLYCCBIHPC0/7%40300x.png 指数的な発展を https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683815213039-TR1B06YMVOS173M77GCI/8-BACK%40300x.png 指数的な発展を https://www.epiqc.cs.uchicago.edu/linear-algebra-jpn daily 0.75 2023-05-15 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683815575120-P1TQHB0F0ZBSFX536GIN/1-COVER%40300x.png 線形代数 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683815575205-SMGSGKQC7OCM156IZOA2/2%40300x.png 線形代数 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683815575771-SGTTZF8ZVZX3ZSCCR26A/3%40300x.png 線形代数 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683815575843-2H4GYJ0FLO3BNXNMG8S4/4%40300x.png 線形代数 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683815576481-JBK2MTGUXGJFE8T7YVX6/5%40300x.png 線形代数 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683815576524-PCL6COVSJ00CRLPTA61K/6%40300x.png 線形代数 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683815577152-S4ILIOTIOKU0KMTMA5F5/7%40300x.png 線形代数 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683815577250-DBENQ9HLVWT6M85E8UFF/8-COVER%40300x.png 線形代数 https://www.epiqc.cs.uchicago.edu/superconducting-qcs-jpn daily 0.75 2023-05-15 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683816403657-QH5UFMMQ0LE2T8MT2Q1C/1-COVER%40300x.png 超伝導量子コンピュータ https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683816403666-C1MDXSC1LXY2ROISNYO4/2%40300x.png 超伝導量子コンピュータ https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683816404291-EZXBOSLIYZ6KZXQ95AVJ/3%40300x.png 超伝導量子コンピュータ https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683816404374-ZTMZO3IJ52T6RLOLAYJI/4%40300x.png 超伝導量子コンピュータ https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683816405038-2F2GKGX1KU5E2XR7XWIP/5%40300x.png 超伝導量子コンピュータ https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683816405075-UKD8WX2EZCH0166LP5UN/6%40300x.png 超伝導量子コンピュータ https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683816405840-HFJAVZWMQBODMNRNCAOM/7%40300x.png 超伝導量子コンピュータ https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683816405957-TRQE5LJ9MR3PNHTTEJ0S/8-BACK%40300x.png 超伝導量子コンピュータ https://www.epiqc.cs.uchicago.edu/trapped-ion-qcs-jpn daily 0.75 2023-05-15 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683819231578-5JT8GWKNCIZBH97N7IKX/1-COVER%40300x.png イオントラップ型量子コンピュータ https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683819231624-C3PNSLTE9U1P6JMKXUYC/2%40300x.png イオントラップ型量子コンピュータ https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683819232264-KKG8P7EM3YFEGN4K4D61/3%40300x.png イオントラップ型量子コンピュータ https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683819232386-NHAZGB6JMT7DRL0V49PJ/4%40300x.png イオントラップ型量子コンピュータ https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683819233078-CCN9VVAMD20EIJPQNM9O/5%40300x.png イオントラップ型量子コンピュータ https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683819233179-K90CU97BRJ96QOQ9YYII/6%40300x.png イオントラップ型量子コンピュータ https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683819233750-K293PAWSTTPQ33LZ45S3/7%40300x.png イオントラップ型量子コンピュータ https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1683819233882-UKX563VYHJQZKUF2OFB0/8-BACK%40300x.png イオントラップ型量子コンピュータ https://www.epiqc.cs.uchicago.edu/scaling-superconducting-quantum-computers daily 0.75 2023-06-05 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1c9344b2-1d3f-4bfc-9fff-db034e2af2e4/Scaling+Superconducting+Quantum+Computers.png Scaling Superconducting Quantum Computers - Make it stand out Infidelity and yield trade-off vs. individual QC module size in qubits https://www.epiqc.cs.uchicago.edu/navigating-dynamic-noise-in-vqa daily 0.75 2023-06-05 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/b499bd71-184f-4672-864f-2e7a374036bd/QISMET_Graph4.jpg Navigating Dynamic Noise in VQA - Make it stand out Optimal VQA convergence is obtained in the ideal noise-free scenario (orange). In reality, VQA is affected by static and transient noise, and estimates can be much worse than ideal (red). QISMET (green) attempts to avoid significant transient error and thereby reaches close to the otherwise unrealistic blue line with only static noise. Prior error miti- gation proposals can help bring the blue (and green) closer to the orange. https://www.epiqc.cs.uchicago.edu/btwc-decoding-for-error-correction daily 0.75 2023-06-05 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/89b3b1e6-a285-44f5-a2c5-6b600dbf261f/Clique_for_web.jpg BTWC Decoding for Error Correction - Make it stand out The Clique better-than-worst-case decoder reduces bandwidth and cryogenic resource bottlenecks for quantum error correction. https://www.epiqc.cs.uchicago.edu/clifford-ansatz-for-quantum-accuracy daily 0.75 2023-06-06 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/04d6527c-f598-4845-ae1f-0a91b615c21a/CAFQA_Scope2.jpg Clifford Ansatz For Quantum Accuracy - Make it stand out Clifford portion of the VQA space explored by CAFQA https://www.epiqc.cs.uchicago.edu/quantum-computing-for-everyone daily 0.75 2023-06-06 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/ba214cb1-6c60-44a1-ae12-795b16a06b1f/edx_graph.Liu.png Quantum Computing for Everyone - Make it stand out A graph of EdX Course Engagement, showing complete retention during the math portions of the course (Modules 4-5). https://www.epiqc.cs.uchicago.edu/noise-aware-training-of-vqc daily 0.75 2023-08-10 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/f00eaa41-108a-4fde-ab8a-1a634707c7dc/Screen+Shot+2023-08-10+at+2.23.20+PM.jpg Noise-aware Training of VQC - Make it stand out The three steps in the QuantumNAT framework. (1) Post-measurement normalization matches the distribution of measurement results between noise-free simulation and real QC. (2) Based on realistic noise models, noise-injection inserts quantum error gates to the training process to increase the classification margin between classes. (3) Measurement outcomes are further quantized for denoising. https://www.epiqc.cs.uchicago.edu/nonstandard-two-qubit-gates daily 0.75 2023-08-14 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/db0dcfac-3ce4-4a74-804a-0a523c2750d1/Nonstandard+two_qubit.gates.png Nonstandard two-qubit gates - Make it stand out The Weyl chamber helps visualize the space of two-qubit gates. The highlighted polygon in the middle represents the gates with high-entangling power. Two two-qubit gates are projected to the same point if only one-qubit gates are needed to convert between them. https://www.epiqc.cs.uchicago.edu/quantum-compiler-push-button-verification daily 0.75 2023-08-14 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/5b449340-5727-4caf-beda-9215707c4a6b/giallar_workflow_square.png Quantum Compiler Push-Button Verification - Make it stand out The workflow of Giallar to verify and execute quantum compiler passes. https://www.epiqc.cs.uchicago.edu/quancorde-boosting-quantum-fidelity-with-clifford-ensembles daily 0.75 2023-08-14 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/a21a42c3-8dc5-4cc1-bcc8-5f0cee80cd1f/Quancorde.jpg Quancorde: Boosting Quantum Fidelity with Clifford Ensembles - Make it stand out Quancorde overview: (1) A canary circuit for the target application is constructed by replacing the non-Clifford gates in the target (orange) with the nearest Clifford gates (green). (2) The target circuit is executed on the diverse noisy quantum ensemble R1-R5 (e.g., different machines or qubits/mappings). (3) In parallel, the canary is also executed on the same noisy ensemble. (4) The correct output of the canary is obtained by running it ideally (noise-free) on a classical machine - possible since Clifford circuits are efficiently classically simulable. (5) Since the correct canary outcome is known, the ensemble is ordered based on the noisy execution fidelity of the canary - R5<R4<R2<R3<R1. (6) The noisy distribution on any machine is selected as the baseline - the correct answer `11' has low probability. (7) Ensemble orderings are produced for the different noisy outputs (of non-negligible probability) of the original circuit and are compared with the canary ordering to estimate a correlation value for each output - `11' has a high correlation. (8) The correlations are then used to weight the baseline distribution to produce a new distribution in which the `11' probability is boosted to become the winner. https://www.epiqc.cs.uchicago.edu/quander daily 0.75 2023-08-14 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/98cfddd2-a956-4976-a9bf-baf3a2926790/QuanderLogo1.png Quander - Quander Games https://quander.cs.uchicago.edu https://www.epiqc.cs.uchicago.edu/qc-financial-times daily 0.75 2023-08-14 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/22033bfb-b1fb-4475-b854-7fb73677bf67/QC-FinTimes.png QC could break the internet - Quander Games https://quander.cs.uchicago.edu https://www.epiqc.cs.uchicago.edu/clifford-ansatz-for-quantum-accuracy-copy daily 0.75 2023-08-15 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/04d6527c-f598-4845-ae1f-0a91b615c21a/CAFQA_Scope2.jpg Clifford Ansatz For Quantum Accuracy - Make it stand out Clifford portion of the VQA space explored by CAFQA https://www.epiqc.cs.uchicago.edu/btwc-decoding-for-error-correction-copy daily 0.75 2023-08-15 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/89b3b1e6-a285-44f5-a2c5-6b600dbf261f/Clique_for_web.jpg BTWC Decoding for Error Correction (Copy) - Make it stand out The Clique better-than-worst-case decoder reduces bandwidth and cryogenic resource bottlenecks for quantum error correction. https://www.epiqc.cs.uchicago.edu/navigating-dynamic-noise-in-vqa-copy daily 0.75 2023-08-15 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/b499bd71-184f-4672-864f-2e7a374036bd/QISMET_Graph4.jpg Navigating Dynamic Noise in VQA (Copy) - Make it stand out Optimal VQA convergence is obtained in the ideal noise-free scenario (orange). In reality, VQA is affected by static and transient noise, and estimates can be much worse than ideal (red). QISMET (green) attempts to avoid significant transient error and thereby reaches close to the otherwise unrealistic blue line with only static noise. Prior error miti- gation proposals can help bring the blue (and green) closer to the orange. https://www.epiqc.cs.uchicago.edu/scaling-superconducting-quantum-computers-copy daily 0.75 2023-08-15 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1c9344b2-1d3f-4bfc-9fff-db034e2af2e4/Scaling+Superconducting+Quantum+Computers.png Scaling Superconducting Quantum Computers (Copy) - Make it stand out Infidelity and yield trade-off vs. individual QC module size in qubits https://www.epiqc.cs.uchicago.edu/quancorde-boosting-quantum-fidelity-with-clifford-ensembles-copy daily 0.75 2023-08-15 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/a21a42c3-8dc5-4cc1-bcc8-5f0cee80cd1f/Quancorde.jpg Quancorde: Boosting Quantum Fidelity with Clifford Ensembles (Copy) - Make it stand out Quancorde overview: (1) A canary circuit for the target application is constructed by replacing the non-Clifford gates in the target (orange) with the nearest Clifford gates (green). (2) The target circuit is executed on the diverse noisy quantum ensemble R1-R5 (e.g., different machines or qubits/mappings). (3) In parallel, the canary is also executed on the same noisy ensemble. (4) The correct output of the canary is obtained by running it ideally (noise-free) on a classical machine - possible since Clifford circuits are efficiently classically simulable. (5) Since the correct canary outcome is known, the ensemble is ordered based on the noisy execution fidelity of the canary - R5<R4<R2<R3<R1. (6) The noisy distribution on any machine is selected as the baseline - the correct answer `11' has low probability. (7) Ensemble orderings are produced for the different noisy outputs (of non-negligible probability) of the original circuit and are compared with the canary ordering to estimate a correlation value for each output - `11' has a high correlation. (8) The correlations are then used to weight the baseline distribution to produce a new distribution in which the `11' probability is boosted to become the winner. https://www.epiqc.cs.uchicago.edu/nonstandard-twoqubit-gates-copy daily 0.75 2023-08-15 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/db0dcfac-3ce4-4a74-804a-0a523c2750d1/Nonstandard+two_qubit.gates.png Nonstandard two-qubit gates (Copy) - Make it stand out The Weyl chamber helps visualize the space of two-qubit gates. The highlighted polygon in the middle represents the gates with high-entangling power. Two two-qubit gates are projected to the same point if only one-qubit gates are needed to convert between them. https://www.epiqc.cs.uchicago.edu/quantum-compiler-pushbutton-verification-copy daily 0.75 2023-08-15 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/5b449340-5727-4caf-beda-9215707c4a6b/giallar_workflow_square.png Quantum Compiler Push-Button Verification (Copy) - Make it stand out The workflow of Giallar to verify and execute quantum compiler passes. https://www.epiqc.cs.uchicago.edu/longdistance-interactions-copy daily 0.75 2023-08-15 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/1633539886682-XTKBHMQR0T05U9A0NKKZ/Baker.long.dist.neutral.png Long-Distance Interactions (Copy) Figures showing best performing codes and pseudothresholds for different error models and sets of codes. In (a,b,c) we are comparing codes in the set {Surface-17, Bacon-Shor-13, Shor-6X2Z, Shor-6Z2X}, while in (d,e,f) we restrict our set to only consider codes with a transversal Hadamard gate, {Surface-17, Bacon-Shor-13}. In (a,d) we look at the intersection of overrotation error (parameterized by the two qubit gate error) and T2 dephasing, in (b,e) we look at overrotation and crosstalk, and in (c,f) we look at T2 dephasing and crosstalk with a background overrotation characterized by a Mølmer-Sørensen error rate of 10−4 . The colored regions indicate which code is optimal at those error parameters, with darker shading implying the code is outperforming a physical CNOT. The colored curves are the pseudothreshold curves for which the logical error rate is equal to the physical error rate in Eq. 5 and the black curves are borders between regions in which different codes are preferred. https://www.epiqc.cs.uchicago.edu/training-quantum-boltzmann-machines-with-coresets daily 0.75 2023-08-16 https://images.squarespace-cdn.com/content/v1/5a56fca2c027d8a33aa5c48f/7edfec71-6cb3-4b36-99ea-dee8c7bd6c39/qbm.jpg Training Quantum Boltzmann Machines with Coresets Figures showing best performing codes and pseudothresholds for different error models and sets of codes. In (a,b,c) we are comparing codes in the set {Surface-17, Bacon-Shor-13, Shor-6X2Z, Shor-6Z2X}, while in (d,e,f) we restrict our set to only consider codes with a transversal Hadamard gate, {Surface-17, Bacon-Shor-13}. In (a,d) we look at the intersection of overrotation error (parameterized by the two qubit gate error) and T2 dephasing, in (b,e) we look at overrotation and crosstalk, and in (c,f) we look at T2 dephasing and crosstalk with a background overrotation characterized by a Mølmer-Sørensen error rate of 10−4 . The colored regions indicate which code is optimal at those error parameters, with darker shading implying the code is outperforming a physical CNOT. 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