Room-Temperature Quantum Sensing in CMOS: On-Chip Detection of Electronic Spin States in Diamond Color Centers for Magnetometry
|
|
- Nancy Bryan
- 5 years ago
- Views:
Transcription
1 Room-Temperature Quantum Sensing in CMOS: On-Chip Detection of Electronic Spin States in Diamond Color Centers for Magnetometry Mohamed I. Ibrahim*, Christopher Foy*, Donggyu Kim*, Dirk R. Englund, and Ruonan Han *Equal Contribution Massachusetts Institute of Technology
2 Introduction CMOS-Based Quantum Magnetometer System Architecture Microwave Signal Generation Optical Excitation Filtering Optical Fluorescence Readout Experimental Data Measurement Results Using Layer of Nano-Diamonds Measurement Results Using Bulk Diamond Conclusion Outline Slide 1
3 Nitrogen Vacancy (NV) in Diamond Magnetometer Nitrogen vacancy center in diamond Optically detected magnetic resonance (ODMR) Slide 2
4 Nitrogen Vacancy (NV) in Diamond Magnetometer nt/ Hz Ensemble of NVs Clevenson, et al. Nature Physics 2015 Clevenson, et al. Nature Physics 2015 Sensitivity Where N is number of NVs Slide 3
5 Nitrogen Vacancy (NV) in Diamond Magnetometer Magnetic structure imaging Balasubramanian, et al. Nature (2008) Bacteria magnetic imaging Le Sage, et al. Nature 2013 Nano-tesla sensitivity Nanometer spatial resolution Vector field measurements Ambient conditions (room temperature) Slide 4
6 NV Magnetometer System Components Green Laser Signal generator Photodetector Microwave antenna CMOS integrated NV magnetometer (TSMC 65nm Le Sage, LP et process) al. Nature 2013 Optical filters Slide 5
7 Introduction CMOS Based Quantum Magnetometer System Architecture Microwave Signal Generation Optical Excitation Filtering Optical Fluorescence Readout Experimental Results Measurement Results Using Layer of Nano-Diamonds Measurement Results Using Bulk Diamond Conclusion Outline Slide 6
8 CMOS Based Quantum Magnetometer Slide 7
9 Microwave Signal Generation 2.87 GHz microwave signal generation 2.6 GHz 3.1 GHz for optically detected magnetic resonance (ODMR) measurements 10 Gauss field strength at 2.87 GHz with 95% homogeneity To increase the contrast To drive the NVs with equal strength for spin control pulsed sequences (Echo, Ramsey,..) Slide 8
10 Microwave Signal Generation Microwave Coil B z = B 0 1 π Q E k 1 α2 β 2 + K k Q 4α α =, β =, k =, r = x + y and Q = 1 + a + β ma is required to get 10 Gauss for diameter coil Slide 9
11 Microwave Signal Generation Microwave Coil Slide 10
12 Microwave Signal Generation Microwave Coil EM simulated performance Slide 11
13 Microwave Signal Generation 10 Gauss with 95% uniformity 6 ma DC current in the driver 25x field strength more than simple non-resonant loop 2.6 GHz-3.1 GHz Microwave frequency sweep Slide 12
14 Optical Spin Readout Optical filter is required for green light rejection Photodiode is used to detect red fluorescence Slide 13
15 Optical Excitation Filtering Plasmonic Filter Green light (532 nm) Filter 3D structure 800 nm Red light (700 nm) Filter cross section 900 nm Measured isolation is 10 db FDTD simulated performance Slide 14
16 Optical Fluorescence Readout P+ N-well Photo-diode P Eddy L L diode P Eddy 4 Cuts the losses in anode and cathode n n diode P Eddy L3 n L 3 Measured responsivity is 0.23 A/W Slide 15
17 Introduction CMOS Based Quantum Magnetometer System Architecture Microwave Signal Generation Optical Excitation Filtering Optical Fluorescence Readout Experimental Results Measurement Results Using Layer of Nano-Diamonds Measurement Results Using Bulk Diamond Conclusion Outline Slide 16
18 Passivation Layer Removal Background fluorescence is emitted from the passivation (silicon nitrite) layer Reactive ion etching (RIE) for passivation layer removal 250 µm 250 µm Fluorescence Intensity Fluorescence Intensity Before etching After etching Slide 17
19 Nano-Diamonds Deposition Deposition of diamond nano-crystals solution 250 µm 250 µm Before deposition After deposition & evaporation Slide 18
20 Nano-Diamonds Measurement Results Sensitivity: CW where γ = 1 σδν γ C = 2.8 MHz/Gauss, σ Std. dev., Δν Linewidth, C Contrast, t Integration Time Slide 19
21 Bulk Diamond Measurement Results Sensitivity: CW where γ = 1 σ γ m = 2.8 MHz/Gauss, σ Std. dev., m, t Integration Time Slide 20
22 Bulk Diamond Measurement Results Slide 21
23 Introduction CMOS Based Quantum Magnetometer System Architecture Microwave Signal Generation Optical Excitation Filtering Optical Fluorescence Readout Experimental Results Measurement Results Using Layer of Nano-Diamonds Measurement Results Using Bulk Diamond Conclusion Outline Slide 22
24 Performance Summary Technology Vector meas. Optical isolation Sensing area Form factor Sensitivity This work (Nanodiamonds) 65nm CMOS No 10 db 50 μm 50 μm ~ 1 3 ** 73 μt Hz This work (Bulk Diamond) 65nm CMOS Yes 20 db 50 μm 50 μm ~ 1 3 ** 2.5 μt Hz Nature physics (2015) * Discrete devices Yes >60 db 1 mm 1mm ~ nt Hz *Clevenson, et al. Nature Physics 2015 ** Does not include LASER Slide 23
25 Conclusion Combines the advantages of CMOS and NV center in diamond in a small form factor Couples tightly the CMOS components with NV qubits Offers on-chip spin state readout Easy integration of control logic Less IOs Closed-loop feedback between spin-manipulation and readout Enables compact and scalable advanced quantum systems. Slide 24
Nitrogen-Vacancy Centers in Diamond A solid-state defect with applications from nanoscale-mri to quantum computing
Nitrogen-Vacancy Centers in Diamond A solid-state defect with applications from nanoscale-mri to quantum computing Research into nitrogen-vacancy centers in diamond has exploded in the last decade (see
More informationPhotoelectric readout of electron spin qubits in diamond at room temperature
Photoelectric readout of electron spin qubits in diamond at room temperature. Bourgeois,, M. Gulka, J. Hruby, M. Nesladek, Institute for Materials Research (IMO), Hasselt University, Belgium IMOMC division,
More informationMIT Department of Nuclear Science & Engineering
1 MIT Department of Nuclear Science & Engineering Thesis Prospectus for the Bachelor of Science Degree in Nuclear Science and Engineering Nicolas Lopez Development of a Nanoscale Magnetometer Through Utilization
More informationQuantum control of proximal spins using nanoscale magnetic resonance imaging
Quantum control of proximal spins using nanoscale magnetic resonance imaging M. S. Grinolds, P. Maletinsky, S. Hong, M. D. Lukin, R. L. Walsworth and A. Yacoby Nature Physics vol 7 (5) pp.1-6, 2011 DOI:
More informationMagnetic Resonance in Quantum Information
Magnetic Resonance in Quantum Information Christian Degen Spin Physics and Imaging group Laboratory for Solid State Physics www.spin.ethz.ch Content Features of (nuclear) magnetic resonance Brief History
More informationQuantum manipulation of NV centers in diamond
Quantum manipulation of NV centers in diamond 12.09.2014 The University of Virginia Physics Colloquium Alex Retzker Jianming Cai, Andreas Albrect, M. B. Plenio,Fedor Jelezko, P. London, R. Fisher,B. Nayedonov,
More informationUltra-High-Sensitivity emiccd Cameras Enable Diamond Quantum Dynamics Research
2015 Princeton Instruments, Inc. All rights reserved. Ultra-High-Sensitivity emiccd Cameras Enable Diamond Quantum Dynamics Research The PI-MAX4:512EM emiccd camera deliver[s] quantitative, ultra-high-sensitivity
More informationPrecision sensing using quantum defects
Precision sensing using quantum defects Sang-Yun Lee 3rd Institute of Physics, University of Stuttgart, Germany Quantum and Nano Control, IMA at University of Minnesota April 14, 2016 Single spin probes
More informationConfocal Microscope Imaging of Single-Emitter Fluorescence and Photon Antibunching
Confocal Microscope Imaging of Single-Emitter Fluorescence and Photon Antibunching By Dilyana Mihaylova Abstract The purpose of this lab is to study different types of single emitters including quantum
More informationarxiv: v2 [cond-mat.mes-hall] 24 Jan 2011
Coherence of nitrogen-vacancy electronic spin ensembles in diamond arxiv:006.49v [cond-mat.mes-hall] 4 Jan 0 P. L. Stanwix,, L. M. Pham, J. R. Maze, 4, 5 D. Le Sage, T. K. Yeung, P. Cappellaro, 6 P. R.
More informationLecture 18 Luminescence Centers
Lecture 18 Luminescence Centers Read: FS9 (Al2O3 sapphire with different colors) Purdue University Spring 2016 Prof. Yong P. Chen (yongchen@purdue.edu) Lecture 18 (3/24/2016) Slide 1 Basic physics: Vibronic
More informationCMSC 33001: Novel Computing Architectures and Technologies. Lecture 06: Trapped Ion Quantum Computing. October 8, 2018
CMSC 33001: Novel Computing Architectures and Technologies Lecturer: Kevin Gui Scribe: Kevin Gui Lecture 06: Trapped Ion Quantum Computing October 8, 2018 1 Introduction Trapped ion is one of the physical
More informationMagnetic Resonance in Quantum
Magnetic Resonance in Quantum Information Christian Degen Spin Physics and Imaging group Laboratory for Solid State Physics www.spin.ethz.ch Content Features of (nuclear) magnetic resonance Brief History
More informationHyperfine Interaction Estimation of Nitrogen Vacancy Center in Diamond
Hyperfine Interaction Estimation of Nitrogen Vacancy Center in Diamond Yutaka Shikano Massachusetts Institute of Technology Tokyo Institute of Technology In collaboration with Shu Tanaka (Kinki University,
More informationTowards quantum simulator based on nuclear spins at room temperature
Towards quantum simulator based on nuclear spins at room temperature B. Naydenov and F. Jelezko C. Müller, Xi Kong, T. Unden, L. McGuinness J.-M. Cai and M.B. Plenio Institute of Theoretical Physics, Uni
More informationQuantum Information NV Centers in Diamond General Introduction. Zlatko Minev & Nate Earnest April 2011
Quantum Information NV Centers in Diamond General Introduction Zlatko Minev & Nate Earnest April 2011 QIP & QM & NVD Outline Interest in Qubits. Why? Quantum Information Motivation Qubit vs Bit Sqrt(Not)
More informationHybrid Quantum Circuit with a Superconducting Qubit coupled to a Spin Ensemble
Hybrid Quantum Circuit with a Superconducting Qubit coupled to a Spin Ensemble, Cécile GREZES, Andreas DEWES, Denis VION, Daniel ESTEVE, & Patrice BERTET Quantronics Group, SPEC, CEA- Saclay Collaborating
More informationSupplementary Figure 1: Determination of the ratio between laser photons and photons from an ensemble of SiV - centres under Resonance Fluorescence.
Supplementary Figure 1: Determination of the ratio between laser photons and photons from an ensemble of SiV - centres under Resonance Fluorescence. a To determine the luminescence intensity in each transition
More informationOptical Magnetometry Using Nitrogen-Vacancy Centers
Optical Magnetometry Using Nitrogen-Vacancy Centers Michael Onyszczak Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, U.S.A. Submitted: August 18, 2017 Revised: October 19,
More informationOptically Detected Magnetic Resonance Imaging. Technology, 32000, Haifa, Israel
Optically Detected Magnetic Resonance Imaging Aharon Blank, * Guy Shapiro, + Ran Fischer, + Paz London, + and David Gershoni + * Schulich Faculty of Chemistry, Technion- Israel Institute of Technology,
More information1 Ioffe Physical-Technical Institute, St. Petersburg, Russia
Point defects in SiC as a promising basis for single-defect, singlephoton spectroscopy with room temperature controllable quantum states Pavel G. Baranov 1, a, Victor A. Soltamov 1, Alexandra A.Soltamova
More informationSingle-photon NV sources. Pauli Kehayias March 16, 2011
Single-photon NV sources 1 Outline Quantum nature of light Photon correlation functions Single-photon sources NV diamond single-photon sources 2 Wave/particle duality Light exhibits wave and particle properties
More informationElements of magnetism and magnetic measurements
Elements of magnetism and magnetic measurements Ruslan Prozorov Oct 2009, Feb 2014, Oct 2018 Physics 590B magnetic moment of free currents Magnetic moment of a closed loop carrying current I: Magnetic
More informationNuclear spin control in diamond. Lily Childress Bates College
Nuclear spin control in diamond Lily Childress Bates College nanomri 2010 Hyperfine structure of the NV center: Excited state? Ground state m s = ±1 m s = 0 H = S + gµ S 2 z B z r s r r + S A N I N + S
More informationQuantum technologies based on nitrogen-vacancy centers in diamond: towards applications in (quantum) biology
Quantum technologies based on nitrogen-vacancy centers in diamond: towards applications in (quantum) biology 3 E 532 nm 1 2δω 1 Δ ESR 0 1 A 1 3 A 2 Microwaves 532 nm polarization Pulse sequence detection
More informationSupplemental Material. Electron spin contrast of Purcell-enhanced nitrogen-vacancy ensembles in nanodiamonds
Supplemental Material for Electron spin contrast of Purcell-enhanced nitrogen-vacancy ensembles in nanodiamonds 1. Sample preparation The 200-nm thick TiN films used in this work were grown on c-sapphire
More informationSuperconducting Qubits Lecture 4
Superconducting Qubits Lecture 4 Non-Resonant Coupling for Qubit Readout A. Blais, R.-S. Huang, A. Wallraff, S. M. Girvin, and R. J. Schoelkopf, PRA 69, 062320 (2004) Measurement Technique Dispersive Shift
More informationarxiv: v1 [quant-ph] 12 Nov 2012
Dressed-State Polarization Transfer between Bright & Dark Spins in Diamond C. Belthangady 1,2, N. Bar-Gill 1,2, L. M. Pham 3, K. Arai 4, D. Le Sage 1,2, P. Cappellaro 5, and R. L. Walsworth 1,2 1 Harvard-Smithsonian
More informationSide resonances and metastable excited state of NV - center in diamond
Side resonances and metastable excited state of NV - center in diamond Alexander Ivanov 1 and Alexei Ivanov 1 1 Immanuel Kant Baltic Federal University, Nevskogo 14, 236041 Kaliningrad, Russia. aivanov023@gmail.com,
More informationREPORT DOCUMENTATION PAGE Form Approved OMB NO
REPORT DOCUMENTATION PAGE Form Approved OMB NO. 0704-0188 The public reporting burden for this collection of information is estimated to average 1 hour per response, including the time for reviewing instructions,
More informationSupplemental Material to the Manuscript Radio frequency magnetometry using a single electron spin
Supplemental Material to the Manuscript Radio frequency magnetometry using a single electron spin M. Loretz, T. Rosskopf, C. L. Degen Department of Physics, ETH Zurich, Schafmattstrasse 6, 8093 Zurich,
More informationMicromechanical Instruments for Ferromagnetic Measurements
Micromechanical Instruments for Ferromagnetic Measurements John Moreland NIST 325 Broadway, Boulder, CO, 80305 Phone:+1-303-497-3641 FAX: +1-303-497-3725 E-mail: moreland@boulder.nist.gov Presented at
More informationElectron spin qubits in P donors in Silicon
Electron spin qubits in P donors in Silicon IDEA League lectures on Quantum Information Processing 7 September 2015 Lieven Vandersypen http://vandersypenlab.tudelft.nl Slides with black background courtesy
More informationSurvey on Laser Spectroscopic Techniques for Condensed Matter
Survey on Laser Spectroscopic Techniques for Condensed Matter Coherent Radiation Sources for Small Laboratories CW: Tunability: IR Visible Linewidth: 1 Hz Power: μw 10W Pulsed: Tunabality: THz Soft X-ray
More informationEnergy transport in metal nanoparticle plasmon waveguides
Energy transport in metal nanoparticle plasmon waveguides Stefan A. Maier, Pieter G. Kik, and Harry A. Atwater California Institute of Technology Thomas J. Watson Laboratory of Applied Physics, Pasadena,
More informationSeries CCR-39S Multi-Throw DC-12 GHz, SP9T & SP10T Latching Coaxial Switch
PART NUMBER CCR-39S DESCRIPTION Commercial Latching Multi-throw, DC-12GHz The CCR-39Sis a broadband, multi-throw, electromechanical coaxial switch designed to switch a microwave signal from a common input
More informationThree-dimensional solid-state qubit arrays with long-lived spin coherence
Three-dimensional solid-state qubit arrays with long-lived spin coherence C.J. Stephen 1, B.L. Green 1, Y.N.D. Lekhai 1, L. Weng 2, P. Hill 3,4, S. Johnson 2, A.C. Frangeskou 1, P.L. Diggle 1,4, M.J. Strain
More informationExperimental Quantum Computing: A technology overview
Experimental Quantum Computing: A technology overview Dr. Suzanne Gildert Condensed Matter Physics Research (Quantum Devices Group) University of Birmingham, UK 15/02/10 Models of quantum computation Implementations
More informationMagnetic Resonance with Single Nuclear-Spin Sensitivity. Alex Sushkov
1 Magnetic Resonance with Single Nuclear-Spin Sensitivity Alex Sushkov 2 MRI scanner $2 million 7 tons 1500 liters of He 3 4 5 µm magnetic force microscopy (MFM) image of hard drive surface topological
More informationSingle Photon Generation & Application
Single Photon Generation & Application Photon Pair Generation: Parametric down conversion is a non-linear process, where a wave impinging on a nonlinear crystal creates two new light beams obeying energy
More informationOptical determination and magnetic manipulation of single nitrogen-vacancy color center in diamond nanocrystal
Optical determination and magnetic manipulation of single nitrogen-vacancy color center in diamond nanocrystal Ngoc Diep Lai, Dingwei Zheng, François Treussart, Jean-François Roch To cite this version:
More informationSUPPLEMENTARY INFORMATION
SUPPLEMENTARY INFORMATION doi: 10.1038/nnano.2011.64 Quantum measurement and orientation tracking of fluorescent nanodiamonds inside living cells L. P. McGuinness, Y. Yan, A. Stacey, D. A. Simpson, L.
More informationOptogalvanic spectroscopy of the Zeeman effect in xenon
Optogalvanic spectroscopy of the Zeeman effect in xenon Timothy B. Smith, Bailo B. Ngom, and Alec D. Gallimore ICOPS-2006 10:45, 5 Jun 06 Executive summary What are we reporting? Xe I optogalvanic spectra
More informationTowards quantum metrology with N00N states enabled by ensemble-cavity interaction. Massachusetts Institute of Technology
Towards quantum metrology with N00N states enabled by ensemble-cavity interaction Hao Zhang Monika Schleier-Smith Robert McConnell Jiazhong Hu Vladan Vuletic Massachusetts Institute of Technology MIT-Harvard
More informationBuilding Blocks for Quantum Computing Part IV. Design and Construction of the Trapped Ion Quantum Computer (TIQC)
Building Blocks for Quantum Computing Part IV Design and Construction of the Trapped Ion Quantum Computer (TIQC) CSC801 Seminar on Quantum Computing Spring 2018 1 Goal Is To Understand The Principles And
More informationDiamond Sensors for Brain Imaging
Revolutions in Biotechnology Diamond Sensors for Brain Imaging This material is based upon work supported by the Assistant Secretary of Defense for Research and Engineering under Air Force ontract No.
More informationContactless Excitation of MEMS Resonant Sensors by Electromagnetic Driving
Presented at the COMSOL Conference 2009 Milan University of Brescia Department of Electronics for Automation Contactless Excitation of MEMS Resonant Sensors by Electromagnetic Driving Marco Baù, VF V.
More informationresonances in diamond
Enhanced dual-beam excitation photoelectric detection of NV magnetic resonances in diamond E. Bourgeois a,b, E. Londero c, K. Buczak d, Y. Balasubramaniam b, G. Wachter d, J. Stursa e, K. Dobes f, F. Aumayr
More informationNanoscale magnetic imaging with single spins in diamond
Nanoscale magnetic imaging with single spins in diamond Ania Bleszynski Jayich UC Santa Barbara Physics AFOSR Nanoelectronics Review Oct 24, 2016 Single spin scanning magnetometer Variable temperature
More informationSeries CCT-58S Multi-Throw DC 18 GHz, SP7T & SP8T Normally Open Coaxial Switch
PART NUMBER CCT-58S DESCRIPTION Commercial Normally Open Multi-throw, DC-18 GHz The CCT-58S/CT-58S is an internally terminated, broadband, multi-throw, electromechanical coaxial switch designed to switch
More informationSeries CCR-39S Multi-Throw DC-12 GHz, SP9T & SP10T Latching Coaxial Switch
COAX SWITCHES Series CCR-39S PART NUMBER CCR-39S DESCRIPTION Commercial Latching Multi-throw, DC-12GHz The CCR-39Sis a broadband, multi-throw, electromechanical coaxial switch designed to switch a microwave
More informationFrequency Tunable Atomic Magnetometer based on an Atom Interferometer
Frequency Tunable Atomic Magnetometer based on an Atom Interferometer D.A. Braje 1, J.P. Davis 2, C.L. Adler 2,3, and F.A. Narducci 2 Blaubeuren Quantum Optics Summer School 29 July 2013 1 MIT Lincoln
More informationLinear and nonlinear spectroscopy
Linear and nonlinear spectroscopy We ve seen that we can determine molecular frequencies and dephasing rates (for electronic, vibrational, or spin degrees of freedom) from frequency-domain or timedomain
More informationMagnetic Field measurements with Csmagnetometers
Magnetic Field measurements with Csmagnetometers in nedm project at PSI A.Pazgalev *, M.Cvijovic, P.Knowles, and A.Weis FRAP, Fribourg University, CH-1700 FRIOURG * on leave from IOFFE Phys.-Tech. Instit.,
More informationLaboratory 3: Confocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown, and Twiss Setup for Photon Antibunching
Laboratory 3: Confocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown, and Twiss Setup for Photon Antibunching Jonathan Papa 1, * 1 Institute of Optics University of Rochester, Rochester,
More informationImage courtesy of Keith Schwab http://www.lbl.gov/science-articles/archive/afrd Articles/Archive/AFRD-quantum-logic.html http://www.wmi.badw.de/sfb631/tps/dqd2.gif http://qist.lanl.gov/qcomp_map.shtml
More informationSiletz APD Products. Model VFP1-xCAA, VFP1-xKAB Packaged APDs
Siletz Packaged APD Features Hermetically packaged reduced-noise NIR InGaAs avalanche photodiode (R-APD) Siletz APD Products Single-Carrier Multiplication APDs (SCM-APD) in hermetic packages with optional
More informationSeries CCR-39S Multi-Throw DC-12 GHz, SP7T & SP8T Latching Coaxial Switch
PART NUMBER CCR-39S DESCRIPTION Commercial Latching Multi-throw, DC-12GHz The CCR-39S is a broadband, multi-throw, electromechanical coaxial switch designed to switch a microwave signal from a common input
More informationarxiv: v1 [quant-ph] 17 Mar 2016
Review Article: Quantum Nanophotonics in Diamond arxiv:1603.05339v1 [quant-ph] 17 Mar 2016 Tim Schröder, 1 Sara Mouradian, 1 Jiabao Zheng, 1, 2 Matthew E. Trusheim, 1 Michael Walsh, 1 Edward H. Chen, 1
More informationPulsed photoelectric coherent manipulation and detection of NV centre spins in diamond
Pulsed photoelectric coherent manipulation and detection of NV centre spins in diamond Michal Gulka a,b, Emilie Bourgeois a,c, Jaroslav Hruby a, Petr Siyushev d, Georg Wachter e, Friedrich Aumayr f, Philip
More informationExcited-state spectroscopy of single NV defect in diamond using optically detected magnetic resonance arxiv: v2 [quant-ph] 10 Feb 2009
Excited-state spectroscopy of single NV defect in diamond using optically detected magnetic resonance arxiv:0807.2379v2 [quant-ph] 10 Feb 2009 P Neumann 1, R Kolesov 1, V Jacques 1, J Beck 1, J Tisler
More informationEnhanced Single Photon Emission from a Diamond-Silver Aperture
Enhanced Single Photon Emission from a Diamond-Silver Aperture Jennifer T. Choy 1*, Birgit J. M. Hausmann 1*, Thomas M. Babinec 1*, Irfan Bulu 1*, Mughees Khan 2, Patrick Maletinsky 3, Amir Yacoby 3, Marko
More informationQuantum Logic Spectroscopy and Precision Measurements
Quantum Logic Spectroscopy and Precision Measurements Piet O. Schmidt PTB Braunschweig and Leibniz Universität Hannover Bad Honnef, 4. November 2009 Overview What is Quantum Metrology? Quantum Logic with
More informationQuantum error correction on a hybrid spin system. Christoph Fischer, Andrea Rocchetto
Quantum error correction on a hybrid spin system Christoph Fischer, Andrea Rocchetto Christoph Fischer, Andrea Rocchetto 17/05/14 1 Outline Error correction: why we need it, how it works Experimental realization
More informationCircuit Quantum Electrodynamics. Mark David Jenkins Martes cúantico, February 25th, 2014
Circuit Quantum Electrodynamics Mark David Jenkins Martes cúantico, February 25th, 2014 Introduction Theory details Strong coupling experiment Cavity quantum electrodynamics for superconducting electrical
More informationShallow Donors in Silicon as Electron and Nuclear Spin Qubits Johan van Tol National High Magnetic Field Lab Florida State University
Shallow Donors in Silicon as Electron and Nuclear Spin Qubits Johan van Tol National High Magnetic Field Lab Florida State University Overview Electronics The end of Moore s law? Quantum computing Spin
More informationFriday, April 24, Hybrid approaches to quantum information science
Hybrid approaches to quantum information science Challenge of simultaneous isolation and control of many-body system Challenge of simultaneous isolation and control of many-body system Photons: leading
More informationElectron Spin Echo and Coherence Times. in Silicon Carbide Defects. Kyle G. Miller
Electron Spin Echo and Coherence Times in Silicon Carbide Defects Kyle G. Miller A senior thesis submitted to the faculty of Brigham Young University in partial fulfillment of the requirements for the
More informationLaboratory 3&4: Confocal Microscopy Imaging of Single-Emitter Fluorescence and Hanbury Brown and Twiss setup for Photon Antibunching
Laboratory 3&4: Confocal Microscopy Imaging of Single-Emitter Fluorescence and Hanbury Brown and Twiss setup for Photon Antibunching Jose Alejandro Graniel Institute of Optics University of Rochester,
More informationImplantation of labelled single nitrogen vacancy centers in diamond using 15 N
Implantation of labelled single nitrogen vacancy centers in diamond using 15 N J. R. Rabeau *, P. Reichart School of Physics, Microanalytical Research Centre, The University of Melbourne, Parkville, Victoria
More informationQuantum Computation with Neutral Atoms Lectures 14-15
Quantum Computation with Neutral Atoms Lectures 14-15 15 Marianna Safronova Department of Physics and Astronomy Back to the real world: What do we need to build a quantum computer? Qubits which retain
More informationUltrafast solid-state quantum optics
Ultrafast solid-state quantum optics Department of Physics and Center for Applied Photonics (CAP) Rudolf Bratschitsch University of Konstanz, Germany Outline Solid-state systems for quantum optics Semiconductor
More informationOPTICAL GAIN AND LASERS
OPTICAL GAIN AND LASERS 01-02-1 BY DAVID ROCKWELL DIRECTOR, RESEARCH & DEVELOPMENT fsona COMMUNICATIONS MARCH 6, 2001 OUTLINE 01-02-2 I. DEFINITIONS, BASIC CONCEPTS II. III. IV. OPTICAL GAIN AND ABSORPTION
More informationQuantum gates in rare-earth-ion doped crystals
Quantum gates in rare-earth-ion doped crystals Atia Amari, Brian Julsgaard Stefan Kröll, Lars Rippe Andreas Walther, Yan Ying Knut och Alice Wallenbergs Stiftelse Outline Rare-earth-ion doped crystals
More informationMultipath Interferometer on an AtomChip. Francesco Saverio Cataliotti
Multipath Interferometer on an AtomChip Francesco Saverio Cataliotti Outlook Bose-Einstein condensates on a microchip Atom Interferometry Multipath Interferometry on an AtomChip Results and Conclusions
More informationCMOS compatible integrated ferroelectric tunnel junctions (FTJ)
CMOS compatible integrated ferroelectric tunnel junctions (FTJ) Mohammad Abuwasib 1*, Hyungwoo Lee 2, Chang-Beom Eom 2, Alexei Gruverman 3, Jonathan Bird 1 and Uttam Singisetti 1 1 Electrical Engineering,
More informationError Corrected Spin-State Readout in a Nanodiamond
Error Corrected Spin-State Readout in a Nanodiamond Jeffrey Holzgrafe 1,2, *, Jan Beitner 1, *, Dhiren Kara 1, Helena S. Knowles 1,3, and Mete Atatüre 1, 1 Cavendish Laboratory, University of Cambridge,
More informationOptical Properties of CdSe Colloidal Quantum Dots and NV-Nanodiamonds
Optical Properties of CdSe Colloidal Quantum Dots and NV-Nanodiamonds James MacNeil and Madhu Ashok University of Rochester The Institute of Optics Submitted to Dr. Svetlana Lukishova on 11/20/2013 Abstract:
More informationBecause light behaves like a wave, we can describe it in one of two ways by its wavelength or by its frequency.
Light We can use different terms to describe light: Color Wavelength Frequency Light is composed of electromagnetic waves that travel through some medium. The properties of the medium determine how light
More informationElectron Spin Coherence in Silicon Vacancy Defects of. Proton-irradiated Silicon Carbide. Jacob Steven Embley
Electron Spin Coherence in Silicon Vacancy Defects of Proton-irradiated Silicon Carbide Jacob Steven Embley A senior thesis submitted to the faculty of Brigham Young University in partial fulfillment of
More informationCantilever enhanced tunable diode laser photoacoustic spectroscopy in gas purity measurement case study: acetylene in ethylene
Cantilever enhanced tunable diode laser photoacoustic spectroscopy in gas purity measurement case study: acetylene in ethylene Juho Uotila, Jussi Raittila, Ismo Kauppinen ¹Gasera Ltd., Tykistökatu 4, 20520
More informationКвантовые цепи и кубиты
Квантовые цепи и кубиты Твердотельные наноструктуры и устройства для квантовых вычислений Лекция 2 А.В. Устинов Karlsruhe Institute of Technology, Germany Russian Quantum Center, Russia Trapped ions Degree
More informationA Miniature Cold-Atom Frequency Standard
A Miniature Cold-Atom Frequency Standard 1 V.Shah, 2 M. Mescher, 2 R. Stoner, 3 V. Vuletic, 1 R. Lutwak 1 Symmetricom Technology Realization Centre, Beverly, MA, 01915 2 The Charles Stark Draper Laboratory,
More informationMagnetometry of random AC magnetic fields using a single Nitrogen- Vacancy center
Magnetometry of random AC magnetic fields using a single Nitrogen- Vacancy center Abdelghani Laraoui 1, Jonathan S. Hodges 2, Carlos A. Meriles 1 1 Department of Physics, City College of New York CUNY,
More informationLab 3 and 4: Single Photon Source
Lab 3 and 4: Single Photon Source By: Justin Deuro, December 10 th, 2009 Abstract We study methods of single photon emission by exciting single colloidal quantum dot (QD) samples. We prepare the single
More informationMartes cuántico Zaragoza, 8 th October Atomic and molecular spin qubits. Fernando LUIS Instituto de Ciencia de Materiales de Aragón
Martes cuántico Zaragoza, 8 th October 2013 Atomic and molecular spin qubits Fernando LUIS Instituto de Ciencia de Materiales de Aragón Outline Quantum information with spins 1 0 Atomic defects in semiconductors
More informationProbing Surface Spin Interaction Dynamics using Nitrogen-Vacancy Center Quantum Sensors with High-Fidelity State-Selective Transition Control
Probing Surface Spin Interaction Dynamics using Nitrogen-Vacancy Center Quantum Sensors with High-Fidelity State-Selective Transition Control by Zimeng Wang A thesis presented to the University of Waterloo
More informationConfocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown and Twiss Photon Antibunching Setup
1 Confocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown and Twiss Photon Antibunching Setup Abstract Jacob Begis The purpose of this lab was to prove that a source of light can be
More informationMagnetic and optic sensing. Magnetic sensors
Magnetic and optic sensing Magnetic sensors 1 Literature Physics of Semiconductor Devices S.M. Sze, Kwok K. Ng Available as ebook on http://www.lub.lu.se/en/search/lubsearch.ht ml This lecture chapters
More informationCoherent Control of a Single Electron Spin with Electric Fields
Coherent Control of a Single Electron Spin with Electric Fields Presented by Charulata Barge Graduate student Zumbühl Group Department of Physics, University of Basel Date:- 9-11-2007 Friday Group Meeting
More informationScanning Tunneling Microscopy
Scanning Tunneling Microscopy References: 1. G. Binnig, H. Rohrer, C. Gerber, and Weibel, Phys. Rev. Lett. 49, 57 (1982); and ibid 50, 120 (1983). 2. J. Chen, Introduction to Scanning Tunneling Microscopy,
More informationReference literature. (See: CHEM 2470 notes, Module 8 Textbook 6th ed., Chapters )
September 17, 2018 Reference literature (See: CHEM 2470 notes, Module 8 Textbook 6th ed., Chapters 13-14 ) Reference.: https://slideplayer.com/slide/8354408/ Spectroscopy Usual Wavelength Type of Quantum
More informationManipulating Single Atoms
Manipulating Single Atoms MESUMA 2004 Dresden, 14.10.2004, 09:45 Universität Bonn D. Meschede Institut für Angewandte Physik Overview 1. A Deterministic Source of Single Neutral Atoms 2. Inverting MRI
More informationQuantum Informa,on with NV- Centers (QINVC)
Quantum Informa,on with NV- Centers (QINVC) Jan Meijer (Uni Leipzig) Coopera,on between CEA Saclay France, ENS Cachan France, University StuKgart Germany, University Leipzig Germany, University Warwick
More informationElectron spin coherence exceeding seconds in high-purity silicon
Electron spin coherence exceeding seconds in high-purity silicon Alexei M. Tyryshkin, Shinichi Tojo 2, John J. L. Morton 3, H. Riemann 4, N.V. Abrosimov 4, P. Becker 5, H.-J. Pohl 6, Thomas Schenkel 7,
More informationDielectric Meta-Reflectarray for Broadband Linear Polarization Conversion and Optical Vortex Generation
Supporting Information Dielectric Meta-Reflectarray for Broadband Linear Polarization Conversion and Optical Vortex Generation Yuanmu Yang, Wenyi Wang, Parikshit Moitra, Ivan I. Kravchenko, Dayrl P. Briggs,
More informationNeutron spin filter based on dynamically polarized protons using photo-excited triplet states
The 2013 International Workshop on Polarized Sources, Targets & Polarimetry Neutron spin filter based on dynamically polarized protons using photo-excited triplet states Tim Eichhorn a,b, Ben van den Brandt
More informationMagnetic measurements (Pt. IV) advanced probes
Magnetic measurements (Pt. IV) advanced probes Ruslan Prozorov October 2018 Physics 590B types of local probes microscopic (site-specific) NMR neutrons Mossbauer stationary Bitter decoration magneto-optics
More informationScalable Quantum Photonics with Single Color
Scalable Quantum Photonics with Single Color Centers in Silicon Carbide Marina Radulaski,* Matthias Widmann,* Matthias Niethammer, Jingyuan Linda Zhang, Sang-Yun Lee, Torsten Rendler, Konstantinos G. Lagoudakis,
More informationQuantum Optics with Electrical Circuits: Circuit QED
Quantum Optics with Electrical Circuits: Circuit QED Eperiment Rob Schoelkopf Michel Devoret Andreas Wallraff David Schuster Hannes Majer Luigi Frunzio Andrew Houck Blake Johnson Emily Chan Jared Schwede
More information