Thermodynamic of computing. Fisica dell Energia  a.a. 2015/2016


 Adelia Daniels
 1 years ago
 Views:
Transcription
1 Thermodynamic of computing Fisica dell Energia  a.a. 2015/2016
2 Landauer principle Minimum amount of energy required greater than zero Let assume the operation of bit reset # of initial states: 2 # of final states: 1
3 Landauer principle S = k B log W Q apple T S Initial condition: two possible states Final condition: one possible state Heat produced S i = k B log 2 S f = k B log 1 S = S f S i = k B log 2 Q apple T S = k B T log 2
4 Landauer principle experimental verification The physics of information: from Maxwell s demon to Landauer  Eric Lutz  University of ErlangenNürnberg
5 Landauer principle experimental verification Even if you're not burning books, destroying information generates heat.  Sergio Cicliberto
6 Landauer principle experimental verification The physics of information: from Maxwell s demon to Landauer  Eric Lutz  University of ErlangenNürnberg
7 Landauer principle experimental verification The physics of information: from Maxwell s demon to Landauer  Eric Lutz  University of ErlangenNürnberg
8 Landauer principle experimental verification The physics of information: from Maxwell s demon to Landauer  Eric Lutz  University of ErlangenNürnberg
9 Landauer principle experimental verification Jun, Y., Gavrilov, M., & Bechhoefer, J. (2014). HighPrecision Test of Landauer s Principle in a Feedback Trap. Physical Review Letters, 113(19),
10 Landauer principle experimental verification Feedback Trap Jun, Y., Gavrilov, M., & Bechhoefer, J. (2014). HighPrecision Test of Landauer s Principle in a Feedback Trap. Physical Review Letters, 113(19),
11 Landauer principle experimental verification Erasure protocol Jun, Y., Gavrilov, M., & Bechhoefer, J. (2014). HighPrecision Test of Landauer s Principle in a Feedback Trap. Physical Review Letters, 113(19),
12 Landauer principle experimental verification Work series for individual cycles Jun, Y., Gavrilov, M., & Bechhoefer, J. (2014). HighPrecision Test of Landauer s Principle in a Feedback Trap. Physical Review Letters, 113(19),
13 Timedependent study of bit reset
14 Reset on colloidal particles Chiuchiú, D. "Timedependent study of bit reset." EPL (Europhysics Letters) (2015):
15 Timedependent study For a fixed τpr with Q(τpr) T S(τpr), study T S(t), Q(t), W (t), E(t). Chiuchiú, D. "Timedependent study of bit reset." EPL (Europhysics Letters) (2015):
16 Unconventional computing
17 Robust Soldier Crab Ball Gate YukioPegio Gunji, Yuta Nishiyama, Andrew Adamatzky
18 Robust Soldier Crab Ball Gate OR gate Robust Soldier Crab Ball Gate  YukioPegio Gunji, Yuta Nishiyama, Andrew Adamatzky
19 Robust Soldier Crab Ball Gate AND gate Robust Soldier Crab Ball Gate  YukioPegio Gunji, Yuta Nishiyama, Andrew Adamatzky
20 Robust Soldier Crab Ball Gate Robust Soldier Crab Ball Gate  YukioPegio Gunji, Yuta Nishiyama, Andrew Adamatzky
21 Robust Soldier Crab Ball Gate How much energy? Crabs usually eat algae. Crabs are omnivorous, meaning that they will eat both plants and other animals for sustenance. Energy Content of Algae: 5kcal for 3g Average weight of the crabs was 42g Suppose daily need is 50% of its weight: 21g of algae and thus 35kcal J of energy for daily operating a crab logic gate or 1.7W of power
22 NEMS Memory Device
23 NEMS Memory Devices Ionescu, Adrian M. "Nano Electro Mechanical (NEM) Memory Devices." Emerging Nanoelectronic Devices (2014):
24 NEMS Memory Devices Ionescu, Adrian M. "Nano Electro Mechanical (NEM) Memory Devices." Emerging Nanoelectronic Devices (2014):
25 NEMS Memory Devices Ionescu, Adrian M. "Nano Electro Mechanical (NEM) Memory Devices." Emerging Nanoelectronic Devices (2014):
26 NEMS Memory Devices
27 NEMS system
28 NEMS system Rebo Rebo
29 NEMS system armchair direction 6x1 nm atoms a = 2.42 Å Y = 0.85 TPa T = 10 K Neri, I., et al. "Reset and switch protocols at Landauer limit in a graphene buckled ribbon." EPL (Europhysics Letters) (2015):
30 Heat production evaluation Neri, I., et al. "Reset and switch protocols at Landauer limit in a graphene buckled ribbon." EPL (Europhysics Letters) (2015):
31 2DOF potential landscape Energy (J) A2 A A1 (Å) A2 (Å) 5 Neri, I., et al. "Reset and switch protocols at Landauer limit in a graphene buckled ribbon." EPL (Europhysics Letters) (2015):
32 Reset protocol Objective: move the system from an unknown state to known state ΔS = kb log(2) Qmin = kb T log(2) A1 A1 A2 Neri, I., et al. "Reset and switch protocols at Landauer limit in a graphene buckled ribbon." EPL (Europhysics Letters) (2015): A2
33 Reset protocol Quick and dirty: apply a positive force along Z on all atoms WRONG: it is not possible to control the velocity!
34 Reset protocol Quick and dirty: apply a positive force along Z on all atoms
35 Reset protocol Controlled way: apply a set of forces in to gently put the system in the desired configuration f MaxUp f 0Up f MaxDw f 0Dw t 0 t 1 t 2 t 3 t 4 Neri, I., et al. "Reset and switch protocols at Landauer limit in a graphene buckled ribbon." EPL (Europhysics Letters) (2015):
36 t 0 t 1 t 2 t 3 t 4 Reset protocol Controlled way: apply a set of forces in to gently put the system in the desired configuration f MaxUp f 0Up f MaxDw f 0Dw
37 Reset protocol Controlled way: apply a set of forces in to gently put the system in the desired configuration Neri, I., et al. "Reset and switch protocols at Landauer limit in a graphene buckled ribbon." EPL (Europhysics Letters) (2015):
38 Reset protocol Controlled way: apply a set of forces in to gently put the system in the desired configuration 0.4 τ p =110 ns counts 0.2 Q/kBT Q/kBT QL=kBTln2 τp (ns) Neri, I., et al. "Reset and switch protocols at Landauer limit in a graphene buckled ribbon." EPL (Europhysics Letters) (2015):
39 Switch protocol Objective: move the system from a known state to another known state ΔS = 0 Qmin = 0 A1 A1 A2 Neri, I., et al. "Reset and switch protocols at Landauer limit in a graphene buckled ribbon." EPL (Europhysics Letters) (2015): A2
40 Switch protocol Controlled way: apply a set of forces in to gently put the system in the desired configuration f MaxUp f 0Up f MaxDw f 0Dw t 0 t 1 t 2 t 3 t 4 t 5 t 6 Neri, I., et al. "Reset and switch protocols at Landauer limit in a graphene buckled ribbon." EPL (Europhysics Letters) (2015):
41 t t t t t t t Switch protocol Controlled way: apply a set of forces in to gently put the system in the desired configuration f MaxUp f 0Up f MaxDw f 0Dw
42 Switch protocol Controlled way: apply a set of forces in to gently put the system in the desired configuration Neri, I., et al. "Reset and switch protocols at Landauer limit in a graphene buckled ribbon." EPL (Europhysics Letters) (2015):
43 Switch protocol Controlled way: apply a set of forces in to gently put the system in the desired configuration 0.4 τ p =210 ns counts 0.2 Q/kBT Q/kBT τp (ns) Neri, I., et al. "Reset and switch protocols at Landauer limit in a graphene buckled ribbon." EPL (Europhysics Letters) (2015):
44 t t t t t t t Switch protocol Wrong way: apply the switch protocol from the wrong initial state f MaxUp f 0Up f MaxDw f 0Dw
45 Switch protocol Wrong way: apply the switch protocol from the wrong initial state Qmin > 2QL
46 Mechanical logic gate
47 Mechanical logic gate AND gate
48 Mechanical logic gate LopezSuarez, M. et al.. "Sub kbt micro electromechanical irreversible logic gate." arxiv preprint arxiv: (2015).
49 Mechanical logic gate Transfer function Thermomechanical noise limit
50 Mechanical logic gate x 2 = 1R 1 0 S(!) d! 2 k BT = 1 2 k x 2
51 Mechanical logic gate LopezSuarez, M. et al.. "Sub kbt micro electromechanical irreversible logic gate." arxiv preprint arxiv: (2015).
52 Mechanical logic gate Ω0 Ω1 LopezSuarez, M. et al.. "Sub kbt micro electromechanical irreversible logic gate." arxiv preprint arxiv: (2015).
53 Mechanical logic gate LopezSuarez, M. et al.. "Sub kbt micro electromechanical irreversible logic gate." arxiv preprint arxiv: (2015).
54 Mechanical logic gate ΔU = W Q = 0 LopezSuarez, M. et al.. "Sub kbt micro electromechanical irreversible logic gate." arxiv preprint arxiv: (2015).
55 Mechanical logic gate Structural damping > constant term Viscous + thermoelastic damping > t 1 Clamp recoil losses > t 3 LopezSuarez, M. et al.. "Sub kbt micro electromechanical irreversible logic gate." arxiv preprint arxiv: (2015).
56 Mechanical logic gate LopezSuarez, M. et al.. "Sub kbt micro electromechanical irreversible logic gate." arxiv preprint arxiv: (2015).
57
Thermodynamic of computing. Fisica dell Energia  a.a. 2017/2018
Thermodynamic of computing Fisica dell Energia  a.a. 2017/2018 Landauer principle Minimum amount of energy required greater than zero Let assume the operation of bit reset # of initial states: 2 # of
More informationPhysics of switches. Luca Gammaitoni NiPS Laboratory
Physics of switches Luca Gammaitoni NiPS Laboratory Logic switches A logic switch is a device that can assume physically distinct states as a result of external inputs. Usually the output of a physical
More informationDEMONS: MAXWELL S DEMON, SZILARD S ENGINE AND LANDAUER S ERASURE DISSIPATION
In: Proceedings of the first conference on Hot Topics in Physical Informatics (HoTPI, 2013 November). Paper is in press at International Journal of Modern Physics: Conference Series (2014). DEMONS: MAXWELL
More informationInformation to energy conversion in an electronic Maxwell s demon and thermodynamics of measurements.
Information to energy conversion in an electronic Maxwell s demon and thermodynamics of measurements Stony Brook University, SUNY Dmitri V Averin and iang Deng LowTemperature Lab, Aalto University Jukka
More informationMaxwell s Demon. Kirk T. McDonald Joseph Henry Laboratories, Princeton University, Princeton, NJ (October 3, 2004)
1 Problem Maxwell s Demon Kirk T. McDonald Joseph Henry Laboratories, Princeton University, Princeton, NJ 08544 (October 3, 2004) This problem is prob. 2 of [1]. One of the earliest conceptual supercomputers
More informationThermodynamical cost of accuracy and stability of information processing
Thermodynamical cost of accuracy and stability of information processing Robert Alicki Instytut Fizyki Teoretycznej i Astrofizyki Uniwersytet Gdański, Poland email: fizra@univ.gda.pl Fields Institute,
More informationDemons: Maxwell demon; Szilard engine; and Landauer's erasuredissipation
"Everything should be made as simple as possible, but not simpler." Albert Einstein Demons: Maxwell demon; Szilard engine; and Landauer's erasuredissipation Laszlo B. Kish (1), ClaesGöran Granqvist (2),
More informationON BROWNIAN COMPUTATION
ON BROWNIAN COMPUTATION JOHN D. NORTON Department of History and Philosophy of Science Center for Philosophy of Science University of Pittsburgh Pittsburgh PA USA 15260 jdnorton@pitt.edu Draft: October10,
More information04. Information and Maxwell's Demon. I. Dilemma for InformationTheoretic Exorcisms.
04. Information and Maxwell's Demon. I. Dilemma for InformationTheoretic Exorcisms. Two Options: (S) (Sound). The combination of object system and demon forms a canonical thermal system. (P) (Profound).
More informationMEASUREMENT THEORY QUANTUM AND ITS APPLICATIONS KURT JACOBS. University of Massachusetts at Boston. fg Cambridge WW UNIVERSITY PRESS
QUANTUM MEASUREMENT THEORY AND ITS APPLICATIONS KURT JACOBS University of Massachusetts at Boston fg Cambridge WW UNIVERSITY PRESS Contents Preface page xi 1 Quantum measurement theory 1 1.1 Introduction
More information2.2 Classical circuit model of computation
Chapter 2 Classical Circuit Models for Computation 2. Introduction A computation is ultimately performed by a physical device. Thus it is a natural question to ask what are the fundamental limitations
More informationDemon Dynamics: Deterministic Chaos, the Szilard Map, & the Intelligence of Thermodynamic Systems.
Demon Dynamics: Deterministic Chaos, the Szilard Map, & the Intelligence of Thermodynamic Systems http://csc.ucdavis.edu/~cmg/ Jim Crutchfield Complexity Sciences Center Physics Department University of
More informationLecture 14: State Tables, Diagrams, Latches, and Flip Flop
EE210: Switching Systems Lecture 14: State Tables, Diagrams, Latches, and Flip Flop Prof. YingLi Tian Nov. 6, 2017 Department of Electrical Engineering The City College of New York The City University
More informationİlke Ercan, PhD Assistant Professor, Electrical & Electronics Eng. Dep. Boğaziçi University, İstanbul, Turkey
ENERGY EFFICIENCY LIMITS IN BROWNIAN CIRCUITS A PHYSICALINFORMATIONTHEORETIC APPROACH, PhD Assistant Professor, Electrical & Electronics Eng. Dep. Boğaziçi University, İstanbul, Turkey Micro Energy 2017
More informationLandauer s principle in the quantum domain
Landauer s principle in the quantum domain Janet Anders Dept of Physics & Astronomy University College London London WC1E 6BT, UK j.anders@ucl.ac.uk Saroosh Shabbir Stefanie Hilt Department of Physics
More informationDM Bit Addressable Latch
8Bit Addressable Latch General Description The DM9334 is a high speed 8bit Addressable Latch designed for general purpose storage applications in digital systems. It is a multifunctional device capable
More information1. Introduction : 1.2 New properties:
Nanodevices In Electronics Rakesh Kasaraneni(PID : 4672248) Department of Electrical Engineering EEL 5425 Introduction to Nanotechnology Florida International University Abstract : This paper describes
More informationQuantum thermodynamics
Quantum thermodynamics a primer for the curious quantum mechanic Lídia del Rio, ETH Zurich QIP 2017 Seattle This talk is licensed under a Creative Commons Attribution 4.0 International License. Why quantum
More informationAPPLIED PHYSICS OPTIONS WITH REQUIREMENTS
APPLIED PHYSICS OPTIONS WITH REQUIREMENTS Minimum Applied Required = 30. One or two areas of focus allowed. Choose at least 14 credit hours if one area of focus chosen, or 9 credit hours of each if two
More informationHybrid Control and Switched Systems. Lecture #1 Hybrid systems are everywhere: Examples
Hybrid Control and Switched Systems Lecture #1 Hybrid systems are everywhere: Examples João P. Hespanha University of California at Santa Barbara Summary Examples of hybrid systems 1. Bouncing ball 2.
More informationIntroduction to Quantum Dynamics and Control
EE 290O. Advanced Topics in Control: Introduction to Quantum Dynamics and Control Instructor: Alireza Shabani Contact : shabani@berkeley.edu Office: Gilman, Room 19 Cory 278 Office Hours: Wednesdays 34
More informationNonlinear Mechanics of Monolayer Graphene Rui Huang
Nonlinear Mechanics of Monolayer Graphene Rui Huang Center for Mechanics of Solids, Structures and Materials Department of Aerospace Engineering and Engineering Mechanics The University of Texas at Austin
More informationQuantum measurement theory
1 Quantum measurement theory 1.1 Introduction and overview Much that is studied in quantum measurement theory, and thus in this book, is very different from that studied in its classical counterpart, Bayesian
More informationRelating Maxwell s Demon and Quantitative Analysis of Information Leakage for Practical Imperative Programs
Relating Maxwell s Demon and Quantitative Analysis of Information Leakage for Practical Imperative Programs Kushal Anjaria, Arun Mishra To cite this version: Kushal Anjaria, Arun Mishra. Relating Maxwell
More informationThe End of the Thermodynamics of Computation: A No Go Result
December 22, 28, 2011 June 20, 2012 March 31, August 20, 2013 The End of the Thermodynamics of Computation: A No Go Result John D. Norton Department of History and Philosophy of Science Center for Philosophy
More informationInformation in Biology
Information in Biology CRI  Centre de Recherches Interdisciplinaires, Paris May 2012 Information processing is an essential part of Life. Thinking about it in quantitative terms may is useful. 1 Living
More informationImplementation of Optimized Reversible Sequential and Combinational Circuits for VLSI Applications
V. G. Santhi Swaroop et al Int. Journal of Engineering Research and Applications RESEARCH ARTICLE OPEN ACCESS Implementation of Optimized Reversible Sequential and Combinational Circuits for VLSI Applications
More informationPractical Attacks on HB and HB+ Protocols
Practical Attacks on HB and HB+ Protocols Zbigniew Gołębiewski 1, Krzysztof Majcher 2, Filip Zagórski 3, and Marcin Zawada 3 1 Institute of Computer Science, Wrocław University 2 Mathematical Institute,
More informationQUANTUM TECHNOLOGIES: THE SECOND QUANTUM REVOLUTION* Jonathan P. Dowling
QUANTUM TECHNOLOGIES: THE SECOND QUANTUM REVOLUTION* Jonathan P. Dowling Quantum Science & Technologies Group Hearne Institute for Theoretical Physics Louisiana State University http://quantum.phys.lsu.edu
More informationINTEGRATED CIRCUITS. For a complete data sheet, please also download:
INTEGRATED CIRCUITS DATA SEET For a complete data sheet, please also download: The IC06 7C/CT/CU/CMOS Logic Family Specifications The IC06 7C/CT/CU/CMOS Logic Package Information The IC06 7C/CT/CU/CMOS
More informationProtection of an Unknown Quantum State against Decoherence via Weak Measurement and Quantum Measurement Reversal
Comput. Sci. Appl. Volume 1, Number 1, 2014, pp. 6066 Received: May 19, 2014; Published: July 25, 2014 Computer Science and Applications www.ethanpublishing.com Protection of an Unknown Quantum State
More informationLecture 6: TimeDependent Behaviour of Digital Circuits
Lecture 6: TimeDependent Behaviour of Digital Circuits Two rather different quasiphysical models of an inverter gate were discussed in the previous lecture. The first one was a simple delay model. This
More information93L34 8Bit Addressable Latch
93L34 8Bit Addressable Latch General Description The 93L34 is an 8bit addressable latch designed for general purpose storage applications in digital systems It is a multifunctional device capable of
More informationEntropy Evaluation for Oscillatorbased True Random Number Generators
Entropy Evaluation for Oscillatorbased True Random Number Generators Yuan Ma DCS Center Institute of Information Engineering Chinese Academy of Sciences Outline RNG Modeling method Experiment Entropy
More informationINTRODUCTION À LA PHYSIQUE MÉSOSCOPIQUE: ÉLECTRONS ET PHOTONS INTRODUCTION TO MESOSCOPIC PHYSICS: ELECTRONS AND PHOTONS
Chaire de Physique Mésoscopique Michel Devoret Année 2007, Cours des 7 et 14 juin INTRODUCTION À LA PHYSIQUE MÉSOSCOPIQUE: ÉLECTRONS ET PHOTONS INTRODUCTION TO MESOSCOPIC PHYSICS: ELECTRONS AND PHOTONS
More informationQUANTUM MEASUREMENT THEORY AND ITS APPLICATIONS
QUANTUM MEASUREMENT THEORY AND ITS APPLICATIONS Recent experimental advances in the control of quantum superconducting circuits, nanomechanical resonators and photonic crystals have meant that quantum
More informationBilayer GNR Mobility Model in Ballistic Transport Limit
ilayer GNR Mobility Model in allistic Transport Limit S. Mahdi Mousavi, M.Taghi Ahmadi, Hatef Sadeghi, and Razali Ismail Computational Nanoelectronics (CoNE) Research Group, Electrical Engineering Faculty,
More informationDM74LS670 3STATE 4by4 Register File
DM74LS670 3STATE 4by4 Register File General Description August 1986 Revised March 2000 These register files are organized as 4 words of 4 bits each, and separate onchip decoding is provided for addressing
More informationExam for Physics 4051, October 31, 2008
Exam for Physics 45, October, 8 5 points  closed book  calculators allowed  show your work Problem : (6 Points) The 4 bit shift register circuit shown in Figure has been initialized to contain the following
More informationSequential Circuit Design
Sequential Circuit esign esign Procedure. Specification 2. Formulation Obtain a state diagram or state table 3. State Assignment Assign binary codes to the states 4. FlipFlop Input Equation etermination
More information6 Synchronous State Machine Design
Design of synchronous counters. Based on the description of the problem, determine the required number n of the FFs  the smallest value of n is such that the number of states N 2 n and the desired counting
More informationCS 256: Neural Computation Lecture Notes
CS 56: Neural Computation Lecture Notes Chapter : McCullochPitts Neural Networks A logical calculus of the ideas immanent in nervous activity M. Minsky s adaptation (Computation: Finite and Infinite Machines,
More information1.10 (a) Function of AND, OR, NOT, NAND & NOR Logic gates and their input/output.
Chapter 1.10 Logic Gates 1.10 (a) Function of AND, OR, NOT, NAND & NOR Logic gates and their input/output. Microprocessors are the central hardware that runs computers. There are several components that
More informationControl gates as building blocks for reversible computers
Control gates as building blocks for reversible computers A. De Vos 1, B. Desoete 2, F. Janiak 3, and A. Nogawski 3 1 Universiteit Gent and Imec v.z.w., B9000 Gent, Belgium 2 Universiteit Gent, B9000
More informationNRAM: High Performance, Highly Reliable Emerging Memory
NRAM: High Performance, Highly Reliable Emerging Memory Sheyang Ning,2, Tomoko Ogura Iwasaki, Darlene Viviani 2, Henry Huang 2, Monte Manning 2, Thomas Rueckes 2, Ken Takeuchi Chuo University 2 Nantero
More informationChapter 3 Combinational Logic Design
Logic and Computer Design Fundamentals Chapter 3 Combinational Logic Design Part 1 Implementation Technology and Logic Design Overview Part 1Implementation Technology and Logic Design Design Concepts
More informationQuantERA Cofunded Call 2017: Scientific Scope
QuantERA Cofunded Call 2017: Scientific Scope Konrad Banaszek Konrad.Banaszek@ncn.gov.pl This project has received funding from the European Union s Horizon 2020 research and innovation programme under
More informationIntroduction EE 224: INTRODUCTION TO DIGITAL CIRCUITS & COMPUTER DESIGN. Lecture 6: Sequential Logic 3 Registers & Counters 5/9/2010
EE 224: INTROUCTION TO IGITAL CIRCUITS & COMPUTER ESIGN Lecture 6: Sequential Logic 3 Registers & Counters 05/10/2010 Avinash Kodi, kodi@ohio.edu Introduction 2 A FlipFlop stores one bit of information
More informationFinding the Missing Memristor
February 11, 29 Finding the Missing Memristor 3 nm Stan Williams HP 26 HewlettPackard Development Company, L.P. The information contained herein is subject to change without notice Acknowledgments People
More informationParallel Processing and Circuit Design with NanoElectroMechanical Relays
Parallel Processing and Circuit Design with NanoElectroMechanical Relays Elad Alon 1, TsuJae King Liu 1, Vladimir Stojanovic 2, Dejan Markovic 3 1 University of California, Berkeley 2 Massachusetts
More informationHong Ou Mandel experiment with atoms
BEC on an MCP Hong Ou Mandel experiment with atoms Chris Westbrook Laboratoire Charles Fabry, Palaiseau FRISNO 13, Aussois 18 march 2015 2 particles at a beam splitter 1 particle at each input 4 possibilities:
More informationQuantum Cellular Automata: The Physics of Computing with Arrays of Quantum Dot Molecules
Quantum Cellular Automata: The Physics of Computing with Arrays of Quantum Dot Molecules Craig. S. Lent, P. Douglas Tougaw, and Wolfgang Porod Department of Electrical Engineering, University of Notre
More information24.2: SelfBiased, HighBandwidth, LowJitter 1to4096 Multiplier Clock Generator PLL
24.2: SelfBiased, HighBandwidth, LowJitter 1to4096 Multiplier Clock Generator PLL John G. Maneatis 1, Jaeha Kim 1, Iain McClatchie 1, Jay Maxey 2, Manjusha Shankaradas 2 True Circuits, Los Altos,
More informationSTOCHASTIC LOGIC Architectures for postcmos switches
STOCHASTIC LOGIC Architectures for postcmos switches David S. Ricketts Electrical & Computer Carnegie Mellon University www.ece.cmu.edu/~ricketts Jehoshua (Shuki) Bruck Engineering Electrical Engineering
More informationVLSI Design Verification and Test Simulation CMPE 646. Specification. Design(netlist) Truevalue Simulator
Design Verification Simulation used for ) design verification: verify the correctness of the design and 2) test verification. Design verification: Response analysis Specification Design(netlist) Critical
More informationCD4028BC BCDtoDecimal Decoder
CD4028BC BCDtoDecimal Decoder General Description The CD4028BC is a BCDtodecimal or binarytooctal decoder consisting of 4 inputs, decoding logic gates, and 10 output buffers. A BCD code applied to
More informationarxiv: v1 [physics.appph] 1 May 2017
Magnetic Skyrmions for Cache Memory MeiChin Chen 1 and Kaushik Roy 1 1 School of Electrical and Computer Engineering, Purdue University, West Lafayette, 47906, USA * chen1320@purdue.edu ABSTRACT arxiv:1705.01095v1
More informationTopological insulator particles as optically induced oscillators: Towards dynamical force measurements and optical rheology
Topological insulator particles as optically induced oscillators: Towards dynamical force measurements and optical rheology Warlley Hudson Campos warlley.campos@ufv.br Departamento de Física  Universidade
More informationMASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics 8.02 Spring 2003 Experiment 17: RLC Circuit (modified 4/15/2003) OBJECTIVES
MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics 8. Spring 3 Experiment 7: R Circuit (modified 4/5/3) OBJECTIVES. To observe electrical oscillations, measure their frequencies, and verify energy
More informationNotes on Landauer s principle, reversible computation, and Maxwell s Demon
Studies in History and Philosophy of Modern Physics 34 (2003) 501 510 Notes on Landauer s principle, reversible computation, and Maxwell s Demon Charles H. Bennett IBM Research Division, Yorktown Heights,
More informationCMOS Comparators. Kyungpook National University. Integrated Systems Lab, Kyungpook National University. Comparators
IsLab Analog Integrated ircuit Design OMP21 MOS omparators כ Kyungpook National University IsLab Analog Integrated ircuit Design OMP1 omparators A comparator is used to detect whether a signal is greater
More informationSession Chair: Prof. Haiping Cheng (University of Florida) Dr. Lei Shen. National University of Singapore
B1. Modeling Quantum Transport at Nanoscale Chair(s): Chun ZHANG, National University of Singapore, Singapore Session s Title (if available) Tue  17 Jan 2017 13:00 ~ 14:30 Room 2 Session Chair: Prof.
More informationModeling Airplane Wings
Modeling Airplane Wings Lauren Ault Physics Department, The College of Wooster, Wooster, Ohio 9 May 5, 000 Abstract: An air gyroscope is used to determine the nature of the viscous force of a sphere floating
More informationThermodynamics/Optics
Thermodynamics/Optics Survey! Survey! I hate calculus! Survey! I hate calculus! Overview of Last Lecture Foundation of physics, classical mechanics Copernican Revolution Galileo/Newton experimentation
More informationCMOS compatible integrated ferroelectric tunnel junctions (FTJ)
CMOS compatible integrated ferroelectric tunnel junctions (FTJ) Mohammad Abuwasib 1*, Hyungwoo Lee 2, ChangBeom Eom 2, Alexei Gruverman 3, Jonathan Bird 1 and Uttam Singisetti 1 1 Electrical Engineering,
More information5. Sequential Logic x Computation Structures Part 1 Digital Circuits. Copyright 2015 MIT EECS
5. Sequential Logic 6.004x Computation Structures Part 1 igital Circuits Copyright 2015 MIT EECS 6.004 Computation Structures L5: Sequential Logic, Slide #1 Something We Can t Build (Yet) What if you were
More informationCombinational Logic Design Principles
Combinational Logic Design Principles Switching algebra Doru Todinca Department of Computers Politehnica University of Timisoara Outline Introduction Switching algebra Axioms of switching algebra Theorems
More informationThe Leader Election Protocol (IEEE 1394)
The Leader Election Protocol (IEEE 1394) J.R. Abrial, D. Cansell, D. Méry July 2002 This Session  Background :)  An informal presentation of the protocol :)  Step by step formal design :  Short
More informationDr Ian R. Manchester Dr Ian R. Manchester AMME 3500 : Review
Week Date Content Notes 1 6 Mar Introduction 2 13 Mar Frequency Domain Modelling 3 20 Mar Transient Performance and the splane 4 27 Mar Block Diagrams Assign 1 Due 5 3 Apr Feedback System Characteristics
More informationEECS 579: Logic and Fault Simulation. Simulation
EECS 579: Logic and Fault Simulation Simulation: Use of computer software models to verify correctness Fault Simulation: Use of simulation for fault analysis and ATPG Circuit description Input data for
More informationDM5490 DM7490A DM7493A Decade and Binary Counters
DM5490 DM7490A DM7493A Decade and Binary Counters General Description Each of these monolithic counters contains four masterslave flipflops and additional gating to provide a dividebytwo counter and
More informationINTEGRATED CIRCUITS. For a complete data sheet, please also download:
INTEGRATED CIRCUITS DATA SHEET For a complete data sheet, please also download: The IC6 74HC/HCT/HCU/HCMOS ogic Family Specifications The IC6 74HC/HCT/HCU/HCMOS ogic Package Information The IC6 74HC/HCT/HCU/HCMOS
More information9334 DM Bit Addressable Latch
9334 DM9334 8Bit Addressable Latch General Description The DM9334 is a high speed 8bit Addressable Latch designed for general purpose storage applications in digital systems It is a multifunctional device
More informationThe Compton Effect. Martha Buckley MIT Department of Physics, Cambridge, MA (Dated: November 26, 2002)
The Compton Effect Martha Buckley MIT Department of Physics, Cambridge, MA 02139 marthab@mit.edu (Dated: November 26, 2002) We measured the angular dependence of the energies of 661.6 kev photons scattered
More informationStructure and electronic transport in graphene wrinkles
Supplementary Information: Structure and electronic transport in graphene wrinkles Wenjuan Zhu*, Tony Low, Vasili Pereeinos, Ageeth A. Bol, Yu Zhu, Hugen Yan, Jerry Tersoff and Phaedon Avouris* IBM Thomas
More informationDigital Integrated Circuits A Design Perspective
Digital Integrated Circuits A Design Perspective Jan M. Rabaey Anantha Chandrakasan Borivoje Nikolic Designing Sequential Logic Circuits November 2002 Sequential Logic Inputs Current State COMBINATIONAL
More informationIrreversible Processes
Irreversible Processes Examples: Block sliding on table comes to rest due to friction: KE converted to heat. Heat flows from hot object to cold object. Air flows into an evacuated chamber. Reverse process
More informationStudents should be able to (a) produce a truth table from a given logic diagram
Truth tables Teacher s Notes Lesson Plan Length 60 mins Specification Link 2.1.2/f inary logic Learning objective Students should be able to (a) produce a truth table from a given logic diagram Time (min)
More informationDS0026 Dual HighSpeed MOS Driver
Dual HighSpeed MOS Driver General Description DS0026 is a low cost monolithic high speed two phase MOS clock driver and interface circuit. Unique circuit design provides both very high speed operation
More informationFloating Point Representation and Digital Logic. Lecture 11 CS301
Floating Point Representation and Digital Logic Lecture 11 CS301 Administrative Daily Review of today s lecture w Due tomorrow (10/4) at 8am Lab #3 due Friday (9/7) 1:29pm HW #5 assigned w Due Monday 10/8
More informationENGG1015 Homework 1 Question 1. ENGG1015: Homework 1
ENGG1015 Homework 1 Question 1 ENGG1015: Homework 1 Due: Nov 5, 2012, 11:55pm Instruction: Submit your answers electronically through Moodle (Link to Homework 1). You may type your answers using any text
More informationAn Autonomous Nonvolatile Memory Latch
Radiant Technologies, Inc. 2835D Pan American Freeway NE Albuquerque, NM 87107 Tel: 5058428007 Fax: 5058420366 email: radiant@ferrodevices.com www.ferrodevices.com An Autonomous Nonvolatile Memory
More informationAxiomatic Information Thermodynamics. Received: 1 February 2018; Accepted: 26 March 2018; Published: 29 March 2018
entropy Article Axiomatic Information Thermodynamics Austin Hulse 1, Benjamin Schumacher 1, * and Michael D. Westmoreland 2 1 Department of Physics, Kenyon College, Gambier, OH 43022, USA; hulsea@kenyon.edu
More informationCreation of a StateSpace Model from a Finite Element Model for the active control algorithm efficiency tests.
Creation of a StateSpace Model from a Finite Element Model for the active control algorithm efficiency tests. N. Geffroy, L. Brunetti, B. Bolzon, A. Jeremie, Laboratoire d AnnecyleVieux de Physique
More informationBoolean State Transformation
Quantum Computing Boolean State Transformation Quantum Computing 2 Boolean Gates Boolean gates transform the state of a Boolean system. Conventionally a Boolean gate is a map f : {,} n {,}, where n is
More informationEE141Microelettronica. CMOS Logic
Microelettronica CMOS Logic CMOS logic Power consumption in CMOS logic gates Where Does Power Go in CMOS? Dynamic Power Consumption Charging and Discharging Capacitors Short Circuit Currents Short Circuit
More informationNoise effects and thermally induced switching errors in Josephson junctions
3479 Noise effects and thermally induced switching errors in Josephson junctions Andrey L. Pankratov 1 and Bernardo Spagnolo 2 1 Institute for Physics of Microstructures of RAS, Nizhny Novgorod, Russia
More informationCS/COE0447: Computer Organization
Logic design? CS/COE0447: Computer Organization and Assembly Language Logic Design Review Digital hardware is implemented by way of logic design Digital circuits process and produce two discrete values:
More informationAn Overview of Spinbased Integrated Circuits
ASPDAC 2014 An Overview of Spinbased Integrated Circuits Wang Kang, Weisheng Zhao, Zhaohao Wang, JacquesOlivier Klein, Yue Zhang, Djaafar Chabi, Youguang Zhang, Dafiné Ravelosona, and Claude Chappert
More informationDistributed by: www.jameco.com 18008314242 The content and copyrights of the attached material are the property of its owner. INTEGRATED CIRCUITS DATA SHEET For a complete data sheet, please also download:
More informationEmerging Interconnect Technologies for CMOS and beyondcmos Circuits
Emerging Interconnect Technologies for CMOS and beyondcmos Circuits SouChi Chang, Rouhollah M. Iraei Vachan Kumar, Ahmet Ceyhan and Azad Naeemi School of Electrical & Computer Engineering Georgia Institute
More informationUniversity of New Mexico
Quantum State Reconstruction via Continuous Measurement Ivan H. Deutsch, Andrew Silberfarb University of New Mexico Poul Jessen, Greg Smith University of Arizona Information Physics Group http://info.phys.unm.edu
More informationTrajectory tracking & Pathfollowing control
Cooperative Control of Multiple Robotic Vehicles: Theory and Practice Trajectory tracking & Pathfollowing control EECI Graduate School on Control Supélec, Feb. 2125, 2011 A word about T Tracking and
More informationMM74C90 MM74C93 4Bit Decade Counter 4Bit Binary Counter
4Bit Decade Counter 4Bit Binary Counter General Description The MM74C90 decade counter and the MM74C93 binary counter and complementary MOS (CMOS) integrated circuits constructed with N and Pchannel
More informationDigital Electronics Final Examination. Part A
Digital Electronics Final Examination Part A Spring 2009 Student Name: Date: Class Period: Total Points: /50 Converted Score: /40 Page 1 of 13 Directions: This is a CLOSED BOOK/CLOSED NOTES exam. Select
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 informationThermoelectricity with cold atoms?
Thermoelectricity with cold atoms? Ch. Grenier, C. Kollath & A. Georges Centre de physique Théorique  Université de Genève  Collège de France Université de Lorraine Séminaire du groupe de physique statistique
More informationOn GibbsShannon Entropy
On GibbsShannon Entropy Raphael Chetrite CNRS J.A Dieudonne Nice. Graduate School of Science, Kyoto. LARGE DEVIATION THEORY IN STATISTICAL PHYSICS : RECENT ADVANCES AND FUTURE CHALLENGES M. Gavrilov,
More informationBoolean Algebra and Digital Logic 2009, University of Colombo School of Computing
IT 204 Section 3.0 Boolean Algebra and Digital Logic Boolean Algebra 2 Logic Equations to Truth Tables X = A. B + A. B + AB A B X 0 0 0 0 3 Sum of Products The OR operation performed on the products of
More informationarxiv:quantph/ v1 12 Dec 1996
A quantummechanical Maxwell s demon arxiv:quantph/9612034v1 12 Dec 1996 Seth Lloyd d Arbeloff Laboratory for Information Systems and Technology Department of Mechanical Engineering Massachusetts Institute
More information