A Generalized HSPICE* Macro-Model for Pseudo-Spin-Valve GMR Memory Bits

Similar documents
Mon., Feb. 04 & Wed., Feb. 06, A few more instructive slides related to GMR and GMR sensors

From Hall Effect to TMR

Giant Magnetoresistance

Giant Magnetoresistance

Low Energy Spin Transfer Torque RAM (STT-RAM / SPRAM) Zach Foresta April 23, 2009

Where, τ is in seconds, R is in ohms and C in Farads. Objective of The Experiment

MRAM: Device Basics and Emerging Technologies

From Spin Torque Random Access Memory to Spintronic Memristor. Xiaobin Wang Seagate Technology

Magnetic Sensor (3B) Magnetism Hall Effect AMR Effect GMR Effect. Young Won Lim 9/23/09

Chapter 1 Electronic and Photonic Materials - DMS. Diluted Magnetic Semiconductor (DMS)

Giant Magnetoresistance

5 Magnetic Sensors Introduction Theory. Applications

A Review of Spintronics based Data Storage. M.Tech Student Professor

01 Development of Hard Disk Drives

Magneto-Seebeck effect in spin-valve with in-plane thermal gradient

Wouldn t it be great if

The exchange interaction between FM and AFM materials

Perpendicular MTJ stack development for STT MRAM on Endura PVD platform

J 12 J 23 J 34. Driving forces in the nano-magnetism world. Intra-atomic exchange, electron correlation effects: Inter-atomic exchange: MAGNETIC ORDER

Author : Fabrice BERNARD-GRANGER September 18 th, 2014

SIMULATIONS ON DILUTE MAGNETIC SEMICONDUCTOR PROPERTIES

Giant Magnetoresistance

Spintronics. Seminar report SUBMITTED TO: SUBMITTED BY:

Some pictures are taken from the UvA-VU Master Course: Advanced Solid State Physics by Anne de Visser (University of Amsterdam), Solid State Course

Magnetic RAM. Presented at the THIC Meeting at the Raytheon ITS Auditorium, 1616 McCormick Dr Upper Marlboro MD November 5-6, 2002

ENGR4300 Fall 2005 Test 3S. Name solution. Section. Question 1 (25 points) Question 2 (25 points) Question 3 (25 points) Question 4 (25 points)

GMR Read head. Eric Fullerton ECE, CMRR. Introduction to recording Basic GMR sensor Next generation heads TMR, CPP-GMR UCT) Challenges ATE

ELECTRONIC SYSTEMS. Basic operational amplifier circuits. Electronic Systems - C3 13/05/ DDC Storey 1

Overview Of Spintronics

DC and AC modeling of minority carriers currents in ICs substrate

Physics and applications (I)

During such a time interval, the MOS is said to be in "deep depletion" and the only charge present in the semiconductor is the depletion charge.

V High frequency magnetic measurements

SPIN TRANSFER TORQUES IN HIGH ANISOTROPY MAGNETIC NANOSTRUCTURES

Study of the areal density in the read heads with spin valves with nano-oxide-layer insertion

Integrating Circuit Simulation with EIT FEM Models

9/18/2008 GMU, ECE 680 Physical VLSI Design

GMU, ECE 680 Physical VLSI Design

Digital Integrated Circuits A Design Perspective

Test System Requirements For Wafer Level MRAM Test

High-frequency measurements of spin-valve films and devices invited

Jan M. Rabaey Anantha Chandrakasan Borivoje Nikolic. November Digital Integrated Circuits 2nd Sequential Circuits

TRANSVERSE SPIN TRANSPORT IN GRAPHENE

TEPZZ A_T EP A1 (19) (11) EP A1. (12) EUROPEAN PATENT APPLICATION published in accordance with Art.

Wafer Charging in Process Equipment and its Relationship to GMR Heads Charging Damage

Advanced Lab Course. Tunneling Magneto Resistance

P-CHANNEL MOSFET Qualified per MIL-PRF-19500/564

High Reliability Hallogic Hall- Effect Sensors OMH090, OMH3019, OMH3020, OMH3040, OMH3075, OMH3131 (B, S versions)

Ferromagnetism and Electronic Transport. Ordinary magnetoresistance (OMR)

Introduction to Spintronics and Spin Caloritronics. Tamara Nunner Freie Universität Berlin

Colossal magnetoresistance:

MCP9700/9700A MCP9701/9701A

Center for Spintronic Materials, Interfaces, and Novel Architectures. Voltage Controlled Antiferromagnetics and Future Spin Memory

Digital Integrated Circuits A Design Perspective

Digital Integrated Circuits A Design Perspective

Focused-ion-beam milling based nanostencil mask fabrication for spin transfer torque studies. Güntherodt

Cover Page. The handle holds various files of this Leiden University dissertation

Chapter 14. Optical and Magnetic Materials. 경상대학교 Ceramic Design Lab.

Digital Integrated Circuits A Design Perspective

Giant Magnetoresistance in Magnetic Recording

1. Introduction : 1.2 New properties:

Hallogic Hall-effect Sensors OH090U, OH180U, OH360U OHN3000 Series, OHS3000 Series OHN3100 Series, OHS3100 Series

Magnetic tunnel junction beyond memory from logic to neuromorphic computing WANJUN PARK DEPT. OF ELECTRONIC ENGINEERING, HANYANG UNIVERSITY

Ferromagnetism and Electronic Transport. Ordinary magnetoresistance (OMR)

MSE 7025 Magnetic Materials (and Spintronics)

JUNE SiYaueo Department of Materials Science & Engineering May 21, 2007

Novel Magnetoelectronic Materials and Devices

Introduction to magnetic recording + recording materials

AUTOMOTIVE CURRENT TRANSDUCER OPEN LOOP TECHNOLOGY HC5FW 500-S

NEW CONCEPT FOR ANGULAR POSITION MEASUREMENTS. I.A. Premaratne, S.A.D.A.N. Dissanayake and D.S. Wickramasinghe

Hallogic Hall-Effect Sensors OH090U, OH180U, OH360U OHN3000 series, OHS3000 series OHN3100 series, OHS3100 series

Lecture 320 Improved Open-Loop Comparators and Latches (3/28/10) Page 320-1

introduction: what is spin-electronics?

MM74C922 MM74C Key Encoder 20-Key Encoder

AN ABSTRACT OF THE THESIS OF

ATS177. General Description. Features. Applications. Ordering Information SINGLE OUTPUT HALL EFFECT LATCH ATS177 - P L - X - X

Making Non-Volatile Nanomagnet Logic Non-Volatile

AUTOMOTIVE CURRENT TRANSDUCER OPEN LOOP TECHNOLOGY HC5FW 200-S/SP1

Magnetically Engineered Spintronic Sensors and Memory

N-CHANNEL MOSFET Qualified per MIL-PRF-19500/557

THE HALL EFFECT. Theory

Problem Solving 6: Ampere s Law and Faraday s Law. Part One: Ampere s Law

Computational materials design and its application to spintronics

Nonlinear AC Response and Noise of a Giant Magnetoresistive Sensor

Spin Switch: Model built using Verilog-A Spintronics Library

μ (vector) = magnetic dipole moment (not to be confused with the permeability μ). Magnetism Electromagnetic Fields in a Solid

Reliability of semiconductor I Cs. Reliability of semiconductor I Cs plus

Nomenclature, Advantages, Applications. Logic States, Read Ops, Write Ops

ESE 570: Digital Integrated Circuits and VLSI Fundamentals

SPINTRONICS. Waltraud Buchenberg. Faculty of Physics Albert-Ludwigs-University Freiburg

UNISONIC TECHNOLOGIES CO., LTD

A Perpendicular Spin Torque Switching based MRAM for the 28 nm Technology Node

Fabrication and Measurement of Spin Devices. Purdue Birck Presentation

Safety Barriers Series 9001, 9002 Standard Applications

Digital Integrated Circuits A Design Perspective. Semiconductor. Memories. Memories

UNIT 4 DC EQUIVALENT CIRCUIT AND NETWORK THEOREMS

A Universal Memory Model for Design Exploration. Ketul Sutaria, Chi-Chao Wang, Yu (Kevin) Cao School of ECEE, ASU

MM54C14 MM74C14 Hex Schmitt Trigger

MAGNETORESISTANCE PHENOMENA IN MAGNETIC MATERIALS AND DEVICES. J. M. De Teresa

PI3B V, Dual 4:1 Mux/DeMux NanoSwitch

Transcription:

A Generalized HSPICE* Macro-Model for Pseudo-Spin-Valve GMR Memory Bits by Bodhisattva Das William C. Black, Jr. Department of Electrical and Computer Engineering, Iowa State University (Work sponsored in part by Honeywell SSEC; and DARPA) *HSPICE is an authorized trademark of Avant! Corporation IEEE ISCAS 98 Monterey, CA 1

Outline Introduction to Giant Magneto Resistance (GMR) Devices GMR Characteristics and Applications Pseudo-Spin-Valve Characteristics Typical Generalized HSPICE Macro-Model Schematic Attributes Simulation Current and Future Work Summary and Conclusion B. Das, W. C. Black ECpE - ISU 2

Introduction to GMR Devices Two ferromagnetic layers separated by non-magnetic spacer layer Spin-Valve : one layer pinned by anti-ferromagnetic layer Pseudo-Spin-Valve : both the layers are free to rotate (not pinned) Permalloy 1 R R max k.cosφ M 2 φ M 1 H Permalloy 2 Nonmagnetic Inner Layer Resistance is function of difference between magnetizations Variations of 6%+ have been demonstrated for practical bits B. Das, W. C. Black ECpE - ISU 3

Typical Characteristics and Applications of GMR Characteristics: Stable magnetic states (non-volatile) Resistant to ionizing radiation Significant signal improvement relative to older singlelayered Anisotropic Magneto Resistance (AMR) material Applications: Non-volatile memory (MRAM) Magnetic sensors Disk read-heads Isolation devices B. Das, W. C. Black ECpE - ISU 4

Basic GMR Bit Configuration sn1 sense current wd1 wd0 word current sn0 Read with sense current (may stack bits) Write design options: word current alone (small memories) coincident sense and word current (large memories) B. Das, W. C. Black ECpE - ISU 5

Spin-Valve Characteristics N1 N2 R H RN3 P6 P5 Graph N N4 I N Graph P P4 P3 C R L P2 I P N5 N6 P1 I W (word) Hysteretic in nature Combination of graphs P and N. I W >I P : Graph P; I W <I N : Graph N Two distinct states : Graph P : St. 1 ; Graph N : St. 0 (or vice versa) I W >I P : write to St. 1 ; I W <I N : write to St. 0 ; I N <I W <I P : read I N and I P are weak functions of sense current B. Das, W. C. Black ECpE - ISU 6

Typical Pseudo-Spin-Valve P6 P5 P9 N9 N5 N6 N1 N2 N7 N8 P8 P7 N10 N3 P3 P10 Bottom (harder) layer magnetization curve: higher coercive force P2 P1 P6 P5 P9 N9 N5 N6 N1 N2 N7 N8 P8 P7 N10 N3 P3 P10 Top (softer) layer magnetization curve: lower coercive force P2 P1 B. Das, W. C. Black ECpE - ISU 7

Typical Pseudo-Spin-Valve (contd.) P6 R H R P5 P9 N9 N5 N6 N1 P8 N2 P7 R L N10 P4 N4 N7 N3 P3 P10 Combination of two curves : one for actual top layer and the other for bottom layer The graph is the absolute difference of the two Symmetric Major and Minor loops C P2 I W N8 P1 B. Das, W. C. Black ECpE - ISU 8

Macro-model Four terminal sub-circuit : Two word line terminals, two sense line terminals sn1 wd1 GMR wd0 Four simple parts : Input (word) circuit sn0 Bistable multivibrator or Schmitt Trigger Decision circuit Output (sense) circuit B. Das, W. C. Black ECpE - ISU 9

Macro-model (contd.) V TL L+ V TH = -L (R1/R2) V TL = -L + (R1/R2) Eopamp : VCVS Gd : VCR [1:1] cntl by V(7,wd0) Gr : VCCS (+/-1) = V(4,wd0)/L [ L = L + = -L ] Gb : PWL VCR cntl by V(3,wd0) Vc wd1 7 R1 5 wd1 Rw wd0 Input (word) Circuit 3 Gd wd0 wd0 Decision Circuit Gr Bistable Multivibrator wd0 R2 Gb Vmax= L + Vmin= L sn1 sn0 B. Das, W. C. Black ECpE - ISU 10 L 4 Eopamp wd0 V TH Output (sense) Circuit

Generalized PSV Characteristics R P6 N9 P5 N5 P9 N6 R H N1 P8 N2 P7 N10 R L P4 N3 P3 N4 P10 N7 P2 Hysteretic in nature: combination of systems P and N I W > I P2 : System P ; I W < I N2 : System N Each system can be divided into two graphs Four distinct states can be utilized: two bit memory C I W N8 P1 B. Das, W. C. Black ECpE - ISU 11

Generalized PSV Charac. (contd.) As two-state memory : I W >I P2, I W <I N2 : write ; I N2 <I W <I P2 : read I N2 and I P2 (write thresholds) are weak functions of sense current N9 N5 N6 Graph Nb N4 N1 N2 Graph Na N7 N10 N3 N8 System N can be divided into two graphs : Na and Nb B. Das, W. C. Black ECpE - ISU 12

Generalized PSV Charac. (contd.) P6 P5 P9 Graph Pb P8 P7 P4 Graph Pa P3 P10 System P can be divided into two graphs : Pa and Pb Non-symmetric Major and Minor loops Major loop : Na and Pa Minor loop : Nb and Pb P2 P1 B. Das, W. C. Black ECpE - ISU 13

Versatility Attributes of the Model Usable with any kind of PSV GMR elements Generalized and simple : can be modified easily to represent other kinds of hysteretic characteristics Flexibility All variables parameterized :.PARAM statements No component needing power supply : non-volatile Portability subcircuit (.inc) can be included in any HSPICE netlist: great help for GMR memory testing No semiconductor device : no variation with different device models B. Das, W. C. Black ECpE - ISU 14

Simulation Results Sub-circuit simulated with HSPICE : did converge! Simulations give proper results R for the GMR bit : 5% with R L =100Ω, R H =105Ω DC analysis done for a wide range of word currents Transient analysis shows proper major and minor loop characteristics Simulation of non-volatile latch structures with this GMR model Simulation of novel Pseudo-Spin-Valve GMR memory structures with this model (the structure can detect all four states but destructive read) B. Das, W. C. Black ECpE - ISU 15

Current and Future Work Already done: Thermal behavior (transient and dc) incorporated Asteroid curve incorporated: write thresholds depend on sense current value In the pipeline: Noise analysis (transient?), esp. near the write thresholds A universal GMR model usable for both memory and magnetic sensors (including read heads) B. Das, W. C. Black ECpE - ISU 16

B. Das, W. C. Black ECpE - ISU 17

Summary and Conclusion First HSPICE circuit model for Pseudo-Spin- Valve GMR element Successfully modeled the resistance vs. word current characteristic of a Pseudo-Spin-Valve GMR bit The model is simple, flexible and versatile Simulations show proper results The model is very general in nature, can be applied to other hysteretic characteristics Extended to include thermal effects and sense-currentdependency of write thresholds B. Das, W. C. Black ECpE - ISU 18

Questions? B. Das, W. C. Black ECpE - ISU 19