Work Sponsored By… Georgia Tech Foundation High-Frequency RFID: Applications and Challenges Center for Organic Photonics and Electronics Georgia Research Alliance NSF CAREER Grant ECS-0546955 Prof. Gregory D. Durgin www.propagation.gatech.edu Copyright 2006 Georgia Institute of Technology, All rights reserved For Further Reading… H. Stockman, “Communication by Means of Reflected Power,” in Proceedings of the IRE, October 1948, p. 11961204. K. Finkenzeller, RFID Handbook: Fundamentals and Applications in Contactless Smart Cards and Identification, 2nd ed., Wiley Inc., 2003 http://www.rfidjournal.com J.D. Griffin, G.D. Durgin, A. Haldi, and B. Kippelen, “Radio Link Budgets for 915 MHz RFID Antennas Placed on Various Objects,” in WCNG Wireless Symposium ’05, Austin TX, October 2005. D. Kim, M. A. Ingram, and W.W. Smith Jr., “Measurements of Small-Scale Fading and Path Loss for Long Range RF Tags,” IEEE Transactions on Antennas and Propagation, vol. 51, no. 8, pp. 17401749, Aug 2003. J.D. Griffin, “A Radio Assay for the Study of Radio Frequency Tag Antenna Presentation Overview Background Overview of RFID Challenges for RFID Radio Links Challenges for RFID Tags Challenges for RFID Readers Cross-Disciplinary Challenges The Future of RFID Performance,” Tech. Report PG-TR-050504-JDG, Georgia Tech Propagation Group MS Thesis, http://www.propagation.gatech.edu, 2005. D.M. Dobkin and S.M. Weigand, “UHF RFID and Tag Antenna Scattering, Part I: Experimental Results” and “Part II: Tag Array Scattering Theory”, Microwave Journal of Theory and Techniques, 2006 Copyright 2006 Georgia Institute of Technology, All rights reserved Copyright 2006 Georgia Institute of Technology, All rights reserved What This Talk Does NOT Address Detailed Signal-Processing Issues Software and Backhaul Issues Database and Inventory Software Privacy and Security Issues Integrated Circuit Design Copyright 2006 Georgia Institute of Technology, All rights reserved Background Copyright 2006 Georgia Institute of Technology, All rights reserved 1 Prof. Durgin Background The Propagation Group at GT Prof. Durgin has been teaching for 3 years at Georgia Tech Virginia Tech 1992 – 2000 PhD from MPRG in Dec. 2000 Post Doc. 2001-2002 at Osaka University Director of The Propagation Group at Georgia Tech Authored first Space- Time/MIMO textbook Frequent consultant to industry http://www.propagation.gatech.edu Copyright 2006 Georgia Institute of Technology, All rights reserved The Propagation Group at GT Copyright 2006 Georgia Institute of Technology, All rights reserved Faculty Collaborators Radio Wave Propagation RFID Emag/ RF Radiolocation (E911) Propagation Modeling Direction Finding and Array Technology Steffes Peterson Kenney Kippelen Perry Marder Space-Time/MIMO Radio Channels Applied Electromagnetics Chem/ COPE Copyright 2006 Georgia Institute of Technology, All rights reserved Copyright 2006 Georgia Institute of Technology, All rights reserved Specific Contributors to this Talk Joshua Griffin Joel Prothro Radio Assay, MIMO, Multi-Antenna Interrogation Organic Dielectrics for RF, On-Metal Antenna Performance (PhD) (MS) Albert Lu Anil Rohatgi Antennas, RFID Receiver design, Applied Emag Spread Spectrum and Anti-Collision What is Far-Field RFID? (MS) (Eng./LumoFlex) Copyright 2006 Georgia Institute of Technology, All rights reserved Copyright 2006 Georgia Institute of Technology, All rights reserved 2 Historical Perspective RF Terminology in This Presentation 1935 – Watson-Watt invents RADAR 1948 – Stockman publishes seminal work on backscatter Reader (Interrogator) – a device that retrieves radio in Proceedings of the IRE 1973 – Watson’s keylesss doorway entry patent 1980s – First deployments of electronic article surveillance (EAS) 1993 – First highway toll tags deployed in NY City (EZ Pass) 1999 – AutoID center established at MIT by Proctor and Gamble 2003 – Walmart mandate to suppliers for providing RFID tags on inventory palettes information from an RF tag Beacon – an RF device that periodically transmits information without reception Transponder – an RF device that retransmits without any waveform reconstruction (no modulation or demodulation capability) Transceiver – an RF device capable of modulation and demodulation Copyright 2006 Georgia Institute of Technology, All rights reserved Copyright 2006 Georgia Institute of Technology, All rights reserved What is an RF Tag? RF Tag Power Supply Differentiators RFID is just one application of RF Tags Purely-Passive Tags Our Definition of an RF Tag: A low-profile, low-power transponder Actually, there are 3 types of RF Tags Battery Assisted Tags Near-field transponder Far-field transponder Full Transceiver Powered solely from received RF signals Requires rectification of incoming waves Battery is used instead of in-coming RF power Finite lifetime Energy Scavenging Tags Super capacitors Solar cells Thermocouples Piezoelectrics Copyright 2006 Georgia Institute of Technology, All rights reserved Near vs. Far-field RFID Trade-offs Far-field RFID Near-field RFID Long range (1-10m) Range less than 1m High-frequency Conventional circuitry electronics effective Malevolent, high-loss RF channel Resistance to on-object degradations High bandwidth available Small bandwidth Compact, multiple Only one loop antenna antennas on a tag possible Copyright 2006 Georgia Institute of Technology, All rights reserved Copyright 2006 Georgia Institute of Technology, All rights reserved Example Applications Passive Data Exchange Sensors Measure glucose levels in the human body Pace maker monitor Environmental monitoring Radio Frequency Identification (RFID) Toll collection Airport luggage security Access control Medical ID bracelets Livestock tracking Self checkout Inventory management Copyright 2006 Georgia Institute of Technology, All rights reserved 3 The RF Tag System (Near-Field) Inductive Coupling between reader & RF tag Near-Field RFID Attributes Low Frequency Short Range (always less than 1m) Direct Influence of RFID Tag on Reader Physically limited in range and orientation. Copyright 2006 Georgia Institute of Technology, All rights reserved Hertzian Dipole (Simplest Radiator) Tiny current element Copyright 2006 Georgia Institute of Technology, All rights reserved Radiation Equations Field solution for a radiating current I∆z Radiates at the Origin Points up (z-direction) Simplest possible radiation scenario All radiation theory is based on this simple result Near-fields fall off 1/r2 and 1/r3 Far-fields fall off 1/r (1/r2 in power) Copyright 2006 Georgia Institute of Technology, All rights reserved Copyright 2006 Georgia Institute of Technology, All rights reserved The RF Tag System (Far-Field) Far-Field RFID Attributes Transmitter antenna Higher Frequency radiates Tag antenna scatters wave with modulation Receiver antenna captures information In some architectures, one antenna for RX & TX Potentially Longer Range (more than 1m) Copyright 2006 Georgia Institute of Technology, All rights reserved RFID Tag Effects Sensed via Traveling Wave Copyright 2006 Georgia Institute of Technology, All rights reserved 4 Classes of RFID Emitters The RF Tag System RF Tag Components EPC Class Characteristic Programmability Class 0 "Read Only" passive tags Programmed as part of the semiconductor manufacturing process Class 0+ "Write-Once, Read-Many" passive tags Extension of standards allows 0+ to be rewriteable Class 1 "Write-Once, Read-Many" passive Programmed once by the customer then Class 2 Rewritable passive tags Can be reprogrammed many times Class 3 Semi-passive tags Can be reprogrammed many times Class 4 Active tags Can be reprogrammed many times Class 5 Readers N/A Antennas: Far field Backscatter Printed Inverted F Printed Dipole Antenna (PIFA) Printed Folded Dipole Patch Antenna Table 1. RFID tag classifications. (ImpInj) Copyright 2006 Georgia Institute of Technology, All rights reserved Copyright 2006 Georgia Institute of Technology, All rights reserved The RF Tag System PIN Diode Modulation Modulation Circuitry Forward DC Bias => RF Short Load Modulation -- the carrier signal is modulated by switching an impedance from a matched condition to an un-matched condition to alter the reflection coefficient Reverse DC Bias => RF Open Forward Bias (RF short) Reverse Bias (RF open) Copyright 2006 Georgia Institute of Technology, All rights reserved PIN Diode Modulation Copyright 2006 Georgia Institute of Technology, All rights reserved Measurement of Backscatter Modulation Example PIN diode modulator built by Propagation Group Researcher Joshua Griffin Connects to antenna units and modulation waveforms Sample Output Copyright 2006 Georgia Institute of Technology, All rights reserved Copyright 2006 Georgia Institute of Technology, All rights reserved 5 Challenges for RFID Links Power-Up Link Budget Backscatter Link Budget Radiation Safety Levels Challenges for RFID Links Polarization Mismatch Small-Scale Fading Multi-Band Operation Copyright 2006 Georgia Institute of Technology, All rights reserved Copyright 2006 Georgia Institute of Technology, All rights reserved Conventional RF Link Budget Highlights of Forward Link Budget ⎛ 4π ⎞ PR = PT + GTX _ reader + GTag − 20 log d − 20 log⎜ ⎟ − Object Penalty ⎝ λ ⎠ Power loss is to the square of the distance (d2) Losses increase with higher frequency Reader Transmit Antenna Gain Free-Space Tag Antenna Gain Tag-Reader Separation Distance Measured In the Radio Assay Directional antennas are easier to make at higher frequency Limits power-up on a passive tag Copyright 2006 Georgia Institute of Technology, All rights reserved RF Tag Backscatter Link Budget Copyright 2006 Georgia Institute of Technology, All rights reserved RF Tag Backscatter Link Budget Backscattered Power Antenna Gains At Reader Transmit Power Tag-Reader Separation Distance ⎛ 4π ⎞ PR = GTX _ reader + GRX _ reader + PT − 40 log d − 40 log⎜ ⎟ ⎝ λ ⎠ + 2GTag + 20 log10 ΓA − ΓB − 2 Object Penalty Tag Antenna Gain Copyright 2006 Georgia Institute of Technology, All rights reserved Reflection Change Between Switched Loads ΓA, B = Z A, B − Z*0 Z A, B + Z 0 Adjustment For on-Object Degradations Copyright 2006 Georgia Institute of Technology, All rights reserved 6 Highlights of Backscatter Link Budget Radiation Safety Levels Power loss is to the fourth power of the distance High Transmit Power Required (d4) in line-of-sight channel Additional losses due to material attachments Directional antennas at the reader make a big difference in the link budget Must consider RF tag loading effects Limits the actual information exchange between tag and reader Forward Link Power-Up Weak Modulated Backscatter (1/r4 losses) Limiting Factor is often Radiation Safety Readers and People share space Repeated exposure in the work place Microwave safety levels must be strictly observed Copyright 2006 Georgia Institute of Technology, All rights reserved Polarization Issues Copyright 2006 Georgia Institute of Technology, All rights reserved Analogy to a Famous Physics Problem Two polarizers allow light through if they are aligned Example has vertical polarization If one polarizer is set at 90 degrees, there is complete on all three antennas Optimum for backscatter link budget Analogy between the reader antennas in the previous Copyright 2006 Georgia Institute of Technology, All rights reserved Analogy to a Famous Physics Problem Insertion of a 45-degree polarizer allows some light to pass through the entire setup. Final polarization has been rotated by 90 degrees. Analogous to the slanted RFID tag setup in previous slide Copyright 2006 Georgia Institute of Technology, All rights reserved blockage slide – near-zero power transfer. Copyright 2006 Georgia Institute of Technology, All rights reserved Polarization Issues Complete polarization mismatch on the backscatter link However, excellent isolation between reader antennas Copyright 2006 Georgia Institute of Technology, All rights reserved 7 First Encounter With Wave Fading Constructive and destructive interference causes voltage to vary along different points in space on the transmission line. Source Pow er L evel Polarization Issues “Mobile” Power Meter Signal Position Voltage Forward Propagating Wave 25% Total Power Loss Extremely Good Carrier- to-Interference Ratio Copyright 2006 Georgia Institute of Technology, All rights reserved Power Level Load Copyright 2006 Georgia Institute of Technology, All rights reserved Small-Scale Fading in Radio Links Propagating Waves Backward Propagating Wave Small-Scale Fading in Radio Links Received Signal Position Mobile Receiver Antenna The principle is the same as constructive/destructive interference on the transmission line. Copyright 2006 Georgia Institute of Technology, All rights reserved Double Fading in Backscatter Links Example measurement at 5.85 GHz made by moving receiver antenna over 1m area. Copyright 2006 Georgia Institute of Technology, All rights reserved Tag Antenna Diversity Use multiple antennas on the same tag Switch antennas when one experiences a fade A deep fade prohibits power-up of a tag A fade can be experienced twice on a backscatter link Copyright 2006 Georgia Institute of Technology, All rights reserved Copyright 2006 Georgia Institute of Technology, All rights reserved 8 Multi-Band Issues 865 MHz, 915 MHz, 955 MHz used in different countries Individual signal may be narrowband, but range of operability is broadband Challenges for RFID Tags Copyright 2006 Georgia Institute of Technology, All rights reserved Challenges for RFID Tags Copyright 2006 Georgia Institute of Technology, All rights reserved Powering Up a Passive Tag Powering Up a Passive Tag Battery Issues Antenna Design Issues Multi-Tag Coupling On-Metal Degradations On-Dielectric Degradations Tag Diversity Manufacturing Issues Copyright 2006 Georgia Institute of Technology, All rights reserved Powering Up a Passive Tag Passive RF chip must convert incoming RF to DC voltage Basic rectifier shown above Half-wave rectifier circuit shown above Ideal Voltage Conversion: VDC = 0.5 x (VAC)pp − VTO VTO is turn-on Voltage for Diode Copyright 2006 Georgia Institute of Technology, All rights reserved Powering Up a Passive Tag Voltage Doubler circuit capable of producing twice the DC ouput with a few more capacitors and diodes Ideal Voltage Conversion: VDC = (VAC)pp − 2VTO Copyright 2006 Georgia Institute of Technology, All rights reserved Ideal Voltage Conversion: VDC = 2 (VAC)pp − 4VTO Copyright 2006 Georgia Institute of Technology, All rights reserved 9 Powering Up a Passive Tag Full RF Tag Hardware Schematic Charge pump rectifier Diodes and capacitors AC voltage converted to DC Voltage stepped up (current stepped down) A: B: C: D: Ideal Voltage Conversion: VDC = N(VAC)pp − 2NVTO Drawbacks Higher complexity Diminishing returns for added stages Longer charging transient Copyright 2006 Georgia Institute of Technology, All rights reserved Note potential self-modulation problem Copyright 2006 Georgia Institute of Technology, All rights reserved Battery Issues Flexible Batteries? Cost Fledgling technology Lifetime Difficult to manufacture Disposability Form-factor Antenna Modulator Charge Pump Signaling Electronics batteries > 1.5V Zinc-Carbon structure: non-rechargeable Supply issues Flexibility Cell reliability is poor Battery specifications are heavily influenced by propagation issues Copyright 2006 Georgia Institute of Technology, All rights reserved Antenna Design Issues Bending/exposure limits Copyright 2006 Georgia Institute of Technology, All rights reserved Multi-Tag Coupling Wire designs Area antennas Patch antennas Unorthodox designs Each tag has a radar cross-section (RCS) RCS ~ electromagnetic area Overlapping antennas steal each other’s power Copyright 2006 Georgia Institute of Technology, All rights reserved Copyright 2006 Georgia Institute of Technology, All rights reserved 10 Multi-Tag Coupling On-Object Degradations Coplanar strip has most fringing fields Realistic scenarios many involve many RFID tags Environment will affect Higher-gain antennas have larger electromagnetic area operation Trade-off: an efficient individual RFID tag is a neighbor to other RFID tags Copyright 2006 Georgia Institute of Technology, All rights reserved Antenna Design and Manufacture Copyright 2006 Georgia Institute of Technology, All rights reserved Key Fabrication Issue: Skin Depth Conductor Materials Stamped Metal Electroless Cu, Ag Silver Inks Exotics Substrates Papers PET plastic Liquid Crystal Polymer (LCP) Copyright 2006 Georgia Institute of Technology, All rights reserved Key Fabrication Issue: Skin Depth Goals: Low Temperature Process Minimal Metal Deposition …but Stay Thicker than the Skin Depth Copyright 2006 Georgia Institute of Technology, All rights reserved RF Tag Antennas Planar folded dipole for 915 MHz Flexible PET* Substrate Silver – Electroless Silver Copper – Electroless Copper Rigid FR4 Substrate Baseline – 1 oz. milled copper on FR4 substrate *Polyethylene Copyright 2006 Georgia Institute of Technology, All rights reserved terephthalate Copyright 2006 Georgia Institute of Technology, All rights reserved 11 On-Dielectric Degradations RF Tag Antenna Material Attachment RFID tag pattern changes when placed on dielectric media Copyright 2006 Georgia Institute of Technology, All rights reserved Radio Assay Copyright 2006 Georgia Institute of Technology, All rights reserved Tag Pattern on a Wooden Slab Picture shows equipment at Georgia Tech for measurement RF Tag dipole placed on 1-inch plywood J.D. Griffin, “A Radio Assay for the Study of Radio Frequency Tag Antenna Performance,” Master’s thesis, Georgia Institute of Technology, 2005. Copyright 2006 Georgia Institute of Technology, All rights reserved Balun-Transformer Copyright 2006 Georgia Institute of Technology, All rights reserved Tag Pattern on a Wooden Slab Back Side Front Side Balun + Transformer allows an RF tag antenna, connected with co-planar strip feeds, to be read by 50Ohm coaxial cable Allows emulation of a chip on arbitrary antenna designs Copyright 2006 Georgia Institute of Technology, All rights reserved Question: On which side of the antenna is the dielectric wooden slab? Copyright 2006 Georgia Institute of Technology, All rights reserved 12 On-Dielectric Degradations On-Dielectric Degradations Dielectric material actually draws radiated power into Simple equivalent circuit medium Usually this is opposite the desired direction of operation Penalty is assessed twice on the backscatter link budget for explaining dielectric degradation Lower Impedance medium draws power Virtually all non-magnetic materials have higher medium impedance than free space µ0 ε rε 0 η= Copyright 2006 Georgia Institute of Technology, All rights reserved On-Metal Degradations Copyright 2006 Georgia Institute of Technology, All rights reserved RF Isolation with Engineered Polymers Ideal signaling occurs when switch between open and short circuit Formula depends on radiation resistance of antenna, Z0 ΓA, B = Z A, B − Z 0 Z A, B + Z 0 Maximum difference between reflections: Γopen = +1, Γshort = -1 Incident Wave Incident Wave Antenna Antenna Dielectric Air Ground Plane Ground Plane Find practical, low cost techniques for making thin, flexible substrates for RF tags. Substrates have low velocity of propagation that retard phase progression and isolate printed antennas. Copyright 2006 Georgia Institute of Technology, All rights reserved On-Metal Degradation Ohms Copyright 2006 Georgia Institute of Technology, All rights reserved On-Metal Degradations Formula depends on radiation resistance of antenna, Z0 Γshort = Z short − Z 0 >> −1 Z short + Z 0 Difference between states diminished: Γopen = +1, Γshort ~ +0.9 Copyright 2006 Georgia Institute of Technology, All rights reserved on metal impedance drop (Z0 drops below Zshort) Copyright 2006 Georgia Institute of Technology, All rights reserved 13 Tag Pattern for Foil-Coated Wood Tunable Impedance Matching Network Pi Network Back Side Front Side Loss of average gain (about 10 dB) and significant shielding on metal side of the pattern. Copyright 2006 Georgia Institute of Technology, All rights reserved Measured E-Plane Antenna Patterns J. H. Sinksy and C.R. Westgate, “Design of an Electronically Tunable Microwave Impedance Transformer,” in Proc. of the 1997 IEEE MTT-S Int. Microwave Symposium. Part 2 (of 3), ser. IEEE MTT-S Int. Microwave Symposium Digest, vol. 2 Denver, CO USA : IEEE, pp. 647-650, 1997. Copyright 2006 Georgia Institute of Technology, All rights reserved Measured E-Plane Antenna Patterns G.S. Smith, “Directive Properties of Antennas for Transmission into a Material Half-Space,” IEEE Transactions on Antennas and Propagation, vol. 32, pp. 232-246, 1984. Copyright 2006 Georgia Institute of Technology, All rights reserved Gain Penalty Copyright 2006 Georgia Institute of Technology, All rights reserved Gain Penalty Results AGP – Average gain penalty due to each material * These values were interpolated to 915 MHz from data of similar materials given by : A.R.V. Hippel, Dielectric Materials and Applications. New York : The Technology Press of M.I.T. and John Wiley and Sons, Inc., 1954. ** Undiluted antifreeze *** At approximately room temperature Copyright 2006 Georgia Institute of Technology, All rights reserved Copyright 2006 Georgia Institute of Technology, All rights reserved 14 Gain Penalty Example Backscatter Communication Power Radio Link Radio Link Budget Budget Copyright 2006 Georgia Institute of Technology, All rights reserved Challenges for RFID Readers Copyright 2006 Georgia Institute of Technology, All rights reserved Challenges for RFID Readers Directional Antennas Antenna Selection When used to transmit, they focus energy in a Self-Interference Interrogation through Portals Mechanical Spinning particular direction When used to receive, they reject radiation from sources outside their major lobe Single-Antenna Readers Copyright 2006 Georgia Institute of Technology, All rights reserved Directional Antennas Copyright 2006 Georgia Institute of Technology, All rights reserved Industry Portal Design Tagged object moves through portal via conveyor belt Time-varying, space-varying radio channel Copyright 2006 Georgia Institute of Technology, All rights reserved Copyright 2006 Georgia Institute of Technology, All rights reserved 15 Spinning Through Portals Single-Antenna Readers Object can be spun through the portal to increase Using one antenna for transmit and receive Inexpensive and Compact, but… Need a good match on the antenna Requires excellent, high-isolation coupler Dynamic range issues successful read rate Spinning provides both space and polarization diversity Copyright 2006 Georgia Institute of Technology, All rights reserved Copyright 2006 Georgia Institute of Technology, All rights reserved Single Antenna Architecture Circulator/coupler allows dual-use antenna Design is extremely sensitive to mismatched antenna Coupler must provide extremely high isolation between ports The Future of RFID Copyright 2006 Georgia Institute of Technology, All rights reserved Copyright 2006 Georgia Institute of Technology, All rights reserved The Future of RFID Energy Scavenging and Power Storage Energy Scavenging Mechanical Vibrations Low-Cost Fabrication Procedures Thermocouples (body heat?) Organic Electronics Solar Power Localization Capability Supercapacitors Array Interrogation Thin, flexible batteries Copyright 2006 Georgia Institute of Technology, All rights reserved Copyright 2006 Georgia Institute of Technology, All rights reserved 16 Low-Cost Fabrication Organic Electronics Silver Inks Pros Low-temperature processing Inexpensive fabrication Non-toxic Electroless Metal Depositions Exotic Materials Organic Substrates Cons High turn-on voltage Barrier technology issues Low frequency cut-off Temporal degradation Screen Printing Any good ideas? Exotic antenna: see-through Indium-Tin Oxide (ITO) dipole Copyright 2006 Georgia Institute of Technology, All rights reserved Localization and Array Interrogation Copyright 2006 Georgia Institute of Technology, All rights reserved Spatio-Temporal Backscatter Signaling Arrays for reading RFID tags (transmitter and receiver) Localization with arrays and direction finding Limitless signal-processing possibilities Copyright 2006 Georgia Institute of Technology, All rights reserved Copyright 2006 Georgia Institute of Technology, All rights reserved Key Questions How can spread-spectrum be used in an anti- collision scheme? How can this scheme lower complexity and Spread Spectrum for RFID and Anti-Collision Copyright 2006 Georgia Institute of Technology, All rights reserved power consumption? How many simultaneous reads are ultimately possible? Copyright 2006 Georgia Institute of Technology, All rights reserved 17 What is AntiAnti-Collision? Spread Spectrum TheoryTheory-Encoding Multiple tag backscatter simultaneously Each tag generates a unique How to separate one tag’s information high-frequency pseudo-random chipping sequence The sequence is multiplied by low-frequency data and then transmitted Signal a(t) represents the data and c(t) represents the chipping sequence. The transmitted waveform is thus x(t) = a(t) * c(t) from the sea of backscatter? Copyright 2006 Georgia Institute of Technology, All rights reserved Spread Spectrum TheoryTheory-Decoding Copyright 2006 Georgia Institute of Technology, All rights reserved M-Sequence Generation The received signal is a superposition of multiple tag backscatter y(t)=x1(t) + x2(t) Å high frequency We wish to recover x1(t) Å low frequency If both chipping sequences were of the range –1 : 1, then: y(t)*c1(t) = x1(t) + x2(t) * c1(t) (low freq) + (high freq) Low pass filtering the result will leave behind only x1(t): the desired data. Copyright 2006 Georgia Institute of Technology, All rights reserved Easy to generate and decode N shift registers result in 2N-1 length codes Low complexity, low power consumption No need for reception and decoding Copyright 2006 Georgia Institute of Technology, All rights reserved DifferentialDifferential-Offset Sequences Tag Design Each chip is equipped with a set of two PN generators Supports Anti-Collision for up to 255 tags tapped to create maximal length sequences of 255 bits. The two sequences are XORed together with a set phase shift between them. This phase shift determines the ID of the tag ID is set by delaying the clock to the second PN generator Copyright 2006 Georgia Institute of Technology, All rights reserved Tag IDs are reset able on the fly Copyright 2006 Georgia Institute of Technology, All rights reserved 18 Receiver Software Sequence Convergence The chipping sequences are easily simulated for a Measured RF Tag Data a.) x1(t) = y(t) * c(t) desired tag using Matlab The received signal is then captured, sampled, and processed in Labview. LPF Received Signal (Single Tag) Frequency Spectrum b.) Low frequency component Copyright 2006 Georgia Institute of Technology, All rights reserved c.) Low freq Data…(RSS in this figure) Copyright 2006 Georgia Institute of Technology, All rights reserved 19