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RTU 1 A-5 A 25 GHz 3. 3 d. B NF Low Noise Amplifier RTU 1 A-5 A 25 GHz 3. 3 d. B NF Low Noise Amplifier based upon Slow Wave Transmission Lines and the 0. 18 μm CMOS Technology A. Sayag(1), S. Levin(2), D. Regev(2), D. Zfira(2), S. Shapira(2), D. Goren(3) and D. Ritter(1) Department of Electrical Engineering, Technion, Haifa, Israel (2) Tower Semiconductors inc. , Migdal Ha. Emek, Israel (3) IBM Haifa Research Laboratories, Haifa, Israel

Outline • Low Noise Amplifier design methodology • New semi-analytic model for slow wave Outline • Low Noise Amplifier design methodology • New semi-analytic model for slow wave transmission lines • LNA performance

Motivation • Can we get close to the transistor minimum NF in 24 GHz Motivation • Can we get close to the transistor minimum NF in 24 GHz LNA design? @ 24 GHz Best 0. 18 μm 24 GHz LNA: NF=3. 9 [Shih-Chieh Shin et al. , IEEE MWCL, 2005. ]

LNA Design Methodology 1. Determine the optimal current density 2. Determine critical circuit element LNA Design Methodology 1. Determine the optimal current density 2. Determine critical circuit element values 3. Choose the transistor width

Transistor Performance Determined by Current Density @ 24 GHz RFIC – Atlanta June 15 Transistor Performance Determined by Current Density @ 24 GHz RFIC – Atlanta June 15 -17, 2008

Transistor Performance Determined by Current Density RFIC – Atlanta June 15 -17, 2008 Transistor Performance Determined by Current Density RFIC – Atlanta June 15 -17, 2008

Circuit Topology: Common source with inductive source degeneration RFIC – Atlanta June 15 -17, Circuit Topology: Common source with inductive source degeneration RFIC – Atlanta June 15 -17, 2008

Source Inductor value for each Width RFIC – Atlanta June 15 -17, 2008 Source Inductor value for each Width RFIC – Atlanta June 15 -17, 2008

Example: Source Inductor for W=40μm RFIC – Atlanta June 15 -17, 2008 Example: Source Inductor for W=40μm RFIC – Atlanta June 15 -17, 2008

How does the Insertion Loss of the Input Matching Network Depend on Transistor Width? How does the Insertion Loss of the Input Matching Network Depend on Transistor Width? Equal Insertion loss contours • Each point on the Smith Chart corresponds to a hypothetical transistor input impedance • Input impedance is matched to 50 ohms by a matching network with inductors having Q=20 RFIC – Atlanta June 15 -17, 2008

Insertion Loss Map of the Input Matching Network with Q = 10 RFIC – Insertion Loss Map of the Input Matching Network with Q = 10 RFIC – Atlanta June 15 -17, 2008

Insertion Loss Map of the Input Matching Network with Q = 30 RFIC – Insertion Loss Map of the Input Matching Network with Q = 30 RFIC – Atlanta June 15 -17, 2008

We need Q > 20 ! RFIC – Atlanta June 15 -17, 2008 We need Q > 20 ! RFIC – Atlanta June 15 -17, 2008

Choosing the Transistor Widths (assuming a two identical stage amplifier) W [um] Transistor Max Choosing the Transistor Widths (assuming a two identical stage amplifier) W [um] Transistor Max Min NF [d. B] gs [d. B] NF total [d. B] Gain [d. B] 20 7. 2 0. 82 0. 3 1. 2 40 8 0. 9 0. 8 1. 3 80 8. 2 1 1. 44 1. 6 * g. S - normalized source gain factor RFIC – Atlanta June 15 -17, 2008

Choosing the Transistor Widths (assuming a two identical stage amplifier) W [um] Max Gain Choosing the Transistor Widths (assuming a two identical stage amplifier) W [um] Max Gain Min NF [d. B] gs [d. B] NF total [d. B] 20 7. 2 0. 82 0. 3 1. 2 40 8 0. 9 0. 8 1. 3 80 8. 2 1 1. 44 1. 6 RFIC – Atlanta June 15 -17, 2008

High Q Slow Wave Transmission Lines • Effective dielectric constant larger than that of High Q Slow Wave Transmission Lines • Effective dielectric constant larger than that of the surrounding dielectric material • The effective dielectric constant determined by geometry RFIC – Atlanta June 15 -17, 2008

Properties of Slow Wave TL • Isolation from the lossy silicon substrate • Shorter Properties of Slow Wave TL • Isolation from the lossy silicon substrate • Shorter wavelength shorter matching networks • Lower loss per wave length higher Q of resonators • Smaller die area • Higher characteristic impedance • Complicated EM simulations • Complicated layout RFIC – Atlanta June 15 -17, 2008

Measured and Simulated Slow Wave Transmission Line Parameters twice the effective dielectric cons. of Measured and Simulated Slow Wave Transmission Line Parameters twice the effective dielectric cons. of Si. O 2 RFIC – Atlanta June 15 -17, 2008

Properties of Slow Wave Transmission Line RFIC – Atlanta June 15 -17, 2008 Properties of Slow Wave Transmission Line RFIC – Atlanta June 15 -17, 2008

Our Compact Analytic RLCG Model of Slow Wave Transmission Lines *A. Sayag et al. Our Compact Analytic RLCG Model of Slow Wave Transmission Lines *A. Sayag et al. , submitted to TMTT RFIC – Atlanta June 15 -17, 2008

Using our Compact Model to predict Slow wave TL performance RFIC – Atlanta June Using our Compact Model to predict Slow wave TL performance RFIC – Atlanta June 15 -17, 2008

Low Noise Amplifier • All the matching networks are slow wave transmission lines RFIC Low Noise Amplifier • All the matching networks are slow wave transmission lines RFIC – Atlanta June 15 -17, 2008

Measured and Simulated Performance RFIC – Atlanta June 15 -17, 2008 Measured and Simulated Performance RFIC – Atlanta June 15 -17, 2008

Simulated Noise Contributions • Transistors: 70% • Transmissions lines: 23% • Capacitor parasitics: 7% Simulated Noise Contributions • Transistors: 70% • Transmissions lines: 23% • Capacitor parasitics: 7% RFIC – Atlanta June 15 -17, 2008

Comparison with State of the Art LNAs [1] [2] Shih-Chieh. Shin et al. , Comparison with State of the Art LNAs [1] [2] Shih-Chieh. Shin et al. , IEEE Microwave and Wireless Component Letters, July, 2005. E. Adabi et al. , " RFIC Symposium, June 3 -5, 2007, Honolulu, Hawaii. RFIC – Atlanta June 15 -17, 2008

Conclusions • LNA design methodology presented. • New analytic model of slow wave transmission Conclusions • LNA design methodology presented. • New analytic model of slow wave transmission lines. • Record 2. 8 d. B NF @ 24 GHz obtained using 0. 18 μm technology. • Slow wave transmission lines contributed only 23% of the total noise. • Lower NF should be achieved using more advanced technologies RFIC – Atlanta June 15 -17, 2008

Thank You! RFIC – Atlanta June 15 -17, 2008 Thank You! RFIC – Atlanta June 15 -17, 2008

Testing our model: Comparison between Slow Wave Transmission Line and Grounded Coplanar Waveguide Grounded Testing our model: Comparison between Slow Wave Transmission Line and Grounded Coplanar Waveguide Grounded coplanar RFIC – Atlanta June 15 -17, 2008 Slow wave

Comparison of Slow Wave and Grounded Coplanar Waveguide RFIC – Atlanta June 15 -17, Comparison of Slow Wave and Grounded Coplanar Waveguide RFIC – Atlanta June 15 -17, 2008

Comparison between Slow Wave Transmission Line and Coplanar Waveguide RFIC – Atlanta June 15 Comparison between Slow Wave Transmission Line and Coplanar Waveguide RFIC – Atlanta June 15 -17, 2008 slow wave

Comparison between Slow Wave and Coplanar Waveguide RFIC – Atlanta June 15 -17, 2008 Comparison between Slow Wave and Coplanar Waveguide RFIC – Atlanta June 15 -17, 2008