Application of Generalized Scattering Matrix for Prediction of Power Supply Noise
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1 Application of Generalized Scattering Matrix for Prediction of Power Supply Noise System Level Interconnect Prediction 2010 June 13, 2010 K. Yamanaga (1),K. Masu (2), and T. Sato (3) (1) Murata Manufacturing Co., Ltd. (2)Integrated Research Institute, Tokyo Institute of Technology (3) Kyoto University
2 Background 2 Progress of LSI fabrication technologies Low power supply voltage High power consumption Issues caused by power supply noise Deteriorate Signal Integrity (SI) Interference to another circuits, such as RF Reduction of power supply noise is important for interconnect and RF circuits
3 Power supply noise: voltage fluctuation 3 Z(ω) VDD DC Power Supply Capacitor Package & PCB *PCB: Printed Circuit Board LSI I(ω) V(ω) VSS Deteriorate signal timing and integrity of noise source LSI V = ZI
4 Power supply noise: conducted noise Magnetic and electric coupling VDD 4 Another circuit Conducted noise Package & PCB I(ω) VSS LSI Ramifications on another circuit through AC coupling or parasitic antenna
5 5 Purpose of this work Issues Noise analysis is inaccurate and takes too much time Noise measurements are difficult Purpose Propose a simple but accurate method for predicting power supply noise generalized scattering matrix Validate the proposed method through test-chip measurements
6 6 Prediction method of power supply noise
7 Conventional method: Z-parameter of interposer capacitor 7 I Port-1 V 1 Port-2 V 2 V 1 = Z 11 I pkg Voltage fluctuation : Z pkg 11 Conducted noise : Z pkg 21 Effect of complex input/output impedance has not V been considered 2 = Z 21 I pkg
8 Generalized scattering matrix 8 (K. Kurokawa. Power waves and the scattering matrix. microwave Theory and Techniques, IEEE Transactions on, 13(2): , Mar 1965) Z LSI (ω) S pkg (ω) Z PWR (ω) LSI Package PCB S DUT = F( Z DUT 1 F ii =, Gii = 2 Re( Z ) ZDUT i G * )( Z DUT Z i + G) 1 :Impedance matrix of DUT Correction of an S parameter when reference impedances are complex F 1
9 Proposed prediction method 9 Indicator of voltage fluctuation Z = Z sys LSI // Zpkg 11 Impedance calculated by reflection parameter S pkg 11 Prediction parameter of conducted noise S pkg 21 Transmission parameter of generalized S parameter Exact amplitude of power supply noise is not known Useful when evaluating frequency characteristics of different designs (design changes)
10 Experimental validation 10
11 11 Test fixture LSI 180-nm CMOS buffer Flip-chip mount on FR-4 PCB Mimics a package interposer Z SYS S pkg 21 Voltage fluctuation Conducted noise Evaluate the change of above parameters for different ceramic capacitors 2-terminal Multi-terminal Feed-through
12 Measurement configuration 12 Measure conducted noise & input DC power 50MHz pulse Measure voltage fluctuation through direct probing Z SYS and S pkg 21 are individually measured by VNA
13 Measured on-chip voltage fluctuation 13 Time Domain Frequency Domain Peak voltages are almost equal Peak frequencies are different depending on the type of capacitors
14 On-chip voltage fluctuation prediction by a conventional method 14 Peak Peak Voltage fluctuation (measurement) Conventional Z pkg 11 (prediction) Peak frequencies of Z pkg 11 are mis-predicted, which leads to ineffective capacitor placement
15 On-chip voltage fluctuation prediction by the proposed parameter 15 Peak Peak Voltage fluctuation (measurement) Proposed Z SYS (prediction) Peak frequencies of Z sys match with those of voltage fluctuation
16 Measured conducted noise 16 Power Supply Spectrum Analyzer Bias T Conducted Noise Peak frequencies and amplitude are different depending on the type of capacitors Feed-through(blue) capacitor drastically reduce conducted noise
17 Conducted noise prediction by a conventional method 17 Conducted noise (measurement) Conventional Z pkg 21 (prediction) Inaccurate noise peak frequencies of Z pkg 21, which leads to ineffective noise-filter placement
18 Conducted noise prediction by the proposed parameter 18 Conducted noise (measurement) Proposed S pkg21 (prediction) Peak frequencies of S pkg 21 match with that of conducted noise
19 19 Conclusions An application of generalized scattering matrix for prediction of power supply noise has been presented Prediction with the proposed parameter matches better with the measurements compared to the vanilla Z parameter The proposed method contributes to the evaluation of power supply noise in early stage of design flow
20 Equivalent circuit of test fixture 20 2 and Multi-terminal Feed-through Clarify the effect of 3 capacitors to conducted noise
21 Cause of the first resonance First resonance 21 2 and Multi-terminal Series resonance between LSI capacitance and board inductance Feed-through
22 Cause of the difference between 2 and multi-terminal 22 2-terminal: Multi-terminal: 324 ph 144 ph Parasitic Inductance of capacitor only is different Resonance frequencies are shifted due to the different
23 Cause of the difference between 2-terminal and feed-through pH 24.5pF 64pH Parasitic inductance and capacitance becomes small due to insertion in series of feed-through capacitor Second resonance frequency is shifted higher and insertion loss becomes large for feed-through capacitor 5pF
24 2-terminal ceramic capacitor 24 VDD The most commonly used capacitor Behave as short component and minify current loop at high frequency
25 Feed-through ceramic capacitor 25 Regulator VDD VSS PDN LSI VSS VDD Regulator VDD VDD LSI Insert between LSI and regulator in series Drastically reduce conducted noise Behave as normal capacitor at the same time
26 Multi-terminal ceramic capacitor 26 Current Multi-terminal capacitor Magnetic coupling VDD Alternately put VDD and VSS electrodes Drastically reduce inductance using magnetic coupling Structure is the same as feed-through capacitor
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