APEMC 2015 Coupling Analysis and Equivalent Circuit Model of the IC Stripline Method JongTae Hwang1,2, WonJoo Jung1, SoYoung Kim1 1 College of Information and Communication Engineering, Sungkyunkwan University, Suwon, Korea 2 DRAM Solution Team, Memory Division, Samsung Electronics, Hwasung, Korea E-mail: ksyoung@skku.edu Abstract—As portable electronic devices are widely used in wireless communication, analysis of RF interference becomes an essential step for IC designers. In order to test electromagnetic compatibility (EMC) of IC operating at high frequencies, IC stripline method is proposed in IEC standard. This method can be applied up to 3 GHz and covers the testing of ICs and small component. This paper represents simulation results of the open version of IC stripline in 3D EM solver. Also, the coupling effect of IC stripline method is analyzed with S-parameter results. The distributed lumped-element equivalent model is presented for explaining coupling relation between IC stripline and package. This model can be used for quick analysis for EMC of ICs. Keywords—IC stripline, Electromagnetic compatibility (EMC), Circuit model, 3D EM simulation I. INTRODUCTION Recently a variety of ICs has been used in electronic devices with the rapidly increased operating frequency. Also, in wireless communications, stacked ICs and reduced PCB dimension cause more electromagnetic coupling in electronic systems. Because radiated electromagnetic emissions from ICs cause malfunction of electronic systems, it is essential for IC designers to get enough margins for EMC. Over the years, many researchers have been working on EMC analysis of ICs [1]. Until recently, the standard EMC test method is transverse electromagnetic (TEM) cell method according to IEC 61967-2 [2]. This method can be used to measure emission and immunity of PCB level. As the operating frequency of IC increases rapidly, IC stripline method was proposed as a new alternative for radiative emission and immunity test in IEC standard [3], [4]. This method shows higher intensity of electromagnetic emission up to 20 dB better than TEM cell method [5]. The operating frequency of IC stripline is up to 3 GHz. The open-version of IC stripline structure is shown in Figure 1. Active conductor is a source of radiated coupling to device under test (DUT). Also it can be a receptor of radiated noise from DUT. While the closed-version has its housing structure, the open-version has smaller dimension without housing and cheaper cost compared to the closed-version [4]. 978-1-4799-6670-7/15/$31.00 Copyright 2015 IEEE Fig. 1. Simplified open-version structure of IC stripline Simulations and tests to compare the IC stripline method and TEM cell method were done in [5], [6]. The optimization technique for improving voltage standing wave ratio (VSWR) is proposed in [7]. Equivalent circuit models of TEM cell are presented in [8], [9]. Also, equivalent circuit models of IC stripline are examined in [10], [11]. In this paper, the dimension of open-version IC stripline meeting the IEC standard will be proposed with the Sparameter results of 3D EM solver. Also, the dominant coupling factors will be presented by comparing the Sparameter simulation results among different DUTs. With this 3D model of the IC stripline and DUT, equivalent lumpedelement circuit for electromagnetic coupling will be proposed. The paper is structured as follows. Section II presents the structure of open-version IC stripline and DUT model used for modeling. Also, S-parameter analysis results using 3D EM solver are examined. Section III introduces equivalent lumped-element circuit model and its accuracy compared to 3D simulation. Finally, the conclusion is given in Section IV. II. IC STRIPLINE SIMULATION WITH 3D EM SOLVER A. IC stripline structure for simulation According to IEC 62132-8 [4], the goal of IC stripline design is to guarantee VSWR of active conductor less than 1.25 up to 3 GHz. Active conductor consists of upper plane and tapered regions of each side. The tapered region is the main part that causes reflection when increasing VSWR. Shape and angle of tapered region are the parameters for impedance matching. The material used for active conductor is copper. The 0.55 mm FR4 and copper ground plane are used for PCB. The height of the active conductor to ground (H1) is chosen APEMC 2015 from [7], [11]. The structural parameters of IC stripline are shown in Figure 2 and the dimensions are listed in Table I. are designed to be lower than those of the package pins. All the cases are simulated including the IC stripline structure using 3D EM solver. Fig. 2. Structure parameters of IC stripline Fig. 4. 5 types of signal path shapes to model the die inside the QFP package TABLE I. W1 35.20 W2 2.00 DIMENSIONS OF IC STRIPLINE Dimension [mm] L1 L2 58.32 48.00 H1 8.00 H2 7.45 The most critical parameter to meet VSWR target is the thickness of active conductor by 3D EM simulation. The relation between thickness and VSWR is described in Figure 3. The simulation result shows that 1mm thick copper gives the lowest VSWR up to 3 GHz. C. S-parameter analysis using 3D EM solver Longitudinal direction of IC package shows more coupling than transverse direction in [11]. So, S-parameter simulations of longitudinal direction were done with 3D EM solver. Figure 5 shows the port definition of S-parameter simulation. S31 and S41 represent near-end coupling and far-end coupling of DUT. The S31 result of five DUTs using 3D EM solver are shown in Figure 6. Fig. 5. Port definition of S-parameter simulation Fig. 3. Simulation result of VSWR versus copper thickness B. DUT structure for simulation DUT type for simulation is a quad flat package (QFP) which has a dimension of 10×10×2.1 mm. Figure 4 shows five possible ICs or die models that can represent inductance or capacitance dominant interconnects of ICs. Two inductive onchip interconnects, the 12-curved and 6-curved signal lines, represent the inductance dominant on-chip interconnect lines. Small-plate and large-plate cases are representing capacitive interconnects. These two models are developed to better capture the capacitance dominant on-chip interconnects compared to the models developed in [11]. In addition to the signal line, two ground lines are place on both sides to better model the on-chip interconnect structure. The distance between the signal and ground lines are 5 pitches (package pin pitch) apart from signal path in both directions. They are connected to the PCB ground plane through via. In order to minimize the coupling of interconnects, the heights of on-chip interconnects Fig. 6. S31 simulation result of DUTs using 3D EM solver In Figure 6, large-plate line has the largest couplings among five DUTs while 12-curved line shows the least. Highly capacitive signal line tends to receive more radiated noise at the near-end than the inductive one. Figure 7 shows the relation between capacitance and S31 where S31 increase is estimated by | (S31 of each DUT) – (S31 of 12-curved line DUT) | APEMC 2015 The coupling capacitance between the IC stripline and DUT is extracted from 3D EM solver. The trend of the coupling capacitance between stripline and DUT is highly correlated to the S31 increase. conductor and DUT is modeled by mutual inductance and coupling capacitance. The main methodology of creating the equivalent model in this paper follows the modeling concept of [11]. Figure 9 shows the final simplified model of equivalent circuit. A new parameter for the capacitance between middle active conductor and ground, Csl, is added to the previous model. Compared to single LC T-model of [11], distributed lumped-element model can provide more precise results. When using distributed lumped-element model, the number of segments should be determined. Tr is set to 0.1 ns which is the shortest signal rise time derived from the higher test frequency range which is 3GHz. The lengths of coupling dominant region and the side parts are 16 mm respectively. The number of segments of distributed model is calculated as follows. number of segments Fig. 7. Comparison between the S31 increase and the coupling capacitance The S41 results of five DUTs are shown in Figure 8. The straight line shows the highest coupling compared to others. The12-curved line which has the highest inductive coupling and the large-plate that has the highest capacitive coupling shows the least S41 coupling result. The S31 results show about 5~8 dB more coupling at 2 GHz than S41 result. 10 length Tr velocity (1) If the DUT dimension changes, the number of segments for the coupling dominant region needs to be changed. Three DUTs selected for equivalent model are straight line, 12-curved line and large-plate line. The latter two lines represent inductive line and capacitive line, respectively. All parts of DUT including IC, wire and other interconnects are modeled as a distributed lumped-element circuit for analyzing the coupling dominant region. Because the S31 difference between 48mm and 70mm of L2 is under 0.5dB, the effect of tapered region is negligible same as in [11]. Each region consists of 50-cascaded lumped LC elements based on T-model. The LC parameters of Figure 9 are listed in Table II. All parameters of distributed model are validated using 3D EM solver and Raphael [12]. The LC values are further refined by comparing the extracted values of the entire structure and each part. Also, equations in [11] are used to different parameter values for three sections of the IC stripline. Fig. 8. S41 simulation result of DUTs using 3D EM solver The wires which are lower than signal line show 0.5 dB less coupling at 2 GHz compared to the wires which are 0.4 mm higher than signal line in [11]. This result shows that interconnect design should be considered for minimizing EM disturbance. III. SIMULATION OF EQUIVALENT CIRCUIT MODEL A. Definition of equivalent circuit model With the availability of the equivalent circuit model, IC designer can analyze the effect of RF interference at the circuit simulation stage. Also, an intuitive interpretation is possible with LC parameters of equivalent circuit model. In this section, the improved lumped-element LC circuit model is proposed to analyze the coupling between IC stripline and DUT. An equivalent lumped-element circuit of IC stripline is proposed in [11]. In this work, the equivalent circuit models of the three region of the IC stripline, coupling dominant region and other side parts of the active conductor, are replaced by the distributed T-model. Electromagnetic coupling between active Fig. 9. Proposed distributed LC model for coupling TABLE II. PARAMETER OF EQUIVALENT CIRCUIT MODEL Csub [fF] Csl [fF] 43.38 29.04 Straight Line 12-curved Line Large-pate Line Ccoupl [fF] Cic [fF] 1.38 23.66 1.42 22.96 1.78 29.70 Lsub [pH] Lsl [pH] 96.80 114.96 Lic [pH] M [pH] 169.72 7.960 207.76 7.559 138.76 7.672 APEMC 2015 B. S-parameter analysis using equivalent circuit The S-parameter results from the simulation of the equivalent circuit are shown in Figure 10. The coupling characteristics of three DUTs in the equivalent circuit simulation are same as those of the 3D EM simulation. The S31 of large-plate line and the S41 of straight line shows the highest coupling. Because the maximum difference of S31 and S41 among three models is below 3dB, the average parameter of three models can be representing the ICs using same package. IV. CONCLUSION In this paper, the S-parameter analysis results of IC stripline method with different types of DUTs are presented. Among the five DUTs, the DUT with the largest capacitive coupling shows the highest noise injection from IC stripline to package and IC. Also, the equivalent distributed lumped-element circuit model is proposed to model the inductive and the capacitive coupling. This model can accurately predict the S-parameters obtained from 3D EM simulation results. One of the advantages of equivalent circuit model is that IC designer can apply the equivalent circuit model to evaluate the EMC characteristics of DUT. The proposed equivalent circuit represents the coupled electromagnetic field from IC stripline to ICs. Future research includes the fabrication and measurement of IC stripline method for different types of ICs. ACKNOWLEDGEMENT (a) S31 result of equivalent circuit (b) S41 result of equivalent circuit This work was supported by the National Research Foundation of Korea (NRF) grant funded by the Korea government (MSIP) (No. NRF-2014R1A2A2A01006595). Fig. 10. S-parameter result of equivalent circuit The 3D EM and equivalent circuit simulation results of each DUT case are compared in Figure 11. Both simulation results of S31 representing near-end coupling and S41 showing far-end coupling are matched well. This proposed model is applicable to frequencies up to 3 GHz which is the maximum range of IC stripline specified in IEC standards. The comparison between single element and 50 segments of largeplate line case is shown in Figure 11(d). The single element shows the deviation at frequencies over 2GHz. (a) The result of straight line (b) The result of 12-curved line (c) The result of large-plate line (d) Equivalent model comparison Fig. 11. S-parameter comparison between 3D EM solver and equivalent circuit REFERENCES [1] M. Ramdani, E. Sicard, A. Boyer, S. Ben Dhia, J. Whalen, T. Hubing, M. Coenen, and O. Wada, “The electromagnetic compatibility of integrated circuits - past, present, and future,” Electromagnetic Compatibility, IEEE Transactions on, vol. 51, no. 1, pp. 78 –100, feb. 2009. [2] Integrated Circuits Measurement of Electromagnetic Emissions, 150 kHz to 1 GHz- Part 2: Measurement of Radiated Emissions, TEM-cell and Wideband TEM-cell method, IEC 61967-2 First edition, Sep. 2005. [3] Integrated circuits - Measurement of electromagnetic emissions - Part 8: Measurement of radiated emissions - IC stripline method, IEC 61967-8, First edition, Aug. 2011. [4] Integrated circuits - Measurement of electromagnetic immunity - Part 8: Measurement of radiated immunity - IC stripline method, IEC 62132-8, First edition, Jul. 2012. [5] B. Koerber, M. Trebeck, N. Mueller, F. Klotz, and V. Muellerwiebus, “IC-stripline for susceptibility and emission testing of ICs,” Electromagnetic Compatibility of Integrated Circuits (EMC Compo), 7th International Workshop on, Nov. 2009. [6] L. Decrock, J. Catrysse, F. Vanhee, D. Pissoort, “Measuring and simulating EMI on very small components at high frequencies” Electromagnetic Compatibility (EMC EUROPE), 2013 International Symposium on, pp.961–965, Sept. 2013. [7] T. Mandic, R. Gillon, B. Nauwelaers, A. Baric, “Design and modelling of IC-Stripline having improved VSWR performance,” Electromagnetic Compatibility of Integrated Circuits (EMC Compo), 8th International Workshop on, pp. 82–87, Nov. 2011. [8] T. Mandic, R. Gillon, B. Nauwelaers, and A. Baric, “Characterizing the TEM cell electric and magnetic field coupling to PCB transmission lines,” Electromagnetic Compatibility, IEEE Transactions on, vol. 54, no. 5, pp. 976–985, Oct. 2012. [9] T. Mandic, F. Vanhee, R. Gillon, J. Catrysse, A. Baric, “Equivalent Circuit Model of the TEM Cell Electric and Magnetic Field Coupling to Microstrip Lines,” Electronics, Circuit, and System (ICECS), 16th IEEE International Conference on, pp. 247–250, Dec. 2009. [10] T. Mandic, R. Gillon, A. Baric, “IC-stripline design optimization using response surface methodology” Electromagnetic Compatibility of Integrated Circuits (EMC Compo), 9th International Workshop on, pp. 69–73, Dec. 2013. [11] HeeWon Kang, WonJoo Jung, KyungSoo Kim, HyunHo Park, SoYoung Kim, “Equivalent circuit model of the IC-stripline coupling to IC package,” Signal and Power Integrity (SPI), 18th Workshop on, pp.1–4, May. 2014. [12] Raphael, Synopsys, http://www.synopsys.com