Research Journal of Applied Sciences, Engineering and Technology 4(6): 670-674, 2012 ISSN: 2040-7467 © Maxwell Scientific Organization, 2012 Submitted: December 06, 2011 Accepted: December 26, 2011 Published: March 15, 2012 Application of Implicit Space Mapping in the Design of Hammerhead Filter in Millimeter-Wave Band Fuqun Zhong, Bo Zhang, Yong Fan, Minghua Zhao and Guan Gui School of Electronic Engineering, University of Electronic Science and Technology of China, Chengdu, 611731, China Abstract: In this study, we present advances in microwave and millimeter-wave device modeling exploiting the Space Mapping (SM) technology. New SM-based modeling techniques are used that are easy to implement entirely in the Agilent ADS framework. The implicit space mapping algorithm is applied to the design of hammerhead filter in millimeter-wave band. The validity of this method is confirmed by comparison with fullwave EM simulation result and measured data. Based on the proposed method, a filter was designed and fabricated on a substrate with thickness of 0.254 mm and dielectric constant of 2.2. The experimental results show good agreement with simulated results. It is proved that the accuracy can be achieved using the implicit space mapping algorithm, and the design efficiency can be greatly improved. Key words: Accuracy and high efficiency, hammerhead filter, implicit space mapping algorithm INTRODUCTION of reducing CPU demand. Implicit Space Mapping (SM) technology (Bandler et al., 2004) addresses the issue of reducing the time-consuming full-wave Electromagnetic (EM) simulations of microwave structures with the help of a fast physics-based model or surrogate for device modeling and optimization. In the design of microstrip hammerhead filter, coarse models are realized in Agilent ADS. We use HFSS as the fine model evaluators. Agilent ADS schematics organize the ADS optimization engine and coarse and fine models to perform parameter extraction and surrogate optimization. In this study, we adopt the simplified space mapping implementation in Agilent ADS, all the space mapping steps are integrated into ADS schematic. The processing of design for microstrip hammerhead filter was described. Filters play an important role in the successful operation of millimeter and submillimeter-wave mixers and frequency multipliers (Xue et al., 2003; Marsh et al., 2007; Porterfield, 2007; Maestrini and Ward, 2008; Zhang et al., 2011; Zhong et al., 2011a,b). Many simple filters can be designed with direct full-wave electromagnetic (EM) simulation optimization. However, occasionally it is necessary to achieve a larger bandwidth of operation and a greater level of stopband rejection which often involves the use of more complicated filter geometries which would spend so much time doing the direct EM optimization. The relative simplicity and flexibility of the implicit space mapping algorithm make it a particalarly attractive tool for design of these more complex circuits. The microstrip hammerhead filter has been an attractive candidate for use in wide stop-band mixer and frequency multiplier circuits since its introduction many years ago (MaMaster et al., 1976). Compared with the traditional low-and-high-impedance microstrip filter, the microstrip hammerhead filter is characterized by lowinsertion loss, sharp rejection, shorter size and wider stopband. These superior characteristics can be used to improve the performance of the mixer and multiplier in microwave and millimeter-wave band. However, complex structures, too much variables and absence of a simple and quick method for design have hindered its widespread use. Electromagnetic (EM) simulation is accurate, but CPU intensive; hence, using a full-wave EM simulators such as Ansoft HFSS, or Agilent Momentum, in the hope Implicit space mapping algorithm: The formulation of the implicit space mapping algorithm is presented in (Bandler et al., 2004; Cheng et al., 2009). A fine model optimal solution can be expressed as: x * = arg min U ( R f ( x )) x (1) where, Rf (x) is fine-model response vector, U is typically a minimax objective function with upper and lower specifications (Zhu et al., 2007), x is fine-model design parameters, and x* is the optimal design to be determined. In order to solve Eq. (1), the following iterative procedure is used by implicit space mapping: x k +1 = arg min U ( Rc ( x , p k )) x (2) Corresponding Author: Fuqun Zhong, School of Electronic Engineering, University of Electronic Science and Technology of China, Chengdu, 611731, China 670 Res. J. Appl. Sci. Eng. Technol., 4(6): 670-674, 2012 where, Rc (x, p) is a response vector of the coarse model with x and p being the design variables and preassigned parameters, respectively, Rc (x, pk) is an implicit space mapping surrogate model with preassigned parameters pk obtained at iteration k using the parameter extraction procedure. p k = arg min R f ( x k ) − Rc ( x k , p) (3) p In which we try to match the surrogate to the fine model. The initial surrogate model is Rc (x, p0), where p0 represents the initial preassigned parameter values. In other words, the surrogate model is the coarse model with updated values of the preassigned parameters. From the above derivation of the formulation of the implicit space mapping algorithm, we can find that our goal is to obtain the fine model optimal design without going to direct optimization of the fine model but instead using the surrogate model; i.e., the coarse model with updated values of the preassigned parameters. Parameter extraction and design optimization are performed solely on the surrogate model. A prediction of the next fine model design is also obtained through the surrogate. Fig. 1: The structure of microstrip hammerhead filter. ADS schematic design framework: We implement implicit space mapping optimization in the ADS schematic framework in an interactive way to greatly raise efficiency of microstrip hammerhead filter design. The space mapping implemented in 5 steps is as fellows: Step 1: Set up and optimize the coarse model in ADS schematic Step 2: Create the parameterized fine model in HFSS, the structure dimension is same as the value obtained in Step1 GOAL Goal OptimGoal6 Expr="sub_wide" SimInstanceName="S P1" Min= Max=9 Weight=1000 RangeV ar[1]= RangeMin[1]= RangeMax[1]= S-P ARAMETERS MSub S_Param SP1 Start=0 GHz Stop=9 GHz Step=1 GHz Meas Eqn MSUB MSub1 H=1.27 mm Er=2.2 Mur=1 Cond=5. 8E+7 Hu=3.73 mm T=90 um TanD=0. 0009 Var Eqn MeasEqn Meas1 sub_wide=W1+2* W3+2*L2 banch_long=L2-L4 structure=L1-W3-L3 cent er_structure=L5-2*(L3+W3) V AR V AR1 GOAL W1=1.65728 {o} L4=0.8147 {o} W2=0.603471 {o} W3=1.13307 {o} L3=1.85819 {o} L1=4.09479 {o} L5=10.8342 {o} L2=2.51905 {o} Rough=0 mil W=0. 7 mm L=1 mm Min=1 Max= Weight=1/0. 01 RangeVar[1]= RangeMin[1]= RangeMax[1]= MCORN Corn2 Subst="MSub1" Subst="MSub1" W=W3 mm L=L3 mm TL3 Subst="MS ub1" W=W2 mm L=L2 mm MLIN TL2 Subst="MSub1" MSTEP Step2 Subst="MS ub1" W1=W1 mm W2=0.7 mm W=W1 mm L=L1 mm MLIN TL9 S ubst="MSub1" W=W3 mm L=L3 mm MLOC TL26 Subst="MSub1" W=W3 mm L=L4mm L=L4 mm Subst="MSub1" W=W3 mm L=L3 mm TL29 Subst="MSub1" W=W2 mm L=L2 mm W=W1 mm L=L5 mm W1=W1 mm W2=W2 mm W3=W1 mm W4=W2 mm MLIN TL11 Subst="MSub1" W=W3mm L=L3 mm MCORN Corn4 Subst="MSub1" W=W3 mm MCORN Corn12 Subst="MSub1" W=W3 mm Fig. 2: The coarse model in ADS 671 MCORN Corn9 Subst="MSub1" Subst="MSub1" W=W3 mm L=L3 mm W1=W1 mm W2=W2 mm W3=W1 mm W4=W2 mm MTE E_ADS Tee2 Subst="MSub1" W1=W3mm W2=W3mm W3=W2mm SaveSolns=yes SaveGoals=yes SaveOptimVars=no UpdateDataset=yes MLIN MCROSO Cros2 S ubst="MSub1" MLOC TL31 Subst="MSub1" W=W3 mm L=L4 mm UseAllGoal s=yes SaveCurrentEF=no SaveNominal=no SaveAllIterations=no UseAllOptV ars=yes MLIN TL27 MLIN TL13 S ubst="MSub1" MLOC TL12 Subst="MSub1" W=W3 mm L=L4 mm Optim Optim1 OptimType=Random MaxIters=10000 DesiredError=0.0 StatusLevel=4 FinalAnalysis="SP1" NormalizeGoals=no SetBestValues=yes Seed= W=W3mm MLIN TL28 MLOC TL8 Subst="MSub1" W=W3 mm Goal OptimGoal5 Expr="center_structure" SimInstanceName="SP1" Min=1 Max= Weight=1/0.01 RangeVar[1]= RangeMin[1]= RangeMax[1]= MTEE_ADS Tee5 Subst="MSub1" W1=W3 mm W2=W3 mm W3=W2 mm MCORN Corn10 S ubst="MSub1" W=W3 mm OPTIM GOAL Goal OptimGoal4 E xpr="structure" S imInstanceName="SP1" Min=1 Max= Weight=1/0.01 RangeVar[1]= RangeMin[1]= RangeMax[1]= MCROSO Cros1 Subst="MSub1" MLIN TL4 Subst="MS ub1" W=W2 mm L=L2 mm MLOC TL10 S ubst="MSub1" W=W3 mm L=L4 mm MCORN Corn3 Subst="MSub1" W=W3 mm Min= Max=-25 Weight=1 RangeVar[ 1]="freq" RangeMin[ 1]=7 GHz RangeMax[1]=9 GHz MLIN L=L4 mm MLIN TL1 Subst="MSub1" Min= Max=-20 Weight=1/0.09 RangeVar[1]="freq" RangeMin[1]=0 GHz RangeMax[1]=3 GHz MLIN TL6 Subst="MS ub1" W=W3 mm L=L3 mm MLOC TL7 Subst="MSub1" W=W3 mm Term Term1 Num=1 Z=50Ohm Goal OptimGoal3 Expr="banch_long" SimInstanceName="SP1" W=W3 mm MLIN TL5 GOAL GOA L Goal OptimGoal 2 Expr="dB(S (2,1))" SimInstanceName="SP 1" MTEE_ADS Tee1 Subst="MSub1" W1=W3 mm W2=W3 mm W3=W2 mm MCORN Corn1 Subst="MS ub1" W=W3 mm GOAL Goal OptimGoal1 E xpr="dB(S(1,1))" S imInstanceName="SP1" L=L4 mm MS TEP Step12 Subst="MSub1" W1=W1 mm W2=0.7 mm MLIN TL34 Subst="MSub1" W=W2 mm L=L2 mm MLIN TL33 Subst="MSub1" W=W3 mm L=L3 mm MLOC TL25 Subst="MSub1" W=W3 mm MLOC TL30 Subst="MSub1" W=W3 mm L=L4 mm MTEE_A DS Tee6 Subst="MSub1" W1=W3 mm W2=W3 mm W3=W2 mm MLIN TL32 Subst="MSub1" W=W3 mm L=L3 mm MCORN Corn11 Subst="MSub1" W=W3 mm MLIN TL24 Subst="MSub1" W=0.7mm L=1 mm Term Term2 Num=2 Z=50 Ohm Res. J. Appl. Sci. Eng. Technol., 4(6): 670-674, 2012 S-PARAMETERS MLOC TL7 Subst="MSub1" W=W3 mm L=L4 mm Term Term1 Num=1 Z=50 Ohm MLIN TL1 Subst="MS ub1" W=0.7 mm L=1mm MLIN TL5 S ubst="MSub1" W=W3 mm L=L3 mm MCORN Corn2 Subst="MSub1" W=W3 mm MLIN TL6 Subst="MSub1" W=W3 mm L=L3 mm MCORN Corn3 Subst="MSub1" W=W3 mm MLIN TL9 Subst="MSub1" W=W3 mm L=L3 mm MLOC TL12 Subst="MSub1" W=W3 mm L=L4 mm MTEE_ADS Tee2 Subst="MSub1" W1=W3 mm W2=W3 mm W3=W2 mm MLIN TL11 Subst="MSub1" W=W3 mm L=L3mm Term Term3 Num=3 Z=50 Ohm VA R VA R2 E1=2.0213 {o} H1=0.539067{o} MCORN Corn9 S ubst="MSub1" W=W3 mm MLIN TL28 Subst="MS ub1" W=W3mm L=L3 mm MLIN TL27 Subst="MSub1" W=W3 mm L=L3 mm MLIN TL29 Subst="MS ub1" W=W2 mm L=L2 mm MLOC TL25 Subst="MSub1" W=W3 mm L=L4 mm MSTEP S tep12 S ubst="MSub1" W1=W1 mm W2=0.7 mm MCROSO Cros2 S ubst="MSub1" W1=W1 mm W2=W2 mm W3=W1 mm W4=W2 mm MLIN TL34 Subst="MS ub1" W=W2mm L=L2 mm MLOC TL31 Subst="MSub1" W=W3 mm L=L4 mm MCORN Corn4 Subst="MSub1" W=W3 mm Var Eqn MTE E_ADS Tee5 Subst="MSub1" W1=W3 mm W2=W3 mm W3=W2 mm MCORN Corn10 Subst="MSub1" W=W3 mm MLIN TL13 S ubst="MSub1" W=W1 mm L=L5 mm MLIN TL4 S ubst="MSub1" W=W2 mm L=L2 mm MLOC TL10 Subst="MSub1" W=W3 mm L=L4 mm Goal OptimGoal1 Expr="abs(db(S(2,1))-db(S(4,3)))" SimInstanceName="SP 1" Min= Max=0 Weight= RangeV ar[1]= RangeMin[1]= RangeMax[1]= MLOC TL26 S ubst="MSub1" W=W3mm L=L4 mm MCROSO Cros1 Subst="MSub1" W1=W1 mm W2=W2 mm W3=W1 mm W4=W2 mm VAR VAR1 W1=1.66 {-o} L4=0.81 {-o} W2=0.6 {-o} W3=1.13 {-o} L3=1.86 {-o} L1=4.09 {-o} L5=10.83 {-o} L2=2.52 {-o} Var Eqn GOAL Optim Optim1 OptimType=GradientSaveCurrentEF=no MaxIters=100 DesiredError=0.0 S tatusLevel=4 FinalAnalysis="S P1" NormalizeGoals=no S etB estV alues=yes S aveS olns=yes S aveGoals=yes S aveOptimVars=no UpdateDataset=yes S aveNominal=no S aveA llIterations=no UseAllOptV ars=yes UseAllGoals=yes MLOC TL8 Subst="MSub1" W=W3 mm L=L4 mm MLIN TL3 S ubst="MSub1" W=W2 mm L=L2 mm MLIN TL2 Subst="MSub1" W=W1 mm L=L1 mm MSTEP S tep2 S ubst="MSub1" W1=W1 mm W2=0.7 mm MSUB MSub1 H=H1mm E r=E1 Mur=1 Cond=5.8E+7 Hu=3.73 mm T=90 um TanD=0.0009 Rough=0 mil MTEE_ADS Tee1 Subst="MS ub1" W1=W3 mm W2=W3 mm W3=W2 mm MCORN Corn1 S ubst="MS ub1" W=W3 mm OP TIM MSub S_Param SP1 Start=0 GHz Stop=9 GHz Step=1 GHz MCORN Corn12 Subst="MS ub1" W=W3 mm MLIN TL33 Subst="MS ub1" W=W3 mm L=L3 mm MLIN TL24 Subst="MSub1" W=0.7 mm L=1mm Term Term2 Num=2 Z=50 Ohm MLOC TL30 Subst="MSub1" W=W3mm L=L4 mm MTEE_A DS Tee6 S ubst="MSub1" W1=W3 mm W2=W3 mm W3=W2 mm MLIN TL32 Subst="MSub1" W=W3 mm L=L3 mm MCORN Corn11 S ubst="MSub1" W=W3 mm Term Term4 Num=4 Z=50 Ohm S2P SNP 1 File="C:\design_THz\wenzhang\cmrc_SM\cmrc_ori_scale_model_ori.s2p" 1 2 Re f Fig. 3: Parameter extraction in ADS Surrogate responses Fine responses Surrogate responses Fine responses 20 0 0 -20 -20 | S21| in dB | S21| indB 20 -40 -40 -60 -60 -80 -80 -100 -100 0 1 2 3 7 5 6 4 Frequence (GHz) 8 9 0 10 (a) 1 2 3 7 5 6 4 Frequence (GHz) 8 9 10 (b) Fig. 4: (a) The response of our initial tuning model and fine model,. (b) The response of our tuning model and fine model after the first iteration of the fine model and coarse model is very small; if Step 3: Simulate the fine model and import the S parameter into ADS. Check the stopping criteria which are that the difference between responses satisfied, stop. Otherwise, optimize ADS coarse model to match fine model to perform parameter extraction Step 4: Reoptimize the calibrated coarse model design parameters to predict the next fine model design Step 5: Update the fine model design and go to Step3 0.254 mm, dielectric constant is er = 2.2, loss tangent is 0.0009, and the metallization is copper. The design specifications are # S11#< - 15 dB for DC #w#15 GHz, and # S21##- 25 dB for 35GHz #w# 45GHz. Because the microstrip hammerhead filter works at high frequency, we use the scale model with scale factor of 5 to improve the accuracy of the coarse model in ADS. In this design, the fine model is simulated in Ansoft HFSS, the coarse model is constructed and optimized in Agilent ADS (Fig. 2). The initial guess is x(0) = [4.09, 2.52, 1.86, 0.81, 10.83, 1.66, 0.6, 1.13]T, the response of our initial tuning model and fine model is shown in Fig. 4a. One of the most important steps, parameter extraction, is implemented entirely in ADS (Fig. 3). We compensate the deviation between the tuning model and the fine model Design of microstrip hammerhead filter: Microstrip hammerhead filter with a rogers 5880 substrate is shown in Fig. 1. Design parameters are x = [L1, L2, L3, L4, L5, W1, W2, W3]T mm. Thickness of the substrate is H = 672 Res. J. Appl. Sci. Eng. Technol., 4(6): 670-674, 2012 model and the corresponding fine model are shown in Fig. 5. Clearly, difference between responses of the fine model and coarse model is very small. After structure dimensions of the scale model are divided by the scale factor of 5, we can get the final microstrip hammerhead filter satisfying the design specifications, which will be fabricated in section 5. Surrogate responses Fine responses 10 |S21| in dB 0 -10 -20 -30 Filter measurement: The hammerhead filter is fabricated using current microelectronics technology without any additional process, and the entire physical configuration of filter circuit is shown in Fig. 6a, The dimensions of microstrip hammerhead filter are as follows: L1 = 0.5 mm, L2 = 0.71 mm, L3 = 0.2 mm, L4 = 0.24 mm, L5 =1.53 mm, W1 = 0.18 mm, W2 = 0.1 mm, W3 = 0.1 mm. The measured S-parameter is shown in Fig. 6b. The LPF with two hammerhead cells in series has a 25 GHz stopband from 25 to 50 GHz. This achieves above 100% (-10 dB) relative bandwidth. As can be seen from Fig. 6b, the insertion loss from DC to 20 GHz is less than 1.1 dB, and the return loss is better than 18 dB in the passband. -40 -50 0 1 2 3 7 5 6 4 Frequence (GHz) 8 9 10 Fig. 5: The optimized tuning model and the corresponding fine model responses. CONCLUSION In this study we reviewed the implicit space mapping concept and adopt the simplified space mapping implementation in Agilent ADS, all the space mapping steps are integrated into one ADS schematic. A detailed and easy-to-follow design optimization procedure was provided and the Agilent ADS implementation of the algorithm was described. Implicit SM algorithm greatly improves the efficiency of the design of complex structure. It will create favorable conditions for the widespread use of microstrip hammerhead filter in field of mixer and frequency multiplier. (a) |S21| in dB 0 -20 -40 -60 ACKNOWLEDGMENT -80 0 10 20 40 Frequence (GHz) 50 This study is supported by the National Natural Science Foundation of China under Grant No.61001030 and supported by The Fundamental Research Funds for the Central Universities under Grant No. ZYGX2009J022 60 (b) Fig. 6: (a) Photograph of hammerhead filter, (b) The measurement result of hammerhead filter REFERENCES by calibrating the dielectric constant er and the height H of the substrate as tuning parameters. We can see that the specification is not satisfied after the first iteration, but the parameter extraction using implicit SM yields a good match between the coarse and fine models (Fig.4b). The coarse model is then optimized in ADS with respect to the design parameter. The new design parameters are assigned to the fine model. The optimal values obtained are x* = [2.52, 3.55, 1.01, 1.18, 7.64, 0.9, 0.5, 0.5]T mm after three iterations. The responses of optimized tuning Bandler, J.W., Q.S. Cheng, N.K. Nikolova and M.A. Ismail, 2004. Implicit space mapping optimization exploiting preassigned parameters. IEEE Trans. Microwave Theory Tech., 52(1): 378385. Cheng, Q.S., J.W. Bandler and J.E. Rayas-Sanchez, 2009. Tuning-aided implicit space mapping. Int. J. RF Microwave Computer-Aided Eng., 18(5). Maestrini, A. and J.S. Ward, 2008. In-phase powercombined frequency triplers at 300 GHz. IEEE Microwave Wireless Component. Lett., 18(3). 673 Res. J. Appl. Sci. Eng. Technol., 4(6): 670-674, 2012 MaMaster, L.L., M.V. Schneider and W.W. Snell, 1976. Millimeter-wave receivers with subharmonic pump. IEEE Trans. Microwave Theory Tech., MTT-24, 12: 948-952. Marsh, S., B. Alderman, D. Matheson and P. de Maagt, 2007. Design of low-cost 183 GHz subharmonic mixers for commercial applications. IEEE Circ. Device Syst., 1(1). Porterfield, D.W., 2007. High-efficiency terahertz frequency triplers. Microwave Symposium, IEEE/MTT-S International. Xue, Q., K.M. Shum and C.H. Chan, 2003. Low conversion-loss fourth subharmonic mixers incorporating CMRC for millimeter-wave applications. IEEE Trans. MTT, 51(5). Zhang, B., Y. Fan, Z. Chen, X.F. Yang and F.Q. Zhong, 2011. An improved 110-130 GHz fix-tuned subharmonic mixer with compact microstrip resonant cell structure. J. Electromagnetic. Waves Appl., 25: 411-420. Zhong, F., Z. Bo, F. Yong, Z. Minghua and Y. Xiaofan, 2011a. A broadband W-band subharmonic mixers circuit based on planar schottky diodes. IEEE International Conference on Opto-Electronics Engineering and Information Science. Zhong, F.Q., B. Zhang, Y. Fan, M.H. Zhao and X.F. Yang, 2011b. 170 GHz high-efficiency frequency doubler. IEEE International Symposium on Microwave, Antenna, Propagation and EMC Technologies for Wireless Communications. Zhu, J., J.W. Bandler, N.K. Nikolova and S. Koziel, 2007. Antenna optimization through space mapping. IEEE Trans. Antennas Propag, 55(3): 651-658. 674