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Rajkumar Gehlot, Nidhi Maheshwari, Suruchi Gour / International Journal of Engineering
          Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com
                    Vol. 2, Issue 5, September- October 2012, pp.667-670
     Parallel-coupled-line microstrip band-pass filter using space
                         mapping Technique
    Rajkumar Gehlot (Assistant Professor), Nidhi Maheshwari (Assistant
             Professor), Suruchi Gour (Assistant Professor)
     *Electronics & Communication Engg. Department, Lord Krishna College of Technology, Indore, India
    **Electronics & Communication Engg. Department, Lord Krishna College of Technology, Indore, India
     **Electronics & Communication Engg. Department, Mandsaur Instituted of Technology, Indore, India


Abstract
         Space mapping is a powerful technique to         multi-layer technology can be used as a reduced size
optimize such complex models by efficiently               bandpass filter [6], [7]. However, conventionally the
substituting      accurate       but      expensive       electrical length has been recommended by 45º or
electromagnetic models, fine models, with fast and        less for efficient coupling [8]. Nowadays SAW filters
approximate models, coarse models. In this paper,         are widely used in the mobile communication
we apply space mapping, an explicit space                 market. But they are still not compatible with
mapping techniques to Design, a micro strip pass          standard IC technology and presently available in the
band filter. The filter structure is made of a            frequency range up to 3GHz [9]. An active bandpass
perfect conductor on the top of a substrate               filter can be integrated in single manufacturing
(RT_DURROID_5880) with a relative dielectric              process. In this case, the active circuit which behaves
constant of 2.2 and a height of 20 mil, backed with       as a negative resistance is inserted [10] and has a
a perfect conductor ground plane The proposed             drawback associated with nonlinearity and poor noise
passband filter 9-10 GHz is designed and                  figures [11].
simulated with Advanced Design System                               Considering the development of computer-
(ADS2009) and was implemented with good                   aided design techniques, optimization plays a vital
compactness and low insertion loss.                       role in modeling and design of microwave circuits. A
                                                          typical design problem is to choose the design
Index Terms— ADS, space mapping, microstrip,              parameters to get the desired response. Space
passband filter                                           mapping (SM) approach, introduced by Bindley et al.
                                                          [12], is a powerful technique to optimize complex
    1. INTRODUCTION                                       models. It substitutes efficiently expensive
          In modern wireless communication systems,       electromagnetic models, fine models, with fast and
the miniaturized MMIC microwave bandpass filters          approximate models, coarse models. To obtain the
are required to reduce the cost and lower the efforts     optimal design for the fine model, the SM establishes
of RF system design, especially for single RF             a mapping between parameters of the two models
transceiver chip. Therefore, many studies on reducing     iteratively [12- 13]. SM techniques can be classified
the large size of conventional bandpass filter have       to original or explicit SM [14] and implicit SM (ISM)
been made. The lumped element approach, which             [15] methods. Both methods use an iterative
uses spiral inductor and lumped capacitor, is one of      approach to update the mapping and predict new
the solutions to this problem. However, the design of     design parameters. In this paper, we apply space
lumped element circuits must be somewhat empirical        mapping, an explicit space mapping technique to
and these circuit demonstrations have been confined       Design, a microstrip passband filter. Therefore, a
to frequencies up to few GHz due to the low quality       passband filter can be formed. The proposed
factor (Q) [1] and low resonant frequencies. The          passband filter with passband 9-10 GHz is designed
folded hairpin resonator filters, stepped-impedance       and simulated with Advanced Design System
resonator (SIR) filters [2]-[4] and slow wave open-       (ADS2009).
loop resonator filters [5] were developed. Using these
methods, a relative compact bandpass filter can be        II. MICROSTRIP
designed. However, they still take up quite a large                 One of the main requirements for a
circuit area. Another disadvantage of these traditional   transmission structure to be suitable as a circuit
microstrip filters is that they can’t effectively         element in microwave integrated circuits (MICs) is
suppress the spurious passband, which may seriously       that the structure should be planar in configuration. A
degrade the attenuation level in the stopband and         planar configuration implies that characteristics of
passband response symmetry and could restrict the         the element can be determined by dimensions in a
applicability of the filters.                             single plane. There are several transmission
          Combline filters using low temperature co-      structures that satisfy the requirement of being
fired ceramic (LTCC) or ceramic materials with the        planar. The most common of these are: i) microstrip,



                                                                                                   667 | P a g e
Rajkumar Gehlot, Nidhi Maheshwari, Suruchi Gour / International Journal of Engineering
          Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com
                    Vol. 2, Issue 5, September- October 2012, pp.667-670
ii) coplanar waveguide, iii) slot line, and iv) coplanar   particularly useful characteristics of microstrip
strips. A microstrip is the most popular of these          include the following [16].
transmission structures. The mode of propagation in a      - DC as well as AC signals may be transmitted.
micro strip is almost transverse electromagnetic           - Active devices, diodes and transistors may be
(TEM). This allows easy approximate analysis and           readily incorporated.
yields wide band circuits. The microstrip line has a       - Shunt connections can be made quite easily.
single upper conductor above an infinite ground plate      - In-circuit characterization of devices is relatively
with a dielectric substrate as carrier. Since microstrip   straight forward to implement.
is an open structure, devices can be easily attached to    -Line wave length is reduced considerably (typically
it and post fabrication adjustments can be performed       one-third) from its free space value, because of the
                                                           substrate dielectric constant.
                                                           - The structure is quite rugged and can with stand
                                                           moderately high voltage and power levels.

                                                           III. THE SPACE MAPPING CONCEPT
                                                                     Space Mapping (SM) is a novel concept for
                                                           circuit design and optimization that combines the
                                                           computational efficiency of coarse models with the
                                                           accuracy of fine models. The coarse models are
Figure 1. Microstrip geometry                              typically empirical equivalent circuit engineering
                                                           models, which are computationally very efficient but
         There are several variations of the               often have a limited validity range for their
transmission line configuration that are also found in     parameters, beyond which the simulation results may
MICs. These include coplanar-waveguide (CPW),              become inaccurate. On the other hand, detailed or
inverted microstrip, trapped inverted microstrip and       “fine” models can be provided by an electromagnetic
suspended strip line.                                      (EM) simulator, or even by direct measurements:
                                                           they are very accurate but CPU intensive. The SM
                                                           technique establishes a mathematical link between
                                                           the coarse and the fine models, and directs the bulk of
                                                           CPU intensive evaluations to the coarse model, while
                                                           preserving the accuracy and confidence offered by
                                                           the fine model. The modeling procedure starts with
                                                           optimization of the coarse model to obtain the
                                                           reference point of the region of interest. According to
                                                           star distribution, shown in Figure 1, an n dimensional
                                                           interval centered at the reference point is created.
                                                           Then, the input and output’s mapping parameters are
                                                           calibrated such that multiple sets of responses of the
                                                           SM-based surrogate model match those of the fine
                                                           model, simultaneously. To check the validity of the
                                                           resulting model, it is tested with some test points in
                                                           the region of interest. If the test results are not
                                                           satisfactory, more data should be provided. The SM-
                                                           based surrogate model’s response is generated in
Figure2. Common quasi-TEM mode transmission                specific points over a range of frequencies because
lines: a) microstrip b) slot line c) coplanar waveguide    the size of output mapping matrices is fixed. To
[17].                                                      generate the SM-based surrogate model’s response
                                                           over all points of the frequency range, optimized
          The characteristic impedance range of a          output mapping matrices should be interpolated using
microstrip is typically 20 Ω to 120 Ω. The upper limit     linear frequency interpolation techniques [18]. Then,
is set by technological constraints on the minimum         the resulting model, provided for any frequency
line width that can be realized and the production         sweep, is optimized to determine optimal design
tolerances, while the lower limit is essentially set by    parameters satisfying design specifications.
the appearance of higher order modes. The
fabrication of microstrip circuits is relatively simple
and done with low-cost technology. The dimensions
of microstrip on standard substrates are relatively
large, so that the demand for highly precise
photolithography is not stringent. Some of the




                                                                                                    668 | P a g e
Rajkumar Gehlot, Nidhi Maheshwari, Suruchi Gour / International Journal of Engineering
          Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com
                    Vol. 2, Issue 5, September- October 2012, pp.667-670




Figure 3. Three-dimentional star set for the base          Figure 6. Simulated results of the passband filter by
points                                                     ideal transmission line

                                                           B. Layout and Momentum Simulation
IV.DESIGN AND SIMULATION                            OF
                                                                    After the schematic circuit has been
MICROSTRIP FILTER WITH ADS                                 modified, we created Layout. Figure 7 shows
The structure of the parallel-coupled-line microstrip      Microstrip Layout of the passband filter and Figures
filter is illustrated in Figure 4.                         8, 9 shows S21, S11 of the passband filter by
                                                           Momentum Simulation.




                                                           Figure 7. Microstrip Layout of the passband filter


Figure 4. Parallel-coupled-line microstrip band-pass
filter.

         The filter structure is made of a perfect
conductor     on    the    top    of    a    substrate
(RT_DURROID_5880) with a relative dielectric
constant of 2.2 and a height of 20 mil, backed with a
perfect conductor ground plane. To simplify the
modeling and design procedure by reducing the
number of design parameters, the following
parameters (all in mm) are assumed to be constant.
w0=0.59, w1=0.42, w2=0.52, w3=0.48
L0=3, L1=6, L2=5.8, L3=5.7
s1=0.21, s2=0.42, s3=0.51                                  Figure 8. S21 of the passband filter by Momentum
                                                           Simulation
A. Ideal Transmition line
         We simulated design in ADS using the
above lengths and widths for the microstrip
dimensions. We then used the optimization tool using
our design goal as the goal for optimization. The final
circuit schematic (coarse model) passband filter
shown in Figure 5 and Simulated results of the
passband shown in Figure 6.




                                                           Figure 9. S11 of the passband filter by Momentum
Figure 5. final circuit schematic of the passband filter   Simulation
by ideal transmision line


                                                                                                   669 | P a g e
Rajkumar Gehlot, Nidhi Maheshwari, Suruchi Gour / International Journal of Engineering
          Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com
                    Vol. 2, Issue 5, September- October 2012, pp.667-670
V. CONCLUSIONS                                         pass Filter,” IEEE MTT-S Int. Microwave
         This paper aimed to model a parallel-                     Symp. Dig., pp. 772-775, June 2006.
coupled-line microstrip passband filter simulation          [11]   Jia-Sheng Hong and M.J. Lancaster,
and design parameters. Using explicit space mapping                “Microstrip Filters for RF/Microwave
modeling approach, a surrogate model was used                      Applications,” Advanced Materials and
instead of fine one to simplify the design procedure.              Technologies, pp. 217-219, 2001.
To get satisfactory results, the accuracy of coarse         [12]   J. W. Bandler, R. M. Biernacki, S. H. Chen,
models should be good enough. The proposed                         P. A. Grobelny, and R. H. Hemmers, “Space
passband filter 9-10 GHz is designed and simulated                 Mapping Technique for Electromagnetic
with Advanced Design System (ADS2009) and was                      Optimization”, IEEE Transactions on.
implemented with good compactness and low                          Microwave Theory an Technology, vol. 42,
insertion loss.                                                    pp. 2536–2544, 1994.
                                                            [13]   J. W. Bandler, Q. S. Cheng, S. A. Dakroury,
REFERENCES                                                         A. S. Mohamed, M. H. Bakr, K. Madsen,
  [1]    B. Piernas, K. Nishikawa, T. Nakagawa and                 and J. Søndergaard, “Space Mapping: the
         K. Araki, “Improved Three-Dimensional                     Sstate of the Art”, IEEE Transactions on.
         GaAs Inductors,” IEEE MTT-S Int.                          Microwave Theory and Technology, vol. 52,
         Microwave Symp. Dig., pp. 189-192, May                    pp. 337–361, 2004.
         2001.                                              [14]   J. W. Bandler, Q. S. Cheng, N. K. Nikolova,
  [2]    M. Sagawa, K. Takahashi, and M.                           and M. A. Ismail, “Implicit Space Mapping
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         5, pp. 1929-1936, May 2006.                        [18]   J. W.Bandler, Q. S. Cheng, S. Koziel,
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         2365, 1997.                                               2006; 16(5):518–535.
  [6]    C. W. Tang, Y. C. Lin and C. Y. Chang,
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         10, pp. 2112-2118, Oct 2003.
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  • 1. Rajkumar Gehlot, Nidhi Maheshwari, Suruchi Gour / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 2, Issue 5, September- October 2012, pp.667-670 Parallel-coupled-line microstrip band-pass filter using space mapping Technique Rajkumar Gehlot (Assistant Professor), Nidhi Maheshwari (Assistant Professor), Suruchi Gour (Assistant Professor) *Electronics & Communication Engg. Department, Lord Krishna College of Technology, Indore, India **Electronics & Communication Engg. Department, Lord Krishna College of Technology, Indore, India **Electronics & Communication Engg. Department, Mandsaur Instituted of Technology, Indore, India Abstract Space mapping is a powerful technique to multi-layer technology can be used as a reduced size optimize such complex models by efficiently bandpass filter [6], [7]. However, conventionally the substituting accurate but expensive electrical length has been recommended by 45º or electromagnetic models, fine models, with fast and less for efficient coupling [8]. Nowadays SAW filters approximate models, coarse models. In this paper, are widely used in the mobile communication we apply space mapping, an explicit space market. But they are still not compatible with mapping techniques to Design, a micro strip pass standard IC technology and presently available in the band filter. The filter structure is made of a frequency range up to 3GHz [9]. An active bandpass perfect conductor on the top of a substrate filter can be integrated in single manufacturing (RT_DURROID_5880) with a relative dielectric process. In this case, the active circuit which behaves constant of 2.2 and a height of 20 mil, backed with as a negative resistance is inserted [10] and has a a perfect conductor ground plane The proposed drawback associated with nonlinearity and poor noise passband filter 9-10 GHz is designed and figures [11]. simulated with Advanced Design System Considering the development of computer- (ADS2009) and was implemented with good aided design techniques, optimization plays a vital compactness and low insertion loss. role in modeling and design of microwave circuits. A typical design problem is to choose the design Index Terms— ADS, space mapping, microstrip, parameters to get the desired response. Space passband filter mapping (SM) approach, introduced by Bindley et al. [12], is a powerful technique to optimize complex 1. INTRODUCTION models. It substitutes efficiently expensive In modern wireless communication systems, electromagnetic models, fine models, with fast and the miniaturized MMIC microwave bandpass filters approximate models, coarse models. To obtain the are required to reduce the cost and lower the efforts optimal design for the fine model, the SM establishes of RF system design, especially for single RF a mapping between parameters of the two models transceiver chip. Therefore, many studies on reducing iteratively [12- 13]. SM techniques can be classified the large size of conventional bandpass filter have to original or explicit SM [14] and implicit SM (ISM) been made. The lumped element approach, which [15] methods. Both methods use an iterative uses spiral inductor and lumped capacitor, is one of approach to update the mapping and predict new the solutions to this problem. However, the design of design parameters. In this paper, we apply space lumped element circuits must be somewhat empirical mapping, an explicit space mapping technique to and these circuit demonstrations have been confined Design, a microstrip passband filter. Therefore, a to frequencies up to few GHz due to the low quality passband filter can be formed. The proposed factor (Q) [1] and low resonant frequencies. The passband filter with passband 9-10 GHz is designed folded hairpin resonator filters, stepped-impedance and simulated with Advanced Design System resonator (SIR) filters [2]-[4] and slow wave open- (ADS2009). loop resonator filters [5] were developed. Using these methods, a relative compact bandpass filter can be II. MICROSTRIP designed. However, they still take up quite a large One of the main requirements for a circuit area. Another disadvantage of these traditional transmission structure to be suitable as a circuit microstrip filters is that they can’t effectively element in microwave integrated circuits (MICs) is suppress the spurious passband, which may seriously that the structure should be planar in configuration. A degrade the attenuation level in the stopband and planar configuration implies that characteristics of passband response symmetry and could restrict the the element can be determined by dimensions in a applicability of the filters. single plane. There are several transmission Combline filters using low temperature co- structures that satisfy the requirement of being fired ceramic (LTCC) or ceramic materials with the planar. The most common of these are: i) microstrip, 667 | P a g e
  • 2. Rajkumar Gehlot, Nidhi Maheshwari, Suruchi Gour / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 2, Issue 5, September- October 2012, pp.667-670 ii) coplanar waveguide, iii) slot line, and iv) coplanar particularly useful characteristics of microstrip strips. A microstrip is the most popular of these include the following [16]. transmission structures. The mode of propagation in a - DC as well as AC signals may be transmitted. micro strip is almost transverse electromagnetic - Active devices, diodes and transistors may be (TEM). This allows easy approximate analysis and readily incorporated. yields wide band circuits. The microstrip line has a - Shunt connections can be made quite easily. single upper conductor above an infinite ground plate - In-circuit characterization of devices is relatively with a dielectric substrate as carrier. Since microstrip straight forward to implement. is an open structure, devices can be easily attached to -Line wave length is reduced considerably (typically it and post fabrication adjustments can be performed one-third) from its free space value, because of the substrate dielectric constant. - The structure is quite rugged and can with stand moderately high voltage and power levels. III. THE SPACE MAPPING CONCEPT Space Mapping (SM) is a novel concept for circuit design and optimization that combines the computational efficiency of coarse models with the accuracy of fine models. The coarse models are Figure 1. Microstrip geometry typically empirical equivalent circuit engineering models, which are computationally very efficient but There are several variations of the often have a limited validity range for their transmission line configuration that are also found in parameters, beyond which the simulation results may MICs. These include coplanar-waveguide (CPW), become inaccurate. On the other hand, detailed or inverted microstrip, trapped inverted microstrip and “fine” models can be provided by an electromagnetic suspended strip line. (EM) simulator, or even by direct measurements: they are very accurate but CPU intensive. The SM technique establishes a mathematical link between the coarse and the fine models, and directs the bulk of CPU intensive evaluations to the coarse model, while preserving the accuracy and confidence offered by the fine model. The modeling procedure starts with optimization of the coarse model to obtain the reference point of the region of interest. According to star distribution, shown in Figure 1, an n dimensional interval centered at the reference point is created. Then, the input and output’s mapping parameters are calibrated such that multiple sets of responses of the SM-based surrogate model match those of the fine model, simultaneously. To check the validity of the resulting model, it is tested with some test points in the region of interest. If the test results are not satisfactory, more data should be provided. The SM- based surrogate model’s response is generated in Figure2. Common quasi-TEM mode transmission specific points over a range of frequencies because lines: a) microstrip b) slot line c) coplanar waveguide the size of output mapping matrices is fixed. To [17]. generate the SM-based surrogate model’s response over all points of the frequency range, optimized The characteristic impedance range of a output mapping matrices should be interpolated using microstrip is typically 20 Ω to 120 Ω. The upper limit linear frequency interpolation techniques [18]. Then, is set by technological constraints on the minimum the resulting model, provided for any frequency line width that can be realized and the production sweep, is optimized to determine optimal design tolerances, while the lower limit is essentially set by parameters satisfying design specifications. the appearance of higher order modes. The fabrication of microstrip circuits is relatively simple and done with low-cost technology. The dimensions of microstrip on standard substrates are relatively large, so that the demand for highly precise photolithography is not stringent. Some of the 668 | P a g e
  • 3. Rajkumar Gehlot, Nidhi Maheshwari, Suruchi Gour / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 2, Issue 5, September- October 2012, pp.667-670 Figure 3. Three-dimentional star set for the base Figure 6. Simulated results of the passband filter by points ideal transmission line B. Layout and Momentum Simulation IV.DESIGN AND SIMULATION OF After the schematic circuit has been MICROSTRIP FILTER WITH ADS modified, we created Layout. Figure 7 shows The structure of the parallel-coupled-line microstrip Microstrip Layout of the passband filter and Figures filter is illustrated in Figure 4. 8, 9 shows S21, S11 of the passband filter by Momentum Simulation. Figure 7. Microstrip Layout of the passband filter Figure 4. Parallel-coupled-line microstrip band-pass filter. The filter structure is made of a perfect conductor on the top of a substrate (RT_DURROID_5880) with a relative dielectric constant of 2.2 and a height of 20 mil, backed with a perfect conductor ground plane. To simplify the modeling and design procedure by reducing the number of design parameters, the following parameters (all in mm) are assumed to be constant. w0=0.59, w1=0.42, w2=0.52, w3=0.48 L0=3, L1=6, L2=5.8, L3=5.7 s1=0.21, s2=0.42, s3=0.51 Figure 8. S21 of the passband filter by Momentum Simulation A. Ideal Transmition line We simulated design in ADS using the above lengths and widths for the microstrip dimensions. We then used the optimization tool using our design goal as the goal for optimization. The final circuit schematic (coarse model) passband filter shown in Figure 5 and Simulated results of the passband shown in Figure 6. Figure 9. S11 of the passband filter by Momentum Figure 5. final circuit schematic of the passband filter Simulation by ideal transmision line 669 | P a g e
  • 4. Rajkumar Gehlot, Nidhi Maheshwari, Suruchi Gour / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 2, Issue 5, September- October 2012, pp.667-670 V. CONCLUSIONS pass Filter,” IEEE MTT-S Int. Microwave This paper aimed to model a parallel- Symp. Dig., pp. 772-775, June 2006. coupled-line microstrip passband filter simulation [11] Jia-Sheng Hong and M.J. Lancaster, and design parameters. Using explicit space mapping “Microstrip Filters for RF/Microwave modeling approach, a surrogate model was used Applications,” Advanced Materials and instead of fine one to simplify the design procedure. Technologies, pp. 217-219, 2001. To get satisfactory results, the accuracy of coarse [12] J. W. Bandler, R. M. Biernacki, S. H. Chen, models should be good enough. The proposed P. A. Grobelny, and R. H. Hemmers, “Space passband filter 9-10 GHz is designed and simulated Mapping Technique for Electromagnetic with Advanced Design System (ADS2009) and was Optimization”, IEEE Transactions on. implemented with good compactness and low Microwave Theory an Technology, vol. 42, insertion loss. pp. 2536–2544, 1994. [13] J. W. Bandler, Q. S. Cheng, S. A. Dakroury, REFERENCES A. S. Mohamed, M. H. Bakr, K. Madsen, [1] B. Piernas, K. Nishikawa, T. Nakagawa and and J. Søndergaard, “Space Mapping: the K. Araki, “Improved Three-Dimensional Sstate of the Art”, IEEE Transactions on. GaAs Inductors,” IEEE MTT-S Int. Microwave Theory and Technology, vol. 52, Microwave Symp. Dig., pp. 189-192, May pp. 337–361, 2004. 2001. [14] J. W. Bandler, Q. S. Cheng, N. K. Nikolova, [2] M. Sagawa, K. Takahashi, and M. and M. A. Ismail, “Implicit Space Mapping Kakimoto, “Miniaturized hairpin resonator Optimization Exploiting Preassigned filters and their application to receiver front- Parameters”, IEEE Transactions on. end MICs,” IEEE Trans. Microwave Theory Microwave Theory and Technology, vol. 52, Tech., vol. 37, pp. 1991-1997, 1989. pp. 378–385, 2004. [3] M. Makimoto and S. Yamashita, “Bandpass [15] S. Koziel, Q. S. Cheng, and J. W. Bandler, filters using parallel coupled strip-line “Space Mapping”, IEEE Microwave stepped impedance resonators,” IEEE Trans. Magazine, pp.105-122, Dec. 2008 Microwave Theory Tech., vol. MTT-28, no. [16] Terry Edwards, Foundations for microstrip 12, pp. 1413–1417, Dec 1980. circuit design. New York: Wiley- [4] A. Djaiz and T. A. Denidni, “A new Interscience, 1991. compact microstrip two-layer bandpass filter [17] R. K. Mongia, I. J. Bahl, P. Bhartia and J. using apertured-coupled SIR-hairpin Hong, RF and microwave coupled-line resonators with transmission zeros,” IEEE circuits. Norwood, MA: Artech House, Trans. Microwave Theory Tech., vol. 54, no. 2007. 5, pp. 1929-1936, May 2006. [18] J. W.Bandler, Q. S. Cheng, S. Koziel, [5] J. S. Hong and M. J. Lancaster, “Theory and “Simplified Space Mapping Approach to experiment of novel microstrip slow-wave Enhancement of Microwave Device open- loop resonator filters,” IEEE Trans. Models”. International Journal of RF and Microwave Theory Tech., vol. 45, pp. 2358- Microwave Computer- Aided Engineering 2365, 1997. 2006; 16(5):518–535. [6] C. W. Tang, Y. C. Lin and C. Y. Chang, “Realization of transmission zeros in combline filters using an auxiliary inductively coupled ground plane,” IEEE Trans. Microwave Theory Tech., vol. 51, no. 10, pp. 2112-2118, Oct 2003. [7] A. Kundu and N. Mellen, “Miniaturized Multilayer Bandpass Filter with multiple Transmission Line Zeros”, IEEE MTT-S Int. Microwave Symp. Dig., pp. 760-763, June 2006. [8] G. Matthaei, L. Young, E. M. T. Jones, Microwave Filters, Impedance-Matching networks, and Coupling Structures. Artech House, pp. 500, 1980. [9] A. Hussain, Advanced RF Engineering for Wireless systems and Network, Wiley, pp. 262, 2005. [10] C. Tzuang, H. Wu, H. Wu and J. Chen, “A CMOS Miniaturized C-Band Active Band 670 | P a g e