# Inkjet-Printed Interdigital Bandpass Filter with Wide Stopband Using Multilayer Liquid Crystal Polymer Technique

Authors: Li-Chun Chang; Cheng-Lin Cho; Sameer Kamrudin Bachani; Hsuan-Ling Kao
Journal: International Journal of Antennas and Propagation
 (2018)

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## Abstract

This article presents a two-layer inkjet-printed interdigital bandpass filter using lamination bonding process on liquid crystal polymer (LCP) substrates for radio frequency electronic applications. Various percentages of torque force were applied over a 4 × 4 cm2 area with a 942 kg fixed force in the lamination bonding process. The insertion loss and surface morphology of the inkjet-printed silver film were examined on various torque forces to develop the lamination bonding process. The lamination bonding was performed at 12% torque and 270°C. A three-dimensional bandpass filter was realized with a S21 of −2.2 dB at 11.5 GHz with a 17% fractional bandwidth. A multilayer inkjet-printed bandpass filter was successfully developed to verify the design methodology and fabrication of inkjet-printing technology and lamination bonding technique for a three-dimensional integrated circuit package.


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## Body

## 1. Introduction

Three-dimensional (3D) technologies [1–3] provide more designs and compact sizes for radio frequency (RF) and millimeter wave devices. Low-temperature cofired ceramic (LTCC) packaging method is useful for microwave applications because of excellent physical and electrical properties [3–5]. However, the sintering temperature of LTCC should be at the level of 850°C. Compared to printed circuit board, the cost of LTCC is expensive. Recently, liquid crystal polymers (LCPs) have become a favorable material for RF applications because of an impressive loss tangent, lower thermal expansion coefficient, and lower moisture absorption. Additionally, the dielectric constant of LCP is 2.9, which is lower than that of LTCC [6, 7] and is favorable for multilayer lamination because it provides more tolerances for registration error. Several authors have presented studies on the ultrawideband bandpass filter using multilayer LCP technology at different frequencies [6, 8]. Multilayer inductors and capacitors using LCP technology have been demonstrated for high-pass filter design [7, 9]. A low-loss integrated waveguide bandpass filter using LCP substrate was published to provide an inexpensive low-loss hermetic packaging solution [10]. No losses were recorded over a frequency range of 25 GHz and 15 GHz for coplanar waveguide (CPW), and microstrip via transitions were examined, respectively [11]. Therefore, multilayer LCP technologies are suitable for RF applications.Inkjet printing technology has gained popularity because of its cost-effective direct-write technology and being environmentally friendly. Several studies on the implementation and characterization of inkjet-printed silver film on an LCP substrate have been conducted [12, 13]. In our study, the multilayer LCP technology was utilized at high torque forces and a high temperature. The strength of the inkjet-printed silver film at various torque forces was studied. According to the strength results, a multilayer inkjet-printed interdigital bandpass filter was realized to demonstrate a high performance and cost-effective integration circuit for electronic package applications. This paper is organized as follows. Section 2 describes the processes for fabricating the inkjet-printed silver film and the lamination bonding process for multilayer LCP substrates. Section 3.1 focuses on the insertion loss and surface morphology of inkjet-printed silver film under various torque forces. Section 3.2 describes the structure and fabrication of the multilayer bandpass filter. In Section 4, we provide the conclusions.


## 2. Fabrication Process

Figure1 illustrates the process flow of inkjet printing and lamination bonding for three-dimensional interdigital bandpass filter. DGP-40LT-15C silver ink was used to print the metal layers using a DMP-2800 inkjet printer. Two types of Rogers LCP substrates including ULTRALM 3850 (core film) and 3908 bondply (bonding film) were adopted which have similar thermal expansion and dielectric constants [14]. The steps for fabricating the inkjet-printed three-dimensional interdigital bandpass filter are as follows:
(1)
Plasma polymerization process was applied at 3 W, 5 s for surface treatment.
(2)
Ten-pass silver ink was printed at 60°C onto the front of the core.
(3)
Three vias were drilled in the core film for subsequent alignment.
(4)
The LCP was flipped to layer 2 and treated by plasma polymerization.
(5)
Layer 2 was aligned using the horizontal vias, and then the intersected vertical via was the starting point for layer 2 printing.
(6)
The backside of the silver film was printed.
(7)
The double-sided silver films were subjected to 270°C for 1 h.
(8)
A two-layer inkjet-printed silver film was achieved.
(9)
The core film and a copper ground film were laminated using a bonding film at various torques and 270°C, throughout which its properties were studied. The sample was protected at the top and bottom by two buffer layers.
(10)
Eight ground vias were drilled using a drilling machine with a 0.2 mm diameter needle.
(11)
The eight vias were filled with a conductive paste to connect the background plane.
(12)
Fabrication of the inkjet-printed bandpass filter by lamination bonding was finished.Figure 1
Inkjet printing and lamination bonding process flow.


## 3. Results and Discussion

### 3.1. Various Lamination Bonding Percentages

The lamination bonding process was applied at a constant pressure from 25°C to 270°C, and the temperature was cooled down to room temperature. Various percentages of torque force were tuned over a 4 × 4 cm2 area with a 942 kg fixed force. The sample was clearly open while the torque force was smaller than 12%. An obvious crack was observed at 15% torque force. Therefore, the samples were measured at torque force of 12 to 14%. Figure 2 shows the changes in the insertion losses of the printed line (width, 100 μm; length, 4000 μm) and a probing pad on a 100 μm LCP substrate during several torque force experiments. The inserted figure shows the S-parameters of the silver line, and the resonant frequency of the printed line was approximately 22 GHz. The insertion loss at the resonant frequency was dependent on the torque force. The insertion loss at 12% (<0.68 dB at 22 GHz) was comparable to that of the 0% sample. The insertion losses at the resonant frequency below the 12% printed line were 0.22 and 0.09 dB when torque forces were 13% and 14%, respectively. However, the average degradations in the value of insertion losses over a whole frequency range were −1 and −1.9 dB at 13% and 14%, respectively. Figure 3 shows the surface morphologies at various torque forces. The surface roughness of the silver film increased with torque force. No crack was observed at a torque force of 0% and 12%. At 13%, few cracks were found occasionally on the surface of the silver film. A lot of surface cracks were generated in the microstructure images while bonding at 14%. The surface morphology was consistent with the S21 value. Therefore, 12% was the optimal torque force for the lamination bonding process.Figure 2
Insertion loss and S-parameters (inserted figure) of silver lines at various torque forces.Figure 3
Surface morphology of silver film at various torque forces.


### 3.2. Multilayer Inkjet-Printed Bandpass Filter

Figure4 illustrates the interdigital bandpass filter comprising two LCP layers and three metal layers. The bandpass filter comprises two feeding lines on layer 1, two quarter-wavelength resonators on layer 2, and a ground on layer 3 for the transmission lines on the other layers. The feeding lines provided a broadside coupling to the resonators on layer 2. At the other end of the feeding lines, the ground vias were connected to generate three transmission zeros (TZs) because of the inductive source-load coupling [15]. Two resonators were meandered on layer 2 and coupled with each other using an interdigital capacitor. The bandpass filter was simulated using electromagnetic simulation software. The proposed filter was designed with the following parameters: a permittivity (εr) of 2.9 and a loss tangent (tanδ) of 0.0025 for LCP substrate and a conductivity of 1 × 107 S/m and a thickness of 3.4 μm for silver film. Figure 5 shows the simulated transmission characteristic of the layout for various spaces of inductive source-load coupling (S1). No transmission zero was produced without inductive source-load coupling, and the strength of broadside coupling was weak. With inductive source-load coupling (S1 = 0.3 mm), two transmission zeros (TZ1 and TZ2) near the passband were produced because of the cross coupling between feeding lines. Additionally, transmission zero (TZ3) at stopband is generated while S1 ≦ 0.2 mm because the two transmission paths for the signals (source-load path and source-resonator 1-resonator 2-load path) have the same magnitudes but are out of phase. The transmission zeros can be tuned by S1 because the strength of the source-load coupling is changed. This also verifies that the three transmission zeros were generated by the inductive source-load coupling. Figure 6 shows the frequency responses of various finger numbers (nr) for interdigital capacitor. The interdigital capacitor shortened the length of the coupling region, and the resonant frequency was tuned by adjusting the capacitance. The coupling ratio (k) between two resonators affected the insertion loss. Figure 7 shows the extracted coupling ratio at f0 against L13 and S2. From the resonant frequency and the required k, the size of the interdigital capacitor was determined. Figure 8 shows the three TZ positions relative to the various couple length of two feeding lines (L7). The TZ3 can be tuned by adjusting the coupling length between two feeding lines on layer 1 to improve the skirt selectivity and to enhance stopband while the TZ1 and TZ2 remain fixed. The TZ3 was saturated at 28.7 GHz, while L7 was 0.95 mm. Considering a wide stopband and compact size, we selected L7 as 1.15 mm. Based on the required responses, the parameters are determined as follows: L1=0.7, L2=0.3, L3=1.18, L4=0.3, L5=1.05, L6=0.79, L7=1.15, L8=0.8, L9=0.7, L10=0.88, L11=1, L12=0.45, L13=1, W1=0.07, W2=0.3, W3=0.2, W4=0.4, W5=0.3, W6=0.12, W7=0.3, W8=0.6, S1=0.1, S2=0.15, S3=0.2mm, and nr=4. These prototypes occupied an LCP area of 5.28 × 3.32 × 0.25 mm3 (0.32λg×0.2λg×0.015λg) including probing pads.Figure 4
Structure and photograph of proposed bandpass filter.
(a)
(b)
(c)Figure 5
Simulated frequency responses without inductive source-load coupling and with inductive source-load coupling at variousS1.Figure 6
Simulated frequency responses for the finger number of interdigital capacitor.Figure 7
Coupling ratio with the value ofS2 and L13.Figure 8
Three transmission zeros versusL7.Figures9(a) and 9(b) show the photographs of the bandpass filter on layer 1 and layer 2, respectively. With 20 μm drop spacing and 30 μm droplet size, the resolution of inkjet-printed film resolution was 50 μm. The registration error is approximately 50 μm because the diameter of alignment is 100 μm. The registration error was approximately 50 μm because the diameter of alignment was 100 μm. Figure 9(c) compares the simulated and measured S-parameters of the proposed bandpass filter. The measured maximal S21 of 2.24 dB at 11.4 GHz and the S11 was larger than the 12 dB in the passband. A 3 dB passband was centered at 11.5 GHz with a fractional bandwidth of 17%. The three transmission zeros located at 8.5, 17.5, and 26.5 GHz provided high skirt selectivity and enhanced rejection levels. The stopband rejection is more than 24 dB up to 31 GHz. Note that the transmission zero at 20 GHz is due to the high resistance of drilled vias. Drilling process causes cracks on the surface of silver films resulting in high resistance of vias (inserted in Figure 9(c)). The high resistance vias induced leakages of the signal and produced a redundant transmission zero in the stopband. It was difficult to control the formation of cracks by drilling vias. Moreover, the slight discrepancy between the measured and simulated results is mainly from the resolution of the inkjet-printed films and the registration error of alignment process. The overall agreement between the simulated results and measured data was observed.Figure 9
Photographs of the bandpass filter on (a) layer 1 and (b) layer 2. (c) S-parameters of the interdigital bandpass filter.
(a)
(b)
(c)


## 3.1. Various Lamination Bonding Percentages

The lamination bonding process was applied at a constant pressure from 25°C to 270°C, and the temperature was cooled down to room temperature. Various percentages of torque force were tuned over a 4 × 4 cm2 area with a 942 kg fixed force. The sample was clearly open while the torque force was smaller than 12%. An obvious crack was observed at 15% torque force. Therefore, the samples were measured at torque force of 12 to 14%. Figure 2 shows the changes in the insertion losses of the printed line (width, 100 μm; length, 4000 μm) and a probing pad on a 100 μm LCP substrate during several torque force experiments. The inserted figure shows the S-parameters of the silver line, and the resonant frequency of the printed line was approximately 22 GHz. The insertion loss at the resonant frequency was dependent on the torque force. The insertion loss at 12% (<0.68 dB at 22 GHz) was comparable to that of the 0% sample. The insertion losses at the resonant frequency below the 12% printed line were 0.22 and 0.09 dB when torque forces were 13% and 14%, respectively. However, the average degradations in the value of insertion losses over a whole frequency range were −1 and −1.9 dB at 13% and 14%, respectively. Figure 3 shows the surface morphologies at various torque forces. The surface roughness of the silver film increased with torque force. No crack was observed at a torque force of 0% and 12%. At 13%, few cracks were found occasionally on the surface of the silver film. A lot of surface cracks were generated in the microstructure images while bonding at 14%. The surface morphology was consistent with the S21 value. Therefore, 12% was the optimal torque force for the lamination bonding process.Figure 2
Insertion loss and S-parameters (inserted figure) of silver lines at various torque forces.Figure 3
Surface morphology of silver film at various torque forces.


## 3.2. Multilayer Inkjet-Printed Bandpass Filter

Figure4 illustrates the interdigital bandpass filter comprising two LCP layers and three metal layers. The bandpass filter comprises two feeding lines on layer 1, two quarter-wavelength resonators on layer 2, and a ground on layer 3 for the transmission lines on the other layers. The feeding lines provided a broadside coupling to the resonators on layer 2. At the other end of the feeding lines, the ground vias were connected to generate three transmission zeros (TZs) because of the inductive source-load coupling [15]. Two resonators were meandered on layer 2 and coupled with each other using an interdigital capacitor. The bandpass filter was simulated using electromagnetic simulation software. The proposed filter was designed with the following parameters: a permittivity (εr) of 2.9 and a loss tangent (tanδ) of 0.0025 for LCP substrate and a conductivity of 1 × 107 S/m and a thickness of 3.4 μm for silver film. Figure 5 shows the simulated transmission characteristic of the layout for various spaces of inductive source-load coupling (S1). No transmission zero was produced without inductive source-load coupling, and the strength of broadside coupling was weak. With inductive source-load coupling (S1 = 0.3 mm), two transmission zeros (TZ1 and TZ2) near the passband were produced because of the cross coupling between feeding lines. Additionally, transmission zero (TZ3) at stopband is generated while S1 ≦ 0.2 mm because the two transmission paths for the signals (source-load path and source-resonator 1-resonator 2-load path) have the same magnitudes but are out of phase. The transmission zeros can be tuned by S1 because the strength of the source-load coupling is changed. This also verifies that the three transmission zeros were generated by the inductive source-load coupling. Figure 6 shows the frequency responses of various finger numbers (nr) for interdigital capacitor. The interdigital capacitor shortened the length of the coupling region, and the resonant frequency was tuned by adjusting the capacitance. The coupling ratio (k) between two resonators affected the insertion loss. Figure 7 shows the extracted coupling ratio at f0 against L13 and S2. From the resonant frequency and the required k, the size of the interdigital capacitor was determined. Figure 8 shows the three TZ positions relative to the various couple length of two feeding lines (L7). The TZ3 can be tuned by adjusting the coupling length between two feeding lines on layer 1 to improve the skirt selectivity and to enhance stopband while the TZ1 and TZ2 remain fixed. The TZ3 was saturated at 28.7 GHz, while L7 was 0.95 mm. Considering a wide stopband and compact size, we selected L7 as 1.15 mm. Based on the required responses, the parameters are determined as follows: L1=0.7, L2=0.3, L3=1.18, L4=0.3, L5=1.05, L6=0.79, L7=1.15, L8=0.8, L9=0.7, L10=0.88, L11=1, L12=0.45, L13=1, W1=0.07, W2=0.3, W3=0.2, W4=0.4, W5=0.3, W6=0.12, W7=0.3, W8=0.6, S1=0.1, S2=0.15, S3=0.2mm, and nr=4. These prototypes occupied an LCP area of 5.28 × 3.32 × 0.25 mm3 (0.32λg×0.2λg×0.015λg) including probing pads.Figure 4
Structure and photograph of proposed bandpass filter.
(a)
(b)
(c)Figure 5
Simulated frequency responses without inductive source-load coupling and with inductive source-load coupling at variousS1.Figure 6
Simulated frequency responses for the finger number of interdigital capacitor.Figure 7
Coupling ratio with the value ofS2 and L13.Figure 8
Three transmission zeros versusL7.Figures9(a) and 9(b) show the photographs of the bandpass filter on layer 1 and layer 2, respectively. With 20 μm drop spacing and 30 μm droplet size, the resolution of inkjet-printed film resolution was 50 μm. The registration error is approximately 50 μm because the diameter of alignment is 100 μm. The registration error was approximately 50 μm because the diameter of alignment was 100 μm. Figure 9(c) compares the simulated and measured S-parameters of the proposed bandpass filter. The measured maximal S21 of 2.24 dB at 11.4 GHz and the S11 was larger than the 12 dB in the passband. A 3 dB passband was centered at 11.5 GHz with a fractional bandwidth of 17%. The three transmission zeros located at 8.5, 17.5, and 26.5 GHz provided high skirt selectivity and enhanced rejection levels. The stopband rejection is more than 24 dB up to 31 GHz. Note that the transmission zero at 20 GHz is due to the high resistance of drilled vias. Drilling process causes cracks on the surface of silver films resulting in high resistance of vias (inserted in Figure 9(c)). The high resistance vias induced leakages of the signal and produced a redundant transmission zero in the stopband. It was difficult to control the formation of cracks by drilling vias. Moreover, the slight discrepancy between the measured and simulated results is mainly from the resolution of the inkjet-printed films and the registration error of alignment process. The overall agreement between the simulated results and measured data was observed.Figure 9
Photographs of the bandpass filter on (a) layer 1 and (b) layer 2. (c) S-parameters of the interdigital bandpass filter.
(a)
(b)
(c)


## 4. Conclusions

Inkjet-printed interdigital bandpass filter using multilayer technique on LCP substrates was successfully developed based on the insertion loss and surface morphology. The three-dimensional interdigital bandpass filter achieved a minimum insertion loss of 2.2 dB with a 17% bandwidth at a centered frequency of 11.5 GHz. Combining inkjet printing and multilayer LCP lamination bonding processes provides inexpensive and compact electronic components for electronic package applications.



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*Source: 6161427-2018-05-15.xml*