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Design Methodologies of LTCC Bandpass Filters, Diplexer, and ...

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720 IEEE TRANSACTIONS ON MICROWAVE THEORY AND TECHNIQUES, VOL. 54, NO. 2, FEBRUARY 2006<br />

Fig. 8. Fabricated 2.4-GHz b<strong>and</strong>pass filter with transmission zero at the<br />

frequency <strong>of</strong> 1.9 GHz. (a) 3-D structure. (b) Measured <strong>and</strong> EM simulated<br />

results.<br />

Two filters mentioned above are fabricated with the substrate<br />

<strong>of</strong> Dupont 951. Their dielectric constant <strong>and</strong> loss tangent are 7.8<br />

<strong>and</strong> 0.0045, respectively. The 2.4-GHz <strong>LTCC</strong> filter is designed<br />

on one upper layer with the sheet <strong>of</strong> 1.57 mil, six middle layers<br />

with the sheet <strong>of</strong> 3.6 mil, <strong>and</strong> three lower layers with the sheet<br />

<strong>of</strong> 1.57 mil. Its overall size is 110 mil 92 mil 28 mil. After<br />

circuit simulation, these values are converted into the <strong>LTCC</strong><br />

structure. The simulation is carried out with the assistant <strong>of</strong> the<br />

full-wave electromagnetic (EM) simulator Sonnet from Sonnet<br />

S<strong>of</strong>tware Inc., North Syracuse, NY. In the 3-D structure, the parallel-coupled<br />

line is placed on the lower layer to reduce the coupling<br />

effect with other capacitors. Fig. 8(a) shows the three-dimensional<br />

(3-D) structure <strong>of</strong> 2.4-GHz <strong>LTCC</strong> b<strong>and</strong>pass filter.<br />

The on-wafer tester has been chosen to improve the accuracy <strong>of</strong><br />

measurement. The network analyzer Agilent N5230A PNA_L<br />

is used to measure, <strong>and</strong> the short-open-load-through (SOLT) is<br />

adopted to calibrate.<br />

Fig. 9. Fabricated 2-GHz b<strong>and</strong>pass filter with transmission zero at the<br />

frequency <strong>of</strong> 2.5 GHz. (a) 3-D structure. (b) Measured <strong>and</strong> EM simulated<br />

results.<br />

As shown in Fig. 8(b), the frequencies <strong>of</strong> measured <strong>and</strong> EM<br />

simulated transmission zeros are 1.84 <strong>and</strong> 1.9 GHz, respectively.<br />

At the frequency <strong>of</strong> 2.4 GHz, the measured <strong>and</strong> EM simulated<br />

insertion losses are less than 1.44 <strong>and</strong> 1.3 dB, respectively; the<br />

return losses are greater than 15 <strong>and</strong> 17 dB, respectively.<br />

A 2-GHz b<strong>and</strong>pass filter is given as another design example.<br />

This 2-GHz <strong>LTCC</strong> filter is designed on five upper layers with the<br />

sheet <strong>of</strong> 3.6 mil, four middle layers with the sheet <strong>of</strong> 1.57 mil,<br />

<strong>and</strong> two lower layers with the sheet <strong>of</strong> 3.6 mil. Its overall size<br />

is 107 mil 102 mil 32 mil. The 3-D structure <strong>of</strong> the 2-GHz<br />

<strong>LTCC</strong> b<strong>and</strong>pass filter is shown in Fig. 9(a). In the 3-D structure,<br />

the parallel-coupled line is the same placed on the lower layer<br />

to reduce the coupling effect with other capacitors. As shown<br />

in Fig. 9(b), the frequencies <strong>of</strong> the measured <strong>and</strong> EM simulated<br />

transmission zeros are 2.45 <strong>and</strong> 2.5 GHz, respectively. At the<br />

frequency <strong>of</strong> 2 GHz, the measured <strong>and</strong> EM simulated insertion<br />

losses are less than 1.45 <strong>and</strong> 1.26 dB, respectively; the return<br />

losses are greater than 19 <strong>and</strong> 39 dB, respectively.<br />

The <strong>LTCC</strong> technology is a kind <strong>of</strong> thick-film process. In order<br />

to realize the physical 3-D circuit, the parasitic effect among ca-

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