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Radio Fr equency System-on-Package (RF SOP)   281


                                                  Inductor




                                                 Air cavity                    Dielectric




                                                 Ground plane
                    FIGURE 5.20  Inductor on an LTCC platform with an enclosed air cavity. [43]
                    high volume. A number of LTCC designs have been reported in the literature. One fully
                    embedded LTCC spiral inductor incorporating an air cavity between the spiral and
                    ground plane has been reported to achieve a quality factor of about 51 with an SRF of
                    9.1 GHz [44]. The air cavity employed under the spiral reduces the shunt parasitic
                    capacitance of the inductor resulting in a high Q factor and a high SRF of embedded
                    inductors. The inductors were designed using a low-loss LTCC dielectric of 114 μm
                    thickness and silver conductor of 12 μm thickness. The spiral inductors, with an air
                    cavity incorporated, were fully embedded in a five-layer LTCC block as well as those
                    without an air cavity. The cross section of such a structure is shown in Figure 5.20.
                       Another example of LTCC resulted in a quality factor of 93 at 1.1 GHz and an SRF
                    of 3.11 GHz when 3D helical inductors with circular turns were designed on 2a 0-layer
                    LTCC-951-AT ceramic [45]. The 3D helical inductors occupied less space. An inductance
                    of about 9.6 nH was reported. Such a helical inductor fabrication is shown in Figure 5.21.
                    In addition to occupying less space, the helical configuration reduces the coupling
                    capacitance by increasing the distance between the top turns and the underlying turns,
                    thereby preventing a considerable reduction in SRF. For higher Q, MEMS technologies
                    have been implemented by numerous authors [46–53]. The fabricated devices exhibit
                    very high performances such as Q values above 100 and self-resonance frequencies as
                    high as 50 GHz [46].

























                    FIGURE 5.21  Diagram of a 3D helical inductor. [44]
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