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Mixed-Signal (SOP) Design   175





                                                              = 3.48, tanδ = 0.004)
                                       Rogers hydrocarbon (7.7 mils, ε r


                                                           = 10, tanδ = 0.019)
                                            BC12TM (12 μm, ε r

                                       Rogers hydrocarbon (7.7 mils, ε  = 3.48, tanδ = 0.004)
                                                             r



                    FIGURE 4.22  Stackup for balun implementation using high-K material.



                    where R source  and R load  are the source and load impedances, and w = 2πf  is the frequency
                                                                          0
                                                                               0
                    of operation.
                       To demonstrate the operation of the lumped element balun, a balun operating at
                    2.44 GHz with a 100-MHz bandwidth has been designed. For an R source  and R load  of 50
                    and 100 Ω, respectively, this yields values of 0.92 pF and 4.6 nH for the capacitance and
                    inductance. With the thickness limitation restricting the use of multiple dielectric layers
                    and size limitations restricting the use of low-K materials, it is difficult to realize such
                    baluns using homogenous dielectrics. Figure 4.22 shows a 0.5-mm-thick stackup
                    incorporating a high dielectric constant material (Oak-Mitsui’s FaradFlex BC-12TM).
                    With a tan d of 0.019 and e = 10 (at 1 MHz) and a thickness of 12 μm, the material has
                                           r
                    been developed for embedded digital decoupling applications. However, the high
                    capacitance density (11 nF/in  at 1 MHz) makes this a suitable candidate for small size
                                             2
                    low-profile baluns. The lattice topology is particularly suitable for design using this
                    material, as it uses low-pass and high-pass structures that are more tolerant to dielectric
                    losses compared to bandpass structures. The shielded device measures 1.25 mm × 2 mm
                    in area with a thickness of 0.507 mm, 1 dB of insertion loss, an amplitude imbalance of
                    2 dB, and a phase imbalance of ±10°. Table 4.4 shows the comparison of the fabricated
                    balun with a commercially available Marchand balun, also built on an organic substrate.
                    As can be seen from Table 4.3 the present balun implementation compares to the
                    commercially available balun with a 42 percent reduction in size. In addition, the
                    present balun can be embedded into the layers of LCP.
                       A third alternative in balun design is the use of transformers. Although compact
                    designs are possible, the performance of the balun in this case is very much dependent
                    on the coupling between primary and secondary coils. An SOP technology with high
                    coupling coefficients, achieved through tight metal-to-metal spacing or low dielectric
                    thickness or a combination of both, is required for the implementation of these baluns.

                    4.2.5 Filter-Balun Networks
                    In a receiver, the signal coming in from the antenna is single-ended in nature, but the
                    active circuitry (beginning with the LNA) is usually differential, as shown in Figure 4.23.
                    The single-ended signal is filtered using a bandpass filter and then converted to
                    differential mode using a balun. With SOP-based implementation, a circuit embedded
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