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LT5519 Datasheet(PDF) 8 Page - Linear Technology |
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LT5519 Datasheet(HTML) 8 Page - Linear Technology |
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8 / 12 page ![]() LT5519 8 5519f APPLICATIO S I FOR ATIO Though the LO input is internally matched to 50 Ω, there may be some cases, particularly at higher frequencies or with different source impedances, where a further opti- mized match is desired. Table 2 includes the single-ended input impedance and reflection coefficient vs frequency for the LO input for use in such cases. Table 2. Single-Ended LO Input Impedance FREQUENCY INPUT S11 (MHz) IMPEDANCE MAG ANGLE 200 72.3 – j16.1 0.223 –28.4 400 63.3 – j11.3 0.153 –34.7 600 61.6 – j7.5 0.124 – 29.2 800 61.9 – j6.0 0.119 – 23.6 1000 62.7 – j6.1 0.125 –22.7 1200 63.2 – j7.4 0.134 –25.5 1400 63.3 – j9.5 0.144 –30.8 1600 62.8 – j12.0 0.155 –37.1 1800 61.6 – j14.2 0.163 –43.4 RF Output Port An internal RF transformer, shown in Figure 5, reduces the mixer-core impedance to provide an impedance of 50 Ω across the RF+ and RF– pins. The LT5519 is designed and tested with the outputs configured for single-ended opera- tion, as shown in the Figure 5; however, the outputs can be used differentially as well. A center tap in the transformer provides the DC connection to the mixer core and the transformer provides DC isolation at the RF output. The RF+ and RF– pins are connected together through the secondary windings of the transformer; thus a DC voltage should not be applied across these pins. The impedance data for the RF output, listed in Table 3, can be used to develop matching networks for different load impedances. Table 3. Single-Ended RF Output Impedance FREQUENCY OUTPUT S11 (MHz) IMPEDANCE MAG ANGLE 700 27.6 + j32.0 0.465 103 800 39.7 + j32.1 0.354 88.1 900 50.9 + j23.5 0.227 74.7 1000 53.5 + j10.3 0.105 65.5 1100 48.3 + j1.3 0.022 143 1200 42.0 – j3.1 0.093 –157 1300 36.6 – j3.4 0.159 –164 1400 33.0 – j2.0 0.207 –172 Operation at Different Input Frequencies On the evaluation board shown in Figure 10, the input of the LT5519 can be easily matched for different frequencies by changing the capacitors, C1, C2 and C3. Capacitors C1 and C2 set the input matching frequency while C3 im- proves the LO to RF leakage performance. Decreasing the value of C3 at higher input frequencies reduces its impact on conversion gain. Table 4 lists some actual values used at selected frequencies. Figure 4. LO Input Circuit LOIN 50 Ω 14 15 VCC 5519 F04 85 Ω LO– LO+ LT5519 5pF 5pF 220 Ω 220 Ω Figure 5. RF Output Circuit RFOUT 50 Ω 11 10 VCC 10pF LT5519 VCC3 5519 F05 RF– RF+ 8 |
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