APN1006

APPLICATION NOTE APN1006: A Colpitts VCO for Wideband (0.95–2.15 GHz) Set-Top TV Tuner Applications Introduction Modern set-top DBS TV tuners require high-performance, broadband voltage control oscillator (VCO) designs at a competitive cost. To meet these goals, design engineers are challenged to create high-performance, low-cost VCOs. The Colpitts oscillator is a traditional design used for many VCO applications. Designing a broadband Colpitts oscillator with coverage from 1–2 GHz requires the selection and interaction of an appropriate varactor diode for its resonator. This application note describes the design of a broadband Colpitts VCO that incorporates the SMV1265-011 varactor diode. This varactor diode was specifically developed at Skyworks for this application. The VCO design, based on Libra Series IV simulation, shows good correlation between measured and simulated performance. This application note includes a board layout and materials list. VCO Model Figure 1 shows the VCO model built for open loop analysis in Libra Series IV. Figure 1. VCO Model Built for Open Loop Analysis in Libra Series IV Skyworks Solutions, Inc. • Phone [781] 376-3000 • Fax [781] 376-3100 • sales@skyworksinc.com • www.skyworksinc.com 200316 Rev. A • Skyworks Proprietary Information • Products and Product Information are Subject to Change Without Notice. • July 21, 2005 1 APPLICATION NOTE • APN1006 This circuit schematic, which is a simple Colpitts structure, uses a series back-to-back connection of two SMV1265-011 varactors instead of a single varactor. This connection allows lower capacitance at high voltages, while maintaining the tuning ratio of a single varactor. The back-to-back varactor connection also helps reduce distortion and the effect of fringing and mounting capacitances. These parasitic capacitances are included in the model as C5, valued at 0.6 pF. This value may change depending on the layout of the board. DC bias is provided through resistors R1 and R4, both 3 kΩ, which may affect phase noise, but allows the exclusion of chokes. This reduces costs and the possibility of parasitic resonances — the common cause of spurious responses and frequency instability. The resonator inductance was modeled as a lossy inductor (with Q = 25 at 100 MHz) in parallel with a capacitance of 0.25 pF. This is typical for a multilayer inductor of style 0603 (60 x 30 mil) footprint (TOKO Coils and Filters catalog). The inductor value of 5.6 nH was optimized to fit the desired 1–2 GHz frequency band. The DC blocking series capacitance (CSER) was modeled as an SRC network, including associated parasitics; it was selected at 1000 pF to avoid affecting the resonator (Q). The Colpitts feedback capacitances (CDIV1 = 1 pF and CDIV2 = 1.62 pF) were optimized to provide a flat power response over the tuning range. These values may also be re-optimized for phase noise if required. The NEC NE68533 transistor was selected to fit the required bandwidth performance. Note: The circuit is very sensitive to the transistor choice (tuning range and stability) due to the wide bandwidth requirement. The output is supplied from the emitter load resistance (RL1) through the 2 pF coupling capacitor, modeled as a series SLC1 component. The microstrip line (TL1) simulates the design layout which may be incorporated in the resonator. Figure 2 shows the Libra test bench. In the test bench, we define an open loop gain (Ku = VOUT/VIN) as a ratio of voltage phasors at input and output ports of an OSCTEST component. Defining the oscillation point requires the balancing of input (loop) power to provide zero gain for a zero loop phase shift. Once the oscillation point is defined, the frequency and output power can be measured. Use of the OSCTEST2 component for the close loop analysis is not recommended, since it may not converge in some cases, and doesn’t allow clear insight into understanding the VCO behavior. These properties are considered an advantage of modeling over a purely experimental study. Figure 2. Libra Test Bench Skyworks Solutions, Inc. • Phone [781] 376-3000 • Fax [781] 376-3100 • sales@skyworksinc.com • www.skyworksinc.com 2 July 21, 2005 • Skyworks Proprietary Information • Products and Product Information are Subject to Change Without Notice. • 200316 Rev. A APPLICATION NOTE • APN1006 Figure 3. Default Test Bench Figure 3 shows the default bench. The variables used for more convenient tuning during performance analysis and optimization are listed in a “variables and equations” component. SMV1265-011 SPICE Model Figure 4 shows a SPICE model for the SMV1265-011 varactor diode, defined for the Libra IV environment, with a description of the parameters employed. Figure 4. SMV1265-011 Libra IV SPICE Model Skyworks Solutions, Inc. • Phone [781] 376-3000 • Fax [781] 376-3100 • sales@skyworksinc.com • www.skyworksinc.com 200316 Rev. A • Skyworks Proprietary Information • Products and Product Information are Subject to Change Without Notice. • July 21, 2005 3 APPLICATION NOTE • APN1006 Parameter IS RS N TT CJO VJ M EG XTI KF AF FC BV IBV ISR NR IKF NBV IBVL NBVL TNOM FFE Series resistance Description Saturation current (with N, determine the DC characteristics of the diode) Emission coefficient (with IS, determines the DC characteristics of the diode) Transit time Zero-bias junction capacitance (with VJ and M, defines nonlinear junction capacitance of the diode) Junction potential (with VJ and M, defines nonlinear junction capacitance of the diode) Grading coefficient (with VJ and M, defines nonlinear junction capacitance of the diode) Energy gap (with XTI, helps define the dependence of IS on temperature) Saturation current temperature exponent (with EG, helps define the dependence of IS on temperature) Flicker noise coefficient Flicker noise exponent Forward-bias depletion capacitance coefficient Reverse breakdown voltage Current at reverse breakdown voltage Recombination current parameter Emission coefficient for ISR High injection knee current Reverse breakdown ideality factor Low-level reverse breakdown knee current Low-level reverse breakdown ideality factor Nominal ambient temperature at which these model parameters were derived Flicker noise frequency exponent Unit A Ω S F V EV V A A A A °C Default 1e-14 0 1 0 0 1 0.5 1.11 3 0 1 0.5 Infinity 1e-3 0 2 Infinity 1 0 1 27 1 Table 1. Silicon Varactor Diode Default Values Table 1 describes the model parameters. It shows default values appropriate for silicon varactor diodes which may be used by the Libra IV simulator. According to the SPICE model in Figure 4, the varactor capacitance (CV) is a function of the applied reverse DC voltage (VR) and may be expressed as follows: CJO CV = + CP VR ) M (1 + VJ This equation is a mathematical expression of the capacitance characteristic. The model is accurate for abrupt junction varactors (SMV1400 series); however, the model is less accurate for hyperabrupt junction varactors because the coefficients are dependent on the applied voltage. To make the equation fit the hyperabrupt performances for the SMV1265-011, a piece-wise approach was employed. Here the coefficients (VJ, M, CJO, and CP) are made piece-wise functions of the varactor DC voltage applied. Thus, the whole range of the usable varactor voltages is segmented into a number of subranges each with a unique set of the VJ, M, CJO, and CP parameters as given in the Table 2. Voltage Range (V) 0–2.5 2.5–6.5 6.5–11 11–up CJO (pF) 22.5 21 20 20 M 2 25 7.3 1.8 VJ (V) 4 68 14 1.85 CP (pF) 0 0 0.9 0.56 Table 2. Varactor Voltages These subranges are made to overlap each other. Thus, if a reasonable RF swing (one that is appropriate in a practical VCO case) exceeds limits of the subrange, the CV function described by the current subrange will still fit in the original curve. Skyworks Solutions, Inc. • Phone [781] 376-3000 • Fax [781] 376-3100 • sales@skyworksinc.com • www.skyworksinc.com 4 July 21, 2005 • Skyworks Proprietary Information • Products and Product Information are Subject to Change Without Notice. • 200316 Rev. A APPLICATION NOTE • APN1006 100 Approximation Measured 1.0 0.8 2.6 2.4 Series Resistance (Ω) Capacitance (pF) 10 0.6 0.4 1 0.2 0.1 0 5 10 15 20 25 30 0 2.2 2.0 1.8 1.6 1.4 RS Measured 1.2 0 5 10 15 20 25 30 RS_PWL Varactor Voltage (V) Figure 5. SMV1265 Capacitance vs. Voltage Varactor Voltage (V) Figure 6. SMV1265 Resistance vs. Voltage Figure 5 demonstrates the quality of the piece-wise fitting approach. Special consideration was given to the fit at the lowest capacitance range (high-voltage area) since it dramatically affects the upper frequency limit of the VCO. To incorporate this function into Libra, the pwl() built-in function was used in the “variables” component of the schematic bench. M = pwl (VVAR 0 2 2.5 2 2.500009 25 6.5 25 6.50009 7.3 11 7.3 11.0009 1.8 40 1.8) VJ = pwl (VVAR 0 4 2.5 4 2.500009 68 6.5 68 6.50009 14 11 14 11.0009 1.85 40 1.85) CP = pwl (VVAR 0 0 2.5 0 2.500009 0 6.5 0 6.50009 0.9 11 0.9 11.0009 0.56 40 0.56) CJO = pwl (VVAR 0 22.5 2.5 22.5 2.500009 21 6.5 21 6.50009 20 11 20 11.0009 20 40 20)*1012 Note: While CP is given in picofarads, CGO is given in farads to comply with the default nominations in Libra. (For more details regarding pwl() function see Circuit Network Items, Variables and Equations, Series IV Manuals, p. 19–15). Since the epitaxial layer for this kind of hyperabrupt varactor has relatively high resistivity, the series resistance is strongly dependent on the reverse voltage applied to varactor junction. The value of series resistance (RS) measured at 500 MHz is shown in Figure 6, with a piece-wise approximation of RS also given. The piece-wise function may be used as follows: RS = pwl (VVAR 0 2.4 3 2.4 4 2.3 5 2.2 6 2 7 1.85 8 1.76 9 1.7 10 1.65 11 1.61 12 1.5 40 1.5) Note: The pwl() function in Libra IV is defined for the evaluation of harmonic balance parameters rather than variables. Therefore, although series resistance was defined as dependent on reverse voltage, for harmonic balance it remains parametric and linear. The same applies to capacitance, which remains the same as in the original diode model, but its coefficients (VJ, M, CJO, and CP) become parametric functions of the reverse voltage. Skyworks Solutions, Inc. • Phone [781] 376-3000 • Fax [781] 376-3100 • sales@skyworksinc.com • www.skyworksinc.com 200316 Rev. A • Skyworks Proprietary Information • Products and Product Information are Subject to Change Without Notice. • July 21, 2005 5 APPLICATION NOTE • APN1006 VCO Design Materials, Layout, and Performance Figure 7 shows the VCO circuit diagram. Table 3 shows the bill of materials used. Designator C1 C2 C3 C4 C5 C6 D1 Part Type 0603AU561JAT9 (AVX) 0603AU2R0JAT9 (AVX) 0603AU561JAT9 (AVX) 0603AU201JAT9 (AVX) 0603AU1R0JAT9 (AVX) 0603AU1R6JAT9 (AVX) NE68519 (NEC) LL1608-F5N6S (TOKO) CR10-332J-T (AVX) CR10-912J-T (AVX) CR10-201J-T (AVX) CR10-302J-T (AVX) CR10-302J-T (AVX) SMV1265-011 (Skyworks) SMV1265-011 ( Skyworks) Footprint 0603 0603 0603 0603 0603 0603 SOT-419 0603 0603 0603 0603 0603 0603 SOD-323 SOD-323 3.3 k VTUNE 5.6 nH 320 x 30 mils 560 p NE68519 VCC = 5 V Icc = 9 mA SMV1265-011 3k 3k SMV1265-011 300 p 9.1 k 1p 2p RF Output 1.62 p 200 L1 R1 R2 R3 R4 R5 Figure 7. VCO Circuit Diagram V1 V2 Table 3. Bill of Materials Figure 8 shows the PCB layout. The board is made of standard FR4 material 60 mils thick. 720 MIL Figure 8. PCB Layout Skyworks Solutions, Inc. • Phone [781] 376-3000 • Fax [781] 376-3100 • sales@skyworksinc.com • www.skyworksinc.com 6 July 21, 2005 • Skyworks Proprietary Information • Products and Product Information are Subject to Change Without Notice. • 200316 Rev. A 720 MIL APPLICATION NOTE • APN1006 Figure 9 shows both the measured performance of this circuit and the simulated results, obtained with the above model. The simulated tuning curve (frequency vs. voltage) is in excellent agreement with measured data, proving the effectiveness of the piece-wise approximation technique. The measured power response, shows some differences from its simulation, but is within the same range. A possible reason for the discrepancy could be the effect of higher harmonics. To simulate this would require significantly more complicated modeling of the components, board parasitics, and discontinuities. However, for most engineering purposes, the circuit performance prediction indicated here should be satisfactory. 2.2 2.1 2.0 1.9 1.8 1.7 1.6 1.5 1.4 1.3 1.2 1.1 1.0 0.9 0 5 10 7 POUT_MODEL POUT_EXP FEXP 6 5 List of Available Documents 1. Colpitts Wideband VCO Simulation Project Files for Libra IV. 2. Colpitts Wideband VCO Circuit Schematic and PCB Layout for Protel EDA Client, 1998 version. 3. Colpitts Wideband VCO Gerber Photo-plot Files 4. A Colpitts VCO for Wideband (0.95–2.15 GHz) Set-Top TV Tuner Applications. (Current Document). 5. Detailed measurement and simulation data. For the availability of the listed materials, please call our applications engineering staff. © Skyworks Solutions, Inc., 1999. All rights reserved. Frequency (GHz) POUT (dBm) 4 FMODEL 3 2 1 0 15 20 25 30 Varactor Voltage (V) Figure 9. Measured and Simulated Frequency vs. Varactor Voltage Table 4 shows tabulated measurement data. In voltage ranges of 1–27 V, the usable frequency coverage was estimated from 0.98–2.15 GHz. VVAR (V) 0.5 1 2 4 8 12 14 18 22 25 30 Frequency (GHz) 0.95 0.974 1.018 1.184 1.68 1.886 1.932 2.008 2.076 2.12 2.188 POUT (dBm) 5.7 5.5 5.4 4.7 3.2 5.2 4.9 5 3.9 3.5 2.2 Table 4. Tabulated Measurement Data Skyworks Solutions, Inc. • Phone [781] 376-3000 • Fax [781] 376-3100 • sales@skyworksinc.com • www.skyworksinc.com 200316 Rev. A • Skyworks Proprietary Information • Products and Product Information are Subject to Change Without Notice. • July 21, 2005 7 APPLICATION NOTE • APN1006 Copyright © 2002, 2003, 2004, 2005, Skyworks Solutions, Inc. All Rights Reserved. Information in this document is provided in connection with Skyworks Solutions, Inc. (“Skyworks”) products or services. These materials, including the information contained herein, are provided by Skyworks as a service to its customers and may be used for informational purposes only by the customer. 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