APN1005 [SKYWORKS]

A Balanced Wideband VCO for Set-Top TV Tuner Applications; 一个平衡的宽带VCO的机顶盒电视调谐器的应用
APN1005
型号: APN1005
厂家: SKYWORKS SOLUTIONS INC.    SKYWORKS SOLUTIONS INC.
描述:

A Balanced Wideband VCO for Set-Top TV Tuner Applications
一个平衡的宽带VCO的机顶盒电视调谐器的应用

电视
文件: 总11页 (文件大小:266K)
中文:  中文翻译
下载:  下载PDF数据表文档文件
APPLICATION NOTE  
APN1005: A Balanced Wideband VCO  
for Set-Top TV Tuner Applications  
Introduction  
VCO Model  
Modern set-top TV DBS tuner systems require more channel  
coverage, while maintaining competitive prices. This situation  
creates tough design goals: to improve performance and simplify  
design.  
Figure 1 shows the VCO model built for open loop analysis in Libra  
Series IV including the SMV1265-011 varactor model.  
The circuit schematic in Figure 2 shows a pair of transistors in a  
single feedback loop, connected so that collector currents would  
be 180° shifted (ideally). A pair of back-to-back connected  
SMV1265-011 varactors is used, rather than a single one. This  
allows lower capacitance at the high-voltage range, without  
changing the tuning ratio. The reason is that, apart from package  
capacitance, certain mounting fringing capacitances, though  
small, may strongly affect higher frequency margins. The effects  
Balanced VCO configuration could be a competitive circuit  
solution, since it provides the widest tuning range with practical  
circuitry and layout. However, tuning margins would be further  
improved by optimizing the varactor manufacturing process.  
Skyworks has developed such a process to satisfy the most  
ambitious wideband design goals.  
of parasitic capacitances were summarized in the model as C  
4
In this publication, we will address the design of the balanced-  
type voltage control oscillator (VCO) based on the newly  
developed varactor SMV1265-011 with the unique set of  
capacitance tuning ratios and Q-quality.  
and C , valued 0.4 pF each. These values may vary depending on  
3
the layout of the board. Varactor DC biasing is provided through  
resistors R and R , both 1 k, which may affect the phase noise,  
6
8
but eliminate the need for inductive chokes. This minimizes  
overall costs and the possibility of parasitic resonances — the  
usual cause for frequency instability and spurs.  
The phase corrector DC chokes, SRL and SRL , were modeled  
1
2
as lossless inductors at 33 nH since their losses are dominated  
by the 30 emitter biasing resistors. DC blocking series capaci-  
tances (C  
and C ) are modeled as an SRC network,  
SER2  
SER1  
including associated parasitics. Their values were optimized to  
10 pF providing smooth tuning over the design band.  
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200314 Rev. A • Skyworks Proprietary Information • Products and Product Information are Subject to Change Without Notice. • July 21, 2005  
1
APPLICATION NOTE • APN1005  
Figure 1. VCO Model, Including SMV1265-011 Varactor Model  
Figure 2. Transistor Pair in Single Feedback Loop  
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2
APPLICATION NOTE • APN1005  
The pseudo-resonator inductance is formed by microstrip trans-  
In the Libra test bench shown in Figure 3 we defined an open  
mission line TL , which provides necessary circuit response at  
loop gain (Ku = V /V ) as the ratio of voltage phasors at the  
2
OUT IN  
high frequencies. This has little effect at the lower band due to  
the resonator’s dominantly capacitive nature.  
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 mea-  
sured. Use of the OSCTEST2 component for the close loop  
analysis is not recommended, since it may fail to converge in  
some cases, and doesn’t allow clear insight into the under-  
standing of VCO behavior. This property is considered an  
advantage of modeling over a purely experimental study.  
The function of transmission line TL is both feedback and  
1
phase alignment — providing flat power response over the  
tuning range.  
Power output is supplied from the collectors of X or X through  
1
2
the series connected resistance and DC blocking capacitance  
SRC and SRC .  
2
3
DC biasing for both of the transistors is supplied through a resis-  
tive divider R /R /R .  
In the default bench shown in Figure 4 the variables used for  
more convenient tuning during performance analysis and opti-  
mization are listed in a “variables and equations” component.  
1
3 2  
The NEC NE68119 bipolar transistors were selected to best fit  
performances. Note: The circuit is very sensitive to the transistor  
choice (in terms of tuning range and stability) due to wide band-  
width design requirements.  
For the model of NEC NE68119 we used the Gumel Poon model  
of Libra IV with the coefficients provided by CEL RF & Microwave  
Semiconductors Catalogue,1997-98.  
Figure 3. Libra Test Bench  
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200314 Rev. A • Skyworks Proprietary Information • Products and Product Information are Subject to Change Without Notice. • July 21, 2005  
3
APPLICATION NOTE • APN1005  
Figure 4. Default Bench  
SMV1265-011 SPICE Model  
Figure 5 shows a SPICE model for the SMV1265-011 varactor  
diode, defined for the Libra IV environment, with a description of  
the parameters employed.  
Figure 5. SMV1265-011 Libra IV SPICE Model  
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July 21, 2005 • Skyworks Proprietary Information • Products and Product Information are Subject to Change Without Notice. • 200314 Rev. A  
4
APPLICATION NOTE • APN1005  
Parameter  
Description  
Saturation current (with N, determine the DC characteristics of the diode)  
Series resistance  
Unit  
A
-
Default  
IS  
1e-14  
R
S
0
N
Emission coefficient (with IS, determines the DC characteristics of the diode)  
Transit time  
1
TT  
S
F
0
C
JO  
Zero-bias junction capacitance (with V and M, defines nonlinear junction capacitance of the diode)  
0
J
V
J
Junction potential (with V and M, defines nonlinear junction capacitance of the diode)  
V
1
J
M
Grading coefficient (with V and M, defines nonlinear junction capacitance of the diode)  
-
0.5  
J
E
Energy gap (with XTI, helps define the dependence of IS on temperature)  
EV  
-
1.11  
G
XTI  
KF  
AF  
FC  
Saturation current temperature exponent (with E , helps define the dependence of IS on temperature)  
3
G
Flicker noise coefficient  
-
0
Flicker noise exponent  
-
1
Forward-bias depletion capacitance coefficient  
Reverse breakdown voltage  
-
0.5  
B
V
Infinity  
V
I
Current at reverse breakdown voltage  
Recombination current parameter  
Emission coefficient for ISR  
A
A
-
1e-3  
BV  
ISR  
NR  
0
2
IKF  
High injection knee current  
A
-
Infinity  
NBV  
IBVL  
NBVL  
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  
1
0
A
-
1
T
NOM  
°C  
27  
1
FFE  
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.  
whole range of the usable varactor voltages is segmented into a  
number of subranges each with a unique set of the V , M, C ,  
J
JO  
and C parameters as given in the Table 2.  
P
According to the SPICE model in Figure 4, the varactor capaci-  
Voltage Range  
(V)  
C
V
(V)  
C
(pF)  
JO  
J
P
tance (C ) is a function of the applied reverse DC voltage (V ) and  
V
R
(pF)  
22.5  
21.0  
20.0  
20.0  
M
2.0  
25.0  
7.3  
1.8  
may be expressed as follows:  
0–2.5  
2.5–6.5  
6.5–11  
11–up  
4.00  
0.00  
0.00  
0.90  
0.56  
C
JO  
68.00  
14.00  
1.85  
C =  
V
+ C  
P
M
V
R
1 +  
(
)
V
J
Table 2. Varactor Voltages  
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 hyper-  
abrupt 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  
These subranges are made to overlap each other. Thus, if a rea-  
sonable RF swing (one that is appropriate in a practical VCO  
case) exceeds limits of the subrange, the C function described  
V
by the current subrange will still fit in the original curve.  
employed. Here the coefficients (V , M, C , and C ) are made  
J
JO  
P
piece-wise functions of the varactor DC voltage applied. Thus, the  
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200314 Rev. A • Skyworks Proprietary Information • Products and Product Information are Subject to Change Without Notice. • July 21, 2005  
5
APPLICATION NOTE • APN1005  
100  
1.0  
0.8  
0.6  
0.4  
0.2  
0
2.6  
2.4  
2.2  
2.0  
1.8  
1.6  
1.4  
1.2  
Approximation  
Measured  
10  
1
RS_PWL  
RS Measured  
20  
0.1  
0
5
10  
15  
20  
25  
30  
0
5
10  
15  
25  
30  
Varactor Voltage (V)  
Figure 6. SMV1265 Capacitance vs. Voltage  
Varactor Voltage (V)  
Figure 7. SMV1265 Resistance vs. Voltage  
Figure 6 demonstrates the quality of the piece-wise fitting  
approach.  
Since the epitaxial layer for this kind of hyperabrupt varactor has  
relatively high resistivity, the series resistance is strongly depen-  
dent on the reverse voltage applied to varactor junction. The  
Special consideration was given to the fit at the lowest capaci-  
tance range (high-voltage area) since it dramatically affects the  
upper frequency limit of the VCO.  
value of series resistance (R ) measured at 500 MHz is shown in  
S
Figure 7, with a piece-wise approximation of R also given.  
S
The piece-wise function may be used as follows:  
To incorporate this function into Libra, the pwl() built-in function  
was used in the “variables” component of the schematic bench.  
R = pwl (V 0 2.4 3 2.4 4 2.3 5 2.2 6 2 7 1.85 8 1.76 9  
S
VAR  
1.7 10 1.65 11 1.61 12 1.5 40 1.5)  
M = pwl (V 0 2 2.5 2 2.500009 25 6.5 25 6.50009 7.3 11  
VAR  
7.3 11.0009 1.8 40 1.8)  
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  
V = pwl (V 0 4 2.5 4 2.500009 68 6.5 68 6.50009 14 11  
J
VAR  
14 11.0009 1.85 40 1.85)  
C = pwl (V 0 0 2.5 0 2.500009 0 6.5 0 6.50009 0.9 11  
P
VAR  
0.9 11.0009 0.56 40 0.56)  
the original diode model, but its coefficients (V , M, C , and C )  
J
JO  
P
C
JO  
= pwl (V 0 22.5 2.5 22.5 2.500009 21 6.5 21 6.50009  
become parametric functions of the reverse voltage.  
VAR  
20 11 20 11.0009 20 40 20)*1012  
Note: While C is given in picofarads, C is given in farads to  
P
GO  
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).  
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July 21, 2005 • Skyworks Proprietary Information • Products and Product Information are Subject to Change Without Notice. • 200314 Rev. A  
6
APPLICATION NOTE • APN1005  
VCO Design and Performance  
Figure 8 shows the VCO schematic.  
R10  
2.4k  
VCC1  
5-8 V  
R3  
C6  
1000  
R6  
820  
120  
C4  
100  
R4  
120  
R7  
51  
R5  
R8  
1k  
820  
C5  
100  
T1  
16 x 0.4 mm  
V1  
V2  
NE68119  
NE68119  
R1  
R2  
L2  
L1  
R12  
50  
33  
33 33 nH  
33 nH  
A
C2  
10  
C1  
10  
T2  
15 x 0.7 mm  
D2  
D1  
T3  
R9  
1k  
SMV1265  
SMV1265  
3 X 0.7 mm  
R11  
1000  
VVAR1  
C3  
100  
Figure 8. VCO Schematic  
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200314 Rev. A • Skyworks Proprietary Information • Products and Product Information are Subject to Change Without Notice. • July 21, 2005  
7
APPLICATION NOTE • APN1005  
Table 3 shows the bill of materials used.  
Figure 9 shows the PCB layout. The board is made of standard FR4  
material 30 mils thick.  
Designators  
Comment  
Footprint  
0603  
The results measured with the circuit in Figure 8, as well as the  
simulated results obtained with the model in Figure 9, are shown  
in Figures 10 and 11.  
C
C
C
C
C
C
C
D
D
0603AU100JAT9 (AVX)  
0603AU100JAT9 (AVX)  
0603AU101JAT9 (AVX)  
0603AU101JAT9 (AVX)  
0603AU101JAT9 (AVX)  
0603AU102JAT9 (AVX)  
0603AU102JAT9 (AVX)  
SMV1265-011 (Skyworks)  
SMV1265-011 (Skyworks)  
LL1608-F33NJ (TOKO)  
LL1608-F33NJ (TOKO)  
CR10-330J-T (AVX)  
CR10-242J-T (AVX)  
CR10-102J-T (AVX)  
CR10-330J-T (AVX)  
CR10-121J-T (AVX)  
CR10-121J-T (AVX)  
CR10-821J-T (AVX)  
CR10-821J-T (AVX)  
CR10-510J-T (AVX)  
CR10-102J-T (AVX)  
CR10-102J-T (AVX)  
NE68119 (NEC)  
1
2
3
4
5
6
6
1
2
1
2
0603  
0603  
Note: The simulated tuning curve in Figure 10 agrees with mea-  
sured data, which proves the effectiveness of the above piece-wise  
approximation technique.  
0603  
0603  
0603  
Note: In the middle of the tuning range there is disagreement  
between our model and the measured results. This could be attrib-  
uted to the imperfection of the model, which is highly sensitive to  
the way different parasitic effects are treated. The other problem of  
modeling this oscillator case was the convergence of the harmonic  
balance. To facilitate convergence in this case, we kept the number  
of harmonics to at least five. The sweeping frequency range is rec-  
ommended to keep as close to the oscillation point as possible —  
especially when analyzing the middle band area.  
0603  
SOD-323  
SOD-323  
0603  
L
L
0603  
R
1
0603  
R
10  
R
11  
0603  
0603  
R
0603  
2
3
4
5
6
7
8
9
1
2
In Figure 11, the power response modeled at 7 V was very close to  
the measurement. Higher measured power is attributed to the ana-  
lyzer calibration (the calibration error of the analyzer is known to be  
within a couple of decibels). The general trend of the simulated  
results reflects the real VCO response almost exactly, which clearly  
demonstrates the model’s effectiveness.  
R
0603  
R
R
R
R
R
R
0603  
0603  
0603  
0603  
0603  
0603  
V
V
SOT-416  
SOT-416  
NE68119 (NEC)  
Table 3. Bill of Materials  
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July 21, 2005 • Skyworks Proprietary Information • Products and Product Information are Subject to Change Without Notice. • 200314 Rev. A  
8
APPLICATION NOTE • APN1005  
Figure 9. PCB Layout  
8
6
Measured  
2.2  
2.0  
1.8  
1.6  
1.4  
1.2  
1.0  
0.8  
Measured @ 7 V  
Simulated @ 7 V  
4
2
Simulations  
0
-2  
-4  
-6  
-8  
Measured @ 5 V  
0
5
10  
15  
20  
25  
30  
0
5
10  
15  
20  
25  
30  
Varactor Voltage (V)  
Figure 11. Power Response  
Varactor Voltage (V)  
Figure 10. Frequency Tuning  
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200314 Rev. A • Skyworks Proprietary Information • Products and Product Information are Subject to Change Without Notice. • July 21, 2005  
9
APPLICATION NOTE • APN1005  
Table 4 shows the measurement data and shows a useful tuning range  
of 0.84–2.23 GHz for the applied varactor voltage from 1–27 V.  
List of Available Documents  
1. Balanced Wideband VCO Simulation Project Files for Libra IV.  
2. Balanced Wideband VCO Circuit Schematic and PCB Layout for  
Protel EDA Client, 1998 version.  
V
Frequency  
(GHz)  
0.788  
0.842  
0.91  
P
OUT  
@ 7 V  
P
OUT  
@ 5 V  
VAR  
(V)  
0
(dBm)  
(dBm)  
3. Balanced Wideband VCO Gerber Photo-plot Files  
4. Detailed measurement and simulation data.  
3.5  
3.7  
3.7  
4.8  
6.5  
6.4  
6
-8.3  
-7.6  
-6.1  
-2.8  
1
1
For the availability of the listed materials, please call our applica-  
tions engineering staff.  
2
4
1.144  
1.492  
1.714  
1.848  
1.946  
2.016  
2.066  
2.106  
2.134  
2.198  
2.225  
2.238  
© Skyworks Solutions, Inc., 1999. All rights reserved.  
6
8
1.8  
10  
12  
14  
16  
18  
20  
25  
28  
30  
1.2  
5.2  
4.8  
4.4  
4.3  
4.4  
3.7  
3.5  
3.4  
-0.1  
-0.9  
-1.5  
-1.8  
-2.4  
-3.3  
-3.7  
-4  
Table 4. Tabulated Measurement Data  
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10  
APPLICATION NOTE • APN1005  
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. Skyworks assumes no responsibility for errors or omissions in these materials or the  
information contained herein. Skyworks may change its documentation, products, services, specifications or product descriptions at any time, without notice. Skyworks makes no commitment to  
update the materials or information and shall have no responsibility whatsoever for conflicts, incompatibilities, or other difficulties arising from any future changes.  
No license, whether express, implied, by estoppel or otherwise, is granted to any intellectual property rights by this document. Skyworks assumes no liability for any materials, products or  
information provided hereunder, including the sale, distribution, reproduction or use of Skyworks products, information or materials, except as may be provided in Skyworks Terms and  
Conditions of Sale.  
THE MATERIALS, PRODUCTS AND INFORMATION ARE PROVIDED “AS IS” WITHOUT WARRANTY OF ANY KIND, WHETHER EXPRESS, IMPLIED, STATUTORY, OR OTHERWISE, INCLUDING FITNESS FOR A  
PARTICULAR PURPOSE OR USE, MERCHANTABILITY, PERFORMANCE, QUALITY OR NON-INFRINGEMENT OF ANY INTELLECTUAL PROPERTY RIGHT; ALL SUCH WARRANTIES ARE HEREBY EXPRESSLY  
DISCLAIMED. SKYWORKS DOES NOT WARRANT THE ACCURACY OR COMPLETENESS OF THE INFORMATION, TEXT, GRAPHICS OR OTHER ITEMS CONTAINED WITHIN THESE MATERIALS. SKYWORKS  
SHALL NOT BE LIABLE FOR ANY DAMAGES, INCLUDING BUT NOT LIMITED TO ANY SPECIAL, INDIRECT, INCIDENTAL, STATUTORY, OR CONSEQUENTIAL DAMAGES, INCLUDING WITHOUT LIMITATION,  
LOST REVENUES OR LOST PROFITS THAT MAY RESULT FROM THE USE OF THE MATERIALS OR INFORMATION, WHETHER OR NOT THE RECIPIENT OF MATERIALS HAS BEEN ADVISED OF THE  
POSSIBILITY OF SUCH DAMAGE.  
Skyworks products are not intended for use in medical, lifesaving or life-sustaining applications, or other equipment in which the failure of the Skyworks products could lead to personal injury,  
death, physical or environmental damage. Skyworks customers using or selling Skyworks products for use in such applications do so at their own risk and agree to fully indemnify Skyworks for any  
damages resulting from such improper use or sale.  
Customers are responsible for their products and applications using Skyworks products, which may deviate from published specifications as a result of design defects, errors, or operation of  
products outside of published parameters or design specifications. Customers should include design and operating safeguards to minimize these and other risks. Skyworks assumes no liability for  
applications assistance, customer product design, or damage to any equipment resulting from the use of Skyworks products outside of stated published specifications or parameters.  
Skyworks, the Skyworks symbol, and “Breakthrough Simplicity” are trademarks or registered trademarks of Skyworks Solutions, Inc., in the United States and other countries. Third-party brands and  
names are for identification purposes only, and are the property of their respective owners. Additional information, including relevant terms and conditions, posted at www.skyworksinc.com, are  
incorporated by reference.  
Skyworks Solutions, Inc. • Phone [781] 376-3000 • Fax [781] 376-3100 • sales@skyworksinc.com • www.skyworksinc.com  
200314 Rev. A • Skyworks Proprietary Information • Products and Product Information are Subject to Change Without Notice. • July 21, 2005  
11  

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