design and simulation of wideband and low phase noise uhf synthesizer
DESCRIPTION
Journal of Telecommunications, ISSN 2042-8839, Volume 22, Issue 1, October 2013 www.journaloftelecommunications.co.ukTRANSCRIPT
JOURNAL OF TELECOMMUNICATIONS, VOLUME 22, ISSUE 1, OCTOBER 2013 14
Design and Simulation of Wideband and Low Phase Noise UHF Synthesizer
M. Majdi, F. Hodjat Kashani
Abstract—Design and simulation of a UHF wideband and low noise frequency synthesizer from 470 MHz to 860 MHz is presented. The proposed voltage controlled oscillator (VCO) in the phase lock loop (PLL) covers wide frequency bandwidth of 58% while phase noise performance has been optimized simultaneously, using parallel tuning diodes in the LC tank of modified Colpitts VCO. The result of the harmonic balance simulation shows an overall SSB phase noise less than -105 dBc/Hz at 10 KHz offset. The output power is more than 0dBm with maximum variation of 0.93 dB while using a high pass filter in the output. Index Terms—Frequency Synthesizer, SSB phase noise, Voltage Controlled Oscillator (VCO), Resonator Circuit, phase lock loop (PLL).
1 INTRODUCTION
The explosive growth of today’s telecommunication market has brought an increasing demand for high performance, low cost, low power consumption radio frequency circuits. Among all the RF blocks, the design of voltage-controlled oscillators (VCOs), which generate the LO carrier signal, is a major challenge and thus has received the most attention in recent years, as evidenced by the large number of publications [1-9]. The LOs are usually a frequency-synthesizer based on a phase locked loop (PLL) as depicted in the Fig. 1, in which the output oscillation signal is provided by a VCO.
Due to the ever-increasing demand for bandwidth in
communications, very stringent requirements are placed on the spectral purity of LOs, making the VCO design as a critical sub-circuit to the overall system performance. Some of digital video broadcasting (DVB) standards which are now spread throughout the world are operating in different parts of the UHF band. Therefore, in order to improve quality of service, RF unit components such as synthesizers should obtain appropriate spectral purity in desired bandwidth. The purpose of this paper is designing the low phase noise wideband UHF frequency synthesizer from 470 MHz to 860 MHz. The paper has been organized as follows: In section 2, UHF frequency synthesizer is designed. In this section, selecting resonator and oscillator structure and VCO topology are explained in detail. Then design and simulation of proposed VCO and proper loop filter are demonstrated. Finally simulation of UHF
frequency synthesizer is presented . in section 3, some conclusions are offered. 2 DESIGNING THE UHF FREQUENCY SYNTHESIZER In this paper, we are going to design the low phase noise UHF frequency synthesizer with the frequency range of 470MHz to 860MHz. So as to design the low
noise wideband UHF frequency synthesizer, the Δ−Σ based fractional-N frequency synthesizer has been used which contains a low noise digital phase frequency detector (PFD),a precision charge pump ,a programmable reference divider and also the programmable N-fractional
loop divider with the third-order Δ−Σ modulator. Designing VCO with the wideband structure considering the minimum output power variations along the band and also a minimum phase noise, designing an appropriate loop filter, choosing a suitable reference crystal with the minimum phase noise with the highest stability have been considered as important parts in designing of the proposed synthesizer [1].
2.1 DESIGNING THE VOLTAGE CONTROLLED OSCILLATOR
Each VCO contains three main parts. One of them is the active circuit which its main element is the transistor and it converts the dc power to the ac power by creating the negative resistance. The second part is a load network which receives the generated ac power and the third part is a resonator network which allows transmitting the generated power to the load only in its resonant frequency. In accordance with the vital VCO features such as the output power, phase noise characteristic and the required frequency bandwidth, the structure of the oscillator and its resonator circuit have been determined. The optimum design of the VCO and decreasing its phase noise level as one of the main sources of the PLL output phase noise plays a significant role in declining the phase noise level of synthesizer.
2.1.1 ACTIVE DEVICE AND VARACTOR DIODE SELECTION
Fig. 1. Block diagram of PLL-based frequency synthesizers.
———————————————— • M. Majdi is with the Electrical Engineering Department of Islamic Azad
University Tehran south branch. • F. Hodjat Kashani is with Iran University of Science and Technology,
Narmak, Tehran, Iran.
JOURNAL OF TELECOMMUNICATIONS, VOLUME 22, ISSUE 1, OCTOBER 2013 15
BJT and HBT Transistors with lower Flickr noise are used in applications such as oscillators, VCO and multipliers in order to obtain the output spectrum with the high purity. So, the chosen transistor in this part is a low-noise BJT, NPN type which its fT is equal 45GHz and hFE is approximately 140. If Ic is 20 mA, the 1-dB compression point will be 12dBm. Furthermore, for Ic=7mA, the mentioned amount is 5dBm. Varactor diode is another semiconductor device of the circuit which should be chosen based on the requirements. Abrupt varactors possess the higher Q, so those VCOs, which use this kind of diode, have better characteristic of the phase noise and the lower bandwidth. But, in return, the hyperabrupt varactor has the greater capacitance change for a given voltage change as well as a linear frequency versus voltage characteristic over a limited voltage range. So it can cover a greater frequency bandwidth. Our proposed UHF VCO covers wide frequency bandwidth more than 10%, so varactor has been selected which includes a high capacitance ratio and low series resistance. Therefore, the SMV1800-079LF silicon hyperabrupt varactor diode has been used. The control voltage of the mentioned varactor diode has the potential to sweep along 0 to 30 volt. If the voltage is 0 and 30, its capacitance will be 15.78 pF and 0.84 pF respectively. In order to covering the frequency band in the range of 470 to 860 MHZ, the control voltage has been declined to the range of 1.35 to 4.68 voltage based on the arrangements of varactor diodes in the resonator circuit. The curves relevant to characteristic of the capacitor in terms of the voltage for the mentioned varactor diode has been shown in fig. 2.
2.1.2 BIAS POINT SELECTION The DC bias point of oscillators is selected in the class A like the power amplifiers. Voltage and current of the bias should be enough to allow the necessary voltage and current changes of the output RF to generate the vital output power. It is usually attempted to consider collector voltage and current small in the low noise oscillators however by this way, output power would be reduced. In the specific situations that output power is not a significant and impressive parameter in designing, bias point could be selected in the saturation zone of the transistor which the transistor indicates the linear behavior itself and the harmonics have a negligible effect on the output power of the major harmonic. The bias point and DC parameters of oscillator circuit are represented in
table 1.
2.1.3 STRUCTURE OF THE OSCILLATOR
The prerequisite to have a fluctuation in the output of an oscillator is that the stability factor (K) of the network which is used as an active device and the supplier of the negative resistance related to the oscillator, should be less than 1. So, if the stability factor of the applied transistor in the oscillator is more than 1, it should be made unstable in a possible manner. In this design due to cover a variety of the frequency range at the UHF band nearly 58%, modified colpitts structure is used. The colpitts is modified by inductive resistance of limited Q of the inductor, with the aim of its parallel negative resistance
observed on the transistor base. Fig. 3 presents the modified colpitts oscillator with its bias circuit that its active segment is a BJT transistor. The inductors and capacitors values have been considered as follows: C1=3.3 pF, C2=3.9 pF, Lt=10 nH, [10].
In order to analysis of possibility and stability of the oscillation related to the oscillator by using S parameters of BFP520 transistor, stability factor (k) in the various frequencies from 470MHz to 860MHz, is less than 1. Achieved results of surveying the transistor stability in the common emitter at the mentioned frequency limit, present that K values are less than one in the whole frequency ranges, so the transistor is unstable in the range. So, to expand the unstable region, the capacitive feedback has been used in the transistor emitter.
TABLE 1 BIAS CIRCUIT PARAMETERS OF THE
TRANSISTOR
Fig. 2. C-V characteristic of the SMV1800-079LF varactor diode.
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2.1.4 STRUCTURE OF THE FREQUENCY RESONATOR
In designing the wide band, the most common resonators are adjustable ones with hyperabrupt varactor diode. C-V characteristic of this kind of diodes is approximately non linear. So, by connecting the frequency resonator to the transistor’s base, it could be made to increase the bandwidth of VCO. Moreover, the small current of the transistor’s base-when the resonator is connected to it- will be more effective than other transistor pins to decrease the phase noise of the VCO output. To prevent the effect of bias voltage of the varactors on the oscillator circuit, varactor diode and transistor should be isolated on dc side respect to each other, for this purpose, resonator and oscillator have to be coupled together with a large dc coupled capacitor. If the varactor diode is located on the resonator circuit serially, a further bandwidth would be attained. Different states of the varactor diode (Ctot) which could be existed with the inductor (Lt) on the transistor’s base in fig. 3, are presented in fig. 4. Cp capacitor could be resulted to the non ideal inductor in fig. 4,Series capacitor Cs has been used to complete the circuit for alternating current but isolates the cathode of the tuner diode from the coil and thus from the negative terminal of the tuning voltage. For high-frequency purposes the biasing resistor is connected in parallel with the series capacitor. The parallel loss resistance transformed into the circuit Rc, is calculated as in (1).
( )
2
2
2
1⎟⎟⎠
⎞⎜⎜⎝
⎛
−+=
PS
SBC CCL
LCRR
ωω (1)
If two varactors are used in the resonator as shown in
fig. 4, Rc resistance will be independent of frequency across the entire tuning range, as in (2).
BC RR 4= (2)
So, bias resistor does not have any influence on bandwidth of the circuit. This arrangement has the
advantage that the capacitance shift caused by the ac modulation acts in opposite directions in these diodes and therefore, cancels itself.
So as to close the circuit for alternating current, series capacitor Cs is used. Although the existence of Cs makes increase the quality factor, it decreases the capacitance ratio and range of varactor adjustment voltage, as in (3).
Thus, in designing the circuit, it is notable that the amount of the series capacitor Cs should be chosen large enough in order not to restrict the effective capacitance variation. The parallel capacitance Cp is always present, since wiring capacitances are inevitable and every coil has its self-capacitances.as in (4),
⎪⎪⎪⎪
⎩
⎪⎪⎪⎪
⎨
⎧
+
+
=⎟⎟⎠
⎞⎜⎜⎝
⎛
⎟⎟⎠
⎞⎜⎜⎝
⎛+=
⇒⎟⎟⎠
⎞⎜⎜⎝
⎛+=
min
max
min
max
min
max
1
1
1
1
CCCC
CC
CC
CC
CC
CC
P
P
eff
tot
Peff
tot
Ptoteff
(4)
Fig. 3. The modified colpitts oscillator and biasing circuit.
⎪⎪⎪⎪⎪⎪
⎩
⎪⎪⎪⎪⎪⎪
⎨
⎧
+=
+
+
=⎟⎟⎠
⎞⎜⎜⎝
⎛
⎟⎟⎠
⎞⎜⎜⎝
⎛+=
⇒+
=
S
toteff
S
S
eff
S
toteff
S
tottoteff
CC
VV
CCCC
CC
CC
CC
CC
CC
1
1ˆˆ
1
1
1
1
1max
min
min
max
min
max
(3)
Fig. 4. (a) parallel-resonant circuit with two varactor diode, (b) parallel-resonant circuit with varactor diode, and bias resistor in parallel to the diode.
Fig. 5. The final scheme of the UHF VCO.
JOURNAL OF TELECOMMUNICATIONS, VOLUME 22, ISSUE 1, OCTOBER 2013 17
The Q of the effective tuning capacitance rises with the magnitude of the parallel capacitance. In view of the fact that even a comparatively small shunt capacitance reduces the capacitance ratio considerably, it is necessary to ensure low wiring and coil capacitance in the layout stage of the
circuit design. So high quality inductors ought to be used. The frequency range can be tuned by means of the tuning diode depends on the useful capacitance ratio of the diode and on the parallel and series capacitances present in the circuit, as in (5).
⎟⎟⎠
⎞⎜⎜⎝
⎛+
+
⎟⎟⎠
⎞⎜⎜⎝
⎛+
+
=
SP
SP
CC
CC
C
CCC
C
C
ff
max
min
max
max
max
max
min
max
1
11
(5)
Now, if Cs is large enough, (5) could be written as (6).
P
P
CCCC
ff
min
max
min
max
1
1
+
+
= (6)
As presented in the (6), while Cs value is large enough, frequency range will be dependent on Cp. Thus, the larger series capacitor Cs and smaller parallel parasitic capacitor Cp would make less restriction on bandwidth. According to different techniques and their features as mentioned above, the proposed resonator circuit has been designed by using several tuning diodes in parallel arrangement. Improved phase-noise and bandwidth performance can be obtained by using this structure.
2.1.5 DESIGN AND SIMULATION OF VCO The design of proposed VCO has been represented in fig. 5. In this design, the mentioned frequency resonator is used. After simulating by ADS software it implies that arrangements of the varactor diodes, improve capacitance ratio which is required to cover the desired bandwidth. In addition, it causes to decline the total resistance of diodes
and decrease diode’s noise contribution. Indeed, by keeping the capacitance ratio, we can decrease the required control voltage. In addition, by connecting the resonator circuit to the base of the transistor, we achieved an appropriate structure for VCO to reach a better output phase noise characteristic [11],[12].
As illustrated in fig. 5, by using parallel inductor as a high pass filter in the VCO output the variation of the output power decrease from 1.78dB to 0.93dB at the frequency range of 470 to 860 MHz as shown in fig. 6.
The Results of the output parallel inductor value optimization is introduced in table 2. P1, p2 and p3 are the output power at the first, middle and the end of UHF
band, respectively.
Other designed VCO parameters have been shown in
Fig. 6. (a) VCO output power before variation optimization. (b) VCO output power after variation optimization.
TABLE 2 RESULTS OF THE OUTPUT PARALLEL INDUCTOR VALUE
OPTIMIZATION
Fig. 9. SSB phase noise power spectrum of VCO output.
TABLE 3 CHARACTERISTICS AND PERFORMANCE SUMMARY
OF PROPOSED VCO
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table 3.
Also, VCO output frequency variations in terms of varactor diode control voltage variations, VCO output voltage waveforms in terms of the time and its spectrum and SSB phase noise power spectrum of VCO output in frequency terms are shown in fig. 7, fig. 8, and fig. 9.
2.2 LOOP FILTER DESIGN
In this design, to prevent increasing phase noise, the
second order passive filter as shown in fig. 10, is proposed
[1].
The bandwidth of 38 KHz and 45º phase margin is resulted in simulation of optimized loop filter. The
amplitude and phase of the open and closed loop gain for this filter have been shown in fig. 11, and fig. 12.
2.3 DESIGN AND SIMULATION OF SYNTHESIZER
The N-fractional frequency synthesizer chip that is used in
this design consists of a digital phase-frequency detector, charging pump, programmable reference frequency divider and the N-fractional main divider of the loop with
third order ∑-∆ modulator which is programmable. Fig. 13 shows lock time of the loop in 636MHz and fig. 14 shows output phase error of the loop.
Fig. 10. Second Order Passive Low-Pass Filter.
Fig. 8. VCO output voltage waveforms in terms of the time and its spectrum.
Fig. 7. VCO output frequency variations in terms of varactor diode control voltage variations.
Fig. 11. Amplitude and phase of open loop system gain.
Fig. 12. Amplitude and phase of closed loop system gain.
Fig. 15. Phase Noise Of The Synthesizer.
TABLE 4 CHARACTERISTICS AND PERFORMANCE SUMMARY OF
FREQUENCY SYNTHESIZER
JOURNAL OF TELECOMMUNICATIONS, VOLUME 22, ISSUE 1, OCTOBER 2013 19
Fig. 15 shows the phase noise of the designed synthesizer and table 4 illustrated characteristics and performance summary of this synthesizer.
3 CONCLUSION
In this paper, design and simulation of the wideband and low phase noise UHF frequency synthesizer have been presented. A wideband VCO, as a key circuit in the PLL, with respect to the low phase noise is designed by using modified colpitts structure and a number of tuning diodes in different arrangement as the parallel resonator. The simulation results show -119.833 dBc/Hz phase noise at 100 KHz offset frequency and the tuning range is as wide as 58% from 470MHz to 860MHz. The output power variation of the VCO is optimized to 0.93dB. Finally, a PLL is designed using a proper crystal and loop filter with the bandwidth of 38 KHz. The desirable bandwidth (470MHz
to 860MHz) is achieved for the synthesizer while the SSB phase noise is less than -105dBc/Hz at 10 KHz offset
frequency in the output of the PLL.
REFERENCES [1] Ulrich L. Rohde, Microwave and Wireless Synthesizers: Theory and
Design, by John Wiley & Sons, New York, NY,ISBN: 0471-‐52019-‐5 , August, 1997 .
[2] J. Hojung, K. Jongsun, “A Low-‐Power Wideband multi-‐frequency synthesizer for mobile TV tuner ICs,” IEICE Electronics Express, vol. 7, no. 2, 92-‐97, January, 2010.
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[5] J. P. Mathurin, J. Mercier, “Wide Band frequency synthesis”, Radar Conference-‐Surveillance for a Safer World, 2009. (IEEE Conferences)
[6] Y. Peng, G. Zheng, G. Ming, S. Yin, F.F. Dai, “A 430MHz-‐2.15GHz fractional-‐N frequency synthesizer for DVB and ABS-‐S applications,” Custom Integrated Circuits Conference, 2009. CICC ’09. IEEE. (IEEE Conferences)
[7] S. Saeedi, M. Atarodi, “Single-‐VCO multi-‐band DTV frequency Synthesizer with a divide-‐by-‐3 frequency divider for quadrature signal generation,” Electrical Engineering Department, Sharif University, 2009.
[8] J. Shin, J. Kim, S. Kim, J. Choi, ,N. Kim,Y. S. Eo,H. Shin, ”A Wideband Fractional-‐N Frequency Synthesizer with Linearized Coarse-‐Tuned VCO for UHF/VHF Mobile Broadcasting Tuners,” Korea IEEE Aslan Solid-‐State Circuits Conference, 2007.
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[10] U. L. Rohde, A. K. Poddar, “An Analytical Approach of Minimizing VCO Phase Noise,” Synergy Microwave Corporation, IEEE, APMC2005.
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M. Majdi received her B.S. and M.S. degrees both in electrical engineering from Islamic Azad University Tehran south branch, in 2005 and 2010, respectively. She is with the Civil Aviation Technology College since 2007. Her research interests include frequency synthesizers and active microwave circuit design. F. Hodjat Kashani received his B.S. degree in Electrical Engineering from University of Tehran, M.S. degree in Electrical Engineering from UCLA and Ph.D. degree in Electrical Engineering from University of California Los Angeles, in 1962, 1968 and 1970, respectively. he is Full Prof. of Electrical Engineering of Iran University of Science and Technology. His Expertise is about Antenna Design, Microwave and Millimeter Wave Community, Meta-materials and EBG structures. He has more than twenty Research and Industrial Projects as “Design and Implementation of a Conical Wraparound Antenna”.
Fig.13. Lock Time of Output Frequency (at 636MHz).
0 100 200 300 400 500 600 700 800 900 1000Time (us)
-50 -40 -30 -20 -10
010 20 30 40 50
Phas
e Er
ror (
deg)
Output Phase Error
Fig.14. Loop Output Phase Error.