This application claims benefit of Serial No. 2006-121248, filed 19 May 2009 in Japan and which application is incorporated herein by reference. To the extent appropriate, a claim of priority is made to the above disclosed application.
1. Field of the Invention
The present invention relates to a voltage-controlled oscillator (VCO), which oscillates at a frequency proportional to a control input voltage, and more particularly to an LC-tank voltage-controlled oscillator (LC-VCO).
2. Description of the Related Art
The phase noise of an LC-tank voltage-controlled oscillator is determined by the S/N ratio (Signal-to-Noise Ratio) in the LC tank. The root mean square values of signal voltage Vsig and noise voltage Vn are respectively expressed as
Vsig2=Rt2Isig2
Vn2=4kTRt
where k is the Boltzmann constant, T is the absolute temperature, Rt is the parallel impedance of the LC tank, and Isig is the signal current amplitude.
Hence, the root mean square value of the S/N ratio is given as
(S/N)2=Rt2Isig2/4kT
From the above equation, it can be seen that phase noise improves with increasing signal amplitude. However, since the signal amplitude is limited by supply voltage, the phase noise degrades when VCO is operated at a low supply voltage.
In the prior art, a transformer-feedback (TF) VCO is proposed as a VCO that operates at a low supply voltage (refer to non-patent document 1 listed below). In this transformer-feedback VCO, each source node voltage in a cross-coupled transistor pair is lowered below 0 [V] by a transformer, and the voltage amplitude in the LC tank is increased. However, since the operation involves current flow in a region where the impulse sensitivity function (ISF) is large, it is difficult to achieve a low-phase-noise design with this technique.
On the other hand, an LC-VCO known as a Class-C VCO is proposed (refer to non-patent documents 2 and 3 listed below). This VCO is constructed so that, in an LC-VCO having a cross-coupled transistor pair, the transistor gate portion is DC-cut by a capacitor to lower the gate bias below the threshold, thereby causing the transistor to operate as if it were a class-C amplifier.
In a VCO, the ISF from thermal noise to phase noise differs depending on the phase of oscillation. More specifically, the ISF is smaller for a phase where the amplitude of the oscillation voltage is larger. The class-C VCO is intended to achieve low phase noise by flowing a current only in a phase range where the ISF is small. However, in the class-C VCO, the gate bias must be reduced below the threshold voltage. As a result, under low supply voltage conditions, the amplitude cannot be made large enough, and oscillations may not occur. On the other hand, under low amplitude conditions, the conduction angle cannot be reduced to take advantage of the characteristics of the class-C VCO, and the intended low phase noise cannot be achieved.
Non-patent document 1: K. Kwok, and H. C. Luong, “Ultra-Low-Voltage High-Performance CMOS VCOs Using Transformer Feedback,” IEEE JSSC, vol. 40, no. 3, pp. 652-660, March 2005.
Non-patent document 2: A. Mazzanti, and P. Andreani, “Class-C Harmonic CMOS VCOs, With a General Result on Phase Noise,” IEEE JSSC, vol. 44, no. 12, pp. 2716-2729, December 2008.
Non-patent document 3: A. Mazzanti, and P. Andreani, “A 1.4 mW 4.90-to-5.65 GHz Class-C CMOS VCO with an Average FoM of 194.5 dBc/Hz,” ISSCC, No. 26-2, February 2008.
The present invention has been devised in view of the above problem, and it is an object of the invention to provide a voltage-controlled oscillator that can achieve low phase noise while ensuring stable oscillation startup and stable oscillation maintenance even under low supply voltage conditions.
To achieve the above object, according to the present invention, a voltage-controlled oscillator is provided, which includes an LC parallel resonant circuit whose impedance varies with a control input voltage and a negative resistance circuit for introducing negative resistance into the LC parallel resonant circuit, the negative resistance circuit comprising at least: a first amplifier circuit, provided in parallel with the LC parallel resonant circuit and having a first pair of transistors cross-coupled via a capacitor, that achieves class-C amplifier operation by biasing a gate or base of each transistor in the first transistor pair with a first bias voltage; and a second amplifier circuit, provided in parallel with the LC parallel resonant circuit and having a second pair of transistors cross-coupled via a capacitor, that achieves class-C amplifier operation by biasing a gate or base of each transistor in the second transistor pair with a second bias voltage which is different from the first bias voltage.
In the voltage-controlled oscillator according to the present invention, amplifier circuits each having a cross-coupled transistor pair are provided in parallel (dual configuration), and are respectively biased with different DC bias voltages, achieving class-C amplifier operation with different conduction angles. In this configuration, the amplifier circuit having the smaller conduction angle acts to reduce the phase noise, while the amplifier circuit having the larger conduction angle acts to ensure stable oscillation startup. As a result, the voltage-controlled oscillator according to the present invention achieves low phase noise while ensuring stable oscillation startup and stable oscillation maintenance even under low supply voltage conditions.
Further features and advantages of the present invention will be apparent from the following description with reference to the accompanying drawings, in which:
The embodiments of the present invention will be described below with reference to the accompanying drawings.
The LC parallel resonant circuit 100 is essentially a loop, which as shown in
The first and second amplifier circuits 120 and 140 act as a negative resistance circuit that supplies energy to the LC parallel resonant circuit 100 in such a manner as to cancel out the resistance of the resonant circuit 100 by introducing negative resistance into the resonant circuit 100. That is, N-channel MOS (Metal-Oxide Semiconductor) FET (Field-Effect) transistors contained in the respective amplifier circuits act to increase the current that flows through the LC parallel resonant circuit 100.
More specifically, the first amplifier circuit 120 is provided in parallel with the LC parallel resonant circuit 100, and includes a first transistor pair formed from transistors (NMOSFETs) Q11 and Q12 cross-coupled via capacitors C11 and C12. That is, the first output signal voltage VOUT1 is connected not only to the drain of the transistor Q11 but also to the gate of the transistor Q12 via the DC-cut capacitor C11. Likewise, the second output signal voltage VOUT2 is connected not only to the drain of the transistor Q12 but also to the gate of the transistor Q11 via the DC-cut capacitor C12. The sources of the transistors Q11 and Q12 are both grounded. On the other hand, the gates of the transistors Q11 and Q12 are connected to a bias voltage Vgbias1 via resistors R11 and R12, respectively.
The second amplifier circuit 140 has essentially the same circuit configuration as the first amplifier circuit 120. The difference is that the gates of the transistors Q21 and Q22 are connected to a bias voltage Vgbias2, which is higher than Vgbias1.
The VCO shown in
f=½π√(LC)
The two output signal voltages VOUT1 and VOUT2 of the VCO are 180° out of phase with each other as shown by the following equations, where At is the amplitude of each output voltage and φ is the phase of either one of the output voltages. Here, VDS represents the drain-source voltage of the transistor Q11.
V
OUT1
=V
DD
−A
t cos φ=VDS
V
OUT2
=V
DD
+A
t cos φ
At<VDD
In the amplifier circuits 120 and 140, the gate bias voltage Vgbiasn (n is 1 or 2) is adjusted relative to the transistor threshold voltage Vth such that
V
gbiasn
+A
t
−V
th>0
Further, the gate bias voltage Vgbiasn is set so that the following relationship holds.
Vgbias1<Vgbias2
The transistor Q11 conducts in the phase range represented by −Φ1[rad]<φ<+Φ1[rad] where Vgs1-Vth>0. In the illustrated example, Φ1=π/5. On the other hand, the transistor Q21 conducts in the phase range represented by −Φ2[rad]<φ<+Φ2[rad] where Vgs2Vth>0. In the illustrated example, Φ2=π/2>Φ1.
As a result, drain-source currents Ids1 and Ids2 with current waveforms shown in
Then, the current Ids1 having the smaller conduction angle 2Φ1 contributes to achieving low phase noise, since the current flows in a concentrated manner in a region centered about the phase φ=0 where the ISF (Impulse Sensitivity Function) is the smallest. On the other hand, the current Ids2 having the larger conduction angle 2Φ2 serves as an oscillation startup current to ensure stable oscillation startup and stable oscillation maintenance.
For transistors Q21 and Q22, where the current Ids2 having the larger conduction angle flows, it is preferable to reduce their transistor sizes. Further, the conduction angle 2Φ1 can be reduced by reducing Vgbias1 as much as possible under conditions determined by the amplitude.
With the above operation, the VCO shown in
Further, in each of the circuits shown in
It is also possible to use NPN bipolar transistors or PNP bipolar transistors instead of the N-channel MOSFETs or the P-channel MOSFETs, respectively. When bipolar transistors are used instead of the field-effect transistors (unipolar transistors), the sources are replaced by the emitters, the gates by the bases, and the drains by the collectors.
While the above embodiments have each been described as being provided with two amplifiers each having a cross-coupled transistor pair, it is also possible to connect a third amplifier circuit in parallel with the LC parallel resonant circuit and to achieve class-C amplifier operation with a third conduction angle by applying a third bias voltage to its gate or base. Such a VCO configuration can achieve a further precise oscillation-startup and low-noise design. In other words, the number of amplifier circuits each having a cross-coupled transistor pair can be suitably chosen according to the design.
The voltage-controlled oscillator according to the present invention can be used in application that require ultra-low power consumption, such as wireless sensor networks, battery-driven mobile devices, and biometrics.
The invention may be embodied in other specific forms without departing from the spirit or essential characteristics thereof. The present embodiment is therefore to be considered in all respects as illustrative and not restrictive, the scope of the invention being indicated by the appended claims rather than by the foregoing description and all changes which come within the meaning and range of equivalency of the claims are therefore intended to be embraced therein.
Number | Date | Country | Kind |
---|---|---|---|
2009-121248 | May 2009 | JP | national |