1. Field of the Invention
The present invention relates to a piezoelectric oscillator for oscillating a piezoelectric vibrator, such as a crystal vibrator.
2. Description of the Related Art
A temperature-compensated crystal oscillator is a crystal oscillator that is employed to provide a reference frequency for a cellular phone, and that offsets a thermal characteristic of a crystal vibrator (a piezoelectric vibrator), and possesses a property such that there is little variation in frequency due to temperature changes. Regards oscillator use, there has been a recent increased demand for temperature-compensated crystal oscillators that can be operated, at low voltages, in cellular phones and GPS systems.
A conventional crystal oscillator circuit (prior art 1) is shown in
Another crystal oscillator circuit (prior art 2) is shown in
Patent Document 1: JP-A-2003-318417
In the crystal oscillator circuit in
In order to obtain an appropriate negative resistance for the crystal oscillator circuit in prior art 1, generally, about three times the threshold voltage of an MOS transistor is required as the internal regulator voltage that drives the CMOS inverter amplifier 40.
When the internal regulator voltage is dropped, a satisfactory gate-source voltage VGS cannot be obtained, and the gain of the CMOS inverter amplifier 40 is lowered. As a result, problems such as degradation of the negative resistance and a delayed oscillation start time occur.
As one method for improving the negative resistance, the size of an MOS transistor is increased to obtain a large gain for the CMOS inverter amplifier 40. When this method is employed, however, the consumption of power is increased.
Further, for the crystal oscillator in
The present invention is provided while taking these conventional problems into account, and one objective of the present invention is to provide a piezoelectric oscillator that can be operated at a low voltage.
A piezoelectric oscillator according to the invention comprises an amplifier connected in parallel to a piezoelectric vibrator; and a load capacitor connected in parallel to the piezoelectric vibrator, wherein the amplifier includes an inverter that is comprised of a first PMOS transistor and an NMOS transistor that are connected in series, a DC cut capacitor connected between a gate terminal of the first PMOS transistor and a gate terminal of the NMOS transistor and a feedback resistor connected to the gate terminal of the NMOS transistor and an output terminal of the amplifier, and wherein a bias voltage that is smaller than half of a source voltage of the inverter is applied to the gate terminal of the first PMOS transistor.
According to this arrangement, when a bias voltage that is smaller than half of a source voltage of the inverter is applied to the gate terminal of the first PMOS transistor, which is a constituent of the amplifier, the gate-source voltage VGS of the first PMOS transistor can be raised, and accordingly, a gain of the amplifier can be increased. Therefore, during a low-voltage operation, a satisfactory negative resistance can still be obtained. Furthermore, since the phases of the oscillation amplitudes of the gate terminal of the first PMOS transistor and of the gate terminal of the NMOS transistor are the same, when the NMOS transistor is ON, the PMOS transistor is OFF. Thus, the consumption of power can be reduced, compared with when a constant current is supplied to the NMOS transistor.
The piezoelectric oscillator of this invention further comprises a high-frequency elimination resistor connected to the gate terminal of the first PMOS transistor, wherein the predetermined bias voltage is to be applied via the high-frequency elimination resistor.
Furthermore, the piezoelectric oscillator of this invention comprises a bias voltage generator circuit for generating the predetermined bias voltage, wherein the bias voltage generator circuit includes a second PMOS transistor that is diode-connected, and a current source connected in series to the second PMOS transistor. In addition, the piezoelectric oscillator of this invention comprises a bias voltage generator circuit for generating the predetermined bias voltage, wherein the bias voltage generator circuit includes a second PMOS transistor that is diode-connected, and a load resistor connected in series to the second PMOS transistor.
According to this arrangement, the bias voltage generator circuit generates a bias voltage that offsets a variation in the threshold voltage of the first PMOS transistor and the thermal characteristic thereof, and applies the bias voltage to the gate terminal of the first PMOS transistor. Thus, power consumption, variations in the negative resistance and changes due to the thermal characteristics can be reduced. Further, since with this arrangement, noise produced by the power source of the amplifier can be offset, while phase noise can also be reduced.
Moreover, according to the present invention, a piezoelectric oscillator comprises an amplifier connected in parallel to a piezoelectric vibrator; and a load capacitor connected in parallel to the piezoelectric vibrator, wherein the amplifier includes an inverter that is comprised of a PMOS transistor and an NPN transistor connected in series, a DC cut capacitor connected between a gate terminal of the PMOS transistor and a base terminal of the NPN transistor, and a feedback resistor connected to a gate terminal of the NPN transistor and an output terminal of the amplifier, and wherein a bias voltage that is smaller than half of a source voltage of the inverter is to be applied to the gate terminal of the PMOS transistor.
According to this arrangement, since an arbitrary bias voltage is applied to the gate of the PMOS transistor that is a constituent of the amplifier, the gate-source voltage of the PMOS transistor can be raised, and accordingly, the amplifier gain can be increased. Further, by using the NPN transistor, a greater improvement in the negative resistance can be obtained, even during a low-voltage operation.
According to the piezoelectric oscillator of the invention, a predetermined bias voltage is applied to the gate terminal of the first PMOS transistor, which is a constituent of the amplifier, the gate-source voltage VGS of the first PMOS transistor can be raised and the gain of the amplifier can be increased. Therefore, a satisfactory negative resistance can still be obtained during a low-voltage operation.
The embodiments of the present invention will now be described while referring to drawings.
The operation of the piezoelectric oscillator of this embodiment will now be described while referring to
Furthermore, the input terminal 30 and the output terminal 31 of the CMOS inverter amplifier 40 are connected via the feedback resistor 1, and their bias voltages are equal. For example, when the power voltage VDD of the CMOS inverter amplifier 40 is 1.5 V, the gate voltage (a voltage at the gate terminals of the PMOS transistor 2 and the NMOS transistor 3) is an intermediate voltage, i.e., 0.75 V, and the gate-source voltage VGS1 of an MOS transistor, which is a constituent of the CMOS inverter amplifier 40, is also 0.75 V. Since the threshold voltage of the general MOS transistor is about 0.7 V, a satisfactory gain cannot be obtained for the CMOS inverter amplifier 40.
According to the piezoelectric oscillator shown in
When as shown in
As described above, according to the piezoelectric oscillator of this embodiment, when an arbitrary bias voltage is applied to the gate terminal of the PMOS transistor 15, which constitutes the amplifier 41, the gate-source voltage VGS of the PMOS transistor 15 can be raised and a large gain for the amplifier 41 can be obtained. Therefore, a satisfactory negative resistance is ensured, even during low-voltage operation. In addition, when the internal regulator voltage is three times or higher than the threshold voltage of an MOS transistor, the negative resistance can still be increased in a high frequency band.
Further, the phases of oscillated signals at the gate terminal of the PMOS transistor 15 and at the gate terminal of the NMOS transistor 17 are the same, and when the NMOS transistor 17 is ON, the PMOS transistor 15 is OFF. Thus, power consumption can be reduced, compared with when, as in prior art 2 in
As shown in
With this arrangement, a bias voltage is applied to the gate terminal 30 of the first PMOS transistor 15 in order to offset a threshold voltage VT and the thermal characteristics of the first PMOS transistor 15. Here, in order to offset the threshold voltage VT and the thermal characteristics of the PMOS transistor 15, it is necessary to set a condition in which a power voltage VDD of the first PMOS transistor 15 is equal to a power voltage VDD of the second PMOS transistor 25, a gate-source voltage of the first PMOS transistor 15 is equal to a gate-source voltage of the second PMOS transistor 25, a gate width of the first PMOS transistor 15 is larger than a gate width of the second PMOS transistor 25, and a gate length of the first PMOS transistor 15 is smaller than a gate width of the second PMOS transistor 25.
As described above, according to the piezoelectric oscillator of this embodiment, since a bias voltage is applied to the gate terminal of the PMOS transistor 15 to offset a variation in the threshold voltage VT and the thermal characteristics of the PMOS transistor 15, power consumption, a variation in the negative resistance and a change due to the thermal characteristics can be reduced. Furthermore, since noise produced by the power source of the amplifier 41 can be offset, phase noise can also be lowered.
In the first and second embodiments, the negative resistance depends on the gain for the NMOS transistor 17, and when as shown in
As described above, according to the piezoelectric oscillator of this embodiment, when an arbitrary bias voltage is applied to the gate of a PMOS transistor 15 of an amplifier 41, the gate-source voltage VGS of the PMOS transistor 15 can be increased, and for the amplifier 41, a large gain can be obtained. Furthermore, even during a low-voltage operation, a greater improvement in negative resistance is possible.
Although an arbitrary bias voltage is to be applied to the gate terminal of the PMOS transistor in the first embodiment, as shown in the fourth embodiment, it is possible to configure so that an arbitrary bias voltage can be applied to the gate terminal of the NMOS transistor.
Here, although the arbitrary bias voltage that is smaller than half of the power voltage VDD of the CMOS inverter amplifier needs to be applied in the first embodiment, in the forth embodiment, the arbitrary bias voltage 124 that is larger than half of the power voltage VDD of the amplifier 141 need to be applied.
As described above, according to the piezoelectric oscillator of this fourth embodiment, even when an arbitrary bias voltage is applied to the gate terminal of the NMOS transistor 117, which constitutes the amplifier 141, a satisfactory negative resistance is also ensured, even during low-voltage operation.
Also, although an arbitrary bias voltage is to be applied to the gate terminal of the PMOS transistor in the second embodiment, as shown in the fifth embodiment, it is possible to configure so that an arbitrary bias voltage can be applied to the gate terminal of the NMOS transistor.
Here, although the arbitrary bias voltage that is smaller than half of the power voltage VDD of the CMOS inverter amplifier needs to be applied in the second embodiment, in the fifth embodiment, the arbitrary bias voltage that is larger than half of the power voltage VDD of the amplifier 241 need to be applied.
As shown in
With this arrangement, a bias voltage is applied to the gate terminal 232 of the first NMOS transistor 217 in order to offset a threshold voltage VT and the thermal characteristics of the first NMOS transistor 217. Here, in order to offset the threshold voltage VT and the thermal characteristics of the first NMOS transistor 217, it is necessary to set a condition in which a power voltage VDD of the first NMOS transistor 217 is equal to a power voltage VDD of the second PMOS transistor 227, a gate-source voltage of the first NMOS transistor 217 is equal to a gate-source voltage of the second PMOS transistor 227, a gate width of the first NMOS transistor 217 is larger than a gate width of the second PMOS transistor 227, and a gate length of the first NMOS transistor 217 is smaller than a gate width of the second NMOS transistor 227.
As described above, according to the piezoelectric oscillator of this embodiment, since a bias voltage is applied to the gate terminal of the NMOS transistor 217 to offset a variation in the threshold voltage VT and the thermal characteristics of the first NMOS transistor 217, power consumption, a variation in the negative resistance and a change due to the thermal characteristics can be reduced. Furthermore, since noise produced by the power source of the amplifier 241 can be offset, phase noise can also be lowered.
Also, although the NPN transistor 50 is replaced with the NMOS transistor 17 of the piezoelectric oscillator in the third embodiment, as shown in the sixth embodiment, it is possible to configure so that an PNP transistor 70 is used to replace the PMOS transistor 15 of the piezoelectric oscillator in
As shown in
The effects provided by the present invention are that a satisfactory negative resistance can continue to be obtained when the invention is employed during a low-voltage operation, and that the temperature-compensated crystal oscillator of the invention can be used for the low-voltage operation of a cellular phone or a GPS.
Number | Date | Country | Kind |
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P. 2007-094573 | Mar 2007 | JP | national |