Frequency multiplier without spurious oscillation

Miscellaneous active electrical nonlinear devices – circuits – and – Signal converting – shaping – or generating – Frequency or repetition rate conversion or control

Reexamination Certificate

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Details

C327S116000, C327S123000, C333S218000

Reexamination Certificate

active

06529051

ABSTRACT:

BACKGROUND OF THE INVENTION
The present invention relates to a frequency multiplier without spurious oscillation, and particularly, to a frequency multiplier producing a microwave or a millimeter wave signal having double or quadruple the frequency of an incoming fundamental microwave signal of the order of 10 GHz or higher.
FIG. 14
is a circuit diagram showing a balanced frequency multiplier disclosed in JP No. 2807508.
This frequency multiplier includes a common source FET
10
and a common gate FET
11
, wherein the gate G, as the input, of the FET
10
and the source S, as the input, of the FET
11
are both coupled to an input transmission line
12
, and the drain D, as the output, of the FET
10
and the drain D, as the output, of the FET
11
are both connected directly to an output transmission line
13
.
A dc cutoff capacitor
14
is connected between the gate G of the FET
10
and the input transmission line
12
, and a reactance element
15
producing a phase lag is connected between the source S of the FET
11
and the input transmission line
12
.
In order to operate the FETs
10
and
11
near the pinch-off, dc bias voltages are applied to respective gates of the FETs
10
and
11
from respective constant-voltage power sources
16
and
17
through respective resistances
18
and
19
. A dc cutoff capacitor C is connected between the gate of the FET
11
and ground.
When a sine wave is provided to a microwave input terminal T
1
, the FET
10
rectifies the positive half cycles of the sine wave, while the FET
11
rectifies the negative half cycles of the sine wave and inverts the polarity thereof. Thereby, a fundamental and odd harmonics included in the drain current of the FET
10
are in opposite phase to respective those of the FET
11
, and they are mutually canceled at an output terminal T
2
. In contrast to this, since even harmonics included in the drain current of the FET
10
are in phase with those of the FET
11
, they are mutually enhanced at the output terminal T
2
. The amplitude of the fourth harmonic is considerably smaller than that of the second harmonic.
By properly determining the impedance of the reactance element
15
, it is possible to prevent shifts from being in phase and in opposite phase at the output terminal T
2
, caused by a difference in transmission characteristics between the FET
10
and the FET
11
.
According to the frequency multiplier of
FIG. 14
, since it is not required to provide a hybrid circuit for producing a pair of fundamentals in opposite phase from an incoming fundamental microwave signal, the frequency multiplier has an advantage in downsizing.
However, the present inventors found that this frequency multiplier has a below problem when it receives a microwave having a frequency of the order of 10 GHz or higher.
That is, when the input frequency exceeds the order of 10 GHz and as a result, the output frequency exceeds 20 GHz, then the common gate FET
11
comes to show unstableness such as a negative resistance at the gate G or the drain D thereof. In this case, it was not possible to prevent a spurious oscillation from occurring although an attenuator was connected near the output terminal T
2
as a countermeasure.
It has been a common practice that in design of the above described frequency multiplier, a stub is connected to the drain D of the FET
11
to supply a dc bias and furthermore, impedance matching is achieved such that the output is maximized in regard to a target multiplied frequency.
However, there arises oscillation due to a combination of the stub and the negative resistance or due to a closed loop including the FETs
10
and
11
. The spurious oscillation becomes remarkable especially in a case where a matching between the output of the frequency multiplier and an output buffer amplifier connected thereto is seriously poor (a reflection coefficient is a value close to 1).
Further, when realizing a frequency multiplier by 4 with deleting the second harmonic, an output frequency comes into a millimeter waveband, therefore it is required to employ the common gate FET
11
having a high performance (the maximum oscillating frequency fmax, or the maximum response frequency, is high) sufficient to realize the frequency multiplier by 4, resulting in that the negative resistance or a reflection gain of the common gate FET
11
becomes larger, which makes the above problem more serious.
Causes by which the negative resistance arises are a parasitic inductance of a conductor for grounding the gate G of the FET
11
and a tiny parasitic feedback capacitance between the drain D and the source S of the FET
11
. Since the common gate FET especially has its output signal in phase with its input signal, the parasitic inductance forces the common gate FET
11
to produce positive feedback (in a common source FET whose output signal is in opposite phase with its input signal, negative feedback is produced and the common source FET is usually employed in a low-noise amplifier).
In formation of a common gate FET, it is indispensable to form a kind of lead for grounding, such as a bonding wire, a via formed in a substrate, or a lead up to the grounded conductor of a co-planar line. Alternatively, there is available a method of grounding by forming a ¼ wavelength transmission line with an open end on a substrate. However, since grounding is achieved only for a given frequency component or band, the parasitic inductance arises except for the given frequency component or band.
Consequently, there have been a problem that a circuit including a common gate FET is rendered unstable with ease in a millimeter waveband or a high frequency waveband close thereto since it is hard to decrease the parasitic inductance to such a small value that no unstableness is brought about for all frequencies in operation of a common gate FET.
SUMMARY OF THE INVENTION
Accordingly, it is an object of the present invention to provide a stable frequency multiplier without spurious oscillation due to a inevitable parasitic inductance of a conductor for grounding a control input of a transistor.
In one aspect of the present invention, there is provided a frequency multiplier comprising: a first damping resistance, connected between a first end of the current path of a first transistor and an output transmission line; and a second damping resistance, connected between a first end of the current path of a second transistor and the output transmission line. Each of a second end of the first current path and a control input of the second transistor is grounded through a conductor having an inevitable parasitic inductance. The control input of the first transistor and the second end of the second current path receive microwaves of the same frequency and phase through an input transmission line.
With this configuration, when the input transmission line receives a sine microwave, the first transistor rectifies the positive half cycles of the sine microwave, while the second transistor rectifies the negative half cycles thereof and inverts their polarity. Thereby, the fundamentals and the odd harmonics on the output transmission line coming from the first and second current paths are in opposite phase and canceled by each other. In contrast to this, the even harmonics on the output transmission line coming from the first and second current paths are in phase and enhanced by each other.
Although the amplitudes of the waves passing through the first and second damping resistances are reduced, no shift in phase occurs. Hence, the even harmonics in phase are enhanced on the output transmission line.
The negative resistance is produced by the parasitic inductance of the conductor grounding the control input of the second transistor. However, the second damping resistance negates the formation of a pseudo-oscillating circuit comprising the second transistor and the output transmission line. That is, a loss on the output transmission line functioning as a resonator of the pseudo-oscillating circuit can be increased to nullify the establishment of oscill

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