Single side-band mixer

Pulse or digital communications – Transmitters – Amplitude modulation

Reexamination Certificate

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Details

C375S270000, C332S170000, C445S047000, C445S060000

Reexamination Certificate

active

06496545

ABSTRACT:

BACKGROUND OF THE INVENTION
This invention relates to mixer circuits and, in particular, to single-sideband mixers which may be used to produce single or dual frequencies with high sideband rejection.
It is known to use “mixers” to mix two input signals, where one input signal has a frequency &ohgr;
1
(i.e., 2&pgr; f
1
) and the other input signal has a frequency &ohgr;
2
(i.e., 2&pgr; f
2
), to produce a first output signal having a lower frequency (i.e., the lower sideband) equal to the difference (i.e., &ohgr;
1
−&ohgr;
2
) of the two input signal frequencies and/or a second output signal having an upper frequency (i.e., the upper sideband) equal to the sum (i.e., &ohgr;
1
+&ohgr;
2
) of the two input signal frequencies. A single-sideband (SSB) mixer system is highly suited for generating dual-band (i.e., upper and/or lower sidebands) carrier signals for frequency translations with electronic band selection capability since it can provide either an upper or a lower sideband output by means of an electronic control.
However, it is essential for the single sideband (SSB) mixer system to have high sideband rejection in both frequency bands. That is, when the lower sideband is selected to be produced at the output of the SSB mixer system, there must be a high degree of rejection of the upper sideband and, vice versa, when the upper sideband is selected to be produced at the output of the SSB mixer system, there must be a high degree of rejection of the lower sideband.
A problem in accomplishing this result is illustrated by referring to
FIG. 1
which shows a block diagram of a prior art single-frequency SSB mixer system
10
. The mixer system
10
includes a first 90-degree phase shifter,
12
, a second 90-degree phase shifter,
14
, a first mixer,
16
, a second mixer,
18
, and an output combiner/summer,
20
. Each one of 90-degree phase shifters
12
and
14
, has two outputs. Phase shifter
12
has two “quadrature” outputs V
11
and V
12
, where V
11
is equal to A
1
cos &ohgr;
1
t and V
12
is equal to B
1
sin(&ohgr;
1
t+&thgr;
1
); and phase shifter
14
has two “quadrature” outputs V
21
and V
22
, where V
21
is equal to A
2
cos &ohgr;
2
t and V
22
is equal to B
2
sin(&ohgr;
2
t+&thgr;
2
).
Ideally, the two outputs of each phase shifter should have the same amplitude (i.e., A
1
=B
1
and A
2
=B
2
) and the two outputs should be at 90 degrees (orthogonal or in quadrature) with respect to each other (i.e., &thgr;
1
=&thgr;
2
=0). However, in practice, the amplitude of the two outputs of each phase shifter may not be equal to each other (i.e., there is an amplitude imbalance) and there is a phase error, denoted by the phase angle &thgr;, which is equal to the angle by which the difference between the two supposedly orthogonal outputs of a phase shifter is greater, or less, than 90 degrees. Accordingly, in the discussion to follow and in the appended claims, when reference is made to a 90° phase shifter, without further qualification, what is meant is a phase shifter which is intended to produce two equal amplitude signals which are at 90° to each other. However, in practice, due to various circuit limitations, the amplitude of the two output signals may not be equal (unless otherwise specified) and the phase angle between the two supposedly orthogonal output signals of a “90° phase shifter” may be greater, or less, than 90°.
In the ideal case, the single frequency SSB mixer of
FIG. 1
generates an output (V
OUT
) at the output of the combiner
20
, whose frequency is solely equal to the upper sideband components (&ohgr;
1
+&ohgr;
2
). [If the outputs of the first phase shifter
12
were switched so that V
11
were applied to mixer
18
and V
12
to mixer
16
, then the output V
OUT
would have a frequency which, ideally, would solely equal to the lower sideband components (1−&ohgr;
2
).] In practice, however, both sidebands are present at the output of the combiner
20
due to non-quadrature phase (non-zero &thgr;
1
and &thgr;
2
) or amplitude imbalance (between A
1
and B
1
, and between A
2
and B
2
) introduced by phase shifters,
12
and
14
.
It is known to form the phase shifters using conventional high-pass low-pass RC-CR networks of the type shown in FIG.
2
A. The
FIG. 2A
networks yield two single-ended quadrature signals V
1
and V
2
These signals generally have the proper phasal relationship (i.e., 90° ) but, the amplitudes of V
1
and V
2
are balanced only when &ohgr;RC=1. Supplying “quadrature” signals to the mixers which have the correct phasal relationship (i.e., 90° ) but which have unequal amplitude is problematic because the mixers introduce amplitude nonlinearity which makes the amplitude compensation difficult. The amplitude imbalance can be reduced by using a limiting stage to equalize the amplitude of the quadrature signals. However, these attempts normally result in excessive nonlinear limiting which, while equalizing the amplitude of the signals, causes significant phase error and the deterioration of the overall mixer system performance.
Thus, production of upper and lower sidebands with high sideband rejection is not readily achieved with single sideband mixer systems formed with high-pass low-pass 90° phase shifters.
SUMMARY OF THE INVENTION
Applicant's invention resides, in part, in the recognition that a single sideband mixer including two supposedly 90° phase shifters may be used to produce upper and/or lower sidebands with a high degree of sideband rejection even when the phase shifters have a phase angle error (&thgr;), so long as the phase angle error of the two phase shifters are substantially equal and the amplitude of the two orthogonal outputs of each phase shifter have substantially equal amplitudes.
Thus, in contrast to the prior art, a single sideband mixer system embodying the invention includes the application of first and second input frequencies (&ohgr;
1
, &ohgr;
2
) to first and second 90° all-pass phase shifters to produce first and second supposedly orthogonal outputs per phase shifter. The outputs of the two phase shifters are then applied to inputs of first and second mixer circuits whose outputs are then combined to produce either the upper (the sum of &ohgr;
1
and &ohgr;
2
) or the lower (the difference between &ohgr;
1
and &ohgr;
2
) sidebands of the two input frequencies. The all-pass type phase shifters are used to ensure that there is little, if any, amplitude imbalance in the 90° degree phase shifter outputs.
The first and second 90° phase shifters embodying the invention are preferably formed such that any phase error (i.e., &thgr;
1
) in the first phase shifter is essentially equal to any phase error (i.e., &thgr;
2
) in the second phase shifter and that the phase errors &thgr;
1
and &thgr;
2
track each other. Accordingly, in systems embodying the invention, the first and second phase shifters are preferably formed within an integrated circuit and in close proximity to each other so that they track each other over time and varying ambient and voltage conditions. The outputs of the first and second phase shifters are supplied to mixer circuits whose outputs are combined. If the phase error of the two phase shifters track, the phase errors are significantly reduced when the mixer outputs are combined to produce an output signal V
OUT
.
According to one aspect of the invention, the first and second supposedly orthogonal outputs of the first 90° phase shifter are respectively coupled via selectively enabled switching means to the inputs of the first and second mixers and the first and second supposedly orthogonal outputs of the second 90° phase shifter are respectively fixedly coupled to the inputs of the first and second mixers. The outputs of the first and second mixers are then combined to produce either the upper sidebands or the lower sidebands of the first and second frequency input signals applied to the first and second 90° phase shifters. For one condition of the selectively enabled switching means (e.g., the “thru

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