Note: Descriptions are shown in the official language in which they were submitted.
Case 2086 s
i637~l
This lnvention relates to a communication system
for transmitting and receiving binary signals.
Communication systems using binary signals usually
encode the binary signals into either frequency steps
(frequency-shift keying) or phase steps (phase-shift keying).
While known ~requency-shi~t keying (FSK) systems have -the
advantage of simpler circuitry, it has been generally
considered that phase-shift keying (PSK) has the advantage of
better utilization of bandwidth and signal-to-noise ratio.
In cons~dering FSK systems, an important
parameter which is frequently referred to is the frequency
deviation ratio (symbol h). The frequency deviation ratio
is de~ined as the chan~e in frequency (from mark to space)
divided by the bit rate. Prior investigations by others
have been made for FSK systems using small values of h, and
in particular for the c~ses where h = 1 and h = 0.71. For
h = 1, it is known that part of the signalling power is
wasted by the presence of spectral lines at the two
` signalling frequencies~ Also, the case where h = 0.71
has been clai~ed to be optimum under certain conditions.
.
The case where h = 0O5 has previously been
investigated to a degree. For example, it is known that an
FSK signal having h = 0.5 has good spectral occupancy, with
no spectral lines as with h ~ 1. In general, howe~er, an
FSK system with ~ - 0.5 has previously not been considered
to be as suitable as a PSK system.
I have found, however, that use of phase-coherent
FSK haying h _ 0~5 has cextain advantages. This is
particularl~ so when this FSK system is used with the
optimal demodulator Which I have devised. This self-
synchronizing demodulator used in an FSK system having
h = 0.5 can receive faster pulse trains than can be received
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Case 2086 B
-~663~
with any other binary FSK or PSK system of equal bandwlth,
siynal-to-noise ratio and error rate.
In accordance with my invention, an apparatus is
provided for generating a phase-coherent frequency-shift
keyed signal which is keyed in response to a binary signal of
a predetermined bit rate. A clock pulse generator provides
a train of clock pulses having a repetition rate of n(n + 1)
times the bit rate, where n is an integer. A scale-of-n
counter connected to the clock pulse generator produces in
response to the clock pulses a first train of pulses having
a repetition rate of (n + 1) times the bit rate. A scale-
of-(n + 1) counter connected to the clock pulse generator
produces in response to the clock pulses a second train of
pulses having a repetition rate of n times the bit rate~
A scale-of-n(n + 1) counter connected to the clock pulse
generator produces in response to the clock pulses a train
of control pulses having a repetition rate equal to the bit ~-
rate. A logic circuit is connected to accept the binary
signal and is connected also to the scale-of-n counter, to
the scale-of-(n + 1) counter, to the scale-of-n(n + 1)
counter and to a scale-of-two counter. The logic circuit
is responsive to both the control pulses and the binary
signal for providing the first train of pulses to the scale-
of-two counter when the binary signal is in a first binary
state and providing the second train of pulses to the scale-
of-two counter when the binary signal is in a second binary
state. The scale-of-two counter is responsive to the ~irst
and second pulse trains to produce a frequency-shift keyed
square wave. A ~ilter connected to the scale-of-two
counter is responsive to the frequency-shift keyed square
wave for pa.ssing the fundamental frequency component of the
square wave and attenuating the second harmonic frequency
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Case 2086 B
~63'~ ~.
component ana the higher harmonic frequency componen-ts
of the square wave, thus producing a phase-coherent
frequency-shift keyed output signal. This output signal
has a firs-t frequency when the binary signal is in the first
binary state and a second frequency when the binary signal
is in the second binary state. Also, the difference between
the first frequency and the second frequency is equal to
exactly one-half the bit rate.
In the apparatus described, the scale-of-n counter
consists of a circulating register having n flip-flop stages,
and the scale-of-(n + 1) counter consists of a circulating
register having (n + 1) flip-flop stages. The scale-of-n
(n + 1) co~mter consists of the n-stage circulating register,
the (n + l)-stage circulating register, and a control AND
gate having a first input connected to the n-stage
circulating register and a second input connected to the
(n + l)-stage circulating register.
The logic circuit used includes a flip-flop having
` a first input connected to accept the binary signal, a
second input connected through an inverter to the first input,
and a timing input connected to accept the control pulses
from the control AND gate. A first pulse train AND gate
has a first input connected to the scale-of-n counter and a
second input connected to a first output of the flip-flop.
A second pulse train AND gate has a first input connected to
the scale-of-(n + 1) counter and a second input connected to
a second output of the flip-flop. An OR gate has a first
input connected to the first pulse train AND gate, a second
input connected to the second pulse train AND gate, and an
output connected to the scale-of-two counter. The flip-flop
is responsive to each control pulse to switch to a first
stable state or a second stable state in response to the
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Case 2086 B
~6~6~7~
binary signal being in the first binary state or the
second binary state, respectively. The flip-flop is
- adapted in the first stable state to provide at the first
output an enabling signal to enable the first pulse train AND
gate to pass the first train of pulses by way of the OP~
gate to the scale-of-two counter. Also, the flip-flop
is adapted in the second stable state to provide at the
second output an enabling signal to enable the second
pulse train AND gate to pass the second train of pulses by
way of the OR gate to the scale-of-two counter.
In the apparatus disclosed, the convention followed
is that the first binary state is a binary zero representing
a space, and the second binary state is a binary one
representing a mark. This convention is, of course,
arbitrary. The apparatus can readily be used with the
` opposite convention.
Also in accordance with my invention, a self-
synchronizing receiver is provided for demodulating a
phase-coherent frequency-shift ke!yed (FSK) signal having a
first frequency representing a first binary state of a binary
signal and a second frequency representing a second binary
state of the binary signal, where the difference between
the first and second frequencies is equal to one-half the
bit rate of the binary signal. The receiver consists of
demodulator circuit means and frequency-doubler circuit
means. The demodulator circuit means has an in-phase
channel and a ~uadrature channel, each of the channels
including integrate-dump circuit means. The frequency-doubler
circuit means is responsive to the FSK signal for generating
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reference signals, these reference signals including a
` carrier reference signal for each of the channels and a
bit~synchronous clock reference signal. The demodulator
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Case 2086 B
63~7~
circuit means is responsive to the reference signals for
demodulating the FSK signal.
The frequency-doubler circuit means includes
first and second non-linear circuit means. The first
non-linear circuit means is responsive to the FSK signal
for producing first and second phase-coherent output
signals having frequencies respectively at twice the first
frequency and twice the second frequency. The second non-
linear circuit means is responsive to the output signals
for generating the reference signals. In the embodiments
described, the second non-linear circuit means genera-tes
- the carrier reference signal for each of the channels by
generating two phase-coherent carrier reference signals.
The first non-linear circuit means consists of
a frequency doubler and first ancl second phase-locked loops.
The frequency doubler is responsive to the FSK signal for
producing an output containing a spectral line at twice the
first frequency and a spectral line at twice the second
frequency. The first phase-locked loop is connected to the
frequency doubler and is responsive to the spectral
line at twice the first frequency for producing the first
output signal. Similarly, the second phase-locked loop is
connected to the frequency doubler and is responsive to
the spectral line at twice the second frequency for
producing the second output signal.
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The second non-linear circuit means includes
a balanced modulator, a low-pass filter and a hard limiter. ;
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The balanced modulator is connected to the two phase-locked
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loops and is responsive to the two output signals for -
30 producing the clock reference signal at the difference
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frequency of the output signals. The low-pass filter is
connected to the balanced modulator for selecting the
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Case 2086 B
37~
clock reference signal at this difference frequency. The
hard limiter is connected to the low-pass filter for providing
the clock reference signal as a square wave.
A first embodiment of the receiver makes use
of the fact that the balanced modulator is further
responsive to the two output signals for producing a
high-frequency signal at the sum frequency of the output
signals. In the first embodiment, the second non-linear
circuit means further includes (in addition to the
balanced modulator, the low-pass filter and the hard
limiter) a high-pass filter and a divide-by-four freauency
divider. The high-pass filter is connected to the
balanced modulator for selecting the high-frequency
signal at this sum frequency. The divide-by-four
frequency divider is connected to the high-pass filter
for producing the two phase-coherent carrier reference
signals in the form cos 2 ~fot and sin 21rfot where t is
time and fO is a frequency mid-way between the first
frequency and the second frequency.
In a second embodiment (a preferred embodiment)
of the receiver, the second non-linear circuit means further
includes (in addition to the balanced modulator, the
low pass filter and the hard limiter) first and second
divide-by-two frequency dividers and first and second
adder circuits. The first divide-by-two frequency divider
is connected to the first phase-locked loop and is
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responsive to the first output signal for producin~ a '
first divider output at the first frequency. The
second divide-by-two frequency divider is connected to
; 30 the second phase-locked loop and is responsive to the ~;
second output signal for producing a second divider output
at the second frequency. The first adder circuit is
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~63~ Case 2086 ~
connected to the first and second divide-by-two frequency
dividers for adding the first and second divider outputs
and producing one of the phase-coherent carrier reference
signals in the form (cos 2t) (cos ~fot) where t is timP
and T is the duration of one bit and fO is a fre~uency
mid-way between the first frequency and the second frequency.
The second adder circuit is connected to the first and
second divide-by~two frequency dividers for
subtracting the first and second divider outputs and producing
the other of the phase-coherent carrier reference signals
in the form (sin ~L~ ) (sin 2~Tfot) .
; In drawings which illustrate embodiments of the invention:
Fig. 1 is a block diagram showing the circuit
` of an apparatus for generating a phase-coherent binary
FSK signal having h = 0.5;
Fig. 2 shows the waveforms of voltages which
: are present at various identified points in the circuit of
Fig. l;
Fig. 3 is a graph showing the change of phase
with time for a phase-coherent binary FSK signal; -~
Fig. 4 is a block diagram showing the circuit
of one embodiment of a receiver for demodulating a ;
phase-coherent binary FSK signal having h = 0.5;
Fig. 5 is a block diagram showing the
circuit of a preferred embodiment of a receiver for
`~ demodulating a phase coherent binary FSK signal
having h = 0~5; and -
Fig. 6 (located on the third sheet of
drawings) shows the waveforms of voltages which are
present at certain identified points in the circuits of
Figs. 4 and 5.
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Case 2086 B
~663~7~
Referring to Fig. 1, this block diagram shows
the circuit of a particular embodiment of the FSK generator
described earlier in this dislcosure. In the embodiment
of Fig. 1, the integer n equals 4. Flip-flops 11, 12, 13
and 14 are connected to form a conventional circulating
register having four stages. Similarly, flip-flops 15, 16,
17, 18 and l9 are connected as a five-stage circulating
register. Clock pulse generator 20 provides a train of
uniformly-spaced clock pulses (waveform B in Fig. 2) to drive
each of the flip-flops 11 to 19 at its timing input T.
The repetition rate of the clock pulses is twenty times the
bit rate. Thus, as shown in Fig. 2, there are twenty clock
pulses for each bit of the modulating binary signal of
waveform A. It will be noted that positive logic is used
throughout this disclosure. That is, a logic "one" is
` shown as being more positive than a logic "zero".
Initially, each of the two circulating registers
is arranged to have only one of its flip-flop stages set
(i.e. a logic "one" at its Q output). Each clock pulse
then advances the logic "one" by one stage of the register. ~
Waveforms C (Q output at flip-flop ll) and D (Q output ;~i
at flip-flop 14) for the four-stage register show trains of
uniformly-spaced pulses, one pulse being produced for every
four clock pulses. The four-stage register thus acts as ~;
a scale-of-four counter for the clock pulses. Similarly, -~
waveforms ~E (Q output at flip-flop 15) and F (Q output at
flip-flop 19) for the five-stage register show trains of
~ uniformly-spaced pulses, one pulse being produced for every
`~ five clock pulses. The five-stage register thus acts as a -
` 30 scale-of-five counter for the clock pulses.
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~6~ Case 2086 B
Waveforms C and E are applied to the two inputs
of control AND gate 21. Since pulses of waveforms C and
E are in coincidence only once every twenty clock pulses, the
output of control AND gate 21 (waveform G) provides one
pulse for every twenty clock pulses (i.e. one pulse for
each bit of waveform A).
Waveform G i5 applied to the timing input T
~ of flip-flop 22. The modulating binary signal (waveform A)
; is applied directly to the set input S of flip-flop 22, and
through inverter 23 to the reset input R of flip-flop 22.
If waveform A is a mark (binary one) the flip-flop 22 is
caused to assume its "set" state when the pulse of waveform
G occurs, producing a "one" at the Q output(waveform H) and
simultaneously a "zero" at the complementary Q output
(waveform H). If waveform A is a space ~blnary zero) the
~` flip-flop 22 is "reset" when the pulse of waveform G
occurs, producing a "zero" at the Q output (waveform H)
and a "one" at the Q output (waveform H).
Thus, for a space in waveform A, H is "one",
enabling AND gate 24 (waveform K) to pass waveform D via
OR gate 25 (waveform L) to flip-flop 26. Similarly, for a
mark in waveform A, H is "one", enabling AND gate 27
(waveform J) to pass waveform F via OR gate 25 (waveform L)
; to flip-flop 26. The waveform L applied to flip-flop 26 has
a fundamental frequency component which is an FSK signal
having h = 1. Flip-flop 26 is connected as a scale-of two
counter. Its output (waveform M) is thus at half the
frequency of its input (waveform L). The value of h is
also obviously divided by two, so that the fundamental
frequency component of waveform M is an FSK signal having
h = 0.5. The filter 28, which conveniently implemented
as a low-pass filter, serves to pass the fundamental
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Case 2086 B
3~
fre~uency c~mponent of waveform M and attenuate the harmonic
frequency components. By inspection of waveform M it can
readily be seen that the fundamental fre~uency component
is phase-coherent. That is, in switching from one
signalling frequency to the other there is no phase
discontinuity in the waveform.
As is well known, in a phase-coherent FSK
signal the phase of the signal changes linearly with time
during either a mark or a space. Fig. 3 shows the changes
in phase which occur from time t = 0, at which time it is
assumed the signal starts at centre frequency (i.e.
halfway bet~een the two signalling frequencies ). Assuming
the convention that a space is higher in fre~uency than a
mark, for each space the phase increases by~ h,
and for each mark the phase decreases byl~h, the duration i-
of one bit being shown in Fig. 3 as T. Since all phases
are modulo 21~ , when h = 0.5 it is seen from Fig. 3
that the phase can take only two possible values of
+ 1r at odd multiples of T, ancl only two possible
values of 0 and ~ at even multiples of T.
The receiver of my invention uses a phase
~` detector to establish the values of phase at each ~
`~ multiple of T. From Fig. 3 it is seen that if the phase ~-
is known at each multiple of T, then a simple logic circuit
can readily establish whether the change in phase in an
interval between multiples of T was positive or negative, -
and hence whether a space or a mark was received during the
interval.
If the signal is received in white Gaussian
noise, the optimal receiver structure is a clocked matched
filter for instance implemented by an integrate-dump circuit
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~6~37~ Case 2086 B
in base band. The integrate-dump circuit performs an
integration using the real part of the signal pre-envelope:
J(o) = S cos 2 T Re [~ (t)e ]dt
and decides ~(o) = O if J~o) is positive
or ~(o) = 1r if J(o) is negative.
That is, the integration is performed over a two-bit
interval centered on an even multiple of T (in this case
t = O). In the above formula,
T = duration of one bit
t = time
~(t) = pre-envelope of the FSX signal
fO = centre frequency = 1 2
fl = frequency for a mark
f2 ( ~ fl ) = frequency for a space.
Corresponding decisions in every second bit interval pair
give the phase for even multiples of T, yielding half the
information needed.
Similarly, the integrate-dump circuit also
performs an integration using the imaginary part of the
signal pre-envelope:
J (T) =~ sin1~2T Im [~(t) e ]dt
and decides ~ (T) = 1t if J (T) is positive
or ~ (T) = ~ 2 if J(T) is negative.
This integration is performed over a two-bit interval
centered on an odd multiple of T(in this case t = T).
Corresponding decisions in every second bit interval pair
give the phase for odd multiples of T, yielding the other
half of the information needed. Conventional logic
circuitry can thus re-construct the ori~inal modulating
binary signal from the outputs of the integrate-dump circuits.
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3~
Referring to Fig. 4, one embodiment of the receiver
circuit is shown. In this example, a receiver I.F.
amplifier 29 provides the signal to frequency doubler 30,
which provides an output which is an FSK at h = 1 thus
having spectral lines containing no modulation at
2fl and 2f2. Phase-locked loops 31 and 32 are tuned to
2fl and 2f2 respectively, providing output signals at
these frequencies. The signals at 2fl and 2f2 are
multiplied in balanced modulator 33, and the modulator
output at (2f2 - 2fl ) or T is passed by low-pass filter
34 to hard limiter 35 where it is converted to a square
wave and fed as signal V (see Fig. 6) to frequency divider 36.
Frequenc~ divider 36 has complementary outputs W and W
(see Fig. 6) applied to frequency dividers 37 and 38,
whose complementary outputs X,X amd Y,Y are used
to control gates 39, 40, 41 and 42 so that the integrate-
dump circuits 43, 44, 45 and 46 are gated on at the
correct times to integrate over the time intervals shown
at their outputs. These integrations are performed in
sequence cyclically, feeding output signals to combining
logic ~7, which, as discussed previously, reconstructs
the original modulating binary signal.
` The high frequency output from balanced
-,~ modulator 33 ~i.e. 2f2 + 2f1 - 4fO) is passed by high-pass
filter 48 to divide-by-four frequency divider 49 to
give the phase-coherent carrier reference signals of the
- form cos2~r~0t and sin2 1r fot. These reference signals
are applied to balanced modulators 50 and 51 which also
~! receive the FSK signal from I.F. amplifier 29. The
outputs of balanced modulators 50 and 51 are passed through
low-pass filters 52 and 53 to remove the harmonics,
and via the I-channel and the Q-channel to the gated
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~637~ Case 2086 B
integrate-dump circuits as previously discllssed.
Fig. 5 shows a preferred embodiment of the
receiver circuit, the difference between Fig. 4 and this
embodiment being in the means to provide the phase-coherent
carrier reference signals. As shown in Fig. 5, the outputs
of phase-locked loops 31 and 32 are fed to frequency dividers
54 and 55 respectively. The outputs of frequency dividers
54 and 55 are added in adder 56 and subtracted in adder 57
to produce carrier reference signals of the form
(cos ~ T ) (cos 2 ~fot ) for balanced modulator 50 and
(sin 2 t ) (sin 2~ fot) for balanced modulator 51. Also,
envelope demodulators 58 and 59 are included so that
logic circuitry in frequency divider 36 can decide which
of outputs W and W should go to the frequency dividers 37
and 38, thus ensuring that the integrate-dump circuits
integra~e between envelope nulls for the signal in the
corresponding channel.
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