Signal detector with matched filter coefficient

Telephonic communications – Supervisory or control line signaling – Signal receiver

Reexamination Certificate

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Details

C379S283000

Reexamination Certificate

active

06556674

ABSTRACT:

BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention relates generally to the detection of dual tone multi-frequency (DTMF) coded signals, and more particularly, to detecting DTMF coded signals with improved frequency selectivity.
2. Description of the Related Art
DTMF is the signaling standard for the Touch Tone system. Two tones are combined to define a DTMF digit. Table 1 shows the matrix of frequencies used to encode the 16 DTMF symbols on a typical 4×4 matrix telephone keypad. Each DTMF tone consists of two sine waves. One sine wave is from the low-frequency band (row frequency), and the other frequency is from the high-frequency band (column frequency).
TABLE 1
1209
1336
1477
1633
697
1
2
3
A
770
4
5
6
B
852
7
8
9
C
941
*
0
#
D
Various methods have been used for DTMF generation and detection. Previously, analog circuitry had been used to generate and decode DTMF digits. More recently, the functions have been implemented using digital signal processors (DSP) to improve the accuracy, precision, stability, reprogrammability, and cost. A popular DSP algorithm for DTMF detection is the Goertzel algorithm. One such previous method is described in U.S. Pat. No. 5,644,634, issued to Zheng-yi Xie et al., entitled “System and Method for Dual Tone Multifrequency Detection Using Variable Frame Widths,” the specification of which is hereby incorporated by reference in its entirety.
In general, a DTMF detector examines the line or communication channel for the presence of two sinusoids using dedicated frequency domain algorithms, including modified Goertzel algorithms, DFT/FFTs, auto-correlation, zero crossing counting, and narrow band filter-based methods, among others.
A common technique for determining energy values in the frequency domain is performed by transforming the time domain sampling data to frequency domain data using a variant of the discrete Fourier transform (DFT) called the Goertzel algorithm. The transfer function for the Goertzel algorithm is:
H
k
=
1
-

-
j2π

k
N
1
-
c
·
z
-
1
+
z
-
2
,
(
1
)
where c is the Goertzel coefficient,
c
=
2



cos



(
2

π



k
N
)
and N is the number of samples in a frame. The value of k is defined by:
k
=
N
F
s
·
F
tone
,
(
2
)
where F
s
is the sampling frequency (i.e., 8 kHz in typical telephone systems), F
tone
is the frequency nearest the DTMF frequency that keeps the value of k to an integer. The energy of each DTMF frequency point, k, is calculated by the feed forward and feedback phase. The feedback phase is calculated as:
Q
k
(
n
)=
c·Q
k
(
n−
1)−
Q
k
(
n−
2)+
x
(
n
),  (3)
where Q
k
(−1)=Q
k(−
2)=0, n=0, 1, 2, . . . , N−1. Q
k
(n−1) and Q
k
(n−2) are feedback storage elements for a frequency point, and x(n) is the current input sample value.
The energy in each DTMF frequency bin, k, is calculated in the feedforward phase (i.e., n=N) by the equation:
E
(
dtmf
)=|
Y
k
(
N
)|
2
=Q
k
2
(
N−
1)+
Q
k
2
(
N−
2)−
Q
k
(
N−
1)·
Q
k
(
N−
2)·c  (4)
After the energy of each DTMF frequency is calculated, the largest magnitude in each frequency band is compared to a threshold. If the energy in one of the bins exceeds the threshold, a DTMF tone may be present.
The Goertzel algorithm has difficulties meeting the required DTMF frequency distortion test. According to the industry standards, DTMF signals within a certain percentage of frequency distortion must be detected as valid DTMF tones. The DTMF signals must be rejected if the distortion exceeds certain larger percentages. FDTMF is defined as a standard DTMF frequency, and F is the actual frequency of the received signal. Based on the AT&T standard, if the F is within ±1.5% of F
DTMF
, it is a valid tone. If F is not within ±3.5% of F
DTMF
, it is not a valid tone.
Since the Goertzel algorithm finds energy aligned at the frequency of the N-point DFT, the corresponding frequency point, F
tone
, is not exactly aligned with the desired DTMF frequency, because N and k are integers. As a result, the energy is distributed among neighboring frequency bins, referred to as leakage. Leakage degrades the accuracy of the frequency domain outputs.
Suppose the calculated frequency is 2.0% larger than the desired DTMF frequency. A −2.0% error in the input signal moves the frequency to be exactly on the bin, and a +2.0% error moves the frequency further away from the bin and generates a very small output. The asymmetric effect complicates the selection of a frequency distortion threshold. Significant computational resources are required to determine if an energy value is at the left or right side of a frequency bin. Accordingly, setting different thresholds for left and right side distortion is not practical. Changing the window size, N, for the DTMF detection minimizes the asymmetric effect. However, no window size can completely eliminate the asymmetric effect.
Industry standards suggest a frame size of 205 samples, or 25.625 ms. A detector should detect a tone of at least 40 ms, but no less than 20 ms. The tone should be preceded by at least 40 ms of non-DTMF signal. To accept a DTMF tone detection, the detector should detect the tone in two consecutive frames. Considering a tone length of 40 ms, using the standard sample size of 205 causes detection difficulties.
The received tone may not be well aligned with the frame boundary, resulting in the timing diagram shown in FIG.
1
A. The timing for three consecutive frames
11
,
12
, and
13
is shown. Each frame represents 205 samples, and the length of a received signal
15
is 40 ms. The received signal
15
is misaligned with respect to the boundaries of the frames
11
,
12
,
13
. The second frame
12
is a full energy frame, but the first and third frames
11
,
13
are only artial energy frames. Depending on the degree of misalignment, the DTMF detector could fail to detect the tone in both of the partial energy frames
11
,
13
, and the two consecutive frame hit requirement would not be met. Accordingly, the tone would be missed.
Previous methods to accommodate for frame misalignment have employed special processing techniques to align the received signal
15
with the frame boundary, as shown in FIG.
1
B. Even with frame alignment, the third frame
13
is still a partial energy frame. As a result, the energy response shape for the third frame
13
will differ from that of the second frame
12
.
FIG. 1C
illustrates a full frame frequency response
16
and a partial frame frequency response
17
. The energy variation between the full and partial energy responses
16
,
17
may result in the evaluation results not being consistent across the frames
12
,
13
, thus reducing the detection accuracy. The frame alignment method helps to improve the accuracy of the detector, but results in a more complicated and costly implementation.
The present invention is directed to overcoming, or at least reducing the effects of, one or more of the problems set forth above.
SUMMARY OF THE INVENTION
In one aspect of the present invention, an signal detector is provided for detecting at least a first signal having a first frequency. The signal detector includes a matched transform unit and an energy level threshold unit. The matched transform unit is adapted to receive at least a first frame of time domain input samples at a sampling frequency and generate at least a first frequency energy value for the first frame based on at least a first subset of the time domain input samples and a first matched filter coefficient. The sampling frequency is a non-integral multiple of the first frequency, and the first matched filter coefficient depends on the first frequency. The energy level threshold unit is adapted to compare the first frequency energy value to a threshold energy value to determine the presence of the first signal.
In another aspect of the prese

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