Synchronization of ofdm signals with improved windowing

BACKGROUND OF THE INVENTION

The present invention relates generally to broadband transmission of information and, more particularly, to time synchronization of a received OFDM signal.

Orthogonal Frequency Division Multiplexing (OFDM) is a spread spectrum technology wherein the available bandwidth is subdivided into a number of discrete channels or subcarriers that are overlapping and orthogonal to each other. Each channel has a well defined frequency. Data are transmitted in the form of symbols that encompass some number of subcarrier frequencies. The amplitude and/or phase of the subcarriers represents the encoded information. Before a received OFDM symbol can be decoded, frequency and time synchronization of the signal have to be determined. This process is referred to as synchronization.

Time synchronization may be achieved through the use of time-based correlation in the time domain or phase correlation in the frequency domain. Phase correlation has several advantages over time-based correlation. Phase correlation is more robust as it is significantly less affected by amplitude variations than time-based correlation. Also, symbols can be synchronized in the presence of a much stronger jammer by correlation in the frequency domain.

OFDM symbols can be synchronized in the frequency domain by correlating the phases of the carriers with the phases of a reference symbol. Alternatively, or in addition, autocorrelation can be performed by correlating the phases of a received symbol with those of an earlier received symbol.

Time synchronization of the received OFDM signals is more difficult to achieve, in particular, in the presence of narrow band interference in the OFDM channel. Apodizing window functions, such as Hanning windows, are typically used to deal with the effects of a narrowband interferer, such as a jammer signal, in samples that are passed to a phase correlator. While the apodizing window confines interference from the narrowband interferer to only several of the OFDM subcarriers, it introduces intercarrier interference into the subcarrier frequencies. The intercarrier interference can result in destructive canceling (i.e., frequency nulls") in transmitting subcarriers of equal amplitude and phase. In the presence of a frequency null, a phase correlator may miss a peak correlation pulse and thus provide unreliable synchronization. The intercarrier interference can also cause phase and amplitude distortion in each of the transmitted subcarriers processed by the apodizing window. Phase distortion in sample phases, as well as in the autocorrelation or reference phases with which they are compared, can result in poor phase correlation. Even using a best possible set of reference phases (typically, nonwindowed referenced phases), in conjunction with Hanning windowed phases reduces correlation by some factor. That is, it takes a much stronger signal to perform correlation than would be needed if a Hanning window was not used.

US 5357502 discloses a device for the reception of Coded OFDM (COFDM) digital data broadcast at a high bit rate for reception by mobile receivers. A digital signal is distributed in the frequency-time space and transmitted in the form of symbols each constituted by a multiplex of orthogonal carrier frequencies modulated by a set of digital elements and broadcast simultaneously. A receiving device includes a module for transposition by a local oscillator, baseband filtering and analog-digital conversion, a Nyquist type of temporal windowing module with a non-zero roll-off for the collection of useful samples and a mathematical transformation module. Use of a Nyquist temporal window results in smaller secondary lobes.

EP 0814587 discloses a method of increasing the maximum available bit rate on a single data link, in order to gain capacity within single cells. The method uses the fact that pulse shaping, for example by using an appropriate window function such as a Harming window, introduces inter-symbol interference and utilises the idea of overcoming this interference by equalization. An equaliser located in the receiver compensates for loss of carrier orthogonality induced by pulse shaping.

SUMMARY OF THE INVENTION

The present invention provides a method according to claim 1 and a phase correlation unit according to claim 9.

In one aspect of the invention, a method of determining phases of a symbol for phase correlation includes performing symmetric apodizing windowing function on a symbol sample having a symbol period of T and a time-offset symbol sample time-offset from the symbol sample by T/2 to produce first windowed values for the symbol sample and second windowed values for the time-offset symbol sample. The method further includes applying a time shift to re-align the time-offset symbol sample with the symbol sample and therefore align the second windowed values with corresponding first windowed values. The first and second windowed values are then summed together and the summing values are converted to phases. The symmetric apodizing window function is an apodizing window function W having the property W_j + W_{(FFTSize/2+j)}=constant, where FFTSize is the size of the FFT sample.

Embodiments of the invention may include one or more of the following features.

The symmetric apodizing window function may be performed in the time domain.

The symmetric apodizing window function may be performed in the frequency domain and may be applied to FFT frequency coefficients of the symbol sample and the time-offset symbol sample.

The symmetric apodizing window function may be a Hanning window.

The windowing scheme of the invention offers several advantages. It eliminates the effects of a "symmetric" apodizing window (e.g., Hanning window) on adjacent carriers, that is, the intercarrier interference. In addition, it provides the benefits of the Hanning window, such as improved jammer performance, without introducing phase and amplitude distortion into each of the carrier frequencies of a windowed signal. Such phase distortion can lead to poor phase correlation during synchronization.

BRIEF DESCRIPTION OF THE DRAWINGS

<ul id="ul0001" list-style="none" compact="compact"><li>FIG. 1 is a temporal OFDM symbol;</li><li>FIG. 2 illustrates symbolically a frequency distribution of OFDM channels;</li><li>FIG. 3 is a schematic diagram of a phase correlator module including an OFDM symbol processing unit;</li><li>FIG. 4 is a block diagram of the OFDM symbol processing unit;</li><li>FIG. 5 is a depiction of a Hanning window applied to a symbol sample and the symbol sample with time-offset in the frequency domain;</li><li>FIG. 6 is a depiction of autocorrelation between samples processed by the OFDM symbol processing unit of FIG. 4;</li><li>FIG. 7 is a flow diagram of a frequency domain based windowing process performed by the OFDM symbol processing unit of FIG. 4;</li><li>FIG. 8 is an alternative embodiment of the OFDM symbol processing unit of FIG. 3;</li><li>FIGS. 9A-C are depictions of a Hanning window applied to a symbol sample and the symbol sample with time-offset in the time domain;</li><li>FIG. 10 is a time domain based windowing process performed by the OFDM symbol processing unit of FIG. 8;</li><li>FIG. 11 is a depiction of a jammer signal superimposed on a temporal waveform including three consecutive symbols;</li><li>FIGS. 12A-C are illustrations of the phases and amplitudes of the waveform (of FIG. 11) demodulated without windowing;</li><li>FIGS. 13A-C are illustrations of the phases and amplitudes of the waveform (of FIG. 11) demodulated after applying a Hanning window in the time domain;</li><li>FIG. 14A is an illustration of the time domain based windowing process (of FIG. 10) as applied to the waveform (of FIG. 11) and FIGS. 14B-D are illustrations of the phases and amplitudes of the waveform demodulated after using the time-domain based windowing process of FIG. 14A; and</li><li>FIG. 15A is an illustration of the frequency domain based windowing process (of FIG. 7) as applied to the waveform of FIG. 11. FIGS. 15B-D are illustrations of the phases and amplitudes of the waveform demodulated after using the frequency domain based windowing process of FIG. 15A.</li></ul>

DETAILED DESCRIPTION

In OFDM transmission, data are transmitted in the form of symbols. Each symbol has a predetermined time duration or symbol time T_s. Each symbol is comprised of N sinusoidal waveforms that are orthogonal to each other and form the OFDM channels and subcarriers. Each subcarrier has a frequency f_i and a Φ_i measured from the beginning of the symbol. Orthogonality of the subcarriers requires that a whole number of periods of each waveform are contained within the symbol time T_s. The phases Φ_i and amplitudes A_i of the waveforms can be set arbitrarily without affecting the orthogonality of the waveforms. The OFDM subcarriers occupy a frequency range between frequencies f₁ and f_N referred to as OFDM bandwidth. Each subcarrier frequency fi has a uniform frequency Δf from the adjacent subcarrier frequency f_i±1. The Δf is inversely proportional to the symbol time Ts.

Referring to FIGS. 1 and 2, an exemplary OFDM symbol 10 has a symbol time Ts of 6.4 us, which produces a channel spacing Δf =1/6.4us=156.25 kHz. The symbol includes 84 subcarrier frequencies that are uniformly spaced between a first subcarrier frequency f₁ = 3.594 MHz and a last subcarrier frequency of f_N = 16.563 MHz, corresponding to a system bandwidth of 13.125 MHz. In the example of FIG. 1, the phases of the 84 carriers are selected to be random and independent of each other. However, any other sets of phases may be selected. For the purpose of digital signal processing, the symbol is sampled during the symbol time T_s at 256 sample points at a clock rate of 40 MHz. As mentioned above, the unmodulated amplitudes A_i of each of the 84 OFDM channels are identical.

Referring now to FIG. 3, a phase correlator module 150 is shown. A temporal waveform S_in is received by the phase correlator module 20 and is processed by an OFDM symbol processing unit (the unit) 22, which transforms the temporal waveform into the frequency domain. A first converter 26 converts the output of the unit 22 to respective amplitude values A_i and phase values Φ_i at each of the OFDM subcarrier frequencies f_i. A phase correlator 30 is coupled to the first converter 26 and compares the phases Φ_i to known reference phases Φ_i^ref that may be stored in a reference phase memory 28, or to phases Φ_i of a processed symbol that was received earlier. The phases Φ_i of the earlier received, processed symbol may be stored in an autocorrelation phase memory 32 that may be identical to the reference phase memory 28. The phase correlator 30 then either compares the phases to produce an autocorrelation value indicating a repeating symbol pattern or aligns the phases with the reference phases. A second converter 34 computes from the aligned phases a corresponding time shift Δt_s, which represents the temporal shift between the received symbols and the reference, and is used for synchronization. The details of the phase correlator have been omitted for sake of clarity. Details of an exemplary phase correlator may be had with reference to copending U.S. application US 6,111,919.

Referring to FIG. 4, the unit 22 (from FIG. 3) is shown. The unit 22 includes a time delay or offset element 82, a "dual" FFT engine 84, a window filter 86, a time shift element 88 and a summation unit (or "adder") 90. The output of the adder 90 is connected to the first converter 26 (of FIG. 3), shown in dashed lines. The window filter 86 includes a first Hanning window function 92 and a second Hanning function 94, as will be described later. The dual FFT module receives a sample of the original signal r(t) and a time-offset sample r(t-t_o) offset by t_o = T/2. The dual FFT engine transforms the time-offset sample into first (time-offset&gt; frequency coefficients R(ω)*e^-jωto and transforms the original sample, that is, the non-offset sample, into second frequency coefficients R(ω). The frequency coefficients are processed by the window filter 86, which is selected as a "symmetric" apodizing window function. The symmetric apodizing window function is defined herein as an apodizing window function W having the property W_j + W_{(FFTSize/2+j)}=constant, where FFTSize is the size of the FFT sample. In the illustrated embodiment, the symmetric apodizing window function (window filter 86) is the Hanning window, for which all values of j add up to one and thus has the aforementioned property. As shown in the figure, the first frequency coefficients are processed by the first Hanning window 92, and the second frequency coefficients are processed by the second Hanning window 94.

The processed first frequency coefficients are time-shifted to realign them with the corresponding processed second frequency coefficients. The time-shift re-alignment is achieved by multiplying the odd ones of the time-offset coefficients by -1, as will be described. The now realigned (processed) second frequency coefficients are added to their corresponding (processed) first frequency coefficients output by the second Hanning window and the resultant values are provided to the first converter 26 (of FIG. 3), which converts the values from rectangular to polar coordinates and transfers the phases of the polar coordinates to the phase correlator 30 (of FIG. 3), not shown. Optionally, the time shift element 88 is coupled to a memory 91, which stores copies of the windowed values shifted by the time shift element 88. These windowed values stored in the memory 91 may be retrieved and added to next windowed values output by the Hanning window function 94, and stored in the autocorrelation memory 30 (FIG. 3) for autocorrelation purposes, as later described.

Referring now to FIG. 5, a depiction of a sample and a time-offset version of the sample windowed in the frequency domain is shown. The windowed sample X (of a symbol having a symbol period T) is the convolution of the sample and the Hanning window function. Likewise, the windowed time-offset sample Y (offset by T/2) is the convolution of the time-offset sample and the Hanning window function. As shown in the figure, the time-offset sample includes a T/2 cyclic extension of X that is identical to the first half of X since synchronization symbols are repeating OFDM symbols.

The time shift relationship of r(t) in the time domain and R(ω) in the frequency domain can be expressed as follows:<maths id="math0001" num=""><math display="block"><mrow><msub><mrow><mtext>r(t-t</mtext></mrow><mrow><mtext>o</mtext></mrow></msub><msup><mrow><mtext>) =&gt; e</mtext></mrow><mrow><mtext>-jωto</mtext></mrow></msup><mtext>R(ω)</mtext></mrow></math><img file="EP1183774B1_D0001.tif" /></maths>    where f=c*(1/T), ω=c*(2π/T) and t_o=T/2, then<maths id="math0002" num=""><math display="block"><mrow><msup><mrow><mtext>r(t-T/2) =&gt; e</mtext></mrow><mrow><mtext>-jc(2π/T)T/2</mtext></mrow></msup><mtext>R(ω)</mtext><mspace linebreak="newline" /><msup><mrow><mtext> =&gt; e</mtext></mrow><mrow><mtext>-jcπ</mtext></mrow></msup><mtext>R(ω)</mtext><mspace linebreak="newline" /><msup><mrow><mtext> for even c, e</mtext></mrow><mrow><mtext>-jcπ</mtext></mrow></msup><mtext> = 1</mtext><mspace linebreak="newline" /><msup><mrow><mtext> for odd c, e</mtext></mrow><mrow><mtext>-jcπ</mtext></mrow></msup><mtext> = -1</mtext></mrow></math><img file="EP1183774B1_D0002.tif" /></maths>

It will be appreciated that the noise applied to Q(ω) (shown in FIG. 4) and R(ω) is different. However, it can be assumed that Q(ω) and e^-jωtoR(ω) are approximately equal since Q(ω) is essentially a time-offset sample of R(ω).

Referring back to FIG. 4, the even ones of the time-offset frequency coefficients, referred to now as "A_c", are multiplied by +1 and the odd ones of the time-offset coefficients A_c are multiplied by -1. For subcarrier frequencies A₂₃ through A₂₆, for example, the coefficients are represented as the following: <tables id="tabl0001" num="0001"><table frame="all"><tgroup cols="2" colsep="1" rowsep="0"><colspec colnum="1" colname="col1" colwidth="78.75mm" /><colspec colnum="2" colname="col2" colwidth="78.75mm" /><thead valign="top"><row rowsep="1"><entry namest="col1" nameend="col1" align="center">non-offset</entry><entry namest="col2" nameend="col2" align="center">time-offset</entry></row></thead><tbody valign="top"><row><entry namest="col1" nameend="col1" align="center">A₂₃</entry><entry namest="col2" nameend="col2" align="right">-A₂₃</entry></row><row><entry namest="col1" nameend="col1" align="center">A₂₄</entry><entry namest="col2" nameend="col2" align="right">A₂₄</entry></row><row><entry namest="col1" nameend="col1" align="center">A₂₅</entry><entry namest="col2" nameend="col2" align="right">-A₂₅</entry></row><row rowsep="1"><entry namest="col1" nameend="col1" align="center">A₂₆</entry><entry namest="col2" nameend="col2" align="right">A₂₆</entry></row></tbody></tgroup></table></tables> It may be recalled that the windowed frequency for a Hanning window is obtained by subtracting for each subcarrier one half the sum of the coefficients at the two adjacent carriers, i. e. , A_c-1/2 (A_c-1+A_c+1). Thus, for the carrier sample c=24, the Hanning window provides A₂₄-1/2 (A₂₃+A₂₅) for the non-offset coefficient and A₂₄+1/2 (A₂₃+A₂₅) for the time-offset coefficient.

For an odd carrier c=25, the Hanning window provides for the non-offset coefficient the Hanning value A₂₅-1/2 (A₂₄+A₂₆) and for the time-offset coefficient the Hanning value -A₂₅-1/2 (A₂₄+A₂₆). To realign the offset sample points back with the original sample, the odd carriers C are multiplied by -1. Thus, in this example, the time-offset frequency coefficient becomes A₂₅+1/2 (A₂₄+A₂₆) and the resulting Hanning values for each of the sample points are added. The sum is 2A₂₄ for c=24 and 2A₂₅ for c=25. Thus, it can be seen that the components of the adjacent signals typically found in each carrier signal after a Hanning window function are removed.

The single-unit dual FFT engine shown in FIG. 4 may be implemented using a dual FFT engine which was designed to complex signals. Rather than setting the imaginary parts of the complex entries to zero, a use which results in redundancy and does not utilize the full bandwidth of the engine, the complex FFT engine can be fully utilized by applying real numbers at both the real and imaginery inputs. This makes use of the fact that the real part of the frequency spectrum of a real signal is an even function and the imaginery part of the frequency spectrum of a real signal is an odd function. The practice of performing dual-real transforms with complex FFTs is well-known and, therefore, will not be described in further detail. Of course, it will be recognized that the dual FFT engine 84 can also be implemented as two separate FFT engines.

Referring now to FIG. 6, a plurality of samples A1, A2 and A3 and their corresponding time-offset samples B1, B2 and B3 are shown. Assuming each sample is 256 points, each time-offset sample is forward-shifted by 128 points. If A3 is the current sample being processed by the unit 22 (of FIG. 4) and the output of the unit 22 is sample C33, the output C33 is sent to the phase correlator 30 for comparison with reference phases as described above. Alternatively, C33 is "autocorrelated" with an earlier sample C22. Because there is a signal portion common to C33 and C22, the resulting autocorrelation value may be slightly biased towards correlation. Thus, to eliminate such bias (however slight), an alternative autocorrelation may be achieved by comparing C33 to C21. This is accomplished by storing each time-offset windowed sample output by the time shift element 88 (of FIG. 4) and subsequently combining that stored sample with a next non-offset windowed sample, that is, the non-offset windowed sample for the next symbol that is processed. The resulting sum is stored in the autocorrelation memory 30. When the following symbol is processed, the stored sum is used for autocorrelation. Thus, with reference to the example shown in FIG. 6, when C22 is output by the unit 22 (of FIG. 4), C21 is computed by retrieving B1 from the memory 91 (of FIG. 4). When C33 is subsequently output by the unit 22, it is correlated with C21 to produce an autocorrelation value.

Referring to FIG. 7, a frequency domain windowing process (160) performed by the receiver 80 of FIG. 12 is shown. The process performs (102) a first FFT on a first sample of a temporal symbol waveform sampled at a number (s) of sample points, e.g., s=256 sample points, during the symbol time T_s. The process performs (104) a second FFT on a second sample that is time-offset from the first sample by a time = T/2. The process applies (106) the first Hanning window to the second (time-offset) sample and applies (108) the second Hanning window to the first sample in the frequency domain. The processed second sample is time-shifted 110 (i.e., the odd ones are multiplied by -1) to realign the second sample points with corresponding ones of the first sample points. The process then (112) adds the processed second sample points to the processed first sample points of the OFDM symbol.

In an alternative embodiment of the OFDM symbol processing unit 22 (of FIG. 3), the Hanning window filter is placed before the FFT engine. Referring to FIG. 8, an OFDM processing unit 118 includes a Hanning window filter 120. The Hanning window filter includes a first Hanning window function 122 for receiving a waveform S(t) and a second Hanning window function 124 for receiving a time-offset waveform S(t-T/2) offset by T/2 by time delay element 119. The unit further includes a time shift element 125 for time-shifting (e.g., rotating) the windowed time-shifted waveform or sample into re-alignment with the windowed, non-offset waveform. Also included is an adder 126 coupled to one output of the Hanning window filter 120 and the time shift element 125, as well as the input of an FFT engine 128. The output of the FFT engine is received by the first converter 26 (from FIG. 3), which converts the output to phases and transfers the phases to the phase correlator 30 (FIG. 3), not shown.

It will be recognized that, like the frequency domain based approach described with reference to FIGS 4-7, autocorrelation can be performed in much the same way as was described with reference to FIG. 6 so that any minimal effects of the common sample portion (as would be seen in any two consecutive outputs of the OFDM symbol processing unit 118) on the correlation are eliminated. However, as the time domain based approach normally uses a single FFT, the alternative autocorrelation would require the addition of a second FFT engine or a dual FFT engine (as is used in the illustrated frequency domain windowing process). Because the time domain based approach is already more computation intensive, the added complexity of the second FFT makes the frequency domain based approach a more practical solution if the alternative autocorrelation is to be used.

Referring now to FIGS. 9A-C, an example of the time-domain windowing process performed by the receiver 118 of FIG. 15 is shown. FIG. 9A illustrates a Hanning window H 130 containing 256 points: H₀, H₁, H₂, H₃, ..., H₂₅₅. The Hanning window 130 has the property H_j= 1 - H_128+j. FIG. 9B depicts an OFDM symbol 132 of a sample size (number of sample points) s = 256: A₀ to A₂₅₅. The OFDM symbol has a cyclic extension (prefix) 134 P_j = A_j, j = 128 to 255, in the originally transmitted signal. That is, prefix P is identical to the second half of A. The cyclic prefix P, together with the first half of the symbol A, thus represent a time-offset version of sample A. The time-offset sample is offset by T/2 (128 points, in this example). FIG. 9C shows a first Hanning window applied to sample A, that is, (A_0-A₂₅₅) * (H₀-H₂₅₅), to give Hanning values X₀-X₂₅₅, collectively, windowed sample X 136. Further illustrated is a second Hanning window applied to the points (P₁₂₈-A₁₂₇) * (H₀-H₂₅₅) to give Hanning values (Y₀ - Y₂₅₅), collectively, windowed sample Y 138. Therefore, with reference to FIG. 9C, X_j = A_j*H_j, and for j= 0 to 127, Y_j = P_j+128*H_j and Y_j+128 = A_j*H_j+128.

Referring again to FIG. 9C, to time align the two windowed samples X_j and Y_j, Y_j+128, sample P is moved by 256 points (as indicated by the arrow). Thus, after the shift, Y₀-Y₂₅₅ is Y₁₂₈, Y₁₂₉, ...Y₂₅₅, Y₀, Y₁, ... Y₁₂₆, Y₁₂₇, collectively, Y 140. Combining the two samples X 136 and Y 140 gives X₀+Y₁₂₈, X₁+Y₁₂₉ ... X₁₂₇+Y₂₅₅, X₁₂₈+Y₀, X₁₂₉+Y₁...X₂₅₄+Y₁₂₆, X₂₅₅+Y₁₂₇.

More specifically, for the first 128 points of the combined windowed samples (j=0 to 127):<maths id="math0003" num=""><math display="block"><mrow><msub><mrow><mtext>X</mtext></mrow><mrow><mtext>j</mtext></mrow></msub><msub><mrow><mtext>+Y</mtext></mrow><mrow><mtext>j+128</mtext></mrow></msub><msub><mrow><mtext> = A</mtext></mrow><mrow><mtext>j</mtext></mrow></msub><msub><mrow><mtext>*H</mtext></mrow><mrow><mtext>j</mtext></mrow></msub><msub><mrow><mtext> + A</mtext></mrow><mrow><mtext>j</mtext></mrow></msub><msub><mrow><mtext>*H</mtext></mrow><mrow><mtext>j+128</mtext></mrow></msub><mspace linebreak="newline" /><msub><mrow><mtext> = A</mtext></mrow><mrow><mtext>j</mtext></mrow></msub><msub><mrow><mtext>* [Hj + H</mtext></mrow><mrow><mtext>j+128</mtext></mrow></msub><mtext>]</mtext><mspace linebreak="newline" /><msub><mrow><mtext> = A</mtext></mrow><mrow><mtext>j</mtext></mrow></msub><msub><mrow><mtext>* [H</mtext></mrow><mrow><mtext>j</mtext></mrow></msub><msub><mrow><mtext> + 1-H</mtext></mrow><mrow><mtext>j</mtext></mrow></msub><mtext>]</mtext><mspace linebreak="newline" /><msub><mrow><mtext> = A</mtext></mrow><mrow><mtext>j</mtext></mrow></msub></mrow></math><img file="EP1183774B1_D0003.tif" /></maths>

For the second 128 points of the combined windowed samples X and Y (where j=0 to 127):<maths id="math0004" num=""><math display="block"><mrow><msub><mrow><mtext>X</mtext></mrow><mrow><mtext>j+128</mtext></mrow></msub><msub><mrow><mtext>+Y</mtext></mrow><mrow><mtext>j</mtext></mrow></msub><msub><mrow><mtext> = A</mtext></mrow><mrow><mtext>j+128</mtext></mrow></msub><msub><mrow><mtext>*H</mtext></mrow><mrow><mtext>j+128</mtext></mrow></msub><msub><mrow><mtext> + P</mtext></mrow><mrow><mtext>j+128</mtext></mrow></msub><msub><mrow><mtext>*H</mtext></mrow><mrow><mtext>j</mtext></mrow></msub><mspace linebreak="newline" /><msub><mrow><mtext> = A</mtext></mrow><mrow><mtext>j+128</mtext></mrow></msub><msub><mrow><mtext>*H</mtext></mrow><mrow><mtext>j+128</mtext></mrow></msub><msub><mrow><mtext> + P</mtext></mrow><mrow><mtext>j+128</mtext></mrow></msub><msub><mrow><mtext>* [1-H</mtext></mrow><mrow><mtext>j+128</mtext></mrow></msub><mtext>]</mtext><mspace linebreak="newline" /><msub><mrow><mtext> ~ A</mtext></mrow><mrow><mtext>j+128</mtext></mrow></msub><msub><mrow><mtext>*H</mtext></mrow><mrow><mtext>j+128</mtext></mrow></msub><msub><mrow><mtext> + A</mtext></mrow><mrow><mtext>j+128</mtext></mrow></msub><mtext>* [1-</mtext><mspace linebreak="newline" /><msub><mrow><mtext> H</mtext></mrow><mrow><mtext>j+128</mtext></mrow></msub><mtext>]</mtext><mspace linebreak="newline" /><msub><mrow><mtext> ~ A</mtext></mrow><mrow><mtext>j+128</mtext></mrow></msub><msub><mrow><mtext>* [H</mtext></mrow><mrow><mtext>j+128</mtext></mrow></msub><msub><mrow><mtext> + 1-H</mtext></mrow><mrow><mtext>j+128</mtext></mrow></msub><mtext>]</mtext><mspace linebreak="newline" /><msub><mrow><mtext> ~ A</mtext></mrow><mrow><mtext>j+128</mtext></mrow></msub></mrow></math><img file="EP1183774B1_D0004.tif" /></maths> It should be noted that, because A and P are different signals and therefore noise and channel distortion are applied to each differently, there is actually a small but negligible difference between the two. Thus, A_j+128 is approximately equal to P_j+128 in the substitution above.

It will be recognized that, although a full Hanning window can be applied to both the original and the time-offset samples (as described above), the summing of the resultant Hanning values in samples X 136 and Y 140 for the 128 points of A which are common to both samples yields no more than the original sample Aj. Therefore, the same results could be achieved by applying a first half Hanning window (H₀ to H₁₂₇) to P and a second half Hanning window (H₁₂₈ to H₂₅₅) to the second half of A. The half Hanning window approach is less computationally intensive than the full Hanning window approach and is therefore a more desirable implementation.

Referring to FIG. 10, a time-domain based windowing process (140) performed by the OFDM symbol processing unit 118 shown in FIG. 8 (and depicted in the example of FIGS. 9B-C) is shown. The process applies (152) a first half of a Hanning window to the first half (e.g., points 0 to 127 in a 256 point sample) of a T/2 time-offset sample and applies (154) a second half of a Hanning window to the second half (e.g., points 128 to 256 in a 256 point sample) of a first, non-offset sample. The windowed values in the first sample are added (156) to corresponding windowed values in the second sample (i.e., values separated by T are added together). The summed values, along with the points in the first half of the first sample, are then Fourier-transformed (158) by a single FFT engine.

Thus, the Hanning window effectively limits the effect of a non-orthogonal narrowband interferer by tapering the endpoints of the signal smoothly to zero. Since the original signal is also distorted by the window, the realignment and combination of the signals restores the original signal without changing the benefit gain (reduction in effects of narrowband interferer) achieved by applying the window.

Collectively, FIGS. 11-15 illustrate advantages of employing the above-described time domain and frequency domain based windowing processes during phase correlation. Referring to FIG. 11, an exemplary temporal signal waveform is composed of three identical consecutive symbols. Added to the symbols is a jammer signal emitting an interfering signal at a single frequency f_i=55 MHz. In this example, the jammer-to-signal amplitude ratio is 20 dB. As seen in the figure, the jammer is the predominant signal.

The waveform of FIG. 11 is transformed and demodulated into amplitudes and phases of its 84 carriers. Referring to FIGS. 12A-C, it can be seen that the effects of the jammer are spread across the carrier frequencies for carriers 23-106, but there is not distortion to the amplitudes or phases.

Referring to FIGS. 13A-C, the waveform of FIG. 11 is processed by a Hanning window. It can be seen that the original amplitudes and phases are distorted. Also illustrated in FIG. 13A are frequency nulls, which can sometimes occur with a Hanning window for adjacent carriers of the same amplitude and phase.

Referring now to FIGS. 14A-D, the same waveform shown in FIG. 11 is processed by the time domain based windowing process described above in reference to FIG. 10. FIG. 14A is an illustration of the time domain based windowing process as applied to the waveform of FIG. 11. FIGS. 14B-D are illustrations of the phases and amplitudes of the waveform demodulated after using the time-domain based windowing process of FIG. 14A. The time domain based windowing technique has eliminated the distortion caused by the Hanning window (as illustrated in FIGS. 13A-C). Referring to FIG. 14B, it can be seen that all but the frequencies closest to the jammer frequency are usable.

Referring to FIGS. 15A-D, the waveform of FIG. 11 is processed by the frequency domain based windowing process described above in reference to FIG. 7. FIG. 15A is an illustration of the frequency domain based windowing process as it is applied to the waveform of FIG. 11. FIGS. 15B-D are illustrations of the phases and amplitudes of the waveform demodulated after using the frequency domain based windowing process of FIG. 15A. The figures show results which are comparable to those obtained using the time domain based windowing technique.

It will be appreciated by those skilled in the art that the windowing function may be selected as any "symmetric" apodizing window function, that is, an apodizing window function which has the property W_j + W_{(FFTSize/2+j)}=constant, where FFTSize is the size of the FFT sample. In the case of the Hanning window, all values of j add up to 1. Thus, the Hanning window has this property. Another example of such a symmetric apodizing window function would be a triangular window.

Other Embodiments

It is to be understood that while the invention has been described in conjunction with the detailed description thereof, the foregoing description is intended to illustrate and not limit the scope of the invention, which is defined by the scope of the appended claims. Other embodiments are within the scope of the following claims.