EQUALIZATION SCHEME FOR
DSL RECEIVERS IN PRESENCE OF AN UNDER-SAMPLED
OR OVER-SAMPLED TRANSMIT IDFT
[0001] The present invention relates generally to digital subscriber line (DSL) technology, and specifically to a method for improving data transmission in a discrete multi tone (DMT)-based cornήiunication system.
BACKGROUND OF THE INVENTION [0002] It is well known that some current modems operating in accordance with G.992.1 and G.992.2 standards implement a transmitter with an Inverse Discrete Fourier Transform (IDFT) size greater than the one specified by the standards. These modems may implement the transmitter in either the upstream or downstream direction, or both. There are many reasons that may influence this decision. For example, for an upstream channel the standard IDFT size is 64 points. However, an IDFT size greater than 64 points may be justified for two reasons. The first reason is hardware symmetry with the downstream channel, since the downstream channel requires a larger Discrete Fourier Transform
(DFT). The second reason is ease of implementation of different Annexes of the G.992.1 and G.992.2 standards with the same data path.
[0003] It is well know that Asymmetric Digital Subscriber Loop (ADSL) systems suffer from some performance degradation whenever there is a mismatch between the transmitter IDFT and receiver DFT sizes. This is particular true on short loops where the channel is Inter-Symbol Interference (ISI) - Inter-Channel Interference (ICI) dominated, as the DFT/TDFT size mismatch increases the ISI-ICI effects. Laboratory tests show that if the transmitter uses an IDFT other than that suggested by the standard on short loops, data rate penalties of approximately 25 to 30% are experienced. [0004] However, if the transmitter IDFT size is known a priori, that is before training the receiver equalizer, the receiver DFT could possibly be changed to match the size of the transmit IFFT. This allows the performance to be optimized regardless of the IDFT size used by the transmitter. However, this solution has two potential problems. The first problem is the IDFT size may simply not be known a priori. The problem particularly applies to G.992.1 and G.992.2 modems, while new G.dmt-bis and G.lite-bis standards have G.hs codepoints defined for exchanging information about the transmitter IDFT. The
second problem is the receiver may not be able to change the DFT size on the fly due to "Millions of Instructions per Second" (MIPS) or hardware limitations. [0005] Thus there is a need for a system and method for allowing the transmitter to use an IDFT having a size different to that specified in the standard, while reducing data rate penalties. It is an object of the present invention to obviate or mitigate at least some of the above-mentioned disadvantages.
BRIEF SUMMARY OF THE INVENTION [0006] In accordance with an aspect of the present invention, there is provided a circuit and method for reducing the effect of having potentially different sizes for an Inverse Discrete Fourier Transform (IDFT) at a transmitter and a Discrete Fourier Transform (DFT) at a receiver in a telecommunications system without requiring a change in the DFT's size. The method includes following steps. The first step includes determining whether the IDFT size is greater than, equal to, or less than the DFT size. The second step includes selecting a target impulse response length from a predefined set of impulse response lengths in accordance with a result the previous step. The third step includes training an equalizer at the receiver to the target impulse response length. The circuit includes hardware and software for implementing the method.
[0007] It is an advantage of the present invention that the transmitter can use an IDFT having a size different to that specified in the standard without requiring a priori knowledge of the transmitter size IDFT or requiring the DFT size to change.
BRIEF DESCRIPTION OF THE DRAWINGS
[0008] Embodiments of the present invention will now be described by way of example only with reference to the following drawings in which:
[0009] Fig. 1 is block diagram of a Discrete MultiTone (DMT) communication system (prior art);
[0010] Fig. 2 is digital model of an improvement on the system illustrated in Fig. 1 according to an embodiment of the present invention;
[0011] Fig. 3 is a further simplified digital model of the system illustrated in Fig. 2 for an under-sampled IFFT; [0012] Fig. 4a is a sample DMT symbol;
[0013] Fig. 4b is an upsampled version of the DMT symbol illustrated in Fig. 4a;
[0014] Fig. 4c is a sample impulse response;
[0015] Fig. 5 is a further simplified digital model of the system illustrated in Fig. 2 for an over-sampled IFFT; and
[0016] Fig. 6 is a block diagram of a method according to an embodiment of the present invention.
DETAILED DESCRIPTION OF THE INVENTION
[0017] For convenience, like numerals in the description refer to like structures in the drawings. In the present embodiment, the IDFT is implemented using an Inverse Fast Fourier Transform (IFFT) and the DFT is implemented using a Fast Fourier Transform (FFT). Other implementations will be apparent to a person skilled in the art. [0018] Referring to Figure 1, a Discrete MultiTone (DMT) communication system in accordance with the prior art is illustrated generally by numeral 100. The communication system comprises a transmitter 101, a loop 114 and a receiver 123. The transmitter includes an IFFT 102, a prefix adder 104, digital filters 106a, a digital-to-analog (D/A) converter 108, analog filters 110a, and a line driver 112. The receiver 123 includes analog filters 110b, digital filters 106b, an analog-to-digital (A/D) converter 116, a time domain equalizer (TDEQ) 118, a prefix remover 120, and an FFT 122. Typically, the prefix is a cyclic prefix (CP). The IFFT 102 is coupled to the loop 114 via the prefix adder 104, the digital filters 106a, the D/A converter 108, the analog filters 110a, and the line driver 112, which is coupled to the loop 114. The FFT 122 is coupled to the loop 114 via the prefix remover 120, the TDEQ 118, the digital filters 106b, the A/D converter 116, and the analog filters 110b, which are coupled to the loop 114. Further, the receiver 123 includes circuitry for implementing the method described herein, as will be appreciated by a person skilled in the art. [0019] In the transmitter 101, for every DMT symbol period, a set of N/ Quadrature Amplitude Modification (QAM) symbols is used to modulate a set of N; tones. For simplicity, N; is referred to as the size of the IFFT even though the actual size is 2*N/, including the conjugate pairs for each carrier. This is achieved by feeding the QAM symbols c , where
to the IFFT input, and where the index i indicates the DMT symbol period. [0020] Each QAM symbol c{ carries b
/ bits, where hi is referred to as the bit allocation table and
Further, each QAM symbol c{ is scaled by a fine gain g
/, where
before being processed by the IFFT 102. These fine gains are used to change the transmit power in each tone individually. In order for the transmission signal
to be real, complex Hermitian symmetry has to be met among the transmit QAM symbols c}. That is, c/= c*N
/-7,*. At the IFFT output, the CP is added to the DMT symbol, or transmit frame, which is then further conditioned by the transmitter's front end, including the digital filters 106a, D/A converter 108, analog filters 110a and line driver 112, before being transmitted on the line. At the receiver side, the receiver's front end processes the received signal using analog filtering 110b, A/D conversion 116 and digital filtering 106b. The TDEQ 118 then partially equalizes the signal at the output of the receiver front end. After the CP has been stripped off, an FFT is performed on the receiver frame. At the FFT output, a per-tone single tap Frequency Domain Equalizer (FDEQ) 124 completes the equalization of the signal, and a set of slicers 126 finally retrieves the transmitted QAM symbols c{.
[0021] The size N2 of the receiver FFT 122 can, in general, be different than the size Nj of the transmitter IFFT 102. Similarly to the IFFT, the actual size of the FFT is 2*N2, including the conjugate pairs for each carrier. It will be apparent that the factor of two can be dropped from both the size of the IFFT and the size of the FFT for the purpose of the present discussion as they will be compared as a ratio. While it is always possible to choose a value for N2 that is greater than Ni, N2 can be less than Ny only if the number of tones that carry data is less than Nι/2. Note also, that if the values for N2 and N; are not equal, the clocks at which the IFFT and FFT run, fs_ andfs respectively, are also different. Particularly, in order to have the same carrier spacing at the transmitter and the receiver, the following relationship should be met:
(1) [0022] Accordingly, the number of samples added in the transmitter and removed in the receiver as a CP varies in accordance with
( 2) where Cpi and Cp2 are the number of samples corresponding to the cyclic prefix in the transmitter and the receiver respectively.
[0023] The following description examines the situations for which N; is a multiple of N2, representing an over-sampled IFFT, and N2 is a multiple of N/, representing an under- sampled IFFT. It is possible, but unlikely, that Ni is not an integer multiple of N2 and vice
versa. This is because the standard specifies DSL bands as having power-of-two number of carriers and because the most efficient algorithms to implement a DFT/IDFT (including FFT) are powers of two. That being said, it is believed the analysis as follows is applicable to cases where the ratio of Ny to N2, or vice versa, is non-integer. [0024] Referring to Figure 2, an all-digital model of an improvement on the system depicted in Figure 1 is illustrated by numeral 200. For this model 200 it has been assumed that the analog portion 110 of the communication channel has a finite bandwidth B so that it can be simulated by a digital filter 202 with impulse response hChan(k) at sampling frequency fs>2B. Further, - fs/fsι=Mι
( 3) and fs/fs2-M2 (
4) where Mi and M
2 are integers. Yet further, the transmit and receive digital filters including the TDEQ, can be up-sampled to the same clock frequency and their resulting impulse responses can be convolved with h
cι
mn(k), for a filter 202 with an overall channel impulse response h(k). As a result, DMT symbols from the transmitter are upsampled by Mi, once the CP has been added, from the sampling frequency -'
/ of the transmitter IFFT 204 to the sampling frequency fs of the filter 202. Similarly, at the receiver, the DMT symbols are downsampled by M
2 before removing the CP, from the sampling frequency fs of the filter 202 to the sampling
of the receiver FFT 206. [0025] Under-Sampled Case
[0026] From equations (3) and (4), it can be seen that Mi and M2 are inversely proportional to fsi and fs2, respectively. Thus, for the case of an under-sampled IFFT, the sampling frequency fsj of the IFFT is less than sampling frequency fs2 of the FFT, and ; is greater than M2. As a result, Mi can be expressed as Mι=MxM2, where M is an integer that corresponds to the ratio between the FFT and IFFT sizes. Thus, in the present embodiment, the FFT is M times larger than the IFFT. Also, from equations (2), (3), and (4), it can be seen that
Cp2ICpι=M
( 5)
[0027] Thus, the model 200 illustrated in Figure 2 can be further simplified. Referring to Figure 3, an all-digital model for an over-sampled IFFT is illustrated generally by numeral 300. The filter 302 of the present model is represented by g(k). It can be seen that in the under-sampled case, the system 300 of Figure 3 is equivalent to the system 200 in Figure 2 for g(k)=h(M2xk) and fs=fs2. Thus, output x(k) of the CP adder 304 is upsampled by M from the sampling frequency/-?; of the IFFT 306 to the sampling frequency s of the filter g(k) 302. The upsampled DMT symbol is represented by y(k) and the filtered DMT symbol is represented by z(k).
[0028] For the model 300 illustrated in Figure 3, it is desirable to determine the condition for which the transmission is ISI-ICI free. Toward this end, it is assumed that the filter g(k) 302 is time-limited to an interval [0, L-l] as expressed in number of samples at the sample frequency fs of the filter g(k) 302. In the present embodiment, zero propagation delay is assumed for simplifying the notations. However, a person skilled in the art will be able to verify that the results described herein would also apply in presence of any propagation delay. At the receiver, the frame alignment is such that the first DMT frame to be processed by the FFT 308 is at start time instant t=0. [0029] Referring to Figure 4a, an example of a DMT symbol x(k) to be transmitted is illustrated. Referring to Figure 4b, an upsampled representation y(k) of the DMT x(k) is illustrated for M=4. Referring to Figure 4c, a representation of the transfer function of the filter g(k) is illustrated. It is assumed that the origin of the time axis is fixed as shown in Figures 4a-4c. [0030] As illustrated in Figure 3, the filtered signal z(k) is given by the convolution between yβ): and gβ). Instead of computing the convolution analytically, the desired result can be achieved by inspection of Figures 4a-4c. The convolution between the two functions yβ) and gβ) involves flipping gβ) around the origin and computing the sum of the correlation between the two signals for different relative time delays. It can be seen that the result of the convolution between gβ) and yβ) can be divided into three sections. A first section comprises an initial transient, a second section comprises a steady state-like waveform, and a final section comprises a final transient. Each of these sections corresponds to different values of A; as well as to different relative positions of gβ-n) and y(n) in the convolution operation, as will be appreciated by a person skilled in the art. The
first and the final transients correspond to a partial overlap between the two signals, while the steady state-like waveform corresponds to a full overlap between the two signals. Due to the presence of the zeros in the upsampled signal yβ), it can be seen that the first transient occurs for -MCpi ≤k ≤-MCpι-M+L-1, while the final transient occurs for M(Nr l)+M <k ≤M(N l)+L-l.
[0031] At the receiver, Cp2 samples are removed from received signal zβ). For the first DMT symbol, the cyclic prefix Cp2 is removed for k=-Cp2, ...,-1. The following N2 samples, that is for k=0, ...,N2-l, represent the first DMT symbol itself. For the second DMT symbol, the cyclic prefix Cp2 is removed for the following Cp2 samples, that is for k=N2, ... ,N2+Cp2-1. This process for removing the CP is repeated periodically every N received samples. Therefore, in order to be ISI-ICI free, the first transient of zβ) should be confined to the time window where the first CP is removed, while the last transient of zβ) should be confined to the time window where the second CP is removed. Mathematically, these limitations are represented as follows. [0032] For the initial transient, the lower bound of A: is -MCpi . The lower bound of k for the cyclic prefix for the first DMT symbol is -Cp2. Thus, to ensure that the initial transient is within the cyclic prefix, as desired, the lower bound of the initial transient should be at least equivalent to the lower bound for the cyclic prefix, or MCpι>-Cp2-l (
6)
Since, from equation (5), Cp2=MCpι, equation (6) can be rewritten as Cp <Cp2+l, which is always true.
[0033] Similarly, for the initial transient, the upper bound of ft is -MCpι-M+L-1. The upper bound of A; for the cyclic prefix for the first DMT symbol is -1. Thus, to ensure that the initial transient is with the cyclic prefix, as desired, the upper bound of the initial transient should be at most equivalent to the upper bound for the cyclic prefix, or
( 7)
Equation (7) can be rewritten as -MCpj-M+L<-l, which can be rewritten as L ≤ MCpi+M. From equation (5), the previous equation can be rewritten as L ≤ Cp2+M.
[0034] For the final transient, the lower bound of A: is M(Nι-l)+M. The lower bound of k for the cyclic prefix for the second DMT symbol is N2. Thus, to ensure that the initial transient is within the cyclic prefix, as desired, the lower bound of the initial transient should be at least equivalent to the lower bound for the cyclic prefix, or M(Nι-l)+M>N2-l
( 8)
Equation (8) can be rewritten as MN]-M+M>N2-1 , which can be rewritten as MNι>N2-l. Since N2=MNι, the equation can be rewritten as N2>N2-1, which is always true. [0035] Similarly, for the final transient, the upper bound of A is M(Nι-l) +L-1. The upper bound of A; for the cyclic prefix for the second DMT symbol is N2+Cp2-1. Thus, to ensure that the initial transient is with the cyclic prefix, as desired, the upper bound of the initial transient should be at most equivalent to the upper bound for the cyclic prefix, or M(Nι-l)+L-l< N2+Cp2 (
9)
Equation (9) can be rewritten as M(Nι-l)+L-KMNι+MCpι, which can be rewritten as
L≤MCpj+M. From equation (5), the previous equation becomes L≤=Cp2+M.
[0036] Thus, the conclusion from both the first and final transients is that for an under- sampled IFFT, the ISI-ICI free condition is guaranteed if the length of the total channel impulse response g(k) is less than the CP length at the receiver side plus the ratio between the FFT and IFFT sizes. It should also be noted that the impulse response g(k) also corresponds to the shortened impulse response of the channel, as it matches to the convolution between the TDEQ and the channel impulse response at the FFT clock frequency. Therefore, in order to achieve the desired channel impulse response gβ), when training the TDEQ the target impulse response length can be set to Cp2+M. [0037] Over-Sampled Case
[0038] In the over-sampled case, M
2 can be expressed as
where M is an integer that also corresponds to the ratio between the IFFT and FFT sizes. Thus, in the present embodiment, the IFFT is M times larger than the FFT. Also, the relationship between the cyclic prefix Cpi of the transmitter and the cyclic prefix Cp
2 of the receiver can be expressed as
Cpι/Cp
2=M
( 10)
[0039] Similarly to the under-sampled case, the model 200 illustrated in Figure 2 can be further simplified for the over-sampled case. Referring to Figure 5, an all-digital model for an over-sampled IFFT is illustrated generally by numeral 500. The filter 502 of the present model is represented by gβ). It can be seen that in the over-sampled case, the system of Figure 5 is equivalent to the system in Figure 2 for
Thus, output zβ) of the filter 502 is downsampled by M from the sampling frequency/.*? of the filter gβ) to the sampling frequency /s
2 of the FFT 504. The downsampled DMT symbol is represented by qβ).
[0040] As in the previous embodiment, for the model 500 illustrated in Figure 5 it is desirable to determine the condition for which the transmission is ISI-ICI free. Toward this end, it is assumed that the filter gβ) 502 is time-limited to an interval [0, L-l] as expressed in number of samples at the sampling frequency fs of the filter gβ) 502. In the present embodiment, zero propagation delay is assumed for simplify the notations. However, a person skilled in the art will be able to verify that the results described herein would also apply in presence of any propagation delay. [0041] As illustrated in Figure 5, the filtered signal zβ) is given by the convolution between xβ) and gβ). Similarly to the previous embodiment, the desired result can be achieved by inspection of Figures 4a and 4c. Figure 4b is irrelevant for the present embodiment. The convolution between the two functions xβ) and gβ) involves flipping gβ) around the origin and computing the sum of the correlation between the two signals for different relative time delays. [0042] By resorting to a similar argument as in the previous embodiment, it can be seen that the initial and final transients of the signal z(k) when transmitting only one DMT symbol around the time origin take place for -Cpι<k≤-Cpι-1+L-1 and for Nι≤k≤Nι-1+L- 1. Further, the steady state-like signal occurs for 0<k≤Nι-l. However, the signal z(k) is downsampled by a factor of M to yield qβ), from which Cp
2 samples of cyclic prefix are removed. Therefore, the steady state-like signal for qβ) occurs for 0__^.__Ηι/M-l/M=N
2- 1/M. Since N
2-l/M is not an integer, the upper bound of the interval becomes N
2-l, as expected, since the FFT 504 at the receiver needs N
2 samples for each DMT symbols. For the transient duration, the following constraints apply.
[0043] For the initial transient, the lower bound of A: is -Cp /M. The lower bound of A: for the cyclic prefix for the first DMT symbol is -Cp
2. Thus, to ensure that the initial transient is within the cyclic prefix, as desired, the lower bound of the initial transient should be at least equivalent to the lower bound for the cyclic prefix, or
( 11) Since Cpι/Cpf=M, the equation can be rewritten as Cp2<Cp2+l, which is always true.
[0044] Similarly, for the initial transient, the upper bound of A; is (-Cpι-1+L-1)/M. The upper bound of A for the cyclic prefix for the first DMT symbol is -1. Thus, to ensure that the initial transient is with the cyclic prefix, as desired, the upper bound of the initial transient should be at most equivalent to the upper bound for the cyclic prefix, or (-Cpι-1+L-1)/M<0
( 12)
The equation can be rewritten as L<Cpι+2, which can be rewritten as L≤Cpι+1. [0045] For the final transient, the lower bound of k is Nj/M. The lower bound of k for the cyclic prefix for the second DMT symbol is N2. Thus, to ensure that the initial transient is within the cyclic prefix, as desired, the lower bound of the initial transient should be at least equivalent to the lower bound for the cyclic prefix, or N}/M>N2-1
( 13)
[0046] Similarly, for the final transient, the upper bound of A: is ((Nι-1)+L-1)/M. The upper bound of A: for the cyclic prefix for the second DMT symbol is N2+Cp2-1. Thus, to ensure that the initial transient is with the cyclic prefix, as desired, the upper bound of the initial transient must be at most equivalent to the upper bound for the cyclic prefix, or (NAL-2)/M<N2+Cp2
( 14)
Since N_ =MN2 and Cpι-MCp2, the equation can be rewritten as Nι+L-2<Nι+Cpj, which can be rewritten as L<Cpι+2, which can further be rewritten as L≤Cpj+1.
[0047] Thus, the conclusion from both the first and final transients is for an over- sampled IFFT, the ISI-ICI free condition is guaranteed if the length of the total channel impulse response g(k) is less than the CP length at the transmitter side plus one. It should also be noted that the impulse response g(k) also corresponds to the shortened impulse response of the channel, as it matches to the convolution between the TDEQ and the channel impulse response at the FFT clock frequency. Therefore, in order to achieve the desired channel impulse response gβ), when training the TDEQ the target impulse response length can be set to Cpι+1. [0048] For yet a further embodiment, a situation is illustrated for an over-sampled IFFT where the channel impulse response is advanced by D samples at the IFFT clock frequency. The same steps performed above are repeated, and the results are provided as follows.
[0049] For the initial transient, from the lower bound it can be determined that
(Cpι+D)/M<Cp2+l . This equation can be rewritten as Cpι+D<Cpj+M which is true for all cases where D<M.
[0050] From the upper bound it can be determined that (-Cpι-l-D+1 +L-1)/M<0. This equation can be rewritten as -Cpι-D+L-1<0, or L<Cpι+D+l, which is met if L≤Cpι+1. [0051] For the final transient, from the lower bound it can be determined that (Nι-D)/M>N2-1 , which can be rewritten as Nι-D>N]-M, which is true for all D<M. [0052] From the upper bound it can be determined that (N} +L-D+l-2)/M<N2+Cp2. This equation can be rewritten as Nι+L-D-l≤Nι+Cpι, or, L<Cpι+D+l, which is met if
[0053] Therefore, the ISI-ICI free condition is met even when the channel impulse response g(k) is advanced by up to M-l samples. This result shows that there is not just one optimum frame alignment when the transmitter IFFT is over-sampled. Given the above results, it is easy to envision that when in the presence of the channel impulse response g(k) that is not time strictly time limited, one of the frame alignments as per above would result in the least ISI-ICI interference, or best capacity. [0054] Application [0055] If the transmitter IFFT size is known a priori, then the results of the previous sections can simply be applied at the receiver for improving performance. For the case where Nι=N2, the best equalization technique is to train the TDEQ and the FDEQ with the length of the target impulse response equal to Cpι+1, which is equal to Cp2+1. If,
however, N; is less than N2 then the best strategy is to train the TDEQ and the FDEQ with a target impulse response with length Cp2+M. Lastly, if Nj is greater than N2, then the best strategy is to train the TDEQ and the FDEQ with a target impulse response with length Cpι+1. For this case, the performance can be further improved by searching for an optimum frame alignment between [0, (M-l)/fs{\.
[0056] However, if the IFFT size is not known, a technique referred to herein as a "blind technique" is used to estimate the optimum equalization strategy. It is assumed that the receiver desires to use a fixed FFT size and does not know the transmitter IFFT size. The IFFT can be either equal, lesser (under-sampled IFFT) or greater (over-sampled IFFT) than the receiver FFT size. Given that Mis typically a small number, less than four (4) in most of the cases, the following procedure optimizes the transmission. [0057] A set of TDEQ pairs and FDEQ pairs is trained, each with different target impulse response length, that is Cpι+1, Cp
2+1, Cp
2+2,...,Cp
2+M
max, where M
max is a maximum expected value for M. Typically the value for M
max is programmable. During a Channel Analysis portion of the modem's initialization, each TDEQ/FDEQ pair of the set is applied and a quick per-bin signal to noise ratio (SΝR) estimate is performed. For the TDEQ/FDEQ pair trained with target impulse response Cpι+1, a set of per-bin SΝR estimates is also performed, each for a different time advance in the interval [0, (M-l)/fs . This interval can be quantized such that only a few values need to be tried. The time advance is applied, for example, by reducing the delay of a tap delay line in the modem front end at a clock frequency higher then the FFT clock frequency. The ratio of this
determine the granularity of the search. Lastly, the total per bin SΝR estimates are compared and the one with the highest geometric average is selected together with the associated TDEQ/FDEQ pair and time advance value. [0058] Figure 6 is a block diagram summarizing the steps 600 performed in an embodiment of the present invention. In step 602, it is determined whether the IDFT size of the IDFT is greater than, equal to, or less than the DFT size of the DFT. In step 604, a target impulse response length is selected from a predefined set of impulse response lengths in accordance with a result of step 602. In step 606, the equalizer at the receiver is trained to the target impulse response length. The details of these steps 600 are as described above in the previous sections. These steps 600 and their further details may be performed by implementing the structures 200, 300 and 500 shown in Figures 2, 3 and 5. Such structures may include hardware, software, firmware, programmable logic, etc. as appropriate when implemented by one of ordinary skill in the art.
[0059] Therefore, the process provides an improved equalization strategy for ADSL receivers when in the presence of transmitters with an IFFT size that potentially may not match the FFT size at the receiver. The proposed techniques involve minor modifications to the equalizer's training algorithm and allow use ofa fixed size FFT at the receiver. The performance improvements that result have to shown to be quite significant. [0060] Although the invention has been described with reference to certain specific embodiments, various modifications thereof will be apparent to those skilled in the art without departing from the spirit and scope of the invention as outlined in the claims appended hereto.