Signal Time-Spreading

Module by: Thanh Do-Ngoc, Tuan Do-Hong Translated by: Thanh Do-Ngoc, Tuan Do-Hong

SIGNAL TIME – SPREADING

A simple way to model the fading phenomenon is proposed the notion wide-sense stationary uncorrelated scattering. The model treats arriving at a receive antenna with different delay as uncorrelated.

In figure 1a, a multipath-intensity profile S(τ) is plotted. S(τ) helps us understand how the average received power vary as a function of time delay τ. The term “time delay” is used to refer to the excess delay. It represents the signal’s propagation delay that exceeds the delay of the first signal arrival at the receiver. In wireless channel, the received signal usually consists of several discrete multipath components causing S(τ). For a single transmitted impulse, the time Tm between the first and last received component represents the maximum excess delay.

Figure 1

In a fading channel, the relationship between maximum excess delay time Tm and symbol time Ts can be viewed in terms of two different degradation categories: frequency-selective fading and frequency nonselective or flat fading.

A channel is said to exhibit frequency selective fading if Tm>Ts. This condition occurs whenever the received multipath components of a symbol extend beyond the symbol’s time duration. In fact, another name for this category of fading degradation is channel-induced ISI. In this case of frequency-selective fading, mitigating the distortion is possible because many of the multipath components are resolved by receiver.

A channel is said to exhibit frequency nonselective or flat fading if Tm<Ts. In this case, all of the received multipath components of a symbol arrive within the symbol time duration; hence, the components are not resolvable. There is no channel-induced ISI distortion because the signal time spreading does not result in significant overlap among neighboring received symbols.

A completely analogous characterization of signal dispersion can be specified in the frequency domain. In figure 1b, the spaced-frequency correlation function ∣R(Δf)∣∣R(Δf)∣ size 12{ lline R \( Δf \) rline } {} can be seen, it is the Fourier transform of S(τ). The correlation function ∣R(Δf)∣∣R(Δf)∣ size 12{ lline R \( Δf \) rline } {} represents the correlation between the response of channel to two signals as a function of the frequency difference between two signals. The function ∣R(Δf)∣∣R(Δf)∣ size 12{ lline R \( Δf \) rline } {} helps answer the correlation between received signals that are spaced in the frequency Δf=f1-f2 is what. ∣R(Δf)∣∣R(Δf)∣ size 12{ lline R \( Δf \) rline } {} can be measured by transmitting a pair of sinusoids separated in frequency by Δf, cross-correlating the complex spectra of two separated received signals, and repeating the process many times with ever-larger separation Δf. Spectral components in that range are affected by the channel in a similar manner. Note that the coherence bandwidth f0 and the maximum excess delay time Tm are related as approximation below

f0≈1Tmf0≈1Tm size 12{f rSub { size 8{0} } approx { {1} over {T rSub { size 8{m} } } } } {}(1)

A more useful parameter is the delay spread, most often characterized in terms of its root-mean-square (rms) value, can be calculated as

στ=(τ2¯−τ¯2)1/2στ=(τ2¯−τ¯2)1/2 size 12{σ rSub { size 8{τ} } = \( {overline {τ rSup { size 8{2} } }} - {overline {τ}} rSup { size 8{2} } \) rSup { size 8{1/2} } } {}(2)

Where τˉτˉ size 12{ { bar {τ}}} {} is the mean excess delay, (τˉ)2(τˉ)2 size 12{ \( { bar {τ}} \) rSup { size 8{2} } } {} is the mean squared, τ2¯τ2¯ size 12{ {overline {τ rSup { size 8{2} } }} } {} is the second moment and στστ size 12{σ rSub { size 8{τ} } } {} is the square root of the second central moment of S(τ).

A relationship between coherence bandwidth and delay spread does not exist. However, using Fourier transform techniques an approximation can be derived from actual signal dispersion measurements in various channel. Several approximate relationships have been developed.

If the coherence bandwidth is defined as the frequency interval over which the channel’s complex frequency transfer function has a correlation of at least 0.9, the coherent bandwidth is approximately

f0≈150στf0≈150στ size 12{f rSub { size 8{0} } approx { {1} over {"50"σ rSub { size 8{τ} } } } } {}(3)

With the dense-scatterer channel model, coherence bandwidth is defined as the frequency interval over which the channel’s complex frequency transfer function has a correlation of at least 0.5, to be

f0≈12πστf0≈12πστ size 12{f rSub { size 8{0} } approx { {1} over {2 ital "πσ" rSub { size 8{τ} } } } } {}(4)

Studies involving ionospheric effects often employ the following definition

f0≈15στf0≈15στ size 12{f rSub { size 8{0} } approx { {1} over {5σ rSub { size 8{τ} } } } } {}(5)

The delay spread and coherence bandwidth are related to a channel’s multipath characteristic, differing for different propagation paths. It is important to note that all parameters in last equation independent of signaling speed, a system’s signaling speed only influences its transmission bandwidth W.

A channel is preferred to as frequency-selective if f0<1/Ts = W (the symbol rate is taken to be equal to the signaling rate or signal bandwidth W). Frequency selective fading distortion occurs whenever a signal’s spectral components are not all affected equally by the channel. Some of the signal’s spectra components failing outside the coherent bandwidth will be affected differently, compared with those components contained within the coherent bandwidth (figure 2a).

Frequency- nonselective of flat-fading degradation occurs whenever f0>W. hence, all of signal’s spectral components will be affected by the channel in a similar manner (fading or non-fading) (figure 2b). Flat fading does not introduce channel-induced ISI distortion, but performance degradation can still be expected due to the loss in SNR whenever the signal is fading. In order to avoid channel-induced ISI distortion, the channel is required to exhibit flat fading. This occurs, provide that

f 0 > W ≈ 1 T s f 0 > W ≈ 1 T s size 12{f rSub { size 8{0} } >W approx { {1} over {T rSub { size 8{s} } } } } {}

(6)

Hence, the channel coherent bandwidth f0 set an upper limit on the transmission rate

However, as a mobile radio changes its position, there will be times when the received signal experiences frequency-selective distortion even though f0>W (in figure 2c). When this occurs, the baseband pulse can be especially mutilated by deprivation of its low-frequency components. Thus, even though a channel is categorized as flat-fading, it still manifests frequency-selective fading.

Figure 2

The signal dispersion manifestation of the fading channel is analogous to the signal spreading that characterizes an electronic filter. Figure 3a depicts a wideband filter (narrow impulse response) and its effect on a signal in both time domain and the frequency domain. This filter resembles a flat-fading channel yielding an output that is relatively free of dispersion. Figure 3b shows a narrowband filter (wide impulse response). The output signal suffers much distortion, as shown both time domain and frequency domain. Here the process resembles a frequency-selective channel.

Figure 3

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This work is licensed by Thanh Do-Ngoc and Tuan Do-Hong under a Creative Commons Attribution License (CC-BY 2.0).

Last edited by Tuan Do-Hong on Nov 13, 2007 8:41 pm US/Central.