The raised-cosine filter is a filter frequently used for pulse-shaping in digital modulation due to its ability to minimise intersymbol interference (ISI). Its name stems from the fact that the non-zero portion of the frequency spectrum of its simplest form (
\beta=1
f
The raised-cosine filter is an implementation of a low-pass Nyquist filter, i.e., one that has the property of vestigial symmetry. This means that its spectrum exhibits odd symmetry about
1 | |
2T |
T
Its frequency-domain description is a piecewise-defined function, given by:
H(f)=\begin{cases} 1, &|f|\leq
1-\beta | |
2T |
\\
1 | |
2 |
\left[1+\cos\left(
\piT | |
\beta |
\left[|f|-
1-\beta | |
2T |
\right]\right)\right], &
1-\beta | |
2T |
<|f|\leq
1+\beta | |
2T |
\\ 0, &otherwise \end{cases}
H(f)=\begin{cases} 1, &|f|\leq
1-\beta | |
2T |
\\ \operatorname{hvc}\left(
\piT | |
\beta |
\left[|f|-
1-\beta | |
2T |
\right]\right), &
1-\beta | |
2T |
<|f|\leq
1+\beta | |
2T |
\\ 0, &otherwise \end{cases}
0\leq\beta\leq1
\beta
T
The impulse response of such a filter[1] is given by:
h(t)=\begin{cases}
\pi | \operatorname{sinc}\left( | |
4T |
1 | |
2\beta |
\right), &t=\pm
T | \\ | |
2\beta |
1 | \operatorname{sinc}\left( | |
T |
t | \right) | |
T |
| |||||
|
, &otherwise\end{cases}
in terms of the normalised sinc function. Here, this is the "communications sinc"
\sin(\pix)/(\pix)
The roll-off factor,
\beta
1 | |
2T |
\alpha=\beta
If we denote the excess bandwidth as
\Deltaf
\beta=
\Deltaf | ||||
|
=
\Deltaf | |
RS/2 |
=2T\Deltaf
where
RS=
1 | |
T |
The graph shows the amplitude response as
\beta
\beta
As
\beta
\lim\betaH(f)=\operatorname{rect}(fT)
where
\operatorname{rect}( ⋅ )
h(t)= | 1 | \operatorname{sinc}\left( |
T |
t | |
T |
\right)
When
\beta=1
H(f)|\beta=1=\left\{\begin{matrix}
1 | |
2 |
\left[1+\cos\left(\pifT\right)\right], &|f|\leq
1 | |
T |
\\ 0, &otherwise \end{matrix}\right.
H(f)|\beta=1=\left\{\begin{matrix} \operatorname{hvc}\left(\pifT\right), &|f|\leq
1 | |
T |
\\ 0, &otherwise \end{matrix}\right.
The bandwidth of a raised cosine filter is most commonly defined as the width of the non-zero frequency-positive portion of its spectrum, i.e.:
BW=
RS | |
2 |
(\beta+1), (0<\beta<1)
As measured using a spectrum analyzer, the radio bandwidth B in Hz of the modulated signal is twice the baseband bandwidth BW (as explained in [1]), i.e.:
B=2BW=RS(\beta+1), (0<\beta<1)
The auto-correlation function of raised cosine function is as follows:
R\left(\tau\right)=T\left[\operatorname{sinc}\left(
\tau | |
T |
\right)
| ||||||
|
-
\beta | |
4 |
\operatorname{sinc}\left(\beta
\tau | |
T |
\right)
| ||||||
|
\right]
The auto-correlation result can be used to analyze various sampling offset results when analyzed with auto-correlation.
When used to filter a symbol stream, a Nyquist filter has the property of eliminating ISI, as its impulse response is zero at all
nT
n
n=0
Therefore, if the transmitted waveform is correctly sampled at the receiver, the original symbol values can be recovered completely.
However, in many practical communications systems, a matched filter is used in the receiver, due to the effects of white noise. For zero ISI, it is the net response of the transmit and receive filters that must equal
H(f)
HR(f) ⋅ HT(f)=H(f)
And therefore:
|HR(f)|=|HT(f)|=\sqrt{|H(f)|}
These filters are called root-raised-cosine filters.
Raised cosine is a commonly used apodization filter for fiber Bragg gratings.