SLIDE 4 2010-04-20 Ove Edfors - ETI 051 13
Pulse amplitude modulation (PAM)
Basis pulses and spectrum
Illustration of power spectral density of the (complex) base-band signal, SL
P(f), and the (real) radio signal, SB P (f).
f
( )
LP
S f f
( )
BP
S f
c
f
c
f −
Symmetry (real radio signal) Can be asymmetric, since it is a complex signal.
What we need are basis pulses g(t) with nice properties like:
- Narrow spectrum (low side-lobes)
- Relatively short in time (low delay)
2010-04-20 Ove Edfors - ETI 051 14
Pulse amplitude modulation (PAM)
Basis pulses
Normalized time /
s
t T Normalized time /
s
t T (Root-) Raised-cosine [in freq.] Rectangular [in time] TIME DOMAIN
Normalized freq. f ×T s Normalized freq. f ×T s
2010-04-20 Ove Edfors - ETI 051 15
Pulse amplitude modulation (PAM)
Interpretation as IQ-modulator
f
( ) ( )
( ) Re
I LP
s t s t =
( ) ( )
( ) Im
Q LP
s t s t =
( )
cos 2
c
f t π
( )
sin 2
c
f t π −
Radio signal
For real valued basis functions g(t) we can view PAM as:
Pulse shaping filters
( )
g t
( )
g t
Mapping
m
b
m
c
( )
Re
m
c
( )
Im
m
c
(Both the rectangular and the (root-) raised-cosine pulses are real valued.)
2010-04-20 Ove Edfors - ETI 051 16
Multi-PAM Modulation with multiple pulses
Complex domain Mapping multi-PAM
m
b
m
c
( )
LP
s t
( )
exp 2
c
j f t π
Re{ } Radio signal multi-PAM: Bits Several different pulses
“Standard” basis pulse criteria (energy norm.) (orthogonality) (orthogonality)
sLPt=∑
m−∞ ∞
g cmt−mT s
∫∣gcmt∣
2dt=1 or =T s
∫ gcmt gcn
* t dt=0 for cm≠cn
∫ gcmt gcm
* t−kT s dt=0 for k≠0