Digital Communications
MATCHED FILTER
Dr/ Amr Wageeh
Matched Filter
Threshold
ro(t)
π
ΰ·
ro(T)
• Filter that maximize instantaneous SNR at the output.
•
π1π π −π2π (π) 2
2
SNR = ζ =
ππ2
• Filter is matched to input signal
• Design on difference signal g(t) = S1(t)- S2(t)
SNR = ζ2 is max
hMF(t)
HMF(f)
ro(t)
ro(T)
Threshold
• Design on difference signal g(t) = S1(t)- S2(t)
SNR = ζ2 is max
g(t)+ N(t)
go(t)+ No(t)
hMF(t)
HMF(f)
Threshold
go(T)+ No(T)
Notes
• Dealing with filters: for deterministic signal
x(t)
h(t)
H(f)
y(t) = x(t)*h(t)
Y(f) = X(f).H(f)
y(t)
Notes
• Dealing with filters: for random signal
n(t)
Sn(f)
h(t)
no(t)
So(f)
H(f)
∞
2
Total power at output σ no= β«Χ¬β¬−∞ So(f) ππ
Cauchy Shuartz inequlaity
∞
β«Χ¬β¬−∞ π1 (π₯)π2 (π₯) ππ₯ 2 ≤
∞
∞
2
β«Χ¬β¬−∞ π1 (π₯) ππ₯ . β«Χ¬β¬−∞ π2 (π₯) 2 ππ₯
if f1(x) = const f2*(x)
For Deterministic signal
• go(t) = F-1 {Go(f)}
=
∞
β«Χ¬β¬−∞ πΊπ π
π π2πππ‘ ππ
∞
= β«Χ¬β¬−∞ πΊ π
π»(π) π π2πππ‘ ππ
∞
go(T) = β«Χ¬β¬−∞ πΊ π
π»(π) π π2πππ ππ
For Random Signal
∞
• σ2n= β«Χ¬β¬−∞ Sn(f) |π»(π)|2 ππ
• SNR
ππ (π) 2
2
=ζ =
σ2n
∞
=
β«Χ¬β¬−∞ πΊ π π»(π) π π2πππ ππ 2
β«Χ¬β¬−∞ Sn(f) |π»(π)|2 ππ
∞
∞
=
β«Χ¬β¬−∞ ππ (π) π»(π)
β«Χ¬β¬−∞ Sn(f) |π»(π)|2 ππ
∞
β«Χ¬β¬−∞ Sn(f) |π»(π)|2 ππ
∞
≤
πΊ π
π π2πππ ππ 2
ππ (π)
∞
β«Χ¬β¬−∞
πΊ π
π π2πππ ππ 2
ππ (π)
Sn(f) |π»(π)|2 ππ
∞
= β«Χ¬β¬−∞
πΊ π
ππ (π)
∞
π π2πππ 2 df = β«Χ¬β¬−∞
πΊ π
ππ (π)
2 df
Matched filter design
∗
•
ππ (π) π»(π) = const
πΊ π
ππ (π)
π −π2πππ
∗
πΊ π −π2πππ
• π»ππΉ (π) = const
π
ππ(π)
∗
∗
[π1 π −π2 π ] −π2πππ
• π»ππΉ (π) = const
π
ππ(π)
Summary in MF
• SNR = ζ2=
∞ πΊ2 π
β«Χ¬β¬−∞ π (π) df
π
∗
∗
[π1 π −π2 π ] −π2πππ
• π»ππΉ (π) = const
π
ππ(π)
ζ
ππ = π( )
2
Special case: in AWGN
• ππ π
ππ
=
2
In case of binary Comm and equiprobable system
• βππΉ = π1 π − π‘ − π2 π − π‘ .
πΈ1 −πΈ2
• ππ‘β =
2
• ππ |πππ = π(
πΈπ
2ππ
)
Proof (cont)
• ππ‘β =
ππ‘β =
πΈ1 − πΈ2
2
π1π π +π2π (π)
2
• π10 π‘ = π −1 π10 π
∞
= β«Χ¬β¬−∞ π10 (π)π π2πππ‘ ππ
∞
= β«Χ¬β¬−∞ π1 π π»ππΉ π π π2πππ‘ ππ
∞
• π10 π = β«Χ¬β¬−∞ π1 π π»ππΉ π π π2πππ ππ
∞
= β«Χ¬β¬−∞ π1 π [ π1∗ π − π2∗ π ] π −π2πππ π π2πππ ππ
∞
∞
= β«Χ¬β¬−∞ π1 (π) 2 df - β«Χ¬β¬−∞ π1 π π2∗ π df
= E1 – E12
By the same steps for S20 (T)
• π10 π = E12– E2
• ππ‘β =
πΈ1 −πΈ2
2
Parallel realization of MF
• βππΉ = π1 π − π‘ − π2 π − π‘
r(t)
π1 π − π‘
Threshold
=
π2 π − π‘
πΈ1 − πΈ2
2
Notes
ππ |= π(
πΈπ
2ππ
)
• 1. Prob of error depend on energy not waveform
π1 π‘
π1 π‘
1
T
t
t
T
π2 π‘
π2 π‘
t
T/2
t
T/4
3T/4
Notes
• Why MF is better ?
• MF benefits from entire Eg.
• Magnitude response of MF is equal to spectrum of signal.
• Choice of T
• 0 ≤ T ≤ Tb
• Causal: T must have MF causal
Optimizing Pe
• How to design S1(t) and S2(t).
• Cross correlation factor:
• π12 =
1
∞
β«π)π‘( π Χ¬β¬2 (π‘)ππ‘ =
πΈ πΈ −∞ 1
1 2
1
πΈ1 πΈ2
E12
• Represents the relation between signals S1(t) and S2(t).
• ππ = Q(
πΈ1 +πΈ2 −2 πΈ1 πΈ2 π12
2 ππ
)
-1 ≤ π12 ≤ 1
ππ |= π(
πΈπ
2ππ
• Eg is the energy of g(t).
∞
• πΈπ = β«Χ¬β¬−∞ π(π‘) 2 dt
∞
= β«Χ¬β¬−∞ S1(t)−S2(t) 2 dt
∞
∞
∞
= β«Χ¬β¬−∞ S1(t) 2 dt + β«Χ¬β¬−∞ S2(t) 2 dt – 2 β«Χ¬β¬−∞ S1(t)S2(t) dt
= E1 + E2 – 2 E12
)
Special cases for π12
• π12 = 1
fully correlated
• π12 = -1
antipodal signal
• π12 = 0
1. π12 = 1 fully correlated
• S1(t) = const S2(t)= +αS2(t).
Two signals have the same shape, polarity , with different amplitude
S1(t)
1
t
T
S2(t)
ππ = Q(
1/ α
t
T
πΈ1 +πΈ2 −2 πΈ1 πΈ2
2 ππ
)= Q (
πΈ1 − πΈ2
2 ππ
)
2. π12 = -1 antipodal signal
• S1(t) = const S2(t)= -αS2(t).
Two signals have the same shape, different polarity
S1(t)
1
t
T
S2(t)
ππ = Q(
T
-α
t
πΈ1 +πΈ2 +2 πΈ1 πΈ2
2 ππ
)= Q (
πΈ1 + πΈ2
2 ππ
)
3. π12 = 0
∞
β«Χ¬β¬−∞ π1 (π‘)π2 (π‘)ππ‘= 0
ππ = Q(
πΈ1 +πΈ2
)
2 ππ
Correlator implementation
• Output of MF ro(T) can be implemented using correlator (fixed components).
ππ
• ππ (π) = β«π‘π π‘ π π‘ π πΧ¬β¬
r(t)
X
g(t)
ππ
ΰΆ±
π
ππ (π)
Equivalent to
r(t)
g(T-t)
ππ (π‘)
ππ (π)
NWGN case (whitening filter)
n(t)
NWGN
PSD = Sn(f)
HW(f)
π(π‘)
ΰ·€
WGN
PSD = No/2
• πππ π = ππ π . π»π (π) 2
• No/2 = ππ π . π»π (π) 2
• π»π (π) =
ππΰ΅
2
πα1 π − π‘
ππ π
r(t)
S(t)+n(t)
πα1(t)=S1(t)*hw(t)
HW(f)
πα (π‘) + π(π‘)
ΰ·€
πα2(t)=S2(t)*hw(t)
πα2 π − π‘
-
Proofs
Proof
• Note:
• X(-t)
X*(f)
• X(t-T)
X(f) e-j2πfT
∞
∞
∗
• E = β«Χ¬β¬−∞ π1 (π‘). π2 (π‘) dt = β«Χ¬β¬−∞ π1 (π). π2 (π) df cross energy (correlation between signals).
∗
∗
[π π −π2 π ] −π2πππ
• π»ππΉ (π) = const 1
π
ππ(π)
•
at AWGN
ππ π =
∗
ππ
2
∗
[π π −π π ] −π2πππ
• π»ππΉ (π) = const 1 ππ 2
π
ΰ΅2
∗
ππππ π‘
[π
ππΰ΅
1
2
∗
•
=
•
= S1(-(t-T) - S2(-(t-T)
π − π2
π ] π −π2πππ
Proof (Cont)
ζ
• ππ = π( )
2
• SNRo
= ζ2=
• Pe = Q(
1
2
∞ πΊ2 π
β«Χ¬β¬−∞ π (π) df
π
2πΈπ
ππ
) = Q(
=
πΈπ
2ππ
)
2 ∞
2(π) df = 2 E
πΊ
β«Χ¬β¬
ππ −∞
ππ g
Correlator implementation
• ππ (π‘) =r(t)*hMF(t)
= r(t)*g(T-t)
∞
= β«Χ¬β¬−∞ π π . π π − π‘ − π ππ
∞
• ππ (π‘) = β«Χ¬β¬−∞ π π . π π − π − π
∞
∞
ππ
= β«Χ¬β¬−∞ π π . π π ππ = β«Χ¬β¬−∞ π π‘ . π π‘ ππ‘