[IEEE ICASSP 2014 - 2014 IEEE International Conference on Acoustics, Speech and Signal Processing...
Transcript of [IEEE ICASSP 2014 - 2014 IEEE International Conference on Acoustics, Speech and Signal Processing...
2014 IEEE International Conference on Acoustic, Speech and Signal Processing (ICASSP)
978-1-4799-2893-4/14/$31.00 ©2014 IEEE 2982
x[n]
X[k] =
√2
N
k+N−1∑n=k
x[n]e−jγn, k = 0, . . . ,K − 1,
k
ω0 +Δ ω0
100π 120π Δ
Va, Vb, Vc ≥ 0 ϕa, ϕb, ϕc ∈ [0, 2π]
Va = Vb = Vc ϕa = ϕb +2π3
= ϕc − 2π3
N ω0
⎡⎣ va[n]
vb[n]vc[n]
⎤⎦ =
1
2ejγ
ω0+Δ
ω0nv +
1
2e−jγ
ω0+Δ
ω0nv∗ +wa,b,c[n],
∀n ∈ R γ�= 2π
Nv
�=
[Vae
jϕa , Vbejϕb , Vce
jϕc
]{wa,b,c[n]}n∈Z
σ2I3
I3 3 × 3Va = Vb = Vc
ϕa = ϕb +2π3
= ϕc − 2π3
{va[n]}, {vb[n]}{vc[n]}
k+N−1∑n=k
ejαn =sin(αN/2)
sin(α/2)ejα(k+
N−12 ), ∀α ∈ R,
⎡⎣ Va[k]
Vb[k]Vc[k]
⎤⎦ =
1√2Pe
jγ Δω0
kv +
1√2Qe
−jγ2ω0+Δ
ω0kv∗
+
√2
N
k+N−1∑n=k
wa,b,c[n]e−jγn,
k = 0, . . . ,K − 1
P =sin(γN Δ
2ω0)
N sin(γ Δ2ω0
)ejγ Δ
ω0
N−12
Q =sin(γN 2ω0+Δ
2ω0)
N sin(γ 2ω0+Δ2ω0
)e−jγ
2ω0+Δ
ω0
N−12 .
P QΔ k
PQ Δ
⎡⎣ V0[k]
V+[k]V−[K]
⎤⎦ =
1
3
⎡⎣ 1 1 1
1 α α2
1 α2 α
⎤⎦
︸ ︷︷ ︸�=H
⎡⎣ Va[k]
Vb[k]Vc[k]
⎤⎦ ,
∀k = 0, 1, . . . ,K − 1 V0[k], V+[k] V−[k]
α = ej2π/3
V0[k] = Pejγ Δ
ω0kC0 +Qe
−jγ2ω0+Δ
ω0kC∗
0 +W0[k]
V+[k] = Pejγ Δ
ω0kC+ +Qe
−jγ2ω0+Δ
ω0kC∗
− +W+[k]
V−[k] = Pejγ Δ
ω0kC− +Qe
−jγ2ω0+Δ
ω0kC∗
+ +W−[k]
k = 0, . . . ,K − 1
[C0, C+, C−]T =
√2
6Hv
⎡⎣ W0[k]
W+[k]W−[k]
⎤⎦ =
√2
3NH
k+N−1∑n=k
wa,b,c[n]e−jγn,
∀k = 0, . . . ,K − 1 HHH = 3I3
{W0[k]}K−1k=1 {W+[k]}K−1
k=1 {W−[k]}K−1k=1
2σ2
3N
C0 C+
C−
KK
ν0 = PC0e1 +QC∗0 e2 + w0
ν+ = PC+e1 +QC∗−e2 + w+
ν− = PC−e1 +QC∗+e2 + w−,
e1 =[1, e
jγ Δω0 , . . . , e
jγ Δω0
(K−1)]T
,
e2 =
[1, e
−jγ2ω0+Δ
ω0 , . . . , e−jγ
2ω0+Δ
ω0(K−1)
]T
,
ν0 = [V0[0], . . . , V0[K − 1]] ν+ = [V+[0], . . . , V+[K − 1]]ν− = [V−[0], . . . , V−[K − 1]]
e1 e2
w0 w+ w−
R R
K ×K k, l
[R]k,l =2σ2
3N2
{N − |k − l| −N ≤ k − l ≤ N0
.
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R− 1
2
ν0 = PC0e1 +QC∗0e2 +w0
ν+ = PC+e1 +QC∗−e2 +w+
ν− = PC−e1 +QC∗+e2 +w−,
em�= R
− 12 em m = 1, 2
ν0 = R− 1
2 ν0 ν+ = R− 1
2 ν+ ν− = R− 1
2 ν−
w0 = R− 1
2 w0 w+ = R− 1
2 w+ w− =
R− 1
2 w− IK
θ = [C0, C+, C−,Δ]
θ
θ = maxθ L(θ)
L(θ) = 3K log π − ||ν0 − PC0e1 −QC∗0e2||2
− ||ν+ − PC+e1 −QC∗−e2||2
− ||ν− − PC−e1 −QC∗+e2||2 .
ΔC0 C+ C−
C0 =z0 − κ2(C0)
∗
κ1
C+ =z+ − κ2(C−)
∗
κ1,
C− =z− − (C+)
∗κ2
κ1,
z0�= P ∗
eH1 ν0 + Qν
H0 e2, z+
�= P ∗
eH1 ν+ +
QνH−e2, z−
�= P ∗
eH1 ν−+Qν
H+e2, κ1
�= |P |2eH
1 e1 + |Q|2eH2 e2
κ2�= 2P ∗Qe
H1 e2
C0 =κ1z0 − κ2z
∗0
κ21 − |κ2|2 ,
C+ =κ1z+ − κ2z
∗−
κ21 − |κ2|2 ,
C− =κ1z− − κ2z
∗+
κ21 − |κ2|2 .
C0 C+ C−
L(θ) = 3K log π − ||ν0||2 − ||ν+||2 − ||ν−||2
+κ1
(|C0|2 + |C+|2 + |C−|2
)+
{κ∗2
(C2
0 + 2C+C−
)}.
Δ
Δ = argmaxΔ
[κ1
(|C0|2 + |C+|2 + |C−|2
)
+{κ∗2
(C2
0 + 2C+C−
)}].
Δ[−Nω0
2, Nω0
2
)
Vaejϕa = Vbe
j(ϕb+2π3
) = Vcej(ϕc−
2π3
)
C0 = 0 C− = 0
⎧⎨⎩
ν0 = w0
ν+ = PC+e1 +w+
ν− = QC∗+e2 +w−
.
C+
C(b)0 = 0, C
(b)+ =
z+κ1
, C(b)− = 0.
V+[k] = e−jγa(Δ)V+[k − 1]− e−j2γV+[k − 2]
+W+[k]− e−jγa(Δ)W+[k − 1] + e−j2γW+[k − 2],
k = 2, . . . ,K − 1
a(Δ) = 2 cos
(γω0 +Δ
ω0
).
ΔK
⎡⎣ E1ν0
E1ν+
E1ν−
⎤⎦ = a(Δ)
⎡⎣ E2ν0
E2ν+
E2ν−
⎤⎦+wAR[k],
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E1�=
⎡⎢⎢⎢⎣
e−j2γ 0 1 0 . . . . . . 00 e−j2γ 0 1 0 . . . 0
. . . . . . 00 . . . 0 e−j2γ 0 1
⎤⎥⎥⎥⎦ ,
E2�=
⎡⎢⎢⎢⎣
0 e−jγ 0 . . . 00 0 e−jγ 0 . . . 0
0 . . . . . . 00 . . . 0 e−jγ 0
⎤⎥⎥⎥⎦ .
wAR[k] k = 0, . . . ,K − 1
⎡⎣ T 0 0
0 T 0
0 0 T
⎤⎦ ,
T�= (E1 − a(Δ)E2)R(E1 − a(Δ)E2)
H .a(Δ)
a(Δ) =(νH0 E
H2 T
−1E2ν0
+νH+E
H2 T
−1E2ν+ + ν
H−E
H2 T
−1E2ν−
)−1
×(νH0 E
H2 T
−1E1ν0 + ν
H+E
H2 T
−1E1ν+
+νH−E
H2 T
−1E1ν−
).
a(Δ)T a(Δ)
a(Δ)T
Δ = 0
Δ = ω0/γ cos−1 (a/2)− ω0,
cos−1(·)
N = 48ω0 = 2π · 60
500 K = 8
Δ = 2.5 · 2π=
V 2a+V 2
b+V 2
c
σ2
Va = Vb = 1Vc = βVa ϕa = π
4ϕb = ϕa − 2π
3ϕc = ϕa + 2π
3+ ε
β = 0 ε = 0
C0 C+
C− C(b)0 C
(b)+ C
(b)−
C(b)0
C(b)+
C(b)−
C0
C+
C−
K = 8 N = 48Δ = 2.5× 2π
γΔω0
Δs =ω0
γ
1
K
K−2∑k=0
(V+[k + 1])− (V+[k]) .
3(K − 1)3K
K
γΔ
ω
γ Δω0
K = 8 N = 48 Δ = 2.5 × 2π
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