
 
 
follows. Section 2 gives the basic aspects of DVC 
and CS, section 3 describes the specific example of 
DCVS and proposed parity-based error control (PEC) 
method for DCVS, section 4 discusses the 
simulation results and section 5 is the conclusion 
and future directions of research. 
2 RELATIVE WORKS 
2.1  Distributed Video Coding (DVC) 
In distributed source coding (DSC), assumed that W 
and  S are two statistically dependent discrete 
signals, which are encoded independently but 
decoded jointly. Slepian-Wolf theorem (Wyner et al., 
1976) asserted the achievable rate region for lossless 
coding is defined by Rw≥H(W/S),  Rs≥H(S/W), and 
Rw+Rs≥H(W,S), where Rw and Rs are the encoding 
rates for W and S, respectively, H(W/S) and H(S/W) 
are the conditional entropy of W and S, respectively, 
and H(W,S) is the joint entropy of W and S. 
Additionally, S is known as the side information (SI) 
of W. 
In distributed video coding (DVC) (Girod et al., 
2005), the kinds of frames in a group of pictures 
(GOP) are divided into Key frame and WZ frame 
(Wyner-Ziv frame). The Key frames are intra-coded 
an intra-decoded like I-frame in conventional video 
compression standards. And some information 
derived from Key frame is viewed as side 
information (SI) at decoding end. At encoder, 
without motion estimation, the compression of WZ 
frame is achieved as parity bits (also called Wyner-
Ziv bits) by channel-encoding like turbo coding or 
LDPC coding. Decoder receives the parity bits of 
WZ frame viewed as W, and uses the SI S viewed as 
noisy version of W to perform channel decoding for 
reconstruction of WZ frame. 
2.2  Compressive Sensing (CS) 
In recent years, compressive sensing (CS) (Donoho, 
2006); (Candès, 2006); (Candès and Tao, 2006) 
provides a theory about broadband analog signals 
sampling. The CS as a new research focus gives a 
novel set of theoretical framework about signal 
representation, signal sampling and signal 
reconstruction. It points out that, if the signal x is 
sparse in time domain or sparse in some transform 
basis  Ψ, then we can employ global measurement 
instead of local sampling with sampling speed far 
below the Nyquist frequency, get measurements y 
less than original sampling number through the 
measurement matrix Φ which is not coherent with 
sparse transform basis Ψ. After that, original high-
dimensional signal x can be
  recovered accurately 
with appropriate reconstruction algorithm from low-
dimensional measurements y. Unlike Nyquist 
sampling theory, the sampling rate is not dependent 
on bandwidth of signal,
  but on two basic criteria: 
sparsity and the restricted  isometry property (RIP) 
(Candès and Tao, 2006). Theoretical framework of 
compressive sampling is shown in Figure 1. 
ˆ
 
Figure 1: Compressive sampling framework. 
CS contains the following four steps based on the 
study of theory, shown as Figure 1.  
  Assume that the original N-dimensional signal 
can be sparse on the basis Ψ (N×N), then get the 
sparse signal θ. If the original signal is sparse 
already, skip this step. 
x
Ψ
 
(1)
 
  Devise the measurement matrix Φ  (M×N) to 
acquire measurements y, where A=ΨΦ called the 
sensing matrix. 
 
yx
ΦΦΨ
 
(2)
 
  Solve the problem of minimum l
0
 norm as 
follows known Φ,  Ψ and y, and reconstruct θ 
from measurements y. 
 
0
ˆ
arg min || || s.t. =y
 A
 
(3)
 
  Obtain the original signal 
ˆ
 using the inverse 
transform of basis 
Ψ. 
 
ˆ
ˆ
x
 Ψ
(4)
 
Sparsity, measurement matrix and reconstruction 
algorithm in the above steps are three key parts of 
CS theory. 
Sparse signal in compressive sampling is defined 
as follows: if a signal only has finite number of non-
zero sample point (the number is K), and other 
sample point is zero or similar to zero, this signal is 
claimed as K-sparse and the sparsity is K. Ref 
(Baraniuk, 2007) shows that the original signal may 
be reconstructed accurately in large probability 
under the condition that the relation between 
measurements  M and sparsity K should  satisfies 
M≥K·log(N), in other words, the signal recovery 
quality will be affected quitely if the measurements 
M is less than a certain number. 
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