TY - JOUR
T1 - Design of two‐channel perfect reconstruction QMF
AU - Ikehara, Masaaki
AU - Yamashita, Akinobu
AU - Kuroda, Hideo
PY - 1993
Y1 - 1993
N2 - This paper proposes a design method for the FIR two‐channel perfect quadrature mirror filter (QMF) with the linear phase. The two‐channel perfect QMF can be designed by Vetterli's method, where a system of equations representing the condition for the perfect reconstruction of the signal is solved. The filter designed by this method, however, does not, in general, have good frequency characteristics. This paper presents the design for the two‐channel QMF with a perfect reconstruction and a good amplitude characteristic. The method is based on Vetterli's method, and a constraint to approximate the amplitude characteristic in the frequency domain is added to the condition of perfect reconstruction in time domain. Then Remez' algorithm is applied to the derived system of equations. The construction of the two‐channel perfect QMF, when the coefficient is quantized, also is discussed. Furthermore, a method is shown in which the two‐dimensional (2‐D) perfect QMF is designed by applying the McClellan transformation to the obtained 1‐D QMF. The condition for the McClellan transformation for the perfect reconstruction is derived.
AB - This paper proposes a design method for the FIR two‐channel perfect quadrature mirror filter (QMF) with the linear phase. The two‐channel perfect QMF can be designed by Vetterli's method, where a system of equations representing the condition for the perfect reconstruction of the signal is solved. The filter designed by this method, however, does not, in general, have good frequency characteristics. This paper presents the design for the two‐channel QMF with a perfect reconstruction and a good amplitude characteristic. The method is based on Vetterli's method, and a constraint to approximate the amplitude characteristic in the frequency domain is added to the condition of perfect reconstruction in time domain. Then Remez' algorithm is applied to the derived system of equations. The construction of the two‐channel perfect QMF, when the coefficient is quantized, also is discussed. Furthermore, a method is shown in which the two‐dimensional (2‐D) perfect QMF is designed by applying the McClellan transformation to the obtained 1‐D QMF. The condition for the McClellan transformation for the perfect reconstruction is derived.
KW - 2‐D QMF
KW - Perfect reconstruction
KW - Remez algorithm
KW - coefficient quantization
UR - http://www.scopus.com/inward/record.url?scp=0027596982&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=0027596982&partnerID=8YFLogxK
U2 - 10.1002/ecjc.4430760503
DO - 10.1002/ecjc.4430760503
M3 - Article
AN - SCOPUS:0027596982
SN - 1042-0967
VL - 76
SP - 28
EP - 38
JO - Electronics and Communications in Japan (Part III: Fundamental Electronic Science)
JF - Electronics and Communications in Japan (Part III: Fundamental Electronic Science)
IS - 5
ER -