Abstract:
Provided is an audio encoding device that can suppress degradation of audio quality. Spectral coefficients of synthesized signal from CELP core layer are utilized to fulfill spectral gaps in error signal spectrum coefficients from a transform coding layer. By both spectral coefficients, decoded signal spectral coefficients are generated. The decoded signal spectral coefficients and the input signal spectral coefficients are divided into a plurality of sub bands. In each sub band, the energy of the input signal spectral coefficient corresponding to a zero decoded error signal spectral coefficient is calculated, and the energy of the decoded signal spectral coefficient corresponding to the zero decoding error signal spectral coefficient is calculated, and their energy ratio is calculated and is quantized and transmitted.

Description:
TECHNICAL FIELD 
       [0001]    The present invention relates to an audio coding apparatus and an audio decoding apparatus, and, for example, to an audio coding apparatus and audio decoding apparatus that employ hierarchical coding (code-excited linear prediction (CELP) and transform coding). 
       BACKGROUND ART 
       [0002]    With respect to audio coding, there are two main types of coding schemes, namely transform coding and linear prediction coding. 
         [0003]    Transform coding involves a signal conversion from the time domain to the frequency domain, as in discrete Fourier transform (DFT), modified discrete cosine transform (MDCT), and/or the like. Spectral coefficients derived through signal conversion are quantized and coded. In the process of quantization or coding, the psychoacoustic model is ordinarily applied to determine the perceptual significances of the spectral coefficients, and the spectral coefficients are quantized or coded in accordance with their perceptual significances. MPEG MP3, MPEG, AAC (see Non-Patent Literature 1), Dolby AC3, and the like, are used widely for transform coding (transform codecs). Transform coding is effective for music, as well as audio signals in general. A simple configuration of a transform codec is shown in  FIG. 1 . 
         [0004]    With respect to the encoder shown in  FIG. 1 , time domain signal S(n) is converted into frequency domain signal S(f) using a method of converting ( 101 ) from the time domain to the frequency domain, such as discrete Fourier transform (DFT), modified discrete cosine transform (MDCT), and/or the like. 
         [0005]    A psychoacoustic model analysis is performed on frequency domain signal S(f), and a masking curve is derived ( 103 ). Frequency domain signal S(f) is quantized ( 102 ) in accordance with the masking curve derived through the psychoacoustic model analysis, thereby making quantization noise inaudible. 
         [0006]    A quantized parameter is multiplexed ( 104 ) and sent to the decoder side. 
         [0007]    With respect to the decoder shown in  FIG. 1 , all bit stream information is first demultiplexed ( 105 ). The quantized parameter is dequantized, and decoded spectral coefficient S˜(f) is reconfigured ( 106 ). 
         [0008]    Decoded spectral coefficient S˜(f) is converted back to the time domain using a method of converting ( 107 ) from the frequency domain to the time domain, such as inverse discrete Fourier transform (IDFT), inverse modified discrete cosine transform (IMDCT), and/or the like, and decoded signal S˜(n) is reconfigured. 
         [0009]    On the other hand, linear predictive coding derives a residual signal (excitation signal) by applying linear prediction to an input audio signal, making use of the predictability of audio signals in the time domain. For vocal regions having similarity with respect to time shifts based on pitch period, this modeling procedure is an extremely efficient expression. Subsequent to linear prediction, the residual signal is typically coded through two types of methods, namely TCX and CELP. 
         [0010]    With respect to TCX (see Non-Patent Literature 2), the residual signal is converted to the frequency domain, and coding is performed. One widely used TCX codec is 3GPP AMR-WB+. A simple configuration of a TCX codec is shown in  FIG. 2 . 
         [0011]    With respect to the encoder shown in  FIG. 2 , an LPC analysis is performed on the input signal ( 201 ). The LPC coefficient determined at the LPC analysis section is quantized ( 202 ), and a quantized parameter is multiplexed ( 207 ) and sent to the decoder side. Residual signal S r (n) is derived by applying LPC inverse filtering ( 204 ) to input signal S(n) using a dequantized LPC coefficient obtained at dequantization section ( 203 ). 
         [0012]    Residual signal S r (n) is converted into residual signal spectral coefficient S r (f) ( 205 ) using a method of converting from the time domain to the frequency domain, such as discrete Fourier transform (DFT), modified discrete cosine transform (MDCT), and/or the like. 
         [0013]    Residual signal spectral coefficient S r (f) is quantized ( 206 ), and a quantized parameter is multiplexed ( 207 ) and sent to the decoder side. 
         [0014]    With respect to the decoder shown in  FIG. 2 , all bit stream information is first demultiplexed ( 208 ). 
         [0015]    The quantized parameter is dequantized, and decoded residual signal spectral coefficient S r ˜(f) is reconfigured ( 210 ). 
         [0016]    Decoded residual signal spectral coefficient S r ˜(f) is converted back to the time domain using a method of converting ( 211 ) from the frequency domain to the time domain, such as inverse discrete Fourier transform (IDFT), inverse modified discrete cosine transform (IMDCT), and/or the like, and decoded residual signal S r ˜(n) is reconfigured. 
         [0017]    Based on the dequantized LPC parameter from dequantization section ( 209 ), decoded residual signal S r ˜(n) is processed with LPC synthesis filter ( 212 ) to obtain decoded signal S˜(n). 
         [0018]    In CELP coding, the residual signal is quantized using a predetermined codebook. In order to further enhance the sound quality, the difference signal between the original signal and the LPC synthesis signal is typically converted to the frequency domain and further encoded. Examples of coding of such a configuration include ITU-T G.729.1 (see Non-Patent Literature 3) and ITU-T G.718 (see Non-Patent Literature 4). A simple configuration of hierarchical coding (embedded coding), which uses CELP at its core section, and transform coding is shown in  FIG. 3 . 
         [0019]    With respect to the encoder shown in  FIG. 3 , CELP coding, which makes use of predictability in the time domain, is executed ( 301 ) on the input signal. Based on CELP coded parameters, a synthesized signal is reconfigured ( 302 ) by a local CELP decoder. By subtracting the synthesized signal from the input signal, error signal S e (n) (the difference signal between the input signal and the synthesized signal) is obtained. 
         [0020]    Error signal S e (n) is converted into error signal spectral coefficient S e (f) through a method of converting ( 303 ) from the time domain to the frequency domain, such as discrete Fourier transform (DFT), modified discrete cosine transform (MDCT), and/or the like. 
         [0021]    S e (f) is quantized ( 304 ), and a quantized parameter is multiplexed ( 305 ) and sent to the decoder side. 
         [0022]    With respect to the decoder shown in  FIG. 3 , all bit stream information is first demultiplexed ( 306 ). 
         [0023]    The quantized parameter is dequantized, and decoded error signal spectral coefficient S e ˜(f) is reconfigured ( 308 ). 
         [0024]    Decoded error signal spectral coefficient S e ˜(f) is converted back to the time domain using a method of converting ( 309 ) from the frequency domain to the time domain, such as inverse discrete Fourier transform (IDFT), inverse modified discrete cosine transform (IMDCT), and/or the like, and decoded error signal S e ˜(n) is reconfigured. 
         [0025]    Based on CELP coded parameters, the CELP decoder reconfigures synthesized signal S syn (n) ( 307 ), and reconfigures decoded signal S˜(n) by adding CELP synthesized signal S syn (n) and decoded error signal S e ˜(n). 
         [0026]    Transform coding is ordinarily carried out using vector quantization. 
         [0027]    Due to bit constraints, it is usually impossible to finely quantize all spectral coefficients. Spectral coefficients are often loosely quantized, where only a portion of the spectral coefficients are quantized. 
         [0028]    By way of example, there are several types of vector quantization methods used in G.718 for spectral coefficient quantization, multi-rate lattice VQ (SMLVQ) (see Non-Patent Literature 5), Factorial Pulse Coding (FPC), and Band Selective-Shape Gain Coding (BS-SGC). Each vector quantization method is used in one of the transform coding layers. Due to bit constraints, only several of the spectral coefficients are selected and quantized at each layer. 
       CITATION LIST 
     Non-Patent Literature 
       [0000]    
       
         NPL 1 
         Karl Heinz Brandenburg, “MP3 and AAC Explained”, AES 17 th  International Conference, Florence, Italy, September 1999. 
         NPL 2 
         Lefebvre, et al., “High quality coding of wideband audio signals using transform coded excitation (TCX)”, IEEE International Conference on Acoustics, Speech, and Signal Processing, vol. 1, pp. I/193-I/196, April 1994 
         NPL 3 
         ITU-T Recommendation G.729.1 (2007) “G.729-based embedded variable bit-rate coder: An 8-32 kbit/s scalable wideband coder bitstream interoperable with G.729” 
         NPL 4 
         T. Vaillancourt et al, “ITU-T EV-VBR: A Robust 8-32 kbit/s Scalable Coder for Error Prone Telecommunication Channels”, in Proc. Eusipco, Lausanne, Switzerland, August 2008 
         NPL 5 
         M. Xie and J.-P. Adoul, “Embedded algebraic vector quantization (EAVQ) with application to wideband audio coding,” IEEE International Conference on Acoustics, Speech, and Signal Processing (ICASSP), Atlanta, Ga., U.S.A, 1996, vol. 1, pp. 240-243 
       
     
       SUMMARY OF INVENTION 
     Technical Problem 
       [0039]    As shown in  FIG. 4 , in hierarchical coding, the input signal is processed through CELP and transform coding. Vector quantization is employed as a means of transform coding. 
         [0040]    When the number of usable bits is limited, it may not always be possible to quantize all spectral coefficients in the transform coding layers, thus resulting in numerous zero spectral coefficients in the decoded spectral coefficients. Under more adverse conditions, a spectral gap occurs in the decoded spectral coefficients. 
         [0041]    Due to the spectral gap in the decoded signal spectral coefficients, the decoded signal is perceived as a dull and muffled sound. In other words, the sound quality drops. 
         [0042]    An object of the present invention is to provide an audio coding apparatus and audio decoding apparatus that are capable of mitigating sound quality degradation. 
       Solution to Problem 
       [0043]    With the present invention, a spectral gap caused by loose quantization is closed. 
         [0044]    As shown in  FIG. 5 , with the present invention, spectral envelope shaping is performed with respect to synthesized signal spectral coefficients from the CELP core layer, and the shaped synthesized signal is used to close (fill) spectral gaps of transform coding layers. 
         [0045]    Details of a spectral envelope shaping process are presented below. 
         [0046]    First, a process of an audio coding apparatus will be presented. (1) Decoded error signal spectral coefficient S e ˜(f) of the transform coding layer is reconfigured. (2) Decoded signal spectral coefficient S˜(f) is reconfigured by adding synthesized signal spectral coefficient S syn (f) from the CELP core layer and decoded error signal spectral coefficient S e ˜(f), such as that given by the equation below, from the transform coding layer. 
         [0000]      [1] 
         [0000]        {tilde over (S)} ( f )= {tilde over (S)}   e ( f )+ S   syn ( f )  (Equation 1)
 
         [0000]    where {tilde over (S)} e (f) is the decoded error signal spectral coefficient, S syn (f) is the synthesized signal spectral coefficient from the CELP core layer, and {tilde over (S)}(f) is the decoded signal spectral coefficient. 
         [0047]    (3) Decoded signal spectral coefficient S˜(f) and input signal spectral coefficient S(f) are both divided into a plurality of subbands. (4) For each subband, the energy of input signal spectral coefficient S(f) corresponding to zero decoded error signal spectral coefficient S e ˜(f) is calculated as indicated by the equation below. The term “zero decoded error signal spectral coefficient” refers to a decoded error signal spectral coefficient whose spectral coefficient value is zero. 
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         [0000]    where E org     —     i  is the energy of the input signal spectral coefficient corresponding to the zero decoded error signal spectral coefficient in subband i, sb_start[i] is the minimum frequency of subband i, sb_end[ i ] is the maximum frequency of subband i, S(f) is the input signal spectral coefficient, and {tilde over (S)} e (f) is the decoded error signal spectral coefficient. 
         [0048]    (5) For each subband, the energy of decoded signal spectral coefficient S˜(f) corresponding to zero decoded error signal spectral coefficient S e ˜(f) is calculated as indicated by the equation below. 
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         [0000]    where E dec     —     i  is the energy of the decoded spectral coefficient corresponding to the zero decoded error signal spectral coefficient in subband i, sb_start[i] is the minimum frequency of subband i, sb_end[ i] is the maximum frequency of subband i, {tilde over (S)}(f) is the decoded signal spectrum, and {tilde over (S)}S   e (f) is the decoded error signal spectrum. 
         [0049]    (6) For each band, an energy ratio such as that given by the equation below is determined. 
         [0000]      [4] 
         [0000]        G   i   =E   org     —     i   /E   dec     —     i   (Equation 4)
 
         [0000]    where E org     —     i  is the energy of the input signal spectral coefficient corresponding to the zero decoded error signal spectral coefficient in subband i, E dec     —     i  is the energy of the decoded spectral coefficient corresponding to the zero decoded error signal spectral coefficient in subband i, and G i  is the energy ratio of the above-mentioned two energies with respect to subband i. 
         [0050]    (7) The energy ratio is quantized and sent to the audio decoding apparatus side. 
         [0051]    Next, a process of an audio decoding apparatus will be presented. (1) The energy ratio is dequantized. (2) The synthesized signal spectral coefficient from the CELP core layer is shaped in accordance with a spectral envelope shaping parameter derived from the decoded energy ratio. (3) The spectral-envelope-shaped spectrum is used to close the spectral gap of the transform coding layer as indicated in the equation below. 
         [0000]      [5] 
         [0000]      if  {tilde over (S)}   e ( f )=0, 
         [0000]        {tilde over (S)}   e ( f )= S   syn ( f )*(√{square root over ( {tilde over (G)}   i )}−1)
 
         [0000]        fε[sb _start[ i],sb _end[ i]]   (Equation 5)
 
         [0000]    where {tilde over (S)} e (f) is the decoded error spectral coefficient, S syn (f) is the synthesized signal spectral coefficient from the CELP core layer, and {tilde over (S)}(f) is the decoded signal spectral coefficient, {tilde over (G)} i  is the decoded energy ratio with respect to subband i, sb_start[i] is the minimum frequency of subband i, and sb_end[ i] is the maximum frequency of subband i.    
       Advantageous Effects of Invention 
       [0052]    With the present invention, by closing the spectral gap in the spectrum, dull and muffled sounds in the decoded signal may be prevented, thereby mitigating sound quality degradation. 
     
    
     
       BRIEF DESCRIPTION OF DRAWINGS 
         [0053]      FIG. 1  is a diagram showing a simple configuration of a transform codec; 
           [0054]      FIG. 2  is a diagram showing a simple configuration of a TCX codec; 
           [0055]      FIG. 3  is a diagram showing a simple configuration of a hierarchical codec (CELP and transform coding); 
           [0056]      FIG. 4  is a diagram showing a problem with hierarchical codecs (CELP and transform coding); 
           [0057]      FIG. 5  is a diagram showing a solution to a problem of the present invention; 
           [0058]      FIG. 6  is a diagram showing a configuration of an audio coding apparatus according to Embodiment 1 of the present invention; 
           [0059]      FIG. 7  is a diagram showing a configuration of a spectral envelope extraction section according to Embodiment 1 of the present invention; 
           [0060]      FIG. 8  is a diagram showing a configuration of a spectrum division method according to Embodiment 1 of the present invention; 
           [0061]      FIG. 9  is a diagram showing a configuration of an audio decoding apparatus according to Embodiment 1 of the present invention; 
           [0062]      FIG. 10  is a diagram showing a configuration of a spectral envelope shaping section according to Embodiment 1 of the present invention; 
           [0063]      FIG. 11  is a diagram showing a configuration of a spectral envelope extraction section according to Embodiment 2 of the present invention; 
           [0064]      FIG. 12  is a diagram showing a configuration of a spectral envelope shaping section according to Embodiment 2 of the present invention; 
           [0065]      FIG. 13  is a diagram showing a configuration of a spectral envelope extraction section according to Embodiment 3 of the present invention; 
           [0066]      FIG. 14  is a diagram showing a configuration of a spectral envelope extraction section according to Embodiment 4 of the present invention; and 
           [0067]      FIG. 15  is a diagram showing a configuration of a spectral envelope shaping section according to Embodiment 4 of the present invention. 
       
    
    
     DESCRIPTION OF EMBODIMENTS 
       [0068]    Embodiments of the present invention are described in detail below with reference to the drawings. With respect to the various embodiments, like elements are designated with like numerals, while omitting redundant descriptions thereof. 
       Embodiment 1 
       [0069]      FIG. 6  is a diagram showing a configuration of an audio coding apparatus according to the present embodiment.  FIG. 9  is a diagram showing a configuration of an audio decoding apparatus according to the present embodiment.  FIG. 6  and  FIG. 9  depict cases where the present invention is applied to hierarchical coding (hierarchical coding, embedded coding) of CELP and transform coding. 
         [0070]    With respect to the audio coding apparatus shown in  FIG. 6 , CELP coding section  601  performs coding making use of signal predictability in the time domain. 
         [0071]    CELP local decoding section  602  reconfigures a synthesized signal using a CELP coded parameter. Multiplexing section  609  multiplexes the CELP coded parameter, and sends it to an audio decoding apparatus. 
         [0072]    Subtractor  610  derives error signal S e (n) (the difference signal between the input signal and the synthesized signal) by subtracting the synthesized signal from the input signal. 
         [0073]    T/F transform sections  603  and  604  convert the synthesized signal and error signal S e (n) into a synthesized signal spectral coefficient and error signal spectral coefficient S e (f) using a method of converting from the time domain to the frequency domain, e.g., discrete Fourier transform (DFT), modified discrete cosine transform (MDCT), and/or the like. 
         [0074]    Vector quantization section  605  carries out vector quantization on error signal spectral coefficient S e (f), and generates a vector quantized parameter. 
         [0075]    Multiplexing section  609  multiplexes the vector quantized parameter and sends it to the audio decoding apparatus. 
         [0076]    At the same time, vector dequantization section  606  dequantizes the vector quantized parameter, and reconfigures decoded error signal spectral coefficient S e ˜(f). 
         [0077]    Spectral envelope extraction section  607  extracts spectral envelope shaping parameter {G i } from the synthesized signal spectral coefficient, the error signal spectral coefficient, and the decoded error signal spectral coefficient. 
         [0078]    Quantization section  608  quantizes spectral envelope shaping parameter {G i }. Multiplexing section  609  multiplexes the quantized parameter, and sends it to the audio decoding apparatus. 
         [0079]      FIG. 7  shows details of spectral envelope extraction section  607 . 
         [0080]    As shown in  FIG. 7 , the input to spectral envelope extraction section  607  includes synthesized signal spectral coefficient S syn (f), error signal spectral coefficient S e (f), and decoded error signal spectral coefficient S e ˜(f). The output includes spectral envelope shaping parameter {G i }. 
         [0081]    First, adder  708  adds synthesized signal spectral coefficient S syn (f) and error signal spectral coefficient S e (f) to form input signal spectral coefficient S(f). Adder  707  adds synthesized signal spectral coefficient S syn (f) and decoded error signal spectral coefficient S e ˜(f) to form decoded signal spectral coefficient S˜(f). 
         [0082]    Next, band division sections  702  and  701  divide input signal spectral coefficient S(f) and decoded signal spectral coefficient S˜(f) into a plurality of subbands. 
         [0083]    Next, spectral coefficient division sections  704  and  703  reference the decoded error signal spectral coefficient, and classify each of the input signal spectral coefficient and the decoded signal spectral coefficient into two classes. First, the input signal spectral coefficient will be described. With respect to each subband, spectral coefficient division section  704  performs classification according to two types, where an input signal spectral coefficient corresponding to a band for which the decoded signal spectral coefficient value is zero is classified as a zero input signal spectral coefficient, and where an input signal spectral coefficient corresponding to a band for which the decoded signal spectral coefficient value is not zero is classified as a non-zero input signal spectral coefficient. Spectral coefficient division section  703  applies to the decoded signal spectral coefficient a similar classification based on the decoded error signal spectral coefficient to determine a zero decoded error signal spectral coefficient and a non-zero decoded signal spectral coefficient. 
         [0084]    As shown in  FIG. 8 , spectral coefficient division section  704  divides the ith subband into a band for which the decoded error spectral coefficient value is zero (the zero decoded error signal spectral coefficient) and a band for which the decoded error spectral coefficient value is no zero (the non-zero decoded error signal spectral coefficient). In a manner corresponding to zero decoded error signal spectral coefficient S″ ei ˜(f) and non-zero decoded error signal spectral coefficient S′ ei ˜(f), input signal spectral coefficient S i (f) of the ith subband is so classified that a spectral coefficient included in the band where zero decoded error signal spectral coefficient S″ ei ˜(f) is located is classified as zero input signal spectral coefficient S″ i (f), while a spectral coefficient included in the band where non-zero decoded error signal spectral coefficient S′ ei ˜(f) is located is classified as non-zero input signal spectral coefficient S′ i (f). Similarly, in a manner corresponding to zero decoded error signal spectral coefficient S″ ei ˜(f) and non-zero decoded error signal spectral coefficient S′ ei ˜(f), spectral coefficient division section  703  classifies decoded signal spectral coefficient S i ˜(f) of the ith subband into zero decoded signal spectral coefficient S″ i ˜(f) and non-zero decoded signal spectral coefficient S′ i ˜(f). 
         [0085]    Subband energy computation sections  706  and  705  calculate energy for each subband with respect to zero input signal spectral coefficient S″ i (f) and zero decoded signal spectral coefficient S″ i ˜(f). Energy is calculated in the manner indicated by the equation below. 
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         [0000]    where E″ org     —     i  is the energy of the zero input signal spectral coefficients in subband i, S″ i (f) is the zero input signal spectral coefficient in subband i, and N zero [i] is the number of zero input signal spectral coefficients in subband i. 
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         [0000]    where E″ dec     —     i  is the energy of the zero decoded signal spectral coefficients in subband i, {tilde over (S)}″ i (f) is the zero decoded signal spectral coefficient in subband i, and N zero [i] is the number of zero decoded signal spectral coefficients in subband i. 
         [0086]    The ratio between the above-mentioned two energies is calculated as follows. 
         [0000]      [8] 
         [0000]        G   i   =E″   org     —     i   /E″   dec     —     i   (Equation 8)
 
         [0000]    where E″ org     —     i  is the energy of the zero input signal spectral coefficients in subband i, E″ dec     —     i  is the energy of the zero decoded signal spectral coefficients in subband i, and G i  is the energy ratio between the above-mentioned two energies with respect to subband i. 
         [0087]    This {G i } is outputted as a spectral envelope shaping parameter from divider  707 . 
         [0088]    With respect to the audio decoding apparatus shown in  FIG. 9 , demultiplexing section  901  first demultiplexes all bit stream information, generates a CELP coded parameter, a vector quantized parameter, and a quantized parameter, and outputs them to CELP decoding section  902 , vector dequantization section  904 , and dequantization section  905 , respectively. 
         [0089]    By means of the CELP coded parameter, CELP decoding section  902  reconfigures synthesized signal S syn (n). 
         [0090]    T/F transform section  903  converts synthesized signal S syn (n) into decoded signal spectral coefficient S syn (f) using a method of converting from the time domain to the frequency domain, e.g., discrete Fourier transform (DFT), modified discrete cosine transform (MDCT), and/or the like. 
         [0091]    Vector dequantization section  904  dequantizes the vector quantized parameter, and reconfigures decoded error signal spectral coefficient S e ˜(f). 
         [0092]    Dequantization section  905  dequantizes the quantized parameter intended for the spectral envelope shaping parameter, and reconfigures decoded spectral envelope shaping parameter {G i ˜}. 
         [0093]    Spectral envelope shaping section  906  closes the spectral gap of the decoded error signal spectral coefficient by means of decoded spectral envelope shaping parameter {G i ˜}, synthesized signal spectral coefficient S syn (f), and decoded error signal spectral coefficient S e ˜(f) to generate post-processing error signal spectral coefficient S post-e ˜(f). 
         [0094]    F/T transform section  907  transforms post-processing error signal spectral coefficient S post-e ˜(f) back to the time domain, and reconfigures decoded error signal S e ˜(n) using a method of converting from the frequency domain to the time domain, such as inverse discrete Fourier transform (IDFT), inverse modified discrete cosine transform (IMDCT), and/or the like. 
         [0095]    Adder  908  reconfigures decoded signal S˜(n) by adding synthesized signal S syn (n) and decoded error signal S e ˜(n). 
         [0096]      FIG. 10  shows details of spectral envelope shaping section  906 . 
         [0097]    As shown in  FIG. 10 , the input to spectral envelope shaping section  906  includes decoded spectral envelope shaping parameter {G i ˜} synthesized signal spectral coefficient S syn (f), and decoded error signal spectral coefficient S e ˜(f). The output includes post-processing error signal spectral coefficient S post-e ˜(f). 
         [0098]    Band division section  1001  divides synthesized signal spectral coefficient S syn (f) into a plurality of subbands. 
         [0099]    Next, as shown in  FIG. 8 , spectral coefficient division section  1002  references the decoded error signal spectral coefficient, and classifies synthesized signal spectral coefficients into two classes. Specifically, with respect to each subband, spectral coefficient division section  1002  performs classification according to two types, such that a synthesized signal spectral coefficient corresponding to a band for which the decoded error signal spectral coefficient value is zero is classified as zero synthesized signal spectral coefficient S″ syn     —     i (f), and that a synthesized signal spectral coefficient corresponding to a band for which the decoded error signal spectral coefficient value is not zero is classified as non-zero synthesized signal spectral coefficient S′ syn     —     i (f). 
         [0100]    Spectral envelope shaping parameter generation section  1003  processes decoded spectral envelope shaping parameter G i ˜, and calculates an appropriate spectral envelope shaping parameter. One such method is presented through the equation below. 
         [0000]      [9] 
         [0000]        P   i √{square root over ({tilde over (G)} i )}−1  (Equation 9)
 
         [0000]    where P i  is the derived spectral envelope shaping parameter, and {tilde over (G)} is the decoded spectral envelope shaping parameter of the ith subband. 
         [0101]    Then, as indicated by the following equations, the synthesized signal spectral coefficients from the CELP layer are shaped by multiplier  1004  in accordance with the spectral envelope shaping parameter, and a post-processing error signal spectrum is generated by adder  1005 . 
         [0000]      [10] 
         [0000]      if  {tilde over (S)}   e ( f )=0, 
         [0000]        {tilde over (S)}   post     —     e ( f )= S   syn ( f )* P   i   (Equation 10)
 
         [0000]      [11] 
         [0000]      if  {tilde over (S)}   e ( f )!=0, 
         [0000]        {tilde over (S)}   post     —     e ( f )= {tilde over (S)}   e ( f ) 
         [0000]        fε[sb _start[ i],sb _end[ i]]   (Equation 11)
 
         [0000]    where {tilde over (S)} e (f) is the decoded error signal spectral coefficient, S syn (f) is the synthesized signal spectral coefficient from the CELP layer, {tilde over (S)}(f) is the decoded signal spectral coefficient, P i  is the derived spectral envelope shaping parameter, {tilde over (S)}S post     —     e (f) is the post-processing error signal spectral coefficient, sb_start[i] is the minimum frequency of the ith subband, and sb_end[ i] is the maximum frequency of the ith subband.    
         [0102]    &lt;Variation&gt; 
         [0103]    With respect to the coding section, after at least one of the zero input signal spectral coefficient and the zero decoded signal spectral coefficient has been classified, and, with respect to the decoding section, after the zero synthesized signal spectral coefficient has been classified, band division may be performed taking these classification results into account. This enables subbands to be determined efficiently. 
         [0104]    The present invention may be applied to a configuration where the number of bits available for spectral envelope shaping parameter quantization is variable from frame to frame. By way of example, this may include cases where a variable bit rate coding scheme, or a scheme in which the number of bits quantized at vector quantization section  605  in  FIG. 6  varies from frame to frame, is used. In such cases, band division may be performed in accordance with the magnitude of the bit count available for spectral envelope shaping parameter quantization. By way of example, if a large number of bits are available, more spectral envelope shaping parameters may be quantized (i.e., a greater resolution may be achieved) by performing band division into a greater number of subbands. Conversely, if few bits are available, fewer spectral envelope shaping parameters are quantized (i.e., a lesser resolution is achieved) by performing band division into fewer subbands. By thus adaptively varying the number of subbands in accordance with the number of available bits, it becomes possible to quantize spectral envelope shaping parameters in numbers commensurate with the number of bits available, and to improve sound quality. 
         [0105]    In quantizing spectral envelope shaping parameters, quantization may be performed in order from the higher frequency bands to the lower frequency bands. The reason being that, with respect to low frequency bands, CELP is able to code audio signals extremely efficiently through linear prediction modeling. Accordingly, when employing CELP in the core layer, it is perceptually more important to close the spectral gap of the high frequency bands. 
         [0106]    If the number of bits available for spectral envelope shaping parameter quantization falls short, a spectral envelope shaping parameter having a large Gi value (G i &gt;1) or small Gi value (G i &lt;1) may be selected, and sent to the decoder side with quantization being performed only on the selected spectral envelope shaping parameter. In other words, what this signifies is that spectral envelope shaping parameters are quantized only with respect to subbands for which there is a large difference between the energy of the zero input signal spectral coefficients and the energy of the zero decoded signal spectral coefficients. Since this means that information of subbands that result in greater perceptual improvement will be selected and quantized, sound quality may be improved. In the case above, a flag indicating the subband of the selected energy is sent. 
         [0107]    In quantizing spectral envelope shaping parameters, quantization may be performed with a bound provided so that the spectral envelope shaping parameter decoded after quantization does not exceed the value of the spectral envelope shaping parameter subject to quantization. Consequently, the post-processing error signal spectral coefficient that closes the spectral gap may be prevented from becoming unnecessarily large, and sound quality may be improved. 
       Embodiment 2 
       [0108]    In the case of a configuration where coding is performed at a low bit rate, coding accuracy is sometimes insufficient even for bands where there is no spectral gap (i.e., bands coded at a transform coding layer), resulting in a large coding error relative to the input signal spectral coefficient. Under such conditions, it is possible to improve sound quality by applying spectral envelope shaping to bands where there is no spectral gap, just like it is applied to bands where there is a spectral gap. Furthermore, in this case, greater sound quality improving effects are attained when spectral envelope shaping is carried out with respect to bands in which there is no spectral gap, separately from bands in which there is a spectral gap. 
         [0109]    A configuration of a spectral envelope extraction section according to the present embodiment is shown in  FIG. 11 . It differs from  FIG. 7  in that subband energy computation sections  1108  and  1107  perform energy computations also with respect to non-zero input signal spectral coefficients and non-zero decoded signal spectral coefficients, and in that divider  1009  also outputs, as a spectral envelope shaping parameter, the energy ratio computed here. 
         [0110]    A configuration of a spectral envelope shaping section of the present embodiment is shown in  FIG. 12 . It differs from  FIG. 10  in that a spectral envelope shaping parameter for a band in which there is no spectral gap is also decoded, and in that this is also used to generate a post-processing error signal spectral coefficient. 
         [0111]    As shown in  FIG. 12 , spectral envelope shaping parameter generation section  1203  processes decoded spectral envelope shaping parameter G′ i ˜ intended for a band in which there is no spectral gap, and calculates an appropriate shaping parameter. One such method is presented through the equation below. 
         [0000]    [12] 
         [0000]        P′   i   =√{square root over ({tilde over (G)}′   i −1  (Equation 12)
 
         [0000]    where P′ i  is the derived spectral envelope shaping parameter, and {tilde over (G)}′ i  is the spectral envelope shaping parameter of the ith subband. 
         [0112]    Adder  1204  adds the synthesized signal spectral coefficient and the decoded error signal spectral coefficient to form the decoded signal spectral coefficient as indicated by the equation below. 
         [0000]      [13] 
         [0000]        {tilde over (S)} ( f )= {tilde over (S)}   e ( f ) S   syn ( f )  (Equation 13)
 
         [0000]    where {tilde over (S)} e (f) is the decoded error spectral coefficient, {tilde over (S)}(f) is the decoded signal spectral coefficient, and S syn (f) is the synthesized signal spectral coefficient from the CELP layer. 
         [0113]    As indicated by the following equations, by means of band division section  1001 , spectral coefficient division section  1002 , multipliers  1004 - 1  and  1004 - 2 , and adders  1005 - 1  and  1005 - 2 , the decoded signal spectral coefficients is shaped for each subband in accordance with the spectral envelope shaping parameter to generate the post-processing error signal spectrum. 
         [0000]      [14] 
         [0000]      if  {tilde over (S)}   e ( f )=0, 
         [0000]        {tilde over (S)}   post     —     e ( f )= {tilde over (S)} ( f )* P   i   (Equation 14)
 
         [0000]      if  {tilde over (S)}   e ( f )!=0, 
         [0000]        {tilde over (S)}   post     —     e ( f )= {tilde over (S)}   e ( f )+ {tilde over (S)} ( f )* P′   i    
         [0000]        fε[sb _start[ i],sb _end[ i]]   (Equation 15)
 
         [0000]    where {tilde over (S)} e (f) is the decoded error signal spectral coefficient, {tilde over (S)}(f) is the decoded signal spectral coefficient, P i  is the spectral envelope shaping parameter for a band in which there is a spectral gap, P′ i  is the spectral envelope shaping parameter for a band in which there is no spectral gap, {tilde over (S)} post     —     e (f) is the post-processing error signal spectral coefficient, sb_start[i] is the minimum frequency of the ith subband, and sb_end[ i] is the maximum frequency of the ith subband.    
         [0114]    &lt;Variation&gt; 
         [0115]    In the case of a low-bit-rate configuration, a spectral envelope shaping parameter to be used across all bands in which there is no spectral gap may be sent with respect to all bands. The spectral envelope shaping parameter in this case may be calculated as indicated by the equation below. 
         [0000]    
       
         
           
             
               
                 
                   ( 
                   
                     Equation 
                      
                     
                         
                     
                      
                     16 
                   
                   ) 
                 
               
               
                 
                     
                 
               
             
             
               
                 
                   
                     G 
                     ′ 
                   
                   = 
                   
                     
                       
                         ∑ 
                         
                           i 
                           = 
                           0 
                         
                         
                           
                             N 
                             sb 
                           
                           - 
                           1 
                         
                       
                        
                       
                           
                       
                        
                       
                         E 
                         
                           org 
                            
                           _ 
                            
                           i 
                         
                         ′ 
                       
                     
                     
                       
                         ∑ 
                         
                           i 
                           = 
                           0 
                         
                         
                           
                             N 
                             sb 
                           
                           - 
                           1 
                         
                       
                        
                       
                           
                       
                        
                       
                         E 
                         
                           dec 
                            
                           _ 
                            
                           i 
                         
                         ′ 
                       
                     
                   
                 
               
               
                 
                   [ 
                   16 
                   ] 
                 
               
             
           
         
       
     
         [0000]    where E′ org     —     i  is the energy of the non-zero input signal spectral coefficient in the ith subband, E′ dec     —     i  is the energy of the non-zero decoded signal spectral coefficient in the ith subband, and G′ is the energy ratio of the above-mentioned two energies with respect to the entire band (spectral envelope shaping parameter). 
         [0116]    At the audio decoding apparatus, the spectral envelope shaping parameter is used as indicated by the equation below. 
         [0000]      [17] 
         [0000]        P′i=√{square root over ({tilde over (G)}′− 1  (Equation 17)
 
         [0000]    where P′ i  is the derived spectral envelope shaping parameter, and {tilde over (G)}′ is the decoded spectral envelope shaping parameter for the non-zero synthesized signal spectral coefficient. 
       Embodiment 3 
       [0117]    One important factor in maintaining the sound quality of the input signal is to maintain an energy balance between different frequency bands. Accordingly, it is extremely important that the energy balance between a band that has a spectral gap in the decoded signal and a band that does not be maintained so as to resemble the input signal. What follows is a description of an embodiment capable of maintaining the energy balance between a band that has a spectral gap and a band that does not. 
         [0118]      FIG. 13  is a diagram showing a configuration of a spectral envelope extraction section according to the present embodiment. As shown in  FIG. 13 , full band energy computation sections  1308  and  1307  calculate energy E′ org  of the non-zero input signal spectral coefficients and energy E′ dec  of the non-zero decoded signal spectral coefficients. The equations below represent an example energy calculation method. 
         [0000]    
       
         
           
             
               
                 
                   ( 
                   
                     Equation 
                      
                     
                         
                     
                      
                     18 
                   
                   ) 
                 
               
               
                 
                     
                 
               
             
             
               
                 
                   
                     E 
                     org 
                     ′ 
                   
                   = 
                   
                     
                       ∑ 
                       
                         i 
                         = 
                         0 
                       
                       
                         
                           N 
                           sb 
                         
                         - 
                         1 
                       
                     
                      
                     
                         
                     
                      
                     
                       
                         ∑ 
                         
                           f 
                           = 
                           0 
                         
                         
                           
                             
                               N 
                               nonzero 
                             
                              
                             
                               [ 
                               i 
                               ] 
                             
                           
                           - 
                           1 
                         
                       
                        
                       
                           
                       
                        
                       
                         
                           
                             S 
                             i 
                             ′ 
                           
                            
                           
                             ( 
                             f 
                             ) 
                           
                         
                         2 
                       
                     
                   
                 
               
               
                 
                   [ 
                   18 
                   ] 
                 
               
             
           
         
       
     
         [0000]    where E′ org  is the energy of the non-zero input signal spectral coefficients with respect to all subbands, S′ i (f) is the non-zero input signal spectral coefficient with respect to the ith subband, N sb  is the total number of subbands, and N nonzero [i] is the number of non-zero decoded signal spectral coefficients with respect to the ith subband. 
         [0000]    
       
         
           
             
               
                 
                   ( 
                   
                     Equation 
                      
                     
                         
                     
                      
                     19 
                   
                   ) 
                 
               
               
                 
                     
                 
               
             
             
               
                 
                   
                     E 
                     dec 
                     ′ 
                   
                   = 
                   
                     
                       ∑ 
                       
                         i 
                         = 
                         0 
                       
                       
                         
                           N 
                           sb 
                         
                         - 
                         1 
                       
                     
                      
                     
                         
                     
                      
                     
                       
                         ∑ 
                         
                           f 
                           = 
                           0 
                         
                         
                           
                             N 
                             
                               nonzero 
                                
                               
                                 [ 
                                 i 
                                 ] 
                               
                             
                           
                           - 
                           1 
                         
                       
                        
                       
                           
                       
                        
                       
                         
                           
                             
                               S 
                               ~ 
                             
                             i 
                             ′ 
                           
                            
                           
                             ( 
                             f 
                             ) 
                           
                         
                         2 
                       
                     
                   
                 
               
               
                 
                   [ 
                   19 
                   ] 
                 
               
             
           
         
       
     
         [0000]    where E′ dec  is the energy of the non-zero decoded signal spectral coefficients with respect to all subbands, S i (f) is the non-zero decoded signal spectral coefficient with respect to the ith subband, N sb  is the total number of subbands, and N nonzero [i] is the number of non-zero decoded signal spectral coefficients with respect to the ith subband. 
         [0119]    Energy ratio computation sections  1310  and  1309  calculate an energy ratio relative to the input signal spectral coefficient and an energy ratio relative to the decoded signal spectral coefficient, respectively, according to the equations below. 
         [0000]      [20] 
         [0000]        R   org     —     i   =E″   org     —     i   /E′   org   (Equation 20)
 
         [0000]    where E″ org     —     i  is the energy of the zero input signal spectral coefficients with respect to the ith subband, E′ org  is the energy of the non-zero input signal spectral coefficients with respect to all subbands, and R org     —     i  is the energy ratio between the above-mentioned two energies with respect to the ith subband. 
         [0000]      [21] 
         [0000]        R   dec     —     i   =E″   dec     —     i   /E′   dec   (Equation 21)
 
         [0000]    where E″ dec     —     i  is the energy of the zero decoded signal spectral coefficients with respect to the ith subband, E′ dec  is the energy of the non-zero decoded signal spectral coefficients with respect to all subbands, and R dec     —     i  is the energy ratio between the above-mentioned two energies with respect to the ith subband. 
         [0120]    At divider  707 , a spectral envelope shaping parameter is computed as indicated by the following equation. 
         [0000]      [22] 
         [0000]        G   i   =R   org     —     i   /R   dec     —     i   (Equation 22)
 
         [0000]    where R org     —     i  is the energy ratio of the input signal spectrum corresponding to the ith subband, R dec     —     i  is the energy ratio of the decoded signal spectrum corresponding to the ith subband, and G i  is the ratio between the above-mentioned two energy ratios. 
       Embodiment 4 
       [0121]    In the case of a configuration where coding is performed at a low bit rate, coding accuracy is sometimes insufficient even for bands where there is no spectral gap (i.e., bands coded at a transform coding layer), resulting in a large coding error relative to the input signal spectral coefficient. Under such conditions, it is possible to improve sound quality by applying spectral envelope shaping to bands where there is no spectral gap, just like it is applied to bands where there is a spectral gap. The present embodiment is one where this idea has been applied to Embodiment 3. 
         [0122]      FIG. 14  is a diagram showing a configuration of a spectral envelope extraction section according to the present embodiment. As shown in  FIG. 14 , energy ratio computation section  1411  determines, as G′, the energy ratio of energy E′ org  of the non-zero input signal spectral coefficients to energy E′ dec  of the non-zero decoded signal spectral coefficients. Energy ratio G′ thus computed is also outputted as a spectral envelope shaping parameter. 
         [0123]      FIG. 15  is a diagram showing a configuration of a spectral envelope shaping section with respect to the present embodiment. Spectral envelope shaping parameter generation section  1503  calculates a spectral envelope shaping parameter for a band in which there is no spectral gap in the manner indicated by the following equation. 
         [0000]      [23] 
         [0000]        P   i   =√{square root over ({tilde over (G)}   i   /{tilde over (G)}′− 1  (Equation 23)
 
         [0000]    where P i  is the obtained spectral envelope shaping parameter, {tilde over (G)} i  is the decoded energy ratio with respect to the ith subband, and {tilde over (G)}′ is the decoded energy ratio with respect to non-zero spectral coefficients. 
         [0124]    Embodiments 1 through 4 of the present invention have been described above. 
         [0125]    For these embodiments, the apparatuses were referred to as audio coding apparatuses/audio decoding apparatuses, but the term “audio” as used herein refers to audio in a broad sense. Specifically, an input signal with respect to an audio coding apparatus and a decoded signal with respect to an audio decoding apparatus may include any kind of signal, e.g., an audio signal, a music signal, or an acoustic signal including both of the above, and so forth. 
         [0126]    The embodiments above have been described taking as examples cases where the present invention is configured with hardware. However, the present invention may also be realized through software in cooperation with hardware. 
         [0127]    The functional blocks used in the descriptions for the embodiments above are typically realized as LSIs, which are integrated circuits. These may be individual chips, or some or all of them may be integrated into a single chip. Although the term LSI is used above, depending on the level of integration, they may also be referred to as IC, system LSI, super LSI, or ultra LSI. 
         [0128]    The method of circuit integration is by no means limited to LSI, and may instead be realized through dedicated circuits or general-purpose processors. Field programmable gate arrays (FPGAs), which are programmable after LSI fabrication, or reconfigurable processors, whose connections and settings of circuit cells inside the LSI are reconfigurable, may also be used. 
         [0129]    Furthermore, should there arise a technique for circuit integration that replaces LSI due to advancements in semiconductor technology or through other derivative techniques, such a technique may naturally be employed to integrate functional blocks. Applications of biotechnology, and/or the like, are conceivable possibilities. 
         [0130]    The disclosure of the specification, drawings, and abstract included in Japanese Patent Application No. 2010-234088, filed on Oct. 18, 2010, is incorporated herein by reference in its entirety. 
       INDUSTRIAL APPLICABILITY 
       [0131]    The present invention is applicable to wireless communications terminal apparatuses, base station apparatuses, teleconference terminal apparatuses, video conference terminal apparatuses, voice over Internet Protocol (VoIP) terminal apparatuses, and/or the like, of mobile communications systems. 
       REFERENCE SIGNS LIST 
       [0000]    
       
           601  CELP coding section 
           602  CELP local decoding section 
           603 ,  604  T/F transform section 
           605  Vector quantization section 
           606  Vector dequantization section 
           607  Vector envelope extraction section 
           608  Quantization section 
           609  Multiplexing section 
           901  Demultiplexing section 
           902  CELP decoding section 
           903  T/F transform section 
           904  Vector dequantization section 
           905  Dequantization section 
           906  Spectral envelope shaping section 
           907  F/T transform section 
           908  Adder