Increasing the temporal resolution of transients
Apply a one-level Haar transform (or Hadamard) on each short MDCT to nearly double the time-domain resolution.
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1 changed files with 35 additions and 2 deletions
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@ -452,6 +452,19 @@ static void deinterleave_vector(celt_norm *X, int N0, int stride)
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RESTORE_STACK;
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}
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static void haar1(celt_norm *X, int N0, int stride)
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{
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int i, j;
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N0 >>= 1;
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for (i=0;i<stride;i++)
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for (j=0;j<N0;j++)
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{
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celt_norm tmp = X[stride*2*j+i];
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X[stride*2*j+i] = MULT16_16_Q15(QCONST16(.7070678f,15), X[stride*2*j+i] + X[stride*(2*j+1)+i]);
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X[stride*(2*j+1)+i] = MULT16_16_Q15(QCONST16(.7070678f,15), tmp - X[stride*(2*j+1)+i]);
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}
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}
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/* This function is responsible for encoding and decoding a band for both
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the mono and stereo case. Even in the mono case, it can split the band
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in two and transmit the energy difference with the two half-bands. It
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@ -466,19 +479,33 @@ static void quant_band(int encode, const CELTMode *m, int i, celt_norm *X, celt_
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int imid=0, iside=0;
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int N0=N;
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int N_B=N;
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int N_B0;
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int spread0=spread;
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int do_haar = 0;
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if (spread)
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N_B /= spread;
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N_B0 = N_B;
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split = stereo = Y != NULL;
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if (!stereo && spread>1 && level==0)
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{
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if ((N_B&1) == 0)
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{
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spread <<= 1;
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N_B >>= 1;
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do_haar = 1;
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if (encode)
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deinterleave_vector(X, N_B, spread);
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haar1(X, N_B0, spread0);
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if (lowband)
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deinterleave_vector(lowband, N_B, spread);
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haar1(lowband, N_B0, spread0);
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spread0 = spread;
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}
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if (encode)
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deinterleave_vector(X, N_B, spread0);
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if (lowband)
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deinterleave_vector(lowband, N_B, spread0);
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}
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/* If we need more than 32 bits, try splitting the band in two. */
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@ -752,6 +779,12 @@ static void quant_band(int encode, const CELTMode *m, int i, celt_norm *X, celt_
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interleave_vector(X, N_B, spread0);
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if (lowband)
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interleave_vector(lowband, N_B, spread0);
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if (do_haar)
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{
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haar1(X, N_B0, spread0>>1);
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if (lowband)
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haar1(lowband, N_B0, spread0>>1);
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}
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}
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if (lowband_out && !stereo)
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