| /* |
| * Copyright (C) 2013 The Android Open Source Project |
| * |
| * Licensed under the Apache License, Version 2.0 (the "License"); |
| * you may not use this file except in compliance with the License. |
| * You may obtain a copy of the License at |
| * |
| * http://www.apache.org/licenses/LICENSE-2.0 |
| * |
| * Unless required by applicable law or agreed to in writing, software |
| * distributed under the License is distributed on an "AS IS" BASIS, |
| * WITHOUT WARRANTIES OR CONDITIONS OF ANY KIND, either express or implied. |
| * See the License for the specific language governing permissions and |
| * limitations under the License. |
| */ |
| |
| #ifndef ANDROID_AUDIO_RESAMPLER_FIR_GEN_H |
| #define ANDROID_AUDIO_RESAMPLER_FIR_GEN_H |
| |
| #include "utils/Compat.h" |
| |
| namespace android { |
| |
| /* |
| * generates a sine wave at equal steps. |
| * |
| * As most of our functions use sine or cosine at equal steps, |
| * it is very efficient to compute them that way (single multiply and subtract), |
| * rather than invoking the math library sin() or cos() each time. |
| * |
| * SineGen uses Goertzel's Algorithm (as a generator not a filter) |
| * to calculate sine(wstart + n * wstep) or cosine(wstart + n * wstep) |
| * by stepping through 0, 1, ... n. |
| * |
| * e^i(wstart+wstep) = 2cos(wstep) * e^i(wstart) - e^i(wstart-wstep) |
| * |
| * or looking at just the imaginary sine term, as the cosine follows identically: |
| * |
| * sin(wstart+wstep) = 2cos(wstep) * sin(wstart) - sin(wstart-wstep) |
| * |
| * Goertzel's algorithm is more efficient than the angle addition formula, |
| * e^i(wstart+wstep) = e^i(wstart) * e^i(wstep), which takes up to |
| * 4 multiplies and 2 adds (or 3* and 3+) and requires both sine and |
| * cosine generation due to the complex * complex multiply (full rotation). |
| * |
| * See: http://en.wikipedia.org/wiki/Goertzel_algorithm |
| * |
| */ |
| |
| class SineGen { |
| public: |
| SineGen(double wstart, double wstep, bool cosine = false) { |
| if (cosine) { |
| mCurrent = cos(wstart); |
| mPrevious = cos(wstart - wstep); |
| } else { |
| mCurrent = sin(wstart); |
| mPrevious = sin(wstart - wstep); |
| } |
| mTwoCos = 2.*cos(wstep); |
| } |
| SineGen(double expNow, double expPrev, double twoCosStep) { |
| mCurrent = expNow; |
| mPrevious = expPrev; |
| mTwoCos = twoCosStep; |
| } |
| inline double value() const { |
| return mCurrent; |
| } |
| inline void advance() { |
| double tmp = mCurrent; |
| mCurrent = mCurrent*mTwoCos - mPrevious; |
| mPrevious = tmp; |
| } |
| inline double valueAdvance() { |
| double tmp = mCurrent; |
| mCurrent = mCurrent*mTwoCos - mPrevious; |
| mPrevious = tmp; |
| return tmp; |
| } |
| |
| private: |
| double mCurrent; // current value of sine/cosine |
| double mPrevious; // previous value of sine/cosine |
| double mTwoCos; // stepping factor |
| }; |
| |
| /* |
| * generates a series of sine generators, phase offset by fixed steps. |
| * |
| * This is used to generate polyphase sine generators, one per polyphase |
| * in the filter code below. |
| * |
| * The SineGen returned by value() starts at innerStart = outerStart + n*outerStep; |
| * increments by innerStep. |
| * |
| */ |
| |
| class SineGenGen { |
| public: |
| SineGenGen(double outerStart, double outerStep, double innerStep, bool cosine = false) |
| : mSineInnerCur(outerStart, outerStep, cosine), |
| mSineInnerPrev(outerStart-innerStep, outerStep, cosine) |
| { |
| mTwoCos = 2.*cos(innerStep); |
| } |
| inline SineGen value() { |
| return SineGen(mSineInnerCur.value(), mSineInnerPrev.value(), mTwoCos); |
| } |
| inline void advance() { |
| mSineInnerCur.advance(); |
| mSineInnerPrev.advance(); |
| } |
| inline SineGen valueAdvance() { |
| return SineGen(mSineInnerCur.valueAdvance(), mSineInnerPrev.valueAdvance(), mTwoCos); |
| } |
| |
| private: |
| SineGen mSineInnerCur; // generate the inner sine values (stepped by outerStep). |
| SineGen mSineInnerPrev; // generate the inner sine previous values |
| // (behind by innerStep, stepped by outerStep). |
| double mTwoCos; // the inner stepping factor for the returned SineGen. |
| }; |
| |
| static inline double sqr(double x) { |
| return x * x; |
| } |
| |
| /* |
| * rounds a double to the nearest integer for FIR coefficients. |
| * |
| * One variant uses noise shaping, which must keep error history |
| * to work (the err parameter, initialized to 0). |
| * The other variant is a non-noise shaped version for |
| * S32 coefficients (noise shaping doesn't gain much). |
| * |
| * Caution: No bounds saturation is applied, but isn't needed in this case. |
| * |
| * @param x is the value to round. |
| * |
| * @param maxval is the maximum integer scale factor expressed as an int64 (for headroom). |
| * Typically this may be the maximum positive integer+1 (using the fact that double precision |
| * FIR coefficients generated here are never that close to 1.0 to pose an overflow condition). |
| * |
| * @param err is the previous error (actual - rounded) for the previous rounding op. |
| * For 16b coefficients this can improve stopband dB performance by up to 2dB. |
| * |
| * Many variants exist for the noise shaping: http://en.wikipedia.org/wiki/Noise_shaping |
| * |
| */ |
| |
| static inline int64_t toint(double x, int64_t maxval, double& err) { |
| double val = x * maxval; |
| double ival = floor(val + 0.5 + err*0.2); |
| err = val - ival; |
| return static_cast<int64_t>(ival); |
| } |
| |
| static inline int64_t toint(double x, int64_t maxval) { |
| return static_cast<int64_t>(floor(x * maxval + 0.5)); |
| } |
| |
| /* |
| * Modified Bessel function of the first kind |
| * http://en.wikipedia.org/wiki/Bessel_function |
| * |
| * The formulas are taken from Abramowitz and Stegun, |
| * _Handbook of Mathematical Functions_ (links below): |
| * |
| * http://people.math.sfu.ca/~cbm/aands/page_375.htm |
| * http://people.math.sfu.ca/~cbm/aands/page_378.htm |
| * |
| * http://dlmf.nist.gov/10.25 |
| * http://dlmf.nist.gov/10.40 |
| * |
| * Note we assume x is nonnegative (the function is symmetric, |
| * pass in the absolute value as needed). |
| * |
| * Constants are compile time derived with templates I0Term<> and |
| * I0ATerm<> to the precision of the compiler. The series can be expanded |
| * to any precision needed, but currently set around 24b precision. |
| * |
| * We use a bit of template math here, constexpr would probably be |
| * more appropriate for a C++11 compiler. |
| * |
| * For the intermediate range 3.75 < x < 15, we use minimax polynomial fit. |
| * |
| */ |
| |
| template <int N> |
| struct I0Term { |
| static const CONSTEXPR double value = I0Term<N-1>::value / (4. * N * N); |
| }; |
| |
| template <> |
| struct I0Term<0> { |
| static const CONSTEXPR double value = 1.; |
| }; |
| |
| template <int N> |
| struct I0ATerm { |
| static const CONSTEXPR double value = I0ATerm<N-1>::value * (2.*N-1.) * (2.*N-1.) / (8. * N); |
| }; |
| |
| template <> |
| struct I0ATerm<0> { // 1/sqrt(2*PI); |
| static const CONSTEXPR double value = |
| 0.398942280401432677939946059934381868475858631164934657665925; |
| }; |
| |
| #if USE_HORNERS_METHOD |
| /* Polynomial evaluation of A + Bx + Cx^2 + Dx^3 + ... |
| * using Horner's Method: http://en.wikipedia.org/wiki/Horner's_method |
| * |
| * This has fewer multiplications than Estrin's method below, but has back to back |
| * floating point dependencies. |
| * |
| * On ARM this appears to work slower, so USE_HORNERS_METHOD is not default enabled. |
| */ |
| |
| inline double Poly2(double A, double B, double x) { |
| return A + x * B; |
| } |
| |
| inline double Poly4(double A, double B, double C, double D, double x) { |
| return A + x * (B + x * (C + x * (D))); |
| } |
| |
| inline double Poly7(double A, double B, double C, double D, double E, double F, double G, |
| double x) { |
| return A + x * (B + x * (C + x * (D + x * (E + x * (F + x * (G)))))); |
| } |
| |
| inline double Poly9(double A, double B, double C, double D, double E, double F, double G, |
| double H, double I, double x) { |
| return A + x * (B + x * (C + x * (D + x * (E + x * (F + x * (G + x * (H + x * (I)))))))); |
| } |
| |
| #else |
| /* Polynomial evaluation of A + Bx + Cx^2 + Dx^3 + ... |
| * using Estrin's Method: http://en.wikipedia.org/wiki/Estrin's_scheme |
| * |
| * This is typically faster, perhaps gains about 5-10% overall on ARM processors |
| * over Horner's method above. |
| */ |
| |
| inline double Poly2(double A, double B, double x) { |
| return A + B * x; |
| } |
| |
| inline double Poly3(double A, double B, double C, double x, double x2) { |
| return Poly2(A, B, x) + C * x2; |
| } |
| |
| inline double Poly3(double A, double B, double C, double x) { |
| return Poly2(A, B, x) + C * x * x; |
| } |
| |
| inline double Poly4(double A, double B, double C, double D, double x, double x2) { |
| return Poly2(A, B, x) + Poly2(C, D, x) * x2; // same as poly2(poly2, poly2, x2); |
| } |
| |
| inline double Poly4(double A, double B, double C, double D, double x) { |
| return Poly4(A, B, C, D, x, x * x); |
| } |
| |
| inline double Poly7(double A, double B, double C, double D, double E, double F, double G, |
| double x) { |
| double x2 = x * x; |
| return Poly4(A, B, C, D, x, x2) + Poly3(E, F, G, x, x2) * (x2 * x2); |
| } |
| |
| inline double Poly8(double A, double B, double C, double D, double E, double F, double G, |
| double H, double x, double x2, double x4) { |
| return Poly4(A, B, C, D, x, x2) + Poly4(E, F, G, H, x, x2) * x4; |
| } |
| |
| inline double Poly9(double A, double B, double C, double D, double E, double F, double G, |
| double H, double I, double x) { |
| double x2 = x * x; |
| #if 1 |
| // It does not seem faster to explicitly decompose Poly8 into Poly4, but |
| // could depend on compiler floating point scheduling. |
| double x4 = x2 * x2; |
| return Poly8(A, B, C, D, E, F, G, H, x, x2, x4) + I * (x4 * x4); |
| #else |
| double val = Poly4(A, B, C, D, x, x2); |
| double x4 = x2 * x2; |
| return val + Poly4(E, F, G, H, x, x2) * x4 + I * (x4 * x4); |
| #endif |
| } |
| #endif |
| |
| static inline double I0(double x) { |
| if (x < 3.75) { |
| x *= x; |
| return Poly7(I0Term<0>::value, I0Term<1>::value, |
| I0Term<2>::value, I0Term<3>::value, |
| I0Term<4>::value, I0Term<5>::value, |
| I0Term<6>::value, x); // e < 1.6e-7 |
| } |
| if (1) { |
| /* |
| * Series expansion coefs are easy to calculate, but are expanded around 0, |
| * so error is unequal over the interval 0 < x < 3.75, the error being |
| * significantly better near 0. |
| * |
| * A better solution is to use precise minimax polynomial fits. |
| * |
| * We use a slightly more complicated solution for 3.75 < x < 15, based on |
| * the tables in Blair and Edwards, "Stable Rational Minimax Approximations |
| * to the Modified Bessel Functions I0(x) and I1(x)", Chalk Hill Nuclear Laboratory, |
| * AECL-4928. |
| * |
| * http://www.iaea.org/inis/collection/NCLCollectionStore/_Public/06/178/6178667.pdf |
| * |
| * See Table 11 for 0 < x < 15; e < 10^(-7.13). |
| * |
| * Note: Beta cannot exceed 15 (hence Stopband cannot exceed 144dB = 24b). |
| * |
| * This speeds up overall computation by about 40% over using the else clause below, |
| * which requires sqrt and exp. |
| * |
| */ |
| |
| x *= x; |
| double num = Poly9(-0.13544938430e9, -0.33153754512e8, |
| -0.19406631946e7, -0.48058318783e5, |
| -0.63269783360e3, -0.49520779070e1, |
| -0.24970910370e-1, -0.74741159550e-4, |
| -0.18257612460e-6, x); |
| double y = x - 225.; // reflection around 15 (squared) |
| double den = Poly4(-0.34598737196e8, 0.23852643181e6, |
| -0.70699387620e3, 0.10000000000e1, y); |
| return num / den; |
| |
| #if IO_EXTENDED_BETA |
| /* Table 42 for x > 15; e < 10^(-8.11). |
| * This is used for Beta>15, but is disabled here as |
| * we never use Beta that high. |
| * |
| * NOTE: This should be enabled only for x > 15. |
| */ |
| |
| double y = 1./x; |
| double z = y - (1./15); |
| double num = Poly2(0.415079861746e1, -0.5149092496e1, z); |
| double den = Poly3(0.103150763823e2, -0.14181687413e2, |
| 0.1000000000e1, z); |
| return exp(x) * sqrt(y) * num / den; |
| #endif |
| } else { |
| /* |
| * NOT USED, but reference for large Beta. |
| * |
| * Abramowitz and Stegun asymptotic formula. |
| * works for x > 3.75. |
| */ |
| double y = 1./x; |
| return exp(x) * sqrt(y) * |
| // note: reciprocal squareroot may be easier! |
| // http://en.wikipedia.org/wiki/Fast_inverse_square_root |
| Poly9(I0ATerm<0>::value, I0ATerm<1>::value, |
| I0ATerm<2>::value, I0ATerm<3>::value, |
| I0ATerm<4>::value, I0ATerm<5>::value, |
| I0ATerm<6>::value, I0ATerm<7>::value, |
| I0ATerm<8>::value, y); // (... e) < 1.9e-7 |
| } |
| } |
| |
| /* A speed optimized version of the Modified Bessel I0() which incorporates |
| * the sqrt and numerator multiply and denominator divide into the computation. |
| * This speeds up filter computation by about 10-15%. |
| */ |
| static inline double I0SqrRat(double x2, double num, double den) { |
| if (x2 < (3.75 * 3.75)) { |
| return Poly7(I0Term<0>::value, I0Term<1>::value, |
| I0Term<2>::value, I0Term<3>::value, |
| I0Term<4>::value, I0Term<5>::value, |
| I0Term<6>::value, x2) * num / den; // e < 1.6e-7 |
| } |
| num *= Poly9(-0.13544938430e9, -0.33153754512e8, |
| -0.19406631946e7, -0.48058318783e5, |
| -0.63269783360e3, -0.49520779070e1, |
| -0.24970910370e-1, -0.74741159550e-4, |
| -0.18257612460e-6, x2); // e < 10^(-7.13). |
| double y = x2 - 225.; // reflection around 15 (squared) |
| den *= Poly4(-0.34598737196e8, 0.23852643181e6, |
| -0.70699387620e3, 0.10000000000e1, y); |
| return num / den; |
| } |
| |
| /* |
| * calculates the transition bandwidth for a Kaiser filter |
| * |
| * Formula 3.2.8, Vaidyanathan, _Multirate Systems and Filter Banks_, p. 48 |
| * Formula 7.76, Oppenheim and Schafer, _Discrete-time Signal Processing, 3e_, p. 542 |
| * |
| * @param halfNumCoef is half the number of coefficients per filter phase. |
| * |
| * @param stopBandAtten is the stop band attenuation desired. |
| * |
| * @return the transition bandwidth in normalized frequency (0 <= f <= 0.5) |
| */ |
| static inline double firKaiserTbw(int halfNumCoef, double stopBandAtten) { |
| return (stopBandAtten - 7.95)/((2.*14.36)*halfNumCoef); |
| } |
| |
| /* |
| * calculates the fir transfer response of the overall polyphase filter at w. |
| * |
| * Calculates the DTFT transfer coefficient H(w) for 0 <= w <= PI, utilizing the |
| * fact that h[n] is symmetric (cosines only, no complex arithmetic). |
| * |
| * We use Goertzel's algorithm to accelerate the computation to essentially |
| * a single multiply and 2 adds per filter coefficient h[]. |
| * |
| * Be careful be careful to consider that h[n] is the overall polyphase filter, |
| * with L phases, so rescaling H(w)/L is probably what you expect for "unity gain", |
| * as you only use one of the polyphases at a time. |
| */ |
| template <typename T> |
| static inline double firTransfer(const T* coef, int L, int halfNumCoef, double w) { |
| double accum = static_cast<double>(coef[0])*0.5; // "center coefficient" from first bank |
| coef += halfNumCoef; // skip first filterbank (picked up by the last filterbank). |
| #if SLOW_FIRTRANSFER |
| /* Original code for reference. This is equivalent to the code below, but slower. */ |
| for (int i=1 ; i<=L ; ++i) { |
| for (int j=0, ix=i ; j<halfNumCoef ; ++j, ix+=L) { |
| accum += cos(ix*w)*static_cast<double>(*coef++); |
| } |
| } |
| #else |
| /* |
| * Our overall filter is stored striped by polyphases, not a contiguous h[n]. |
| * We could fetch coefficients in a non-contiguous fashion |
| * but that will not scale to vector processing. |
| * |
| * We apply Goertzel's algorithm directly to each polyphase filter bank instead of |
| * using cosine generation/multiplication, thereby saving one multiply per inner loop. |
| * |
| * See: http://en.wikipedia.org/wiki/Goertzel_algorithm |
| * Also: Oppenheim and Schafer, _Discrete Time Signal Processing, 3e_, p. 720. |
| * |
| * We use the basic recursion to incorporate the cosine steps into real sequence x[n]: |
| * s[n] = x[n] + (2cosw)*s[n-1] + s[n-2] |
| * |
| * y[n] = s[n] - e^(iw)s[n-1] |
| * = sum_{k=-\infty}^{n} x[k]e^(-iw(n-k)) |
| * = e^(-iwn) sum_{k=0}^{n} x[k]e^(iwk) |
| * |
| * The summation contains the frequency steps we want multiplied by the source |
| * (similar to a DTFT). |
| * |
| * Using symmetry, and just the real part (be careful, this must happen |
| * after any internal complex multiplications), the polyphase filterbank |
| * transfer function is: |
| * |
| * Hpp[n, w, w_0] = sum_{k=0}^{n} x[k] * cos(wk + w_0) |
| * = Re{ e^(iwn + iw_0) y[n]} |
| * = cos(wn+w_0) * s[n] - cos(w(n+1)+w_0) * s[n-1] |
| * |
| * using the fact that s[n] of real x[n] is real. |
| * |
| */ |
| double dcos = 2. * cos(L*w); |
| int start = ((halfNumCoef)*L + 1); |
| SineGen cc((start - L) * w, w, true); // cosine |
| SineGen cp(start * w, w, true); // cosine |
| for (int i=1 ; i<=L ; ++i) { |
| double sc = 0; |
| double sp = 0; |
| for (int j=0 ; j<halfNumCoef ; ++j) { |
| double tmp = sc; |
| sc = static_cast<double>(*coef++) + dcos*sc - sp; |
| sp = tmp; |
| } |
| // If we are awfully clever, we can apply Goertzel's algorithm |
| // again on the sc and sp sequences returned here. |
| accum += cc.valueAdvance() * sc - cp.valueAdvance() * sp; |
| } |
| #endif |
| return accum*2.; |
| } |
| |
| /* |
| * evaluates the minimum and maximum |H(f)| bound in a band region. |
| * |
| * This is usually done with equally spaced increments in the target band in question. |
| * The passband is often very small, and sampled that way. The stopband is often much |
| * larger. |
| * |
| * We use the fact that the overall polyphase filter has an additional bank at the end |
| * for interpolation; hence it is overspecified for the H(f) computation. Thus the |
| * first polyphase is never actually checked, excepting its first term. |
| * |
| * In this code we use the firTransfer() evaluator above, which uses Goertzel's |
| * algorithm to calculate the transfer function at each point. |
| * |
| * TODO: An alternative with equal spacing is the FFT/DFT. An alternative with unequal |
| * spacing is a chirp transform. |
| * |
| * @param coef is the designed polyphase filter banks |
| * |
| * @param L is the number of phases (for interpolation) |
| * |
| * @param halfNumCoef should be half the number of coefficients for a single |
| * polyphase. |
| * |
| * @param fstart is the normalized frequency start. |
| * |
| * @param fend is the normalized frequency end. |
| * |
| * @param steps is the number of steps to take (sampling) between frequency start and end |
| * |
| * @param firMin returns the minimum transfer |H(f)| found |
| * |
| * @param firMax returns the maximum transfer |H(f)| found |
| * |
| * 0 <= f <= 0.5. |
| * This is used to test passband and stopband performance. |
| */ |
| template <typename T> |
| static void testFir(const T* coef, int L, int halfNumCoef, |
| double fstart, double fend, int steps, double &firMin, double &firMax) { |
| double wstart = fstart*(2.*M_PI); |
| double wend = fend*(2.*M_PI); |
| double wstep = (wend - wstart)/steps; |
| double fmax, fmin; |
| double trf = firTransfer(coef, L, halfNumCoef, wstart); |
| if (trf<0) { |
| trf = -trf; |
| } |
| fmin = fmax = trf; |
| wstart += wstep; |
| for (int i=1; i<steps; ++i) { |
| trf = firTransfer(coef, L, halfNumCoef, wstart); |
| if (trf<0) { |
| trf = -trf; |
| } |
| if (trf>fmax) { |
| fmax = trf; |
| } |
| else if (trf<fmin) { |
| fmin = trf; |
| } |
| wstart += wstep; |
| } |
| // renormalize - this is needed for integer filter types, use 1 for float or double. |
| constexpr int integralShift = std::is_integral<T>::value ? (sizeof(T) * CHAR_BIT - 1) : 0; |
| const double norm = 1. / (int64_t{L} << integralShift); |
| |
| firMin = fmin * norm; |
| firMax = fmax * norm; |
| } |
| |
| /* |
| * evaluates the |H(f)| lowpass band characteristics. |
| * |
| * This function tests the lowpass characteristics for the overall polyphase filter, |
| * and is used to verify the design. |
| * |
| * For a polyphase filter (L > 1), typically fp should be set to the |
| * passband normalized frequency from 0 to 0.5 for the overall filter (thus it |
| * is the designed polyphase bank value / L). Likewise for fs. |
| * Similarly the stopSteps should be L * passSteps for equivalent accuracy. |
| * |
| * @param coef is the designed polyphase filter banks |
| * |
| * @param L is the number of phases (for interpolation) |
| * |
| * @param halfNumCoef should be half the number of coefficients for a single |
| * polyphase. |
| * |
| * @param fp is the passband normalized frequency, 0 < fp < fs < 0.5. |
| * |
| * @param fs is the stopband normalized frequency, 0 < fp < fs < 0.5. |
| * |
| * @param passSteps is the number of passband sampling steps. |
| * |
| * @param stopSteps is the number of stopband sampling steps. |
| * |
| * @param passMin is the minimum value in the passband |
| * |
| * @param passMax is the maximum value in the passband (useful for scaling). This should |
| * be less than 1., to avoid sine wave test overflow. |
| * |
| * @param passRipple is the passband ripple. Typically this should be less than 0.1 for |
| * an audio filter. Generally speaker/headphone device characteristics will dominate |
| * the passband term. |
| * |
| * @param stopMax is the maximum value in the stopband. |
| * |
| * @param stopRipple is the stopband ripple, also known as stopband attenuation. |
| * Typically this should be greater than ~80dB for low quality, and greater than |
| * ~100dB for full 16b quality, otherwise aliasing may become noticeable. |
| * |
| */ |
| template <typename T> |
| static void testFir(const T* coef, int L, int halfNumCoef, |
| double fp, double fs, int passSteps, int stopSteps, |
| double &passMin, double &passMax, double &passRipple, |
| double &stopMax, double &stopRipple) { |
| double fmin, fmax; |
| testFir(coef, L, halfNumCoef, 0., fp, passSteps, fmin, fmax); |
| double d1 = (fmax - fmin)/2.; |
| passMin = fmin; |
| passMax = fmax; |
| passRipple = -20.*log10(1. - d1); // passband ripple |
| testFir(coef, L, halfNumCoef, fs, 0.5, stopSteps, fmin, fmax); |
| // fmin is really not important for the stopband. |
| stopMax = fmax; |
| stopRipple = -20.*log10(fmax); // stopband ripple/attenuation |
| } |
| |
| /* |
| * Estimate the windowed sinc minimum passband value. |
| * |
| * This is the minimum value for a windowed sinc filter in its passband, |
| * which is identical to the scaling required not to cause overflow of a 0dBFS signal. |
| * The actual value used to attenuate the filter amplitude should be slightly |
| * smaller than this (suggest squaring) as this is just an estimate. |
| * |
| * As a windowed sinc has a passband ripple commensurate to the stopband attenuation |
| * due to Gibb's phenomenon from truncating the sinc, we derive this value from |
| * the design stopbandAttenuationDb (a positive value). |
| */ |
| static inline double computeWindowedSincMinimumPassbandValue( |
| double stopBandAttenuationDb) { |
| return 1. - pow(10. /* base */, stopBandAttenuationDb * (-1. / 20.)); |
| } |
| |
| /* |
| * Compute the windowed sinc passband ripple from stopband attenuation. |
| * |
| * As a windowed sinc has an passband ripple commensurate to the stopband attenuation |
| * due to Gibb's phenomenon from truncating the sinc, we derive this value from |
| * the design stopbandAttenuationDb (a positive value). |
| */ |
| static inline double computeWindowedSincPassbandRippleDb( |
| double stopBandAttenuationDb) { |
| return -20. * log10(computeWindowedSincMinimumPassbandValue(stopBandAttenuationDb)); |
| } |
| |
| /* |
| * Kaiser window Beta value |
| * |
| * Formula 3.2.5, 3.2.7, Vaidyanathan, _Multirate Systems and Filter Banks_, p. 48 |
| * Formula 7.75, Oppenheim and Schafer, _Discrete-time Signal Processing, 3e_, p. 542 |
| * |
| * See also: http://melodi.ee.washington.edu/courses/ee518/notes/lec17.pdf |
| * |
| * Kaiser window and beta parameter |
| * |
| * | 0.1102*(A - 8.7) A > 50 |
| * Beta = | 0.5842*(A - 21)^0.4 + 0.07886*(A - 21) 21 < A <= 50 |
| * | 0. A <= 21 |
| * |
| * with A is the desired stop-band attenuation in positive dBFS |
| * |
| * 30 dB 2.210 |
| * 40 dB 3.384 |
| * 50 dB 4.538 |
| * 60 dB 5.658 |
| * 70 dB 6.764 |
| * 80 dB 7.865 |
| * 90 dB 8.960 |
| * 100 dB 10.056 |
| * |
| * For some values of stopBandAttenuationDb the function may be computed |
| * at compile time. |
| */ |
| static inline constexpr double computeBeta(double stopBandAttenuationDb) { |
| if (stopBandAttenuationDb > 50.) { |
| return 0.1102 * (stopBandAttenuationDb - 8.7); |
| } |
| const double offset = stopBandAttenuationDb - 21.; |
| if (offset > 0.) { |
| return 0.5842 * pow(offset, 0.4) + 0.07886 * offset; |
| } |
| return 0.; |
| } |
| |
| /* |
| * Calculates the overall polyphase filter based on a windowed sinc function. |
| * |
| * The windowed sinc is an odd length symmetric filter of exactly L*halfNumCoef*2+1 |
| * taps for the entire kernel. This is then decomposed into L+1 polyphase filterbanks. |
| * The last filterbank is used for interpolation purposes (and is mostly composed |
| * of the first bank shifted by one sample), and is unnecessary if one does |
| * not do interpolation. |
| * |
| * We use the last filterbank for some transfer function calculation purposes, |
| * so it needs to be generated anyways. |
| * |
| * @param coef is the caller allocated space for coefficients. This should be |
| * exactly (L+1)*halfNumCoef in size. |
| * |
| * @param L is the number of phases (for interpolation) |
| * |
| * @param halfNumCoef should be half the number of coefficients for a single |
| * polyphase. |
| * |
| * @param stopBandAtten is the stopband value, should be >50dB. |
| * |
| * @param fcr is cutoff frequency/sampling rate (<0.5). At this point, the energy |
| * should be 6dB less. (fcr is where the amplitude drops by half). Use the |
| * firKaiserTbw() to calculate the transition bandwidth. fcr is the midpoint |
| * between the stop band and the pass band (fstop+fpass)/2. |
| * |
| * @param atten is the attenuation (generally slightly less than 1). |
| */ |
| |
| template <typename T> |
| static inline void firKaiserGen(T* coef, int L, int halfNumCoef, |
| double stopBandAtten, double fcr, double atten) { |
| const int N = L * halfNumCoef; // non-negative half |
| const double beta = computeBeta(stopBandAtten); |
| const double xstep = (2. * M_PI) * fcr / L; |
| const double xfrac = 1. / N; |
| const double yscale = atten * L / (I0(beta) * M_PI); |
| const double sqrbeta = sqr(beta); |
| |
| // We use sine generators, which computes sines on regular step intervals. |
| // This speeds up overall computation about 40% from computing the sine directly. |
| |
| SineGenGen sgg(0., xstep, L*xstep); // generates sine generators (one per polyphase) |
| |
| for (int i=0 ; i<=L ; ++i) { // generate an extra set of coefs for interpolation |
| |
| // computation for a single polyphase of the overall filter. |
| SineGen sg = sgg.valueAdvance(); // current sine generator for "j" inner loop. |
| double err = 0; // for noise shaping on int16_t coefficients (over each polyphase) |
| |
| for (int j=0, ix=i ; j<halfNumCoef ; ++j, ix+=L) { |
| double y; |
| if (CC_LIKELY(ix)) { |
| double x = static_cast<double>(ix); |
| |
| // sine generator: sg.valueAdvance() returns sin(ix*xstep); |
| // y = I0(beta * sqrt(1.0 - sqr(x * xfrac))) * yscale * sg.valueAdvance() / x; |
| y = I0SqrRat(sqrbeta * (1.0 - sqr(x * xfrac)), yscale * sg.valueAdvance(), x); |
| } else { |
| y = 2. * atten * fcr; // center of filter, sinc(0) = 1. |
| sg.advance(); |
| } |
| |
| if (std::is_same<T, int16_t>::value) { // int16_t needs noise shaping |
| *coef++ = static_cast<T>(toint(y, 1ULL<<(sizeof(T)*8-1), err)); |
| } else if (std::is_same<T, int32_t>::value) { |
| *coef++ = static_cast<T>(toint(y, 1ULL<<(sizeof(T)*8-1))); |
| } else { // assumed float or double |
| *coef++ = static_cast<T>(y); |
| } |
| } |
| } |
| } |
| |
| } // namespace android |
| |
| #endif /*ANDROID_AUDIO_RESAMPLER_FIR_GEN_H*/ |