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https://gitlab.com/libeigen/eigen.git
synced 2024-12-21 07:19:46 +08:00
use a plain matrix to store the upper triangular matrix 'R', instead
of the "compact inside a vector" scheme used by fortran/minpack. The most difficult part is to fix all related code. Tests pass.
This commit is contained in:
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4b859c8554
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91561cded4
@ -74,6 +74,8 @@ public:
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};
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typedef Matrix< Scalar, Dynamic, 1 > FVectorType;
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typedef Matrix< Scalar, Dynamic, Dynamic > JacobianType;
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/* TODO: if eigen provides a triangular storage, use it here */
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typedef Matrix< Scalar, Dynamic, Dynamic > UpperTriangularType;
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Status hybrj1(
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FVectorType &x,
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@ -113,8 +115,9 @@ public:
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void resetParameters(void) { parameters = Parameters(); }
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Parameters parameters;
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FVectorType fvec, R, qtf, diag;
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FVectorType fvec, qtf, diag;
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JacobianType fjac;
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UpperTriangularType R;
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int nfev;
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int njev;
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int iter;
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@ -173,7 +176,6 @@ HybridNonLinearSolver<FunctorType,Scalar>::solveInit(
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wa1.resize(n); wa2.resize(n); wa3.resize(n); wa4.resize(n);
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fvec.resize(n);
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qtf.resize(n);
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R.resize( (n*(n+1))/2);
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fjac.resize(n, n);
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if (mode != 2)
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diag.resize(n);
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@ -218,7 +220,7 @@ HybridNonLinearSolver<FunctorType,Scalar>::solveOneStep(
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const int mode
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)
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{
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int i, j, l;
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int i, j;
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jeval = true;
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/* calculate the jacobian matrix. */
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@ -272,17 +274,10 @@ HybridNonLinearSolver<FunctorType,Scalar>::solveOneStep(
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/* copy the triangular factor of the qr factorization into r. */
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R = qrfac.matrixQR();
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sing = false;
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for (j = 0; j < n; ++j) {
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l = j;
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for (i = 0; i < j; ++i) {
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R[l] = fjac(i,j);
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l = l + n - i -1;
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}
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R[l] = wa1[j];
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if (wa1[j] == 0.)
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sing = true;
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}
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for (j = 0; j < n; ++j)
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if (wa1[j] == 0.) sing = true;
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/* accumulate the orthogonal factor in fjac. */
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ei_qform<Scalar>(n, n, fjac.data(), fjac.rows(), wa1.data());
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@ -328,13 +323,10 @@ HybridNonLinearSolver<FunctorType,Scalar>::solveOneStep(
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/* compute the scaled predicted reduction. */
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l = 0;
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for (i = 0; i < n; ++i) {
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sum = 0.;
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for (j = i; j < n; ++j) {
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sum += R[l] * wa1[j];
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++l;
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}
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for (j = i; j < n; ++j)
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sum += R(i,j) * wa1[j];
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wa3[i] = qtf[i] + sum;
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}
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temp = wa3.stableNorm();
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@ -421,7 +413,7 @@ HybridNonLinearSolver<FunctorType,Scalar>::solveOneStep(
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/* compute the qr factorization of the updated jacobian. */
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ei_r1updt<Scalar>(n, n, R.data(), R.size(), wa1.data(), wa2.data(), wa3.data(), &sing);
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ei_r1updt<Scalar>(n, n, R, wa1.data(), wa2.data(), wa3.data(), &sing);
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ei_r1mpyq<Scalar>(n, n, fjac.data(), fjac.rows(), wa2.data(), wa3.data());
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ei_r1mpyq<Scalar>(1, n, qtf.data(), 1, wa2.data(), wa3.data());
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@ -488,7 +480,6 @@ HybridNonLinearSolver<FunctorType,Scalar>::solveNumericalDiffInit(
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wa1.resize(n); wa2.resize(n); wa3.resize(n); wa4.resize(n);
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qtf.resize(n);
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R.resize( (n*(n+1))/2);
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fjac.resize(n, n);
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fvec.resize(n);
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if (mode != 2)
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@ -536,7 +527,7 @@ HybridNonLinearSolver<FunctorType,Scalar>::solveNumericalDiffOneStep(
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const int mode
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)
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{
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int i, j, l;
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int i, j;
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jeval = true;
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if (parameters.nb_of_subdiagonals<0) parameters.nb_of_subdiagonals= n-1;
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if (parameters.nb_of_superdiagonals<0) parameters.nb_of_superdiagonals= n-1;
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@ -591,26 +582,13 @@ HybridNonLinearSolver<FunctorType,Scalar>::solveNumericalDiffOneStep(
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}
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/* copy the triangular factor of the qr factorization into r. */
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R = qrfac.matrixQR();
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sing = false;
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for (j = 0; j < n; ++j) {
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l = j;
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for (i = 0; i < j; ++i) {
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R[l] = fjac(i,j);
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l = l + n - i -1;
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}
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R[l] = wa1[j];
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if (wa1[j] == 0.)
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sing = true;
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}
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for (j = 0; j < n; ++j)
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if (wa1[j] == 0.) sing = true;
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/* accumulate the orthogonal factor in fjac. */
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ei_qform<Scalar>(n, n, fjac.data(), fjac.rows(), wa1.data());
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#if 0
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std::cout << "ei_qform<Scalar>: " << fjac << std::endl;
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fjac = qrfac.matrixQ();
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std::cout << "qrfac.matrixQ():" << fjac << std::endl;
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#endif
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/* rescale if necessary. */
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@ -653,13 +631,10 @@ HybridNonLinearSolver<FunctorType,Scalar>::solveNumericalDiffOneStep(
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/* compute the scaled predicted reduction. */
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l = 0;
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for (i = 0; i < n; ++i) {
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sum = 0.;
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for (j = i; j < n; ++j) {
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sum += R[l] * wa1[j];
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++l;
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}
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for (j = i; j < n; ++j)
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sum += R(i,j) * wa1[j];
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wa3[i] = qtf[i] + sum;
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}
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temp = wa3.stableNorm();
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@ -747,7 +722,7 @@ HybridNonLinearSolver<FunctorType,Scalar>::solveNumericalDiffOneStep(
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/* compute the qr factorization of the updated jacobian. */
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ei_r1updt<Scalar>(n, n, R.data(), R.size(), wa1.data(), wa2.data(), wa3.data(), &sing);
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ei_r1updt<Scalar>(n, n, R, wa1.data(), wa2.data(), wa3.data(), &sing);
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ei_r1mpyq<Scalar>(n, n, fjac.data(), fjac.rows(), wa2.data(), wa3.data());
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ei_r1mpyq<Scalar>(1, n, qtf.data(), 1, wa2.data(), wa3.data());
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@ -1,14 +1,14 @@
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template <typename Scalar>
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void ei_dogleg(
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Matrix< Scalar, Dynamic, 1 > &r,
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const Matrix< Scalar, Dynamic, Dynamic > &qrfac,
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const Matrix< Scalar, Dynamic, 1 > &diag,
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const Matrix< Scalar, Dynamic, 1 > &qtb,
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Scalar delta,
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Matrix< Scalar, Dynamic, 1 > &x)
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{
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/* Local variables */
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int i, j, k, l, jj;
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int i, j, k;
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Scalar sum, temp, alpha, bnorm;
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Scalar gnorm, qnorm;
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Scalar sgnorm;
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@ -20,26 +20,16 @@ void ei_dogleg(
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assert(n==qtb.size());
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assert(n==x.size());
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/* first, calculate the gauss-newton direction. */
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jj = n * (n + 1) / 2;
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for (k = 0; k < n; ++k) {
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j = n - k - 1;
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jj -= k+1;
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l = jj + 1;
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sum = 0.;
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for (i = j+1; i < n; ++i) {
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sum += r[l] * x[i];
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++l;
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sum += qrfac(j,i) * x[i];
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}
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temp = r[jj];
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temp = qrfac(j,j);
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if (temp == 0.) {
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l = j;
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for (i = 0; i <= j; ++i) {
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/* Computing MAX */
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temp = std::max(temp,ei_abs(r[l]));
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l = l + n - i - 1;
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}
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for (i = 0; i <= j; ++i)
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temp = std::max(temp,ei_abs(qrfac(i,j)));
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temp = epsmch * temp;
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if (temp == 0.)
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temp = epsmch;
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@ -58,13 +48,10 @@ void ei_dogleg(
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/* the gauss-newton direction is not acceptable. */
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/* next, calculate the scaled gradient direction. */
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l = 0;
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for (j = 0; j < n; ++j) {
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temp = qtb[j];
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for (i = j; i < n; ++i) {
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wa1[i] += r[l] * temp;
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++l;
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}
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for (i = j; i < n; ++i)
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wa1[i] += qrfac(j,i) * temp;
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wa1[j] /= diag[j];
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}
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@ -81,16 +68,12 @@ void ei_dogleg(
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/* at which the quadratic is minimized. */
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wa1.array() /= (diag*gnorm).array();
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l = 0;
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for (j = 0; j < n; ++j) {
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sum = 0.;
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for (i = j; i < n; ++i) {
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sum += r[l] * wa1[i];
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++l;
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/* L100: */
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sum += qrfac(j,i) * wa1[i];
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}
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wa2[j] = sum;
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/* L110: */
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}
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temp = wa2.stableNorm();
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sgnorm = gnorm / temp / temp;
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@ -1,34 +1,27 @@
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template <typename Scalar>
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void ei_r1updt(int m, int n, Scalar *s, int /* ls */, const Scalar *u, Scalar *v, Scalar *w, bool *sing)
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template <typename Scalar>
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void ei_r1updt(int m, int n, Matrix< Scalar, Dynamic, Dynamic > &s, const Scalar *u, Scalar *v, Scalar *w, bool *sing)
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{
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/* Local variables */
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int i, j, l, jj, nm1;
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int i, j, nm1;
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Scalar tan__;
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int nmj;
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Scalar cos__, sin__, tau, temp, cotan;
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// ei_r1updt had a broader usecase, but we dont use it here. And, more
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// importantly, we can not test it.
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assert(m==n);
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/* Parameter adjustments */
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--w;
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--u;
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--v;
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--s;
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/* Function Body */
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const Scalar giant = std::numeric_limits<Scalar>::max();
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/* initialize the diagonal element pointer. */
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jj = n * ((m << 1) - n + 1) / 2 - (m - n);
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/* move the nontrivial part of the last column of s into w. */
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l = jj;
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for (i = n; i <= m; ++i) {
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w[i] = s[l];
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++l;
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/* L10: */
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}
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w[n] = s(n-1,n-1);
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/* rotate the vector v into a multiple of the n-th unit vector */
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/* in such a way that a spike is introduced into w. */
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@ -39,7 +32,6 @@ void ei_r1updt(int m, int n, Scalar *s, int /* ls */, const Scalar *u, Scalar *v
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}
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for (nmj = 1; nmj <= nm1; ++nmj) {
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j = n - nmj;
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jj -= m - j + 1;
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w[j] = 0.;
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if (v[j] == 0.) {
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goto L50;
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@ -75,16 +67,12 @@ L30:
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/* apply the transformation to s and extend the spike in w. */
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l = jj;
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for (i = j; i <= m; ++i) {
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temp = cos__ * s[l] - sin__ * w[i];
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w[i] = sin__ * s[l] + cos__ * w[i];
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s[l] = temp;
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++l;
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/* L40: */
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temp = cos__ * s(j-1,i-1) - sin__ * w[i];
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w[i] = sin__ * s(j-1,i-1) + cos__ * w[i];
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s(j-1,i-1) = temp;
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}
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L50:
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/* L60: */
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;
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}
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L70:
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@ -110,9 +98,9 @@ L70:
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/* determine a givens rotation which eliminates the */
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/* j-th element of the spike. */
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if (ei_abs(s[jj]) >= ei_abs(w[j]))
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if (ei_abs(s(j-1,j-1)) >= ei_abs(w[j]))
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goto L90;
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cotan = s[jj] / w[j];
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cotan = s(j-1,j-1) / w[j];
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/* Computing 2nd power */
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sin__ = Scalar(.5) / ei_sqrt(Scalar(0.25) + Scalar(0.25) * ei_abs2(cotan));
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cos__ = sin__ * cotan;
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@ -122,7 +110,7 @@ L70:
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}
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goto L100;
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L90:
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tan__ = w[j] / s[jj];
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tan__ = w[j] / s(j-1,j-1);
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/* Computing 2nd power */
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cos__ = Scalar(.5) / ei_sqrt(Scalar(0.25) + Scalar(0.25) * ei_abs2(tan__));
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sin__ = cos__ * tan__;
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@ -131,13 +119,10 @@ L100:
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/* apply the transformation to s and reduce the spike in w. */
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l = jj;
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for (i = j; i <= m; ++i) {
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temp = cos__ * s[l] + sin__ * w[i];
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w[i] = -sin__ * s[l] + cos__ * w[i];
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s[l] = temp;
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++l;
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/* L110: */
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temp = cos__ * s(j-1,i-1) + sin__ * w[i];
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w[i] = -sin__ * s(j-1,i-1) + cos__ * w[i];
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s(j-1,i-1) = temp;
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}
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/* store the information necessary to recover the */
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@ -148,28 +133,17 @@ L120:
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/* test for zero diagonal elements in the output s. */
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if (s[jj] == 0.) {
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if (s(j-1,j-1) == 0.) {
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*sing = true;
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}
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jj += m - j + 1;
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/* L130: */
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}
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L140:
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/* move w back into the last column of the output s. */
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s(n-1,n-1) = w[n];
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l = jj;
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for (i = n; i <= m; ++i) {
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s[l] = w[i];
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++l;
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/* L150: */
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}
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if (s[jj] == 0.) {
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if (s(j-1,j-1) == 0.) {
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*sing = true;
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}
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return;
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/* last card of subroutine r1updt. */
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} /* r1updt_ */
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}
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