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@sgratzl/science

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Scientific and statistical computing in JavaScript.

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import hypot from '../core/hypot'; export default function decompose() { function decompose(A) { var n = A.length, // column dimension V = [], d = [], e = []; for (var i = 0; i < n; i++) { V[i] = []; d[i] = []; e[i] = []; } var symmetric = true; for (var j = 0; j < n; j++) { for (var i = 0; i < n; i++) { if (A[i][j] !== A[j][i]) { symmetric = false; break; } } } if (symmetric) { for (var i = 0; i < n; i++) V[i] = A[i].slice(); // Tridiagonalize. science_lin_decomposeTred2(d, e, V); // Diagonalize. science_lin_decomposeTql2(d, e, V); } else { var H = []; for (var i = 0; i < n; i++) H[i] = A[i].slice(); // Reduce to Hessenberg form. science_lin_decomposeOrthes(H, V); // Reduce Hessenberg to real Schur form. science_lin_decomposeHqr2(d, e, H, V); } var D = []; for (var i = 0; i < n; i++) { var row = D[i] = []; for (var j = 0; j < n; j++) row[j] = i === j ? d[i] : 0; D[i][e[i] > 0 ? i + 1 : i - 1] = e[i]; } return {D: D, V: V}; } return decompose; }; // Symmetric Householder reduction to tridiagonal form. function science_lin_decomposeTred2(d, e, V) { // This is derived from the Algol procedures tred2 by // Bowdler, Martin, Reinsch, and Wilkinson, Handbook for // Auto. Comp., Vol.ii-Linear Algebra, and the corresponding // Fortran subroutine in EISPACK. var n = V.length; for (var j = 0; j < n; j++) d[j] = V[n - 1][j]; // Householder reduction to tridiagonal form. for (var i = n - 1; i > 0; i--) { // Scale to avoid under/overflow. var scale = 0, h = 0; for (var k = 0; k < i; k++) scale += Math.abs(d[k]); if (scale === 0) { e[i] = d[i - 1]; for (var j = 0; j < i; j++) { d[j] = V[i - 1][j]; V[i][j] = 0; V[j][i] = 0; } } else { // Generate Householder vector. for (var k = 0; k < i; k++) { d[k] /= scale; h += d[k] * d[k]; } var f = d[i - 1]; var g = Math.sqrt(h); if (f > 0) g = -g; e[i] = scale * g; h = h - f * g; d[i - 1] = f - g; for (var j = 0; j < i; j++) e[j] = 0; // Apply similarity transformation to remaining columns. for (var j = 0; j < i; j++) { f = d[j]; V[j][i] = f; g = e[j] + V[j][j] * f; for (var k = j+1; k <= i - 1; k++) { g += V[k][j] * d[k]; e[k] += V[k][j] * f; } e[j] = g; } f = 0; for (var j = 0; j < i; j++) { e[j] /= h; f += e[j] * d[j]; } var hh = f / (h + h); for (var j = 0; j < i; j++) e[j] -= hh * d[j]; for (var j = 0; j < i; j++) { f = d[j]; g = e[j]; for (var k = j; k <= i - 1; k++) V[k][j] -= (f * e[k] + g * d[k]); d[j] = V[i - 1][j]; V[i][j] = 0; } } d[i] = h; } // Accumulate transformations. for (var i = 0; i < n - 1; i++) { V[n - 1][i] = V[i][i]; V[i][i] = 1.0; var h = d[i + 1]; if (h != 0) { for (var k = 0; k <= i; k++) d[k] = V[k][i + 1] / h; for (var j = 0; j <= i; j++) { var g = 0; for (var k = 0; k <= i; k++) g += V[k][i + 1] * V[k][j]; for (var k = 0; k <= i; k++) V[k][j] -= g * d[k]; } } for (var k = 0; k <= i; k++) V[k][i + 1] = 0; } for (var j = 0; j < n; j++) { d[j] = V[n - 1][j]; V[n - 1][j] = 0; } V[n - 1][n - 1] = 1; e[0] = 0; } // Symmetric tridiagonal QL algorithm. function science_lin_decomposeTql2(d, e, V) { // This is derived from the Algol procedures tql2, by // Bowdler, Martin, Reinsch, and Wilkinson, Handbook for // Auto. Comp., Vol.ii-Linear Algebra, and the corresponding // Fortran subroutine in EISPACK. var n = V.length; for (var i = 1; i < n; i++) e[i - 1] = e[i]; e[n - 1] = 0; var f = 0; var tst1 = 0; var eps = 1e-12; for (var l = 0; l < n; l++) { // Find small subdiagonal element tst1 = Math.max(tst1, Math.abs(d[l]) + Math.abs(e[l])); var m = l; while (m < n) { if (Math.abs(e[m]) <= eps*tst1) { break; } m++; } // If m == l, d[l] is an eigenvalue, // otherwise, iterate. if (m > l) { var iter = 0; do { iter++; // (Could check iteration count here.) // Compute implicit shift var g = d[l]; var p = (d[l + 1] - g) / (2 * e[l]); var r = hypot(p, 1); if (p < 0) r = -r; d[l] = e[l] / (p + r); d[l + 1] = e[l] * (p + r); var dl1 = d[l + 1]; var h = g - d[l]; for (var i = l+2; i < n; i++) d[i] -= h; f += h; // Implicit QL transformation. p = d[m]; var c = 1; var c2 = c; var c3 = c; var el1 = e[l + 1]; var s = 0; var s2 = 0; for (var i = m - 1; i >= l; i--) { c3 = c2; c2 = c; s2 = s; g = c * e[i]; h = c * p; r = hypot(p,e[i]); e[i + 1] = s * r; s = e[i] / r; c = p / r; p = c * d[i] - s * g; d[i + 1] = h + s * (c * g + s * d[i]); // Accumulate transformation. for (var k = 0; k < n; k++) { h = V[k][i + 1]; V[k][i + 1] = s * V[k][i] + c * h; V[k][i] = c * V[k][i] - s * h; } } p = -s * s2 * c3 * el1 * e[l] / dl1; e[l] = s * p; d[l] = c * p; // Check for convergence. } while (Math.abs(e[l]) > eps*tst1); } d[l] = d[l] + f; e[l] = 0; } // Sort eigenvalues and corresponding vectors. for (var i = 0; i < n - 1; i++) { var k = i; var p = d[i]; for (var j = i + 1; j < n; j++) { if (d[j] < p) { k = j; p = d[j]; } } if (k != i) { d[k] = d[i]; d[i] = p; for (var j = 0; j < n; j++) { p = V[j][i]; V[j][i] = V[j][k]; V[j][k] = p; } } } } // Nonsymmetric reduction to Hessenberg form. function science_lin_decomposeOrthes(H, V) { // This is derived from the Algol procedures orthes and ortran, // by Martin and Wilkinson, Handbook for Auto. Comp., // Vol.ii-Linear Algebra, and the corresponding // Fortran subroutines in EISPACK. var n = H.length; var ort = []; var low = 0; var high = n - 1; for (var m = low + 1; m < high; m++) { // Scale column. var scale = 0; for (var i = m; i <= high; i++) scale += Math.abs(H[i][m - 1]); if (scale !== 0) { // Compute Householder transformation. var h = 0; for (var i = high; i >= m; i--) { ort[i] = H[i][m - 1] / scale; h += ort[i] * ort[i]; } var g = Math.sqrt(h); if (ort[m] > 0) g = -g; h = h - ort[m] * g; ort[m] = ort[m] - g; // Apply Householder similarity transformation // H = (I-u*u'/h)*H*(I-u*u')/h) for (var j = m; j < n; j++) { var f = 0; for (var i = high; i >= m; i--) f += ort[i] * H[i][j]; f /= h; for (var i = m; i <= high; i++) H[i][j] -= f * ort[i]; } for (var i = 0; i <= high; i++) { var f = 0; for (var j = high; j >= m; j--) f += ort[j] * H[i][j]; f /= h; for (var j = m; j <= high; j++) H[i][j] -= f * ort[j]; } ort[m] = scale * ort[m]; H[m][m - 1] = scale * g; } } // Accumulate transformations (Algol's ortran). for (var i = 0; i < n; i++) { for (var j = 0; j < n; j++) V[i][j] = i === j ? 1 : 0; } for (var m = high-1; m >= low+1; m--) { if (H[m][m - 1] !== 0) { for (var i = m + 1; i <= high; i++) ort[i] = H[i][m - 1]; for (var j = m; j <= high; j++) { var g = 0; for (var i = m; i <= high; i++) g += ort[i] * V[i][j]; // Double division avoids possible underflow g = (g / ort[m]) / H[m][m - 1]; for (var i = m; i <= high; i++) V[i][j] += g * ort[i]; } } } } // Nonsymmetric reduction from Hessenberg to real Schur form. function science_lin_decomposeHqr2(d, e, H, V) { // This is derived from the Algol procedure hqr2, // by Martin and Wilkinson, Handbook for Auto. Comp., // Vol.ii-Linear Algebra, and the corresponding // Fortran subroutine in EISPACK. var nn = H.length, n = nn - 1, low = 0, high = nn - 1, eps = 1e-12, exshift = 0, p = 0, q = 0, r = 0, s = 0, z = 0, t, w, x, y; // Store roots isolated by balanc and compute matrix norm var norm = 0; for (var i = 0; i < nn; i++) { if (i < low || i > high) { d[i] = H[i][i]; e[i] = 0; } for (var j = Math.max(i - 1, 0); j < nn; j++) norm += Math.abs(H[i][j]); } // Outer loop over eigenvalue index var iter = 0; while (n >= low) { // Look for single small sub-diagonal element var l = n; while (l > low) { s = Math.abs(H[l - 1][l - 1]) + Math.abs(H[l][l]); if (s === 0) s = norm; if (Math.abs(H[l][l - 1]) < eps * s) break; l--; } // Check for convergence // One root found if (l === n) { H[n][n] = H[n][n] + exshift; d[n] = H[n][n]; e[n] = 0; n--; iter = 0; // Two roots found } else if (l === n - 1) { w = H[n][n - 1] * H[n - 1][n]; p = (H[n - 1][n - 1] - H[n][n]) / 2; q = p * p + w; z = Math.sqrt(Math.abs(q)); H[n][n] = H[n][n] + exshift; H[n - 1][n - 1] = H[n - 1][n - 1] + exshift; x = H[n][n]; // Real pair if (q >= 0) { z = p + (p >= 0 ? z : -z); d[n - 1] = x + z; d[n] = d[n - 1]; if (z !== 0) d[n] = x - w / z; e[n - 1] = 0; e[n] = 0; x = H[n][n - 1]; s = Math.abs(x) + Math.abs(z); p = x / s; q = z / s; r = Math.sqrt(p * p+q * q); p /= r; q /= r; // Row modification for (var j = n - 1; j < nn; j++) { z = H[n - 1][j]; H[n - 1][j] = q * z + p * H[n][j]; H[n][j] = q * H[n][j] - p * z; } // Column modification for (var i = 0; i <= n; i++) { z = H[i][n - 1]; H[i][n - 1] = q * z + p * H[i][n]; H[i][n] = q * H[i][n] - p * z; } // Accumulate transformations for (var i = low; i <= high; i++) { z = V[i][n - 1]; V[i][n - 1] = q * z + p * V[i][n]; V[i][n] = q * V[i][n] - p * z; } // Complex pair } else { d[n - 1] = x + p; d[n] = x + p; e[n - 1] = z; e[n] = -z; } n = n - 2; iter = 0; // No convergence yet } else { // Form shift x = H[n][n]; y = 0; w = 0; if (l < n) { y = H[n - 1][n - 1]; w = H[n][n - 1] * H[n - 1][n]; } // Wilkinson's original ad hoc shift if (iter == 10) { exshift += x; for (var i = low; i <= n; i++) { H[i][i] -= x; } s = Math.abs(H[n][n - 1]) + Math.abs(H[n - 1][n-2]); x = y = 0.75 * s; w = -0.4375 * s * s; } // MATLAB's new ad hoc shift if (iter == 30) { s = (y - x) / 2.0; s = s * s + w; if (s > 0) { s = Math.sqrt(s); if (y < x) { s = -s; } s = x - w / ((y - x) / 2.0 + s); for (var i = low; i <= n; i++) { H[i][i] -= s; } exshift += s; x = y = w = 0.964; } } iter++; // (Could check iteration count here.) // Look for two consecutive small sub-diagonal elements var m = n-2; while (m >= l) { z = H[m][m]; r = x - z; s = y - z; p = (r * s - w) / H[m + 1][m] + H[m][m + 1]; q = H[m + 1][m + 1] - z - r - s; r = H[m+2][m + 1]; s = Math.abs(p) + Math.abs(q) + Math.abs(r); p = p / s; q = q / s; r = r / s; if (m == l) break; if (Math.abs(H[m][m - 1]) * (Math.abs(q) + Math.abs(r)) < eps * (Math.abs(p) * (Math.abs(H[m - 1][m - 1]) + Math.abs(z) + Math.abs(H[m + 1][m + 1])))) { break; } m--; } for (var i = m+2; i <= n; i++) { H[i][i-2] = 0; if (i > m+2) H[i][i-3] = 0; } // Double QR step involving rows l:n and columns m:n for (var k = m; k <= n - 1; k++) { var notlast = (k != n - 1); if (k != m) { p = H[k][k - 1]; q = H[k + 1][k - 1]; r = (notlast ? H[k + 2][k - 1] : 0); x = Math.abs(p) + Math.abs(q) + Math.abs(r); if (x != 0) { p /= x; q /= x; r /= x; } } if (x == 0) break; s = Math.sqrt(p * p + q * q + r * r); if (p < 0) { s = -s; } if (s != 0) { if (k != m) H[k][k - 1] = -s * x; else if (l != m) H[k][k - 1] = -H[k][k - 1]; p += s; x = p / s; y = q / s; z = r / s; q /= p; r /= p; // Row modification for (var j = k; j < nn; j++) { p = H[k][j] + q * H[k + 1][j]; if (notlast) { p = p + r * H[k + 2][j]; H[k + 2][j] = H[k + 2][j] - p * z; } H[k][j] = H[k][j] - p * x; H[k + 1][j] = H[k + 1][j] - p * y; } // Column modification for (var i = 0; i <= Math.min(n, k + 3); i++) { p = x * H[i][k] + y * H[i][k + 1]; if (notlast) { p += z * H[i][k + 2]; H[i][k + 2] = H[i][k + 2] - p * r; } H[i][k] = H[i][k] - p; H[i][k + 1] = H[i][k + 1] - p * q; } // Accumulate transformations for (var i = low; i <= high; i++) { p = x * V[i][k] + y * V[i][k + 1]; if (notlast) { p = p + z * V[i][k + 2]; V[i][k + 2] = V[i][k + 2] - p * r; } V[i][k] = V[i][k] - p; V[i][k + 1] = V[i][k + 1] - p * q; } } // (s != 0) } // k loop } // check convergence } // while (n >= low) // Backsubstitute to find vectors of upper triangular form if (norm == 0) { return; } for (n = nn - 1; n >= 0; n--) { p = d[n]; q = e[n]; // Real vector if (q == 0) { var l = n; H[n][n] = 1.0; for (var i = n - 1; i >= 0; i--) { w = H[i][i] - p; r = 0; for (var j = l; j <= n; j++) { r = r + H[i][j] * H[j][n]; } if (e[i] < 0) { z = w; s = r; } else { l = i; if (e[i] === 0) { H[i][n] = -r / (w !== 0 ? w : eps * norm); } else { // Solve real equations x = H[i][i + 1]; y = H[i + 1][i]; q = (d[i] - p) * (d[i] - p) + e[i] * e[i]; t = (x * s - z * r) / q; H[i][n] = t; if (Math.abs(x) > Math.abs(z)) { H[i + 1][n] = (-r - w * t) / x; } else { H[i + 1][n] = (-s - y * t) / z; } } // Overflow control t = Math.abs(H[i][n]); if ((eps * t) * t > 1) { for (var j = i; j <= n; j++) H[j][n] = H[j][n] / t; } } } // Complex vector } else if (q < 0) { var l = n - 1; // Last vector component imaginary so matrix is triangular if (Math.abs(H[n][n - 1]) > Math.abs(H[n - 1][n])) { H[n - 1][n - 1] = q / H[n][n - 1]; H[n - 1][n] = -(H[n][n] - p) / H[n][n - 1]; } else { var zz = science_lin_decomposeCdiv(0, -H[n - 1][n], H[n - 1][n - 1] - p, q); H[n - 1][n - 1] = zz[0]; H[n - 1][n] = zz[1]; } H[n][n - 1] = 0; H[n][n] = 1; for (var i = n-2; i >= 0; i--) { var ra = 0, sa = 0, vr, vi; for (var j = l; j <= n; j++) { ra = ra + H[i][j] * H[j][n - 1]; sa = sa + H[i][j] * H[j][n]; } w = H[i][i] - p; if (e[i] < 0) { z = w; r = ra; s = sa; } else { l = i; if (e[i] == 0) { var zz = science_lin_decomposeCdiv(-ra,-sa,w,q); H[i][n - 1] = zz[0]; H[i][n] = zz[1]; } else { // Solve complex equations x = H[i][i + 1]; y = H[i + 1][i]; vr = (d[i] - p) * (d[i] - p) + e[i] * e[i] - q * q; vi = (d[i] - p) * 2.0 * q; if (vr == 0 & vi == 0) { vr = eps * norm * (Math.abs(w) + Math.abs(q) + Math.abs(x) + Math.abs(y) + Math.abs(z)); } var zz = science_lin_decomposeCdiv(x*r-z*ra+q*sa,x*s-z*sa-q*ra,vr,vi); H[i][n - 1] = zz[0]; H[i][n] = zz[1]; if (Math.abs(x) > (Math.abs(z) + Math.abs(q))) { H[i + 1][n - 1] = (-ra - w * H[i][n - 1] + q * H[i][n]) / x; H[i + 1][n] = (-sa - w * H[i][n] - q * H[i][n - 1]) / x; } else { var zz = science_lin_decomposeCdiv(-r-y*H[i][n - 1],-s-y*H[i][n],z,q); H[i + 1][n - 1] = zz[0]; H[i + 1][n] = zz[1]; } } // Overflow control t = Math.max(Math.abs(H[i][n - 1]),Math.abs(H[i][n])); if ((eps * t) * t > 1) { for (var j = i; j <= n; j++) { H[j][n - 1] = H[j][n - 1] / t; H[j][n] = H[j][n] / t; } } } } } } // Vectors of isolated roots for (var i = 0; i < nn; i++) { if (i < low || i > high) { for (var j = i; j < nn; j++) V[i][j] = H[i][j]; } } // Back transformation to get eigenvectors of original matrix for (var j = nn - 1; j >= low; j--) { for (var i = low; i <= high; i++) { z = 0; for (var k = low; k <= Math.min(j, high); k++) z += V[i][k] * H[k][j]; V[i][j] = z; } } } // Complex scalar division. function science_lin_decomposeCdiv(xr, xi, yr, yi) { if (Math.abs(yr) > Math.abs(yi)) { var r = yi / yr, d = yr + r * yi; return [(xr + r * xi) / d, (xi - r * xr) / d]; } else { var r = yr / yi, d = yi + r * yr; return [(r * xr + xi) / d, (r * xi - xr) / d]; } }