libeigen/eigen!2617 Co-authored-by: Rasmus Munk Larsen <rmlarsen@gmail.com>
377 lines
19 KiB
C++
377 lines
19 KiB
C++
// This file is part of Eigen, a lightweight C++ template library
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// for linear algebra.
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//
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// Copyright (C) 2026 Rasmus Munk Larsen <rmlarsen@gmail.com>
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//
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// This Source Code Form is subject to the terms of the Mozilla
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// Public License v. 2.0. If a copy of the MPL was not distributed
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// with this file, You can obtain one at http://mozilla.org/MPL/2.0/.
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// SPDX-License-Identifier: MPL-2.0
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#include "main.h"
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#include "tridiag_test_matrices.h"
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#include <limits>
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#include <Eigen/Eigenvalues>
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// Test TridiagonalEigenSolver (SIMD Sturm-sequence spectral bisection) on the full
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// structured-tridiagonal catalog: compare against the implicit-QR path of
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// SelfAdjointEigenSolver::computeFromTridiagonal(), exercise index/value range subset
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// selection, and verify absolute accuracy against matrices with known spectra.
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template <typename RealScalar>
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void tridiagonal_eigensolver_bisection() {
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typedef Matrix<RealScalar, Dynamic, Dynamic> MatrixType;
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typedef Matrix<RealScalar, Dynamic, 1> VectorType;
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const RealScalar eps = NumTraits<RealScalar>::epsilon();
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const RealScalar tiny = (std::numeric_limits<RealScalar>::min)();
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// (a) Compare bisection against the QR path over every structured matrix, and exercise
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// index- and value-range subset selection.
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test::for_all_symmetric_tridiag_test_matrices<RealScalar>([&](const VectorType& diag, const VectorType& offdiag) {
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const Index n = diag.size();
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SelfAdjointEigenSolver<MatrixType> qr;
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qr.computeFromTridiagonal(diag, offdiag, EigenvaluesOnly);
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if (qr.info() != Success) return; // skip pathological inputs the QR path itself rejects
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const VectorType w = qr.eigenvalues();
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TridiagonalEigenSolver<RealScalar> bz;
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bz.computeEigenvalues(diag, offdiag);
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VERIFY_IS_EQUAL(bz.info(), Success);
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VERIFY_IS_EQUAL(bz.eigenvalues().size(), n);
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for (Index i = 1; i < n; ++i) VERIFY(bz.eigenvalues()(i) >= bz.eigenvalues()(i - 1));
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// Bisection has an absolute accuracy floor of ~pivmin (the smallest safe pivot),
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// so the tolerance carries an absolute term in addition to the eps*||T|| term.
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const RealScalar radius = w.cwiseAbs().maxCoeff();
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const RealScalar tol = RealScalar(64) * RealScalar(n) * (eps * radius + tiny);
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VERIFY((bz.eigenvalues() - w).cwiseAbs().maxCoeff() <= tol);
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// Index-range subsets: the k smallest and the k largest.
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if (n >= 4) {
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const Index k = n / 3;
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TridiagonalEigenSolver<RealScalar> lo, hi;
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lo.computeEigenvalues(diag, offdiag, EigenvalueRange::indices(0, k));
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VERIFY_IS_EQUAL(lo.eigenvalues().size(), k);
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VERIFY((lo.eigenvalues() - w.head(k)).cwiseAbs().maxCoeff() <= tol);
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hi.computeEigenvalues(diag, offdiag, EigenvalueRange::indices(n - k, n));
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VERIFY_IS_EQUAL(hi.eigenvalues().size(), k);
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VERIFY((hi.eigenvalues() - w.tail(k)).cwiseAbs().maxCoeff() <= tol);
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}
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// Value-range subset [vl, vu) about the spectrum center. The count is compared strictly
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// only when no eigenvalue sits within tol of a boundary (otherwise it is legitimately
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// ambiguous which side the boundary eigenvalue falls on).
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if (n >= 2 && radius > tiny) {
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const RealScalar vl = -RealScalar(0.3) * radius, vu = RealScalar(0.3) * radius;
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TridiagonalEigenSolver<RealScalar> bv;
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bv.computeEigenvalues(diag, offdiag, EigenvalueRange::values(double(vl), double(vu)));
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for (Index i = 0; i < bv.eigenvalues().size(); ++i)
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VERIFY(bv.eigenvalues()(i) >= vl - tol && bv.eigenvalues()(i) < vu + tol);
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const bool clean = (w.array() - vl).abs().minCoeff() > tol && (w.array() - vu).abs().minCoeff() > tol;
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if (clean) {
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const Index expected = (w.array() >= vl && w.array() < vu).count();
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VERIFY_IS_EQUAL(bv.eigenvalues().size(), expected);
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if (expected > 0) {
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Index first = 0;
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while (first < n && w(first) < vl) ++first;
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VERIFY((bv.eigenvalues() - w.segment(first, expected)).cwiseAbs().maxCoeff() <= tol);
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}
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}
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}
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});
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// (a2) Half-open value-range convention, fixed-size inputs, and input validation.
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{
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// values(vl, vu) selects the eigenvalues in the lower-closed, upper-open interval [vl, vu) (like
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// indices()): an eigenvalue exactly equal to vl is included, one exactly equal to vu is not. Use a
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// diagonal matrix (zero off-diagonal) with the exact integer spectrum {1, 2, 3} so the endpoints
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// land precisely on eigenvalues.
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VectorType d(3), e(2);
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d << RealScalar(1), RealScalar(2), RealScalar(3);
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e.setZero();
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TridiagonalEigenSolver<RealScalar> bmid;
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bmid.computeEigenvalues(d, e, EigenvalueRange::values(1.0L, 3.0L));
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VERIFY_IS_EQUAL(bmid.eigenvalues().size(), Index(2)); // [1, 3) = {1, 2}: lower end closed, upper end open
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VERIFY_IS_APPROX(bmid.eigenvalues()(0), RealScalar(1));
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VERIFY_IS_APPROX(bmid.eigenvalues()(1), RealScalar(2));
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TridiagonalEigenSolver<RealScalar> bopen;
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bopen.computeEigenvalues(d, e, EigenvalueRange::values(0.0L, 1.0L));
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VERIFY_IS_EQUAL(bopen.eigenvalues().size(), Index(0)); // [0, 1) excludes the eigenvalue at the open end 1
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TridiagonalEigenSolver<RealScalar> blow;
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blow.computeEigenvalues(d, e, EigenvalueRange::values(1.0L, 2.0L));
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VERIFY_IS_EQUAL(blow.eigenvalues().size(), Index(1)); // [1, 2) = {1}: includes the eigenvalue at the closed end 1
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VERIFY_IS_APPROX(blow.eigenvalues()(0), RealScalar(1));
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// Fixed-size input vectors work, including subset selection (the solver's own storage is
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// dynamic, so a subset shorter than the input is not a problem).
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Matrix<RealScalar, 3, 1> fd;
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fd << RealScalar(1), RealScalar(2), RealScalar(3);
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Matrix<RealScalar, 2, 1> fe;
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fe.setZero();
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TridiagonalEigenSolver<RealScalar> fz;
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fz.computeEigenvalues(fd, fe);
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VERIFY_IS_EQUAL(fz.eigenvalues().size(), Index(3));
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fz.computeEigenvalues(fd, fe, EigenvalueRange::indices(0, 1));
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VERIFY_IS_EQUAL(fz.eigenvalues().size(), Index(1));
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VERIFY_IS_APPROX(fz.eigenvalues()(0), RealScalar(1));
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// Querying an uninitialized solver is a usage error.
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TridiagonalEigenSolver<RealScalar> uninit;
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VERIFY_RAISES_ASSERT(uninit.eigenvalues());
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VERIFY_RAISES_ASSERT(uninit.info());
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// A non-finite input (NaN or Inf, diagonal or sub-diagonal) is rejected up front and
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// reported via info().
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VectorType dbad = d;
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dbad(1) = std::numeric_limits<RealScalar>::quiet_NaN();
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TridiagonalEigenSolver<RealScalar> bnan;
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bnan.computeEigenvalues(dbad, e);
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VERIFY_IS_EQUAL(bnan.info(), NoConvergence);
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dbad(1) = std::numeric_limits<RealScalar>::infinity();
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bnan.computeEigenvalues(dbad, e);
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VERIFY_IS_EQUAL(bnan.info(), NoConvergence);
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VectorType ebad = e;
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ebad(0) = std::numeric_limits<RealScalar>::quiet_NaN();
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bnan.computeEigenvalues(d, ebad);
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VERIFY_IS_EQUAL(bnan.info(), NoConvergence);
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}
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// (b) Absolute-accuracy checks against matrices with known spectra (independent of QR).
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// A subnormal-magnitude matrix exercises the normalization: dividing entries by the (subnormal) max
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// magnitude keeps the scaled matrix O(1), whereas multiplying by 1/scale would overflow to infinity
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// and return wrong eigenvalues. Compare against the same matrix in a normal range, scaled back down.
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{
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const Index nn = 7;
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VectorType bd(nn), be(nn - 1);
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test::tridiag_1_2_1(bd, be);
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const RealScalar sub_scale = (std::numeric_limits<RealScalar>::min)() / RealScalar(64); // subnormal
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TridiagonalEigenSolver<RealScalar> bref, bsub;
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bref.computeEigenvalues(bd, be);
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bsub.computeEigenvalues(VectorType(bd * sub_scale), VectorType(be * sub_scale));
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VERIFY_IS_EQUAL(bsub.info(), Success);
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// The subnormal eigenvalues, scaled back to O(1), agree with the reference to the subnormal
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// granularity at this magnitude (denorm_min / sub_scale) plus the usual bisection error.
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const RealScalar radius = bref.eigenvalues().cwiseAbs().maxCoeff();
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const RealScalar gran = (std::numeric_limits<RealScalar>::denorm_min)() / sub_scale;
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VERIFY((bsub.eigenvalues() / sub_scale - bref.eigenvalues()).cwiseAbs().maxCoeff() <=
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RealScalar(16) * (RealScalar(nn) * eps + gran) * radius);
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}
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const double pi = 3.14159265358979323846;
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for (Index n : {7, 16, 33, 64}) {
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VectorType d(n), e(n - 1), wexact(n);
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// 1-2-1 Toeplitz: lambda_k = 2 - 2 cos(k*pi/(n+1)), ascending for k = 1..n.
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test::tridiag_1_2_1(d, e);
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TridiagonalEigenSolver<RealScalar> b121;
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b121.computeEigenvalues(d, e);
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for (Index k = 0; k < n; ++k) wexact(k) = RealScalar(2.0 - 2.0 * std::cos(double(k + 1) * pi / double(n + 1)));
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VERIFY((b121.eigenvalues() - wexact).cwiseAbs().maxCoeff() <= RealScalar(64) * RealScalar(n) * eps * RealScalar(4));
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// Clement / Kac: integer spectrum -(n-1), -(n-3), ..., (n-1).
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test::tridiag_clement(d, e);
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TridiagonalEigenSolver<RealScalar> bcl;
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bcl.computeEigenvalues(d, e);
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for (Index k = 0; k < n; ++k) wexact(k) = RealScalar(-(n - 1) + 2 * k);
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VERIFY((bcl.eigenvalues() - wexact).cwiseAbs().maxCoeff() <= RealScalar(64) * RealScalar(n) * eps * RealScalar(n));
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// Spectra exactly symmetric about 0: signed Wilkinson, Hermite, Legendre, [1,0,1] Toeplitz.
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auto check_symmetric = [&](const VectorType& dd, const VectorType& ee) {
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TridiagonalEigenSolver<RealScalar> bs;
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bs.computeEigenvalues(dd, ee);
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const VectorType s = bs.eigenvalues();
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const RealScalar rad = s.cwiseAbs().maxCoeff();
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const RealScalar tol = RealScalar(64) * RealScalar(n) * (eps * rad + tiny);
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for (Index i = 0; i < n; ++i) VERIFY(numext::abs(s(i) + s(n - 1 - i)) <= tol);
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};
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test::tridiag_wilkinson_signed(d, e);
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check_symmetric(d, e);
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test::tridiag_hermite(d, e);
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check_symmetric(d, e);
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test::tridiag_legendre(d, e);
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check_symmetric(d, e);
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test::tridiag_toeplitz(d, e); // default a = 1, b = 0
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check_symmetric(d, e);
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}
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}
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// Test the inverse-iteration eigenvector stage (LAPACK xSTEIN analog): staged
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// (computeEigenvalues() followed by computeEigenvectors()), one-call compute(), and the direct
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// computeEigenvectors(diag, subdiag, eigenvalues) API.
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template <typename RealScalar>
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void tridiagonal_eigensolver_eigenvectors() {
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typedef Matrix<RealScalar, Dynamic, Dynamic> MatrixType;
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typedef Matrix<RealScalar, Dynamic, 1> VectorType;
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const RealScalar eps = NumTraits<RealScalar>::epsilon();
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const RealScalar tiny = (std::numeric_limits<RealScalar>::min)();
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const double pi = 3.14159265358979323846;
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// (a) Eigenvectors over the structured catalog: staged and direct APIs.
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test::for_all_symmetric_tridiag_test_matrices<RealScalar>([&](const VectorType& diag, const VectorType& offdiag) {
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const Index n = diag.size();
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// Dense form of T for residual / reconstruction checks.
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MatrixType T = MatrixType::Zero(n, n);
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T.diagonal() = diag;
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if (n > 1) {
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T.diagonal(-1) = offdiag;
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T.diagonal(1) = offdiag;
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}
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RealScalar scale = T.cwiseAbs().maxCoeff();
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if (!(numext::isfinite)(scale)) return; // skip non-finite inputs, like the eigenvalue path
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if (numext::is_exactly_zero(scale)) scale = RealScalar(1);
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TridiagonalEigenSolver<RealScalar> es;
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es.computeEigenvalues(diag, offdiag);
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if (es.info() != Success) return;
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es.computeEigenvectors(); // staged inverse-iteration pass
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VERIFY_IS_EQUAL(es.info(), Success);
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const VectorType w = es.eigenvalues();
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const MatrixType V = es.eigenvectors();
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VERIFY_IS_EQUAL(V.rows(), n);
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VERIFY_IS_EQUAL(V.cols(), n);
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const RealScalar tol = RealScalar(128) * RealScalar(n) * (eps * scale + tiny);
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const RealScalar otol = RealScalar(128) * RealScalar(n) * eps;
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// Per-column residual; stableNorm() since the catalog includes near-overflow entries.
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for (Index i = 0; i < n; ++i) VERIFY((T * V.col(i) - w(i) * V.col(i)).stableNorm() <= tol);
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// Orthonormality and full-spectrum reconstruction (the latter in scaled coordinates so the
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// extreme-magnitude catalog entries cannot overflow the products).
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VERIFY((V.transpose() * V - MatrixType::Identity(n, n)).cwiseAbs().maxCoeff() <= otol);
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const RealScalar recon =
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((V * (w / scale).asDiagonal() * V.transpose()) - (T / scale)).cwiseAbs().maxCoeff() * scale;
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VERIFY(recon <= tol);
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// The one-call compute() reproduces the staged result exactly.
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TridiagonalEigenSolver<RealScalar> onecall;
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onecall.compute(diag, offdiag);
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VERIFY_IS_EQUAL(onecall.info(), Success);
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VERIFY_IS_EQUAL((onecall.eigenvalues() - w).cwiseAbs().maxCoeff(), RealScalar(0));
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VERIFY_IS_EQUAL((onecall.eigenvectors() - V).cwiseAbs().maxCoeff(), RealScalar(0));
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// The direct API reproduces the staged result exactly (same eigenvalues -> same deterministic vectors).
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TridiagonalEigenSolver<RealScalar> dir;
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dir.computeEigenvectors(diag, offdiag, w);
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VERIFY_IS_EQUAL(dir.eigenvectors().rows(), n);
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VERIFY_IS_EQUAL(dir.eigenvectors().cols(), n);
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VERIFY_IS_EQUAL((dir.eigenvectors() - V).cwiseAbs().maxCoeff(), RealScalar(0));
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// Index-subset eigenvectors: the bisection range selects a band, inverse iteration produces just
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// those columns; check residual and that they are orthonormal among themselves.
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if (n >= 4) {
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const Index il = n / 4, iu = n - n / 4;
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TridiagonalEigenSolver<RealScalar> sub;
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sub.compute(diag, offdiag, ComputeEigenvectors, EigenvalueRange::indices(il, iu));
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const MatrixType Vs = sub.eigenvectors();
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const VectorType ws = sub.eigenvalues();
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VERIFY_IS_EQUAL(Vs.rows(), n);
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VERIFY_IS_EQUAL(Vs.cols(), iu - il);
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for (Index k = 0; k < iu - il; ++k) VERIFY((T * Vs.col(k) - ws(k) * Vs.col(k)).stableNorm() <= tol);
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VERIFY((Vs.transpose() * Vs - MatrixType::Identity(iu - il, iu - il)).cwiseAbs().maxCoeff() <= otol);
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}
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});
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// (b) Closed-form 1-2-1 Toeplitz eigenvectors: v_k(j) = sin(j*(n-k)*pi/(n+1)) for the k-th
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// (ascending) eigenvalue. An analytic, solver-independent check of the inverse-iteration vectors.
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for (Index n : {5, 16, 33, 64}) {
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VectorType d(n), e(n - 1);
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test::tridiag_1_2_1(d, e);
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TridiagonalEigenSolver<RealScalar> es(d, e);
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const MatrixType V = es.eigenvectors();
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for (Index k = 0; k < n; ++k) {
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VectorType exact(n);
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for (Index j = 0; j < n; ++j) exact(j) = RealScalar(std::sin(double(j + 1) * double(n - k) * pi / double(n + 1)));
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exact.normalize();
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const RealScalar err = (std::min)((V.col(k) - exact).norm(), (V.col(k) + exact).norm());
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VERIFY(err <= RealScalar(256) * RealScalar(n) * eps);
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}
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}
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// (c) Edge cases: fixed-size inputs, eigenvalues-only requests, subnormal-magnitude matrices,
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// and convergence reporting.
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{
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// Fixed-size input vectors work for the full eigendecomposition and for subsets (the solver's
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// own storage is dynamic).
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Matrix<RealScalar, 4, 1> fdiag = Matrix<RealScalar, 4, 1>::Random();
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Matrix<RealScalar, 3, 1> fsub = Matrix<RealScalar, 3, 1>::Random();
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TridiagonalEigenSolver<RealScalar> fz;
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fz.compute(fdiag, fsub);
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VERIFY_IS_EQUAL(fz.info(), Success);
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VERIFY_IS_EQUAL(fz.eigenvectors().cols(), Index(4));
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{
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MatrixType Tf = MatrixType::Zero(4, 4);
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Tf.diagonal() = fdiag;
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Tf.diagonal(-1) = fsub;
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Tf.diagonal(1) = fsub;
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const MatrixType Vf = fz.eigenvectors();
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VERIFY((Vf.transpose() * Vf - MatrixType::Identity(4, 4)).cwiseAbs().maxCoeff() <= RealScalar(64) * eps);
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VERIFY((Tf * Vf - Vf * fz.eigenvalues().asDiagonal()).cwiseAbs().maxCoeff() <=
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RealScalar(64) * eps * Tf.cwiseAbs().maxCoeff());
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}
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// An EigenvaluesOnly compute() does not produce eigenvectors; querying them is a usage error,
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// and the staged computeEigenvectors() supplies them afterwards.
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TridiagonalEigenSolver<RealScalar> staged;
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staged.compute(fdiag, fsub, EigenvaluesOnly);
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VERIFY_IS_EQUAL(staged.info(), Success);
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VERIFY_RAISES_ASSERT(staged.eigenvectors());
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staged.computeEigenvectors();
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VERIFY_IS_EQUAL(staged.info(), Success);
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VERIFY_IS_EQUAL((staged.eigenvectors() - fz.eigenvectors()).cwiseAbs().maxCoeff(), RealScalar(0));
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// A matrix whose entries are all subnormal must still yield genuine unit-norm, orthonormal
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// eigenvectors rather than all-zero columns. Inverse iteration normalizes the tridiagonal by
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// dividing its entries directly by the largest magnitude; doing so (rather than multiplying by its
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// reciprocal) keeps the normalization finite even when that magnitude is subnormal, where 1/scale
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// overflows to infinity and would otherwise let the iterate underflow to zero. The eigenvalues are
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// taken from the same matrix in a normal magnitude range (then scaled back down), so this exercises
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// the eigenvector normalization in isolation from the eigenvalue solver.
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{
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const Index n = 6;
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VectorType base_d(n), base_e(n - 1);
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test::tridiag_1_2_1(base_d, base_e);
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// sub_scale is subnormal and small enough that 1/sub_scale overflows to infinity.
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const RealScalar sub_scale = (std::numeric_limits<RealScalar>::min)() / RealScalar(64);
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const VectorType d = base_d * sub_scale, e = base_e * sub_scale;
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TridiagonalEigenSolver<RealScalar> ref;
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ref.computeEigenvalues(base_d, base_e);
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const VectorType w_sub = ref.eigenvalues() * sub_scale;
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TridiagonalEigenSolver<RealScalar> se;
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se.computeEigenvectors(d, e, w_sub);
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VERIFY_IS_EQUAL(se.info(), Success);
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const MatrixType V = se.eigenvectors();
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for (Index i = 0; i < n; ++i)
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VERIFY(numext::abs(V.col(i).norm() - RealScalar(1)) <= RealScalar(64) * eps); // unit norm, not all-zero
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VERIFY((V.transpose() * V - MatrixType::Identity(n, n)).cwiseAbs().maxCoeff() <=
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RealScalar(64) * RealScalar(n) * eps);
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// Residual in normal-range coordinates (the eigenvectors are invariant under the uniform scale).
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MatrixType Tn = MatrixType::Zero(n, n);
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Tn.diagonal() = base_d;
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Tn.diagonal(-1) = base_e;
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Tn.diagonal(1) = base_e;
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for (Index i = 0; i < n; ++i)
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|
VERIFY((Tn * V.col(i) - ref.eigenvalues()(i) * V.col(i)).norm() <= RealScalar(256) * RealScalar(n) * eps);
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|
}
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|
|
|
// Convergence is reported through info() rather than hard-coded to Success: inverse iteration
|
|
// counts the eigenvectors that fail to converge within its step limit (cf. LAPACK xSTEIN), and a
|
|
// well-conditioned spectrum converges fully, so that count is zero and info() is Success.
|
|
{
|
|
const Index n = 32;
|
|
VectorType d = VectorType::Random(n), e = VectorType::Random(n - 1);
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|
TridiagonalEigenSolver<RealScalar> es2(d, e);
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|
VERIFY_IS_EQUAL(es2.info(), Success);
|
|
}
|
|
}
|
|
}
|
|
|
|
EIGEN_DECLARE_TEST(tridiagonal_eigensolver) {
|
|
for (int i = 0; i < g_repeat; i++) {
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|
CALL_SUBTEST_1(tridiagonal_eigensolver_bisection<double>());
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|
CALL_SUBTEST_2(tridiagonal_eigensolver_bisection<float>());
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|
CALL_SUBTEST_3(tridiagonal_eigensolver_eigenvectors<double>());
|
|
CALL_SUBTEST_4(tridiagonal_eigensolver_eigenvectors<float>());
|
|
}
|
|
}
|