DLAED1(3)
πΈ NAME πΈ
okay bestie, welcome to the DLAED1(3) manual page π
β this one is literally the home page for this file, straight from the Library Functions Manual:
/home/abuild/rpmbuild/BUILD/lapack-static-3.12.0-build/lapack-3.12.0/SRC/dlaed1.f
No cap. Itβs giving LAPACK subroutine energy, and weβre gonna get through every argument together π«Ά.
β¨ SYNOPSIS β¨
π§ Functions/Subroutines π§
subroutine DLAED1 (n, d, q, ldq, indxq, rho, cutpnt, work, iwork, info)βDLAED1is used byDSTEDC. Computes the updated eigensystem of a diagonal matrix after modification by a rank-one symmetric matrix. Used when the original matrix is tridiagonal. π
π Function/Subroutine Documentation π
π subroutine DLAED1 π
subroutine DLAED1 (integer n, double precision, dimension( * ) d, double
precision, dimension( ldq, * ) q, integer ldq, integer, dimension( * )
indxq, double precision rho, integer cutpnt, double precision,
dimension( * ) work, integer, dimension( * ) iwork, integer info)
DLAED1 used by DSTEDC. Computes the updated eigensystem of a diagonal matrix after modification by a rank-one symmetric matrix. Used when the original matrix is tridiagonal. (Yes, she said it twice β sheβs consistent, periodt.)
π Purpose π
okay so the whole vibe: DLAED1 computes the updated eigensystem of a diagonal matrix after modification by a rank-one symmetric matrix. This routine is used only for the eigenproblem which requires all eigenvalues and eigenvectors of a tridiagonal matrix. DLAED7 handles the case in which eigenvalues only or eigenvalues and eigenvectors of a full symmetric matrix (which was reduced to tridiagonal form) are desired. iykyk.
The equation is literally:
T = Q(in) ( D(in) + RHO * Z*Z**T ) Q**T(in) = Q(out) * D(out) * Q**T(out)
where Z = Q**T*u, u is a vector of length N with ones in the CUTPNT and CUTPNT + 1 th elements and zeros elsewhere.
The eigenvectors of the original matrix are stored in Q, and the eigenvalues are in D. The algorithm consists of three stages:
- The first stage consists of deflating the size of the problem when there are multiple eigenvalues or if there is a zero in the
Zvector. For each such occurrence the dimension of the secular equation problem is reduced by one. This stage is performed by the routineDLAED2. - The second stage consists of calculating the updated eigenvalues. This is done by finding the roots of the secular equation via the routine
DLAED4(as called byDLAED3). This routine also calculates the eigenvectors of the current problem. - The final stage consists of computing the updated eigenvectors directly using the updated eigenvalues. The eigenvectors for the current problem are multiplied with the eigenvectors from the overall problem.
π Parameters π
NβNisINTEGER. The dimension of the symmetric tridiagonal matrix.N >= 0.DβDisDOUBLE PRECISION array, dimension (N). On entry, the eigenvalues of the rank-1-perturbed matrix. On exit, the eigenvalues of the repaired matrix.QβQisDOUBLE PRECISION array, dimension (LDQ,N). On entry, the eigenvectors of the rank-1-perturbed matrix. On exit, the eigenvectors of the repaired tridiagonal matrix.LDQβLDQisINTEGER. The leading dimension of the arrayQ.LDQ >= max(1,N).INDXQβINDXQisINTEGER array, dimension (N). On entry, the permutation which separately sorts the two subproblems inDinto ascending order. On exit, the permutation which will reintegrate the subproblems back into sorted order, i.e.D( INDXQ( I = 1, N ) )will be in ascending order.RHOβRHOisDOUBLE PRECISION. The subdiagonal entry used to create the rank-1 modification.CUTPNTβCUTPNTisINTEGER. The location of the last eigenvalue in the leading sub-matrix.min(1,N) <= CUTPNT <= N/2.WORKβWORKisDOUBLE PRECISION array, dimension (4*N + N**2).IWORKβIWORKisINTEGER array, dimension (4*N).INFOβINFOisINTEGER.= 0: successful exit.< 0: ifINFO = -i, the i-th argument had an illegal value.> 0: ifINFO = 1, an eigenvalue did not converge.
π Author π
Univ. of Tennessee
Univ. of California Berkeley
Univ. of Colorado Denver
NAG Ltd.
π Contributors: π
Jeff Rutter, Computer Science Division, University of California at Berkeley, USA Modified by Francoise Tisseur, University of Tennessee
Definition at line 161 of file dlaed1.f.
π Author π
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