SRC/dlaqz0.f(3)
π NAME π
okay bestie, this page is SRC/dlaqz0.f β yes, the file name is the whole NAME section, iconic behavior fr fr. It's from the Library Functions Manual, and we're about to get into the recursive dlaqz0 subroutine. π«Ά
β¨ SYNOPSIS β¨
Functions/Subroutines
recursive subroutine dlaqz0 (wants, wantq, wantz, n, ilo, ihi, a, lda,
b, ldb, alphar, alphai, beta, q, ldq, z, ldz, work, lwork, rec,
info)
DLAQZ0
πΈ Function/Subroutine Documentation πΈ
Here's the full signature, bestie β keep it exactly like this:
recursive subroutine dlaqz0 (character, intent(in) wants, character, intent(in) wantq, character, intent(in) wantz, integer, intent(in) n, integer, intent(in) ilo, integer, intent(in) ihi, double precision, dimension( lda, * ), intent(inout) a, integer, intent(in) lda, double precision, dimension( ldb, * ), intent(inout) b, integer, intent(in) ldb, double precision, dimension( * ), intent(inout) alphar, double precision, dimension( * ), intent(inout) alphai, double precision, dimension( * ), intent(inout) beta, double precision, dimension( ldq, * ), intent(inout) q, integer, intent(in) ldq, double precision, dimension( ldz, * ), intent(inout) z, integer, intent(in) ldz, double precision, dimension( * ), intent(inout) work, integer, intent(in) lwork, integer, intent(in) rec, integer, intent(out) info)
DLAQZ0
π¦ Purpose π¦
Okay so DLAQZ0 computes the eigenvalues of a real matrix pair (H,T), where H is an upper Hessenberg matrix and T is upper triangular, using the double-shift QZ method. Matrix pairs of this type are produced by the reduction to generalized upper Hessenberg form of a real matrix pair (A,B):
A = Q1*H*Z1**T, B = Q1*T*Z1**T,
as computed by DGGHRD.
If JOB='S', then the Hessenberg-triangular pair (H,T) is also reduced to generalized Schur form,
H = Q*S*Z**T, T = Q*P*Z**T,
where Q and Z are orthogonal matrices, P is an upper triangular matrix, and S is a quasi-triangular matrix with 1-by-1 and 2-by-2 diagonal blocks.
The 1-by-1 blocks correspond to real eigenvalues of the matrix pair (H,T) and the 2-by-2 blocks correspond to complex conjugate pairs of eigenvalues.
Additionally, the 2-by-2 upper triangular diagonal blocks of P corresponding to 2-by-2 blocks of S are reduced to positive diagonal form, i.e., if S(j+1,j) is non-zero, then P(j+1,j) = P(j,j+1) = 0, P(j,j) > 0, and P(j+1,j+1) > 0.
Optionally, the orthogonal matrix Q from the generalized Schur factorization may be postmultiplied into an input matrix Q1, and the orthogonal matrix Z may be postmultiplied into an input matrix Z1. If Q1 and Z1 are the orthogonal matrices from DGGHRD that reduced the matrix pair (A,B) to generalized upper Hessenberg form, then the output matrices Q1*Q and Z1*Z are the orthogonal factors from the generalized Schur factorization of (A,B):
A = (Q1*Q)*S*(Z1*Z)**T, B = (Q1*Q)*P*(Z1*Z)**T.
To avoid overflow, eigenvalues of the matrix pair (H,T) (equivalently, of (A,B)) are computed as a pair of values (alpha,beta), where alpha is complex and beta real. If beta is nonzero, lambda = alpha / beta is an eigenvalue of the generalized nonsymmetric eigenvalue problem (GNEP)
A*x = lambda*B*x
and if alpha is nonzero, mu = beta / alpha is an eigenvalue of the alternate form of the GNEP
mu*A*y = B*y.
Real eigenvalues can be read directly from the generalized Schur form:
alpha = S(i,i), beta = P(i,i).
- Ref: C.B. Moler & G.W. Stewart, , SIAM J. Numer. Anal., 10(1973), pp. 241--256.
- Ref: B. Kagstrom, D. Kressner, , SIAM J. Numer. Anal., 29(2006), pp. 199--227.
- Ref: T. Steel, D. Camps, K. Meerbergen, R. Vandebril
yes, the source text saysJOBin a couple of places even though the parameter isWANTSβ I'm keeping that exactly as written, bestie. iykyk π
π Parameters π
WANTS
WANTS is CHARACTER*1
= 'E': Compute eigenvalues only;= 'S': Compute eigenvalues and the Schur form.
WANTQ
WANTQ is CHARACTER*1
= 'N': Left Schur vectors (Q) are not computed;= 'I':Qis initialized to the unit matrix and the matrixQof left Schur vectors of(A,B)is returned;= 'V':Qmust contain an orthogonal matrixQ1on entry and the productQ1*Qis returned.
WANTZ
WANTZ is CHARACTER*1
= 'N': Right Schur vectors (Z) are not computed;= 'I':Zis initialized to the unit matrix and the matrixZof right Schur vectors of(A,B)is returned;= 'V':Zmust contain an orthogonal matrixZ1on entry and the productZ1*Zis returned.
N
N is INTEGER β the order of the matrices A, B, Q, and Z. N >= 0.
ILO
ILO is INTEGER.
IHI
IHI is INTEGER
ILO and IHI mark the rows and columns of A which are in Hessenberg form. It is assumed that A is already upper triangular in rows and columns 1:ILO-1 and IHI+1:N. If N > 0, 1 <= ILO <= IHI <= N; if N = 0, ILO=1 and IHI=0.
A
A is DOUBLE PRECISION array, dimension (LDA, N)
On entry, the N-by-N upper Hessenberg matrix A. On exit, if JOB = 'S', A contains the upper quasi-triangular matrix S from the generalized Schur factorization. If JOB = 'E', the diagonal blocks of A match those of S, but the rest of A is unspecified.
LDA
LDA is INTEGER β the leading dimension of the array A. LDA >= max( 1, N ).
B
B is DOUBLE PRECISION array, dimension (LDB, N)
On entry, the N-by-N upper triangular matrix B. On exit, if JOB = 'S', B contains the upper triangular matrix P from the generalized Schur factorization; 2-by-2 diagonal blocks of P corresponding to 2-by-2 blocks of S are reduced to positive diagonal form, i.e., if A(j+1,j) is non-zero, then B(j+1,j) = B(j,j+1) = 0, B(j,j) > 0, and B(j+1,j+1) > 0. If JOB = 'E', the diagonal blocks of B match those of P, but the rest of B is unspecified.
LDB
LDB is INTEGER β the leading dimension of the array B. LDB >= max( 1, N ).
ALPHAR
ALPHAR is DOUBLE PRECISION array, dimension (N) β the real parts of each scalar alpha defining an eigenvalue of GNEP.
ALPHAI
ALPHAI is DOUBLE PRECISION array, dimension (N) β the imaginary parts of each scalar alpha defining an eigenvalue of GNEP. If ALPHAI(j) is zero, then the j-th eigenvalue is real; if positive, then the j-th and (j+1)-st eigenvalues are a complex conjugate pair, with ALPHAI(j+1) = -ALPHAI(j).
BETA
BETA is DOUBLE PRECISION array, dimension (N) β the scalars beta that define the eigenvalues of GNEP. Together, the quantities alpha = (ALPHAR(j),ALPHAI(j)) and beta = BETA(j) represent the j-th eigenvalue of the matrix pair (A,B), in one of the forms lambda = alpha/beta or mu = beta/alpha. Since either lambda or mu may overflow, they should not, in general, be computed.
Q
Q is DOUBLE PRECISION array, dimension (LDQ, N)
On entry, if COMPQ = 'V', the orthogonal matrix Q1 used in the reduction of (A,B) to generalized Hessenberg form. On exit, if COMPQ = 'I', the orthogonal matrix of left Schur vectors of (A,B), and if COMPQ = 'V', the orthogonal matrix of left Schur vectors of (A,B). Not referenced if COMPQ = 'N'.
LDQ
LDQ is INTEGER β the leading dimension of the array Q. LDQ >= 1. If COMPQ='V' or 'I', then LDQ >= N.
Z
Z is DOUBLE PRECISION array, dimension (LDZ, N)
On entry, if COMPZ = 'V', the orthogonal matrix Z1 used in the reduction of (A,B) to generalized Hessenberg form. On exit, if COMPZ = 'I', the orthogonal matrix of right Schur vectors of (H,T), and if COMPZ = 'V', the orthogonal matrix of right Schur vectors of (A,B). Not referenced if COMPZ = 'N'.
LDZ
LDZ is INTEGER β the leading dimension of the array Z. LDZ >= 1. If COMPZ='V' or 'I', then LDZ >= N.
WORK
WORK is DOUBLE PRECISION array, dimension (MAX(1,LWORK))
On exit, if INFO >= 0, WORK(1) returns the optimal LWORK.
LWORK
LWORK is INTEGER β the dimension of the array WORK. LWORK >= max(1,N).
If LWORK = -1, then a workspace query is assumed; the routine only calculates the optimal size of the WORK array, returns this value as the first entry of the WORK array, and no error message related to LWORK is issued by XERBLA.
REC
REC is INTEGER β REC indicates the current recursion level. Should be set to 0 on first call.
INFO
INFO is INTEGER
= 0: successful exit< 0: ifINFO = -i, the i-th argument had an illegal value= 1,...,N: the QZ iteration did not converge.(A,B)is not in Schur form, butALPHAR(i),ALPHAI(i), andBETA(i),i=INFO+1,...,Nshould be correct.
π«Ά Author π«Ά
Thijs Steel, KU Leuven
π Date π
May 2020
Definition at line 302 of file dlaqz0.f.
π§ Author π§
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