ZTGSEN(3)
π NAME π β ztgsen.f(3) from the Library Functions Manual
/home/abuild/rpmbuild/BUILD/lapack-static-3.12.0-build/lapack-3.12.0/SRC/ztgsen.f β yep, thatβs the whole NAME entry, bestie. Iconic path behavior, honestly. π«Ά
β¨ SYNOPSIS β¨
πΈ Functions/Subroutines πΈ
subroutine ZTGSEN (...)β the main character. Full signature below, copied exactly so nobody has to guess:
subroutine ZTGSEN (ijob, wantq, wantz, select, n, a, lda, b, ldb, alpha,
beta, q, ldq, z, ldz, m, pl, pr, dif, work, lwork, iwork, liwork,
info)
ZTGSEN
π¦ Function/Subroutine Documentation π¦
Hereβs the full type-signature situation, again exactly as given:
subroutine ZTGSEN (integer ijob, logical wantq, logical wantz, logical,
dimension( * ) select, integer n, complex*16, dimension( lda, * ) a,
integer lda, complex*16, dimension( ldb, * ) b, integer ldb, complex*16,
dimension( * ) alpha, complex*16, dimension( * ) beta, complex*16,
dimension( ldq, * ) q, integer ldq, complex*16, dimension( ldz, * ) z,
integer ldz, integer m, double precision pl, double precision pr, double
precision, dimension( * ) dif, complex*16, dimension( * ) work, integer
lwork, integer, dimension( * ) iwork, integer liwork, integer info)
ZTGSEN
π― Purpose π―
Okay so <hotpink>ZTGSEN</hotpink> reorders the generalized Schur decomposition of a complex matrix pair (A, B) β and it does this in terms of a unitary equivalence transformation Q**H * (A, B) * Z, so that a selected cluster of eigenvalues appears in the leading diagonal blocks of the pair (A,B). The leading columns of Q and Z form unitary bases of the corresponding left and right eigenspaces (deflating subspaces). (A, B) must be in generalized Schur canonical form, that is, A and B are both upper triangular. No cap. π
ZTGSEN also computes the generalized eigenvalues
w(j)= ALPHA(j) / BETA(j)
of the reordered matrix pair (A, B).
Optionally, the routine computes estimates of reciprocal condition numbers for eigenvalues and eigenspaces. These are Difu[(A11,B11), (A22,B22)] and Difl[(A11,B11), (A22,B22)], i.e. the separation(s) between the matrix pairs (A11, B11) and (A22,B22) that correspond to the selected cluster and the eigenvalues outside the cluster, resp., and norms of onto left and right eigenspaces w.r.t. the selected cluster in the (1,1)-block. π
π§Έ Parameters π§Έ
IJOB
IJOB is INTEGER. It specifies whether condition numbers are required for the cluster of eigenvalues (PL and PR) or the deflating subspaces (Difu and Difl):
=0: Only reorder w.r.t.SELECT. No extras.=1: Reciprocal of norms of onto left and right eigenspaces w.r.t. the selected cluster (PLandPR).=2: Upper bounds onDifuandDifl. F-norm-based estimate (DIF(1:2)).=3: Estimate ofDifuandDifl. 1-norm-based estimate (DIF(1:2)). About 5 times as expensive asIJOB = 2.=4: ComputePL,PRandDIF(i.e.0,1and2above): Economic version to get it all.=5: ComputePL,PRandDIF(i.e.0,1and3above)
WANTQ
WANTQ is LOGICAL.
.TRUE.: update the left transformation matrixQ;.FALSE.: do not updateQ.
WANTZ
WANTZ is LOGICAL.
.TRUE.: update the right transformation matrixZ;.FALSE.: do not updateZ.
SELECT
SELECT is LOGICAL array, dimension (N). It specifies the eigenvalues in the selected cluster. To select an eigenvalue w(j), SELECT(j) must be set to .TRUE..
N
N is INTEGER. The order of the matrices A and B. N >= 0.
A
A is COMPLEX*16 array, dimension (LDA,N).
- On entry, the upper triangular matrix
A, in generalized Schur canonical form. - On exit,
Ais overwritten by the reordered matrixA.
LDA
LDA is INTEGER. The leading dimension of the array A. LDA >= max(1,N).
B
B is COMPLEX*16 array, dimension (LDB,N).
- On entry, the upper triangular matrix
B, in generalized Schur canonical form. - On exit,
Bis overwritten by the reordered matrixB.
LDB
LDB is INTEGER. The leading dimension of the array B. LDB >= max(1,N).
ALPHA
ALPHA is COMPLEX*16 array, dimension (N).
BETA
BETA is COMPLEX*16 array, dimension (N).
The diagonal elements of A and B, respectively, when the pair (A,B) has been reduced to generalized Schur form. ALPHA(i)/BETA(i) i=1,...,N are the generalized eigenvalues.
Q
Q is COMPLEX*16 array, dimension (LDQ,N).
On entry, if WANTQ = .TRUE., Q is an N-by-N matrix. On exit, Q has been postmultiplied by the left unitary transformation matrix which reorder (A, B); The leading M columns of Q form orthonormal bases for the specified pair of left eigenspaces (deflating subspaces). If WANTQ = .FALSE., Q is not referenced.
LDQ
LDQ is INTEGER. The leading dimension of the array Q. LDQ >= 1. If WANTQ = .TRUE., LDQ >= N.
Z
Z is COMPLEX*16 array, dimension (LDZ,N).
On entry, if WANTZ = .TRUE., Z is an N-by-N matrix. On exit, Z has been postmultiplied by the left unitary transformation matrix which reorder (A, B); The leading M columns of Z form orthonormal bases for the specified pair of left eigenspaces (deflating subspaces). If WANTZ = .FALSE., Z is not referenced.
LDZ
LDZ is INTEGER. The leading dimension of the array Z. LDZ >= 1. If WANTZ = .TRUE., LDZ >= N.
M
M is INTEGER. The dimension of the specified pair of left and right eigenspaces, (deflating subspaces) 0 <= M <= N.
PL
PL is DOUBLE PRECISION.
PR
PR is DOUBLE PRECISION.
If IJOB = 1, 4 or 5, PL, PR are lower bounds on the reciprocal of the norm of onto left and right eigenspace with respect to the selected cluster. 0 < PL, PR <= 1. If M = 0 or M = N, PL = PR = 1. If IJOB = 0, 2 or 3 PL, PR are not referenced.
DIF
DIF is DOUBLE PRECISION array, dimension (2).
If IJOB >= 2, DIF(1:2) store the estimates of Difu and Difl. If IJOB = 2 or 4, DIF(1:2) are F-norm-based upper bounds on Difu and Difl. If IJOB = 3 or 5, DIF(1:2) are 1-norm-based estimates of Difu and Difl, computed using reversed communication with ZLACN2. If M = 0 or N, DIF(1:2) = F-norm([A, B]). If IJOB = 0 or 1, DIF is not referenced.
WORK
WORK is COMPLEX*16 array, dimension (MAX(1,LWORK)). On exit, if INFO = 0, WORK(1) returns the optimal LWORK.
LWORK
LWORK is INTEGER. The dimension of the array WORK. LWORK >= 1. If IJOB = 1, 2 or 4, LWORK >= 2*M*(N-M). If IJOB = 3 or 5, LWORK >= 4*M*(N-M).
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.
IWORK
IWORK is INTEGER array, dimension (MAX(1,LIWORK)). On exit, if INFO = 0, IWORK(1) returns the optimal LIWORK.
LIWORK
LIWORK is INTEGER. The dimension of the array IWORK. LIWORK >= 1. If IJOB = 1, 2 or 4, LIWORK >= N+2; If IJOB = 3 or 5, LIWORK >= MAX(N+2, 2*M*(N-M));
If LIWORK = -1, then a workspace query is assumed; the routine only calculates the optimal size of the IWORK array, returns this value as the first entry of the IWORK array, and no error message related to LIWORK is issued by XERBLA.
INFO
INFO is INTEGER.
=0: Successful exit.<0: IfINFO = -i, thei-th argument had an illegal value.=1: Reordering of(A, B)failed because the transformed matrix pair(A, B)would be too far from generalized Schur form; the problem is very ill-conditioned.(A, B)may have been partially reordered. If requested,0is returned inDIF(*),PLandPR.
π¨ bestie, thatINFO = 1case is the βthis pair is giving very ill-conditionedβ situation. Itβs not a cute little glitch β(A, B)may have been partially reordered, and0can come back inDIF(*),PLandPRif requested.
π Author π
- Univ. of Tennessee
- Univ. of California Berkeley
- Univ. of Colorado Denver
- NAG Ltd.
π Further Details π
(Nothing listed here in the original page β itβs literally empty at this point, bestie.)
Okay bestie, so ZTGSEN first collects the selected eigenvalues by computing unitary U and W that move them to the top left corner of (A, B). In other words, the selected eigenvalues are the eigenvalues of (A11, B11) in
U**H*(A, B)*W = (A11 A12) (B11 B12) n1
( 0 A22),( 0 B22) n2
n1 n2 n1 n2
where N = n1+n2 and U**H means the conjugate transpose of U. The first n1 columns of U and W span the specified pair of left and right eigenspaces (deflating subspaces) of (A, B).
If (A, B) has been obtained from the generalized real Schur decomposition of a matrix pair (C, D) = Q*(A, B)*Z**H, then the reordered generalized Schur form of (C, D) is given by
(C, D) = (Q*U)*(U**H *(A, B)*W)*(Z*W)**H,
and the first n1 columns of Q*U and Z*W span the corresponding deflating subspaces of (C, D) (Q and Z store Q*U and Z*W, resp.).
π note time: if the selected eigenvalue is sufficiently ill-conditioned, then its value may differ significantly from its value before reordering. no cap, thatβs just how it is.
The reciprocal condition numbers of the left and right eigenspaces spanned by the first n1 columns of U and W (or Q*U and Z*W) may be returned in DIF(1:2), corresponding to Difu and Difl, resp.
The Difu and Difl are defined as:
Difu[(A11, B11), (A22, B22)] = sigma-min( Zu )
and
Difl[(A11, B11), (A22, B22)] = Difu[(A22, B22), (A11, B11)],
where sigma-min(Zu) is the smallest singular value of the (2*n1*n2)-by-(2*n1*n2) matrix
Zu = [ kron(In2, A11) -kron(A22**H, In1) ]
[ kron(In2, B11) -kron(B22**H, In1) ].
Here, Inx is the identity matrix of size nx and A22**H is the conjugate transpose of A22. kron(X, Y) is the Kronecker product between the matrices X and Y.
When DIF(2) is small, small changes in (A, B) can cause large changes in the deflating subspace. An approximate (asymptotic) bound on the maximum angular error in the computed deflating subspaces is
EPS * norm((A, B)) / DIF(2),
where EPS is the machine precision.
The reciprocal norm of the projectors on the left and right eigenspaces associated with (A11, B11) may be returned in PL and PR. They are computed as follows. First we compute L and R so that P*(A, B)*Q is block diagonal, where
P = ( I -L ) n1 Q = ( I R ) n1
( 0 I ) n2 and ( 0 I ) n2
n1 n2 n1 n2
and (L, R) is the solution to the generalized Sylvester equation
A11*R - L*A22 = -A12
B11*R - L*B22 = -B12
Then PL = (F-norm(L)**2+1)**(-1/2) and PR = (F-norm(R)**2+1)**(-1/2). An approximate (asymptotic) bound on the average absolute error of the selected eigenvalues is
EPS * norm((A, B)) / PL.
There are also global error bounds which valid for perturbations up to a certain restriction: a lower bound (x) on the smallest F-norm(E,F) for which an eigenvalue of (A11, B11) may move and coalesce with an eigenvalue of (A22, B22) under perturbation (E,F), (i.e. (A + E, B + F), is
x = min(Difu,Difl)/((1/(PL*PL)+1/(PR*PR))**(1/2)+2*max(1/PL,1/PR)).
An approximate bound on x can be computed from DIF(1:2), PL and PR.
If y = ( F-norm(E,F) / x) <= 1, the angles between the perturbed (L', R') and unperturbed (L, R) left and right deflating subspaces associated with the selected cluster in the (1,1)-blocks can be bounded as
max-angle(L, L') <= arctan( y * PL / (1 - y * (1 - PL * PL)**(1/2))
max-angle(R, R') <= arctan( y * PR / (1 - y * (1 - PR * PR)**(1/2))
See LAPACK User's Guide section 4.11 or the following references for more information.
π«Ά also: if the default method for computing the Frobenius-norm-based estimateDIFis not wanted (seeZLATDF), then the parameterIDIFJB(see below) should be changed from3to4(routineZLATDF(IJOB = 2will be used)). SeeZTGSYLfor more details. iykyk.
π«Ά Contributors
Bo Kagstrom and Peter Poromaa, Department of Computing Science, Umea University, S-901 87 Umea, Sweden.
π References
- [1] B. Kagstrom; A Direct Method for Reordering Eigenvalues in the Generalized Real Schur Form of a Regular Matrix Pair (A, B), in M.S. Moonen et al (eds), Linear Algebra for Large Scale and Real-Time Applications, Kluwer Academic Publ. 1993, pp 195-218.
- [2] B. Kagstrom and P. Poromaa; Computing Eigenspaces with Specified Eigenvalues of a Regular Matrix Pair (A, B) and Condition Estimation: Theory, Algorithms and Software, Report UMINF - 94.04, Department of Computing Science, Umea University, S-901 87 Umea, Sweden, 1994. Also as LAPACK Working Note 87. To appear in Numerical Algorithms, 1996.
- [3] B. Kagstrom and P. Poromaa, LAPACK-Style Algorithms and Software for Solving the Generalized Sylvester Equation and Estimating the Separation between Regular Matrix Pairs, Report UMINF - 93.23, Department of Computing Science, Umea University, S-901 87 Umea, Sweden, December 1993, Revised April 1994, Also as LAPACK working Note 75. To appear in ACM Trans. on Math. Software, Vol 22, No 1, 1996.
π§Ύ Definition
Definition at line 430 of file ztgsen.f.
βοΈ Author
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