tgsen(3)
๐ธ tgsen(3) โ Library Functions Manual ๐ธ
okay so bestie, welcome to tgsen(3) from the Library Functions Manual. This is part 1 of the page, and it's giving generalized Schur reorder energy โ we are literally about to move a selected cluster of eigenvalues into the leading diagonal blocks. ๐
โจ
๐ NAME ๐
tgsen โ reorder generalized Schur form. That's the whole vibe: reorder the generalized Schur form, bestie. ๐ฆ
โจ SYNOPSIS โจ
๐ Functions ๐
ctgsenโ the complex single-precision one, and yes it gets its own whole signature:
subroutine ctgsen (ijob, wantq, wantz, select, n, a, lda, b, ldb, alpha,
beta, q, ldq, z, ldz, m, pl, pr, dif, work, lwork, iwork, liwork,
info)
CTGSEN
dtgsenโ the double-precision real one withalpharandalphaiin the mix:
subroutine dtgsen (ijob, wantq, wantz, select, n, a, lda, b, ldb,
alphar, alphai, beta, q, ldq, z, ldz, m, pl, pr, dif, work, lwork,
iwork, liwork, info)
DTGSEN
stgsenโ same real double-precision energy but single precision, slay:
subroutine stgsen (ijob, wantq, wantz, select, n, a, lda, b, ldb,
alphar, alphai, beta, q, ldq, z, ldz, m, pl, pr, dif, work, lwork,
iwork, liwork, info)
STGSEN
ztgsenโ the complex double-precision icon:
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
๐ Detailed Description ๐
This is the big-picture section before we get into the function docs, bestie. ๐ซถ
๐ฆ Function Documentation ๐ฆ
๐
ctgsen โ CTGSEN ๐
subroutine ctgsen (integer ijob, logical wantq, logical wantz, logical,
dimension( * ) select, integer n, complex, dimension( lda, * ) a,
integer lda, complex, dimension( ldb, * ) b, integer ldb, complex,
dimension( * ) alpha, complex, dimension( * ) beta, complex, dimension(
ldq, * ) q, integer ldq, complex, dimension( ldz, * ) z, integer ldz,
integer m, real pl, real pr, real, dimension( * ) dif, complex,
dimension( * ) work, integer lwork, integer, dimension( * ) iwork,
integer liwork, integer info)
CTGSEN
โจ Purpose โจ
CTGSEN reorders the generalized Schur decomposition of a complex matrix pair (A, B) โ in terms of an unitary equivalence transformation Q**H * (A, B) * Z โ 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. ๐ฆ
CTGSEN also computes the generalized eigenvalues
w(j)= ALPHA(j) / BETA(j)
of the reordered matrix pair (A, B). โจ
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. ๐
๐ธ Parameters ๐ธ
IJOBโIJOB is INTEGER. Specifies whether condition numbers are required for the cluster of eigenvalues (PLandPR) or the deflating subspaces (DifuandDifl):=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, 1 and 2 above): Economic version to get it all.=5: ComputePL,PRandDIF(i.e. 0, 1 and 3 above)
WANTQโWANTQ is LOGICAL..TRUE.: update the left transformation matrixQ;.FALSE.: do not updateQ.WANTZโWANTZ is LOGICAL..TRUE.: update the right transformation matrixZ;.FALSE.: do not updateZ.SELECTโSELECT is LOGICAL array, dimension (N).SELECTspecifies the eigenvalues in the selected cluster. To select an eigenvaluew(j),SELECT(j)must be set to.TRUE..NโN is INTEGER. The order of the matricesAandB.N >= 0.AโA is COMPLEX array, dimension(LDA,N). On entry, the upper triangular matrixA, in generalized Schur canonical form. On exit,Ais overwritten by the reordered matrixA.LDAโLDA is INTEGER. The leading dimension of the arrayA.LDA >= max(1,N).BโB is COMPLEX array, dimension(LDB,N). On entry, the upper triangular matrixB, in generalized Schur canonical form. On exit,Bis overwritten by the reordered matrixB.LDBโLDB is INTEGER. The leading dimension of the arrayB.LDB >= max(1,N).ALPHAโALPHA is COMPLEX array, dimension (N).BETAโBETA is COMPLEX array, dimension (N). The diagonal elements ofAandB, respectively, when the pair(A,B)has been reduced to generalized Schur form.ALPHA(i)/BETA(i)i=1,...,Nare the generalized eigenvalues.QโQ is COMPLEX array, dimension (LDQ,N). On entry, ifWANTQ = .TRUE.,Qis anN-by-Nmatrix. On exit,Qhas been postmultiplied by the left unitary transformation matrix which reorder(A, B); The leadingMcolumns ofQform orthonormal bases for the specified pair of left eigenspaces (deflating subspaces). IfWANTQ = .FALSE.,Qis not referenced.LDQโLDQ is INTEGER. The leading dimension of the arrayQ.LDQ >= 1. IfWANTQ = .TRUE.,LDQ >= N.ZโZ is COMPLEX array, dimension (LDZ,N). On entry, ifWANTZ = .TRUE.,Zis anN-by-Nmatrix. On exit,Zhas been postmultiplied by the left unitary transformation matrix which reorder(A, B); The leadingMcolumns ofZform orthonormal bases for the specified pair of left eigenspaces (deflating subspaces). IfWANTZ = .FALSE.,Zis not referenced.LDZโLDZ is INTEGER. The leading dimension of the arrayZ.LDZ >= 1. IfWANTZ = .TRUE.,LDZ >= N.MโM is INTEGER. The dimension of the specified pair of left and right eigenspaces, (deflating subspaces)0 <= M <= N.PLโPL is REAL.PRโPR is REAL. IfIJOB = 1, 4 or 5,PL,PRare lower bounds on the reciprocal of the norm of onto left and right eigenspace with respect to the selected cluster.0 < PL, PR <= 1. IfM = 0 or M = N,PL = PR = 1. IfIJOB = 0, 2 or 3PL,PRare not referenced.DIFโDIF is REAL array, dimension (2).IfIJOB >= 2,DIF(1:2)store the estimates ofDifuandDifl. IfIJOB = 2 or 4,DIF(1:2)are F-norm-based upper bounds onDifuandDifl. IfIJOB = 3 or 5,DIF(1:2)are 1-norm-based estimates ofDifuandDifl, computed using reversed communication withCLACN2. IfM = 0 or N,DIF(1:2) = F-norm([A, B]). IfIJOB = 0 or 1,DIFis not referenced.WORKโWORK is COMPLEX array, dimension (MAX(1,LWORK)). On exit, ifINFO = 0,WORK(1)returns the optimalLWORK.LWORKโLWORK is INTEGER. The dimension of the arrayWORK.LWORK >= 1. IfIJOB = 1, 2 or 4,LWORK >= 2*M*(N-M). IfIJOB = 3 or 5,LWORK >= 4*M*(N-M). IfLWORK = -1, then a workspace query is assumed; the routine only calculates the optimal size of theWORKarray, returns this value as the first entry of theWORKarray, and no error message related toLWORKis issued byXERBLA.IWORKโIWORK is INTEGER array, dimension (MAX(1,LIWORK)). On exit, ifINFO = 0,IWORK(1)returns the optimalLIWORK.LIWORKโLIWORK is INTEGER. The dimension of the arrayIWORK.LIWORK >= 1. IfIJOB = 1, 2 or 4,LIWORK >= N+2; IfIJOB = 3 or 5,LIWORK >= MAX(N+2, 2*M*(N-M)); IfLIWORK = -1, then a workspace query is assumed; the routine only calculates the optimal size of theIWORKarray, returns this value as the first entry of theIWORKarray, and no error message related toLIWORKis issued byXERBLA.INFOโINFO 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.
๐ Author ๐
- Univ. of Tennessee
- Univ. of California Berkeley
- Univ. of Colorado Denver
- NAG Ltd.
๐ฆ Further Details: ๐ฆ
okay so back to the math, bestie: CTGSEN 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). ๐
If (A, B) has been obtained from the generalized real Schur decomposition of a matrix pair (C, D) = Q*(A, B)*Z', 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.). ๐ธ
โ ๏ธ Note that if the selected eigenvalue is sufficiently ill-conditioned, then its value may differ significantly from its value before reordering. no cap, that's 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. โจ
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. ๐ง
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. ๐ญ
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. ๐
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. ๐ฆ
Note that if the default method for computing the Frobenius-norm-based estimateDIFis not wanted (seeCLATDF), then the parameterIDIFJB(see below) should be changed from3to4(routineCLATDF(IJOB = 2will be used)). SeeCTGSYLfor more details. ๐
๐ Contributors ๐
Bo Kagstrom and Peter Poromaa, Department of Computing Science, Umea University, S-901 87 Umea, Sweden.
๐ References ๐
[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.
Definition at line 430 of file ctgsen.f.
subroutine dtgsen (integer ijob, logical wantq, logical wantz, logical,
dimension( * ) select, integer n, double precision, dimension( lda, * )
a, integer lda, double precision, dimension( ldb, * ) b, integer ldb,
double precision, dimension( * ) alphar, double precision, dimension( *
) alphai, double precision, dimension( * ) beta, double precision,
dimension( ldq, * ) q, integer ldq, double precision, dimension( ldz, *
) z, integer ldz, integer m, double precision pl, double precision pr,
double precision, dimension( * ) dif, double precision, dimension( * )
work, integer lwork, integer, dimension( * ) iwork, integer liwork,
integer info)
๐ฆ DTGSEN ๐ฆ
๐ Purpose ๐
okay so DTGSEN reorders the generalized real Schur decomposition of a real matrix pair (A, B) (in terms of an orthonormal equivalence transformation Q**T * (A, B) * Z), so that a selected cluster of eigenvalues appears in the leading diagonal blocks of the upper quasi-triangular matrix A and the upper triangular B. The leading columns of Q and Z form orthonormal bases of the corresponding left and right eigenspaces (deflating subspaces). (A, B) must be in generalized real Schur canonical form (as returned by DGGES), i.e. A is block upper triangular with 1-by-1 and 2-by-2 diagonal blocks. B is upper triangular. ๐ฅ
DTGSEN also computes the generalized eigenvalues
w(j) = (ALPHAR(j) + i*ALPHAI(j))/BETA(j)
of the reordered matrix pair (A, B). ๐
Optionally, DTGSEN computes the 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. ๐ซถ
โจ Parameters โจ
IJOBโIJOBisINTEGER. Specifies whether condition numbers are required for the cluster of eigenvalues (PLandPR) or the deflating subspaces (DifuandDifl):=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)
WANTQโWANTQisLOGICAL..TRUE.: update the left transformation matrixQ;.FALSE.: do not updateQ.WANTZโWANTZisLOGICAL..TRUE.: update the right transformation matrixZ;.FALSE.: do not updateZ.SELECTโSELECTisLOGICALarray, dimension(N).SELECTspecifies the eigenvalues in the selected cluster. To select a real eigenvaluew(j),SELECT(j)must be set to.TRUE.. To select a complex conjugate pair of eigenvaluesw(j)andw(j+1), corresponding to a2-by-2diagonal block, eitherSELECT(j)orSELECT(j+1)or both must be set to.TRUE.; a complex conjugate pair of eigenvalues must be either both included in the cluster or both excluded. ๐NโNisINTEGER. The order of the matricesAandB.N >= 0.AโAisDOUBLE PRECISIONarray, dimension(LDA,N). On entry, the upper quasi-triangular matrixA, with(A, B)in generalized real Schur canonical form. On exit,Ais overwritten by the reordered matrixA.LDAโLDAisINTEGER. The leading dimension of the arrayA.LDA >= max(1,N).BโBisDOUBLE PRECISIONarray, dimension(LDB,N). On entry, the upper triangular matrixB, with(A, B)in generalized real Schur canonical form. On exit,Bis overwritten by the reordered matrixB.LDBโLDBโINTEGER. It's the leading dimension of arrayB, bestie. Rule:LDB >= max(1,N).ALPHARโDOUBLE PRECISIONarray, dimension(N).ALPHAIโDOUBLE PRECISIONarray, dimension(N).BETAโDOUBLE PRECISIONarray, dimension(N).
Okay so on exit, (ALPHAR(j) + ALPHAI(j)*i)/BETA(j), for j=1,...,N, gives you the generalized eigenvalues. Slay. And ALPHAR(j) + ALPHAI(j)*i together with BETA(j), j=1,...,N, are the diagonals of the complex Schur form (S,T) โ the one you'd get if those 2-by-2 diagonal blocks of the real generalized Schur form of (A,B) got further reduced to triangular form using complex unitary transformations. If ALPHAI(j) is zero, then the j-th eigenvalue is real ๐ธ. If it's positive, then the j-th and (j+1)-st eigenvalues form a complex conjugate pair, with ALPHAI(j+1) negative. Iconic behaviour tbh.
QโDOUBLE PRECISIONarray, dimension(LDQ,N).
On entry: if WANTQ = .TRUE., Q is an N-by-N matrix. On exit, Q has been postmultiplied by the left orthogonal transformation matrix which reorder (A, B) โ and yes, that's exactly how the original words it ๐ญ. The leading M columns of Q form orthonormal bases for the specified pair of left eigenspaces (deflating subspaces). If WANTQ = .FALSE., Q is simply not referenced. Leave her alone ๐
.
LDQโINTEGER. The leading dimension of the arrayQ.LDQ >= 1; and ifWANTQ = .TRUE., thenLDQ >= N.ZโDOUBLE PRECISIONarray, dimension(LDZ,N).
On entry: if WANTZ = .TRUE., Z is an N-by-N matrix. On exit, Z has been postmultiplied by the left orthogonal 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, no thoughts, head empty ๐ซถ.
LDZโINTEGER. The leading dimension of the arrayZ.LDZ >= 1; ifWANTZ = .TRUE., thenLDZ >= N.MโINTEGER. The dimension of the specified pair of left and right eigenspaces (deflating subspaces). Range:0 <= M <= N.PLโDOUBLE PRECISION.PRโDOUBLE PRECISION.
If IJOB = 1, 4 or 5, then PL and PR are lower bounds on the reciprocal of the norm of onto left and right eigenspaces with respect to the selected cluster. And 0 < PL, PR <= 1. If M = 0 or M = N, then PL = PR = 1. If IJOB = 0, 2 or 3, then PL and PR are justโฆ not referenced โจ.
DIFโDOUBLE PRECISIONarray, dimension(2).
If IJOB >= 2, then DIF(1:2) store the estimates of Difu and Difl. If IJOB = 2 or 4, then DIF(1:2) are F-norm-based upper bounds on Difu and Difl. If IJOB = 3 or 5, then DIF(1:2) are 1-norm-based estimates of Difu and Difl. And if M = 0 or N, then DIF(1:2) = F-norm([A, B]). If IJOB = 0 or 1, DIF is not referenced. Periodt.
WORKโDOUBLE PRECISIONarray, dimension(MAX(1,LWORK)).
On exit, if INFO = 0, then WORK(1) returns the optimal LWORK. Chef's kiss ๐
LWORKโINTEGER. The dimension of the arrayWORK. Constraint:LWORK >= 4*N+16. IfIJOB = 1, 2or4, thenLWORK >= MAX(4*N+16, 2*M*(N-M)). IfIJOB = 3or5, thenLWORK >= MAX(4*N+16, 4*M*(N-M)).
And check this: if LWORK = -1, then a workspace query is assumed ๐ง โ 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. Free info, no scolding.
IWORKโINTEGERarray, dimension(MAX(1,LIWORK)).
On exit, if INFO = 0, then IWORK(1) returns the optimal LIWORK.
LIWORKโINTEGER. The dimension of the arrayIWORK. Constraint:LIWORK >= 1. IfIJOB = 1, 2or4, thenLIWORK >= N+6. IfIJOB = 3or5, thenLIWORK >= MAX(2*M*(N-M), N+6).
Same deal as before: if LIWORK = -1, then a workspace query is assumed โ 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. Very demure, very mindful ๐.
INFOโINTEGER. The receipts:=0: successful exit, we ate ๐<0: ifINFO = -i, the i-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 โ the problem is very ill-conditioned. Heads up:(A, B)may have been partially reordered. And if requested,0is returned inDIF(*),PLandPR. Not a full slay, sorry bestie ๐ญ
๐ Author
Univ. of Tennessee
Univ. of California Berkeley
Univ. of Colorado Denver
NAG Ltd.
๐ Further Details:
ok this is the part where it gets really good, grab a snack ๐
DTGSEN first collects the selected eigenvalues by computing orthogonal 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**T*(A, B)*W = (A11 A12) (B11 B12) n1
( 0 A22),( 0 B22) n2
n1 n2 n1 n2
where N = n1+n2 and U**T means the 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) โจ
If (A, B) has been obtained from the generalized real Schur decomposition of a matrix pair (C, D) = Q*(A, B)*Z**T, then the reordered generalized real Schur form of (C, D) is given by:
(C, D) = (Q*U)*(U**T*(A, B)*W)*(Z*W)**T,
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.). That's the whole vibe ๐ค
โ ๏ธ Note that if the selected eigenvalue is sufficiently ill-conditioned, then its value may differ significantly from its value before reordering. So likeโฆ don't be surprised. It's giving chaos.
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**T, In1) ]
[ kron(In2, B11) -kron(B22**T, In1) ].
Here, Inx is the identity matrix of size nx and A22**T is the transpose of A22. And kron(X, Y) is the Kronecker product between the matrices X and Y. Big math energy, we love to see it ๐
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. Tiny DIF(2) = big oof, basically ๐ง
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. Bookkeeping queen behaviour fr fr ๐
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 ๐
โญ Note that if the default method for computing the Frobenius-norm-based estimateDIFis not wanted (seeDLATDF), then the parameterIDIFJB(see below) should be changed from3to4(routineDLATDF(IJOB = 2will be used)). SeeDTGSYLfor more details. Iykyk.
๐ธ Contributors:
Bo Kagstrom and Peter Poromaa, Department of Computing Science, Umea University, S-901 87 Umea, Sweden.
๐ฆ References:
okay so the reference receipts for dtgsen first, because citations are lowkey the moment ๐โจ:
[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.
and the exact coordinate: Definition at line 448 of file dtgsen.f.
now bestie, spot the single-precision twin โ STGSEN is here and it's giving โsame energy, different precisionโ ๐
:
subroutine stgsen (integer ijob, logical wantq, logical wantz, logical,
dimension( * ) select, integer n, real, dimension( lda, * ) a, integer
lda, real, dimension( ldb, * ) b, integer ldb, real, dimension( * )
alphar, real, dimension( * ) alphai, real, dimension( * ) beta, real,
dimension( ldq, * ) q, integer ldq, real, dimension( ldz, * ) z, integer
ldz, integer m, real pl, real pr, real, dimension( * ) dif, real,
dimension( * ) work, integer lwork, integer, dimension( * ) iwork,
integer liwork, integer info)
STGSEN
๐ธ STGSEN ๐ธ
โจ Purpose โจ
okay so STGSEN reorders the generalized real Schur decomposition of a real matrix pair (A, B) โ and yes, it does that through an orthonormal equivalence transformation Q**T * (A, B) * Z โ so that a selected cluster of eigenvalues appears in the leading diagonal blocks of the upper quasi-triangular matrix A and the upper triangular B. the leading columns of Q and Z form orthonormal bases of the corresponding left and right eigenspaces (deflating subspaces). and listen: (A, B) must be in generalized real Schur canonical form (as returned by SGGES), meaning A is block upper triangular with 1-by-1 and 2-by-2 diagonal blocks, and B is upper triangular. no cap. ๐
STGSEN also computes the generalized eigenvalues
w(j) = (ALPHAR(j) + i*ALPHAI(j))/BETA(j)
of the reordered matrix pair (A, B).
optionally, STGSEN computes the 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.
๐ Parameters ๐
bestie, here's every single arg โ no skips, no โwe'll come back to it,โ we're doing this properly ๐ซถ:
IJOBโIJOB is INTEGER. specifies whether condition numbers are required for the cluster of eigenvalues (PLandPR) or the deflating subspaces (DifuandDifl):=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, 1 and 2 above): Economic version to get it all.=5: ComputePL,PRandDIF(i.e. 0, 1 and 3 above)
WANTQโWANTQ is LOGICAL..TRUE.: update the left transformation matrixQ;.FALSE.: do not updateQ.WANTZโWANTZ is LOGICAL..TRUE.: update the right transformation matrixZ;.FALSE.: do not updateZ.SELECTโSELECT is LOGICAL array, dimension (N).SELECTspecifies the eigenvalues in the selected cluster. to select a real eigenvaluew(j),SELECT(j)must be set to.TRUE.. to select a complex conjugate pair of eigenvaluesw(j)andw(j+1), corresponding to a2-by-2diagonal block, eitherSELECT(j)orSELECT(j+1)or both must be set to.TRUE.; a complex conjugate pair of eigenvalues must be either both included in the cluster or both excluded.NโN is INTEGER. the order of the matricesAandB.N >= 0.AโA is REAL array, dimension(LDA,N). on entry, the upper quasi-triangular matrixA, with(A, B)in generalized real Schur canonical form. on exit,Ais overwritten by the reordered matrixA.LDAโLDA is INTEGER. the leading dimension of the arrayA.LDA >= max(1,N).BโB is REAL array, dimension(LDB,N). on entry, the upper triangular matrixB, with(A, B)in generalized real Schur canonical form. on exit,Bis overwritten by the reordered matrixB.LDBโLDB is INTEGER. the leading dimension of the arrayB.LDB >= max(1,N).ALPHARโALPHAR is REAL array, dimension (N).ALPHAIโALPHAI is REAL array, dimension (N).BETAโBETA is REAL array, dimension (N). on exit,(ALPHAR(j) + ALPHAI(j)*i)/BETA(j),j=1,...,N, will be the generalized eigenvalues.ALPHAR(j) + ALPHAI(j)*iandBETA(j),j=1,...,N arethe diagonals of the complex Schur form(S,T)that would result if the2-by-2diagonal blocks of the real generalized Schur form of(A,B)were further reduced to triangular form using complex unitary transformations. ifALPHAI(j)is zero, then thej-th eigenvalue is real; if positive, then thej-th and(j+1)-st eigenvalues are a complex conjugate pair, withALPHAI(j+1)negative.QโQ is REAL array, dimension (LDQ,N). on entry, ifWANTQ = .TRUE.,Qis anN-by-Nmatrix. on exit,Qhas been postmultiplied by the left orthogonal transformation matrix which reorder(A, B); The leadingMcolumns ofQform orthonormal bases for the specified pair of left eigenspaces (deflating subspaces). ifWANTQ = .FALSE.,Qis not referenced.LDQโLDQ is INTEGER. the leading dimension of the arrayQ.LDQ >= 1; and ifWANTQ = .TRUE.,LDQ >= N.ZโZ is REAL array, dimension (LDZ,N). on entry, ifWANTZ = .TRUE.,Zis anN-by-Nmatrix. on exit,Zhas been postmultiplied by the left orthogonal transformation matrix which reorder(A, B); The leadingMcolumns ofZform orthonormal bases for the specified pair of left eigenspaces (deflating subspaces). ifWANTZ = .FALSE.,Zis not referenced.LDZโLDZ is INTEGER. the leading dimension of the arrayZ.LDZ >= 1; IfWANTZ = .TRUE.,LDZ >= N.MโM is INTEGER. the dimension of the specified pair of left and right eigenspaces (deflating subspaces).0 <= M <= N.PLโPL is REAL.PRโPR is REAL. ifIJOB = 1, 4 or 5,PL,PRare lower bounds on the reciprocal of the norm of onto left and right eigenspaces with respect to the selected cluster.0 < PL, PR <= 1. ifM = 0 or M = N,PL = PR = 1. ifIJOB = 0, 2 or 3,PLandPRare not referenced.DIFโDIF is REAL array, dimension (2). ifIJOB >= 2,DIF(1:2)store the estimates ofDifuandDifl. ifIJOB = 2 or 4,DIF(1:2)are F-norm-based upper bounds onDifuandDifl. ifIJOB = 3 or 5,DIF(1:2)are 1-norm-based estimates ofDifuandDifl. ifM = 0 or N,DIF(1:2) = F-norm([A, B]). ifIJOB = 0 or 1,DIFis not referenced.WORKโWORK is REAL array, dimension (MAX(1,LWORK)). on exit, ifINFO = 0,WORK(1)returns the optimalLWORK.LWORKโLWORK is INTEGER. the dimension of the arrayWORK.LWORK >= 4*N+16. ifIJOB = 1, 2 or 4,LWORK >= MAX(4*N+16, 2*M*(N-M)). ifIJOB = 3 or 5,LWORK >= MAX(4*N+16, 4*M*(N-M)). ifLWORK = -1, then a workspace query is assumed; the routine only calculates the optimal size of theWORKarray, returns this value as the first entry of theWORKarray, and no error message related toLWORKis issued byXERBLA.IWORKโIWORK is INTEGER array, dimension (MAX(1,LIWORK)). on exit, ifINFO = 0,IWORK(1)returns the optimalLIWORK.LIWORK
It's an INTEGER ๐ โ the dimension of the array IWORK. So the rules are:
LIWORK >= 1.- If
IJOB = 1, 2 or 4, thenLIWORK >= N+6. - If
IJOB = 3 or 5, thenLIWORK >= MAX(2*M*(N-M), N+6).
๐ซถ Special case, bestie, listen up: ifLIWORK = -1, that means a workspace query is happening. The routine only calculates the optimal size of theIWORKarray, returns that value as the first entry of theIWORKarray, and no error message related toLIWORKgets issued byXERBLA.
INFOis anINTEGER๐ฉบ โ the vibe report card:=0: Successful exit. slay.<0: IfINFO = -i, the i-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 โ the problem is very ill-conditioned. ๐ญ(A, B)may have been partially reordered. If requested,0is returned inDIF(*),PLandPR.
๐ Author
Univ. of Tennessee
Univ. of California Berkeley
Univ. of Colorado Denver
NAG Ltd.
๐งฎ Further Details
okay so STGSEN first collects the selected eigenvalues by computing orthogonal 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**T*(A, B)*W = (A11 A12) (B11 B12) n1
( 0 A22),( 0 B22) n2
n1 n2 n1 n2
where N = n1+n2 and U**T means the 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**T, then the reordered generalized real Schur form of (C, D) is given by
(C, D) = (Q*U)*(U**T*(A, B)*W)*(Z*W)**T,
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.).
โ ๏ธ Note that if the selected eigenvalue is sufficiently ill-conditioned, then its value may differ significantly from its value before reordering. ๐ซ
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**T, In1) ]
[ kron(In2, B11) -kron(B22**T, In1) ].
Here, Inx is the identity matrix of size nx and A22**T is the 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.
๐ธ Heads up: if the default method for computing the Frobenius-norm-based estimateDIFis not wanted (seeSLATDF), then the parameterIDIFJB(see below) should be changed from3to4(routineSLATDF(IJOB = 2will be used)). SeeSTGSYLfor more details.
๐ธ Contributors
Bo Kagstrom and Peter Poromaa, Department of Computing Science, Umea University, S-901 87 Umea, Sweden.
๐ 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.
Definition at line 448 of file stgsen.f.
okay and now the complex twin enters the chat ๐
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
๐ ZTGSEN
Purpose
okay so ZTGSEN reorders the generalized Schur decomposition of a complex matrix pair (A, B) (in terms of an 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. ๐
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.
Parameters
IJOBis anINTEGER๐๏ธ โ specifies whether condition numbers are required for the cluster of eigenvalues (PLandPR) or the deflating subspaces (DifuandDifl):=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, 1 and 2 above): Economic version to get it all. ๐๏ธ=5: ComputePL,PRandDIF(i.e. 0, 1 and 3 above)
WANTQis aLOGICAL๐ฆ.TRUE.: update the left transformation matrixQ;.FALSE.: do not updateQ.
WANTZis aLOGICAL๐.TRUE.: update the right transformation matrixZ;.FALSE.: do not updateZ.
SELECTis aLOGICAL array, dimension (N)๐ฏ โSELECTspecifies the eigenvalues in the selected cluster. To select an eigenvaluew(j),SELECT(j)must be set to.TRUE..NโNโNisINTEGER. The order of the matricesAandB.N >= 0. ๐ธAโAisCOMPLEX*16 array,dimension(LDA,N). On entry, the upper triangular matrixA, in generalized Schur canonical form. On exit,Ais overwritten by the reordered matrixA. โจLDAโLDAisINTEGER. The leading dimension of the arrayA.LDA >= max(1,N). ๐BโBisCOMPLEX*16 array,dimension(LDB,N). On entry, the upper triangular matrixB, in generalized Schur canonical form. On exit,Bis overwritten by the reordered matrixB. ๐ฆLDBโLDBisINTEGER. The leading dimension of the arrayB.LDB >= max(1,N). ๐ALPHAโALPHAisCOMPLEX*16 array,dimension (N). ๐BETAโBETAisCOMPLEX*16 array,dimension (N). The diagonal elements ofAandB, respectively, when the pair(A,B)has been reduced to generalized Schur form.ALPHA(i)/BETA(i)i=1,...,Nare the generalized eigenvalues. ๐QโQisCOMPLEX*16 array,dimension (LDQ,N). On entry, ifWANTQ = .TRUE.,Qis anN-by-Nmatrix. On exit,Qhas been postmultiplied by the left unitary transformation matrix which reorder(A, B); The leadingMcolumns ofQform orthonormal bases for the specified pair of left eigenspaces (deflating subspaces). IfWANTQ = .FALSE.,Qis not referenced. ๐LDQโLDQisINTEGER. The leading dimension of the arrayQ.LDQ >= 1. IfWANTQ = .TRUE.,LDQ >= N. ๐ZโZisCOMPLEX*16 array,dimension (LDZ,N). On entry, ifWANTZ = .TRUE.,Zis anN-by-Nmatrix. On exit,Zhas been postmultiplied by the left unitary transformation matrix which reorder(A, B); The leadingMcolumns ofZform orthonormal bases for the specified pair of left eigenspaces (deflating subspaces). IfWANTZ = .FALSE.,Zis not referenced. โญLDZโLDZisINTEGER. The leading dimension of the arrayZ.LDZ >= 1. IfWANTZ = .TRUE.,LDZ >= N. ๐ซMโMisINTEGER. The dimension of the specified pair of left and right eigenspaces, (deflating subspaces)0 <= M <= N. ๐ซถPLโPLisDOUBLE PRECISION. ๐PRโPRisDOUBLE PRECISION. IfIJOB = 1, 4 or 5,PL, PRare lower bounds on the reciprocal of the norm of onto left and right eigenspace with respect to the selected cluster.0 < PL, PR <= 1. IfM = 0 or M = N,PL = PR = 1. IfIJOB = 0, 2 or 3PL, PRare not referenced. ๐งDIFโDIFisDOUBLE PRECISION array,dimension (2). IfIJOB >= 2,DIF(1:2)store the estimates ofDifuandDifl. IfIJOB = 2 or 4,DIF(1:2)are F-norm-based upper bounds onDifuandDifl. IfIJOB = 3 or 5,DIF(1:2)are 1-norm-based estimates ofDifuandDifl, computed using reversed communication withZLACN2. IfM = 0 or N,DIF(1:2) = F-norm([A, B]). IfIJOB = 0 or 1,DIFis not referenced. ๐ฅWORKโWORKisCOMPLEX*16 array,dimension (MAX(1,LWORK)). On exit, ifINFO = 0,WORK(1)returns the optimalLWORK. ๐LWORKโLWORKisINTEGER. The dimension of the arrayWORK.LWORK >= 1IfIJOB = 1, 2 or 4,LWORK >= 2*M*(N-M)IfIJOB = 3 or 5,LWORK >= 4*M*(N-M)IfLWORK = -1, then a workspace query is assumed; the routine only calculates the optimal size of theWORKarray, returns this value as the first entry of theWORKarray, and no error message related toLWORKis issued byXERBLA. ๐IWORKโIWORKisINTEGER array,dimension (MAX(1,LIWORK)). On exit, ifINFO = 0,IWORK(1)returns the optimalLIWORK. ๐LIWORKโLIWORKisINTEGER. The dimension of the arrayIWORK.LIWORK >= 1. IfIJOB = 1, 2 or 4,LIWORK >= N+2;IfIJOB = 3 or 5,LIWORK >= MAX(N+2, 2*M*(N-M));IfLIWORK = -1, then a workspace query is assumed; the routine only calculates the optimal size of theIWORKarray, returns this value as the first entry of theIWORKarray, and no error message related toLIWORKis issued byXERBLA. ๐INFOโINFOisINTEGER=0: Successful exit. ๐<0: IfINFO = -i, thei-th argument had an illegal value. ๐ญ=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. ๐
๐ Author
- Univ. of Tennessee
- Univ. of California Berkeley
- Univ. of Colorado Denver
- NAG Ltd.
๐ Further Details:
Okay so here's the lore, bestie: 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). โจ
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.). ๐
โ ๏ธ Note that if the selected eigenvalue is sufficiently ill-conditioned, then its value may differ significantly from its value before reordering. That's not a vibe, that's a warning, bestie.
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. ๐ธ
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. ๐ฆ
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. ๐
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. ๐ฅ
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. ๐
Note that if the default method for computing the Frobenius-norm-based estimate DIF is not wanted (see ZLATDF), then the parameter IDIFJB (see below) should be changed from 3 to 4 (routine ZLATDF (IJOB = 2 will be used)). See ZTGSYL for more details. ๐ซถ
๐ Contributors ๐
Okay so the literal legends credited here are:
- Bo Kagstrom
- Peter Poromaa
Both are from the Department of Computing Science, Umea University, S-901 87 Umea, Sweden. Iconic behavior, no cap. ๐
๐ References ๐
These are the receipts, bestie โ all the citation details, kept exactly as printed:
- [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.
And the source pin is right here: Definition at line 430 of file ztgsen.f. ๐ซถ
โจ Author โจ
Generated automatically by Doxygen for LAPACK from the source code. Thatโs the whole author situation โ Doxygen did its little autogenerated thing, periodt. ๐
And thatโs the whole page, bestie! ๐ The footer credits LAPACK, Version 3.12.0, for tgsen(3) โ thatโs the source + version, and thereโs no separate date printed on that footer line, so Iโm not gonna invent one. ๐๐
๐ฆ where this page comes from
- arch rolling: lapack-doc 3.12.1-2 ยท custom
- ๐ girlified by deepseek-ai/DeepSeek-V4.1-Flash-1017 on : a language model's rewrite of the original, under its terms