DGEDMD(3)
π DGEDMD(3) β dgedmd.f90 π
okay so bestie, welcome to the manual page for /home/abuild/rpmbuild/BUILD/lapack-static-3.12.0-build/lapack-3.12.0/SRC/dgedmd.f90 β Library Functions Manual energy, but make it group-chat π
π NAME π
/home/abuild/rpmbuild/BUILD/lapack-static-3.12.0-build/lapack-3.12.0/SRC/dgedmd.f90 β yes, thatβs the whole path, sheβs long and iconic π
β¨ SYNOPSIS β¨
π§ Functions/Subroutines π§
subroutine DGEDMD (jobs, jobz, jobr, jobf, whtsvd, m, n, x, ldx, y, ldy,
nrnk, tol, k, reig, imeig, z, ldz, res, b, ldb, w, ldw, s, lds,
work, lwork, iwork, liwork, info)
DGEDMD computes the Dynamic Mode Decomposition (DMD) for a pair of data snapshot matrices. periodt π
π«Ά Function/Subroutine Documentation π«Ά
subroutine DGEDMD (character, intent(in) jobs, character, intent(in) jobz,
character, intent(in) jobr, character, intent(in) jobf, integer,
intent(in) whtsvd, integer, intent(in) m, integer, intent(in) n,
real(kind=wp), dimension(ldx,*), intent(inout) x, integer, intent(in)
ldx, real(kind=wp), dimension(ldy,*), intent(inout) y, integer,
intent(in) ldy, integer, intent(in) nrnk, real(kind=wp), intent(in) tol,
integer, intent(out) k, real(kind=wp), dimension(*), intent(out) reig,
real(kind=wp), dimension(*), intent(out) imeig, real(kind=wp),
dimension(ldz,*), intent(out) z, integer, intent(in) ldz, real(kind=wp),
dimension(*), intent(out) res, real(kind=wp), dimension(ldb,*),
intent(out) b, integer, intent(in) ldb, real(kind=wp), dimension(ldw,*),
intent(out) w, integer, intent(in) ldw, real(kind=wp), dimension(lds,*),
intent(out) s, integer, intent(in) lds, real(kind=wp), dimension(*),
intent(out) work, integer, intent(in) lwork, integer, dimension(*),
intent(out) iwork, integer, intent(in) liwork, integer, intent(out)
info)
DGEDMD computes the Dynamic Mode Decomposition (DMD) for a pair of data snapshot matrices. sheβs literally the main character of this page π₯
π― Purpose π―
okay so hereβs the tea: DGEDMD computes the Dynamic Mode Decomposition (DMD) for a pair of data snapshot matrices. For the input matrices X and Y such that Y = A*X with an unaccessible matrix A, DGEDMD computes a certain number of Ritz pairs of A using the standard Rayleigh-Ritz extraction from a subspace of range(X) that is determined using the leading left singular vectors of X. Optionally, DGEDMD returns the residuals of the computed Ritz pairs, the information needed for a refinement of the Ritz vectors, or the eigenvectors of the Exact DMD.
For further details see the references listed below. For more details of the implementation see [3]. iykyk π
π References π
- [1] P. Schmid: Dynamic mode decomposition of numerical and experimental data, Journal of Fluid Mechanics 656, 5-28, 2010.
- [2] Z. Drmac, I. Mezic, R. Mohr: Data driven modal decompositions: analysis and enhancements, SIAM J. on Sci. Comp. 40 (4), A2253-A2285, 2018.
- [3] Z. Drmac: A LAPACK implementation of the Dynamic Mode Decomposition I. Technical report. AIMDyn Inc. and LAPACK Working Note 298.
- [4] J. Tu, C. W. Rowley, D. M. Luchtenburg, S. L. Brunton, N. Kutz: On Dynamic Mode Decomposition: Theory and Applications, Journal of Computational Dynamics 1(2), 391 -421, 2014.
π Developed and supported by π
- Developed and coded by Zlatko Drmac, Faculty of Science, University of Zagreb;
drmac@math.hr - In cooperation with AIMdyn Inc., Santa Barbara, CA.
- and supported by
- DARPA SBIR project Contract No:
W31P4Q-21-C-0007 - DARPA PAI project Contract No:
HR0011-18-9-0033 - DARPA MoDyL project Contract No:
HR0011-16-C-0116
- DARPA SBIR project Contract No:
Any opinions, findings and conclusions or recommendations expressed in this material are those of the author and do not necessarily reflect the views of the DARPA SBIR Program Office. no cap, thatβs the official line π«Ά
π Distribution Statement A π
Approved for Public Release, Distribution Unlimited. Cleared by DARPA on September 29, 2022. slay, cleared and iconic β
π Parameters π
JOBS
JOBS (input) is CHARACTER*1. She determines whether the initial data snapshots are scaled by a diagonal matrix. vibe check on scaling π
'S':: The data snapshots matricesXandYare multiplied with a diagonal matrixDso thatX*Dhas unit nonzero columns (in the Euclidean 2-norm)'C':: The snapshots are scaled as with the'S'option. If it is found that an i-th column ofXis zero vector and the corresponding i-th column ofYis non-zero, then the i-th column ofYis set to zero and a warning flag is raised.'Y':: The data snapshots matricesXandYare multiplied by a diagonal matrixDso thatY*Dhas unit nonzero columns (in the Euclidean 2-norm)'N':: No data scaling.
JOBZ
JOBZ (input) is CHARACTER*1. She determines whether the eigenvectors (Koopman modes) will be computed. eigen tea ββ¨
'V':: The eigenvectors (Koopman modes) will be computed and returned in the matrixZ. See the description ofZ.'F':: The eigenvectors (Koopman modes) will be returned in factored form as the productX(:,1:K)*W, whereXcontains a POD basis (leading left singular vectors of the data matrixX) andWcontains the eigenvectors of the corresponding Rayleigh quotient. See the descriptions ofK,X,W,Z.'N':: The eigenvectors are not computed.
JOBR
JOBR (input) is CHARACTER*1. She determines whether to compute the residuals. residuals, bestie π
'R':: The residuals for the computed eigenpairs will be computed and stored in the arrayRES. See the description ofRES. For this option to be legal,JOBZmust be'V'.'N':: The residuals are not computed.
JOBF
JOBF (input) is CHARACTER*1. She specifies whether to store information needed for post-processing (e.g. computing refined Ritz vectors). post-processing princess π
'R':: The matrix needed for the refinement of the Ritz vectors is computed and stored in the arrayB. See the description ofB.'E':: The unscaled eigenvectors of the Exact DMD are computed and returned in the arrayB. See the description ofB.'N':: No eigenvector refinement data is computed.
WHTSVD
WHTSVD (input) is INTEGER, and the original line literally says WHSTVD in { 1, 2, 3, 4 } β yes, that spelling, bestie, we donβt fix it π
. She allows for a selection of the SVD algorithm from the LAPACK library.
1::DGESVD(the QR SVD algorithm)2::DGESDD(the Divide and Conquer algorithm; if enough workspace available, this is the fastest option)3::DGESVDQ(the preconditioned QR SVD ; this and 4 are the most accurate options)4::DGEJSV(the preconditioned Jacobi SVD; this and 3 are the most accurate options)
For the four methods above, a significant difference in the accuracy of small singular values is possible if the snapshots vary in norm so that X is severely ill-conditioned. If small (smaller than EPS*||X||) singular values are of interest and JOBS=='N', then the options (3, 4) give the most accurate results, where the option 4 is slightly better and with stronger theoretical background. If JOBS=='S', i.e. the columns of X will be normalized, then all methods give nearly equally accurate results. math but make it cute π§
M
M (input) is INTEGER, M>= 0. The state space dimension (the row dimension of X, Y). rows on rows π
N
N (input) is INTEGER, 0 <= N <= M. The number of data snapshot pairs (the number of columns of X and Y). columns on columns π
X
X (input/output) is a REAL(KIND=WP) M-by-N array.
On entry: X contains the data snapshot matrix X. It is assumed that the column norms of X are in the range of the normalized floating point numbers.
On exit: the leading K columns of X contain a POD basis, i.e. the leading K left singular vectors of the input data matrix X, U(:,1:K). All N columns of X contain all left singular vectors of the input matrix X. See the descriptions of K, Z and W. POD basis? more like POD baddie π
LDX
LDX (input) is INTEGER, LDX >= M. The leading dimension of the array X. leading dimension, leading lady β¨
Y
Y (input/workspace/output) is a REAL(KIND=WP) M-by-N array.
On entry: Y contains the data snapshot matrix Y.
On exit:
- If
JOBR == 'R', the leadingKcolumns ofYcontain the residual vectors for the computed Ritz pairs. See the description ofRES. - If
JOBR == 'N',Ycontains the original input data, scaled according to the value ofJOBS.
LDY
LDY (input) is INTEGER, LDY >= M. The leading dimension of the array Y. another leading dimension, another slay π
NRNK
NRNK (input) is INTEGER. She determines the mode how to compute the numerical rank, i.e. how to truncate small singular values of the input matrix X. On input, if:
NRNK = -1:: i-th singular valuesigma(i)is truncated ifsigma(i) <= TOL*sigma(1). This option is recommended.NRNK = -2:: i-th singular valuesigma(i)is truncated ifsigma(i) <= TOL*sigma(i-1). This option is included for R&D purposes. It requires highly accurate SVD, which may not be feasible.
The numerical rank can be enforced by using positive value of NRNK as follows:
0 < NRNK <= N :: at most NRNK largest singular values will be used. If the number of the computed nonzero singular values is less than NRNK, then only those nonzero values will be used and the actually used dimension is less than NRNK. The actual number of the nonzero singular values is returned in the variable K. See the descriptions of TOL and K. rank her, sheβs serving numerical rank realness π
TOL
bestie, the TOL tea continues in part 2 β keep scrolling when it drops π
TOLβ inputREAL(KIND=WP), and bestie, it's0 <= TOL < 1π . It's the tolerance for truncating small singular values. See the description ofNRNK.Kβ outputINTEGER,0 <= K <= Nβ¨. The dimension of the POD basis for the data snapshot matrixXand the number of the computed Ritz pairs. The value ofKis determined according to the rule set by the parametersNRNKandTOL. See the descriptions ofNRNKandTOL.REIGβ outputREAL(KIND=WP)N-by-1 array π. The leadingK(K<=N) entries ofREIGcontain the real parts of the computed eigenvaluesREIG(1:K) + sqrt(-1)*IMEIG(1:K). See the descriptions ofK,IMEIG, andZ.IMEIGβ outputREAL(KIND=WP)N-by-1 array π¦. The leadingK(K<=N) entries ofIMEIGcontain the imaginary parts of the computed eigenvaluesREIG(1:K) + sqrt(-1)*IMEIG(1:K). The eigenvalues are determined as follows:- If
IMEIG(i) == 0, then the corresponding eigenvalue is real,LAMBDA(i) = REIG(i). - If
IMEIG(i)>0, then the corresponding complex conjugate pair of eigenvalues readsLAMBDA(i) = REIG(i) + sqrt(-1)*IMAG(i)andLAMBDA(i+1) = REIG(i) - sqrt(-1)*IMAG(i). - That is, complex conjugate pairs have consecutive indices
(i,i+1), with the positive imaginary part listed first. See the descriptions ofK,REIG, andZ.
- If
Zβ workspace/outputREAL(KIND=WP)M-by-N array πΈ. IfJOBZ =='V'thenZcontains real Ritz vectors as follows:- If
IMEIG(i)=0, thenZ(:,i)is an eigenvector of the i-th Ritz value;||Z(:,i)||_2=1. - If
IMEIG(i) > 0(andIMEIG(i+1) < 0) then[Z(:,i) Z(:,i+1)]span an invariant subspace and the Ritz values extracted from this subspace areREIG(i) + sqrt(-1)*IMEIG(i)andREIG(i) - sqrt(-1)*IMEIG(i). The corresponding eigenvectors areZ(:,i) + sqrt(-1)*Z(:,i+1)andZ(:,i) - sqrt(-1)*Z(:,i+1), respectively.|| Z(:,i:i+1)||_F = 1.
- If
If JOBZ == 'F', then the above descriptions hold for the columns of X(:,1:K)*W(1:K,1:K), where the columns of W(1:k,1:K) are the computed eigenvectors of the K-by-K Rayleigh quotient. The columns of W(1:K,1:K) are similarly structured: If IMEIG(i) == 0 then X(:,1:K)*W(:,i) is an eigenvector, and if IMEIG(i)>0 then X(:,1:K)*W(:,i)+sqrt(-1)*X(:,1:K)*W(:,i+1) and X(:,1:K)*W(:,i)-sqrt(-1)*X(:,1:K)*W(:,i+1) are the eigenvectors of LAMBDA(i), LAMBDA(i+1). See the descriptions of REIG, IMEIG, X and W.
LDZβ inputINTEGER,LDZ >= Mπ. The leading dimension of the arrayZ.RESβ outputREAL(KIND=WP)N-by-1 array π₯.RES(1:K)contains the residuals for theKcomputed Ritz pairs. IfLAMBDA(i)is real, thenRES(i) = || A * Z(:,i) - LAMBDA(i)*Z(:,i))||_2.If[LAMBDA(i), LAMBDA(i+1)]is a complex conjugate pair thenRES(i)=RES(i+1) = || A * Z(:,i:i+1) - Z(:,i:i+1) *B||_Fwhere
B = [ real(LAMBDA(i)) imag(LAMBDA(i)) ]
[-imag(LAMBDA(i)) real(LAMBDA(i)) ].
It holds that RES(i) = || A*ZC(:,i) - LAMBDA(i) *ZC(:,i) ||_2 and RES(i+1) = || A*ZC(:,i+1) - LAMBDA(i+1)*ZC(:,i+1) ||_2 where ZC(:,i) = Z(:,i) + sqrt(-1)*Z(:,i+1) and ZC(:,i+1) = Z(:,i) - sqrt(-1)*Z(:,i+1). See the description of REIG, IMEIG and Z.
Bβ outputREAL(KIND=WP)M-by-N array π. IFJOBF =='R',B(1:M,1:K)containsA*U(:,1:K), and can be used for computing the refined vectors; see further details in the provided references. IfJOBF == 'E',B(1:M,1;K)containsA*U(:,1:K)*W(1:K,1:K), which are the vectors from the Exact DMD, up to scaling by the inverse eigenvalues. IfJOBF =='N', thenBis not referenced. See the descriptions ofX,W,K.LDBβ inputINTEGER,LDB >= Mπ. The leading dimension of the arrayB.Wβ workspace/outputREAL(KIND=WP)N-by-N array π. On exit,W(1:K,1:K)contains theKcomputed eigenvectors of the matrix Rayleigh quotient (real and imaginary parts for each complex conjugate pair of the eigenvalues). The Ritz vectors (returned inZ) are the product ofX(containing a POD basis for the input matrixX) andW. See the descriptions ofK,S,XandZ.Wis also used as a workspace to temporarily store the right singular vectors ofX.LDWβ inputINTEGER,LDW >= Nβ. The leading dimension of the arrayW.Sβ workspace/outputREAL(KIND=WP)N-by-N array π. The arrayS(1:K,1:K)is used for the matrix Rayleigh quotient. This content is overwritten during the eigenvalue decomposition byDGEEV. See the description ofK.LDSβ inputINTEGER,LDS >= Nπ§. The leading dimension of the arrayS.WORKβ workspace/outputREAL(KIND=WP)LWORK-by-1 array π. On exit,WORK(1:N)contains the singular values ofX(forJOBS=='N') or column scaledX(JOBS=='S', 'C'). IfWHTSVD==4, thenWORK(N+1)andWORK(N+2)contain scaling factorWORK(N+2)/WORK(N+1)used to scaleXandYto avoid overflow in the SVD ofX. This may be of interest if the scaling option is off and as many as possible smallest eigenvalues are desired to the highest feasible accuracy. If the call toDGEDMDis only workspace query, thenWORK(1)contains the minimal workspace length andWORK(2)is the optimal workspace length. Hence, theleng of workis at least 2. See the description ofLWORK.LWORKβ inputINTEGERπ«Ά. The minimal length of the workspace vectorWORK.LWORKis calculated as follows:
If WHTSVD == 1 ::
If JOBZ == 'V', then
LWORK >= MAX(2, N + LWORK_SVD, N+MAX(1,4*N)).
If JOBZ == 'N' then
LWORK >= MAX(2, N + LWORK_SVD, N+MAX(1,3*N)).
Here LWORK_SVD = MAX(1,3*N+M,5*N) is the minimal
workspace length of DGESVD.
If WHTSVD == 2 ::
If JOBZ == 'V', then
LWORK >= MAX(2, N + LWORK_SVD, N+MAX(1,4*N))
If JOBZ == 'N', then
LWORK >= MAX(2, N + LWORK_SVD, N+MAX(1,3*N))
Here LWORK_SVD = MAX(M, 5*N*N+4*N)+3*N*N is the
minimal workspace length of DGESDD.
If WHTSVD == 3 ::
If JOBZ == 'V', then
LWORK >= MAX(2, N+LWORK_SVD,N+MAX(1,4*N))
If JOBZ == 'N', then
LWORK >= MAX(2, N+LWORK_SVD,N+MAX(1,3*N))
Here LWORK_SVD = N+M+MAX(3*N+1,
MAX(1,3*N+M,5*N),MAX(1,N))
is the minimal workspace length of DGESVDQ.
If WHTSVD == 4 ::
If JOBZ == 'V', then
LWORK >= MAX(2, N+LWORK_SVD,N+MAX(1,4*N))
If JOBZ == 'N', then
LWORK >= MAX(2, N+LWORK_SVD,N+MAX(1,3*N))
Here LWORK_SVD = MAX(7,2*M+N,6*N+2*N*N) is the
minimal workspace length of DGEJSV.
The above expressions are not simplified in order to make the usage of WORK more transparent, and for easier checking. In any case, LWORK >= 2. If on entry LWORK = -1, then a workspace query is assumed and the procedure only computes the minimal and the optimal workspace lengths for both WORK and IWORK. See the descriptions of WORK and IWORK.
IWORKβ workspace/outputINTEGERLIWORK-by-1 array π. Workspace that is required only ifWHTSVDequals 2 , 3 or 4. (See the description ofWHTSVD). If on entryLWORK =-1orLIWORK=-1, then the minimal length ofIWORKis computed and returned inIWORK(1). See the description ofLIWORK.LIWORKβ inputINTEGERπ. The minimal length of the workspace vectorIWORK. IfWHTSVD == 1, then onlyIWORK(1)is used;LIWORK >=1. IfWHTSVD == 2, thenLIWORK >= MAX(1,8*MIN(M,N)). IfWHTSVD == 3, thenLIWORK >= MAX(1,M+N-1). IfWHTSVD == 4, thenLIWORK >= MAX(3,M+3*N). If on entryLIWORK = -1, then a workspace query is assumed and the procedure only computes the minimal and the optimal workspace lengths for bothWORKandIWORK. See the descriptions ofWORKandIWORK.INFOβ outputINTEGERπ. The status tea is literally this:-i < 0:: On entry, the i-th argument had an illegal value= 0:: Successful return.= 1:: Void input. Quick exit (M=0orN=0).= 2:: The SVD computation ofXdid not converge. Suggestion: Check the input data and/or repeat with differentWHTSVD.= 3:: The computation of the eigenvalues did not converge.= 4:: If data scaling was requested on input and the procedure found inconsistency in the data such that for some column indexi,X(:,i) = 0butY(:,i) /= 0, thenY(:,i)is set to zero ifJOBS=='C'. The computation proceeds with original or modified data and warning flag is set withINFO=4.
Author π
Zlatko Drmac
Definition at line 531 of file dgedmd.f90.
Author π€
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