/home/abui...gedmdq.f90(3)
okay bestie π you just opened /home/abui...gedmdq.f90(3) β section 3, Library Functions Manual. It's giving serious linear-algebra main-character energy, and honestly? slay. This is part one, so buckle up. π«Ά
πΈ NAME πΈ
/home/abuild/rpmbuild/BUILD/lapack-static-3.12.0-build/lapack-3.12.0/SRC/cgedmdq.f90
β¨ SYNOPSIS β¨
π Functions/Subroutines π
subroutine CGEDMDQ (jobs, jobz, jobr, jobq, jobt, jobf, whtsvd, m, n, f,
ldf, x, ldx, y, ldy, nrnk, tol, k, eigs, z, ldz, res, b, ldb, v,
ldv, s, lds, zwork, lzwork, work, lwork, iwork, liwork, info)
CGEDMDQ computes the Dynamic Mode Decomposition (DMD) for a pair of data snapshot matrices. That's the whole vibe: snapshots in, DMD out. π«
π¦ Function/Subroutine Documentation π¦
subroutine CGEDMDQ (character, intent(in) jobs, character, intent(in) jobz,
character, intent(in) jobr, character, intent(in) jobq, character,
intent(in) jobt, character, intent(in) jobf, integer, intent(in) whtsvd,
integer, intent(in) m, integer, intent(in) n, complex(kind=wp),
dimension(ldf,*), intent(inout) f, integer, intent(in) ldf,
complex(kind=wp), dimension(ldx,*), intent(out) x, integer, intent(in)
ldx, complex(kind=wp), dimension(ldy,*), intent(out) y, integer,
intent(in) ldy, integer, intent(in) nrnk, real(kind=wp), intent(in) tol,
integer, intent(out) k, complex(kind=wp), dimension(*), intent(out)
eigs, complex(kind=wp), dimension(ldz,*), intent(out) z, integer,
intent(in) ldz, real(kind=wp), dimension(*), intent(out) res,
complex(kind=wp), dimension(ldb,*), intent(out) b, integer, intent(in)
ldb, complex(kind=wp), dimension(ldv,*), intent(out) v, integer,
intent(in) ldv, complex(kind=wp), dimension(lds,*), intent(out) s,
integer, intent(in) lds, complex(kind=wp), dimension(*), intent(out)
zwork, integer, intent(in) lzwork, real(kind=wp), dimension(*),
intent(out) work, integer, intent(in) lwork, integer, dimension(*),
intent(out) iwork, integer, intent(in) liwork, integer, intent(out)
info)
CGEDMDQ computes the Dynamic Mode Decomposition (DMD) for a pair of data snapshot matrices. No cap, that's literally the function's whole job. π
π― Purpose
Bestie, here's the tea: CGEDMDQ computes the Dynamic Mode Decomposition (DMD) for a pair of data snapshot matrices, using a QR factorization based compression of the data. For the input matrices X and Y such that Y = A*X with an unaccessible matrix A, CGEDMDQ 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, CGEDMDQ 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
[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
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.
π Developed and supported by π
Approved for Public Release, Distribution Unlimited.
Cleared by DARPA on September 29, 2022. periodt π
π Parameters π
okay, parameter time. Every single one matters, bestie π«Ά
JOBS
JOBS (input CHARACTER*1) β determines whether the initial data snapshots are scaled by a diagonal matrix. The data snapshots are the columns of F. The leading N-1 columns of F are denoted X and the trailing N-1 columns are denoted Y.
'S'β the data snapshots matricesXandYare multiplied with a diagonal matrixDso thatX*Dhas unit nonzero columns (in the Euclidean 2-norm).'C'β 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'β the data snapshots matricesXandYare multiplied by a diagonal matrixDso thatY*Dhas unit nonzero columns (in the Euclidean 2-norm).'N'β no data scaling.
JOBZ
JOBZ (input CHARACTER*1) β determines whether the eigenvectors (Koopman modes) will be computed.
'V'β the eigenvectors (Koopman modes) will be computed and returned in the matrixZ. See the description ofZ.'F'β the eigenvectors (Koopman modes) will be returned in factored form as the productZ*V, whereZis orthonormal andVcontains the eigenvectors of the corresponding Rayleigh quotient. See the descriptions ofF,V,Z.'Q'β the eigenvectors (Koopman modes) will be returned in factored form as the productQ*Z, whereZcontains the eigenvectors of the compression of the underlying discretised operator onto the span of the data snapshots. See the descriptions ofF,V,Z.Qis from the initial QR factorization.'N'β the eigenvectors are not computed.
JOBR
JOBR (input CHARACTER*1) β determines whether to compute the residuals.
'R'β 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'β the residuals are not computed.
JOBQ
JOBQ (input CHARACTER*1) β specifies whether to explicitly compute and return the unitary matrix from the QR factorization.
'Q'β the matrixQof the QR factorization of the data snapshot matrix is computed and stored in the arrayF. See the description ofF.'N'β the matrixQis not explicitly computed.
JOBT
JOBT (input CHARACTER*1) β specifies whether to return the upper triangular factor from the QR factorization.
'R'β the matrixRof the QR factorization of the data snapshot matrixFis returned in the arrayY. See the description ofYand Further details.'N'β the matrixRis not returned.
JOBF
JOBF (input CHARACTER*1) β specifies whether to store information needed for post-processing (e.g. computing refined Ritz vectors).
'R'β the matrix needed for the refinement of the Ritz vectors is computed and stored in the arrayB. See the description ofB.'E'β the unscaled eigenvectors of the Exact DMD are computed and returned in the arrayB. See the description ofB.'N'β no eigenvector refinement data is computed.
To be useful on exit, this option needs JOBQ='Q'.
WHTSVD
WHTSVD (input INTEGER, WHSTVD in { 1, 2, 3, 4 }) β allows for a selection of the SVD algorithm from the LAPACK library.
1βCGESVD(the QR SVD algorithm)2βCGESDD(the Divide and Conquer algorithm; if enough workspace available, this is the fastest option)3βCGESVDQ(the preconditioned QR SVD ; this and4are the most accurate options)4βCGEJSV(the preconditioned Jacobi SVD; this and3are 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. fr fr, pick wisely β¨
M
M (input INTEGER, M >= 0) β the state space dimension (the number of rows of F).
N
N (input INTEGER, 0 <= N <= M) β the number of data snapshots from a single trajectory, taken at equidistant discrete times. This is the number of columns of F.
F
okay so, picking up right where we left off β the arguments, bestie, one by one, no skipping π
β¨ F β¨
F(input/output)COMPLEX(KIND=WP)M-by-N array β the moment the actual data shows up πΈ- On entry: the columns of
Fare the sequence of data snapshots from a single trajectory, taken at equidistant discrete times. It is assumed that the column norms ofFare in the range of the normalized floating point numbers. - On exit:
- If
JOBQ == 'Q', the arrayFcontains the orthogonal matrix/factor of the QR factorization of the initial data snapshots matrixF. See the description ofJOBQ. - If
JOBQ == 'N', the entries inFstrictly below the main diagonal contain, column-wise, the information on the Householder vectors, as returned byCGEQRF. The remaining information to restore the orthogonal matrix of the initial QR factorization is stored inZWORK(1:MIN(M,N)). See the description ofZWORK.
- If
- On entry: the columns of
β¨ LDF β¨
LDF(input)INTEGER,LDF >= Mβ the leading dimension of the arrayF. that's it, that's the whole job π«Ά
β¨ X β¨
X(workspace/output)COMPLEX(KIND=WP)MIN(M,N)-by-(N-1) array βXis used as workspace to hold representations of the leading N-1 snapshots in the orthonormal basis computed in the QR factorization ofF. π¦
On exit, the leading K columns of X contain the leading K left singular vectors of the above described content of X. To lift them to the space of the left singular vectors U(:,1:K) of the input data, pre-multiply with the Q factor from the initial QR factorization. See the descriptions of F, K, V and Z.
β¨ LDX β¨
LDX(input)INTEGER,LDX >= Nβ the leading dimension of the arrayX. short king, does its one thing π
β¨ Y β¨
Y(workspace/output)COMPLEX(KIND=WP)MIN(M,N)-by-(N) array βYis used as workspace to hold representations of the trailing N-1 snapshots in the orthonormal basis computed in the QR factorization ofF. π
On exit, if JOBT == 'R', Y contains the MIN(M,N)-by-N upper triangular factor from the QR factorization of the data snapshot matrix F.
β¨ LDY β¨
LDY(input)INTEGER,LDY >= Nβ the leading dimension of the arrayY. iconic, minimal, no notes π
β¨ NRNK β¨
NRNK(input)INTEGERβ determines the mode how to compute the numerical rank, i.e. how to truncate small singular values of the input matrixX. on input, if:NRNK = -1:: i-th singular valuesigma(i)is truncated ifsigma(i) <= TOL*sigma(1). This option is recommended. πNRNK = -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. π
The numerical rank can be enforced by using positive value of NRNK as follows:
0 < NRNK <= N-1 :: 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 description of K.
β¨ TOL β¨
TOL(input)REAL(KIND=WP),0 <= TOL < 1β the tolerance for truncating small singular values. See the description ofNRNK. tiny but powerful, fr π
β¨ K β¨
K(output)INTEGER,0 <= K <= Nβ the dimension of the SVD/POD basis for the leading N-1 data snapshots (columns ofF) and the number of the computed Ritz pairs. The value ofKis determined according to the rule set by the parametersNRNKandTOL. See the descriptions ofNRNKandTOL. β
β¨ EIGS β¨
EIGS(output)COMPLEX(KIND=WP)(N-1)-by-1 array β the leadingK(K<=N-1) entries ofEIGScontain the computed eigenvalues (Ritz values). See the descriptions ofK, andZ. π₯
β¨ Z β¨
Z(workspace/output)COMPLEX(KIND=WP)M-by-(N-1) array β okay so this one's a whole vibe check π- If
JOBZ =='V'thenZcontains the Ritz vectors.Z(:,i)is an eigenvector of the i-th Ritz value;||Z(:,i)||_2=1. - If
JOBZ == 'F', then theZ(:,i)'s are given implicitly asZ*V, whereZcontains orthonormal matrix (the product ofQfrom the initial QR factorization and the SVD/POD_basis returned byCGEDMDinX) and the second factor (the eigenvectors of the Rayleigh quotient) is in the arrayV, as returned byCGEDMD. That is,X(:,1:K)*V(:,i)is an eigenvector corresponding toEIGS(i). The columns ofV(1:K,1:K)are the computed eigenvectors of the K-by-K Rayleigh quotient.
- If
See the descriptions of EIGS, X and V.
β¨ LDZ β¨
LDZ(input)INTEGER,LDZ >= Mβ the leading dimension of the arrayZ. yes bestie another leading dimension, they're everywhere, drink some water π
β¨ RES β¨
RES(output)REAL(KIND=WP)(N-1)-by-1 array βRES(1:K)contains the residuals for theKcomputed Ritz pairs,
RES(i) = || A * Z(:,i) - EIGS(i)*Z(:,i))||_2.
See the description of EIGS and Z.
β¨ B β¨
B(output)COMPLEX(KIND=WP)MIN(M,N)-by-(N-1) array β depends entirely on theJOBFsituation π§- IF
JOBF =='R',B(1:N,1:K)containsA*U(:,1:K), and can be used for computing the refined vectors; see further details in the provided references. - If
JOBF == 'E',B(1:N,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.
- IF
In both cases, the content of B can be lifted to the original dimension of the input data by pre-multiplying with the Q factor from the initial QR factorization. Here A denotes a compression of the underlying operator. See the descriptions of F and X.
If JOBF =='N', then B is not referenced. literally not even looked at π
β¨ LDB β¨
LDB(input)INTEGER,LDB >= MIN(M,N)β the leading dimension of the arrayB. πΈ
β¨ V β¨
V(workspace/output)COMPLEX(KIND=WP)(N-1)-by-(N-1) array β on exit,V(1:K,1:K)Vcontains theKeigenvectors of the Rayleigh quotient. The Ritz vectors (returned inZ) are the product ofQfrom the initial QR factorization (see the description ofF),X(see the description ofX) andV. β¨
β¨ LDV β¨
LDV(input)INTEGER,LDV >= N-1β the leading dimension of the arrayV. π«Ά
β¨ S β¨
S(output)COMPLEX(KIND=WP)(N-1)-by-(N-1) array β the arrayS(1:K,1:K)is used for the matrix Rayleigh quotient. This content is overwritten during the eigenvalue decomposition byCGEEV. so don't get attached π See the description ofK.
β¨ LDS β¨
LDS(input)INTEGER,LDS >= N-1β the leading dimension of the arrayS. π
β¨ ZWORK (the array one) β¨
LZWORKβ the label up top saysLZWORKbut this entry is describing theZWORK(workspace/output)COMPLEX(KIND=WP)LWORK-by-1 array, iykyk π
On exit, ZWORK(1:MIN(M,N)) contains the scalar factors of the elementary reflectors as returned by CGEQRF of the M-by-N input matrix F. If the call to CGEDMDQ is only workspace query, then ZWORK(1) contains the minimal complex workspace length and ZWORK(2) is the optimal complex workspace length. Hence, the length of work is at least 2. See the description of LZWORK.
β¨ LZWORK β¨
LZWORK(input)INTEGERβ the minimal length of the workspace vectorZWORK.LZWORKis calculated as follows. Let
MLWQR = N (minimal workspace for CGEQRF[M,N])
MLWDMD = minimal workspace for CGEDMD (see the
description of LWORK in CGEDMD)
MLWMQR = N (minimal workspace for
ZUNMQR['L','N',M,N,N])
MLWGQR = N (minimal workspace for ZUNGQR[M,N,N])
MINMN = MIN(M,N)
Then
LZWORK = MAX(2, MIN(M,N)+MLWQR, MINMN+MLWDMD)
is further updated as follows:
if JOBZ == 'V' or JOBZ == 'F' THEN
LZWORK = MAX( LZWORK, MINMN+MLWMQR )
if JOBQ == 'Q' THEN
LZWORK = MAX( ZLWORK, MINMN+MLWGQR)
(yes, ZLWORK β that's what it says, bestie, we don't fix it, we report it π
)
β¨ WORK β¨
WORK(workspace/output)REAL(KIND=WP)LWORK-by-1 array β on exit,WORK(1:N-1)contains the singular values of the input submatrixF(1:M,1:N-1). If the call toCGEDMDQis only workspace query, thenWORK(1)contains the minimal workspace length andWORK(2)is the optimal workspace length. hence, the length of work is at least 2. See the description ofLWORK. π
β¨ LWORK β¨
LWORK(input)INTEGERβ the minimal length of the workspace vectorWORK.LWORKis the same as inCGEDMD, because inCGEDMDQonlyCGEDMDrequires real workspace for snapshots of dimensionsMIN(M,N)-by-(N-1).
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. π
β¨ IWORK β¨
IWORK(workspace/output)INTEGERLIWORK-by-1 array** β workspace that is required only ifWHTSVDequals2,3or4. (See the description ofWHTSVD.) If on entryLWORK =-1orLIWORK=-1, then the minimal length ofIWORKis computed and returned inIWORK(1). See the description ofLIWORK. π¦
β¨ LIWORK β¨
and that's where we hand off to LIWORK β hold that thought, it's coming π
LIWORK(input) INTEGER β the minimal length of the workspace vectorIWORK. Bestie, this is the size check for the integer workspace, okay? π- If
WHTSVD == 1, then onlyIWORK(1)is used;LIWORK >=1. - Let
M1=MIN(M,N),N1=N-1. Then: - If
WHTSVD == 2, thenLIWORK >= MAX(1,8*MIN(M,N)). - If
WHTSVD == 3, thenLIWORK >= MAX(1,M+N-1). - If
WHTSVD == 4, thenLIWORK >= MAX(3,M+3*N). - If on entry
LIWORK = -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. iykyk, this is the βjust tell me how much space I needβ mode β¨
- If
INFO(output) INTEGER β the status report, and she is very honest:-i < 0β on entry, thei-th argument had an illegal value. π¨= 0β successful return. slay, we love a clean exit π= 1β void input. Quick exit (M=0orN=0). π«₯= 2β the SVD computation ofXdid not converge. Suggestion: check the input data and/or repeat with differentWHTSVD. π= 3β the computation of the eigenvalues did not converge. π= 4β 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. so like, itβs a warning flag, not a vibe cancellation β proceed with the original or modified data, bestie π«Ά
π Author
Zlatko Drmac
Definition at line 552 of file cgedmdq.f90.
π Author
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