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HiPPO LegS, LegT, and LagT matrices have normal-plus-low-rank form after specified similarities
Statement
Index rows and columns by . Define the real LegS coefficient matrix by when , , and when . In the LegS coefficient ODE for this matrix is multiplied by the time-dependent scalar ; the matrix assertion below does not make that ODE time-invariant. For , define the LegT state generator by when and when . Define the original HiPPO LagT state generator by when and when . Here is conjugate transpose, a complex matrix is normal when , and a square matrix is unitary when . For LegS and LagT use the identity similarity; for LegT use the invertible diagonal similarity . Each transformed matrix is a difference with normal and for LegS and LagT and for LegT. Consequently the equivalent finite-dimensional complex state-space matrix has a normal-plus-low-rank representation, and a unitary change of state coordinates gives diagonal-plus-low-rank form. Under any state change , the input and output vectors change to and , respectively.
Statement references
Facts & Assumptions
Given: The finite matrices in the Statement, the parameter for LegT, and finite-dimensional complex state coordinates.
DPLR structured state-space parameterization: a normal-plus-low-rank matrix has form with unitary and diagonal ; under the state change , the input and output vectors become and .
Complex spectral theorem: a normal endomorphism of a finite-dimensional complex inner product space has an orthonormal eigenbasis, and conversely: every normal endomorphism of a finite-dimensional complex inner product space has an orthonormal basis of eigenvectors.
Proof
Put and define the real skew-symmetric matrix by for , for , and . The transpose is , so over its conjugate transpose is also ; hence is normal. With , entrywise comparison gives : below the diagonal the entries are , above they cancel to zero, and on the diagonal they are . Since a scalar shift of a normal matrix is normal and has rank at most one, this is the required LegS decomposition. This assertion concerns the finite coefficient matrix only; the factor in the LegS ODE remains time-dependent.
Define with entries below the diagonal, above it, and zero on the diagonal. It is real skew-symmetric and therefore normal. For , entrywise comparison gives : below the diagonal the two terms sum to , above they sum to zero, and on the diagonal they sum to . Thus the original LagT generator is a normal matrix minus a rank-at-most-one matrix.
For LegT let and . Define for , and for . Then direct entry evaluation gives : for , , while for , . Write , where when and have the same parity and is zero otherwise. The matrix is the sum of the outer products of the even-index and odd-index indicator vectors, so its rank is at most two. For opposite parities, below the diagonal and above it; for equal parities and on the diagonal, . Thus . The invertible diagonal matrix gives . The first term is real skew-symmetric and hence normal; the second has rank at most two. The diagonal similarity is essential: this proves the claim for an equivalent state-space matrix, not unitary similarity of the raw LegT matrix.
In each case write the resulting generator as with normal: for LegS and LagT the factors are the displayed real vectors divided by , and for LegT use the even and odd indicator columns multiplied by as both factors. By [F2], choose a unitary matrix with diagonal. Then , preserving the low-rank bound. If the original coordinates were changed by , the total state change is ; substitution into , gives and output vector . These are exactly the state-coordinate transformations required for an equivalent DPLR model.
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Sources
- Gu, Goel, and Ré, Efficiently Modeling Long Sequences with Structured State Spaces, Theorem 1 and Appendix C.1 (standard reference, not scraped)
- Gu et al., HiPPO: Recurrent Memory with Optimal Polynomial Projections, §2.3 and Appendices D.1–D.3 (standard reference, not scraped)