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Intuitive derivation of loop inverses and array algebra
Abstract Array algebra forms the general base of fast transforms and multilinear algebra making rigorous solutions of a large number (millions) of parameters computationally feasible. Loop inverses are operators solving the problem of general matrix inverses. Their derivation starts from the inconsistent linear equations$$\mathop A\limits_{m n} \mathop X\limits_{n ,1} \ne \mathop L\limits_{m ,1} $$ by a parameter exchangeX→L0, where$$\mathop {L_0 }\limits_{p , 1} = \mathop {A_0 }\limits_{p n} \mathop X\limits_{n , 1} $$X is a set of unknown observables,A0 forming a basis of the so called “problem space”. The resulting full rank design matrix of parameters $ L_{0} $ and its ℓ-inverse reveal properties speeding the computational least squares solution$$\mathop {\hat L_0 }\limits_{p , 1} $$ expressed in observed values$$\mathop L\limits_{m , 1} $$. The loop inverses are found by the back substitution expressing ∧X in terms ofL through$$\hat L_0 $$. Ifp=rank (A) ≤n, this chain operator creates the pseudoinverseA+. The idea of loop inverses and array algebra started in the late60's from the further specialized case,p=n=rank (A), where the loop inverse A0−1(AA0−1)ℓ reduces into the ℓ-inverse $ A^{ℓ} $=($ A^{T} $A)−1$ A^{T} $. The physical interpretation of the design matrixA A0−1 as an interpolator, associated with the parametersL0, and the consideration of its multidimensional version has resulted in extended rules of matrix and tensor calculus and mathematical statistics called array algebra.
Intuitive derivation of loop inverses and array algebra
Abstract Array algebra forms the general base of fast transforms and multilinear algebra making rigorous solutions of a large number (millions) of parameters computationally feasible. Loop inverses are operators solving the problem of general matrix inverses. Their derivation starts from the inconsistent linear equations$$\mathop A\limits_{m n} \mathop X\limits_{n ,1} \ne \mathop L\limits_{m ,1} $$ by a parameter exchangeX→L0, where$$\mathop {L_0 }\limits_{p , 1} = \mathop {A_0 }\limits_{p n} \mathop X\limits_{n , 1} $$X is a set of unknown observables,A0 forming a basis of the so called “problem space”. The resulting full rank design matrix of parameters $ L_{0} $ and its ℓ-inverse reveal properties speeding the computational least squares solution$$\mathop {\hat L_0 }\limits_{p , 1} $$ expressed in observed values$$\mathop L\limits_{m , 1} $$. The loop inverses are found by the back substitution expressing ∧X in terms ofL through$$\hat L_0 $$. Ifp=rank (A) ≤n, this chain operator creates the pseudoinverseA+. The idea of loop inverses and array algebra started in the late60's from the further specialized case,p=n=rank (A), where the loop inverse A0−1(AA0−1)ℓ reduces into the ℓ-inverse $ A^{ℓ} $=($ A^{T} $A)−1$ A^{T} $. The physical interpretation of the design matrixA A0−1 as an interpolator, associated with the parametersL0, and the consideration of its multidimensional version has resulted in extended rules of matrix and tensor calculus and mathematical statistics called array algebra.
Intuitive derivation of loop inverses and array algebra
Rauhala, Urho A. (Autor:in)
Bulletin Géodésique ; 53
1979
Aufsatz (Zeitschrift)
Elektronische Ressource
Englisch
Intuitive derivation of loop inverses and array algebra
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