Complexity of the Fourier transform on the Johnson graph
Abstract
The set of -subsets of an -set has a natural graph structure where two -subsets are connected if and only if the size of their intersection is . This is known as the Johnson graph. The symmetric group acts on the space of complex functions on and this space has a multiplicity-free decomposition as sum of irreducible representations of , so it has a well-defined Gelfand-Tsetlin basis up to scalars. The Fourier transform on the Johnson graph is defined as the change of basis matrix from the delta function basis to the Gelfand-Tsetlin basis. The direct application of this matrix to a generic vector requires arithmetic operations. We show that --in analogy with the classical Fast Fourier Transform on the discrete circle-- this matrix can be factorized as a product of orthogonal matrices, each one with at most two nonzero elements in each column. This factorization shows that the number of arithmetic operations required to apply this matrix to a generic vector is bounded above by . As a consequence, we show that the problem of computing all the weights of the irreducible components of a given function can be solved in operations, improving the previous bound when asymptotically dominates in a non-uniform model of computation. The same improvement is achieved for the problem of computing the isotypic projection onto a single component. The proof is based on the construction of intermediate bases, each one parametrized by certain pairs composed by a standard Young tableau and a word. The parametrization of each basis is obtained via the Robinson-Schensted insertion algorithm.
Keywords
Cite
@article{arxiv.1704.06299,
title = {Complexity of the Fourier transform on the Johnson graph},
author = {Rodrigo Iglesias and Mauro Natale},
journal= {arXiv preprint arXiv:1704.06299},
year = {2018}
}