Partial $\ell_1$ optimization in random linear systems -- finite dimensions
Abstract
In this paper we provide a complementary set of results to those we present in our companion work \cite{Stojnicl1HidParasymldp} regarding the behavior of the so-called partial (a variant of the standard heuristic often employed for solving under-determined systems of linear equations). As is well known through our earlier works \cite{StojnicICASSP10knownsupp,StojnicTowBettCompSens13}, the partial also exhibits the phase-transition (PT) phenomenon, discovered and well understood in the context of the standard through Donoho's and our own works \cite{DonohoPol,DonohoUnsigned,StojnicCSetam09,StojnicUpper10}. \cite{Stojnicl1HidParasymldp} goes much further though and, in addition to the determination of the partial 's phase-transition curves (PT curves) (which had already been done in \cite{StojnicICASSP10knownsupp,StojnicTowBettCompSens13}), provides a substantially deeper understanding of the PT phenomena through a study of the underlying large deviations principles (LDPs). As the PT and LDP phenomena are by their definitions related to large dimensional settings, both sets of our works, \cite{StojnicICASSP10knownsupp,StojnicTowBettCompSens13} and \cite{Stojnicl1HidParasymldp}, consider what is typically called the asymptotic regime. In this paper we move things in a different direction and consider finite dimensional scenarios. Basically, we provide explicit performance characterizations for any given collection of systems/parameters dimensions. We do so for two different variants of the partial , one that we call exactly the partial and another one, possibly a bit more practical, that we call the hidden partial .
Cite
@article{arxiv.1612.07436,
title = {Partial $\ell_1$ optimization in random linear systems -- finite dimensions},
author = {Mihailo Stojnic},
journal= {arXiv preprint arXiv:1612.07436},
year = {2016}
}
Comments
arXiv admin note: text overlap with arXiv:1612.06344