Expected Complexity of Barcode Reduction
Barbara Giunti1, Guillaume Houry2, Michael Kerber3
1Graz University of Technology and SUNY University at Albany, 1400 Washington Avenue, HD-125, Albany, USA.
Abstract:
We study the algorithmic complexity of computing the persistence barcode of a randomly generated filtration. We provide a general technique to bound the expected complexity of reducing the boundary matrix in terms of the density of its reduced form. We apply this technique finding upper bounds for the average fill-in (number of non-zero entries) of the boundary matrix on Čech, Vietoris-Rips and Erdős-Rényi filtrations after matrix reduction, thus obtaining bounds on the expected complexity of the barcode computation. Our method is based on previous results on the expected Betti numbers of the corresponding complexes. Our fill-in bounds for Čech and Vietoris-Rips complexes are asymptotically tight up to a logarithmic factor. In particular, both our fill-in and computation bounds are better than the worst-case estimates. We also provide an Erdős-Rényi filtration realizing the worst-case fill-in and computation.
Related Concept Videos
Block Diagram Reduction
The first step in this process is the identification and relocation of a branch point. A branch point, where a...
Alcohols from Carbonyl Compounds: Reduction
Catalytic hydrogenation is similar to the reduction of an alkene or alkyne by adding H2 across the pi bond in the presence of transition metal catalysts like Raney Ni, Pd–C, Pt, or Ru. Aldehydes and ketones can be reduced by this method, often under mild to moderate heat (25–100°C) and...
Gaussian Elimination: Problem Solving
Probability Laws
Benzene to 1,4-Cyclohexadiene: Birch Reduction Mechanism
Biot-Savart Law: Problem-Solving
Consider a mobile phone battery bank as a source of steady current, which flows through the wire connected between the two. What is the magnitude of the magnetic field created by this current at a field point P?
To estimate the magnitude of the total magnetic field, we first consider a small current element of length dl, at a distance r from the field point. Now the following...


