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Volume 9 (2013) Article 6 pp. 273-282 [Note]
The Complexity of the Fermionant and Immanants of Constant Width
Received: November 11, 2011
Revised: January 20, 2013
Published: February 26, 2013
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Keywords: fermionant, immanant, partition function, statistical physics, determinant, permanent, computational complexity, graph theory, representation theory
ACM Classification: F.2.1
AMS Classification: 68Q17

Abstract: [Plain Text Version]

\newcommand{\Ferm}{\mathrm{Ferm}} \newcommand{\Imm}{\mathrm{Imm}} \newcommand{\oplusP}{\oplus \mathrm{P}} \newcommand{\NP}{\mathrm{NP}} \newcommand{\RP}{\mathrm{RP}}

In the context of statistical physics, Chandrasekharan and Wiese recently introduced the fermionant \Ferm_k, a determinant-like function of a matrix where each permutation \pi is weighted by -k raised to the number of cycles in \pi. We show that computing \Ferm_k is #P-hard under polynomial-time Turing reductions for any constant k > 2, and is \oplusP-hard for k=2, where both results hold even for the adjacency matrices of planar graphs. As a consequence, unless the polynomial-time hierarchy collapses, it is impossible to compute the immanant \Imm_\lambda \,A as a function of the Young diagram \lambda in polynomial time, even if the width of \lambda is restricted to be at most 2. In particular, unless \NP \subseteq \RP, \Ferm_2 is not in P, and there are Young diagrams \lambda of width 2 such that \Imm_\lambda is not in P.