Arnold--Nielsen Geometry for Complexity-Deformed Noncommutative Transport
Abstract
We deform the Carlen--Maas--Wirth framework for noncommutative dynamical optimal transport by an Arnold--Nielsen type complexity operator. A positive state-independent operator $G$ compatible with the Hilbert bimodule structure of a noncommutative differential calculus $\partial\colon\M\to\Hcal$ can be absorbed into the calculus itself, \[ \partial_G:=G^{1/2}\partial. \] The corresponding complexity-weighted transport problem is exactly the unweighted transport problem generated by $\partial_G$,...
Description / Details
We deform the Carlen--Maas--Wirth framework for noncommutative dynamical optimal transport by an Arnold--Nielsen type complexity operator. A positive state-independent operator compatible with the Hilbert bimodule structure of a noncommutative differential calculus can be absorbed into the calculus itself, [ \partial_G:=G^{1/2}\partial. ] The corresponding complexity-weighted transport problem is exactly the unweighted transport problem generated by , whenever the deformed quadratic form remains Dirichlet. In finite dimensions we prove existence of minimizers for density-dependent Petz-class metrics and for fixed physical complexity weights, the latter without commutation between and the state-dependent mobility. On unitary orbits we identify the induced distance with a quotient metric coming from a right-invariant complexity geometry. This yields an exact Bell-state preparation result via Clairaut's relation and an exactly computed restricted-path upper bound for GHZ preparation; the Lindblad detailed-balance case is included only as entropy-gradient-flow background.
Source: arXiv:2607.20388v1 - http://arxiv.org/abs/2607.20388v1 PDF: https://arxiv.org/pdf/2607.20388v1 Original Link: http://arxiv.org/abs/2607.20388v1
Please sign in to join the discussion.
No comments yet. Be the first to share your thoughts!
Jul 23, 2026
Quantum Computing
Quantum Physics
0