Partonic distribution functions and amplitudes using tensor network methods
Zhong-Bo Kang, Noah Moran, Peter Nguyen, Wenyang Qian
TL;DR
The paper addresses the challenge of directly computing parton distribution functions (PDFs) and distribution amplitudes (DAs) from first principles, which are time-dependent light-cone objects. It introduces a uniform tensor-network framework that encodes hadrons as matrix product states and performs real-time evolution to extract PDFs and DAs within the 1+1D Nambu–Jona-Lasinio model, mapping fermionic degrees of freedom to spins via Jordan-Wigner. The authors demonstrate direct extraction of PDFs and DAs, achieving convergence up to 102 qubits and observing mass- and coupling-dependent behavior with qualitative agreement to perturbative and non-relativistic limits, validated against exact diagonalization and quantum circuit simulations. This work establishes tensor networks as a viable path to hadron-structure calculations from first principles and sets the stage for extensions to gauge theories, multiple flavors, and higher dimensions as computational methods and hardware advance.
Abstract
Calculations of the parton distribution function (PDF) and distribution amplitude (DA) are highly relevant to core experimental programs as they provide non-perturbative inputs to inclusive and exclusive processes, respectively. Direct computation of the PDFs and DAs remains challenging because they are non-perturbative quantities defined as light-cone correlators of quark and gluon fields, and are therefore inherently time-dependent. In this work, we use a uniform quantum strategy based on tensor network simulation techniques to directly extract these hadronic quantities from first principles using the matrix product state of the hadrons in the same setup. We present exemplary numerical calculations with the Nambu-Jona-Lasinio model in 1+1 dimensions and compare with available exact diagonalization and quantum circuit simulation results. Using tensor networks, we evaluate the PDF and DA at various strong couplings in the large-qubit limit, which is consistent with expectations at perturbative and non-relativistic limits.
