Pion magnetic polarisability using the background field method
Ryan Bignell, Waseem Kamleh, Derek Leinweber

TL;DR
This paper calculates the pion's magnetic polarisability using lattice QCD with background magnetic fields, introducing new methods for improved precision in understanding hadron structure.
Contribution
It introduces a novel magnetic-field dependent eigenmode projector and employs a background-field corrected fermion action for more accurate lattice QCD calculations.
Findings
Precise determination of pion magnetic polarisability.
Implementation of a new eigenmode projector improves signal quality.
Use of background-field corrected fermion action enhances calculation accuracy.
Abstract
The magnetic polarisability is a fundamental property of hadrons, which provides insight into their structure in the low-energy regime. The pion magnetic polarisability is calculated using lattice QCD in the presence of background magnetic fields. The results presented are facilitated by the introduction of a new magnetic-field dependent quark-propagator eigenmode projector and the use of the background-field corrected clover fermion action. The magnetic polarisabilities are calculated in a relativistic formalism, and the excellent signal-to-noise property of pion correlation functions facilitates precise values.
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