What happens to wavepackets of fermions when scattered by the Maldacena-Ludwig wall?

Fuente: arXiv
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Main Authors: Tachikawa, Yuji, Tsuji, Keita, Watanabe, Masataka
Format: Preprint
Published: 2026
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author Tachikawa, Yuji
Tsuji, Keita
Watanabe, Masataka
author_facet Tachikawa, Yuji
Tsuji, Keita
Watanabe, Masataka
contents We study wavepackets of exotic excitations after two-dimensional fermions are scattered by the boundary condition constructed by Maldacena and Ludwig, which turns elementary excitations into exotic fractionally-charged objects. They are of interest in the s-wave approximation of the fermion-monopole scattering in four-dimensional QED and of the multi-channel Kondo effect. We in particular give an explicit expression of the outgoing state of a pair of such particles; we then examine its properties, such as the charge density $\langle J(x)\rangle$ and the expectation value $\langle N\rangle$ of the number of fermions and anti-fermions in the state. The charge density $\langle J(x)\rangle$ is found to be localized with its integral finite and fractional, while the expectation value $\langle N\rangle$ diverges when the wavepacket is localized to a point.
format Preprint
id arxiv_https___arxiv_org_abs_2603_25508
institution arXiv
publishDate 2026
record_format arxiv
spellingShingle What happens to wavepackets of fermions when scattered by the Maldacena-Ludwig wall?
Tachikawa, Yuji
Tsuji, Keita
Watanabe, Masataka
High Energy Physics - Theory
Strongly Correlated Electrons
We study wavepackets of exotic excitations after two-dimensional fermions are scattered by the boundary condition constructed by Maldacena and Ludwig, which turns elementary excitations into exotic fractionally-charged objects. They are of interest in the s-wave approximation of the fermion-monopole scattering in four-dimensional QED and of the multi-channel Kondo effect. We in particular give an explicit expression of the outgoing state of a pair of such particles; we then examine its properties, such as the charge density $\langle J(x)\rangle$ and the expectation value $\langle N\rangle$ of the number of fermions and anti-fermions in the state. The charge density $\langle J(x)\rangle$ is found to be localized with its integral finite and fractional, while the expectation value $\langle N\rangle$ diverges when the wavepacket is localized to a point.
title What happens to wavepackets of fermions when scattered by the Maldacena-Ludwig wall?
topic High Energy Physics - Theory
Strongly Correlated Electrons
url https://arxiv.org/abs/2603.25508