On the Relationship of the quasilocal angular momentum to Interior Flow Analysis

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Auteur principal: Rayan D. Peru
Format: Recurso digital
Publié: Zenodo 2026
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_version_ 1866901235089539072
author Rayan D. Peru
author_facet Rayan D. Peru
contents <p>A crucial feature of Theorem 4.4 is that it requires <em>only</em> boundary data, no knowledge of the interior of the excised region <span><span>V</span></span> is needed. The angular momentum change is completely determined by the integral of <span><span><span><span>α</span><span>d</span><span>β</span><span>∧</span></span><span><span><span>ξ</span><span><span><span><span><span><span>♭</span></span></span></span></span></span></span></span></span></span> over <span><span>∂V</span><span><span><span>∂</span><span>V</span></span></span></span>. This is not circular; it reflects the fact that angular momentum, when properly defined via the Clebsch-Komar identity, is a quasilocal charge. One does not need to solve the full 3+1 evolution equations or verify entropy monotonicity in the interior to know how angular momentum behaves across surgery. The Surgical Flux Theorem reveals that angular momentum is <em>topologically blind, </em> it depends only on the boundary ∂V, not on the interior topology or its replacement. The surgical procedure could excise a region of any topology (a ball, a torus, a disjoint union) and replace it with any interior satisfying the matching conditions; the angular momentum change is <em>identical</em> as long as the boundary data is fixed. Thus, for angular momentum accounting, the intricate topology of surgical modification is entirely redundant. The boundary flux tells the complete story.</p>
format Recurso digital
id zenodo_https___doi_org_10_5281_zenodo_18722423
institution Zenodo
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publishDate 2026
publisher Zenodo
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spellingShingle On the Relationship of the quasilocal angular momentum to Interior Flow Analysis
Rayan D. Peru
<p>A crucial feature of Theorem 4.4 is that it requires <em>only</em> boundary data, no knowledge of the interior of the excised region <span><span>V</span></span> is needed. The angular momentum change is completely determined by the integral of <span><span><span><span>α</span><span>d</span><span>β</span><span>∧</span></span><span><span><span>ξ</span><span><span><span><span><span><span>♭</span></span></span></span></span></span></span></span></span></span> over <span><span>∂V</span><span><span><span>∂</span><span>V</span></span></span></span>. This is not circular; it reflects the fact that angular momentum, when properly defined via the Clebsch-Komar identity, is a quasilocal charge. One does not need to solve the full 3+1 evolution equations or verify entropy monotonicity in the interior to know how angular momentum behaves across surgery. The Surgical Flux Theorem reveals that angular momentum is <em>topologically blind, </em> it depends only on the boundary ∂V, not on the interior topology or its replacement. The surgical procedure could excise a region of any topology (a ball, a torus, a disjoint union) and replace it with any interior satisfying the matching conditions; the angular momentum change is <em>identical</em> as long as the boundary data is fixed. Thus, for angular momentum accounting, the intricate topology of surgical modification is entirely redundant. The boundary flux tells the complete story.</p>
title On the Relationship of the quasilocal angular momentum to Interior Flow Analysis
url https://doi.org/10.5281/zenodo.18722423