{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:KCFLFTWURT7VMFQT4BFY2QF42A","short_pith_number":"pith:KCFLFTWU","schema_version":"1.0","canonical_sha256":"508ab2ced48cff561613e04b8d40bcd0367eb391c461670ab0ead6cbdfc063f2","source":{"kind":"arxiv","id":"1508.04165","version":3},"attestation_state":"computed","paper":{"title":"Finite Volume Corrections to the Electromagnetic Mass of Composite Particles","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"Brian C. Tiburzi, Jong-Wan Lee","submitted_at":"2015-08-17T21:56:37Z","abstract_excerpt":"The long-range electromagnetic interaction presents a challenge for numerical computations in QCD + QED. In addition to power-law finite volume effects, the standard lattice gauge theory approach introduces non-locality through removal of photon zero-momentum modes. The resulting finite volume effects must be quantitatively understood; and, to this end, non-relativistic effective field theories are an efficient tool, especially in the case of composite particles. Recently an oddity related to non-locality of the standard lattice approach was uncovered by the Budapest-Marseille-Wuppertal collab"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1508.04165","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2015-08-17T21:56:37Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"437143f9ac4daf47d06c3d48f2f7d3d2357b75934f5909a521eb1455f814b942","abstract_canon_sha256":"4b700410fb7c6e3af2c245de3802c08c80411983c92a44b491fa7d6f1335ecc1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:20:34.560122Z","signature_b64":"8HwMMbAD+Kj5qIRO5UvrZ+I4r1BHVK8K7+sNtLsOcB07uFJryKMptLhYGjuR8fCZYDhNKRcZYHNwUUowRTPHAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"508ab2ced48cff561613e04b8d40bcd0367eb391c461670ab0ead6cbdfc063f2","last_reissued_at":"2026-05-18T01:20:34.559653Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:20:34.559653Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Finite Volume Corrections to the Electromagnetic Mass of Composite Particles","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"Brian C. Tiburzi, Jong-Wan Lee","submitted_at":"2015-08-17T21:56:37Z","abstract_excerpt":"The long-range electromagnetic interaction presents a challenge for numerical computations in QCD + QED. In addition to power-law finite volume effects, the standard lattice gauge theory approach introduces non-locality through removal of photon zero-momentum modes. The resulting finite volume effects must be quantitatively understood; and, to this end, non-relativistic effective field theories are an efficient tool, especially in the case of composite particles. Recently an oddity related to non-locality of the standard lattice approach was uncovered by the Budapest-Marseille-Wuppertal collab"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1508.04165","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"1508.04165","created_at":"2026-05-18T01:20:34.559723+00:00"},{"alias_kind":"arxiv_version","alias_value":"1508.04165v3","created_at":"2026-05-18T01:20:34.559723+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1508.04165","created_at":"2026-05-18T01:20:34.559723+00:00"},{"alias_kind":"pith_short_12","alias_value":"KCFLFTWURT7V","created_at":"2026-05-18T12:29:27.538025+00:00"},{"alias_kind":"pith_short_16","alias_value":"KCFLFTWURT7VMFQT","created_at":"2026-05-18T12:29:27.538025+00:00"},{"alias_kind":"pith_short_8","alias_value":"KCFLFTWU","created_at":"2026-05-18T12:29:27.538025+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/KCFLFTWURT7VMFQT4BFY2QF42A","json":"https://pith.science/pith/KCFLFTWURT7VMFQT4BFY2QF42A.json","graph_json":"https://pith.science/api/pith-number/KCFLFTWURT7VMFQT4BFY2QF42A/graph.json","events_json":"https://pith.science/api/pith-number/KCFLFTWURT7VMFQT4BFY2QF42A/events.json","paper":"https://pith.science/paper/KCFLFTWU"},"agent_actions":{"view_html":"https://pith.science/pith/KCFLFTWURT7VMFQT4BFY2QF42A","download_json":"https://pith.science/pith/KCFLFTWURT7VMFQT4BFY2QF42A.json","view_paper":"https://pith.science/paper/KCFLFTWU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1508.04165&json=true","fetch_graph":"https://pith.science/api/pith-number/KCFLFTWURT7VMFQT4BFY2QF42A/graph.json","fetch_events":"https://pith.science/api/pith-number/KCFLFTWURT7VMFQT4BFY2QF42A/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KCFLFTWURT7VMFQT4BFY2QF42A/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KCFLFTWURT7VMFQT4BFY2QF42A/action/storage_attestation","attest_author":"https://pith.science/pith/KCFLFTWURT7VMFQT4BFY2QF42A/action/author_attestation","sign_citation":"https://pith.science/pith/KCFLFTWURT7VMFQT4BFY2QF42A/action/citation_signature","submit_replication":"https://pith.science/pith/KCFLFTWURT7VMFQT4BFY2QF42A/action/replication_record"}},"created_at":"2026-05-18T01:20:34.559723+00:00","updated_at":"2026-05-18T01:20:34.559723+00:00"}