{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2001:2KC4FLNPLYTBBFLK53CGFJX4X7","short_pith_number":"pith:2KC4FLNP","schema_version":"1.0","canonical_sha256":"d285c2adaf5e2610956aeec462a6fcbfe6232b29d0ec17ce913ea8a898114b9a","source":{"kind":"arxiv","id":"hep-ph/0101317","version":1},"attestation_state":"computed","paper":{"title":"Magnetic charge of finite lifetime in SU(2) gluodynamics","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ralf Hofmann","submitted_at":"2001-01-29T11:56:56Z","abstract_excerpt":"A self-dual, localized solution to the classical SU(2) Yang-Mills equation in Euclidean spacetime, which formally possesses infinite action, is investigated in view of its U(1) charge content after Abelian projection. This is suggested by noting that the solution satisfies 't Hooft's differential projection condition away from the singularities. As a result the existence of dynamical, magnetic charge of finite lifetime is established. A covariant cutoff for the action is introduced by demanding the solution to be close to an instanton topologically. This is in analogy to the \\underline{calcula"},"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":"hep-ph/0101317","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2001-01-29T11:56:56Z","cross_cats_sorted":[],"title_canon_sha256":"e13ae723e4636d69c172783ddfdcf01a9bc36c07e497c4fb8faaa8b6a1eeebe3","abstract_canon_sha256":"3cd16f215349a856d54ab97743def427920720b74de8e0175dd537496c16e1db"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:27:47.494006Z","signature_b64":"QTOCuJ7RWhigcRqWTbXNlvMx0ljVj8Ul/moQEsZrtU1d01XMsUyheVqW6mnKYS6YAGVZDpJF9jMTQGkw9+58BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d285c2adaf5e2610956aeec462a6fcbfe6232b29d0ec17ce913ea8a898114b9a","last_reissued_at":"2026-07-04T14:27:47.493549Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:27:47.493549Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Magnetic charge of finite lifetime in SU(2) gluodynamics","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ralf Hofmann","submitted_at":"2001-01-29T11:56:56Z","abstract_excerpt":"A self-dual, localized solution to the classical SU(2) Yang-Mills equation in Euclidean spacetime, which formally possesses infinite action, is investigated in view of its U(1) charge content after Abelian projection. This is suggested by noting that the solution satisfies 't Hooft's differential projection condition away from the singularities. As a result the existence of dynamical, magnetic charge of finite lifetime is established. A covariant cutoff for the action is introduced by demanding the solution to be close to an instanton topologically. This is in analogy to the \\underline{calcula"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0101317","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-ph/0101317/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"hep-ph/0101317","created_at":"2026-07-04T14:27:47.493627+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0101317v1","created_at":"2026-07-04T14:27:47.493627+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0101317","created_at":"2026-07-04T14:27:47.493627+00:00"},{"alias_kind":"pith_short_12","alias_value":"2KC4FLNPLYTB","created_at":"2026-07-04T14:27:47.493627+00:00"},{"alias_kind":"pith_short_16","alias_value":"2KC4FLNPLYTBBFLK","created_at":"2026-07-04T14:27:47.493627+00:00"},{"alias_kind":"pith_short_8","alias_value":"2KC4FLNP","created_at":"2026-07-04T14:27:47.493627+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/2KC4FLNPLYTBBFLK53CGFJX4X7","json":"https://pith.science/pith/2KC4FLNPLYTBBFLK53CGFJX4X7.json","graph_json":"https://pith.science/api/pith-number/2KC4FLNPLYTBBFLK53CGFJX4X7/graph.json","events_json":"https://pith.science/api/pith-number/2KC4FLNPLYTBBFLK53CGFJX4X7/events.json","paper":"https://pith.science/paper/2KC4FLNP"},"agent_actions":{"view_html":"https://pith.science/pith/2KC4FLNPLYTBBFLK53CGFJX4X7","download_json":"https://pith.science/pith/2KC4FLNPLYTBBFLK53CGFJX4X7.json","view_paper":"https://pith.science/paper/2KC4FLNP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0101317&json=true","fetch_graph":"https://pith.science/api/pith-number/2KC4FLNPLYTBBFLK53CGFJX4X7/graph.json","fetch_events":"https://pith.science/api/pith-number/2KC4FLNPLYTBBFLK53CGFJX4X7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2KC4FLNPLYTBBFLK53CGFJX4X7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2KC4FLNPLYTBBFLK53CGFJX4X7/action/storage_attestation","attest_author":"https://pith.science/pith/2KC4FLNPLYTBBFLK53CGFJX4X7/action/author_attestation","sign_citation":"https://pith.science/pith/2KC4FLNPLYTBBFLK53CGFJX4X7/action/citation_signature","submit_replication":"https://pith.science/pith/2KC4FLNPLYTBBFLK53CGFJX4X7/action/replication_record"}},"created_at":"2026-07-04T14:27:47.493627+00:00","updated_at":"2026-07-04T14:27:47.493627+00:00"}