{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:VXMMUXDRENQAPOGLGT3OR4FAFK","short_pith_number":"pith:VXMMUXDR","schema_version":"1.0","canonical_sha256":"add8ca5c71236007b8cb34f6e8f0a02abb16fc02737d6e1647bd5429ee881607","source":{"kind":"arxiv","id":"1704.01276","version":2},"attestation_state":"computed","paper":{"title":"Dyon and magnetic monopole in Yang--Mills theory derived through the complementary gauge-scalar model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Kei-Ichi Kondo, Matthias Warschinke, Ryutaro Matsudo, Shogo Nishino","submitted_at":"2017-04-05T06:03:52Z","abstract_excerpt":"We show that dyon and magnetic monopole can be constructed in the gauge-independent way for the $SU(2)$ Yang--Mills theory even in the absence of the scalar field. This result is derived from the recent proposal for obtaining non-trivial topological configurations responsible for quark confinement in the Yang-Mills theory based on the Confinement-Higgs complementary relationship between the pure Yang-Mills theory and the gauge-scalar model with an adjoint scalar field of the fixed length. We discuss how such configurations have the implications for quark confinement."},"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":"1704.01276","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-04-05T06:03:52Z","cross_cats_sorted":[],"title_canon_sha256":"e5681052843975f038ffcb334efaa8d291e1b434be417a260b0af7d75f20d2bd","abstract_canon_sha256":"2fae754fe909b425698eb7e7c647aa60f61e3d8d360a0a4f12ee001cbd1a4188"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:50:07.558286Z","signature_b64":"ZoUMDjBte4dBuYTWVzGxvQzklpZbsSKsOzE4zdhKtC4D9sA5bSAVqdL7tybNkN6pCLvEnCJmNc6tCLFxZ9SkCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"add8ca5c71236007b8cb34f6e8f0a02abb16fc02737d6e1647bd5429ee881607","last_reissued_at":"2026-05-17T23:50:07.557799Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:50:07.557799Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dyon and magnetic monopole in Yang--Mills theory derived through the complementary gauge-scalar model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Kei-Ichi Kondo, Matthias Warschinke, Ryutaro Matsudo, Shogo Nishino","submitted_at":"2017-04-05T06:03:52Z","abstract_excerpt":"We show that dyon and magnetic monopole can be constructed in the gauge-independent way for the $SU(2)$ Yang--Mills theory even in the absence of the scalar field. This result is derived from the recent proposal for obtaining non-trivial topological configurations responsible for quark confinement in the Yang-Mills theory based on the Confinement-Higgs complementary relationship between the pure Yang-Mills theory and the gauge-scalar model with an adjoint scalar field of the fixed length. We discuss how such configurations have the implications for quark confinement."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.01276","kind":"arxiv","version":2},"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":"1704.01276","created_at":"2026-05-17T23:50:07.557880+00:00"},{"alias_kind":"arxiv_version","alias_value":"1704.01276v2","created_at":"2026-05-17T23:50:07.557880+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.01276","created_at":"2026-05-17T23:50:07.557880+00:00"},{"alias_kind":"pith_short_12","alias_value":"VXMMUXDRENQA","created_at":"2026-05-18T12:31:49.984773+00:00"},{"alias_kind":"pith_short_16","alias_value":"VXMMUXDRENQAPOGL","created_at":"2026-05-18T12:31:49.984773+00:00"},{"alias_kind":"pith_short_8","alias_value":"VXMMUXDR","created_at":"2026-05-18T12:31:49.984773+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/VXMMUXDRENQAPOGLGT3OR4FAFK","json":"https://pith.science/pith/VXMMUXDRENQAPOGLGT3OR4FAFK.json","graph_json":"https://pith.science/api/pith-number/VXMMUXDRENQAPOGLGT3OR4FAFK/graph.json","events_json":"https://pith.science/api/pith-number/VXMMUXDRENQAPOGLGT3OR4FAFK/events.json","paper":"https://pith.science/paper/VXMMUXDR"},"agent_actions":{"view_html":"https://pith.science/pith/VXMMUXDRENQAPOGLGT3OR4FAFK","download_json":"https://pith.science/pith/VXMMUXDRENQAPOGLGT3OR4FAFK.json","view_paper":"https://pith.science/paper/VXMMUXDR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1704.01276&json=true","fetch_graph":"https://pith.science/api/pith-number/VXMMUXDRENQAPOGLGT3OR4FAFK/graph.json","fetch_events":"https://pith.science/api/pith-number/VXMMUXDRENQAPOGLGT3OR4FAFK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VXMMUXDRENQAPOGLGT3OR4FAFK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VXMMUXDRENQAPOGLGT3OR4FAFK/action/storage_attestation","attest_author":"https://pith.science/pith/VXMMUXDRENQAPOGLGT3OR4FAFK/action/author_attestation","sign_citation":"https://pith.science/pith/VXMMUXDRENQAPOGLGT3OR4FAFK/action/citation_signature","submit_replication":"https://pith.science/pith/VXMMUXDRENQAPOGLGT3OR4FAFK/action/replication_record"}},"created_at":"2026-05-17T23:50:07.557880+00:00","updated_at":"2026-05-17T23:50:07.557880+00:00"}