{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:NSUMVS2W5BCKTQVQCGZMSTFDUE","short_pith_number":"pith:NSUMVS2W","schema_version":"1.0","canonical_sha256":"6ca8cacb56e844a9c2b011b2c94ca3a13f6a6aebdf03a6182f2bfe3e1664a449","source":{"kind":"arxiv","id":"1105.3969","version":1},"attestation_state":"computed","paper":{"title":"Seiberg-Witten and \"Polyakov-like\" magnetic bion confinements are continuously connected","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","hep-ph"],"primary_cat":"hep-th","authors_text":"Erich Poppitz, Mithat Unsal","submitted_at":"2011-05-19T19:32:26Z","abstract_excerpt":"We study four-dimensional N=2 supersymmetric pure-gauge (Seiberg-Witten) theory and its N=1 mass perturbation by using compactification S**1 x R**3. It is well known that on R**4 (or at large S**1) the perturbed theory realizes confinement through monopole or dyon condensation. At small S**1, we demonstrate that confinement is induced by a generalization of Polyakov's three-dimensional instanton mechanism to a locally four-dimensional theory - the magnetic bion mechanism - which also applies to a large class of nonsupersymmetric theories. Using a large- vs. small-L Poisson duality, we show tha"},"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":"1105.3969","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-05-19T19:32:26Z","cross_cats_sorted":["hep-lat","hep-ph"],"title_canon_sha256":"24ba8146800feeb47030e51722ea782f962018cb026116d25df88e889f417911","abstract_canon_sha256":"43f9c5090374cecc4b594f0638ecc454b5f305790ef1036004ee6f3625536a71"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:01:53.958415Z","signature_b64":"7UKcW//SG1RrDAckTevT5jSRlYE7iprIw6b4++VXqjzVDvVscnIlggHQlUGXbADEjhbWO+sOvmeLu0DG2mvTBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6ca8cacb56e844a9c2b011b2c94ca3a13f6a6aebdf03a6182f2bfe3e1664a449","last_reissued_at":"2026-05-18T02:01:53.957816Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:01:53.957816Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Seiberg-Witten and \"Polyakov-like\" magnetic bion confinements are continuously connected","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","hep-ph"],"primary_cat":"hep-th","authors_text":"Erich Poppitz, Mithat Unsal","submitted_at":"2011-05-19T19:32:26Z","abstract_excerpt":"We study four-dimensional N=2 supersymmetric pure-gauge (Seiberg-Witten) theory and its N=1 mass perturbation by using compactification S**1 x R**3. It is well known that on R**4 (or at large S**1) the perturbed theory realizes confinement through monopole or dyon condensation. At small S**1, we demonstrate that confinement is induced by a generalization of Polyakov's three-dimensional instanton mechanism to a locally four-dimensional theory - the magnetic bion mechanism - which also applies to a large class of nonsupersymmetric theories. Using a large- vs. small-L Poisson duality, we show tha"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1105.3969","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":""},"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":"1105.3969","created_at":"2026-05-18T02:01:53.957912+00:00"},{"alias_kind":"arxiv_version","alias_value":"1105.3969v1","created_at":"2026-05-18T02:01:53.957912+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1105.3969","created_at":"2026-05-18T02:01:53.957912+00:00"},{"alias_kind":"pith_short_12","alias_value":"NSUMVS2W5BCK","created_at":"2026-05-18T12:26:37.096874+00:00"},{"alias_kind":"pith_short_16","alias_value":"NSUMVS2W5BCKTQVQ","created_at":"2026-05-18T12:26:37.096874+00:00"},{"alias_kind":"pith_short_8","alias_value":"NSUMVS2W","created_at":"2026-05-18T12:26:37.096874+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.27066","citing_title":"Perturbative Coulomb branches on $\\mathbb{R}^3\\times S^1$: the global D-term potential","ref_index":8,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NSUMVS2W5BCKTQVQCGZMSTFDUE","json":"https://pith.science/pith/NSUMVS2W5BCKTQVQCGZMSTFDUE.json","graph_json":"https://pith.science/api/pith-number/NSUMVS2W5BCKTQVQCGZMSTFDUE/graph.json","events_json":"https://pith.science/api/pith-number/NSUMVS2W5BCKTQVQCGZMSTFDUE/events.json","paper":"https://pith.science/paper/NSUMVS2W"},"agent_actions":{"view_html":"https://pith.science/pith/NSUMVS2W5BCKTQVQCGZMSTFDUE","download_json":"https://pith.science/pith/NSUMVS2W5BCKTQVQCGZMSTFDUE.json","view_paper":"https://pith.science/paper/NSUMVS2W","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1105.3969&json=true","fetch_graph":"https://pith.science/api/pith-number/NSUMVS2W5BCKTQVQCGZMSTFDUE/graph.json","fetch_events":"https://pith.science/api/pith-number/NSUMVS2W5BCKTQVQCGZMSTFDUE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NSUMVS2W5BCKTQVQCGZMSTFDUE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NSUMVS2W5BCKTQVQCGZMSTFDUE/action/storage_attestation","attest_author":"https://pith.science/pith/NSUMVS2W5BCKTQVQCGZMSTFDUE/action/author_attestation","sign_citation":"https://pith.science/pith/NSUMVS2W5BCKTQVQCGZMSTFDUE/action/citation_signature","submit_replication":"https://pith.science/pith/NSUMVS2W5BCKTQVQCGZMSTFDUE/action/replication_record"}},"created_at":"2026-05-18T02:01:53.957912+00:00","updated_at":"2026-05-18T02:01:53.957912+00:00"}