{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:K44ZXEVPLHRZJ5IKW45E4AYG3F","short_pith_number":"pith:K44ZXEVP","schema_version":"1.0","canonical_sha256":"57399b92af59e394f50ab73a4e0306d95324bbd0c58a6edde06ca068104d963c","source":{"kind":"arxiv","id":"1706.05281","version":2},"attestation_state":"computed","paper":{"title":"Radiative corrections to the quark masses in the ferromagnetic Ising and Potts field theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"cond-mat.stat-mech","authors_text":"S. B. Rutkevich","submitted_at":"2017-06-16T14:19:48Z","abstract_excerpt":"We consider the Ising Field Theory (IFT), and the 3-state Potts Field Theory (PFT), which describe the scaling limits of the two- dimensional lattice q-state Potts model with q=2, and q=3, respectively. At zero magnetic field h=0, both field theories are integrable away from the critical point, have q degenerate vacua in the ferromagnetic phase, and q(q-1) particles of the same mass - the kinks interpolating between two different vacua. Application of a weak magnetic field induces confinement of kinks into bound states - the mesons (for q =2,3) consisting predominantly of two kinks, and baryon"},"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":"1706.05281","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-06-16T14:19:48Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"7e2ded36018cdc983a2a611d053f42dd8de6e7c0c1d18fe71f2a629b932fc739","abstract_canon_sha256":"a2c8b30ad98f1a934d90c4285e486c5b75a7f60cf1aa4798c052d5142e5686ef"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:34:41.508089Z","signature_b64":"7X5lUuWjEdToRrebK606gpW7YH1eUFznk/3kBvTyQVmdQ41s6XaAo9JktehLT9jbL2Zi02PDPVsPnH5EldOODQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"57399b92af59e394f50ab73a4e0306d95324bbd0c58a6edde06ca068104d963c","last_reissued_at":"2026-05-18T00:34:41.507407Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:34:41.507407Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Radiative corrections to the quark masses in the ferromagnetic Ising and Potts field theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"cond-mat.stat-mech","authors_text":"S. B. Rutkevich","submitted_at":"2017-06-16T14:19:48Z","abstract_excerpt":"We consider the Ising Field Theory (IFT), and the 3-state Potts Field Theory (PFT), which describe the scaling limits of the two- dimensional lattice q-state Potts model with q=2, and q=3, respectively. At zero magnetic field h=0, both field theories are integrable away from the critical point, have q degenerate vacua in the ferromagnetic phase, and q(q-1) particles of the same mass - the kinks interpolating between two different vacua. Application of a weak magnetic field induces confinement of kinks into bound states - the mesons (for q =2,3) consisting predominantly of two kinks, and baryon"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.05281","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":"1706.05281","created_at":"2026-05-18T00:34:41.507518+00:00"},{"alias_kind":"arxiv_version","alias_value":"1706.05281v2","created_at":"2026-05-18T00:34:41.507518+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.05281","created_at":"2026-05-18T00:34:41.507518+00:00"},{"alias_kind":"pith_short_12","alias_value":"K44ZXEVPLHRZ","created_at":"2026-05-18T12:31:24.725408+00:00"},{"alias_kind":"pith_short_16","alias_value":"K44ZXEVPLHRZJ5IK","created_at":"2026-05-18T12:31:24.725408+00:00"},{"alias_kind":"pith_short_8","alias_value":"K44ZXEVP","created_at":"2026-05-18T12:31:24.725408+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/K44ZXEVPLHRZJ5IKW45E4AYG3F","json":"https://pith.science/pith/K44ZXEVPLHRZJ5IKW45E4AYG3F.json","graph_json":"https://pith.science/api/pith-number/K44ZXEVPLHRZJ5IKW45E4AYG3F/graph.json","events_json":"https://pith.science/api/pith-number/K44ZXEVPLHRZJ5IKW45E4AYG3F/events.json","paper":"https://pith.science/paper/K44ZXEVP"},"agent_actions":{"view_html":"https://pith.science/pith/K44ZXEVPLHRZJ5IKW45E4AYG3F","download_json":"https://pith.science/pith/K44ZXEVPLHRZJ5IKW45E4AYG3F.json","view_paper":"https://pith.science/paper/K44ZXEVP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1706.05281&json=true","fetch_graph":"https://pith.science/api/pith-number/K44ZXEVPLHRZJ5IKW45E4AYG3F/graph.json","fetch_events":"https://pith.science/api/pith-number/K44ZXEVPLHRZJ5IKW45E4AYG3F/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/K44ZXEVPLHRZJ5IKW45E4AYG3F/action/timestamp_anchor","attest_storage":"https://pith.science/pith/K44ZXEVPLHRZJ5IKW45E4AYG3F/action/storage_attestation","attest_author":"https://pith.science/pith/K44ZXEVPLHRZJ5IKW45E4AYG3F/action/author_attestation","sign_citation":"https://pith.science/pith/K44ZXEVPLHRZJ5IKW45E4AYG3F/action/citation_signature","submit_replication":"https://pith.science/pith/K44ZXEVPLHRZJ5IKW45E4AYG3F/action/replication_record"}},"created_at":"2026-05-18T00:34:41.507518+00:00","updated_at":"2026-05-18T00:34:41.507518+00:00"}