{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:FEXUIVSA62LZG6GAELRH7JJKCT","short_pith_number":"pith:FEXUIVSA","schema_version":"1.0","canonical_sha256":"292f445640f6979378c022e27fa52a14cf6d2d8b4ede3301d2b11d959345bc60","source":{"kind":"arxiv","id":"2207.00211","version":1},"attestation_state":"computed","paper":{"title":"Quantum nucleation of topological solitons","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mes-hall","hep-ph"],"primary_cat":"hep-th","authors_text":"Minoru Eto, Muneto Nitta","submitted_at":"2022-07-01T05:33:29Z","abstract_excerpt":"The chiral soliton lattice is an array of topological solitons realized as ground states of QCD at finite density under strong magnetic fields or rapid rotation, and chiral magnets with an easy-plane anisotropy. In such cases, topological solitons have negative energy due to topological terms originating from the chiral magnetic or vortical effect and the Dzyaloshinskii-Moriya interaction, respectively. We study quantum nucleation of topological solitons in the vacuum through quantum tunneling in $2+1$ and $3+1$ dimensions, by using a complex $\\phi^4$ (or the axion) model with a topological te"},"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":"2207.00211","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-07-01T05:33:29Z","cross_cats_sorted":["cond-mat.mes-hall","hep-ph"],"title_canon_sha256":"51ebf0b62de2b056bf6278e22b2cfb2dedd76b0d912cc35e8e0fd947e6c69481","abstract_canon_sha256":"2b7a59579924c647ae4b2106840d35a714b55658ef9f653abd97a3ba518007f0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:01:26.284564Z","signature_b64":"0ZEZzLDP4hIXLwVWuoFmBfsTzw8UBgSVbaisK4YBdOyMxM5dwUNinRGWa2STAJ2BP/8gGGbMbluwnBvI3+XKAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"292f445640f6979378c022e27fa52a14cf6d2d8b4ede3301d2b11d959345bc60","last_reissued_at":"2026-07-05T05:01:26.284001Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:01:26.284001Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quantum nucleation of topological solitons","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mes-hall","hep-ph"],"primary_cat":"hep-th","authors_text":"Minoru Eto, Muneto Nitta","submitted_at":"2022-07-01T05:33:29Z","abstract_excerpt":"The chiral soliton lattice is an array of topological solitons realized as ground states of QCD at finite density under strong magnetic fields or rapid rotation, and chiral magnets with an easy-plane anisotropy. In such cases, topological solitons have negative energy due to topological terms originating from the chiral magnetic or vortical effect and the Dzyaloshinskii-Moriya interaction, respectively. We study quantum nucleation of topological solitons in the vacuum through quantum tunneling in $2+1$ and $3+1$ dimensions, by using a complex $\\phi^4$ (or the axion) model with a topological te"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2207.00211","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/2207.00211/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":"2207.00211","created_at":"2026-07-05T05:01:26.284072+00:00"},{"alias_kind":"arxiv_version","alias_value":"2207.00211v1","created_at":"2026-07-05T05:01:26.284072+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2207.00211","created_at":"2026-07-05T05:01:26.284072+00:00"},{"alias_kind":"pith_short_12","alias_value":"FEXUIVSA62LZ","created_at":"2026-07-05T05:01:26.284072+00:00"},{"alias_kind":"pith_short_16","alias_value":"FEXUIVSA62LZG6GA","created_at":"2026-07-05T05:01:26.284072+00:00"},{"alias_kind":"pith_short_8","alias_value":"FEXUIVSA","created_at":"2026-07-05T05:01:26.284072+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2510.09866","citing_title":"Baryons, Skyrmions and $\\theta$-periodicity anomaly in chiral and vector-like gauge theories","ref_index":50,"is_internal_anchor":false},{"citing_arxiv_id":"2512.22023","citing_title":"Fermionic domain-wall Skyrmions of QCD in a magnetic field","ref_index":23,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/FEXUIVSA62LZG6GAELRH7JJKCT","json":"https://pith.science/pith/FEXUIVSA62LZG6GAELRH7JJKCT.json","graph_json":"https://pith.science/api/pith-number/FEXUIVSA62LZG6GAELRH7JJKCT/graph.json","events_json":"https://pith.science/api/pith-number/FEXUIVSA62LZG6GAELRH7JJKCT/events.json","paper":"https://pith.science/paper/FEXUIVSA"},"agent_actions":{"view_html":"https://pith.science/pith/FEXUIVSA62LZG6GAELRH7JJKCT","download_json":"https://pith.science/pith/FEXUIVSA62LZG6GAELRH7JJKCT.json","view_paper":"https://pith.science/paper/FEXUIVSA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2207.00211&json=true","fetch_graph":"https://pith.science/api/pith-number/FEXUIVSA62LZG6GAELRH7JJKCT/graph.json","fetch_events":"https://pith.science/api/pith-number/FEXUIVSA62LZG6GAELRH7JJKCT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FEXUIVSA62LZG6GAELRH7JJKCT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FEXUIVSA62LZG6GAELRH7JJKCT/action/storage_attestation","attest_author":"https://pith.science/pith/FEXUIVSA62LZG6GAELRH7JJKCT/action/author_attestation","sign_citation":"https://pith.science/pith/FEXUIVSA62LZG6GAELRH7JJKCT/action/citation_signature","submit_replication":"https://pith.science/pith/FEXUIVSA62LZG6GAELRH7JJKCT/action/replication_record"}},"created_at":"2026-07-05T05:01:26.284072+00:00","updated_at":"2026-07-05T05:01:26.284072+00:00"}