{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:V2JHFTIZIGTOZ7NBUAXIQGNZDR","short_pith_number":"pith:V2JHFTIZ","schema_version":"1.0","canonical_sha256":"ae9272cd1941a6ecfda1a02e8819b91c591e387097d53ce521b2194973529efe","source":{"kind":"arxiv","id":"1101.5089","version":2},"attestation_state":"computed","paper":{"title":"Charge Fluctuations in Soliton Anti-Soliton Systems Without Conjugation Symmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"O.S. Ventura, R. L. P. G. Amaral, V. E. R. Lemes","submitted_at":"2011-01-26T15:43:10Z","abstract_excerpt":"We construct the charge operator and discuss the limits of their eigenvalues as the separation between background soliton and anti-solitons goes to infinity and analyze the fluctuations of the charge. This is performed in a (1+1)D model with charge conjugation breaking."},"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":"1101.5089","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-01-26T15:43:10Z","cross_cats_sorted":[],"title_canon_sha256":"a1c428fcc00fda0070a8db90e60ca0a1aff25f8429d8eed7fd3c9830edd3fe3f","abstract_canon_sha256":"8e4657fa55151bf49ef0e17687c7fa437f0c2356b8bb5c1d08c0e6e09abf48dc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:20:35.922045Z","signature_b64":"iW3tZuO9mFtTFVC2zOgHWREn+a7QFm6nVzSYjXAfr6LVFM3urhFdVHE5+8AF3ukCA6bgbFoHVIxUAHVrRLuSCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ae9272cd1941a6ecfda1a02e8819b91c591e387097d53ce521b2194973529efe","last_reissued_at":"2026-05-18T03:20:35.921123Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:20:35.921123Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Charge Fluctuations in Soliton Anti-Soliton Systems Without Conjugation Symmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"O.S. Ventura, R. L. P. G. Amaral, V. E. R. Lemes","submitted_at":"2011-01-26T15:43:10Z","abstract_excerpt":"We construct the charge operator and discuss the limits of their eigenvalues as the separation between background soliton and anti-solitons goes to infinity and analyze the fluctuations of the charge. This is performed in a (1+1)D model with charge conjugation breaking."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1101.5089","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":"1101.5089","created_at":"2026-05-18T03:20:35.921284+00:00"},{"alias_kind":"arxiv_version","alias_value":"1101.5089v2","created_at":"2026-05-18T03:20:35.921284+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1101.5089","created_at":"2026-05-18T03:20:35.921284+00:00"},{"alias_kind":"pith_short_12","alias_value":"V2JHFTIZIGTO","created_at":"2026-05-18T12:26:42.757692+00:00"},{"alias_kind":"pith_short_16","alias_value":"V2JHFTIZIGTOZ7NB","created_at":"2026-05-18T12:26:42.757692+00:00"},{"alias_kind":"pith_short_8","alias_value":"V2JHFTIZ","created_at":"2026-05-18T12:26:42.757692+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/V2JHFTIZIGTOZ7NBUAXIQGNZDR","json":"https://pith.science/pith/V2JHFTIZIGTOZ7NBUAXIQGNZDR.json","graph_json":"https://pith.science/api/pith-number/V2JHFTIZIGTOZ7NBUAXIQGNZDR/graph.json","events_json":"https://pith.science/api/pith-number/V2JHFTIZIGTOZ7NBUAXIQGNZDR/events.json","paper":"https://pith.science/paper/V2JHFTIZ"},"agent_actions":{"view_html":"https://pith.science/pith/V2JHFTIZIGTOZ7NBUAXIQGNZDR","download_json":"https://pith.science/pith/V2JHFTIZIGTOZ7NBUAXIQGNZDR.json","view_paper":"https://pith.science/paper/V2JHFTIZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1101.5089&json=true","fetch_graph":"https://pith.science/api/pith-number/V2JHFTIZIGTOZ7NBUAXIQGNZDR/graph.json","fetch_events":"https://pith.science/api/pith-number/V2JHFTIZIGTOZ7NBUAXIQGNZDR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/V2JHFTIZIGTOZ7NBUAXIQGNZDR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/V2JHFTIZIGTOZ7NBUAXIQGNZDR/action/storage_attestation","attest_author":"https://pith.science/pith/V2JHFTIZIGTOZ7NBUAXIQGNZDR/action/author_attestation","sign_citation":"https://pith.science/pith/V2JHFTIZIGTOZ7NBUAXIQGNZDR/action/citation_signature","submit_replication":"https://pith.science/pith/V2JHFTIZIGTOZ7NBUAXIQGNZDR/action/replication_record"}},"created_at":"2026-05-18T03:20:35.921284+00:00","updated_at":"2026-05-18T03:20:35.921284+00:00"}