{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:F3EHBAJ2BEWFGDYTWXXKZLAPW3","short_pith_number":"pith:F3EHBAJ2","schema_version":"1.0","canonical_sha256":"2ec870813a092c530f13b5eeacac0fb6ce2ef7e9ed5848014c6a841f66f162cb","source":{"kind":"arxiv","id":"1504.06420","version":1},"attestation_state":"computed","paper":{"title":"Interacting multiple zero mode formulation and its application to a system consisting of a dark soliton in a condensate","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.quant-gas","authors_text":"J. Takahashi, Y. Nakamura, Y. Yamanaka","submitted_at":"2015-04-24T08:29:16Z","abstract_excerpt":"To formulate the zero modes in a finite-size system with spontaneous breakdown of symmetries in quantum field theory is not trivial, for in the naive Bogoliubov theory, one encounters difficulties such as phase diffusion, the absence of a definite criterion for determining the ground state, and infrared divergences. A new interacting zero mode formulation that has been proposed for systems with a single zero mode to avoid these difficulties is extended to general systems with multiple zero modes. It naturally and definitely gives the interactions among the quantized zero modes, the consequence"},"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":"1504.06420","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2015-04-24T08:29:16Z","cross_cats_sorted":[],"title_canon_sha256":"28d63be64c2071c1c576ca4d761ef7215d84ccb7a4dae185232606e1335c67b7","abstract_canon_sha256":"adda54dce8a582e436301f7c4211e6ccbc5f863e81b81c1705f7832d3c00c740"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:34:49.976192Z","signature_b64":"jZhSjQaVRM2hWmJMy4OME7Hx8BlQFH5sVyiibDwfunm5tVvt/RmeDD+L6JAVXlkTQ9liIboMDVCg6bWWnsUpDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2ec870813a092c530f13b5eeacac0fb6ce2ef7e9ed5848014c6a841f66f162cb","last_reissued_at":"2026-05-18T01:34:49.975736Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:34:49.975736Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Interacting multiple zero mode formulation and its application to a system consisting of a dark soliton in a condensate","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.quant-gas","authors_text":"J. Takahashi, Y. Nakamura, Y. Yamanaka","submitted_at":"2015-04-24T08:29:16Z","abstract_excerpt":"To formulate the zero modes in a finite-size system with spontaneous breakdown of symmetries in quantum field theory is not trivial, for in the naive Bogoliubov theory, one encounters difficulties such as phase diffusion, the absence of a definite criterion for determining the ground state, and infrared divergences. A new interacting zero mode formulation that has been proposed for systems with a single zero mode to avoid these difficulties is extended to general systems with multiple zero modes. It naturally and definitely gives the interactions among the quantized zero modes, the consequence"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1504.06420","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":"1504.06420","created_at":"2026-05-18T01:34:49.975799+00:00"},{"alias_kind":"arxiv_version","alias_value":"1504.06420v1","created_at":"2026-05-18T01:34:49.975799+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1504.06420","created_at":"2026-05-18T01:34:49.975799+00:00"},{"alias_kind":"pith_short_12","alias_value":"F3EHBAJ2BEWF","created_at":"2026-05-18T12:29:19.899920+00:00"},{"alias_kind":"pith_short_16","alias_value":"F3EHBAJ2BEWFGDYT","created_at":"2026-05-18T12:29:19.899920+00:00"},{"alias_kind":"pith_short_8","alias_value":"F3EHBAJ2","created_at":"2026-05-18T12:29:19.899920+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/F3EHBAJ2BEWFGDYTWXXKZLAPW3","json":"https://pith.science/pith/F3EHBAJ2BEWFGDYTWXXKZLAPW3.json","graph_json":"https://pith.science/api/pith-number/F3EHBAJ2BEWFGDYTWXXKZLAPW3/graph.json","events_json":"https://pith.science/api/pith-number/F3EHBAJ2BEWFGDYTWXXKZLAPW3/events.json","paper":"https://pith.science/paper/F3EHBAJ2"},"agent_actions":{"view_html":"https://pith.science/pith/F3EHBAJ2BEWFGDYTWXXKZLAPW3","download_json":"https://pith.science/pith/F3EHBAJ2BEWFGDYTWXXKZLAPW3.json","view_paper":"https://pith.science/paper/F3EHBAJ2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1504.06420&json=true","fetch_graph":"https://pith.science/api/pith-number/F3EHBAJ2BEWFGDYTWXXKZLAPW3/graph.json","fetch_events":"https://pith.science/api/pith-number/F3EHBAJ2BEWFGDYTWXXKZLAPW3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/F3EHBAJ2BEWFGDYTWXXKZLAPW3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/F3EHBAJ2BEWFGDYTWXXKZLAPW3/action/storage_attestation","attest_author":"https://pith.science/pith/F3EHBAJ2BEWFGDYTWXXKZLAPW3/action/author_attestation","sign_citation":"https://pith.science/pith/F3EHBAJ2BEWFGDYTWXXKZLAPW3/action/citation_signature","submit_replication":"https://pith.science/pith/F3EHBAJ2BEWFGDYTWXXKZLAPW3/action/replication_record"}},"created_at":"2026-05-18T01:34:49.975799+00:00","updated_at":"2026-05-18T01:34:49.975799+00:00"}