{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:L2HJVVAGM4XN4YIQN3FA2HUKCW","short_pith_number":"pith:L2HJVVAG","schema_version":"1.0","canonical_sha256":"5e8e9ad406672ede61106eca0d1e8a1596b5e47af2563276e00ce1b34b097089","source":{"kind":"arxiv","id":"1901.01681","version":3},"attestation_state":"computed","paper":{"title":"Analytic Construction of Multi-brane Solutions in Cubic String Field Theory for Any Brane Number","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Hiroyuki Hata","submitted_at":"2019-01-07T06:58:17Z","abstract_excerpt":"We present an analytic construction of multi-brane solutions with any integer brane number in cubic open string field theory (CSFT) on the basis of the $KBc$ algebra. Our solution is given in the pure-gauge form $\\Psi=UQ_\\textrm{B}U^{-1}$ by a unitary string field $U$, which we choose to satisfy two requirements. First, the energy density of the solution should reproduce that of the $(N+1)$-branes. Second, the EOM of the solution should hold against the solution itself. In spite of the pure-gauge form of $\\Psi$, these two conditions are non-trivial ones due to the singularity at $K=0$. For the"},"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":"1901.01681","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2019-01-07T06:58:17Z","cross_cats_sorted":[],"title_canon_sha256":"9a37a87876258fd69b5d35768a4d1465f4859e5c1a5db06a993703c911ca6dd7","abstract_canon_sha256":"061def599cb57a88c686276545c355752d698df50211b06caa643b32388c8111"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:24:05.362223Z","signature_b64":"JPbLEjFslMg7eY5MeMvMLfk5zJdXYR+scie2s5H25xBRckNoVueVdMCiOFHDbTo7pOuFKoaOBp6VwXXE55ozBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5e8e9ad406672ede61106eca0d1e8a1596b5e47af2563276e00ce1b34b097089","last_reissued_at":"2026-07-05T00:24:05.361695Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:24:05.361695Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Analytic Construction of Multi-brane Solutions in Cubic String Field Theory for Any Brane Number","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Hiroyuki Hata","submitted_at":"2019-01-07T06:58:17Z","abstract_excerpt":"We present an analytic construction of multi-brane solutions with any integer brane number in cubic open string field theory (CSFT) on the basis of the $KBc$ algebra. Our solution is given in the pure-gauge form $\\Psi=UQ_\\textrm{B}U^{-1}$ by a unitary string field $U$, which we choose to satisfy two requirements. First, the energy density of the solution should reproduce that of the $(N+1)$-branes. Second, the EOM of the solution should hold against the solution itself. In spite of the pure-gauge form of $\\Psi$, these two conditions are non-trivial ones due to the singularity at $K=0$. For the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1901.01681","kind":"arxiv","version":3},"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/1901.01681/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":"1901.01681","created_at":"2026-07-05T00:24:05.361751+00:00"},{"alias_kind":"arxiv_version","alias_value":"1901.01681v3","created_at":"2026-07-05T00:24:05.361751+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1901.01681","created_at":"2026-07-05T00:24:05.361751+00:00"},{"alias_kind":"pith_short_12","alias_value":"L2HJVVAGM4XN","created_at":"2026-07-05T00:24:05.361751+00:00"},{"alias_kind":"pith_short_16","alias_value":"L2HJVVAGM4XN4YIQ","created_at":"2026-07-05T00:24:05.361751+00:00"},{"alias_kind":"pith_short_8","alias_value":"L2HJVVAG","created_at":"2026-07-05T00:24:05.361751+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1908.07177","citing_title":"Bernoulli Numbers and Multi-brane Solutions in Cubic String Field Theory","ref_index":1,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/L2HJVVAGM4XN4YIQN3FA2HUKCW","json":"https://pith.science/pith/L2HJVVAGM4XN4YIQN3FA2HUKCW.json","graph_json":"https://pith.science/api/pith-number/L2HJVVAGM4XN4YIQN3FA2HUKCW/graph.json","events_json":"https://pith.science/api/pith-number/L2HJVVAGM4XN4YIQN3FA2HUKCW/events.json","paper":"https://pith.science/paper/L2HJVVAG"},"agent_actions":{"view_html":"https://pith.science/pith/L2HJVVAGM4XN4YIQN3FA2HUKCW","download_json":"https://pith.science/pith/L2HJVVAGM4XN4YIQN3FA2HUKCW.json","view_paper":"https://pith.science/paper/L2HJVVAG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1901.01681&json=true","fetch_graph":"https://pith.science/api/pith-number/L2HJVVAGM4XN4YIQN3FA2HUKCW/graph.json","fetch_events":"https://pith.science/api/pith-number/L2HJVVAGM4XN4YIQN3FA2HUKCW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/L2HJVVAGM4XN4YIQN3FA2HUKCW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/L2HJVVAGM4XN4YIQN3FA2HUKCW/action/storage_attestation","attest_author":"https://pith.science/pith/L2HJVVAGM4XN4YIQN3FA2HUKCW/action/author_attestation","sign_citation":"https://pith.science/pith/L2HJVVAGM4XN4YIQN3FA2HUKCW/action/citation_signature","submit_replication":"https://pith.science/pith/L2HJVVAGM4XN4YIQN3FA2HUKCW/action/replication_record"}},"created_at":"2026-07-05T00:24:05.361751+00:00","updated_at":"2026-07-05T00:24:05.361751+00:00"}