{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:WNRU545KMKN6JD7XBTWJYVFUUJ","short_pith_number":"pith:WNRU545K","schema_version":"1.0","canonical_sha256":"b3634ef3aa629be48ff70cec9c54b4a27e9b45a98755604198d2d2068b10cc93","source":{"kind":"arxiv","id":"hep-th/0201159","version":1},"attestation_state":"computed","paper":{"title":"Patterns in Open String Field Theory Solutions","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Ashoke Sen, Barton Zwiebach, Davide Gaiotto, Leonardo Rastelli","submitted_at":"2002-01-21T16:47:40Z","abstract_excerpt":"In open string field theory the kinetic operator mixes matter and ghost sectors, and thus the ghost structure of classical solutions is not universal. Nevertheless, we have found from numerical analysis that certain ratios of expectation values for states involving pure ghost excitations appear to be universal. We give an analytic expression for these ratios and find good evidence that they are common to all known solutions of open string field theory, including the tachyon vacuum solution, lump solutions and string fields representing marginal deformations. We also draw attention to a close c"},"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":"hep-th/0201159","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2002-01-21T16:47:40Z","cross_cats_sorted":[],"title_canon_sha256":"a3203b3b3ac5723d7b4fdb373b3d97f22f4408a870c28083ddc809363b226c62","abstract_canon_sha256":"0dc2adeab1067cc329ca7bb89554397148ba943902fdf001168e9cf2bb375415"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:34:32.207912Z","signature_b64":"BOH7sj05dkkE69wl6NLsf3cg2Wqld5jx5HL2W9AsBLhsa1Fxrqgpmbn50rGVL+eqRb6RWtH7bAsMAHYgj2AFCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b3634ef3aa629be48ff70cec9c54b4a27e9b45a98755604198d2d2068b10cc93","last_reissued_at":"2026-07-04T16:34:32.207555Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:34:32.207555Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Patterns in Open String Field Theory Solutions","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Ashoke Sen, Barton Zwiebach, Davide Gaiotto, Leonardo Rastelli","submitted_at":"2002-01-21T16:47:40Z","abstract_excerpt":"In open string field theory the kinetic operator mixes matter and ghost sectors, and thus the ghost structure of classical solutions is not universal. Nevertheless, we have found from numerical analysis that certain ratios of expectation values for states involving pure ghost excitations appear to be universal. We give an analytic expression for these ratios and find good evidence that they are common to all known solutions of open string field theory, including the tachyon vacuum solution, lump solutions and string fields representing marginal deformations. We also draw attention to a close c"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0201159","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/hep-th/0201159/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":"hep-th/0201159","created_at":"2026-07-04T16:34:32.207619+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0201159v1","created_at":"2026-07-04T16:34:32.207619+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0201159","created_at":"2026-07-04T16:34:32.207619+00:00"},{"alias_kind":"pith_short_12","alias_value":"WNRU545KMKN6","created_at":"2026-07-04T16:34:32.207619+00:00"},{"alias_kind":"pith_short_16","alias_value":"WNRU545KMKN6JD7X","created_at":"2026-07-04T16:34:32.207619+00:00"},{"alias_kind":"pith_short_8","alias_value":"WNRU545K","created_at":"2026-07-04T16:34:32.207619+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/WNRU545KMKN6JD7XBTWJYVFUUJ","json":"https://pith.science/pith/WNRU545KMKN6JD7XBTWJYVFUUJ.json","graph_json":"https://pith.science/api/pith-number/WNRU545KMKN6JD7XBTWJYVFUUJ/graph.json","events_json":"https://pith.science/api/pith-number/WNRU545KMKN6JD7XBTWJYVFUUJ/events.json","paper":"https://pith.science/paper/WNRU545K"},"agent_actions":{"view_html":"https://pith.science/pith/WNRU545KMKN6JD7XBTWJYVFUUJ","download_json":"https://pith.science/pith/WNRU545KMKN6JD7XBTWJYVFUUJ.json","view_paper":"https://pith.science/paper/WNRU545K","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0201159&json=true","fetch_graph":"https://pith.science/api/pith-number/WNRU545KMKN6JD7XBTWJYVFUUJ/graph.json","fetch_events":"https://pith.science/api/pith-number/WNRU545KMKN6JD7XBTWJYVFUUJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WNRU545KMKN6JD7XBTWJYVFUUJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WNRU545KMKN6JD7XBTWJYVFUUJ/action/storage_attestation","attest_author":"https://pith.science/pith/WNRU545KMKN6JD7XBTWJYVFUUJ/action/author_attestation","sign_citation":"https://pith.science/pith/WNRU545KMKN6JD7XBTWJYVFUUJ/action/citation_signature","submit_replication":"https://pith.science/pith/WNRU545KMKN6JD7XBTWJYVFUUJ/action/replication_record"}},"created_at":"2026-07-04T16:34:32.207619+00:00","updated_at":"2026-07-04T16:34:32.207619+00:00"}