{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1994:ZS7CXTGZXMJK4FKZKFLYG64XA2","short_pith_number":"pith:ZS7CXTGZ","schema_version":"1.0","canonical_sha256":"ccbe2bccd9bb12ae15595157837b97068850e10f6a6b96b3b2f239d75a67fad5","source":{"kind":"arxiv","id":"hep-th/9412184","version":1},"attestation_state":"computed","paper":{"title":"String Solitons","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"J. X. Lu, M. J. Duff, Ramzi R. Khuri","submitted_at":"1994-12-22T01:42:57Z","abstract_excerpt":"We review the status of solitons in superstring theory, with a view to understanding the strong coupling regime. These {\\it solitonic} solutions are non-singular field configurations which solve the empty-space low-energy field equations (generalized, whenever possible, to all orders in $\\alpha'$), carry a non-vanishing topological \"magnetic\" charge and are stabilized by a topological conservation law. They are compared and contrasted with the {\\it elementary} solutions which are singular solutions of the field equations with a $\\sigma$-model source term and carry a non-vanishing Noether \"elec"},"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/9412184","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1994-12-22T01:42:57Z","cross_cats_sorted":[],"title_canon_sha256":"1436f7970f9e3f87ae4c293eebe9152ecd6ef20e43df997c7684e461408d2292","abstract_canon_sha256":"bfd199083386281e8c5beff431715797a8233f0ed6b1059904b4a86234c11a09"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:23:57.242725Z","signature_b64":"aSn9+Is7VDZug5tybDh1jbgNiT29gzbA6pRwFPEi1rwEVA2xJ8LfrKR2oJyHZ4gyYQbPJJ1FFFHJjn4LBf9uAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ccbe2bccd9bb12ae15595157837b97068850e10f6a6b96b3b2f239d75a67fad5","last_reissued_at":"2026-07-04T15:23:57.242289Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:23:57.242289Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"String Solitons","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"J. X. Lu, M. J. Duff, Ramzi R. Khuri","submitted_at":"1994-12-22T01:42:57Z","abstract_excerpt":"We review the status of solitons in superstring theory, with a view to understanding the strong coupling regime. These {\\it solitonic} solutions are non-singular field configurations which solve the empty-space low-energy field equations (generalized, whenever possible, to all orders in $\\alpha'$), carry a non-vanishing topological \"magnetic\" charge and are stabilized by a topological conservation law. They are compared and contrasted with the {\\it elementary} solutions which are singular solutions of the field equations with a $\\sigma$-model source term and carry a non-vanishing Noether \"elec"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9412184","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/9412184/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/9412184","created_at":"2026-07-04T15:23:57.242360+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9412184v1","created_at":"2026-07-04T15:23:57.242360+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9412184","created_at":"2026-07-04T15:23:57.242360+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZS7CXTGZXMJK","created_at":"2026-07-04T15:23:57.242360+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZS7CXTGZXMJK4FKZ","created_at":"2026-07-04T15:23:57.242360+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZS7CXTGZ","created_at":"2026-07-04T15:23:57.242360+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":5,"internal_anchor_count":4,"sample":[{"citing_arxiv_id":"2605.31181","citing_title":"Brane flows","ref_index":29,"is_internal_anchor":true},{"citing_arxiv_id":"2606.18344","citing_title":"Black p-brane Thermodynamics without Constructing Solutions","ref_index":2,"is_internal_anchor":true},{"citing_arxiv_id":"2511.16586","citing_title":"Toward a worldsheet theory of entanglement entropy","ref_index":32,"is_internal_anchor":true},{"citing_arxiv_id":"2603.11163","citing_title":"Alice in Warpland: KK modes, Warped Compactifications and the Swampland","ref_index":130,"is_internal_anchor":true},{"citing_arxiv_id":"2604.18488","citing_title":"Branes","ref_index":30,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ZS7CXTGZXMJK4FKZKFLYG64XA2","json":"https://pith.science/pith/ZS7CXTGZXMJK4FKZKFLYG64XA2.json","graph_json":"https://pith.science/api/pith-number/ZS7CXTGZXMJK4FKZKFLYG64XA2/graph.json","events_json":"https://pith.science/api/pith-number/ZS7CXTGZXMJK4FKZKFLYG64XA2/events.json","paper":"https://pith.science/paper/ZS7CXTGZ"},"agent_actions":{"view_html":"https://pith.science/pith/ZS7CXTGZXMJK4FKZKFLYG64XA2","download_json":"https://pith.science/pith/ZS7CXTGZXMJK4FKZKFLYG64XA2.json","view_paper":"https://pith.science/paper/ZS7CXTGZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9412184&json=true","fetch_graph":"https://pith.science/api/pith-number/ZS7CXTGZXMJK4FKZKFLYG64XA2/graph.json","fetch_events":"https://pith.science/api/pith-number/ZS7CXTGZXMJK4FKZKFLYG64XA2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZS7CXTGZXMJK4FKZKFLYG64XA2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZS7CXTGZXMJK4FKZKFLYG64XA2/action/storage_attestation","attest_author":"https://pith.science/pith/ZS7CXTGZXMJK4FKZKFLYG64XA2/action/author_attestation","sign_citation":"https://pith.science/pith/ZS7CXTGZXMJK4FKZKFLYG64XA2/action/citation_signature","submit_replication":"https://pith.science/pith/ZS7CXTGZXMJK4FKZKFLYG64XA2/action/replication_record"}},"created_at":"2026-07-04T15:23:57.242360+00:00","updated_at":"2026-07-04T15:23:57.242360+00:00"}