{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1999:GUOII27QMGJGXNE3STBBA4VMII","short_pith_number":"pith:GUOII27Q","schema_version":"1.0","canonical_sha256":"351c846bf061926bb49b94c21072ac421af226967c6463cc81131f98145d8a57","source":{"kind":"arxiv","id":"hep-th/9907030","version":2},"attestation_state":"computed","paper":{"title":"Self-gravitating fundamental strings and black-holes","license":"","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Gabriele Veneziano, Thibault Damour","submitted_at":"1999-07-06T14:52:32Z","abstract_excerpt":"The configuration of typical highly excited (M >> M_s ~ (alpha')^{-1/2}) string states is considered as the string coupling g is adiabatically increased. The size distribution of very massive single string states is studied and the mass shift, due to long-range gravitational, dilatonic and axionic attraction, is estimated. By combining the two effects, in any number of spatial dimensions d, the most probable size of a string state becomes of order l_s = sqrt{2 alpha'} when g^2 M / M_s ~ 1. Depending on the dimension d, the transition between a random-walk-size string state (for low g) and a co"},"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/9907030","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1999-07-06T14:52:32Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"74fad8cdba54f3e012bfaa7ee1448987a06576de39f68f4ec0497e0bea118911","abstract_canon_sha256":"da49dd1b841a26aeaa6dfca42a1e8a4fbca09bec787bfe959bebaf25a6852fd0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:14:54.148255Z","signature_b64":"YcrurDEL0e6JBSIk9svWAM47ZbU2I1aQ5klUhpPCuoLV75VKZ0LsRRkFs1D+6knVVCPrGOFrCo1nvBcQMNtBDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"351c846bf061926bb49b94c21072ac421af226967c6463cc81131f98145d8a57","last_reissued_at":"2026-07-04T16:14:54.147866Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:14:54.147866Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Self-gravitating fundamental strings and black-holes","license":"","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Gabriele Veneziano, Thibault Damour","submitted_at":"1999-07-06T14:52:32Z","abstract_excerpt":"The configuration of typical highly excited (M >> M_s ~ (alpha')^{-1/2}) string states is considered as the string coupling g is adiabatically increased. The size distribution of very massive single string states is studied and the mass shift, due to long-range gravitational, dilatonic and axionic attraction, is estimated. By combining the two effects, in any number of spatial dimensions d, the most probable size of a string state becomes of order l_s = sqrt{2 alpha'} when g^2 M / M_s ~ 1. Depending on the dimension d, the transition between a random-walk-size string state (for low g) and a co"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9907030","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-th/9907030/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/9907030","created_at":"2026-07-04T16:14:54.147927+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9907030v2","created_at":"2026-07-04T16:14:54.147927+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9907030","created_at":"2026-07-04T16:14:54.147927+00:00"},{"alias_kind":"pith_short_12","alias_value":"GUOII27QMGJG","created_at":"2026-07-04T16:14:54.147927+00:00"},{"alias_kind":"pith_short_16","alias_value":"GUOII27QMGJGXNE3","created_at":"2026-07-04T16:14:54.147927+00:00"},{"alias_kind":"pith_short_8","alias_value":"GUOII27Q","created_at":"2026-07-04T16:14:54.147927+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2601.09707","citing_title":"Precision asymptotics of string amplitudes","ref_index":12,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/GUOII27QMGJGXNE3STBBA4VMII","json":"https://pith.science/pith/GUOII27QMGJGXNE3STBBA4VMII.json","graph_json":"https://pith.science/api/pith-number/GUOII27QMGJGXNE3STBBA4VMII/graph.json","events_json":"https://pith.science/api/pith-number/GUOII27QMGJGXNE3STBBA4VMII/events.json","paper":"https://pith.science/paper/GUOII27Q"},"agent_actions":{"view_html":"https://pith.science/pith/GUOII27QMGJGXNE3STBBA4VMII","download_json":"https://pith.science/pith/GUOII27QMGJGXNE3STBBA4VMII.json","view_paper":"https://pith.science/paper/GUOII27Q","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9907030&json=true","fetch_graph":"https://pith.science/api/pith-number/GUOII27QMGJGXNE3STBBA4VMII/graph.json","fetch_events":"https://pith.science/api/pith-number/GUOII27QMGJGXNE3STBBA4VMII/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GUOII27QMGJGXNE3STBBA4VMII/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GUOII27QMGJGXNE3STBBA4VMII/action/storage_attestation","attest_author":"https://pith.science/pith/GUOII27QMGJGXNE3STBBA4VMII/action/author_attestation","sign_citation":"https://pith.science/pith/GUOII27QMGJGXNE3STBBA4VMII/action/citation_signature","submit_replication":"https://pith.science/pith/GUOII27QMGJGXNE3STBBA4VMII/action/replication_record"}},"created_at":"2026-07-04T16:14:54.147927+00:00","updated_at":"2026-07-04T16:14:54.147927+00:00"}