{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1993:2J6CRFRVJUG36C44DJIOP4XVE7","short_pith_number":"pith:2J6CRFRV","schema_version":"1.0","canonical_sha256":"d27c2896354d0dbf0b9c1a50e7f2f527cdcee298887a537212524638bf9aee51","source":{"kind":"arxiv","id":"hep-th/9309037","version":2},"attestation_state":"computed","paper":{"title":"Planckian Energy Scattering and Surface Terms in the Gravitational Action","license":"","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"G.A. Vilkovisky, G. Veneziano, M. Fabbrichesi, R. Pettorini","submitted_at":"1993-09-07T13:29:57Z","abstract_excerpt":"This is a revised version of our previous paper by the same name and preprint number. It contains various changes, two figures and new results in sect.5. We propose a new approach to four-dimensional Planckian-energy scattering in which the phase of the ${\\cal S}$-matrix is written---to leading order in $\\hbar$ and to all orders in $R/b =Gs/J$---in terms of the surface term of the gravity action and of a boundary term for the colliding quanta. The proposal is checked at the leading order in $R/b$ and also against some known examples of scattering in strong gravitational fields."},"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/9309037","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1993-09-07T13:29:57Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"a7f816f173cc0a6012e1f07c8fe5da46570adc74dbd8e3306068926d46da131d","abstract_canon_sha256":"48f4178fc0180ffc5ade5f7748598d48304e4957defa82a0e0dc249505c0eae4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:56:18.354393Z","signature_b64":"xkSPhOh6KpM2pFmknWrPXaQjtMJD7eD4WUPVKfEsnEuOE2RywLDAsY+1tUUKBQYnrV0po6uyFCQCHXdyopU0AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d27c2896354d0dbf0b9c1a50e7f2f527cdcee298887a537212524638bf9aee51","last_reissued_at":"2026-07-04T15:56:18.353986Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:56:18.353986Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Planckian Energy Scattering and Surface Terms in the Gravitational Action","license":"","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"G.A. Vilkovisky, G. Veneziano, M. Fabbrichesi, R. Pettorini","submitted_at":"1993-09-07T13:29:57Z","abstract_excerpt":"This is a revised version of our previous paper by the same name and preprint number. It contains various changes, two figures and new results in sect.5. We propose a new approach to four-dimensional Planckian-energy scattering in which the phase of the ${\\cal S}$-matrix is written---to leading order in $\\hbar$ and to all orders in $R/b =Gs/J$---in terms of the surface term of the gravity action and of a boundary term for the colliding quanta. The proposal is checked at the leading order in $R/b$ and also against some known examples of scattering in strong gravitational fields."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9309037","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/9309037/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/9309037","created_at":"2026-07-04T15:56:18.354047+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9309037v2","created_at":"2026-07-04T15:56:18.354047+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9309037","created_at":"2026-07-04T15:56:18.354047+00:00"},{"alias_kind":"pith_short_12","alias_value":"2J6CRFRVJUG3","created_at":"2026-07-04T15:56:18.354047+00:00"},{"alias_kind":"pith_short_16","alias_value":"2J6CRFRVJUG36C44","created_at":"2026-07-04T15:56:18.354047+00:00"},{"alias_kind":"pith_short_8","alias_value":"2J6CRFRV","created_at":"2026-07-04T15:56:18.354047+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2501.07136","citing_title":"On symmetries of gravitational on-shell boundary action at null infinity","ref_index":41,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/2J6CRFRVJUG36C44DJIOP4XVE7","json":"https://pith.science/pith/2J6CRFRVJUG36C44DJIOP4XVE7.json","graph_json":"https://pith.science/api/pith-number/2J6CRFRVJUG36C44DJIOP4XVE7/graph.json","events_json":"https://pith.science/api/pith-number/2J6CRFRVJUG36C44DJIOP4XVE7/events.json","paper":"https://pith.science/paper/2J6CRFRV"},"agent_actions":{"view_html":"https://pith.science/pith/2J6CRFRVJUG36C44DJIOP4XVE7","download_json":"https://pith.science/pith/2J6CRFRVJUG36C44DJIOP4XVE7.json","view_paper":"https://pith.science/paper/2J6CRFRV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9309037&json=true","fetch_graph":"https://pith.science/api/pith-number/2J6CRFRVJUG36C44DJIOP4XVE7/graph.json","fetch_events":"https://pith.science/api/pith-number/2J6CRFRVJUG36C44DJIOP4XVE7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2J6CRFRVJUG36C44DJIOP4XVE7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2J6CRFRVJUG36C44DJIOP4XVE7/action/storage_attestation","attest_author":"https://pith.science/pith/2J6CRFRVJUG36C44DJIOP4XVE7/action/author_attestation","sign_citation":"https://pith.science/pith/2J6CRFRVJUG36C44DJIOP4XVE7/action/citation_signature","submit_replication":"https://pith.science/pith/2J6CRFRVJUG36C44DJIOP4XVE7/action/replication_record"}},"created_at":"2026-07-04T15:56:18.354047+00:00","updated_at":"2026-07-04T15:56:18.354047+00:00"}