{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2023:YBRP4KMQKQRZOFKG7VN4AM5TZQ","short_pith_number":"pith:YBRP4KMQ","canonical_record":{"source":{"id":"2312.02127","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2023-12-04T18:53:39Z","cross_cats_sorted":["cond-mat.stat-mech","nlin.CD"],"title_canon_sha256":"76c1052dbe9d2c799bb9792a4b46e2af95f460edcb676cafeca63f0a6ce65231","abstract_canon_sha256":"7a2cb4f4785c1be0c790ab7fbddfe1f09d66c94816cc1322d802a2698edc4446"},"schema_version":"1.0"},"canonical_sha256":"c062fe29905423971546fd5bc033b3cc246945bbc67a5148aebf4ac8d3c7e589","source":{"kind":"arxiv","id":"2312.02127","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2312.02127","created_at":"2026-07-05T09:06:39Z"},{"alias_kind":"arxiv_version","alias_value":"2312.02127v3","created_at":"2026-07-05T09:06:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2312.02127","created_at":"2026-07-05T09:06:39Z"},{"alias_kind":"pith_short_12","alias_value":"YBRP4KMQKQRZ","created_at":"2026-07-05T09:06:39Z"},{"alias_kind":"pith_short_16","alias_value":"YBRP4KMQKQRZOFKG","created_at":"2026-07-05T09:06:39Z"},{"alias_kind":"pith_short_8","alias_value":"YBRP4KMQ","created_at":"2026-07-05T09:06:39Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2023:YBRP4KMQKQRZOFKG7VN4AM5TZQ","target":"record","payload":{"canonical_record":{"source":{"id":"2312.02127","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2023-12-04T18:53:39Z","cross_cats_sorted":["cond-mat.stat-mech","nlin.CD"],"title_canon_sha256":"76c1052dbe9d2c799bb9792a4b46e2af95f460edcb676cafeca63f0a6ce65231","abstract_canon_sha256":"7a2cb4f4785c1be0c790ab7fbddfe1f09d66c94816cc1322d802a2698edc4446"},"schema_version":"1.0"},"canonical_sha256":"c062fe29905423971546fd5bc033b3cc246945bbc67a5148aebf4ac8d3c7e589","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:06:39.980474Z","signature_b64":"/QDXD9j7F/4hCZPjmfDbg/MWoO4bIM4ssSj5XegAElmEAS/4lRBI8bIJe71xiyDtpSSTMhtI1AlQLrOPyTNrAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c062fe29905423971546fd5bc033b3cc246945bbc67a5148aebf4ac8d3c7e589","last_reissued_at":"2026-07-05T09:06:39.979967Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:06:39.979967Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2312.02127","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T09:06:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GScBfye+11x3zmPyzBZoNGsXQw7YjWvgqohLL6/HDRnFc5AAyaqKpn9iAJC3LnsAaT4Cni7d1jPm+KtPq/b7BQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T18:30:57.516196Z"},"content_sha256":"a728136bc11d7ff89d428af0914fefd698e1cb5a1803ed684529dc217f08f787","schema_version":"1.0","event_id":"sha256:a728136bc11d7ff89d428af0914fefd698e1cb5a1803ed684529dc217f08f787"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2023:YBRP4KMQKQRZOFKG7VN4AM5TZQ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Chaotic and Thermal Aspects in the Highly Excited String S-Matrix","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.stat-mech","nlin.CD"],"primary_cat":"hep-th","authors_text":"Anurag Sarkar, Diptarka Das, Santanu Mandal","submitted_at":"2023-12-04T18:53:39Z","abstract_excerpt":"We compute tree level scattering amplitudes involving more than one highly excited states and tachyons in bosonic string theory. We use these amplitudes to understand chaotic and thermal aspects of the excited string states lending support to the Susskind-Horowitz-Polchinski correspondence principle. The unaveraged amplitudes exhibit chaos in the resonance distribution as a function of kinematic parameters, which can be described by random matrix theory. Upon coarse-graining these amplitudes are shown to exponentiate, and capture various thermal features, including features of a stringy versio"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2312.02127","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/2312.02127/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T09:06:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yavoAk2BQJf5djzNK6OenxmTQdBKyVH4AS0R1eGYz6slRxi39x3en2fo8JMqCfpp7bc9VZ7uhVxM2ZoH2F5VDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T18:30:57.516591Z"},"content_sha256":"e5916de76c116d035f14e7a9f9ac7cc02fa3ca840cc12c9625d9e698be473a44","schema_version":"1.0","event_id":"sha256:e5916de76c116d035f14e7a9f9ac7cc02fa3ca840cc12c9625d9e698be473a44"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/YBRP4KMQKQRZOFKG7VN4AM5TZQ/bundle.json","state_url":"https://pith.science/pith/YBRP4KMQKQRZOFKG7VN4AM5TZQ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/YBRP4KMQKQRZOFKG7VN4AM5TZQ/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-08-03T18:30:57Z","links":{"resolver":"https://pith.science/pith/YBRP4KMQKQRZOFKG7VN4AM5TZQ","bundle":"https://pith.science/pith/YBRP4KMQKQRZOFKG7VN4AM5TZQ/bundle.json","state":"https://pith.science/pith/YBRP4KMQKQRZOFKG7VN4AM5TZQ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/YBRP4KMQKQRZOFKG7VN4AM5TZQ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:YBRP4KMQKQRZOFKG7VN4AM5TZQ","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"7a2cb4f4785c1be0c790ab7fbddfe1f09d66c94816cc1322d802a2698edc4446","cross_cats_sorted":["cond-mat.stat-mech","nlin.CD"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2023-12-04T18:53:39Z","title_canon_sha256":"76c1052dbe9d2c799bb9792a4b46e2af95f460edcb676cafeca63f0a6ce65231"},"schema_version":"1.0","source":{"id":"2312.02127","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2312.02127","created_at":"2026-07-05T09:06:39Z"},{"alias_kind":"arxiv_version","alias_value":"2312.02127v3","created_at":"2026-07-05T09:06:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2312.02127","created_at":"2026-07-05T09:06:39Z"},{"alias_kind":"pith_short_12","alias_value":"YBRP4KMQKQRZ","created_at":"2026-07-05T09:06:39Z"},{"alias_kind":"pith_short_16","alias_value":"YBRP4KMQKQRZOFKG","created_at":"2026-07-05T09:06:39Z"},{"alias_kind":"pith_short_8","alias_value":"YBRP4KMQ","created_at":"2026-07-05T09:06:39Z"}],"graph_snapshots":[{"event_id":"sha256:e5916de76c116d035f14e7a9f9ac7cc02fa3ca840cc12c9625d9e698be473a44","target":"graph","created_at":"2026-07-05T09:06:39Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2312.02127/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We compute tree level scattering amplitudes involving more than one highly excited states and tachyons in bosonic string theory. We use these amplitudes to understand chaotic and thermal aspects of the excited string states lending support to the Susskind-Horowitz-Polchinski correspondence principle. The unaveraged amplitudes exhibit chaos in the resonance distribution as a function of kinematic parameters, which can be described by random matrix theory. Upon coarse-graining these amplitudes are shown to exponentiate, and capture various thermal features, including features of a stringy versio","authors_text":"Anurag Sarkar, Diptarka Das, Santanu Mandal","cross_cats":["cond-mat.stat-mech","nlin.CD"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2023-12-04T18:53:39Z","title":"Chaotic and Thermal Aspects in the Highly Excited String S-Matrix"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2312.02127","kind":"arxiv","version":3},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:a728136bc11d7ff89d428af0914fefd698e1cb5a1803ed684529dc217f08f787","target":"record","created_at":"2026-07-05T09:06:39Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"7a2cb4f4785c1be0c790ab7fbddfe1f09d66c94816cc1322d802a2698edc4446","cross_cats_sorted":["cond-mat.stat-mech","nlin.CD"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2023-12-04T18:53:39Z","title_canon_sha256":"76c1052dbe9d2c799bb9792a4b46e2af95f460edcb676cafeca63f0a6ce65231"},"schema_version":"1.0","source":{"id":"2312.02127","kind":"arxiv","version":3}},"canonical_sha256":"c062fe29905423971546fd5bc033b3cc246945bbc67a5148aebf4ac8d3c7e589","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c062fe29905423971546fd5bc033b3cc246945bbc67a5148aebf4ac8d3c7e589","first_computed_at":"2026-07-05T09:06:39.979967Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T09:06:39.979967Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"/QDXD9j7F/4hCZPjmfDbg/MWoO4bIM4ssSj5XegAElmEAS/4lRBI8bIJe71xiyDtpSSTMhtI1AlQLrOPyTNrAg==","signature_status":"signed_v1","signed_at":"2026-07-05T09:06:39.980474Z","signed_message":"canonical_sha256_bytes"},"source_id":"2312.02127","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a728136bc11d7ff89d428af0914fefd698e1cb5a1803ed684529dc217f08f787","sha256:e5916de76c116d035f14e7a9f9ac7cc02fa3ca840cc12c9625d9e698be473a44"],"state_sha256":"63c5e0eb960d1740b3a53a10e970ca5d04c7ea6ea38395743afc200484e85893"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"F9c0QArc5YXFvJ25WtmGSGqazAMEoDNHjDs91bo5lIp7rxX0SmryEEVj6Hy+3/Fieyg+VcMNPN2r/KkTSAlhBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-03T18:30:57.519296Z","bundle_sha256":"9219c8c112e42c373d20700fd199483fee23af815e8c003b76caff47bf8dd65a"}}