{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:BOL7M6FMUYHPK6RDE2PVL73NOB","short_pith_number":"pith:BOL7M6FM","canonical_record":{"source":{"id":"1303.1396","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-03-06T17:31:05Z","cross_cats_sorted":["math-ph","math.MP"],"title_canon_sha256":"af4f876dd258d20a605b3647befe4aa0d1457279426e459217f4127cdac19afd","abstract_canon_sha256":"c245674f9d87defc0946a70608dfd4c8decd221407ad5fb2584957763a226c5e"},"schema_version":"1.0"},"canonical_sha256":"0b97f678aca60ef57a23269f55ff6d705c2a63121d0cbcd33206ed60ecd13cdd","source":{"kind":"arxiv","id":"1303.1396","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1303.1396","created_at":"2026-05-18T03:14:19Z"},{"alias_kind":"arxiv_version","alias_value":"1303.1396v1","created_at":"2026-05-18T03:14:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.1396","created_at":"2026-05-18T03:14:19Z"},{"alias_kind":"pith_short_12","alias_value":"BOL7M6FMUYHP","created_at":"2026-05-18T12:27:40Z"},{"alias_kind":"pith_short_16","alias_value":"BOL7M6FMUYHPK6RD","created_at":"2026-05-18T12:27:40Z"},{"alias_kind":"pith_short_8","alias_value":"BOL7M6FM","created_at":"2026-05-18T12:27:40Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:BOL7M6FMUYHPK6RDE2PVL73NOB","target":"record","payload":{"canonical_record":{"source":{"id":"1303.1396","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-03-06T17:31:05Z","cross_cats_sorted":["math-ph","math.MP"],"title_canon_sha256":"af4f876dd258d20a605b3647befe4aa0d1457279426e459217f4127cdac19afd","abstract_canon_sha256":"c245674f9d87defc0946a70608dfd4c8decd221407ad5fb2584957763a226c5e"},"schema_version":"1.0"},"canonical_sha256":"0b97f678aca60ef57a23269f55ff6d705c2a63121d0cbcd33206ed60ecd13cdd","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:14:19.733687Z","signature_b64":"SLlkZsLMo+ox79vHweIusdAi+QeLu3OBoFgQYl9rajm3bETbY5uniB236nJRp8FJ8oLjz3ytB1kYIvB63dLhDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0b97f678aca60ef57a23269f55ff6d705c2a63121d0cbcd33206ed60ecd13cdd","last_reissued_at":"2026-05-18T03:14:19.733177Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:14:19.733177Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1303.1396","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:14:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yYAUJtK0dL4qAOX5c0qbAYQMrPlBhyRdv1Zv3HiIGz9ud6BtfTOkTrlw9NGYFnb62Qdc/g9q8qzron6ei65fAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-14T08:56:22.346236Z"},"content_sha256":"f026ecb5a54bffba5728115745cc8cb7b3d384efa9ad4792ed0962c1ef018951","schema_version":"1.0","event_id":"sha256:f026ecb5a54bffba5728115745cc8cb7b3d384efa9ad4792ed0962c1ef018951"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:BOL7M6FMUYHPK6RDE2PVL73NOB","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Space-time S-matrix and Flux-tube S-matrix at Finite Coupling","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"Amit Sever, Benjamin Basso, Pedro Vieira","submitted_at":"2013-03-06T17:31:05Z","abstract_excerpt":"We propose a non-perturbative formulation of planar scattering amplitudes in N=4 SYM or, equivalently, polygonal Wilson loops. The construction is based on the OPE approach and introduces a new decomposition of the Wilson loop in terms of fundamental building blocks named Pentagon transitions. These transitions satisfy a simple relation to the worldsheet S-matrix on top of the so called Gubser-Klebanov-Polyakov vacuum which allows us to bootstrap them at any value of the coupling. In this letter we present a subsector of the full solution to scattering amplitudes which we call the gluonic part"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.1396","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":""},"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":"2026-05-18T03:14:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"A4PlytUQIEkhNWph8AbWqEeBGnrOlfJu9WJ9fYllksegKgZuOxFYynO4ZsUq20UwFNxDdONu33CHdmIHYjVqBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-14T08:56:22.346705Z"},"content_sha256":"6bc3bb6b7c66217a636b4204c02dc2c5121ad01182cf8d631a83e2b9aed822be","schema_version":"1.0","event_id":"sha256:6bc3bb6b7c66217a636b4204c02dc2c5121ad01182cf8d631a83e2b9aed822be"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/BOL7M6FMUYHPK6RDE2PVL73NOB/bundle.json","state_url":"https://pith.science/pith/BOL7M6FMUYHPK6RDE2PVL73NOB/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/BOL7M6FMUYHPK6RDE2PVL73NOB/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":"2026-08-14T08:56:22Z","links":{"resolver":"https://pith.science/pith/BOL7M6FMUYHPK6RDE2PVL73NOB","bundle":"https://pith.science/pith/BOL7M6FMUYHPK6RDE2PVL73NOB/bundle.json","state":"https://pith.science/pith/BOL7M6FMUYHPK6RDE2PVL73NOB/state.json","well_known_bundle":"https://pith.science/.well-known/pith/BOL7M6FMUYHPK6RDE2PVL73NOB/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:BOL7M6FMUYHPK6RDE2PVL73NOB","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":"c245674f9d87defc0946a70608dfd4c8decd221407ad5fb2584957763a226c5e","cross_cats_sorted":["math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-03-06T17:31:05Z","title_canon_sha256":"af4f876dd258d20a605b3647befe4aa0d1457279426e459217f4127cdac19afd"},"schema_version":"1.0","source":{"id":"1303.1396","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1303.1396","created_at":"2026-05-18T03:14:19Z"},{"alias_kind":"arxiv_version","alias_value":"1303.1396v1","created_at":"2026-05-18T03:14:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.1396","created_at":"2026-05-18T03:14:19Z"},{"alias_kind":"pith_short_12","alias_value":"BOL7M6FMUYHP","created_at":"2026-05-18T12:27:40Z"},{"alias_kind":"pith_short_16","alias_value":"BOL7M6FMUYHPK6RD","created_at":"2026-05-18T12:27:40Z"},{"alias_kind":"pith_short_8","alias_value":"BOL7M6FM","created_at":"2026-05-18T12:27:40Z"}],"graph_snapshots":[{"event_id":"sha256:6bc3bb6b7c66217a636b4204c02dc2c5121ad01182cf8d631a83e2b9aed822be","target":"graph","created_at":"2026-05-18T03:14:19Z","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"},"paper":{"abstract_excerpt":"We propose a non-perturbative formulation of planar scattering amplitudes in N=4 SYM or, equivalently, polygonal Wilson loops. The construction is based on the OPE approach and introduces a new decomposition of the Wilson loop in terms of fundamental building blocks named Pentagon transitions. These transitions satisfy a simple relation to the worldsheet S-matrix on top of the so called Gubser-Klebanov-Polyakov vacuum which allows us to bootstrap them at any value of the coupling. In this letter we present a subsector of the full solution to scattering amplitudes which we call the gluonic part","authors_text":"Amit Sever, Benjamin Basso, Pedro Vieira","cross_cats":["math-ph","math.MP"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-03-06T17:31:05Z","title":"Space-time S-matrix and Flux-tube S-matrix at Finite Coupling"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.1396","kind":"arxiv","version":1},"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:f026ecb5a54bffba5728115745cc8cb7b3d384efa9ad4792ed0962c1ef018951","target":"record","created_at":"2026-05-18T03:14:19Z","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":"c245674f9d87defc0946a70608dfd4c8decd221407ad5fb2584957763a226c5e","cross_cats_sorted":["math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-03-06T17:31:05Z","title_canon_sha256":"af4f876dd258d20a605b3647befe4aa0d1457279426e459217f4127cdac19afd"},"schema_version":"1.0","source":{"id":"1303.1396","kind":"arxiv","version":1}},"canonical_sha256":"0b97f678aca60ef57a23269f55ff6d705c2a63121d0cbcd33206ed60ecd13cdd","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0b97f678aca60ef57a23269f55ff6d705c2a63121d0cbcd33206ed60ecd13cdd","first_computed_at":"2026-05-18T03:14:19.733177Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:14:19.733177Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"SLlkZsLMo+ox79vHweIusdAi+QeLu3OBoFgQYl9rajm3bETbY5uniB236nJRp8FJ8oLjz3ytB1kYIvB63dLhDA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:14:19.733687Z","signed_message":"canonical_sha256_bytes"},"source_id":"1303.1396","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f026ecb5a54bffba5728115745cc8cb7b3d384efa9ad4792ed0962c1ef018951","sha256:6bc3bb6b7c66217a636b4204c02dc2c5121ad01182cf8d631a83e2b9aed822be"],"state_sha256":"8c74032297e5009db82abd7d63bdc9d2ca73ea40401453e55b16445d1555b2b0"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"NYVAqSZ74aNvC2D+tB/DTQQHM75kPvjkKv7sHEp4kk5aFz5ptbHxtJ9daGUih/LN8FJYX/QgNqgAr5b/NPa7Dg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-14T08:56:22.351359Z","bundle_sha256":"942a1c8527794162aeb447e4986f96190968a84eb9800932a131d05cf5618a90"}}