{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:FG6ZKAYGUKNHX753RGIWIRDNCL","short_pith_number":"pith:FG6ZKAYG","canonical_record":{"source":{"id":"1202.5292","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-02-23T20:43:14Z","cross_cats_sorted":[],"title_canon_sha256":"37ddf6239cf8e0d3ecb892b49e3bb57b5581249eae80dc79fa984a8b593215cf","abstract_canon_sha256":"c689b87fb4dab56e3dbcf2729ac57da0c869e1b9a2e15ad006ea443fae2ad507"},"schema_version":"1.0"},"canonical_sha256":"29bd950306a29a7bffbb899164446d12d9a90384557c61642c59229b5a439e88","source":{"kind":"arxiv","id":"1202.5292","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1202.5292","created_at":"2026-05-18T01:58:20Z"},{"alias_kind":"arxiv_version","alias_value":"1202.5292v2","created_at":"2026-05-18T01:58:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1202.5292","created_at":"2026-05-18T01:58:20Z"},{"alias_kind":"pith_short_12","alias_value":"FG6ZKAYGUKNH","created_at":"2026-05-18T12:27:06Z"},{"alias_kind":"pith_short_16","alias_value":"FG6ZKAYGUKNHX753","created_at":"2026-05-18T12:27:06Z"},{"alias_kind":"pith_short_8","alias_value":"FG6ZKAYG","created_at":"2026-05-18T12:27:06Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:FG6ZKAYGUKNHX753RGIWIRDNCL","target":"record","payload":{"canonical_record":{"source":{"id":"1202.5292","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-02-23T20:43:14Z","cross_cats_sorted":[],"title_canon_sha256":"37ddf6239cf8e0d3ecb892b49e3bb57b5581249eae80dc79fa984a8b593215cf","abstract_canon_sha256":"c689b87fb4dab56e3dbcf2729ac57da0c869e1b9a2e15ad006ea443fae2ad507"},"schema_version":"1.0"},"canonical_sha256":"29bd950306a29a7bffbb899164446d12d9a90384557c61642c59229b5a439e88","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:58:20.214406Z","signature_b64":"ohTP2wA8DUedcUiPcoEnCWdUWUVHUm5eLcdc540oOn8qP1CJilyKQ4H+2q0TMyPAPuBzTKRxRpqNV44BMKX2BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"29bd950306a29a7bffbb899164446d12d9a90384557c61642c59229b5a439e88","last_reissued_at":"2026-05-18T01:58:20.213892Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:58:20.213892Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1202.5292","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:58:20Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"gMUWIbJwVwd6+GzXVI+16UikRAD/FppOt7Ovtz5lh8dFCLCkxVUAexpFdZxiYhpBykVVZWSrHzzn4+FRzE2CCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-23T10:29:56.692685Z"},"content_sha256":"7cbec42a5ec5c9af36576da1e033101dedf20271a33e1001fa4bd02873160c07","schema_version":"1.0","event_id":"sha256:7cbec42a5ec5c9af36576da1e033101dedf20271a33e1001fa4bd02873160c07"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:FG6ZKAYGUKNHX753RGIWIRDNCL","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Exact results for static and radiative fields of a quark in N=4 super Yang-Mills","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Aitor Lewkowycz, Bartomeu Fiol, Blai Garolera","submitted_at":"2012-02-23T20:43:14Z","abstract_excerpt":"In this work (which supersedes our previous preprint arXiv:1112.2345) we determine the expectation value of the N=4$ SU(N) SYM Lagrangian density operator in the presence of an infinitely heavy static particle in the symmetric representation of SU(N), by means of a D3-brane probe computation. The result that we obtain coincides with two previous computations of different observables, up to kinematical factors. We argue that these agreements go beyond the D-brane probe approximation, which leads us to propose an exact formula for the expectation value of various operators. In particular, we pro"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1202.5292","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":""},"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":"2026-05-18T01:58:20Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"CgDMn90/BQB70B8vExxJNl3Ugpm1QBLqffDwp5ATX+Jhl9HcldbY3yB5sb4I5Gg2dh+ylaJg/qEjVslygyN/CQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-23T10:29:56.693420Z"},"content_sha256":"79e019163c0a2a511e32f235a0e6fbc42a8efbebf89b3b7101655f14deb504da","schema_version":"1.0","event_id":"sha256:79e019163c0a2a511e32f235a0e6fbc42a8efbebf89b3b7101655f14deb504da"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/FG6ZKAYGUKNHX753RGIWIRDNCL/bundle.json","state_url":"https://pith.science/pith/FG6ZKAYGUKNHX753RGIWIRDNCL/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/FG6ZKAYGUKNHX753RGIWIRDNCL/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":"2026-05-23T10:29:56Z","links":{"resolver":"https://pith.science/pith/FG6ZKAYGUKNHX753RGIWIRDNCL","bundle":"https://pith.science/pith/FG6ZKAYGUKNHX753RGIWIRDNCL/bundle.json","state":"https://pith.science/pith/FG6ZKAYGUKNHX753RGIWIRDNCL/state.json","well_known_bundle":"https://pith.science/.well-known/pith/FG6ZKAYGUKNHX753RGIWIRDNCL/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:FG6ZKAYGUKNHX753RGIWIRDNCL","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":"c689b87fb4dab56e3dbcf2729ac57da0c869e1b9a2e15ad006ea443fae2ad507","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-02-23T20:43:14Z","title_canon_sha256":"37ddf6239cf8e0d3ecb892b49e3bb57b5581249eae80dc79fa984a8b593215cf"},"schema_version":"1.0","source":{"id":"1202.5292","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1202.5292","created_at":"2026-05-18T01:58:20Z"},{"alias_kind":"arxiv_version","alias_value":"1202.5292v2","created_at":"2026-05-18T01:58:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1202.5292","created_at":"2026-05-18T01:58:20Z"},{"alias_kind":"pith_short_12","alias_value":"FG6ZKAYGUKNH","created_at":"2026-05-18T12:27:06Z"},{"alias_kind":"pith_short_16","alias_value":"FG6ZKAYGUKNHX753","created_at":"2026-05-18T12:27:06Z"},{"alias_kind":"pith_short_8","alias_value":"FG6ZKAYG","created_at":"2026-05-18T12:27:06Z"}],"graph_snapshots":[{"event_id":"sha256:79e019163c0a2a511e32f235a0e6fbc42a8efbebf89b3b7101655f14deb504da","target":"graph","created_at":"2026-05-18T01:58:20Z","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":"In this work (which supersedes our previous preprint arXiv:1112.2345) we determine the expectation value of the N=4$ SU(N) SYM Lagrangian density operator in the presence of an infinitely heavy static particle in the symmetric representation of SU(N), by means of a D3-brane probe computation. The result that we obtain coincides with two previous computations of different observables, up to kinematical factors. We argue that these agreements go beyond the D-brane probe approximation, which leads us to propose an exact formula for the expectation value of various operators. In particular, we pro","authors_text":"Aitor Lewkowycz, Bartomeu Fiol, Blai Garolera","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-02-23T20:43:14Z","title":"Exact results for static and radiative fields of a quark in N=4 super Yang-Mills"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1202.5292","kind":"arxiv","version":2},"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":"sha256:7cbec42a5ec5c9af36576da1e033101dedf20271a33e1001fa4bd02873160c07","target":"record","created_at":"2026-05-18T01:58:20Z","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":"c689b87fb4dab56e3dbcf2729ac57da0c869e1b9a2e15ad006ea443fae2ad507","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-02-23T20:43:14Z","title_canon_sha256":"37ddf6239cf8e0d3ecb892b49e3bb57b5581249eae80dc79fa984a8b593215cf"},"schema_version":"1.0","source":{"id":"1202.5292","kind":"arxiv","version":2}},"canonical_sha256":"29bd950306a29a7bffbb899164446d12d9a90384557c61642c59229b5a439e88","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"29bd950306a29a7bffbb899164446d12d9a90384557c61642c59229b5a439e88","first_computed_at":"2026-05-18T01:58:20.213892Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:58:20.213892Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ohTP2wA8DUedcUiPcoEnCWdUWUVHUm5eLcdc540oOn8qP1CJilyKQ4H+2q0TMyPAPuBzTKRxRpqNV44BMKX2BA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:58:20.214406Z","signed_message":"canonical_sha256_bytes"},"source_id":"1202.5292","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7cbec42a5ec5c9af36576da1e033101dedf20271a33e1001fa4bd02873160c07","sha256:79e019163c0a2a511e32f235a0e6fbc42a8efbebf89b3b7101655f14deb504da"],"state_sha256":"fa297b00bab8929bd37b6050928892dc3139bfa3c537719c5c52cf9aa134ca61"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"YQuosQcoHb+NiNBBgF4KDaVf1wYRAtwQ5BNvqbT/2sxVB8A6fEoM4ekKfNvWyvPzMV3/dLSX1egASKhwyCcYAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-23T10:29:56.697083Z","bundle_sha256":"16f9810f60029bec340225806c2428bf511e5d8ed6030f7cab0d343416871389"}}