{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2023:3MGNQ6MPTQZFK3ZEAHZW6H4TBQ","short_pith_number":"pith:3MGNQ6MP","canonical_record":{"source":{"id":"2306.04571","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2023-06-07T16:17:55Z","cross_cats_sorted":[],"title_canon_sha256":"7be5be6a657b22cefa5a33f779d24f13f127072ba1684c8da3fbbc747d18da8b","abstract_canon_sha256":"3634321b3175ec3228e045358366696dfb0e7750801d0b3a29115247501d0e6c"},"schema_version":"1.0"},"canonical_sha256":"db0cd8798f9c32556f2401f36f1f930c19ffabdb084c750f2461b021ad1061f6","source":{"kind":"arxiv","id":"2306.04571","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2306.04571","created_at":"2026-07-05T08:26:57Z"},{"alias_kind":"arxiv_version","alias_value":"2306.04571v2","created_at":"2026-07-05T08:26:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2306.04571","created_at":"2026-07-05T08:26:57Z"},{"alias_kind":"pith_short_12","alias_value":"3MGNQ6MPTQZF","created_at":"2026-07-05T08:26:57Z"},{"alias_kind":"pith_short_16","alias_value":"3MGNQ6MPTQZFK3ZE","created_at":"2026-07-05T08:26:57Z"},{"alias_kind":"pith_short_8","alias_value":"3MGNQ6MP","created_at":"2026-07-05T08:26:57Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2023:3MGNQ6MPTQZFK3ZEAHZW6H4TBQ","target":"record","payload":{"canonical_record":{"source":{"id":"2306.04571","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2023-06-07T16:17:55Z","cross_cats_sorted":[],"title_canon_sha256":"7be5be6a657b22cefa5a33f779d24f13f127072ba1684c8da3fbbc747d18da8b","abstract_canon_sha256":"3634321b3175ec3228e045358366696dfb0e7750801d0b3a29115247501d0e6c"},"schema_version":"1.0"},"canonical_sha256":"db0cd8798f9c32556f2401f36f1f930c19ffabdb084c750f2461b021ad1061f6","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:26:57.359763Z","signature_b64":"qYvJRHh5TGru6soV2VU7rXk8gzhhLn6uYLh2uXUnDFLw9RSJiOknYqD+zA/XQIgLTAUcdtpVqwz4zqaBRMU3Bw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"db0cd8798f9c32556f2401f36f1f930c19ffabdb084c750f2461b021ad1061f6","last_reissued_at":"2026-07-05T08:26:57.359174Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:26:57.359174Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2306.04571","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":"2026-07-05T08:26:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Q3nF3rjbNth3UWwFJLsaARQ1QQQNJdi0x21wp7VbQzU99QguxYrdsMozKsEms33pYksuRtZcMTljJcHceab8Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-22T09:46:26.001303Z"},"content_sha256":"80f8db3818c924555c5572999f051e8f6c5a4898edb8ade5a88396747de85c53","schema_version":"1.0","event_id":"sha256:80f8db3818c924555c5572999f051e8f6c5a4898edb8ade5a88396747de85c53"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2023:3MGNQ6MPTQZFK3ZEAHZW6H4TBQ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Asymptotic Structure of Higher Dimensional Yang-Mills Theory","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Prahar Mitra, Temple He","submitted_at":"2023-06-07T16:17:55Z","abstract_excerpt":"Using the covariant phase space formalism, we construct the phase space for non-Abelian gauge theories in $(d+2)$-dimensional Minkowski spacetime for any $d \\geq 2$, including the edge modes that symplectically pair to the low energy degrees of freedom of the gauge field. Despite the fact that the symplectic form in odd and even-dimensional spacetimes appear ostensibly different, we demonstrate that both cases can be treated in a unified manner by utilizing the shadow transform. Upon quantization, we recover the algebra of the vacuum sector of the Hilbert space and derive a Ward identity that "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2306.04571","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/2306.04571/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":"2026-07-05T08:26:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1yv34y9hyPoYDO1W0Ai45KAkdSoDFTsfya6qANfVp0cH9gP/tw29tVI54TZcyKE6xMQdiviDktztwn57T+wgCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-22T09:46:26.001874Z"},"content_sha256":"f485e0a917cc36b36c3316fe1ca826f283bc8076ced19a02b8e7d54c67d9ab5e","schema_version":"1.0","event_id":"sha256:f485e0a917cc36b36c3316fe1ca826f283bc8076ced19a02b8e7d54c67d9ab5e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3MGNQ6MPTQZFK3ZEAHZW6H4TBQ/bundle.json","state_url":"https://pith.science/pith/3MGNQ6MPTQZFK3ZEAHZW6H4TBQ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3MGNQ6MPTQZFK3ZEAHZW6H4TBQ/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":"2026-08-22T09:46:26Z","links":{"resolver":"https://pith.science/pith/3MGNQ6MPTQZFK3ZEAHZW6H4TBQ","bundle":"https://pith.science/pith/3MGNQ6MPTQZFK3ZEAHZW6H4TBQ/bundle.json","state":"https://pith.science/pith/3MGNQ6MPTQZFK3ZEAHZW6H4TBQ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3MGNQ6MPTQZFK3ZEAHZW6H4TBQ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:3MGNQ6MPTQZFK3ZEAHZW6H4TBQ","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":"3634321b3175ec3228e045358366696dfb0e7750801d0b3a29115247501d0e6c","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2023-06-07T16:17:55Z","title_canon_sha256":"7be5be6a657b22cefa5a33f779d24f13f127072ba1684c8da3fbbc747d18da8b"},"schema_version":"1.0","source":{"id":"2306.04571","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2306.04571","created_at":"2026-07-05T08:26:57Z"},{"alias_kind":"arxiv_version","alias_value":"2306.04571v2","created_at":"2026-07-05T08:26:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2306.04571","created_at":"2026-07-05T08:26:57Z"},{"alias_kind":"pith_short_12","alias_value":"3MGNQ6MPTQZF","created_at":"2026-07-05T08:26:57Z"},{"alias_kind":"pith_short_16","alias_value":"3MGNQ6MPTQZFK3ZE","created_at":"2026-07-05T08:26:57Z"},{"alias_kind":"pith_short_8","alias_value":"3MGNQ6MP","created_at":"2026-07-05T08:26:57Z"}],"graph_snapshots":[{"event_id":"sha256:f485e0a917cc36b36c3316fe1ca826f283bc8076ced19a02b8e7d54c67d9ab5e","target":"graph","created_at":"2026-07-05T08:26:57Z","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/2306.04571/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Using the covariant phase space formalism, we construct the phase space for non-Abelian gauge theories in $(d+2)$-dimensional Minkowski spacetime for any $d \\geq 2$, including the edge modes that symplectically pair to the low energy degrees of freedom of the gauge field. Despite the fact that the symplectic form in odd and even-dimensional spacetimes appear ostensibly different, we demonstrate that both cases can be treated in a unified manner by utilizing the shadow transform. Upon quantization, we recover the algebra of the vacuum sector of the Hilbert space and derive a Ward identity that ","authors_text":"Prahar Mitra, Temple He","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2023-06-07T16:17:55Z","title":"Asymptotic Structure of Higher Dimensional Yang-Mills Theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2306.04571","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":"sha256:80f8db3818c924555c5572999f051e8f6c5a4898edb8ade5a88396747de85c53","target":"record","created_at":"2026-07-05T08:26:57Z","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":"3634321b3175ec3228e045358366696dfb0e7750801d0b3a29115247501d0e6c","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2023-06-07T16:17:55Z","title_canon_sha256":"7be5be6a657b22cefa5a33f779d24f13f127072ba1684c8da3fbbc747d18da8b"},"schema_version":"1.0","source":{"id":"2306.04571","kind":"arxiv","version":2}},"canonical_sha256":"db0cd8798f9c32556f2401f36f1f930c19ffabdb084c750f2461b021ad1061f6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"db0cd8798f9c32556f2401f36f1f930c19ffabdb084c750f2461b021ad1061f6","first_computed_at":"2026-07-05T08:26:57.359174Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T08:26:57.359174Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"qYvJRHh5TGru6soV2VU7rXk8gzhhLn6uYLh2uXUnDFLw9RSJiOknYqD+zA/XQIgLTAUcdtpVqwz4zqaBRMU3Bw==","signature_status":"signed_v1","signed_at":"2026-07-05T08:26:57.359763Z","signed_message":"canonical_sha256_bytes"},"source_id":"2306.04571","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:80f8db3818c924555c5572999f051e8f6c5a4898edb8ade5a88396747de85c53","sha256:f485e0a917cc36b36c3316fe1ca826f283bc8076ced19a02b8e7d54c67d9ab5e"],"state_sha256":"38bbe04f4b19c9da1c631d777a77aea376b7ffb0c69991be5b6f9e03f07a48b3"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ycb+v1ZNPx2SxLiriswTv085YaL4ljKR6ls3F1KvV7LVUBSourE8z5CeoTkDkfkH1shIIXgSwTtf6+ac6BNLBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-22T09:46:26.007241Z","bundle_sha256":"91323a147bf088082023d0e7697079eb7f62dba6de2e0aca9372706e7f8efd42"}}