{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2023:LLW6E5BLBAMKMTQGQ6DZ2COELU","short_pith_number":"pith:LLW6E5BL","canonical_record":{"source":{"id":"2310.14690","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2023-10-23T08:31:19Z","cross_cats_sorted":[],"title_canon_sha256":"2a786def83050628947d526916af7a3c67e8fcd6c02f39d0f654f7b2b88a5b70","abstract_canon_sha256":"5442f4f75a453fc19611e26456ce35a54d467769ab6eafe857280b00f47bf618"},"schema_version":"1.0"},"canonical_sha256":"5aede2742b0818a64e0687879d09c45d3c640d02ffb0a76ded7310e7e60cfa08","source":{"kind":"arxiv","id":"2310.14690","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2310.14690","created_at":"2026-07-05T07:03:48Z"},{"alias_kind":"arxiv_version","alias_value":"2310.14690v1","created_at":"2026-07-05T07:03:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2310.14690","created_at":"2026-07-05T07:03:48Z"},{"alias_kind":"pith_short_12","alias_value":"LLW6E5BLBAMK","created_at":"2026-07-05T07:03:48Z"},{"alias_kind":"pith_short_16","alias_value":"LLW6E5BLBAMKMTQG","created_at":"2026-07-05T07:03:48Z"},{"alias_kind":"pith_short_8","alias_value":"LLW6E5BL","created_at":"2026-07-05T07:03:48Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2023:LLW6E5BLBAMKMTQGQ6DZ2COELU","target":"record","payload":{"canonical_record":{"source":{"id":"2310.14690","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2023-10-23T08:31:19Z","cross_cats_sorted":[],"title_canon_sha256":"2a786def83050628947d526916af7a3c67e8fcd6c02f39d0f654f7b2b88a5b70","abstract_canon_sha256":"5442f4f75a453fc19611e26456ce35a54d467769ab6eafe857280b00f47bf618"},"schema_version":"1.0"},"canonical_sha256":"5aede2742b0818a64e0687879d09c45d3c640d02ffb0a76ded7310e7e60cfa08","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:03:48.495376Z","signature_b64":"ombFx1VDzK/ydxVzOhNcIENatBWHb3YhbfwQpPo4rmm9z2PQS/O3JA/SyKRcPM08jRNxVCesf9H2gGdgNp8BBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5aede2742b0818a64e0687879d09c45d3c640d02ffb0a76ded7310e7e60cfa08","last_reissued_at":"2026-07-05T07:03:48.494942Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:03:48.494942Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2310.14690","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":"2026-07-05T07:03:48Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"E+LEGkgVL1v4lRatOfKtkyk1YH1Z+RwkFa3guDTAW+tiQZYQ1UMI9Rn2lhXnSUCkihVJNjNAHnO8cGcE5CFQCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-09T05:29:21.124123Z"},"content_sha256":"daf470b0dc06b459a052841109629c2e2e5fad7473ab15e290633113af842660","schema_version":"1.0","event_id":"sha256:daf470b0dc06b459a052841109629c2e2e5fad7473ab15e290633113af842660"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2023:LLW6E5BLBAMKMTQGQ6DZ2COELU","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Entanglement entropy and the boundary action of edge modes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Jyotirmoy Mukherjee","submitted_at":"2023-10-23T08:31:19Z","abstract_excerpt":"We consider an antisymmetric gauge field in the Minkowski space of $d$-dimension and decompose it in terms of the antisymmetric tensor harmonics and fix the gauge. The Gauss law implies that the normal component of the field strength on the spherical entangling surface will label the superselection sectors. From the two-point function of the field strength on the sphere, we evaluate the logarithmic divergent term of the entanglement entropy of edge modes of $p$-form field. We observe that the logarithmic divergent term in entanglement entropy of edge modes coincides with the edge partition fun"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2310.14690","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2310.14690/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":"2026-07-05T07:03:48Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Xa5fuz9WfAfx9OIp9rHrt3+/U0rX6jnfOc+QaghfjAzd2CG0z52KhbQXqyR9q6MLfRPIpMqYyJedw0UqytvCDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-09T05:29:21.125004Z"},"content_sha256":"24451ff56584ad23e4d78098bf6513d882c700150b50a3d039a93a60e6aff8f8","schema_version":"1.0","event_id":"sha256:24451ff56584ad23e4d78098bf6513d882c700150b50a3d039a93a60e6aff8f8"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/LLW6E5BLBAMKMTQGQ6DZ2COELU/bundle.json","state_url":"https://pith.science/pith/LLW6E5BLBAMKMTQGQ6DZ2COELU/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/LLW6E5BLBAMKMTQGQ6DZ2COELU/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":"2026-08-09T05:29:21Z","links":{"resolver":"https://pith.science/pith/LLW6E5BLBAMKMTQGQ6DZ2COELU","bundle":"https://pith.science/pith/LLW6E5BLBAMKMTQGQ6DZ2COELU/bundle.json","state":"https://pith.science/pith/LLW6E5BLBAMKMTQGQ6DZ2COELU/state.json","well_known_bundle":"https://pith.science/.well-known/pith/LLW6E5BLBAMKMTQGQ6DZ2COELU/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:LLW6E5BLBAMKMTQGQ6DZ2COELU","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":"5442f4f75a453fc19611e26456ce35a54d467769ab6eafe857280b00f47bf618","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2023-10-23T08:31:19Z","title_canon_sha256":"2a786def83050628947d526916af7a3c67e8fcd6c02f39d0f654f7b2b88a5b70"},"schema_version":"1.0","source":{"id":"2310.14690","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2310.14690","created_at":"2026-07-05T07:03:48Z"},{"alias_kind":"arxiv_version","alias_value":"2310.14690v1","created_at":"2026-07-05T07:03:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2310.14690","created_at":"2026-07-05T07:03:48Z"},{"alias_kind":"pith_short_12","alias_value":"LLW6E5BLBAMK","created_at":"2026-07-05T07:03:48Z"},{"alias_kind":"pith_short_16","alias_value":"LLW6E5BLBAMKMTQG","created_at":"2026-07-05T07:03:48Z"},{"alias_kind":"pith_short_8","alias_value":"LLW6E5BL","created_at":"2026-07-05T07:03:48Z"}],"graph_snapshots":[{"event_id":"sha256:24451ff56584ad23e4d78098bf6513d882c700150b50a3d039a93a60e6aff8f8","target":"graph","created_at":"2026-07-05T07:03:48Z","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/2310.14690/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We consider an antisymmetric gauge field in the Minkowski space of $d$-dimension and decompose it in terms of the antisymmetric tensor harmonics and fix the gauge. The Gauss law implies that the normal component of the field strength on the spherical entangling surface will label the superselection sectors. From the two-point function of the field strength on the sphere, we evaluate the logarithmic divergent term of the entanglement entropy of edge modes of $p$-form field. We observe that the logarithmic divergent term in entanglement entropy of edge modes coincides with the edge partition fun","authors_text":"Jyotirmoy Mukherjee","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2023-10-23T08:31:19Z","title":"Entanglement entropy and the boundary action of edge modes"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2310.14690","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:daf470b0dc06b459a052841109629c2e2e5fad7473ab15e290633113af842660","target":"record","created_at":"2026-07-05T07:03:48Z","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":"5442f4f75a453fc19611e26456ce35a54d467769ab6eafe857280b00f47bf618","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2023-10-23T08:31:19Z","title_canon_sha256":"2a786def83050628947d526916af7a3c67e8fcd6c02f39d0f654f7b2b88a5b70"},"schema_version":"1.0","source":{"id":"2310.14690","kind":"arxiv","version":1}},"canonical_sha256":"5aede2742b0818a64e0687879d09c45d3c640d02ffb0a76ded7310e7e60cfa08","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5aede2742b0818a64e0687879d09c45d3c640d02ffb0a76ded7310e7e60cfa08","first_computed_at":"2026-07-05T07:03:48.494942Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T07:03:48.494942Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ombFx1VDzK/ydxVzOhNcIENatBWHb3YhbfwQpPo4rmm9z2PQS/O3JA/SyKRcPM08jRNxVCesf9H2gGdgNp8BBg==","signature_status":"signed_v1","signed_at":"2026-07-05T07:03:48.495376Z","signed_message":"canonical_sha256_bytes"},"source_id":"2310.14690","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:daf470b0dc06b459a052841109629c2e2e5fad7473ab15e290633113af842660","sha256:24451ff56584ad23e4d78098bf6513d882c700150b50a3d039a93a60e6aff8f8"],"state_sha256":"99008198aaaf66afc5e004017aeb786c6077f30d5b9533bdade2b5089b701471"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PuTsX3RaqH28Y6VerlbsgAd+M9EoqhTHwtstD5rQ049Zjt5j/IbY2SDrWZFNBqkBwL5wEfqhlchQ9Ixs7NP1Cg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-09T05:29:21.182330Z","bundle_sha256":"67505e030df0227398df62bb719c6712455e6a9afe5dbf6d5ce5d70485065beb"}}