{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:JCIYZVJS6YUGISB77RQUOPCEJN","short_pith_number":"pith:JCIYZVJS","canonical_record":{"source":{"id":"1204.6036","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2012-04-26T17:36:58Z","cross_cats_sorted":[],"title_canon_sha256":"c4bdd8bc78e1161539ca5f7401c3c1787150f6f64fc806042a9817ff8b483229","abstract_canon_sha256":"e2088975a0f88ecca6d45d3085a2c4658694ceaa68a0cf7788a6c0556dd73f5f"},"schema_version":"1.0"},"canonical_sha256":"48918cd532f62864483ffc61473c444b490b78c02735346398746432e5ab0f82","source":{"kind":"arxiv","id":"1204.6036","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1204.6036","created_at":"2026-05-18T03:16:17Z"},{"alias_kind":"arxiv_version","alias_value":"1204.6036v1","created_at":"2026-05-18T03:16:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1204.6036","created_at":"2026-05-18T03:16:17Z"},{"alias_kind":"pith_short_12","alias_value":"JCIYZVJS6YUG","created_at":"2026-05-18T12:27:11Z"},{"alias_kind":"pith_short_16","alias_value":"JCIYZVJS6YUGISB7","created_at":"2026-05-18T12:27:11Z"},{"alias_kind":"pith_short_8","alias_value":"JCIYZVJS","created_at":"2026-05-18T12:27:11Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:JCIYZVJS6YUGISB77RQUOPCEJN","target":"record","payload":{"canonical_record":{"source":{"id":"1204.6036","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2012-04-26T17:36:58Z","cross_cats_sorted":[],"title_canon_sha256":"c4bdd8bc78e1161539ca5f7401c3c1787150f6f64fc806042a9817ff8b483229","abstract_canon_sha256":"e2088975a0f88ecca6d45d3085a2c4658694ceaa68a0cf7788a6c0556dd73f5f"},"schema_version":"1.0"},"canonical_sha256":"48918cd532f62864483ffc61473c444b490b78c02735346398746432e5ab0f82","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:16:17.517682Z","signature_b64":"BEZfLc6UGCrvYDS8ZaU6FrecJlB9HJKR7RnhGmFPArtFZSTi+otANUp2GtYE2ADTvvk1DFSUFVTRkU6yDE9zCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"48918cd532f62864483ffc61473c444b490b78c02735346398746432e5ab0f82","last_reissued_at":"2026-05-18T03:16:17.516829Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:16:17.516829Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1204.6036","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":"2026-05-18T03:16:17Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"huF3fB2Fn7Owscgvvn3BkhvvQ0XZhU1lVwG+G1+fBiI5p53XzbWMHQsii3+Pl/OAXMrrRxHL18zfqWRR6QwtBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-06T18:33:39.937744Z"},"content_sha256":"0d3c29fe860a46fbf254eb0d0853db1b4062e9e64d25484f05882ea33cb94fe9","schema_version":"1.0","event_id":"sha256:0d3c29fe860a46fbf254eb0d0853db1b4062e9e64d25484f05882ea33cb94fe9"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:JCIYZVJS6YUGISB77RQUOPCEJN","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Contrasting Classical and Quantum Vacuum States in Non-Inertial Frames","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Timothy H. Boyer","submitted_at":"2012-04-26T17:36:58Z","abstract_excerpt":"Classical electron theory with classical electromagnetic zero-point radiation (stochastic electrodynamics) is the classical theory which most closely approximates quantum electrodynamics. Indeed, in inertial frames, there is a general connection between classical field theories with classical zero-point radiation and quantum field theories. However, this connection does not extend to noninertial frames where the time parameter is not a geodesic coordinate. Quantum field theory applies the canonical quantization procedure (depending on the local time coordinate) to a mirror-walled box, and, in "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1204.6036","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":"2026-05-18T03:16:17Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fPCaE0vtE9ksH1nL18D369+ovj5kGYq+czQLbi3FnrPO8dY03+/0fgI+JzEhsIu1WxPxu507cb9UGfx88tDgCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-06T18:33:39.938528Z"},"content_sha256":"f16ca078146f27218e1e312401c084b843dd07ac984304eeef6731041bafa470","schema_version":"1.0","event_id":"sha256:f16ca078146f27218e1e312401c084b843dd07ac984304eeef6731041bafa470"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/JCIYZVJS6YUGISB77RQUOPCEJN/bundle.json","state_url":"https://pith.science/pith/JCIYZVJS6YUGISB77RQUOPCEJN/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/JCIYZVJS6YUGISB77RQUOPCEJN/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":"2026-06-06T18:33:39Z","links":{"resolver":"https://pith.science/pith/JCIYZVJS6YUGISB77RQUOPCEJN","bundle":"https://pith.science/pith/JCIYZVJS6YUGISB77RQUOPCEJN/bundle.json","state":"https://pith.science/pith/JCIYZVJS6YUGISB77RQUOPCEJN/state.json","well_known_bundle":"https://pith.science/.well-known/pith/JCIYZVJS6YUGISB77RQUOPCEJN/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:JCIYZVJS6YUGISB77RQUOPCEJN","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":"e2088975a0f88ecca6d45d3085a2c4658694ceaa68a0cf7788a6c0556dd73f5f","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2012-04-26T17:36:58Z","title_canon_sha256":"c4bdd8bc78e1161539ca5f7401c3c1787150f6f64fc806042a9817ff8b483229"},"schema_version":"1.0","source":{"id":"1204.6036","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1204.6036","created_at":"2026-05-18T03:16:17Z"},{"alias_kind":"arxiv_version","alias_value":"1204.6036v1","created_at":"2026-05-18T03:16:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1204.6036","created_at":"2026-05-18T03:16:17Z"},{"alias_kind":"pith_short_12","alias_value":"JCIYZVJS6YUG","created_at":"2026-05-18T12:27:11Z"},{"alias_kind":"pith_short_16","alias_value":"JCIYZVJS6YUGISB7","created_at":"2026-05-18T12:27:11Z"},{"alias_kind":"pith_short_8","alias_value":"JCIYZVJS","created_at":"2026-05-18T12:27:11Z"}],"graph_snapshots":[{"event_id":"sha256:f16ca078146f27218e1e312401c084b843dd07ac984304eeef6731041bafa470","target":"graph","created_at":"2026-05-18T03:16:17Z","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":"Classical electron theory with classical electromagnetic zero-point radiation (stochastic electrodynamics) is the classical theory which most closely approximates quantum electrodynamics. Indeed, in inertial frames, there is a general connection between classical field theories with classical zero-point radiation and quantum field theories. However, this connection does not extend to noninertial frames where the time parameter is not a geodesic coordinate. Quantum field theory applies the canonical quantization procedure (depending on the local time coordinate) to a mirror-walled box, and, in ","authors_text":"Timothy H. Boyer","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2012-04-26T17:36:58Z","title":"Contrasting Classical and Quantum Vacuum States in Non-Inertial Frames"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1204.6036","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":"sha256:0d3c29fe860a46fbf254eb0d0853db1b4062e9e64d25484f05882ea33cb94fe9","target":"record","created_at":"2026-05-18T03:16:17Z","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":"e2088975a0f88ecca6d45d3085a2c4658694ceaa68a0cf7788a6c0556dd73f5f","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2012-04-26T17:36:58Z","title_canon_sha256":"c4bdd8bc78e1161539ca5f7401c3c1787150f6f64fc806042a9817ff8b483229"},"schema_version":"1.0","source":{"id":"1204.6036","kind":"arxiv","version":1}},"canonical_sha256":"48918cd532f62864483ffc61473c444b490b78c02735346398746432e5ab0f82","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"48918cd532f62864483ffc61473c444b490b78c02735346398746432e5ab0f82","first_computed_at":"2026-05-18T03:16:17.516829Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:16:17.516829Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"BEZfLc6UGCrvYDS8ZaU6FrecJlB9HJKR7RnhGmFPArtFZSTi+otANUp2GtYE2ADTvvk1DFSUFVTRkU6yDE9zCw==","signature_status":"signed_v1","signed_at":"2026-05-18T03:16:17.517682Z","signed_message":"canonical_sha256_bytes"},"source_id":"1204.6036","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0d3c29fe860a46fbf254eb0d0853db1b4062e9e64d25484f05882ea33cb94fe9","sha256:f16ca078146f27218e1e312401c084b843dd07ac984304eeef6731041bafa470"],"state_sha256":"8ec2dbe1ac6baf3e26327f1d072881c0e0f1f4f1d2d74371da77ef2985d1bff4"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"unf7ewC1OnWNga7idlfYMTojhYcGKSibeooyGxBYqBLpsmvw7xBPfKaipSiOgFNZH8/A3Z5IqPxN1b5bi6DvCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-06T18:33:39.941695Z","bundle_sha256":"a21011acd2d3cb332033f8c02674e18bd5949087ae0abf3f4e7467a561e8e31c"}}