{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1995:KUGRAYYE6QAEE6NC3XGPWNHHTR","short_pith_number":"pith:KUGRAYYE","canonical_record":{"source":{"id":"hep-ph/9508394","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1995-08-29T15:47:00Z","cross_cats_sorted":[],"title_canon_sha256":"73c358f7e1c5085bc76a37b25ce51471152e609de112ea45d667589c3ce0133f","abstract_canon_sha256":"8882e91c7ac226b16789edda8534498690b008aaa5e5ccfa87107827263ededc"},"schema_version":"1.0"},"canonical_sha256":"550d106304f4004279a2ddccfb34e79c4bf82314d8eef3e0471ac7c1b3d725d3","source":{"kind":"arxiv","id":"hep-ph/9508394","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9508394","created_at":"2026-07-04T15:59:12Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9508394v1","created_at":"2026-07-04T15:59:12Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9508394","created_at":"2026-07-04T15:59:12Z"},{"alias_kind":"pith_short_12","alias_value":"KUGRAYYE6QAE","created_at":"2026-07-04T15:59:12Z"},{"alias_kind":"pith_short_16","alias_value":"KUGRAYYE6QAEE6NC","created_at":"2026-07-04T15:59:12Z"},{"alias_kind":"pith_short_8","alias_value":"KUGRAYYE","created_at":"2026-07-04T15:59:12Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1995:KUGRAYYE6QAEE6NC3XGPWNHHTR","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/9508394","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1995-08-29T15:47:00Z","cross_cats_sorted":[],"title_canon_sha256":"73c358f7e1c5085bc76a37b25ce51471152e609de112ea45d667589c3ce0133f","abstract_canon_sha256":"8882e91c7ac226b16789edda8534498690b008aaa5e5ccfa87107827263ededc"},"schema_version":"1.0"},"canonical_sha256":"550d106304f4004279a2ddccfb34e79c4bf82314d8eef3e0471ac7c1b3d725d3","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:59:12.919871Z","signature_b64":"G44TP0zyeZde3QWQ0eqh8x2OuGmGAi45XARi68VypMZtjFvVytdd/37afOoauU4lqM/a1+DrsvRkB6amzO/KDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"550d106304f4004279a2ddccfb34e79c4bf82314d8eef3e0471ac7c1b3d725d3","last_reissued_at":"2026-07-04T15:59:12.919487Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:59:12.919487Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/9508394","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":"2026-07-04T15:59:12Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"YLbpl5uMhx659322iE3zaypt53DRTvfRwQn92Z/W4cNVGMsuWf/8MFp4q2mMC9psBniwXxVgGpCYBHOlYZ98Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-05T05:23:17.235393Z"},"content_sha256":"b8a1dee94fa9768b294cfc5d14ebe7af4e6a3661e94836fa224ac07451d031ea","schema_version":"1.0","event_id":"sha256:b8a1dee94fa9768b294cfc5d14ebe7af4e6a3661e94836fa224ac07451d031ea"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1995:KUGRAYYE6QAEE6NC3XGPWNHHTR","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Remarks on the Coulomb and Covariant Gauges in Finite Temperature QED","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"J. C. D'Olivo, Jose F. Nieves","submitted_at":"1995-08-29T15:47:00Z","abstract_excerpt":"We compare the use of the Coulomb gauge in finite temperature QED with a recently proposed prescription for covariant gauges, in which only the transverse photon degrees of freedom are thermalized. Using the Landau rule as a guide, we clarify the relation between the retarded electron self-energy and the elements of the self-energy matrix in the real-time formulation of . The general results are illustrated by means of the one-loop expressions for the electron self-energy in a QED plasma."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9508394","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/hep-ph/9508394/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":"2026-07-04T15:59:12Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"BboiTyQd6blGLyUiBeEP2/xVsVhtXlyu1u1XPjoMV3qJn1VLKvi2h4MQ4QqQqHn4fi2MybZlp2kkZx8YFSz9BQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-05T05:23:17.235787Z"},"content_sha256":"fa65479e60b1b77ca7866045e1d671eea3e007496e4a107c31b753769655cce6","schema_version":"1.0","event_id":"sha256:fa65479e60b1b77ca7866045e1d671eea3e007496e4a107c31b753769655cce6"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/KUGRAYYE6QAEE6NC3XGPWNHHTR/bundle.json","state_url":"https://pith.science/pith/KUGRAYYE6QAEE6NC3XGPWNHHTR/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/KUGRAYYE6QAEE6NC3XGPWNHHTR/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":"2026-07-05T05:23:17Z","links":{"resolver":"https://pith.science/pith/KUGRAYYE6QAEE6NC3XGPWNHHTR","bundle":"https://pith.science/pith/KUGRAYYE6QAEE6NC3XGPWNHHTR/bundle.json","state":"https://pith.science/pith/KUGRAYYE6QAEE6NC3XGPWNHHTR/state.json","well_known_bundle":"https://pith.science/.well-known/pith/KUGRAYYE6QAEE6NC3XGPWNHHTR/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1995:KUGRAYYE6QAEE6NC3XGPWNHHTR","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":"8882e91c7ac226b16789edda8534498690b008aaa5e5ccfa87107827263ededc","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1995-08-29T15:47:00Z","title_canon_sha256":"73c358f7e1c5085bc76a37b25ce51471152e609de112ea45d667589c3ce0133f"},"schema_version":"1.0","source":{"id":"hep-ph/9508394","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9508394","created_at":"2026-07-04T15:59:12Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9508394v1","created_at":"2026-07-04T15:59:12Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9508394","created_at":"2026-07-04T15:59:12Z"},{"alias_kind":"pith_short_12","alias_value":"KUGRAYYE6QAE","created_at":"2026-07-04T15:59:12Z"},{"alias_kind":"pith_short_16","alias_value":"KUGRAYYE6QAEE6NC","created_at":"2026-07-04T15:59:12Z"},{"alias_kind":"pith_short_8","alias_value":"KUGRAYYE","created_at":"2026-07-04T15:59:12Z"}],"graph_snapshots":[{"event_id":"sha256:fa65479e60b1b77ca7866045e1d671eea3e007496e4a107c31b753769655cce6","target":"graph","created_at":"2026-07-04T15:59:12Z","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/hep-ph/9508394/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We compare the use of the Coulomb gauge in finite temperature QED with a recently proposed prescription for covariant gauges, in which only the transverse photon degrees of freedom are thermalized. Using the Landau rule as a guide, we clarify the relation between the retarded electron self-energy and the elements of the self-energy matrix in the real-time formulation of . The general results are illustrated by means of the one-loop expressions for the electron self-energy in a QED plasma.","authors_text":"J. C. D'Olivo, Jose F. Nieves","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"1995-08-29T15:47:00Z","title":"Remarks on the Coulomb and Covariant Gauges in Finite Temperature QED"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9508394","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:b8a1dee94fa9768b294cfc5d14ebe7af4e6a3661e94836fa224ac07451d031ea","target":"record","created_at":"2026-07-04T15:59:12Z","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":"8882e91c7ac226b16789edda8534498690b008aaa5e5ccfa87107827263ededc","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1995-08-29T15:47:00Z","title_canon_sha256":"73c358f7e1c5085bc76a37b25ce51471152e609de112ea45d667589c3ce0133f"},"schema_version":"1.0","source":{"id":"hep-ph/9508394","kind":"arxiv","version":1}},"canonical_sha256":"550d106304f4004279a2ddccfb34e79c4bf82314d8eef3e0471ac7c1b3d725d3","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"550d106304f4004279a2ddccfb34e79c4bf82314d8eef3e0471ac7c1b3d725d3","first_computed_at":"2026-07-04T15:59:12.919487Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:59:12.919487Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"G44TP0zyeZde3QWQ0eqh8x2OuGmGAi45XARi68VypMZtjFvVytdd/37afOoauU4lqM/a1+DrsvRkB6amzO/KDw==","signature_status":"signed_v1","signed_at":"2026-07-04T15:59:12.919871Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/9508394","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b8a1dee94fa9768b294cfc5d14ebe7af4e6a3661e94836fa224ac07451d031ea","sha256:fa65479e60b1b77ca7866045e1d671eea3e007496e4a107c31b753769655cce6"],"state_sha256":"c46dea93df634e6f3d66c478a4ceb04a26ca6382a55ed58638dca1580dd0e86e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+zpIZekLblgQq+hp4q7MHkIj5kKuL2JhEmyyYdKqY3JyJiBOamuQfL1s5tAS1mdDobMAOu/SqB1nFcR6pcD2Ag==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-05T05:23:17.237736Z","bundle_sha256":"eacf929ddae50ab25799c99428f5d11b57538294d2ebfb54fb8cb0780a345ea3"}}