{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2024:PSRERN2HC5KH7B7GFN5LNUZXZP","short_pith_number":"pith:PSRERN2H","canonical_record":{"source":{"id":"2411.19135","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2024-11-28T13:36:16Z","cross_cats_sorted":[],"title_canon_sha256":"e5e0791cd6f4da2d79daf1ec18159b18d111cdaae978f082337bb00b9d9453e3","abstract_canon_sha256":"4e7d0a2c92cdf808735c1f302d04d32716727dbcee3dc0cfd810b0e1a6104f8c"},"schema_version":"1.0"},"canonical_sha256":"7ca248b74717547f87e62b7ab6d337cbc56dabe76550804a20709e61a955d4e2","source":{"kind":"arxiv","id":"2411.19135","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2411.19135","created_at":"2026-07-05T10:16:39Z"},{"alias_kind":"arxiv_version","alias_value":"2411.19135v1","created_at":"2026-07-05T10:16:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.19135","created_at":"2026-07-05T10:16:39Z"},{"alias_kind":"pith_short_12","alias_value":"PSRERN2HC5KH","created_at":"2026-07-05T10:16:39Z"},{"alias_kind":"pith_short_16","alias_value":"PSRERN2HC5KH7B7G","created_at":"2026-07-05T10:16:39Z"},{"alias_kind":"pith_short_8","alias_value":"PSRERN2H","created_at":"2026-07-05T10:16:39Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2024:PSRERN2HC5KH7B7GFN5LNUZXZP","target":"record","payload":{"canonical_record":{"source":{"id":"2411.19135","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2024-11-28T13:36:16Z","cross_cats_sorted":[],"title_canon_sha256":"e5e0791cd6f4da2d79daf1ec18159b18d111cdaae978f082337bb00b9d9453e3","abstract_canon_sha256":"4e7d0a2c92cdf808735c1f302d04d32716727dbcee3dc0cfd810b0e1a6104f8c"},"schema_version":"1.0"},"canonical_sha256":"7ca248b74717547f87e62b7ab6d337cbc56dabe76550804a20709e61a955d4e2","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:16:39.607851Z","signature_b64":"vSSCly2uawuw3WzDUQ0vcbuCEXBctFQ4WC+6xv2mWzqEl165luykIBk3xfts3eS812Iy02adUIKvowLGr2RyAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7ca248b74717547f87e62b7ab6d337cbc56dabe76550804a20709e61a955d4e2","last_reissued_at":"2026-07-05T10:16:39.607339Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:16:39.607339Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2411.19135","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":"2026-07-05T10:16:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"gIXVDgPGyUtG6T4xlxBRUtlSl/fdm0vqzldY3akZewtoJLDt15JZBSsxVad5H/gjCY3pSOVfqhdST7Q/OIn2DA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-23T01:49:59.589326Z"},"content_sha256":"b1838ef86e2fca3b872cceb55ae3d5b5317fcce17183e8a8fc48365604b1a88c","schema_version":"1.0","event_id":"sha256:b1838ef86e2fca3b872cceb55ae3d5b5317fcce17183e8a8fc48365604b1a88c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2024:PSRERN2HC5KH7B7GFN5LNUZXZP","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"One-loop electron self-energy with accelerated partial-wave expansion in Coulomb gauge","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"C. H. Keitel, V. A. Yerokhin, Z. Harman","submitted_at":"2024-11-28T13:36:16Z","abstract_excerpt":"Numerical calculations of the electron self-energy without any expansion in the binding nuclear field are required in order to match the rapidly advancing precision of experimental spectroscopy. For the lightest elements, particularly hydrogen, these computations are complicated by large numerical cancellations and the slow convergence of the partial-wave expansion. Methods with accelerated convergence of the partial-wave expansion have been recently put forward [V. A. Yerokhin, K. Pachucki, V. M. Shabaev, Phys. Rev. A 72, 042502 (2005); J. Sapirstein and K. T. Cheng, Phys. Rev. A 108, 042804 "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.19135","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/2411.19135/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":"2026-07-05T10:16:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7vzcao62b7Uc9+9LTeU36uO3SLsNa5BKJd11EjnM6L5GHlMjDIHimhdJ2RdXSL15JszMVzJxbShaj/7E8/mlBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-23T01:49:59.589890Z"},"content_sha256":"d4bf378c272a6267c4bf7a1a571d2776de02a0686e912fb1cfe375894277a7e4","schema_version":"1.0","event_id":"sha256:d4bf378c272a6267c4bf7a1a571d2776de02a0686e912fb1cfe375894277a7e4"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/PSRERN2HC5KH7B7GFN5LNUZXZP/bundle.json","state_url":"https://pith.science/pith/PSRERN2HC5KH7B7GFN5LNUZXZP/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/PSRERN2HC5KH7B7GFN5LNUZXZP/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":"2026-08-23T01:49:59Z","links":{"resolver":"https://pith.science/pith/PSRERN2HC5KH7B7GFN5LNUZXZP","bundle":"https://pith.science/pith/PSRERN2HC5KH7B7GFN5LNUZXZP/bundle.json","state":"https://pith.science/pith/PSRERN2HC5KH7B7GFN5LNUZXZP/state.json","well_known_bundle":"https://pith.science/.well-known/pith/PSRERN2HC5KH7B7GFN5LNUZXZP/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:PSRERN2HC5KH7B7GFN5LNUZXZP","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":"4e7d0a2c92cdf808735c1f302d04d32716727dbcee3dc0cfd810b0e1a6104f8c","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2024-11-28T13:36:16Z","title_canon_sha256":"e5e0791cd6f4da2d79daf1ec18159b18d111cdaae978f082337bb00b9d9453e3"},"schema_version":"1.0","source":{"id":"2411.19135","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2411.19135","created_at":"2026-07-05T10:16:39Z"},{"alias_kind":"arxiv_version","alias_value":"2411.19135v1","created_at":"2026-07-05T10:16:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.19135","created_at":"2026-07-05T10:16:39Z"},{"alias_kind":"pith_short_12","alias_value":"PSRERN2HC5KH","created_at":"2026-07-05T10:16:39Z"},{"alias_kind":"pith_short_16","alias_value":"PSRERN2HC5KH7B7G","created_at":"2026-07-05T10:16:39Z"},{"alias_kind":"pith_short_8","alias_value":"PSRERN2H","created_at":"2026-07-05T10:16:39Z"}],"graph_snapshots":[{"event_id":"sha256:d4bf378c272a6267c4bf7a1a571d2776de02a0686e912fb1cfe375894277a7e4","target":"graph","created_at":"2026-07-05T10:16:39Z","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/2411.19135/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Numerical calculations of the electron self-energy without any expansion in the binding nuclear field are required in order to match the rapidly advancing precision of experimental spectroscopy. For the lightest elements, particularly hydrogen, these computations are complicated by large numerical cancellations and the slow convergence of the partial-wave expansion. Methods with accelerated convergence of the partial-wave expansion have been recently put forward [V. A. Yerokhin, K. Pachucki, V. M. Shabaev, Phys. Rev. A 72, 042502 (2005); J. Sapirstein and K. T. Cheng, Phys. Rev. A 108, 042804 ","authors_text":"C. H. Keitel, V. A. Yerokhin, Z. Harman","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2024-11-28T13:36:16Z","title":"One-loop electron self-energy with accelerated partial-wave expansion in Coulomb gauge"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.19135","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:b1838ef86e2fca3b872cceb55ae3d5b5317fcce17183e8a8fc48365604b1a88c","target":"record","created_at":"2026-07-05T10:16:39Z","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":"4e7d0a2c92cdf808735c1f302d04d32716727dbcee3dc0cfd810b0e1a6104f8c","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2024-11-28T13:36:16Z","title_canon_sha256":"e5e0791cd6f4da2d79daf1ec18159b18d111cdaae978f082337bb00b9d9453e3"},"schema_version":"1.0","source":{"id":"2411.19135","kind":"arxiv","version":1}},"canonical_sha256":"7ca248b74717547f87e62b7ab6d337cbc56dabe76550804a20709e61a955d4e2","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7ca248b74717547f87e62b7ab6d337cbc56dabe76550804a20709e61a955d4e2","first_computed_at":"2026-07-05T10:16:39.607339Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:16:39.607339Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"vSSCly2uawuw3WzDUQ0vcbuCEXBctFQ4WC+6xv2mWzqEl165luykIBk3xfts3eS812Iy02adUIKvowLGr2RyAQ==","signature_status":"signed_v1","signed_at":"2026-07-05T10:16:39.607851Z","signed_message":"canonical_sha256_bytes"},"source_id":"2411.19135","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b1838ef86e2fca3b872cceb55ae3d5b5317fcce17183e8a8fc48365604b1a88c","sha256:d4bf378c272a6267c4bf7a1a571d2776de02a0686e912fb1cfe375894277a7e4"],"state_sha256":"e7b3229ced79a272dd7b2ec1293dde8f42a12467845943fffb66b8e35dcb8e33"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"YdNdSdhLvX+esNdTZuRnzmXCeg/xzxlPUgr5mNVT8POBGYENxImuW95bQmR4u5JHf9IZibQ2kUikhygQyn7qDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-23T01:49:59.595319Z","bundle_sha256":"0118d446d1a14dcb88334ca7226292457289356a41b2da03752acf147d05b5fc"}}