{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:EB5FL2X6JFP5R2QVDNTHFDOWA7","short_pith_number":"pith:EB5FL2X6","canonical_record":{"source":{"id":"1407.8159","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-07-30T19:06:08Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"297034c587a6036aebdb9d27934a88ddbffc4871b2ee38391359da81739c7eb2","abstract_canon_sha256":"601f03e4822a1fea9badbe9934a9d3fb4365825b01d03916e843e34fb39bb1c3"},"schema_version":"1.0"},"canonical_sha256":"207a55eafe495fd8ea151b66728dd607c21b358434062b2bed3193d2664c8279","source":{"kind":"arxiv","id":"1407.8159","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1407.8159","created_at":"2026-05-18T02:38:43Z"},{"alias_kind":"arxiv_version","alias_value":"1407.8159v2","created_at":"2026-05-18T02:38:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.8159","created_at":"2026-05-18T02:38:43Z"},{"alias_kind":"pith_short_12","alias_value":"EB5FL2X6JFP5","created_at":"2026-05-18T12:28:25Z"},{"alias_kind":"pith_short_16","alias_value":"EB5FL2X6JFP5R2QV","created_at":"2026-05-18T12:28:25Z"},{"alias_kind":"pith_short_8","alias_value":"EB5FL2X6","created_at":"2026-05-18T12:28:25Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:EB5FL2X6JFP5R2QVDNTHFDOWA7","target":"record","payload":{"canonical_record":{"source":{"id":"1407.8159","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-07-30T19:06:08Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"297034c587a6036aebdb9d27934a88ddbffc4871b2ee38391359da81739c7eb2","abstract_canon_sha256":"601f03e4822a1fea9badbe9934a9d3fb4365825b01d03916e843e34fb39bb1c3"},"schema_version":"1.0"},"canonical_sha256":"207a55eafe495fd8ea151b66728dd607c21b358434062b2bed3193d2664c8279","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:38:43.770379Z","signature_b64":"pbG3jG14W3X9HUa6Iq0DQY0mS60bkrnIj9dUhaKhrR0sgRqIi/omxjQLrpjhKPvBH5LmVXK9sxDdpXbxOkd1Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"207a55eafe495fd8ea151b66728dd607c21b358434062b2bed3193d2664c8279","last_reissued_at":"2026-05-18T02:38:43.769963Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:38:43.769963Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1407.8159","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":"2026-05-18T02:38:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"NMJ1/5Zqr0C5ftB0YPjh3+rGRACx7wBnKAgDvV2LbAb4Q3iy2pBZG81GDvs8YwdFL8u83esR4whm73o9S0aFCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T22:52:04.131880Z"},"content_sha256":"bd90e86dc096991bd4894f17479099d11422b1ffce99c4cd88143558bf984f07","schema_version":"1.0","event_id":"sha256:bd90e86dc096991bd4894f17479099d11422b1ffce99c4cd88143558bf984f07"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:EB5FL2X6JFP5R2QVDNTHFDOWA7","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Reconciling the lattice background field method with nonrelativistic QED: Spinor case","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"Brian C. Tiburzi, Jong-Wan Lee","submitted_at":"2014-07-30T19:06:08Z","abstract_excerpt":"We show that inconsistency between background field methods, which are relevant for lattice QCD spectroscopy, and effective field theory matching conditions, which are obtained from scattering amplitudes, can be resolved by augmenting nonrelativistic QED with operators related by the equations of motion. To determine the coefficients of such operators, we perform the nonrelativistic expansion of QED for a spin-half hadron including non-minimal electromagnetic couplings. As an effective field theory framework could provide a valuable tool to analyze lattice QCD correlation functions in external"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.8159","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":""},"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":"2026-05-18T02:38:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8LsZXCGPqN6w8ku3yQEs7Dc6j4GXTk8ASL7LY957UoACo+3lxsw1Unb1fJeSVr2NLBcl1xyrbe2Nm+bJ3a1dBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T22:52:04.132328Z"},"content_sha256":"78331a097d7ceec33102f32e555980a56addfece928c4a1ef7ca2d19f419c58d","schema_version":"1.0","event_id":"sha256:78331a097d7ceec33102f32e555980a56addfece928c4a1ef7ca2d19f419c58d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/EB5FL2X6JFP5R2QVDNTHFDOWA7/bundle.json","state_url":"https://pith.science/pith/EB5FL2X6JFP5R2QVDNTHFDOWA7/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/EB5FL2X6JFP5R2QVDNTHFDOWA7/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":"2026-05-28T22:52:04Z","links":{"resolver":"https://pith.science/pith/EB5FL2X6JFP5R2QVDNTHFDOWA7","bundle":"https://pith.science/pith/EB5FL2X6JFP5R2QVDNTHFDOWA7/bundle.json","state":"https://pith.science/pith/EB5FL2X6JFP5R2QVDNTHFDOWA7/state.json","well_known_bundle":"https://pith.science/.well-known/pith/EB5FL2X6JFP5R2QVDNTHFDOWA7/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:EB5FL2X6JFP5R2QVDNTHFDOWA7","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":"601f03e4822a1fea9badbe9934a9d3fb4365825b01d03916e843e34fb39bb1c3","cross_cats_sorted":["hep-ph","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-07-30T19:06:08Z","title_canon_sha256":"297034c587a6036aebdb9d27934a88ddbffc4871b2ee38391359da81739c7eb2"},"schema_version":"1.0","source":{"id":"1407.8159","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1407.8159","created_at":"2026-05-18T02:38:43Z"},{"alias_kind":"arxiv_version","alias_value":"1407.8159v2","created_at":"2026-05-18T02:38:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.8159","created_at":"2026-05-18T02:38:43Z"},{"alias_kind":"pith_short_12","alias_value":"EB5FL2X6JFP5","created_at":"2026-05-18T12:28:25Z"},{"alias_kind":"pith_short_16","alias_value":"EB5FL2X6JFP5R2QV","created_at":"2026-05-18T12:28:25Z"},{"alias_kind":"pith_short_8","alias_value":"EB5FL2X6","created_at":"2026-05-18T12:28:25Z"}],"graph_snapshots":[{"event_id":"sha256:78331a097d7ceec33102f32e555980a56addfece928c4a1ef7ca2d19f419c58d","target":"graph","created_at":"2026-05-18T02:38:43Z","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":"We show that inconsistency between background field methods, which are relevant for lattice QCD spectroscopy, and effective field theory matching conditions, which are obtained from scattering amplitudes, can be resolved by augmenting nonrelativistic QED with operators related by the equations of motion. To determine the coefficients of such operators, we perform the nonrelativistic expansion of QED for a spin-half hadron including non-minimal electromagnetic couplings. As an effective field theory framework could provide a valuable tool to analyze lattice QCD correlation functions in external","authors_text":"Brian C. Tiburzi, Jong-Wan Lee","cross_cats":["hep-ph","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-07-30T19:06:08Z","title":"Reconciling the lattice background field method with nonrelativistic QED: Spinor case"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.8159","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:bd90e86dc096991bd4894f17479099d11422b1ffce99c4cd88143558bf984f07","target":"record","created_at":"2026-05-18T02:38:43Z","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":"601f03e4822a1fea9badbe9934a9d3fb4365825b01d03916e843e34fb39bb1c3","cross_cats_sorted":["hep-ph","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-07-30T19:06:08Z","title_canon_sha256":"297034c587a6036aebdb9d27934a88ddbffc4871b2ee38391359da81739c7eb2"},"schema_version":"1.0","source":{"id":"1407.8159","kind":"arxiv","version":2}},"canonical_sha256":"207a55eafe495fd8ea151b66728dd607c21b358434062b2bed3193d2664c8279","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"207a55eafe495fd8ea151b66728dd607c21b358434062b2bed3193d2664c8279","first_computed_at":"2026-05-18T02:38:43.769963Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:38:43.769963Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"pbG3jG14W3X9HUa6Iq0DQY0mS60bkrnIj9dUhaKhrR0sgRqIi/omxjQLrpjhKPvBH5LmVXK9sxDdpXbxOkd1Ag==","signature_status":"signed_v1","signed_at":"2026-05-18T02:38:43.770379Z","signed_message":"canonical_sha256_bytes"},"source_id":"1407.8159","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:bd90e86dc096991bd4894f17479099d11422b1ffce99c4cd88143558bf984f07","sha256:78331a097d7ceec33102f32e555980a56addfece928c4a1ef7ca2d19f419c58d"],"state_sha256":"3523bbb52c660c1ee382b9759caafa08de47542af1491788d477c21cf9ed4eb1"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"TiSau8wqSokOe+ipUwrGYjlZDXED+Zn2dWxHha8OSarufKzSWNhF+5wdfwq1RZ7Pt6/3HOWmHDy18xQrYs8KCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T22:52:04.136577Z","bundle_sha256":"cfbb65befb689e28110c03c3d980317405f9d5479e564af4a47212a55c9682ec"}}