{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:6DWKWPXGIF6453UZ7AXGO7ZXMK","short_pith_number":"pith:6DWKWPXG","canonical_record":{"source":{"id":"1403.0878","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-03-04T18:13:56Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"390fb76c4b38b233fce7b6e32f46777a5bcc40d083c556ba268b4a992ae5c854","abstract_canon_sha256":"b8e37aa115c13c6e2758684b7d597e7ec12fc4e44ffd0cbca2ada12d6a98441e"},"schema_version":"1.0"},"canonical_sha256":"f0ecab3ee6417dceee99f82e677f37628fc4685936835a81f0d374435c21480c","source":{"kind":"arxiv","id":"1403.0878","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1403.0878","created_at":"2026-05-18T02:53:39Z"},{"alias_kind":"arxiv_version","alias_value":"1403.0878v1","created_at":"2026-05-18T02:53:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1403.0878","created_at":"2026-05-18T02:53:39Z"},{"alias_kind":"pith_short_12","alias_value":"6DWKWPXGIF64","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_16","alias_value":"6DWKWPXGIF6453UZ","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_8","alias_value":"6DWKWPXG","created_at":"2026-05-18T12:28:16Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:6DWKWPXGIF6453UZ7AXGO7ZXMK","target":"record","payload":{"canonical_record":{"source":{"id":"1403.0878","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-03-04T18:13:56Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"390fb76c4b38b233fce7b6e32f46777a5bcc40d083c556ba268b4a992ae5c854","abstract_canon_sha256":"b8e37aa115c13c6e2758684b7d597e7ec12fc4e44ffd0cbca2ada12d6a98441e"},"schema_version":"1.0"},"canonical_sha256":"f0ecab3ee6417dceee99f82e677f37628fc4685936835a81f0d374435c21480c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:53:39.547199Z","signature_b64":"KU9dX4rUPAmX6XZx38yUa/M23S1MIMewcOn9azA/35/ljDzvfjkm+OTseu4OkDReNyYULR6iTbdW4sbzZ0maDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f0ecab3ee6417dceee99f82e677f37628fc4685936835a81f0d374435c21480c","last_reissued_at":"2026-05-18T02:53:39.546547Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:53:39.546547Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1403.0878","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":"2026-05-18T02:53:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"NMgZBFpefUisVpE82zDeRUJmPj7FY9jF5qTQlgNWGw543V+zA6cAOHVn3eXi8MqITJSCPcka6iHhWjJAENsQBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-04T12:19:24.537642Z"},"content_sha256":"2f046b201826316914ad35e13335c602ddd91d9705d6040da32c017b47316142","schema_version":"1.0","event_id":"sha256:2f046b201826316914ad35e13335c602ddd91d9705d6040da32c017b47316142"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:6DWKWPXGIF6453UZ7AXGO7ZXMK","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Neutron in a Strong Magnetic Field: Finite Volume Effects","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","submitted_at":"2014-03-04T18:13:56Z","abstract_excerpt":"We investigate the neutron's response to magnetic fields on a torus with the aid of chiral perturbation theory, and expose effects from non-vanishing holonomies. The determination of such effects necessitates non-perturbative treatment of the magnetic field; and, to this end, a strong-field power counting is employed. Using a novel coordinate-space method, we find the neutron propagates in a coordinate-dependent effective potential that we obtain by integrating out charged pions winding around the torus. Knowledge of these finite volume effects will aid in the extraction of neutron properties "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1403.0878","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":"2026-05-18T02:53:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nrLEDtqlBu66r0c64dE1EfdXVnM0AQbTDBeaFyHNXxwI3NxRKqtN4Q3QzuiNDv4UDKt/gXQ30PS3KAcubw54Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-04T12:19:24.537976Z"},"content_sha256":"5682877e183fa1e3358e46cfd368df7bac5a7274836974f5f5db6fd174f40682","schema_version":"1.0","event_id":"sha256:5682877e183fa1e3358e46cfd368df7bac5a7274836974f5f5db6fd174f40682"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6DWKWPXGIF6453UZ7AXGO7ZXMK/bundle.json","state_url":"https://pith.science/pith/6DWKWPXGIF6453UZ7AXGO7ZXMK/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6DWKWPXGIF6453UZ7AXGO7ZXMK/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":"2026-07-04T12:19:24Z","links":{"resolver":"https://pith.science/pith/6DWKWPXGIF6453UZ7AXGO7ZXMK","bundle":"https://pith.science/pith/6DWKWPXGIF6453UZ7AXGO7ZXMK/bundle.json","state":"https://pith.science/pith/6DWKWPXGIF6453UZ7AXGO7ZXMK/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6DWKWPXGIF6453UZ7AXGO7ZXMK/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:6DWKWPXGIF6453UZ7AXGO7ZXMK","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":"b8e37aa115c13c6e2758684b7d597e7ec12fc4e44ffd0cbca2ada12d6a98441e","cross_cats_sorted":["hep-ph","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-03-04T18:13:56Z","title_canon_sha256":"390fb76c4b38b233fce7b6e32f46777a5bcc40d083c556ba268b4a992ae5c854"},"schema_version":"1.0","source":{"id":"1403.0878","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1403.0878","created_at":"2026-05-18T02:53:39Z"},{"alias_kind":"arxiv_version","alias_value":"1403.0878v1","created_at":"2026-05-18T02:53:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1403.0878","created_at":"2026-05-18T02:53:39Z"},{"alias_kind":"pith_short_12","alias_value":"6DWKWPXGIF64","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_16","alias_value":"6DWKWPXGIF6453UZ","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_8","alias_value":"6DWKWPXG","created_at":"2026-05-18T12:28:16Z"}],"graph_snapshots":[{"event_id":"sha256:5682877e183fa1e3358e46cfd368df7bac5a7274836974f5f5db6fd174f40682","target":"graph","created_at":"2026-05-18T02:53:39Z","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"},"paper":{"abstract_excerpt":"We investigate the neutron's response to magnetic fields on a torus with the aid of chiral perturbation theory, and expose effects from non-vanishing holonomies. The determination of such effects necessitates non-perturbative treatment of the magnetic field; and, to this end, a strong-field power counting is employed. Using a novel coordinate-space method, we find the neutron propagates in a coordinate-dependent effective potential that we obtain by integrating out charged pions winding around the torus. Knowledge of these finite volume effects will aid in the extraction of neutron properties ","authors_text":"Brian C. Tiburzi","cross_cats":["hep-ph","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-03-04T18:13:56Z","title":"Neutron in a Strong Magnetic Field: Finite Volume Effects"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1403.0878","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":"sha256:2f046b201826316914ad35e13335c602ddd91d9705d6040da32c017b47316142","target":"record","created_at":"2026-05-18T02:53:39Z","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":"b8e37aa115c13c6e2758684b7d597e7ec12fc4e44ffd0cbca2ada12d6a98441e","cross_cats_sorted":["hep-ph","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-03-04T18:13:56Z","title_canon_sha256":"390fb76c4b38b233fce7b6e32f46777a5bcc40d083c556ba268b4a992ae5c854"},"schema_version":"1.0","source":{"id":"1403.0878","kind":"arxiv","version":1}},"canonical_sha256":"f0ecab3ee6417dceee99f82e677f37628fc4685936835a81f0d374435c21480c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f0ecab3ee6417dceee99f82e677f37628fc4685936835a81f0d374435c21480c","first_computed_at":"2026-05-18T02:53:39.546547Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:53:39.546547Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"KU9dX4rUPAmX6XZx38yUa/M23S1MIMewcOn9azA/35/ljDzvfjkm+OTseu4OkDReNyYULR6iTbdW4sbzZ0maDw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:53:39.547199Z","signed_message":"canonical_sha256_bytes"},"source_id":"1403.0878","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2f046b201826316914ad35e13335c602ddd91d9705d6040da32c017b47316142","sha256:5682877e183fa1e3358e46cfd368df7bac5a7274836974f5f5db6fd174f40682"],"state_sha256":"9ec5b34b4b5d6ce94fac3c15ebd77cb9d4919e5a438d28438a0be4af76bbd12b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"KtX0zKVt1Kb9BV3lD+Vw2ckpiZ9Hr+US5Mc/f/JssT6GwHHZFpQMTvlocyYTEGPicxAhgika5ADzwi753uu/DA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-04T12:19:24.539864Z","bundle_sha256":"25320004000423678410dc89597725a885cd7c7e8245e9c007cd3021f7ee5941"}}