{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:KMB6W5WC54TGTP7VNFXBFVRKPG","short_pith_number":"pith:KMB6W5WC","schema_version":"1.0","canonical_sha256":"5303eb76c2ef2669bff5696e12d62a798e4778eaf97315235cca21c27fb49fe2","source":{"kind":"arxiv","id":"2504.20786","version":2},"attestation_state":"computed","paper":{"title":"Power corrections to the heavy electron form factor","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Aniruddha Venkata","submitted_at":"2025-04-29T14:02:02Z","abstract_excerpt":"We study the first power correction to the heavy electron form factor in QED and show that it factorizes as a derivative operator. We discuss the result in QED with no light fermions, where the first power correction can be written explicitly in terms of one-loop integrals and the anomalous magnetic moment. In the presence of light fermions, the heavy electron form factor admits a representation as a sum over matrix elements, each of which receives corrections from higher orders in perturbation theory. From this analysis, we are able to extract the next-to-leading power soft photon theorem in "},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2504.20786","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-04-29T14:02:02Z","cross_cats_sorted":[],"title_canon_sha256":"7c4906c0b1eb18c1db3a60aa88f24b7be684f1a6afe5d55732737f3853ff571c","abstract_canon_sha256":"fe4ade647fa0cec0d9610e2e6fae39e51c44936224ec13ecfa22bb3d96c83cd8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:54:30.547211Z","signature_b64":"tEAIg19Rw8SsJJCQ0H74DKWBJMPAq4RPWjbytlRoaqNaLG/8qy4uHInJY3q7VwI0PpZgXOl16cGYFugvZTuGBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5303eb76c2ef2669bff5696e12d62a798e4778eaf97315235cca21c27fb49fe2","last_reissued_at":"2026-07-05T11:54:30.546620Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:54:30.546620Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Power corrections to the heavy electron form factor","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Aniruddha Venkata","submitted_at":"2025-04-29T14:02:02Z","abstract_excerpt":"We study the first power correction to the heavy electron form factor in QED and show that it factorizes as a derivative operator. We discuss the result in QED with no light fermions, where the first power correction can be written explicitly in terms of one-loop integrals and the anomalous magnetic moment. In the presence of light fermions, the heavy electron form factor admits a representation as a sum over matrix elements, each of which receives corrections from higher orders in perturbation theory. From this analysis, we are able to extract the next-to-leading power soft photon theorem in "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2504.20786","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2504.20786/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"},"aliases":[{"alias_kind":"arxiv","alias_value":"2504.20786","created_at":"2026-07-05T11:54:30.546683+00:00"},{"alias_kind":"arxiv_version","alias_value":"2504.20786v2","created_at":"2026-07-05T11:54:30.546683+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2504.20786","created_at":"2026-07-05T11:54:30.546683+00:00"},{"alias_kind":"pith_short_12","alias_value":"KMB6W5WC54TG","created_at":"2026-07-05T11:54:30.546683+00:00"},{"alias_kind":"pith_short_16","alias_value":"KMB6W5WC54TGTP7V","created_at":"2026-07-05T11:54:30.546683+00:00"},{"alias_kind":"pith_short_8","alias_value":"KMB6W5WC","created_at":"2026-07-05T11:54:30.546683+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/KMB6W5WC54TGTP7VNFXBFVRKPG","json":"https://pith.science/pith/KMB6W5WC54TGTP7VNFXBFVRKPG.json","graph_json":"https://pith.science/api/pith-number/KMB6W5WC54TGTP7VNFXBFVRKPG/graph.json","events_json":"https://pith.science/api/pith-number/KMB6W5WC54TGTP7VNFXBFVRKPG/events.json","paper":"https://pith.science/paper/KMB6W5WC"},"agent_actions":{"view_html":"https://pith.science/pith/KMB6W5WC54TGTP7VNFXBFVRKPG","download_json":"https://pith.science/pith/KMB6W5WC54TGTP7VNFXBFVRKPG.json","view_paper":"https://pith.science/paper/KMB6W5WC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2504.20786&json=true","fetch_graph":"https://pith.science/api/pith-number/KMB6W5WC54TGTP7VNFXBFVRKPG/graph.json","fetch_events":"https://pith.science/api/pith-number/KMB6W5WC54TGTP7VNFXBFVRKPG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KMB6W5WC54TGTP7VNFXBFVRKPG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KMB6W5WC54TGTP7VNFXBFVRKPG/action/storage_attestation","attest_author":"https://pith.science/pith/KMB6W5WC54TGTP7VNFXBFVRKPG/action/author_attestation","sign_citation":"https://pith.science/pith/KMB6W5WC54TGTP7VNFXBFVRKPG/action/citation_signature","submit_replication":"https://pith.science/pith/KMB6W5WC54TGTP7VNFXBFVRKPG/action/replication_record"}},"created_at":"2026-07-05T11:54:30.546683+00:00","updated_at":"2026-07-05T11:54:30.546683+00:00"}