{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:RQHO2AJIWIJY73M3POL6XVIM6V","short_pith_number":"pith:RQHO2AJI","schema_version":"1.0","canonical_sha256":"8c0eed0128b2138fed9b7b97ebd50cf551ae5f280138f842a5e0a9bca2543bdf","source":{"kind":"arxiv","id":"1211.0743","version":1},"attestation_state":"computed","paper":{"title":"Pion form factors in the epsilon regime","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"H. Matsufuru, JLQCD collaboration: H. Fukaya, J. Noaki, N. Yamada, S. Aoki, S. Hashimoto, T. Kaneko, T. Onogi","submitted_at":"2012-11-05T02:24:59Z","abstract_excerpt":"We consider how to extract the pion form factors in the epsilon regime. Using the correlators with non-zero momenta and taking appropriate ratios of them, we eliminate the dominant finite volume effect from the zero-momentum pion mode. Our preliminary lattice result for the pion charge radius is consistent with the experiment."},"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":"1211.0743","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-11-05T02:24:59Z","cross_cats_sorted":[],"title_canon_sha256":"163489912881b81c26b5eb45e17deecb7efd8428503bb348ddf694629bf4b074","abstract_canon_sha256":"d5c712673607394e0f1688f47a69a83a8c57c9ca26bac3a73c024c6439879b55"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:41:31.665554Z","signature_b64":"7kZT55vAMUnT6glZGrFUIXxnj2qT05tWhv27/xPQWa1dyDPCdRm2BEbnQMtxCbdI3R42BIAqmAdKHkq0Q+t6Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8c0eed0128b2138fed9b7b97ebd50cf551ae5f280138f842a5e0a9bca2543bdf","last_reissued_at":"2026-05-18T03:41:31.665087Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:41:31.665087Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Pion form factors in the epsilon regime","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"H. Matsufuru, JLQCD collaboration: H. Fukaya, J. Noaki, N. Yamada, S. Aoki, S. Hashimoto, T. Kaneko, T. Onogi","submitted_at":"2012-11-05T02:24:59Z","abstract_excerpt":"We consider how to extract the pion form factors in the epsilon regime. Using the correlators with non-zero momenta and taking appropriate ratios of them, we eliminate the dominant finite volume effect from the zero-momentum pion mode. Our preliminary lattice result for the pion charge radius is consistent with the experiment."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1211.0743","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1211.0743","created_at":"2026-05-18T03:41:31.665156+00:00"},{"alias_kind":"arxiv_version","alias_value":"1211.0743v1","created_at":"2026-05-18T03:41:31.665156+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1211.0743","created_at":"2026-05-18T03:41:31.665156+00:00"},{"alias_kind":"pith_short_12","alias_value":"RQHO2AJIWIJY","created_at":"2026-05-18T12:27:20.899486+00:00"},{"alias_kind":"pith_short_16","alias_value":"RQHO2AJIWIJY73M3","created_at":"2026-05-18T12:27:20.899486+00:00"},{"alias_kind":"pith_short_8","alias_value":"RQHO2AJI","created_at":"2026-05-18T12:27:20.899486+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/RQHO2AJIWIJY73M3POL6XVIM6V","json":"https://pith.science/pith/RQHO2AJIWIJY73M3POL6XVIM6V.json","graph_json":"https://pith.science/api/pith-number/RQHO2AJIWIJY73M3POL6XVIM6V/graph.json","events_json":"https://pith.science/api/pith-number/RQHO2AJIWIJY73M3POL6XVIM6V/events.json","paper":"https://pith.science/paper/RQHO2AJI"},"agent_actions":{"view_html":"https://pith.science/pith/RQHO2AJIWIJY73M3POL6XVIM6V","download_json":"https://pith.science/pith/RQHO2AJIWIJY73M3POL6XVIM6V.json","view_paper":"https://pith.science/paper/RQHO2AJI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1211.0743&json=true","fetch_graph":"https://pith.science/api/pith-number/RQHO2AJIWIJY73M3POL6XVIM6V/graph.json","fetch_events":"https://pith.science/api/pith-number/RQHO2AJIWIJY73M3POL6XVIM6V/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RQHO2AJIWIJY73M3POL6XVIM6V/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RQHO2AJIWIJY73M3POL6XVIM6V/action/storage_attestation","attest_author":"https://pith.science/pith/RQHO2AJIWIJY73M3POL6XVIM6V/action/author_attestation","sign_citation":"https://pith.science/pith/RQHO2AJIWIJY73M3POL6XVIM6V/action/citation_signature","submit_replication":"https://pith.science/pith/RQHO2AJIWIJY73M3POL6XVIM6V/action/replication_record"}},"created_at":"2026-05-18T03:41:31.665156+00:00","updated_at":"2026-05-18T03:41:31.665156+00:00"}