{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:VBTQOXUJBL574TMF4GJZMY3U5T","short_pith_number":"pith:VBTQOXUJ","schema_version":"1.0","canonical_sha256":"a867075e890afbfe4d85e193966374ecc0f12090a78b6ed182b56eab89e0fbdd","source":{"kind":"arxiv","id":"1412.5311","version":1},"attestation_state":"computed","paper":{"title":"Instantaneous stochastic perturbation theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Martin L\\\"uscher","submitted_at":"2014-12-17T09:58:09Z","abstract_excerpt":"A form of stochastic perturbation theory is described, where the representative stochastic fields are generated instantaneously rather than through a Markov process. The correctness of the procedure is established to all orders of the expansion and for a wide class of field theories that includes all common formulations of lattice QCD."},"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":"1412.5311","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-12-17T09:58:09Z","cross_cats_sorted":[],"title_canon_sha256":"f2c0339931af4a3afe43ea9982961f79b4c6f8ed50e10cef99bc88834cbcae74","abstract_canon_sha256":"7ad2f2b18211ac135b31bacf719aa019665715547f3c8ba152b0c5472fa96504"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:04:07.878003Z","signature_b64":"QEwSWPs1izAAgtWjoP9PwwJdKC2MyhH+2POheJPiaFq3VYDxG545ZdORulVG+HvXoNiRMjbLH7XuLb2FjY2oAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a867075e890afbfe4d85e193966374ecc0f12090a78b6ed182b56eab89e0fbdd","last_reissued_at":"2026-05-18T02:04:07.877448Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:04:07.877448Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Instantaneous stochastic perturbation theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Martin L\\\"uscher","submitted_at":"2014-12-17T09:58:09Z","abstract_excerpt":"A form of stochastic perturbation theory is described, where the representative stochastic fields are generated instantaneously rather than through a Markov process. The correctness of the procedure is established to all orders of the expansion and for a wide class of field theories that includes all common formulations of lattice QCD."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.5311","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":"1412.5311","created_at":"2026-05-18T02:04:07.877527+00:00"},{"alias_kind":"arxiv_version","alias_value":"1412.5311v1","created_at":"2026-05-18T02:04:07.877527+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.5311","created_at":"2026-05-18T02:04:07.877527+00:00"},{"alias_kind":"pith_short_12","alias_value":"VBTQOXUJBL57","created_at":"2026-05-18T12:28:52.271510+00:00"},{"alias_kind":"pith_short_16","alias_value":"VBTQOXUJBL574TMF","created_at":"2026-05-18T12:28:52.271510+00:00"},{"alias_kind":"pith_short_8","alias_value":"VBTQOXUJ","created_at":"2026-05-18T12:28:52.271510+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/VBTQOXUJBL574TMF4GJZMY3U5T","json":"https://pith.science/pith/VBTQOXUJBL574TMF4GJZMY3U5T.json","graph_json":"https://pith.science/api/pith-number/VBTQOXUJBL574TMF4GJZMY3U5T/graph.json","events_json":"https://pith.science/api/pith-number/VBTQOXUJBL574TMF4GJZMY3U5T/events.json","paper":"https://pith.science/paper/VBTQOXUJ"},"agent_actions":{"view_html":"https://pith.science/pith/VBTQOXUJBL574TMF4GJZMY3U5T","download_json":"https://pith.science/pith/VBTQOXUJBL574TMF4GJZMY3U5T.json","view_paper":"https://pith.science/paper/VBTQOXUJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1412.5311&json=true","fetch_graph":"https://pith.science/api/pith-number/VBTQOXUJBL574TMF4GJZMY3U5T/graph.json","fetch_events":"https://pith.science/api/pith-number/VBTQOXUJBL574TMF4GJZMY3U5T/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VBTQOXUJBL574TMF4GJZMY3U5T/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VBTQOXUJBL574TMF4GJZMY3U5T/action/storage_attestation","attest_author":"https://pith.science/pith/VBTQOXUJBL574TMF4GJZMY3U5T/action/author_attestation","sign_citation":"https://pith.science/pith/VBTQOXUJBL574TMF4GJZMY3U5T/action/citation_signature","submit_replication":"https://pith.science/pith/VBTQOXUJBL574TMF4GJZMY3U5T/action/replication_record"}},"created_at":"2026-05-18T02:04:07.877527+00:00","updated_at":"2026-05-18T02:04:07.877527+00:00"}