{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2003:LL5NEJWK2U7AVJ7YIHFDQTHRJH","short_pith_number":"pith:LL5NEJWK","schema_version":"1.0","canonical_sha256":"5afad226cad53e0aa7f841ca384cf149e5a1a7f246a1ffddcc5855c501502c5b","source":{"kind":"arxiv","id":"hep-th/0306153","version":2},"attestation_state":"computed","paper":{"title":"Hamiltonian N=2 Superfield Quantization","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"I.A. Batalin, P.H. Damgaard","submitted_at":"2003-06-17T08:04:06Z","abstract_excerpt":"We present a superfield construction of Hamiltonian quantization with N=2 supersymmetry generated by two fermionic charges Q^a. As a byproduct of the analysis we also derive a classically localized path integral from two fermionic objects \\Sigma^a that can be viewed as ``square roots'' of the classical bosonic action under the product of a functional Poisson bracket."},"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":"hep-th/0306153","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2003-06-17T08:04:06Z","cross_cats_sorted":[],"title_canon_sha256":"c0336e3908ae4799ea3e583ec20925422310febacd6f54ee304fe5b3459b0c0a","abstract_canon_sha256":"db29d0d3ece46041a36cb865e9411b266ff7ee8836df2a48ca3778d0f7a60234"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:38:47.045831Z","signature_b64":"RAc0S+rL4UngPq2RfaMrd9Hka8Z/G0hqM1OdHN/bhyi/3iwLywDdwjpu5FLQTSLOs8Bafpi7KZwwemCiDH8+DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5afad226cad53e0aa7f841ca384cf149e5a1a7f246a1ffddcc5855c501502c5b","last_reissued_at":"2026-05-18T01:38:47.045391Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:38:47.045391Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Hamiltonian N=2 Superfield Quantization","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"I.A. Batalin, P.H. Damgaard","submitted_at":"2003-06-17T08:04:06Z","abstract_excerpt":"We present a superfield construction of Hamiltonian quantization with N=2 supersymmetry generated by two fermionic charges Q^a. As a byproduct of the analysis we also derive a classically localized path integral from two fermionic objects \\Sigma^a that can be viewed as ``square roots'' of the classical bosonic action under the product of a functional Poisson bracket."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0306153","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0306153","created_at":"2026-05-18T01:38:47.045463+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0306153v2","created_at":"2026-05-18T01:38:47.045463+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0306153","created_at":"2026-05-18T01:38:47.045463+00:00"},{"alias_kind":"pith_short_12","alias_value":"LL5NEJWK2U7A","created_at":"2026-05-18T12:25:52.051335+00:00"},{"alias_kind":"pith_short_16","alias_value":"LL5NEJWK2U7AVJ7Y","created_at":"2026-05-18T12:25:52.051335+00:00"},{"alias_kind":"pith_short_8","alias_value":"LL5NEJWK","created_at":"2026-05-18T12:25:52.051335+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/LL5NEJWK2U7AVJ7YIHFDQTHRJH","json":"https://pith.science/pith/LL5NEJWK2U7AVJ7YIHFDQTHRJH.json","graph_json":"https://pith.science/api/pith-number/LL5NEJWK2U7AVJ7YIHFDQTHRJH/graph.json","events_json":"https://pith.science/api/pith-number/LL5NEJWK2U7AVJ7YIHFDQTHRJH/events.json","paper":"https://pith.science/paper/LL5NEJWK"},"agent_actions":{"view_html":"https://pith.science/pith/LL5NEJWK2U7AVJ7YIHFDQTHRJH","download_json":"https://pith.science/pith/LL5NEJWK2U7AVJ7YIHFDQTHRJH.json","view_paper":"https://pith.science/paper/LL5NEJWK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0306153&json=true","fetch_graph":"https://pith.science/api/pith-number/LL5NEJWK2U7AVJ7YIHFDQTHRJH/graph.json","fetch_events":"https://pith.science/api/pith-number/LL5NEJWK2U7AVJ7YIHFDQTHRJH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LL5NEJWK2U7AVJ7YIHFDQTHRJH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LL5NEJWK2U7AVJ7YIHFDQTHRJH/action/storage_attestation","attest_author":"https://pith.science/pith/LL5NEJWK2U7AVJ7YIHFDQTHRJH/action/author_attestation","sign_citation":"https://pith.science/pith/LL5NEJWK2U7AVJ7YIHFDQTHRJH/action/citation_signature","submit_replication":"https://pith.science/pith/LL5NEJWK2U7AVJ7YIHFDQTHRJH/action/replication_record"}},"created_at":"2026-05-18T01:38:47.045463+00:00","updated_at":"2026-05-18T01:38:47.045463+00:00"}