{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1996:UGETSZ4ZPWXZ4BOX5B4YOAPYRK","short_pith_number":"pith:UGETSZ4Z","schema_version":"1.0","canonical_sha256":"a1893967997daf9e05d7e8798701f88aa18bb1f52ebdf4df69294df1b8e78e6e","source":{"kind":"arxiv","id":"hep-ph/9606456","version":3},"attestation_state":"computed","paper":{"title":"Systematic 1/M Expansion for Spin 3/2 Particles","license":"","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Barry R. Holstein, Joachim Kambor, Thomas R. Hemmert","submitted_at":"1996-06-27T14:14:34Z","abstract_excerpt":"Starting from a relativistic formulation of the pion-nucleon-delta system, the most general structure of 1/M corrections for a heavy baryon chiral lagrangian including spin 3/2 resonances is given. The heavy components of relativistic nucleons and delta fields are integrated out and their contributions to the next-to-leaing order lagrangians are constructed explicitly. The effective theory obtained admits a systematic expansion in terms of soft momenta, the pion mass $m_\\pi$ and the delta-nucleon mass difference $\\Delta$. As an application, we consider neutral pion photoproduction at threshold"},"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-ph/9606456","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1996-06-27T14:14:34Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"f37fa4eb6a10faafb2312313ab9a791e846e7411c90d92e09c596a33e3ab041c","abstract_canon_sha256":"015b4beb98770797aa88425cbe13a9c6ae5466980bc86cfc3e40ac97691e296e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:01:36.892519Z","signature_b64":"Af1/DcOBZHJwM72DREeQBoGkPZvywERJzO+7hCXi7PdyRIqYxMMnSvO/i/1DI8SJth2wY69ijb5ZlRtswAItBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a1893967997daf9e05d7e8798701f88aa18bb1f52ebdf4df69294df1b8e78e6e","last_reissued_at":"2026-07-04T16:01:36.891990Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:01:36.891990Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Systematic 1/M Expansion for Spin 3/2 Particles","license":"","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Barry R. Holstein, Joachim Kambor, Thomas R. Hemmert","submitted_at":"1996-06-27T14:14:34Z","abstract_excerpt":"Starting from a relativistic formulation of the pion-nucleon-delta system, the most general structure of 1/M corrections for a heavy baryon chiral lagrangian including spin 3/2 resonances is given. The heavy components of relativistic nucleons and delta fields are integrated out and their contributions to the next-to-leaing order lagrangians are constructed explicitly. The effective theory obtained admits a systematic expansion in terms of soft momenta, the pion mass $m_\\pi$ and the delta-nucleon mass difference $\\Delta$. As an application, we consider neutral pion photoproduction at threshold"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9606456","kind":"arxiv","version":3},"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/hep-ph/9606456/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":"hep-ph/9606456","created_at":"2026-07-04T16:01:36.892046+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9606456v3","created_at":"2026-07-04T16:01:36.892046+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9606456","created_at":"2026-07-04T16:01:36.892046+00:00"},{"alias_kind":"pith_short_12","alias_value":"UGETSZ4ZPWXZ","created_at":"2026-07-04T16:01:36.892046+00:00"},{"alias_kind":"pith_short_16","alias_value":"UGETSZ4ZPWXZ4BOX","created_at":"2026-07-04T16:01:36.892046+00:00"},{"alias_kind":"pith_short_8","alias_value":"UGETSZ4Z","created_at":"2026-07-04T16:01:36.892046+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2606.30834","citing_title":"Extraction of the nucleon axial form factor from Lattice QCD using NNLO chiral perturbation theory","ref_index":27,"is_internal_anchor":true},{"citing_arxiv_id":"2604.12535","citing_title":"Neutrinoless double-beta decay of the $\\Delta^-$ resonance","ref_index":74,"is_internal_anchor":false},{"citing_arxiv_id":"2604.09149","citing_title":"Classical and spin polarizabilities of singly heavy baryons within heavy baryon chiral perturbation theory","ref_index":88,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/UGETSZ4ZPWXZ4BOX5B4YOAPYRK","json":"https://pith.science/pith/UGETSZ4ZPWXZ4BOX5B4YOAPYRK.json","graph_json":"https://pith.science/api/pith-number/UGETSZ4ZPWXZ4BOX5B4YOAPYRK/graph.json","events_json":"https://pith.science/api/pith-number/UGETSZ4ZPWXZ4BOX5B4YOAPYRK/events.json","paper":"https://pith.science/paper/UGETSZ4Z"},"agent_actions":{"view_html":"https://pith.science/pith/UGETSZ4ZPWXZ4BOX5B4YOAPYRK","download_json":"https://pith.science/pith/UGETSZ4ZPWXZ4BOX5B4YOAPYRK.json","view_paper":"https://pith.science/paper/UGETSZ4Z","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9606456&json=true","fetch_graph":"https://pith.science/api/pith-number/UGETSZ4ZPWXZ4BOX5B4YOAPYRK/graph.json","fetch_events":"https://pith.science/api/pith-number/UGETSZ4ZPWXZ4BOX5B4YOAPYRK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UGETSZ4ZPWXZ4BOX5B4YOAPYRK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UGETSZ4ZPWXZ4BOX5B4YOAPYRK/action/storage_attestation","attest_author":"https://pith.science/pith/UGETSZ4ZPWXZ4BOX5B4YOAPYRK/action/author_attestation","sign_citation":"https://pith.science/pith/UGETSZ4ZPWXZ4BOX5B4YOAPYRK/action/citation_signature","submit_replication":"https://pith.science/pith/UGETSZ4ZPWXZ4BOX5B4YOAPYRK/action/replication_record"}},"created_at":"2026-07-04T16:01:36.892046+00:00","updated_at":"2026-07-04T16:01:36.892046+00:00"}