{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:2F4PTLYEWCQX7U2A5ZMJKNSAXI","short_pith_number":"pith:2F4PTLYE","schema_version":"1.0","canonical_sha256":"d178f9af04b0a17fd340ee58953640ba04b7ebb7997115c604120b01b6476be0","source":{"kind":"arxiv","id":"1603.08881","version":1},"attestation_state":"computed","paper":{"title":"Light-front representation of chiral dynamics with Delta isobar and large-N_c relations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"C. Granados, C. Weiss","submitted_at":"2016-03-29T18:46:04Z","abstract_excerpt":"Transverse densities describe the spatial distribution of electromagnetic current in the nucleon at fixed light-front time. At peripheral distances b = O(M_pi^{-1}) the densities are governed by chiral dynamics and can be calculated model-independently using chiral effective field theory (EFT). Recent work has shown that the EFT results can be represented in first-quantized form, as overlap integrals of chiral light-front wave functions describing the transition of the nucleon to soft-pion-nucleon intermediate states, resulting in a quantum-mechanical picture of the peripheral transverse densi"},"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":"1603.08881","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-03-29T18:46:04Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"26cb954340e7422f8e0f553c54e3546285764abfd6d1c38c8e03aa46b4fb1348","abstract_canon_sha256":"d61d8035fe237288bae5ebd4f1e7812b188ad467a66af371b393979c23fed6ea"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:11:44.647103Z","signature_b64":"NPIlZHxpUbvy6s/MDOaMM90h3of0paalz98vW6YheNE2lcDt097guuK8bv4HYVc8RWfu1EGjhQ9vjuJ8yCW5Bg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d178f9af04b0a17fd340ee58953640ba04b7ebb7997115c604120b01b6476be0","last_reissued_at":"2026-05-18T01:11:44.646770Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:11:44.646770Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Light-front representation of chiral dynamics with Delta isobar and large-N_c relations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"C. Granados, C. Weiss","submitted_at":"2016-03-29T18:46:04Z","abstract_excerpt":"Transverse densities describe the spatial distribution of electromagnetic current in the nucleon at fixed light-front time. At peripheral distances b = O(M_pi^{-1}) the densities are governed by chiral dynamics and can be calculated model-independently using chiral effective field theory (EFT). Recent work has shown that the EFT results can be represented in first-quantized form, as overlap integrals of chiral light-front wave functions describing the transition of the nucleon to soft-pion-nucleon intermediate states, resulting in a quantum-mechanical picture of the peripheral transverse densi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1603.08881","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":"1603.08881","created_at":"2026-05-18T01:11:44.646824+00:00"},{"alias_kind":"arxiv_version","alias_value":"1603.08881v1","created_at":"2026-05-18T01:11:44.646824+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1603.08881","created_at":"2026-05-18T01:11:44.646824+00:00"},{"alias_kind":"pith_short_12","alias_value":"2F4PTLYEWCQX","created_at":"2026-05-18T12:29:55.572404+00:00"},{"alias_kind":"pith_short_16","alias_value":"2F4PTLYEWCQX7U2A","created_at":"2026-05-18T12:29:55.572404+00:00"},{"alias_kind":"pith_short_8","alias_value":"2F4PTLYE","created_at":"2026-05-18T12:29:55.572404+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/2F4PTLYEWCQX7U2A5ZMJKNSAXI","json":"https://pith.science/pith/2F4PTLYEWCQX7U2A5ZMJKNSAXI.json","graph_json":"https://pith.science/api/pith-number/2F4PTLYEWCQX7U2A5ZMJKNSAXI/graph.json","events_json":"https://pith.science/api/pith-number/2F4PTLYEWCQX7U2A5ZMJKNSAXI/events.json","paper":"https://pith.science/paper/2F4PTLYE"},"agent_actions":{"view_html":"https://pith.science/pith/2F4PTLYEWCQX7U2A5ZMJKNSAXI","download_json":"https://pith.science/pith/2F4PTLYEWCQX7U2A5ZMJKNSAXI.json","view_paper":"https://pith.science/paper/2F4PTLYE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1603.08881&json=true","fetch_graph":"https://pith.science/api/pith-number/2F4PTLYEWCQX7U2A5ZMJKNSAXI/graph.json","fetch_events":"https://pith.science/api/pith-number/2F4PTLYEWCQX7U2A5ZMJKNSAXI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2F4PTLYEWCQX7U2A5ZMJKNSAXI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2F4PTLYEWCQX7U2A5ZMJKNSAXI/action/storage_attestation","attest_author":"https://pith.science/pith/2F4PTLYEWCQX7U2A5ZMJKNSAXI/action/author_attestation","sign_citation":"https://pith.science/pith/2F4PTLYEWCQX7U2A5ZMJKNSAXI/action/citation_signature","submit_replication":"https://pith.science/pith/2F4PTLYEWCQX7U2A5ZMJKNSAXI/action/replication_record"}},"created_at":"2026-05-18T01:11:44.646824+00:00","updated_at":"2026-05-18T01:11:44.646824+00:00"}