{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:2PAMK6GFL2GH4TVAEF3CALR5M4","short_pith_number":"pith:2PAMK6GF","schema_version":"1.0","canonical_sha256":"d3c0c578c55e8c7e4ea02176202e3d671b59556007e2289b27087507d8e24ec5","source":{"kind":"arxiv","id":"1705.07548","version":2},"attestation_state":"computed","paper":{"title":"$K^+$-nucleus elastic scattering revisited from perspective of partial restoration of chiral symmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Daisuke Jido, Kenji Aoki","submitted_at":"2017-05-22T04:04:18Z","abstract_excerpt":"The $K^{+}$ meson properties in the nuclear medium are investigated by considering the wavefunction renormalization as a first step to reveal the in-medium properties of the $K^{+}$ meson in the context of partial restoration of chiral symmetry. The $K^{+}N$ elastic scattering amplitude is constructed using chiral perturbation theory up to the next-to-leading order. Using the constructed amplitude, we calculate the wavefunction renormalization in the Thomas-Fermi approximation. We obtained a good description of the $K^{+}N$ elastic scattering amplitude. The obtained wavefunction renormalizatio"},"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":"1705.07548","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-05-22T04:04:18Z","cross_cats_sorted":[],"title_canon_sha256":"724580b75affa86bf9bb373aca135ffe0b8682fd386a556efa50535bf204ab4b","abstract_canon_sha256":"e76f0bcd77902122aa5d0a9fc261dcb473c2dbecba03ab497391f7adbd39c7da"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:32:36.198352Z","signature_b64":"WnSRvsuA+XeYBkgNEJMY0qNT3TbBd7aq/463zylhiFIjwcdyRtjOynr+QbaeW+RQsp7zhl5UD41kFmYEG0RwDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d3c0c578c55e8c7e4ea02176202e3d671b59556007e2289b27087507d8e24ec5","last_reissued_at":"2026-05-18T00:32:36.197693Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:32:36.197693Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"$K^+$-nucleus elastic scattering revisited from perspective of partial restoration of chiral symmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Daisuke Jido, Kenji Aoki","submitted_at":"2017-05-22T04:04:18Z","abstract_excerpt":"The $K^{+}$ meson properties in the nuclear medium are investigated by considering the wavefunction renormalization as a first step to reveal the in-medium properties of the $K^{+}$ meson in the context of partial restoration of chiral symmetry. The $K^{+}N$ elastic scattering amplitude is constructed using chiral perturbation theory up to the next-to-leading order. Using the constructed amplitude, we calculate the wavefunction renormalization in the Thomas-Fermi approximation. We obtained a good description of the $K^{+}N$ elastic scattering amplitude. The obtained wavefunction renormalizatio"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.07548","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":"1705.07548","created_at":"2026-05-18T00:32:36.197794+00:00"},{"alias_kind":"arxiv_version","alias_value":"1705.07548v2","created_at":"2026-05-18T00:32:36.197794+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.07548","created_at":"2026-05-18T00:32:36.197794+00:00"},{"alias_kind":"pith_short_12","alias_value":"2PAMK6GFL2GH","created_at":"2026-05-18T12:30:55.937587+00:00"},{"alias_kind":"pith_short_16","alias_value":"2PAMK6GFL2GH4TVA","created_at":"2026-05-18T12:30:55.937587+00:00"},{"alias_kind":"pith_short_8","alias_value":"2PAMK6GF","created_at":"2026-05-18T12:30:55.937587+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2512.24721","citing_title":"$S$-wave $KN$ scattering in a renormalizable chiral effective field theory","ref_index":8,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/2PAMK6GFL2GH4TVAEF3CALR5M4","json":"https://pith.science/pith/2PAMK6GFL2GH4TVAEF3CALR5M4.json","graph_json":"https://pith.science/api/pith-number/2PAMK6GFL2GH4TVAEF3CALR5M4/graph.json","events_json":"https://pith.science/api/pith-number/2PAMK6GFL2GH4TVAEF3CALR5M4/events.json","paper":"https://pith.science/paper/2PAMK6GF"},"agent_actions":{"view_html":"https://pith.science/pith/2PAMK6GFL2GH4TVAEF3CALR5M4","download_json":"https://pith.science/pith/2PAMK6GFL2GH4TVAEF3CALR5M4.json","view_paper":"https://pith.science/paper/2PAMK6GF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1705.07548&json=true","fetch_graph":"https://pith.science/api/pith-number/2PAMK6GFL2GH4TVAEF3CALR5M4/graph.json","fetch_events":"https://pith.science/api/pith-number/2PAMK6GFL2GH4TVAEF3CALR5M4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2PAMK6GFL2GH4TVAEF3CALR5M4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2PAMK6GFL2GH4TVAEF3CALR5M4/action/storage_attestation","attest_author":"https://pith.science/pith/2PAMK6GFL2GH4TVAEF3CALR5M4/action/author_attestation","sign_citation":"https://pith.science/pith/2PAMK6GFL2GH4TVAEF3CALR5M4/action/citation_signature","submit_replication":"https://pith.science/pith/2PAMK6GFL2GH4TVAEF3CALR5M4/action/replication_record"}},"created_at":"2026-05-18T00:32:36.197794+00:00","updated_at":"2026-05-18T00:32:36.197794+00:00"}