{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:E2JXKPQDNY4JOEL27ULXAJ7OYK","short_pith_number":"pith:E2JXKPQD","schema_version":"1.0","canonical_sha256":"2693753e036e3897117afd177027eec2950e5fef7c83e88458fcd4bcaa37dee5","source":{"kind":"arxiv","id":"2407.19896","version":3},"attestation_state":"computed","paper":{"title":"Meson-nucleus bound states in quark meson coupling model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Amruta Mishra, Arpita Mondal","submitted_at":"2024-07-29T11:18:58Z","abstract_excerpt":"The formations of the $K(\\bar{K})$, $D(\\bar{D})$, and $B(\\bar{B})$ meson-nucleus bound states in ${\\rm{^{16}O}}$, ${\\rm{^{40}Ca}}$, ${\\rm{^{90}Zr}}$, ${\\rm{^{197}Au}}$, and ${\\rm{^{208}Pb}}$ nucleus are investigated using the quark meson coupling model. The model relies on a mean field description of non-overlapping nucleon bags bound by the self-consistent interactions of scalar ($\\sigma$, $\\delta$) and vector ($\\omega$, $\\rho$) mesons with the (anti)quarks inside the bags, which is further extended to explore the properties of nuclei. We estimate the meson-nucleus bound state energies by sol"},"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":"2407.19896","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2024-07-29T11:18:58Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"d48c72c12f88bf8e86d9e2eef508042dd17849e2959edfb45babf83fef1325ff","abstract_canon_sha256":"00b1769469a338f9527af2986a80dbc3d8ef137aaaa32b2062f19ba0cc1d3dbe"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:54:35.027759Z","signature_b64":"hXRh5Hi923ozkWwHEWVJRtfVSWGv+Y7iUpIkw3YRvfF+yC8jOQ8tbHhpBvPg9u5p20NW6FxBxjGvml3PxjneDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2693753e036e3897117afd177027eec2950e5fef7c83e88458fcd4bcaa37dee5","last_reissued_at":"2026-07-05T10:54:35.027307Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:54:35.027307Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Meson-nucleus bound states in quark meson coupling model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Amruta Mishra, Arpita Mondal","submitted_at":"2024-07-29T11:18:58Z","abstract_excerpt":"The formations of the $K(\\bar{K})$, $D(\\bar{D})$, and $B(\\bar{B})$ meson-nucleus bound states in ${\\rm{^{16}O}}$, ${\\rm{^{40}Ca}}$, ${\\rm{^{90}Zr}}$, ${\\rm{^{197}Au}}$, and ${\\rm{^{208}Pb}}$ nucleus are investigated using the quark meson coupling model. The model relies on a mean field description of non-overlapping nucleon bags bound by the self-consistent interactions of scalar ($\\sigma$, $\\delta$) and vector ($\\omega$, $\\rho$) mesons with the (anti)quarks inside the bags, which is further extended to explore the properties of nuclei. We estimate the meson-nucleus bound state energies by sol"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2407.19896","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/2407.19896/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":"2407.19896","created_at":"2026-07-05T10:54:35.027382+00:00"},{"alias_kind":"arxiv_version","alias_value":"2407.19896v3","created_at":"2026-07-05T10:54:35.027382+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2407.19896","created_at":"2026-07-05T10:54:35.027382+00:00"},{"alias_kind":"pith_short_12","alias_value":"E2JXKPQDNY4J","created_at":"2026-07-05T10:54:35.027382+00:00"},{"alias_kind":"pith_short_16","alias_value":"E2JXKPQDNY4JOEL2","created_at":"2026-07-05T10:54:35.027382+00:00"},{"alias_kind":"pith_short_8","alias_value":"E2JXKPQD","created_at":"2026-07-05T10:54:35.027382+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2505.00539","citing_title":"Unified QMF equation of state for neutron star matter: Static and dynamic properties","ref_index":24,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/E2JXKPQDNY4JOEL27ULXAJ7OYK","json":"https://pith.science/pith/E2JXKPQDNY4JOEL27ULXAJ7OYK.json","graph_json":"https://pith.science/api/pith-number/E2JXKPQDNY4JOEL27ULXAJ7OYK/graph.json","events_json":"https://pith.science/api/pith-number/E2JXKPQDNY4JOEL27ULXAJ7OYK/events.json","paper":"https://pith.science/paper/E2JXKPQD"},"agent_actions":{"view_html":"https://pith.science/pith/E2JXKPQDNY4JOEL27ULXAJ7OYK","download_json":"https://pith.science/pith/E2JXKPQDNY4JOEL27ULXAJ7OYK.json","view_paper":"https://pith.science/paper/E2JXKPQD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2407.19896&json=true","fetch_graph":"https://pith.science/api/pith-number/E2JXKPQDNY4JOEL27ULXAJ7OYK/graph.json","fetch_events":"https://pith.science/api/pith-number/E2JXKPQDNY4JOEL27ULXAJ7OYK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/E2JXKPQDNY4JOEL27ULXAJ7OYK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/E2JXKPQDNY4JOEL27ULXAJ7OYK/action/storage_attestation","attest_author":"https://pith.science/pith/E2JXKPQDNY4JOEL27ULXAJ7OYK/action/author_attestation","sign_citation":"https://pith.science/pith/E2JXKPQDNY4JOEL27ULXAJ7OYK/action/citation_signature","submit_replication":"https://pith.science/pith/E2JXKPQDNY4JOEL27ULXAJ7OYK/action/replication_record"}},"created_at":"2026-07-05T10:54:35.027382+00:00","updated_at":"2026-07-05T10:54:35.027382+00:00"}