{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:SKR7GRJEB5HZQD6GDM7QSGVVWL","short_pith_number":"pith:SKR7GRJE","schema_version":"1.0","canonical_sha256":"92a3f345240f4f980fc61b3f091ab5b2cd3eb315aec601d1fbf4fab1da7060d2","source":{"kind":"arxiv","id":"2607.19125","version":1},"attestation_state":"computed","paper":{"title":"Holographic Soliton Crystals for Dense Nuclear Matter and Neutron Stars","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Anton Rebhan, Jonas Mager, Lorenzo Bartolini, Sven Bjarke Gudnason","submitted_at":"2026-07-21T14:13:04Z","abstract_excerpt":"We construct a nuclear-matter equation of state (EOS) from holographic QCD in the Witten-Sakai-Sugimoto (WSS) model, going beyond the homogeneous ansatz by building dense baryonic matter more directly from the solitonic description of holographic baryons. Employing the two-baryon interaction potential obtained from the linearized soliton tails sourced in the curved background by point-like (core) instantons, we assemble an infinite face-centered cubic (FCC) crystal with nearest neighbors in the most attractive channel as an approximation to the quantum liquid of baryons and compute the energy "},"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":"2607.19125","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2026-07-21T14:13:04Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"d5a7a87d6cf41d2617ffff356e6e48c3ea77271c13225aa4becc4336f7a47410","abstract_canon_sha256":"4e6c9ee3522fe0ec97666b75e3d9e462cfb89737fa08f3cf550cf8c80d4f4756"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-22T01:24:09.889008Z","signature_b64":"qTfqbAYCLIJwyLp0dSNS0C3sVpNvNE5kYb5vuSJap+c4OzNAxZ9fR9tKd8m6TVcgDXemhxiY2tR5Frl0VbbDDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"92a3f345240f4f980fc61b3f091ab5b2cd3eb315aec601d1fbf4fab1da7060d2","last_reissued_at":"2026-07-22T01:24:09.888141Z","signature_status":"signed_v1","first_computed_at":"2026-07-22T01:24:09.888141Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Holographic Soliton Crystals for Dense Nuclear Matter and Neutron Stars","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Anton Rebhan, Jonas Mager, Lorenzo Bartolini, Sven Bjarke Gudnason","submitted_at":"2026-07-21T14:13:04Z","abstract_excerpt":"We construct a nuclear-matter equation of state (EOS) from holographic QCD in the Witten-Sakai-Sugimoto (WSS) model, going beyond the homogeneous ansatz by building dense baryonic matter more directly from the solitonic description of holographic baryons. Employing the two-baryon interaction potential obtained from the linearized soliton tails sourced in the curved background by point-like (core) instantons, we assemble an infinite face-centered cubic (FCC) crystal with nearest neighbors in the most attractive channel as an approximation to the quantum liquid of baryons and compute the energy "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.19125","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2607.19125/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":"2607.19125","created_at":"2026-07-22T01:24:09.888591+00:00"},{"alias_kind":"arxiv_version","alias_value":"2607.19125v1","created_at":"2026-07-22T01:24:09.888591+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.19125","created_at":"2026-07-22T01:24:09.888591+00:00"},{"alias_kind":"pith_short_12","alias_value":"SKR7GRJEB5HZ","created_at":"2026-07-22T01:24:09.888591+00:00"},{"alias_kind":"pith_short_16","alias_value":"SKR7GRJEB5HZQD6G","created_at":"2026-07-22T01:24:09.888591+00:00"},{"alias_kind":"pith_short_8","alias_value":"SKR7GRJE","created_at":"2026-07-22T01:24:09.888591+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/SKR7GRJEB5HZQD6GDM7QSGVVWL","json":"https://pith.science/pith/SKR7GRJEB5HZQD6GDM7QSGVVWL.json","graph_json":"https://pith.science/api/pith-number/SKR7GRJEB5HZQD6GDM7QSGVVWL/graph.json","events_json":"https://pith.science/api/pith-number/SKR7GRJEB5HZQD6GDM7QSGVVWL/events.json","paper":"https://pith.science/paper/SKR7GRJE"},"agent_actions":{"view_html":"https://pith.science/pith/SKR7GRJEB5HZQD6GDM7QSGVVWL","download_json":"https://pith.science/pith/SKR7GRJEB5HZQD6GDM7QSGVVWL.json","view_paper":"https://pith.science/paper/SKR7GRJE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2607.19125&json=true","fetch_graph":"https://pith.science/api/pith-number/SKR7GRJEB5HZQD6GDM7QSGVVWL/graph.json","fetch_events":"https://pith.science/api/pith-number/SKR7GRJEB5HZQD6GDM7QSGVVWL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SKR7GRJEB5HZQD6GDM7QSGVVWL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SKR7GRJEB5HZQD6GDM7QSGVVWL/action/storage_attestation","attest_author":"https://pith.science/pith/SKR7GRJEB5HZQD6GDM7QSGVVWL/action/author_attestation","sign_citation":"https://pith.science/pith/SKR7GRJEB5HZQD6GDM7QSGVVWL/action/citation_signature","submit_replication":"https://pith.science/pith/SKR7GRJEB5HZQD6GDM7QSGVVWL/action/replication_record"}},"created_at":"2026-07-22T01:24:09.888591+00:00","updated_at":"2026-07-22T01:24:09.888591+00:00"}