{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:ISG54WIWFG7Q4MK55RPE4XLUQT","short_pith_number":"pith:ISG54WIW","schema_version":"1.0","canonical_sha256":"448dde591629bf0e315dec5e4e5d7484d64b9bc2d1b22da54cead45663474d68","source":{"kind":"arxiv","id":"1910.03604","version":2},"attestation_state":"computed","paper":{"title":"Inhomogeneous chiral condensates in three-flavor quark matter","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Michael Buballa, Stefano Carignano","submitted_at":"2019-10-08T18:00:14Z","abstract_excerpt":"We investigate the effect of strange quark degrees of freedom on the formation of inhomogeneous chiral condensates in a three-flavor Nambu--Jona-Lasinio model in mean-field approximation. A Ginzburg-Landau study complemented by a stability analysis allow us to determine in a general way the location of the critical and Lifshitz points, together with the phase boundary where the (partially) chirally restored phase becomes unstable against developing inhomogeneities, without resorting to specific assumptions on the shape of the chiral condensate. We discuss the resulting phase structure and stud"},"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":"1910.03604","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-10-08T18:00:14Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"31f470aa51d8a3eeaa7832ac5701f75311480b48903e14dd7b2200fc4a3032e1","abstract_canon_sha256":"94b99801334a239592db0630d4701979613c603dc007896a2f905450423f9723"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:39:14.383378Z","signature_b64":"4yyfAXmQNFE25SX8VVutuxU8HAncqoNRc/Hw10E/5airv3KYhi85K1Bf6NgdYA0jEJtKMq6oqgnRD/ck0HsWDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"448dde591629bf0e315dec5e4e5d7484d64b9bc2d1b22da54cead45663474d68","last_reissued_at":"2026-07-05T00:39:14.382917Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:39:14.382917Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Inhomogeneous chiral condensates in three-flavor quark matter","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Michael Buballa, Stefano Carignano","submitted_at":"2019-10-08T18:00:14Z","abstract_excerpt":"We investigate the effect of strange quark degrees of freedom on the formation of inhomogeneous chiral condensates in a three-flavor Nambu--Jona-Lasinio model in mean-field approximation. A Ginzburg-Landau study complemented by a stability analysis allow us to determine in a general way the location of the critical and Lifshitz points, together with the phase boundary where the (partially) chirally restored phase becomes unstable against developing inhomogeneities, without resorting to specific assumptions on the shape of the chiral condensate. We discuss the resulting phase structure and stud"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1910.03604","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1910.03604/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":"1910.03604","created_at":"2026-07-05T00:39:14.382981+00:00"},{"alias_kind":"arxiv_version","alias_value":"1910.03604v2","created_at":"2026-07-05T00:39:14.382981+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1910.03604","created_at":"2026-07-05T00:39:14.382981+00:00"},{"alias_kind":"pith_short_12","alias_value":"ISG54WIWFG7Q","created_at":"2026-07-05T00:39:14.382981+00:00"},{"alias_kind":"pith_short_16","alias_value":"ISG54WIWFG7Q4MK5","created_at":"2026-07-05T00:39:14.382981+00:00"},{"alias_kind":"pith_short_8","alias_value":"ISG54WIW","created_at":"2026-07-05T00:39:14.382981+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.08674","citing_title":"Thermomagnetic Effects of Quark Matter in the NJL Model: Application of Regularization Schemes","ref_index":28,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ISG54WIWFG7Q4MK55RPE4XLUQT","json":"https://pith.science/pith/ISG54WIWFG7Q4MK55RPE4XLUQT.json","graph_json":"https://pith.science/api/pith-number/ISG54WIWFG7Q4MK55RPE4XLUQT/graph.json","events_json":"https://pith.science/api/pith-number/ISG54WIWFG7Q4MK55RPE4XLUQT/events.json","paper":"https://pith.science/paper/ISG54WIW"},"agent_actions":{"view_html":"https://pith.science/pith/ISG54WIWFG7Q4MK55RPE4XLUQT","download_json":"https://pith.science/pith/ISG54WIWFG7Q4MK55RPE4XLUQT.json","view_paper":"https://pith.science/paper/ISG54WIW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1910.03604&json=true","fetch_graph":"https://pith.science/api/pith-number/ISG54WIWFG7Q4MK55RPE4XLUQT/graph.json","fetch_events":"https://pith.science/api/pith-number/ISG54WIWFG7Q4MK55RPE4XLUQT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ISG54WIWFG7Q4MK55RPE4XLUQT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ISG54WIWFG7Q4MK55RPE4XLUQT/action/storage_attestation","attest_author":"https://pith.science/pith/ISG54WIWFG7Q4MK55RPE4XLUQT/action/author_attestation","sign_citation":"https://pith.science/pith/ISG54WIWFG7Q4MK55RPE4XLUQT/action/citation_signature","submit_replication":"https://pith.science/pith/ISG54WIWFG7Q4MK55RPE4XLUQT/action/replication_record"}},"created_at":"2026-07-05T00:39:14.382981+00:00","updated_at":"2026-07-05T00:39:14.382981+00:00"}