{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:NUY64YIHVTHTR55PHYO7UY2SP7","short_pith_number":"pith:NUY64YIH","schema_version":"1.0","canonical_sha256":"6d31ee6107accf38f7af3e1dfa63527ffe716fe767fd2db770d7c626275dc1b6","source":{"kind":"arxiv","id":"2403.11965","version":2},"attestation_state":"computed","paper":{"title":"Effects of strangeness on the chiral pseudocritical line","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"nucl-th","authors_text":"Amaresh Jaiswal, Deeptak Biswas, Hiranmaya Mishra, Mahammad Sabir Ali","submitted_at":"2024-03-18T17:05:11Z","abstract_excerpt":"Within a 2+1 flavor Nambu\\textendash Jona-Lasinio model, we calculate the curvature coefficients and check them against available lattice QCD estimations. With the observation that the flavor mixing due to the `t Hooft determinant term significantly affects the $\\kappa_{2}^{S}$, we explore the effect of $\\mu_{S}$ on the $T-\\mu_{B}$ crossover lines. With the novel determination of negative $\\kappa_{2}^{B}$ at large $\\mu_{S}$, we advocate the importance of studying the same in lattice QCD."},"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":"2403.11965","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nucl-th","submitted_at":"2024-03-18T17:05:11Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"addaffd41989a4e40e68682b2c015dbbf5a9b5d3a74b719a786e7e8f7430e661","abstract_canon_sha256":"270719dc8dd968d5e5cd067eb4ce44f61a07235cc08205b6344f0d1757e32d9b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:30:51.024701Z","signature_b64":"CO9HKJq0yJaPtO/XwoZ5RUcP0FzcW8+80tv2Uyi5PMKRvN7Q/qB9egZtHzhnUSptPZ0eusWbKpxV8gJFHW4tBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6d31ee6107accf38f7af3e1dfa63527ffe716fe767fd2db770d7c626275dc1b6","last_reissued_at":"2026-07-05T08:30:51.024191Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:30:51.024191Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Effects of strangeness on the chiral pseudocritical line","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"nucl-th","authors_text":"Amaresh Jaiswal, Deeptak Biswas, Hiranmaya Mishra, Mahammad Sabir Ali","submitted_at":"2024-03-18T17:05:11Z","abstract_excerpt":"Within a 2+1 flavor Nambu\\textendash Jona-Lasinio model, we calculate the curvature coefficients and check them against available lattice QCD estimations. With the observation that the flavor mixing due to the `t Hooft determinant term significantly affects the $\\kappa_{2}^{S}$, we explore the effect of $\\mu_{S}$ on the $T-\\mu_{B}$ crossover lines. With the novel determination of negative $\\kappa_{2}^{B}$ at large $\\mu_{S}$, we advocate the importance of studying the same in lattice QCD."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2403.11965","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/2403.11965/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":"2403.11965","created_at":"2026-07-05T08:30:51.024253+00:00"},{"alias_kind":"arxiv_version","alias_value":"2403.11965v2","created_at":"2026-07-05T08:30:51.024253+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2403.11965","created_at":"2026-07-05T08:30:51.024253+00:00"},{"alias_kind":"pith_short_12","alias_value":"NUY64YIHVTHT","created_at":"2026-07-05T08:30:51.024253+00:00"},{"alias_kind":"pith_short_16","alias_value":"NUY64YIHVTHTR55P","created_at":"2026-07-05T08:30:51.024253+00:00"},{"alias_kind":"pith_short_8","alias_value":"NUY64YIH","created_at":"2026-07-05T08:30:51.024253+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.08457","citing_title":"Electron-Ion Collision Environment: Distribution of Quark Spin and Orbital Angular Momentum","ref_index":60,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NUY64YIHVTHTR55PHYO7UY2SP7","json":"https://pith.science/pith/NUY64YIHVTHTR55PHYO7UY2SP7.json","graph_json":"https://pith.science/api/pith-number/NUY64YIHVTHTR55PHYO7UY2SP7/graph.json","events_json":"https://pith.science/api/pith-number/NUY64YIHVTHTR55PHYO7UY2SP7/events.json","paper":"https://pith.science/paper/NUY64YIH"},"agent_actions":{"view_html":"https://pith.science/pith/NUY64YIHVTHTR55PHYO7UY2SP7","download_json":"https://pith.science/pith/NUY64YIHVTHTR55PHYO7UY2SP7.json","view_paper":"https://pith.science/paper/NUY64YIH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2403.11965&json=true","fetch_graph":"https://pith.science/api/pith-number/NUY64YIHVTHTR55PHYO7UY2SP7/graph.json","fetch_events":"https://pith.science/api/pith-number/NUY64YIHVTHTR55PHYO7UY2SP7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NUY64YIHVTHTR55PHYO7UY2SP7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NUY64YIHVTHTR55PHYO7UY2SP7/action/storage_attestation","attest_author":"https://pith.science/pith/NUY64YIHVTHTR55PHYO7UY2SP7/action/author_attestation","sign_citation":"https://pith.science/pith/NUY64YIHVTHTR55PHYO7UY2SP7/action/citation_signature","submit_replication":"https://pith.science/pith/NUY64YIHVTHTR55PHYO7UY2SP7/action/replication_record"}},"created_at":"2026-07-05T08:30:51.024253+00:00","updated_at":"2026-07-05T08:30:51.024253+00:00"}