{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:WRNRQZ6SRTN6HIRLHJECR34QFV","short_pith_number":"pith:WRNRQZ6S","schema_version":"1.0","canonical_sha256":"b45b1867d28cdbe3a22b3a4828ef902d7d6545fa5dd607d9389a1cea6e8cb255","source":{"kind":"arxiv","id":"2301.11484","version":1},"attestation_state":"computed","paper":{"title":"Particle Interferometry in a Moat Regime","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Dirk H. Rischke, Fabian Rennecke, Robert D. Pisarski","submitted_at":"2023-01-27T01:26:45Z","abstract_excerpt":"Dense strongly interacting matter can exhibit regimes with spatial modulations, akin to crystalline phases. In this case particles can have a moat spectrum with minimal energy at nonzero momentum. We show that particle interferometry is a sensitive probe of such a regime in heavy-ion collisions. To this end, we develop a field-theoretical formalism that relates particle spectra to in-medium real-time correlation functions of quantum fields on curved hypersurfaces of spacetime. This is then applied to the study of Bose-Einstein correlations in a moat regime in heavy-ion collisions. The resultin"},"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":"2301.11484","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2023-01-27T01:26:45Z","cross_cats_sorted":["nucl-ex","nucl-th"],"title_canon_sha256":"05b3e0a3f9eb1762211bd4ccd05995546d51e9a22f8526b5c5382752ef2baaea","abstract_canon_sha256":"efdebf5fcf104fd61bdc1bd95811ea725b7468ccb7360ff46a9ec385cb020ef6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:21:58.460731Z","signature_b64":"oSebHHQpuTqS8Kj8Dlw/Qp3rrxOLxk+aUEBBvI8IHvPvKXIjigbXSdNHDt4g7laApCqCCj4JGg7f8nSFgAy5Bw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b45b1867d28cdbe3a22b3a4828ef902d7d6545fa5dd607d9389a1cea6e8cb255","last_reissued_at":"2026-07-05T06:21:58.460290Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:21:58.460290Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Particle Interferometry in a Moat Regime","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Dirk H. Rischke, Fabian Rennecke, Robert D. Pisarski","submitted_at":"2023-01-27T01:26:45Z","abstract_excerpt":"Dense strongly interacting matter can exhibit regimes with spatial modulations, akin to crystalline phases. In this case particles can have a moat spectrum with minimal energy at nonzero momentum. We show that particle interferometry is a sensitive probe of such a regime in heavy-ion collisions. To this end, we develop a field-theoretical formalism that relates particle spectra to in-medium real-time correlation functions of quantum fields on curved hypersurfaces of spacetime. This is then applied to the study of Bose-Einstein correlations in a moat regime in heavy-ion collisions. The resultin"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2301.11484","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/2301.11484/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":"2301.11484","created_at":"2026-07-05T06:21:58.460359+00:00"},{"alias_kind":"arxiv_version","alias_value":"2301.11484v1","created_at":"2026-07-05T06:21:58.460359+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2301.11484","created_at":"2026-07-05T06:21:58.460359+00:00"},{"alias_kind":"pith_short_12","alias_value":"WRNRQZ6SRTN6","created_at":"2026-07-05T06:21:58.460359+00:00"},{"alias_kind":"pith_short_16","alias_value":"WRNRQZ6SRTN6HIRL","created_at":"2026-07-05T06:21:58.460359+00:00"},{"alias_kind":"pith_short_8","alias_value":"WRNRQZ6S","created_at":"2026-07-05T06:21:58.460359+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.31040","citing_title":"FRG analysis of dense two-color QCD within the linear sigma model","ref_index":55,"is_internal_anchor":false},{"citing_arxiv_id":"2510.06712","citing_title":"Dissecting the moat regime at low energies I: Renormalization and the phase structure","ref_index":31,"is_internal_anchor":false},{"citing_arxiv_id":"2604.20196","citing_title":"Chiral first order phase transition at finite baryon density and zero temperature from self-consistent pole masses in the linear sigma model with quarks","ref_index":9,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WRNRQZ6SRTN6HIRLHJECR34QFV","json":"https://pith.science/pith/WRNRQZ6SRTN6HIRLHJECR34QFV.json","graph_json":"https://pith.science/api/pith-number/WRNRQZ6SRTN6HIRLHJECR34QFV/graph.json","events_json":"https://pith.science/api/pith-number/WRNRQZ6SRTN6HIRLHJECR34QFV/events.json","paper":"https://pith.science/paper/WRNRQZ6S"},"agent_actions":{"view_html":"https://pith.science/pith/WRNRQZ6SRTN6HIRLHJECR34QFV","download_json":"https://pith.science/pith/WRNRQZ6SRTN6HIRLHJECR34QFV.json","view_paper":"https://pith.science/paper/WRNRQZ6S","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2301.11484&json=true","fetch_graph":"https://pith.science/api/pith-number/WRNRQZ6SRTN6HIRLHJECR34QFV/graph.json","fetch_events":"https://pith.science/api/pith-number/WRNRQZ6SRTN6HIRLHJECR34QFV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WRNRQZ6SRTN6HIRLHJECR34QFV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WRNRQZ6SRTN6HIRLHJECR34QFV/action/storage_attestation","attest_author":"https://pith.science/pith/WRNRQZ6SRTN6HIRLHJECR34QFV/action/author_attestation","sign_citation":"https://pith.science/pith/WRNRQZ6SRTN6HIRLHJECR34QFV/action/citation_signature","submit_replication":"https://pith.science/pith/WRNRQZ6SRTN6HIRLHJECR34QFV/action/replication_record"}},"created_at":"2026-07-05T06:21:58.460359+00:00","updated_at":"2026-07-05T06:21:58.460359+00:00"}