{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:IXS5LRNSIFVCNYED2WE6BZIHO7","short_pith_number":"pith:IXS5LRNS","schema_version":"1.0","canonical_sha256":"45e5d5c5b2416a26e083d589e0e50777dac06734fec65d00a4fa006c81ec93b1","source":{"kind":"arxiv","id":"2503.23872","version":1},"attestation_state":"computed","paper":{"title":"European Strategy for Particle Physics 2026: the NA60+/DiCE experiment at the SPS","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"nucl-ex","authors_text":"NA60+/DiCE Collaboration","submitted_at":"2025-03-31T09:23:01Z","abstract_excerpt":"The exploration of the phase diagram of Quantum ChromoDynamics (QCD) is carried out by studying ultrarelativistic heavy-ion collisions. The energy range covered by the CERN SPS ($\\sqrt{s_{\\rm {NN}}} \\sim 6-17$ GeV) is ideal for the investigation of the region corresponding to finite baryochemical potential ($\\mu_{\\rm B}$), and was little explored up to now. We propose in this document a new experiment, NA60+/DiCE (Dilepton and Charm Experiment), that will address several observables which are fundamental for the understanding of the phase transition from hadronic matter towards a Quark-Gluon P"},"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":"2503.23872","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nucl-ex","submitted_at":"2025-03-31T09:23:01Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"f0ad1ac18c408ffe60a38c676b1273152e993fa37a51b1888a07419846215dab","abstract_canon_sha256":"07ea78fbedf01a4e04efbfbd99ece3feb620c84705108f812222f916a368dc43"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:42:01.050466Z","signature_b64":"FTlUBbd8SZoJvr5ceC2vaF3kAgpPtMtM0PxPCrC7fuJV1h8HU4M/FO8Pxg8PMSNpN60R58QFVXW0H/ytwnIHAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"45e5d5c5b2416a26e083d589e0e50777dac06734fec65d00a4fa006c81ec93b1","last_reissued_at":"2026-07-05T10:42:01.050008Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:42:01.050008Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"European Strategy for Particle Physics 2026: the NA60+/DiCE experiment at the SPS","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"nucl-ex","authors_text":"NA60+/DiCE Collaboration","submitted_at":"2025-03-31T09:23:01Z","abstract_excerpt":"The exploration of the phase diagram of Quantum ChromoDynamics (QCD) is carried out by studying ultrarelativistic heavy-ion collisions. The energy range covered by the CERN SPS ($\\sqrt{s_{\\rm {NN}}} \\sim 6-17$ GeV) is ideal for the investigation of the region corresponding to finite baryochemical potential ($\\mu_{\\rm B}$), and was little explored up to now. We propose in this document a new experiment, NA60+/DiCE (Dilepton and Charm Experiment), that will address several observables which are fundamental for the understanding of the phase transition from hadronic matter towards a Quark-Gluon P"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2503.23872","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/2503.23872/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":"2503.23872","created_at":"2026-07-05T10:42:01.050061+00:00"},{"alias_kind":"arxiv_version","alias_value":"2503.23872v1","created_at":"2026-07-05T10:42:01.050061+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2503.23872","created_at":"2026-07-05T10:42:01.050061+00:00"},{"alias_kind":"pith_short_12","alias_value":"IXS5LRNSIFVC","created_at":"2026-07-05T10:42:01.050061+00:00"},{"alias_kind":"pith_short_16","alias_value":"IXS5LRNSIFVCNYED","created_at":"2026-07-05T10:42:01.050061+00:00"},{"alias_kind":"pith_short_8","alias_value":"IXS5LRNS","created_at":"2026-07-05T10:42:01.050061+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.05792","citing_title":"Charmonium production in low energy nuclear collisions at SPS and FAIR: achievements $\\&$ prospects","ref_index":136,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/IXS5LRNSIFVCNYED2WE6BZIHO7","json":"https://pith.science/pith/IXS5LRNSIFVCNYED2WE6BZIHO7.json","graph_json":"https://pith.science/api/pith-number/IXS5LRNSIFVCNYED2WE6BZIHO7/graph.json","events_json":"https://pith.science/api/pith-number/IXS5LRNSIFVCNYED2WE6BZIHO7/events.json","paper":"https://pith.science/paper/IXS5LRNS"},"agent_actions":{"view_html":"https://pith.science/pith/IXS5LRNSIFVCNYED2WE6BZIHO7","download_json":"https://pith.science/pith/IXS5LRNSIFVCNYED2WE6BZIHO7.json","view_paper":"https://pith.science/paper/IXS5LRNS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2503.23872&json=true","fetch_graph":"https://pith.science/api/pith-number/IXS5LRNSIFVCNYED2WE6BZIHO7/graph.json","fetch_events":"https://pith.science/api/pith-number/IXS5LRNSIFVCNYED2WE6BZIHO7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IXS5LRNSIFVCNYED2WE6BZIHO7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IXS5LRNSIFVCNYED2WE6BZIHO7/action/storage_attestation","attest_author":"https://pith.science/pith/IXS5LRNSIFVCNYED2WE6BZIHO7/action/author_attestation","sign_citation":"https://pith.science/pith/IXS5LRNSIFVCNYED2WE6BZIHO7/action/citation_signature","submit_replication":"https://pith.science/pith/IXS5LRNSIFVCNYED2WE6BZIHO7/action/replication_record"}},"created_at":"2026-07-05T10:42:01.050061+00:00","updated_at":"2026-07-05T10:42:01.050061+00:00"}