{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:2S2ZGS2XFMNRTE6SKOMJI4NUI7","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"d62f2781e4aed238f7d6ad11b81c4b52a61b725c86462777f13c7d88e867566b","cross_cats_sorted":["cond-mat.str-el","nucl-th"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-02-18T12:52:27Z","title_canon_sha256":"5a199919c1c8be1b855a547b8d66e53e3ec16055ecb519b6a2e6e748886be7b5"},"schema_version":"1.0","source":{"id":"2402.11578","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2402.11578","created_at":"2026-07-05T08:21:50Z"},{"alias_kind":"arxiv_version","alias_value":"2402.11578v2","created_at":"2026-07-05T08:21:50Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2402.11578","created_at":"2026-07-05T08:21:50Z"},{"alias_kind":"pith_short_12","alias_value":"2S2ZGS2XFMNR","created_at":"2026-07-05T08:21:50Z"},{"alias_kind":"pith_short_16","alias_value":"2S2ZGS2XFMNRTE6S","created_at":"2026-07-05T08:21:50Z"},{"alias_kind":"pith_short_8","alias_value":"2S2ZGS2X","created_at":"2026-07-05T08:21:50Z"}],"graph_snapshots":[{"event_id":"sha256:5c22f5b2e3a38886fad7637a051025675676aee8083793fcaff13da114dd0e42","target":"graph","created_at":"2026-07-05T08:21:50Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2402.11578/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We consider the quantum chromodynamics (QCD) Kondo effect for a single heavy quark in quark matter composed of light quarks with chiral symmetry breaking. Introducing several spinor structures in QCD Kondo condensates, i.e., particle-projected condensate, antiparticle-projected condensate, and normal condensate without projection, we calculate the attractive energy gained by the heavy quark within the mean-field approximation in the path-integral formalism. We show that the normal condensate is favored at low density and the particle-projected condensate is favored at high density, when the li","authors_text":"Daiki Suenaga, Kei Suzuki, Shigehiro Yasui","cross_cats":["cond-mat.str-el","nucl-th"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-02-18T12:52:27Z","title":"QCD Kondo effect for single heavy quark in chiral-symmetry broken phase"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2402.11578","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:73ebd76d2a558a441cfcdddae564e612862ad85a50f092cffe9e740970dedadd","target":"record","created_at":"2026-07-05T08:21:50Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"d62f2781e4aed238f7d6ad11b81c4b52a61b725c86462777f13c7d88e867566b","cross_cats_sorted":["cond-mat.str-el","nucl-th"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-02-18T12:52:27Z","title_canon_sha256":"5a199919c1c8be1b855a547b8d66e53e3ec16055ecb519b6a2e6e748886be7b5"},"schema_version":"1.0","source":{"id":"2402.11578","kind":"arxiv","version":2}},"canonical_sha256":"d4b5934b572b1b1993d253989471b447d3e58e1367717c3bf776e2772cdae487","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d4b5934b572b1b1993d253989471b447d3e58e1367717c3bf776e2772cdae487","first_computed_at":"2026-07-05T08:21:50.398736Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T08:21:50.398736Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"l1x0oXbwFra9zaVNnhmuQRM+DM+3Ka3j5jg4ohyrAPpdUuYYbuBUI6bPDYP9rwZZn9N1L93+LzBYhBdF9fHFBA==","signature_status":"signed_v1","signed_at":"2026-07-05T08:21:50.399220Z","signed_message":"canonical_sha256_bytes"},"source_id":"2402.11578","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:73ebd76d2a558a441cfcdddae564e612862ad85a50f092cffe9e740970dedadd","sha256:5c22f5b2e3a38886fad7637a051025675676aee8083793fcaff13da114dd0e42"],"state_sha256":"65a1db53a7b7affac769e7ce71803e6ef1958e56ded20fc40f545123396b3997"}