{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2024:2S2ZGS2XFMNRTE6SKOMJI4NUI7","short_pith_number":"pith:2S2ZGS2X","canonical_record":{"source":{"id":"2402.11578","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-02-18T12:52:27Z","cross_cats_sorted":["cond-mat.str-el","nucl-th"],"title_canon_sha256":"5a199919c1c8be1b855a547b8d66e53e3ec16055ecb519b6a2e6e748886be7b5","abstract_canon_sha256":"d62f2781e4aed238f7d6ad11b81c4b52a61b725c86462777f13c7d88e867566b"},"schema_version":"1.0"},"canonical_sha256":"d4b5934b572b1b1993d253989471b447d3e58e1367717c3bf776e2772cdae487","source":{"kind":"arxiv","id":"2402.11578","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"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2024:2S2ZGS2XFMNRTE6SKOMJI4NUI7","target":"record","payload":{"canonical_record":{"source":{"id":"2402.11578","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-02-18T12:52:27Z","cross_cats_sorted":["cond-mat.str-el","nucl-th"],"title_canon_sha256":"5a199919c1c8be1b855a547b8d66e53e3ec16055ecb519b6a2e6e748886be7b5","abstract_canon_sha256":"d62f2781e4aed238f7d6ad11b81c4b52a61b725c86462777f13c7d88e867566b"},"schema_version":"1.0"},"canonical_sha256":"d4b5934b572b1b1993d253989471b447d3e58e1367717c3bf776e2772cdae487","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:21:50.399220Z","signature_b64":"l1x0oXbwFra9zaVNnhmuQRM+DM+3Ka3j5jg4ohyrAPpdUuYYbuBUI6bPDYP9rwZZn9N1L93+LzBYhBdF9fHFBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d4b5934b572b1b1993d253989471b447d3e58e1367717c3bf776e2772cdae487","last_reissued_at":"2026-07-05T08:21:50.398736Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:21:50.398736Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2402.11578","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T08:21:50Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"pq7yaMUrlNmOc6iPNcYnvNOTdhm+wAknNfUDvDyPyM4BgdA6/b2eThvd7RUb9wt5TioYvh3ZS23X1raaF4OIBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-05T10:52:42.745160Z"},"content_sha256":"73ebd76d2a558a441cfcdddae564e612862ad85a50f092cffe9e740970dedadd","schema_version":"1.0","event_id":"sha256:73ebd76d2a558a441cfcdddae564e612862ad85a50f092cffe9e740970dedadd"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2024:2S2ZGS2XFMNRTE6SKOMJI4NUI7","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"QCD Kondo effect for single heavy quark in chiral-symmetry broken phase","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.str-el","nucl-th"],"primary_cat":"hep-ph","authors_text":"Daiki Suenaga, Kei Suzuki, Shigehiro Yasui","submitted_at":"2024-02-18T12:52:27Z","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"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2402.11578","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/2402.11578/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T08:21:50Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dqgEjU0PuodEjN7YvvGPUi8qsZP4pSi4EVzkS6O+k2LQEuE93NURnYIRjZdoPRXms9l8g+UNH8B7+SVbMPY6CA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-05T10:52:42.745660Z"},"content_sha256":"5c22f5b2e3a38886fad7637a051025675676aee8083793fcaff13da114dd0e42","schema_version":"1.0","event_id":"sha256:5c22f5b2e3a38886fad7637a051025675676aee8083793fcaff13da114dd0e42"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/2S2ZGS2XFMNRTE6SKOMJI4NUI7/bundle.json","state_url":"https://pith.science/pith/2S2ZGS2XFMNRTE6SKOMJI4NUI7/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/2S2ZGS2XFMNRTE6SKOMJI4NUI7/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-08-05T10:52:42Z","links":{"resolver":"https://pith.science/pith/2S2ZGS2XFMNRTE6SKOMJI4NUI7","bundle":"https://pith.science/pith/2S2ZGS2XFMNRTE6SKOMJI4NUI7/bundle.json","state":"https://pith.science/pith/2S2ZGS2XFMNRTE6SKOMJI4NUI7/state.json","well_known_bundle":"https://pith.science/.well-known/pith/2S2ZGS2XFMNRTE6SKOMJI4NUI7/bundle.json"},"state":{"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"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"viNklkIrwBgZZ7MvXw83YXEgrzTveyJLHJA3epdiVHd9rAncz+EZXn+V6vwO6FSrHp4bDYSyv4ZWcJmJwxupCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-05T10:52:42.750027Z","bundle_sha256":"310056e18184bb7aaeccc2a6bcba3c69713db23acc1760917e1eb0026506f8f2"}}