{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2004:P4VY3DJTO3EFVDG7ZI3ZJRUKZU","short_pith_number":"pith:P4VY3DJT","canonical_record":{"source":{"id":"hep-lat/0401001","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2004-01-01T13:56:20Z","cross_cats_sorted":[],"title_canon_sha256":"c2ec3417181a5ebafd9164cdb4ffe17a7ab3dcb67a9349cd7afa172042c9d2a3","abstract_canon_sha256":"54582c28a336e287ac2dc264f5dfb1e55032194eb93d903016eba7a751f89fd9"},"schema_version":"1.0"},"canonical_sha256":"7f2b8d8d3376c85a8cdfca3794c68acd3e62a29609ca1f2f2a17a3bf9b24c267","source":{"kind":"arxiv","id":"hep-lat/0401001","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0401001","created_at":"2026-05-18T00:37:13Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0401001v1","created_at":"2026-05-18T00:37:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0401001","created_at":"2026-05-18T00:37:13Z"},{"alias_kind":"pith_short_12","alias_value":"P4VY3DJTO3EF","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"P4VY3DJTO3EFVDG7","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"P4VY3DJT","created_at":"2026-05-18T12:25:52Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2004:P4VY3DJTO3EFVDG7ZI3ZJRUKZU","target":"record","payload":{"canonical_record":{"source":{"id":"hep-lat/0401001","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2004-01-01T13:56:20Z","cross_cats_sorted":[],"title_canon_sha256":"c2ec3417181a5ebafd9164cdb4ffe17a7ab3dcb67a9349cd7afa172042c9d2a3","abstract_canon_sha256":"54582c28a336e287ac2dc264f5dfb1e55032194eb93d903016eba7a751f89fd9"},"schema_version":"1.0"},"canonical_sha256":"7f2b8d8d3376c85a8cdfca3794c68acd3e62a29609ca1f2f2a17a3bf9b24c267","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:37:13.592884Z","signature_b64":"WsBqjnfcCIypAjb0ueUdJhkahS1p0L1/RVWYPWnQ/NBj+ChfWVyD2v9rECjzqourBSsDqna0zbwOeIJQP9ayDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7f2b8d8d3376c85a8cdfca3794c68acd3e62a29609ca1f2f2a17a3bf9b24c267","last_reissued_at":"2026-05-18T00:37:13.592068Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:37:13.592068Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-lat/0401001","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:37:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yd/xAaM4ZvwEh1y2Ko4ARAobCiKPbCYf80VJbr4B6xTr5MdrGt6BsAjkgvDKDejIdvgUbXP5uq6G752YTsz2Dg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T17:54:36.883304Z"},"content_sha256":"40630ab2a8033b4618bfd5f5c507fac749db026d27e02a3b8922ede54b8ffdbc","schema_version":"1.0","event_id":"sha256:40630ab2a8033b4618bfd5f5c507fac749db026d27e02a3b8922ede54b8ffdbc"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2004:P4VY3DJTO3EFVDG7ZI3ZJRUKZU","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Y-type Flux-Tube Formation in Baryons","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"H. Ichie, H. Suganuma, Toru T. Takahashi","submitted_at":"2004-01-01T13:56:20Z","abstract_excerpt":"For more than 300 different patterns of the 3Q systems, the ground-state 3Q potential $V_{\\rm 3Q}^{\\rm g.s.}$ is investigated using SU(3) lattice QCD with $12^3\\times 24$ at $\\beta=5.7$ and $16^3\\times 32$ at $\\beta=5.8, 6.0$ at the quenched level. As a result of the detailed analyses, we find that the ground-state potential $V_{\\rm 3Q}^{\\rm g.s.}$ is well described with so-called Y-ansatz as $V_{\\rm 3Q}=-A_{\\rm 3Q}\\sum_{i<j}\\frac1{|{\\bf r}_i-{\\bf r}_j|} +\\sigma_{\\rm 3Q} L_{\\rm min}+C_{\\rm 3Q}$, with the accuracy better than 1%. Here, $L_{\\rm min}$ denotes the minimal value of total flux-tube "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0401001","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":""},"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":"2026-05-18T00:37:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9QowJLI08mdI64LPSDvRx+KtqIvFwfXjxB0vmivTd8I9l1rDengKrmiIhZummUdYk6t+lFbiTjDBux93BZ9VCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T17:54:36.883678Z"},"content_sha256":"5dde1c37a21c0d989b7fa2bb0d04647ff06be890d124ba3e090f6da6e2ccf487","schema_version":"1.0","event_id":"sha256:5dde1c37a21c0d989b7fa2bb0d04647ff06be890d124ba3e090f6da6e2ccf487"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/P4VY3DJTO3EFVDG7ZI3ZJRUKZU/bundle.json","state_url":"https://pith.science/pith/P4VY3DJTO3EFVDG7ZI3ZJRUKZU/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/P4VY3DJTO3EFVDG7ZI3ZJRUKZU/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":"2026-06-03T17:54:36Z","links":{"resolver":"https://pith.science/pith/P4VY3DJTO3EFVDG7ZI3ZJRUKZU","bundle":"https://pith.science/pith/P4VY3DJTO3EFVDG7ZI3ZJRUKZU/bundle.json","state":"https://pith.science/pith/P4VY3DJTO3EFVDG7ZI3ZJRUKZU/state.json","well_known_bundle":"https://pith.science/.well-known/pith/P4VY3DJTO3EFVDG7ZI3ZJRUKZU/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2004:P4VY3DJTO3EFVDG7ZI3ZJRUKZU","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":"54582c28a336e287ac2dc264f5dfb1e55032194eb93d903016eba7a751f89fd9","cross_cats_sorted":[],"license":"","primary_cat":"hep-lat","submitted_at":"2004-01-01T13:56:20Z","title_canon_sha256":"c2ec3417181a5ebafd9164cdb4ffe17a7ab3dcb67a9349cd7afa172042c9d2a3"},"schema_version":"1.0","source":{"id":"hep-lat/0401001","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0401001","created_at":"2026-05-18T00:37:13Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0401001v1","created_at":"2026-05-18T00:37:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0401001","created_at":"2026-05-18T00:37:13Z"},{"alias_kind":"pith_short_12","alias_value":"P4VY3DJTO3EF","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"P4VY3DJTO3EFVDG7","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"P4VY3DJT","created_at":"2026-05-18T12:25:52Z"}],"graph_snapshots":[{"event_id":"sha256:5dde1c37a21c0d989b7fa2bb0d04647ff06be890d124ba3e090f6da6e2ccf487","target":"graph","created_at":"2026-05-18T00:37:13Z","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"},"paper":{"abstract_excerpt":"For more than 300 different patterns of the 3Q systems, the ground-state 3Q potential $V_{\\rm 3Q}^{\\rm g.s.}$ is investigated using SU(3) lattice QCD with $12^3\\times 24$ at $\\beta=5.7$ and $16^3\\times 32$ at $\\beta=5.8, 6.0$ at the quenched level. As a result of the detailed analyses, we find that the ground-state potential $V_{\\rm 3Q}^{\\rm g.s.}$ is well described with so-called Y-ansatz as $V_{\\rm 3Q}=-A_{\\rm 3Q}\\sum_{i<j}\\frac1{|{\\bf r}_i-{\\bf r}_j|} +\\sigma_{\\rm 3Q} L_{\\rm min}+C_{\\rm 3Q}$, with the accuracy better than 1%. Here, $L_{\\rm min}$ denotes the minimal value of total flux-tube ","authors_text":"H. Ichie, H. Suganuma, Toru T. Takahashi","cross_cats":[],"headline":"","license":"","primary_cat":"hep-lat","submitted_at":"2004-01-01T13:56:20Z","title":"Y-type Flux-Tube Formation in Baryons"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0401001","kind":"arxiv","version":1},"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":"sha256:40630ab2a8033b4618bfd5f5c507fac749db026d27e02a3b8922ede54b8ffdbc","target":"record","created_at":"2026-05-18T00:37:13Z","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":"54582c28a336e287ac2dc264f5dfb1e55032194eb93d903016eba7a751f89fd9","cross_cats_sorted":[],"license":"","primary_cat":"hep-lat","submitted_at":"2004-01-01T13:56:20Z","title_canon_sha256":"c2ec3417181a5ebafd9164cdb4ffe17a7ab3dcb67a9349cd7afa172042c9d2a3"},"schema_version":"1.0","source":{"id":"hep-lat/0401001","kind":"arxiv","version":1}},"canonical_sha256":"7f2b8d8d3376c85a8cdfca3794c68acd3e62a29609ca1f2f2a17a3bf9b24c267","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7f2b8d8d3376c85a8cdfca3794c68acd3e62a29609ca1f2f2a17a3bf9b24c267","first_computed_at":"2026-05-18T00:37:13.592068Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:37:13.592068Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"WsBqjnfcCIypAjb0ueUdJhkahS1p0L1/RVWYPWnQ/NBj+ChfWVyD2v9rECjzqourBSsDqna0zbwOeIJQP9ayDA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:37:13.592884Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-lat/0401001","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:40630ab2a8033b4618bfd5f5c507fac749db026d27e02a3b8922ede54b8ffdbc","sha256:5dde1c37a21c0d989b7fa2bb0d04647ff06be890d124ba3e090f6da6e2ccf487"],"state_sha256":"4d311bb159ebe5b355cba8e52bca30ceede768d26528993bb0849eb932dc6c14"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ub4/pK+3iDsQaBnOtLF8CujVT9ZBMPUL3FEoIeiBYlA/suCXqpPCuPMXm6RqeInRAC0ADISHaddX5BEtkVXWBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-03T17:54:36.885666Z","bundle_sha256":"ecbee1e5500b02dfe1306eb322937b3cf0be9e20faae75ae886ff1a9fa53f89d"}}