{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2004:FIBMZPXNXL5EXO5GKRZPVIJCTL","short_pith_number":"pith:FIBMZPXN","canonical_record":{"source":{"id":"hep-lat/0407011","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2004-07-07T10:31:58Z","cross_cats_sorted":[],"title_canon_sha256":"162a8c58480027acc95b46abf0222ad6ca9536d0c7b11903b88684bb193847f3","abstract_canon_sha256":"0b4c031068d43a819103cd38303be57b4317ffd1700625094abeac31a8735592"},"schema_version":"1.0"},"canonical_sha256":"2a02ccbeedbafa4bbba65472faa1229ac321b9c08d85d50d2d589d0d36f5ecb3","source":{"kind":"arxiv","id":"hep-lat/0407011","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0407011","created_at":"2026-05-18T00:36:57Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0407011v1","created_at":"2026-05-18T00:36:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0407011","created_at":"2026-05-18T00:36:57Z"},{"alias_kind":"pith_short_12","alias_value":"FIBMZPXNXL5E","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"FIBMZPXNXL5EXO5G","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"FIBMZPXN","created_at":"2026-05-18T12:25:52Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2004:FIBMZPXNXL5EXO5GKRZPVIJCTL","target":"record","payload":{"canonical_record":{"source":{"id":"hep-lat/0407011","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2004-07-07T10:31:58Z","cross_cats_sorted":[],"title_canon_sha256":"162a8c58480027acc95b46abf0222ad6ca9536d0c7b11903b88684bb193847f3","abstract_canon_sha256":"0b4c031068d43a819103cd38303be57b4317ffd1700625094abeac31a8735592"},"schema_version":"1.0"},"canonical_sha256":"2a02ccbeedbafa4bbba65472faa1229ac321b9c08d85d50d2d589d0d36f5ecb3","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:36:57.691015Z","signature_b64":"1uuxC8VLggSkghWNbwets02GTFgKdYOz2RDXi/aB8mgMAJAFDNZnDZPh/c5DbT3AeBP1dX5BpCAwpduJ9cH0Bw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2a02ccbeedbafa4bbba65472faa1229ac321b9c08d85d50d2d589d0d36f5ecb3","last_reissued_at":"2026-05-18T00:36:57.690419Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:36:57.690419Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-lat/0407011","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":"2026-05-18T00:36:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"m2/2eXUvI127fp/Fqhyc/xMieeJ9p05gwMMe9qIZfXr+Y5Dk6RtSSZ4Gk3Wi13V6t7WXb4eHyLvtGleKz285Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-20T08:40:43.298159Z"},"content_sha256":"8329de4976430a83f6a38f55e206a5a1baf2f0e3e6e28c75b51d92d5c01c4066","schema_version":"1.0","event_id":"sha256:8329de4976430a83f6a38f55e206a5a1baf2f0e3e6e28c75b51d92d5c01c4066"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2004:FIBMZPXNXL5EXO5GKRZPVIJCTL","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Y-type Flux-Tube Formation and Gluonic Excitations in Baryons: From QCD to Quark Model","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Hideo Suganuma, Hiroko Ichie, Toru T. Takahashi","submitted_at":"2004-07-07T10:31:58Z","abstract_excerpt":"Using SU(3) lattice QCD, we perform the first systematic study for the ground-state three-quark (3Q) potential $V_{\\rm 3Q}^{\\rm g.s.}$ and the 1st excited-state 3Q potential $V_{\\rm 3Q}^{\\rm e.s.}$, {\\it i.e.}, the energies of the ground state and the 1st excited state of the gluon field in the presence of the static three quarks. From the accurate and thorough calculation for more than 300 different patterns of 3Q systems, the static ground-state 3Q potential $V_{\\rm 3Q}^{\\rm g.s.}$ is found to be well described by the Coulomb plus Y-type linear potential, {\\it i.e.}, Y-Ansatz, within 1%-leve"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0407011","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":"2026-05-18T00:36:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Z5NW+AQq5PRF/r9+wLh/glNmwtyK3qjVHiamZcmxoFBgMRj6lkr2h3DR9aDKDa+yJHL0Pm/qzgIDflPF9P65CA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-20T08:40:43.298526Z"},"content_sha256":"cc8c62963eebcad586fcaf1f45df946ba43b3a9cfc3e2bcd789439ffa04aca80","schema_version":"1.0","event_id":"sha256:cc8c62963eebcad586fcaf1f45df946ba43b3a9cfc3e2bcd789439ffa04aca80"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/FIBMZPXNXL5EXO5GKRZPVIJCTL/bundle.json","state_url":"https://pith.science/pith/FIBMZPXNXL5EXO5GKRZPVIJCTL/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/FIBMZPXNXL5EXO5GKRZPVIJCTL/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":"2026-06-20T08:40:43Z","links":{"resolver":"https://pith.science/pith/FIBMZPXNXL5EXO5GKRZPVIJCTL","bundle":"https://pith.science/pith/FIBMZPXNXL5EXO5GKRZPVIJCTL/bundle.json","state":"https://pith.science/pith/FIBMZPXNXL5EXO5GKRZPVIJCTL/state.json","well_known_bundle":"https://pith.science/.well-known/pith/FIBMZPXNXL5EXO5GKRZPVIJCTL/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2004:FIBMZPXNXL5EXO5GKRZPVIJCTL","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":"0b4c031068d43a819103cd38303be57b4317ffd1700625094abeac31a8735592","cross_cats_sorted":[],"license":"","primary_cat":"hep-lat","submitted_at":"2004-07-07T10:31:58Z","title_canon_sha256":"162a8c58480027acc95b46abf0222ad6ca9536d0c7b11903b88684bb193847f3"},"schema_version":"1.0","source":{"id":"hep-lat/0407011","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0407011","created_at":"2026-05-18T00:36:57Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0407011v1","created_at":"2026-05-18T00:36:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0407011","created_at":"2026-05-18T00:36:57Z"},{"alias_kind":"pith_short_12","alias_value":"FIBMZPXNXL5E","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"FIBMZPXNXL5EXO5G","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"FIBMZPXN","created_at":"2026-05-18T12:25:52Z"}],"graph_snapshots":[{"event_id":"sha256:cc8c62963eebcad586fcaf1f45df946ba43b3a9cfc3e2bcd789439ffa04aca80","target":"graph","created_at":"2026-05-18T00:36:57Z","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":"Using SU(3) lattice QCD, we perform the first systematic study for the ground-state three-quark (3Q) potential $V_{\\rm 3Q}^{\\rm g.s.}$ and the 1st excited-state 3Q potential $V_{\\rm 3Q}^{\\rm e.s.}$, {\\it i.e.}, the energies of the ground state and the 1st excited state of the gluon field in the presence of the static three quarks. From the accurate and thorough calculation for more than 300 different patterns of 3Q systems, the static ground-state 3Q potential $V_{\\rm 3Q}^{\\rm g.s.}$ is found to be well described by the Coulomb plus Y-type linear potential, {\\it i.e.}, Y-Ansatz, within 1%-leve","authors_text":"Hideo Suganuma, Hiroko Ichie, Toru T. Takahashi","cross_cats":[],"headline":"","license":"","primary_cat":"hep-lat","submitted_at":"2004-07-07T10:31:58Z","title":"Y-type Flux-Tube Formation and Gluonic Excitations in Baryons: From QCD to Quark Model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0407011","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":"sha256:8329de4976430a83f6a38f55e206a5a1baf2f0e3e6e28c75b51d92d5c01c4066","target":"record","created_at":"2026-05-18T00:36:57Z","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":"0b4c031068d43a819103cd38303be57b4317ffd1700625094abeac31a8735592","cross_cats_sorted":[],"license":"","primary_cat":"hep-lat","submitted_at":"2004-07-07T10:31:58Z","title_canon_sha256":"162a8c58480027acc95b46abf0222ad6ca9536d0c7b11903b88684bb193847f3"},"schema_version":"1.0","source":{"id":"hep-lat/0407011","kind":"arxiv","version":1}},"canonical_sha256":"2a02ccbeedbafa4bbba65472faa1229ac321b9c08d85d50d2d589d0d36f5ecb3","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2a02ccbeedbafa4bbba65472faa1229ac321b9c08d85d50d2d589d0d36f5ecb3","first_computed_at":"2026-05-18T00:36:57.690419Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:36:57.690419Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"1uuxC8VLggSkghWNbwets02GTFgKdYOz2RDXi/aB8mgMAJAFDNZnDZPh/c5DbT3AeBP1dX5BpCAwpduJ9cH0Bw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:36:57.691015Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-lat/0407011","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8329de4976430a83f6a38f55e206a5a1baf2f0e3e6e28c75b51d92d5c01c4066","sha256:cc8c62963eebcad586fcaf1f45df946ba43b3a9cfc3e2bcd789439ffa04aca80"],"state_sha256":"f31499a856d72e25ab11bba8bd91c3fc2c63b730492ea617814a87e9c48176c7"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"x7merClPf1ZYvG2y34lSMd+JXNa4u+6rKY9Gbg1FP+c7EJAGgwGzhtGgg5KLZmK1IjwKXqH4qN6gVOe3zIR3CQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-20T08:40:43.300454Z","bundle_sha256":"fd92747dc19976356f23335cb168fc71e27de87d0c3551e976fb4107fdcc223f"}}