{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2003:MUNMUTBU6OHEQSWVHLCIBLXZFZ","short_pith_number":"pith:MUNMUTBU","canonical_record":{"source":{"id":"hep-ph/0310130","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2003-10-10T14:44:22Z","cross_cats_sorted":["hep-lat","hep-th"],"title_canon_sha256":"457e3084e364067587fa52b3d27f6fd891a03e2e02b25cf4201dc4b050ab2369","abstract_canon_sha256":"b68b263374e77a235df9b2ed317428940fea717d5bb959f2f4af30467d642033"},"schema_version":"1.0"},"canonical_sha256":"651aca4c34f38e484ad53ac480aef92e4c1b739bed600926b3a064cc1b62d245","source":{"kind":"arxiv","id":"hep-ph/0310130","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0310130","created_at":"2026-05-18T04:30:46Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0310130v1","created_at":"2026-05-18T04:30:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0310130","created_at":"2026-05-18T04:30:46Z"},{"alias_kind":"pith_short_12","alias_value":"MUNMUTBU6OHE","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"MUNMUTBU6OHEQSWV","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"MUNMUTBU","created_at":"2026-05-18T12:25:52Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2003:MUNMUTBU6OHEQSWVHLCIBLXZFZ","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/0310130","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2003-10-10T14:44:22Z","cross_cats_sorted":["hep-lat","hep-th"],"title_canon_sha256":"457e3084e364067587fa52b3d27f6fd891a03e2e02b25cf4201dc4b050ab2369","abstract_canon_sha256":"b68b263374e77a235df9b2ed317428940fea717d5bb959f2f4af30467d642033"},"schema_version":"1.0"},"canonical_sha256":"651aca4c34f38e484ad53ac480aef92e4c1b739bed600926b3a064cc1b62d245","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:30:46.114256Z","signature_b64":"rAojU58W3E2B2UVDRh8XvA2wreykSomHQ7A73wbw24rs3qhfibGB5N6uZvgOhcjM8die149XXaXUN91FhB1kDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"651aca4c34f38e484ad53ac480aef92e4c1b739bed600926b3a064cc1b62d245","last_reissued_at":"2026-05-18T04:30:46.113704Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:30:46.113704Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/0310130","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":"2026-05-18T04:30:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nFbeKJ1QV6Bn+9n155pHoh1Cs97lUJQ043KasU42r6qOscZeOnFQiNs1VD4fjrcXKzXO/iYteyNhUuSPqCGfCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-11T18:01:55.382558Z"},"content_sha256":"c72cce4118f06a80a6b52ff6332b0f08759f0f42511a0b81cfc0c678108b8c6d","schema_version":"1.0","event_id":"sha256:c72cce4118f06a80a6b52ff6332b0f08759f0f42511a0b81cfc0c678108b8c6d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2003:MUNMUTBU6OHEQSWVHLCIBLXZFZ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"QCD phenomenology of static sources and gluonic excitations at short distances","license":"","headline":"","cross_cats":["hep-lat","hep-th"],"primary_cat":"hep-ph","authors_text":"Antonio Pineda (Barcelona), Gunnar S. Bali (Glasgow)","submitted_at":"2003-10-10T14:44:22Z","abstract_excerpt":"New lattice data for the Pi_u and Sigma_u^- potentials at short distances are presented. We compare perturbation theory to the lower static hybrid potentials and find good agreement at short distances, once the renormalon ambiguities are accounted for. We use the non-perturbatively determined continuum-limit static hybrid and ground state potentials at short distances to determine the gluelump energies. The result is consistent with an estimate obtained from the gluelump data at finite lattice spacings. For the lightest gluelump, we obtain Lambda_B^{RS}(nu_f=2.5/r_0)=[2.25\\pm 0.10(latt.)\\pm 0."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0310130","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":"2026-05-18T04:30:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"sAekC14iTXttIOWwDmhj3JF2G4LfkN8Pobjqjib4CYcrB5B7TR46tSBs/Zhg9/nZ40T+/HN+x8ec6IZRMdu+Cw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-11T18:01:55.383524Z"},"content_sha256":"a47d71f537467ae825d62a502eb5a71a808c5932fc3942ada614bff260a7e207","schema_version":"1.0","event_id":"sha256:a47d71f537467ae825d62a502eb5a71a808c5932fc3942ada614bff260a7e207"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/MUNMUTBU6OHEQSWVHLCIBLXZFZ/bundle.json","state_url":"https://pith.science/pith/MUNMUTBU6OHEQSWVHLCIBLXZFZ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/MUNMUTBU6OHEQSWVHLCIBLXZFZ/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":"2026-08-11T18:01:55Z","links":{"resolver":"https://pith.science/pith/MUNMUTBU6OHEQSWVHLCIBLXZFZ","bundle":"https://pith.science/pith/MUNMUTBU6OHEQSWVHLCIBLXZFZ/bundle.json","state":"https://pith.science/pith/MUNMUTBU6OHEQSWVHLCIBLXZFZ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/MUNMUTBU6OHEQSWVHLCIBLXZFZ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2003:MUNMUTBU6OHEQSWVHLCIBLXZFZ","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":"b68b263374e77a235df9b2ed317428940fea717d5bb959f2f4af30467d642033","cross_cats_sorted":["hep-lat","hep-th"],"license":"","primary_cat":"hep-ph","submitted_at":"2003-10-10T14:44:22Z","title_canon_sha256":"457e3084e364067587fa52b3d27f6fd891a03e2e02b25cf4201dc4b050ab2369"},"schema_version":"1.0","source":{"id":"hep-ph/0310130","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0310130","created_at":"2026-05-18T04:30:46Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0310130v1","created_at":"2026-05-18T04:30:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0310130","created_at":"2026-05-18T04:30:46Z"},{"alias_kind":"pith_short_12","alias_value":"MUNMUTBU6OHE","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"MUNMUTBU6OHEQSWV","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"MUNMUTBU","created_at":"2026-05-18T12:25:52Z"}],"graph_snapshots":[{"event_id":"sha256:a47d71f537467ae825d62a502eb5a71a808c5932fc3942ada614bff260a7e207","target":"graph","created_at":"2026-05-18T04:30:46Z","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":"New lattice data for the Pi_u and Sigma_u^- potentials at short distances are presented. We compare perturbation theory to the lower static hybrid potentials and find good agreement at short distances, once the renormalon ambiguities are accounted for. We use the non-perturbatively determined continuum-limit static hybrid and ground state potentials at short distances to determine the gluelump energies. The result is consistent with an estimate obtained from the gluelump data at finite lattice spacings. For the lightest gluelump, we obtain Lambda_B^{RS}(nu_f=2.5/r_0)=[2.25\\pm 0.10(latt.)\\pm 0.","authors_text":"Antonio Pineda (Barcelona), Gunnar S. Bali (Glasgow)","cross_cats":["hep-lat","hep-th"],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"2003-10-10T14:44:22Z","title":"QCD phenomenology of static sources and gluonic excitations at short distances"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0310130","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:c72cce4118f06a80a6b52ff6332b0f08759f0f42511a0b81cfc0c678108b8c6d","target":"record","created_at":"2026-05-18T04:30:46Z","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":"b68b263374e77a235df9b2ed317428940fea717d5bb959f2f4af30467d642033","cross_cats_sorted":["hep-lat","hep-th"],"license":"","primary_cat":"hep-ph","submitted_at":"2003-10-10T14:44:22Z","title_canon_sha256":"457e3084e364067587fa52b3d27f6fd891a03e2e02b25cf4201dc4b050ab2369"},"schema_version":"1.0","source":{"id":"hep-ph/0310130","kind":"arxiv","version":1}},"canonical_sha256":"651aca4c34f38e484ad53ac480aef92e4c1b739bed600926b3a064cc1b62d245","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"651aca4c34f38e484ad53ac480aef92e4c1b739bed600926b3a064cc1b62d245","first_computed_at":"2026-05-18T04:30:46.113704Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:30:46.113704Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"rAojU58W3E2B2UVDRh8XvA2wreykSomHQ7A73wbw24rs3qhfibGB5N6uZvgOhcjM8die149XXaXUN91FhB1kDw==","signature_status":"signed_v1","signed_at":"2026-05-18T04:30:46.114256Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/0310130","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c72cce4118f06a80a6b52ff6332b0f08759f0f42511a0b81cfc0c678108b8c6d","sha256:a47d71f537467ae825d62a502eb5a71a808c5932fc3942ada614bff260a7e207"],"state_sha256":"17cb7f3627212fdadb3b8b693318429c73b4881a6ecc7a720740a03686b106de"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WfWBxsd1wlK5Zn2c1HSwjhEt2Ybf0tYzNzpmWjt66dPju6ri3FriGD+TQZK7dwxVARySJ9i403ls8sha02pmBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-11T18:01:55.389899Z","bundle_sha256":"0e3b91eb0029c846c8fd2f7d943597b7e6ec3884b522dbf75a5771597503857b"}}