{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:KYH3HKLBZGUMFBSVLIJSDAY2BO","short_pith_number":"pith:KYH3HKLB","canonical_record":{"source":{"id":"1411.1083","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-11-04T21:10:04Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"1ffcbfe2705a4c51866ef9d34f56954a9b046637f82b5fe2552d64fe1d875fad","abstract_canon_sha256":"f62c31f2b332b95f41c5d25b7a7cc1551091d7f471460c5dbc7ebaad4c6acab9"},"schema_version":"1.0"},"canonical_sha256":"560fb3a961c9a8c286555a1321831a0ba3aac68fa2859499eb17cf5289d4fa1d","source":{"kind":"arxiv","id":"1411.1083","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1411.1083","created_at":"2026-05-18T01:37:35Z"},{"alias_kind":"arxiv_version","alias_value":"1411.1083v3","created_at":"2026-05-18T01:37:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1411.1083","created_at":"2026-05-18T01:37:35Z"},{"alias_kind":"pith_short_12","alias_value":"KYH3HKLBZGUM","created_at":"2026-05-18T12:28:35Z"},{"alias_kind":"pith_short_16","alias_value":"KYH3HKLBZGUMFBSV","created_at":"2026-05-18T12:28:35Z"},{"alias_kind":"pith_short_8","alias_value":"KYH3HKLB","created_at":"2026-05-18T12:28:35Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:KYH3HKLBZGUMFBSVLIJSDAY2BO","target":"record","payload":{"canonical_record":{"source":{"id":"1411.1083","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-11-04T21:10:04Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"1ffcbfe2705a4c51866ef9d34f56954a9b046637f82b5fe2552d64fe1d875fad","abstract_canon_sha256":"f62c31f2b332b95f41c5d25b7a7cc1551091d7f471460c5dbc7ebaad4c6acab9"},"schema_version":"1.0"},"canonical_sha256":"560fb3a961c9a8c286555a1321831a0ba3aac68fa2859499eb17cf5289d4fa1d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:37:35.454467Z","signature_b64":"t/KRG7TjuwT3VvB0lypgNIZXpr8F04lxcj6/pxiUTRO3g8CQjK/fCz3V5R7y0PDrAsqi5BVGIs9lPq0biSRHDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"560fb3a961c9a8c286555a1321831a0ba3aac68fa2859499eb17cf5289d4fa1d","last_reissued_at":"2026-05-18T01:37:35.454011Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:37:35.454011Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1411.1083","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:37:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"NVJ09lOfv7agr/MeXHvqALsIcgUonHGjB36ElRGEE+jBGa9MnISqA3CkcKB32mq50yZuniwdB4/rZ1extcYmDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T22:29:09.650036Z"},"content_sha256":"25d0e70059975ee8698d184a18ed0992203947e34660ef7d3093b6fa610a4cbf","schema_version":"1.0","event_id":"sha256:25d0e70059975ee8698d184a18ed0992203947e34660ef7d3093b6fa610a4cbf"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:KYH3HKLBZGUMFBSVLIJSDAY2BO","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Wave functions of $SU(3)$ pure gauge glueballs on the lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Jian Liang, Long-Cheng Gui, Ming Gong, Wei-Feng Chiu, Ying Chen, Zhaofeng Liu","submitted_at":"2014-11-04T21:10:04Z","abstract_excerpt":"The Bethe-Salpeter wave functions of $SU(3)$ pure gauge glueballs are revisited in this study. The ground and the first excited states of scalar and tensor glueballs are identified unambiguously by using the variational method on the basis of large operator sets. We calculate their wave functions in the Coulomb gauge and use two lattices with different lattice spacings to check the discretization artifacts. For ground states, the radial wave functions are approximately Gaussian and the size of the tensor is twice as large as that of the scalar. For the first excited states, the radial nodes ar"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1411.1083","kind":"arxiv","version":3},"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":"2026-05-18T01:37:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"IhPs5xe6ACA/I/eoXW1OnaYcEDadN60389bG5yCQeDGb70uAloiR9BOoNdWwTweXRVPMsdFRGdkKC+IO/iTVAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T22:29:09.650696Z"},"content_sha256":"5a0036a617757d3750a3416161556654849ed90373284c1591ead0ef3565304d","schema_version":"1.0","event_id":"sha256:5a0036a617757d3750a3416161556654849ed90373284c1591ead0ef3565304d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/KYH3HKLBZGUMFBSVLIJSDAY2BO/bundle.json","state_url":"https://pith.science/pith/KYH3HKLBZGUMFBSVLIJSDAY2BO/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/KYH3HKLBZGUMFBSVLIJSDAY2BO/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":"2026-05-25T22:29:09Z","links":{"resolver":"https://pith.science/pith/KYH3HKLBZGUMFBSVLIJSDAY2BO","bundle":"https://pith.science/pith/KYH3HKLBZGUMFBSVLIJSDAY2BO/bundle.json","state":"https://pith.science/pith/KYH3HKLBZGUMFBSVLIJSDAY2BO/state.json","well_known_bundle":"https://pith.science/.well-known/pith/KYH3HKLBZGUMFBSVLIJSDAY2BO/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:KYH3HKLBZGUMFBSVLIJSDAY2BO","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":"f62c31f2b332b95f41c5d25b7a7cc1551091d7f471460c5dbc7ebaad4c6acab9","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-11-04T21:10:04Z","title_canon_sha256":"1ffcbfe2705a4c51866ef9d34f56954a9b046637f82b5fe2552d64fe1d875fad"},"schema_version":"1.0","source":{"id":"1411.1083","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1411.1083","created_at":"2026-05-18T01:37:35Z"},{"alias_kind":"arxiv_version","alias_value":"1411.1083v3","created_at":"2026-05-18T01:37:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1411.1083","created_at":"2026-05-18T01:37:35Z"},{"alias_kind":"pith_short_12","alias_value":"KYH3HKLBZGUM","created_at":"2026-05-18T12:28:35Z"},{"alias_kind":"pith_short_16","alias_value":"KYH3HKLBZGUMFBSV","created_at":"2026-05-18T12:28:35Z"},{"alias_kind":"pith_short_8","alias_value":"KYH3HKLB","created_at":"2026-05-18T12:28:35Z"}],"graph_snapshots":[{"event_id":"sha256:5a0036a617757d3750a3416161556654849ed90373284c1591ead0ef3565304d","target":"graph","created_at":"2026-05-18T01:37:35Z","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":"The Bethe-Salpeter wave functions of $SU(3)$ pure gauge glueballs are revisited in this study. The ground and the first excited states of scalar and tensor glueballs are identified unambiguously by using the variational method on the basis of large operator sets. We calculate their wave functions in the Coulomb gauge and use two lattices with different lattice spacings to check the discretization artifacts. For ground states, the radial wave functions are approximately Gaussian and the size of the tensor is twice as large as that of the scalar. For the first excited states, the radial nodes ar","authors_text":"Jian Liang, Long-Cheng Gui, Ming Gong, Wei-Feng Chiu, Ying Chen, Zhaofeng Liu","cross_cats":["hep-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-11-04T21:10:04Z","title":"Wave functions of $SU(3)$ pure gauge glueballs on the lattice"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1411.1083","kind":"arxiv","version":3},"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":"sha256:25d0e70059975ee8698d184a18ed0992203947e34660ef7d3093b6fa610a4cbf","target":"record","created_at":"2026-05-18T01:37:35Z","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":"f62c31f2b332b95f41c5d25b7a7cc1551091d7f471460c5dbc7ebaad4c6acab9","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-11-04T21:10:04Z","title_canon_sha256":"1ffcbfe2705a4c51866ef9d34f56954a9b046637f82b5fe2552d64fe1d875fad"},"schema_version":"1.0","source":{"id":"1411.1083","kind":"arxiv","version":3}},"canonical_sha256":"560fb3a961c9a8c286555a1321831a0ba3aac68fa2859499eb17cf5289d4fa1d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"560fb3a961c9a8c286555a1321831a0ba3aac68fa2859499eb17cf5289d4fa1d","first_computed_at":"2026-05-18T01:37:35.454011Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:37:35.454011Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"t/KRG7TjuwT3VvB0lypgNIZXpr8F04lxcj6/pxiUTRO3g8CQjK/fCz3V5R7y0PDrAsqi5BVGIs9lPq0biSRHDg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:37:35.454467Z","signed_message":"canonical_sha256_bytes"},"source_id":"1411.1083","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:25d0e70059975ee8698d184a18ed0992203947e34660ef7d3093b6fa610a4cbf","sha256:5a0036a617757d3750a3416161556654849ed90373284c1591ead0ef3565304d"],"state_sha256":"52d70e83fc3ed0d439d55e96b9e98c9bc7a4b2990d3c0ee07c652b2d61b8323c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UAUVtnuAXTumq+2UAHDkCij5YQgFejYrziBZI4gPNEkFONLEGJhNVq15TB1EG4NYRErgUlm58Y6pAmRnSiJOAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T22:29:09.654223Z","bundle_sha256":"ae357eab7a31643a0b902ed03dff89ee22997b2409b7f1022922daf634912d6e"}}