{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1995:BU4V5NNCEBUHU2YL7TBUKMIWIC","short_pith_number":"pith:BU4V5NNC","schema_version":"1.0","canonical_sha256":"0d395eb5a220687a6b0bfcc3453116409a7f777f8aef0e40cdb418639dcc0504","source":{"kind":"arxiv","id":"hep-ph/9502235","version":1},"attestation_state":"computed","paper":{"title":"Glueball Masses in QCD_3","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Qi-Zhou Chen, Shuo-Hong Guo, Xiang-Qian Luo, Xi-Yang Fang","submitted_at":"1995-02-06T14:05:47Z","abstract_excerpt":"We discuss how to extract the spectroscopy of quantum chromodynamics (QCD) in the pure gauge sector from the Hamiltonian lattice field theory approach. The recently developed truncated eigenvalue equation method is applied to the estimation of the scalar glueball $0^{++}$ and $0^{--}$ masses in the (2+1)-dimensional case. These masses reach the constant values in a scaling region as required by the renormalizability."},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"hep-ph/9502235","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1995-02-06T14:05:47Z","cross_cats_sorted":[],"title_canon_sha256":"40a2f50b6095d2e9e93e6923177adc7703e1119eb493f0bf0fd51a51b80a8b58","abstract_canon_sha256":"7157f3f858ce163ba4ec9d4ec020a3793cc921b3b2203299c84f710869f20d6c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:06:34.045859Z","signature_b64":"PdO+62eZbg66ZKcefAEAH8uwWQ3E2nwdXEtELZs4K2tzlSAv5vqa/l6kz1yVdGa6zxltI4fdQzl382Vk4fpiDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0d395eb5a220687a6b0bfcc3453116409a7f777f8aef0e40cdb418639dcc0504","last_reissued_at":"2026-05-18T01:06:34.045170Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:06:34.045170Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Glueball Masses in QCD_3","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Qi-Zhou Chen, Shuo-Hong Guo, Xiang-Qian Luo, Xi-Yang Fang","submitted_at":"1995-02-06T14:05:47Z","abstract_excerpt":"We discuss how to extract the spectroscopy of quantum chromodynamics (QCD) in the pure gauge sector from the Hamiltonian lattice field theory approach. The recently developed truncated eigenvalue equation method is applied to the estimation of the scalar glueball $0^{++}$ and $0^{--}$ masses in the (2+1)-dimensional case. These masses reach the constant values in a scaling region as required by the renormalizability."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9502235","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9502235","created_at":"2026-05-18T01:06:34.045274+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9502235v1","created_at":"2026-05-18T01:06:34.045274+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9502235","created_at":"2026-05-18T01:06:34.045274+00:00"},{"alias_kind":"pith_short_12","alias_value":"BU4V5NNCEBUH","created_at":"2026-05-18T12:25:47.700082+00:00"},{"alias_kind":"pith_short_16","alias_value":"BU4V5NNCEBUHU2YL","created_at":"2026-05-18T12:25:47.700082+00:00"},{"alias_kind":"pith_short_8","alias_value":"BU4V5NNC","created_at":"2026-05-18T12:25:47.700082+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/BU4V5NNCEBUHU2YL7TBUKMIWIC","json":"https://pith.science/pith/BU4V5NNCEBUHU2YL7TBUKMIWIC.json","graph_json":"https://pith.science/api/pith-number/BU4V5NNCEBUHU2YL7TBUKMIWIC/graph.json","events_json":"https://pith.science/api/pith-number/BU4V5NNCEBUHU2YL7TBUKMIWIC/events.json","paper":"https://pith.science/paper/BU4V5NNC"},"agent_actions":{"view_html":"https://pith.science/pith/BU4V5NNCEBUHU2YL7TBUKMIWIC","download_json":"https://pith.science/pith/BU4V5NNCEBUHU2YL7TBUKMIWIC.json","view_paper":"https://pith.science/paper/BU4V5NNC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9502235&json=true","fetch_graph":"https://pith.science/api/pith-number/BU4V5NNCEBUHU2YL7TBUKMIWIC/graph.json","fetch_events":"https://pith.science/api/pith-number/BU4V5NNCEBUHU2YL7TBUKMIWIC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BU4V5NNCEBUHU2YL7TBUKMIWIC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BU4V5NNCEBUHU2YL7TBUKMIWIC/action/storage_attestation","attest_author":"https://pith.science/pith/BU4V5NNCEBUHU2YL7TBUKMIWIC/action/author_attestation","sign_citation":"https://pith.science/pith/BU4V5NNCEBUHU2YL7TBUKMIWIC/action/citation_signature","submit_replication":"https://pith.science/pith/BU4V5NNCEBUHU2YL7TBUKMIWIC/action/replication_record"}},"created_at":"2026-05-18T01:06:34.045274+00:00","updated_at":"2026-05-18T01:06:34.045274+00:00"}