{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:TNQK26YCCRRE2FHFZWNU6WJPCF","short_pith_number":"pith:TNQK26YC","schema_version":"1.0","canonical_sha256":"9b60ad7b0214624d14e5cd9b4f592f114d0530f5a1aaf6a72a327550935071d2","source":{"kind":"arxiv","id":"1108.5887","version":1},"attestation_state":"computed","paper":{"title":"A Ginzburg-Landau model of knotted flux-tube and glueball-like $f_{J}$ mesons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Duojie Jia, Yi-Ping Lu","submitted_at":"2011-08-30T09:20:41Z","abstract_excerpt":"A dual Ginzburg-Landau model of the knotted chromo-electric flux-tube is revisited, in which the covariant decomposition of gluon field and the random phase approximation are used. It is shown that the SU(2) QCD vacuum is of type-II superconductor, with the Ginzburg-Landau parameter $\\kappa = \\sqrt{3}$, being independent of the magnetic condensate and strong coupling used, and consistent with the lattice data. The mass spectrum of a number of $f_{J}$ meson states with $J\\leq 2$, which are taken to be of glue dominate, are computed with help of the energies of the knotted(linked) QCD fluxtubes."},"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":"1108.5887","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-08-30T09:20:41Z","cross_cats_sorted":[],"title_canon_sha256":"c54488d6f7b502cac6a2ab48b741c1d48ce5442c4400ed45236a15fc3d78dad0","abstract_canon_sha256":"dcb847bbedac3ec99e43bfeaa5f28c37c9f3761adcb7d6973cafec11d7e37196"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:14:28.290579Z","signature_b64":"92ZpZ1+rlYUThgstuxkUjpUpSaNJzsU7qYMGFP9NvDBeCtDXFoGZUI2RdgsZY1C89eOg8x0wtwLqhdxWG8FeBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9b60ad7b0214624d14e5cd9b4f592f114d0530f5a1aaf6a72a327550935071d2","last_reissued_at":"2026-05-18T04:14:28.290016Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:14:28.290016Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A Ginzburg-Landau model of knotted flux-tube and glueball-like $f_{J}$ mesons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Duojie Jia, Yi-Ping Lu","submitted_at":"2011-08-30T09:20:41Z","abstract_excerpt":"A dual Ginzburg-Landau model of the knotted chromo-electric flux-tube is revisited, in which the covariant decomposition of gluon field and the random phase approximation are used. It is shown that the SU(2) QCD vacuum is of type-II superconductor, with the Ginzburg-Landau parameter $\\kappa = \\sqrt{3}$, being independent of the magnetic condensate and strong coupling used, and consistent with the lattice data. The mass spectrum of a number of $f_{J}$ meson states with $J\\leq 2$, which are taken to be of glue dominate, are computed with help of the energies of the knotted(linked) QCD fluxtubes."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1108.5887","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":"1108.5887","created_at":"2026-05-18T04:14:28.290081+00:00"},{"alias_kind":"arxiv_version","alias_value":"1108.5887v1","created_at":"2026-05-18T04:14:28.290081+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1108.5887","created_at":"2026-05-18T04:14:28.290081+00:00"},{"alias_kind":"pith_short_12","alias_value":"TNQK26YCCRRE","created_at":"2026-05-18T12:26:42.757692+00:00"},{"alias_kind":"pith_short_16","alias_value":"TNQK26YCCRRE2FHF","created_at":"2026-05-18T12:26:42.757692+00:00"},{"alias_kind":"pith_short_8","alias_value":"TNQK26YC","created_at":"2026-05-18T12:26:42.757692+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/TNQK26YCCRRE2FHFZWNU6WJPCF","json":"https://pith.science/pith/TNQK26YCCRRE2FHFZWNU6WJPCF.json","graph_json":"https://pith.science/api/pith-number/TNQK26YCCRRE2FHFZWNU6WJPCF/graph.json","events_json":"https://pith.science/api/pith-number/TNQK26YCCRRE2FHFZWNU6WJPCF/events.json","paper":"https://pith.science/paper/TNQK26YC"},"agent_actions":{"view_html":"https://pith.science/pith/TNQK26YCCRRE2FHFZWNU6WJPCF","download_json":"https://pith.science/pith/TNQK26YCCRRE2FHFZWNU6WJPCF.json","view_paper":"https://pith.science/paper/TNQK26YC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1108.5887&json=true","fetch_graph":"https://pith.science/api/pith-number/TNQK26YCCRRE2FHFZWNU6WJPCF/graph.json","fetch_events":"https://pith.science/api/pith-number/TNQK26YCCRRE2FHFZWNU6WJPCF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TNQK26YCCRRE2FHFZWNU6WJPCF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TNQK26YCCRRE2FHFZWNU6WJPCF/action/storage_attestation","attest_author":"https://pith.science/pith/TNQK26YCCRRE2FHFZWNU6WJPCF/action/author_attestation","sign_citation":"https://pith.science/pith/TNQK26YCCRRE2FHFZWNU6WJPCF/action/citation_signature","submit_replication":"https://pith.science/pith/TNQK26YCCRRE2FHFZWNU6WJPCF/action/replication_record"}},"created_at":"2026-05-18T04:14:28.290081+00:00","updated_at":"2026-05-18T04:14:28.290081+00:00"}