{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:RIPGCZBXKBF3PL2SWRVR2OTZ3M","short_pith_number":"pith:RIPGCZBX","schema_version":"1.0","canonical_sha256":"8a1e616437504bb7af52b46b1d3a79db01560ae11e9ab849a24e6b8d3ce75d36","source":{"kind":"arxiv","id":"1706.06270","version":3},"attestation_state":"computed","paper":{"title":"Dynamical gluon mass in the instanton vacuum model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"M. Musakhanov, O. Egamberdiev","submitted_at":"2017-06-20T05:01:47Z","abstract_excerpt":"We are considering the modifications of gluon properties in Instanton Liquid Model (ILM) for the QCD vacuum. Re-scattering of a gluons on an instantons leads to the dynamical momentum-dependent gluon mass $M_g(q).$ First, we considered scalar \"gluon\", since there are no zero-modes problem and found its dynamical mass $M_s(q)$. At the typical phenomenological values of the average instanton size $\\rho=1/3\\,\\,fm$ and average inter-instanton distance $R=1\\,\\, fm$ we got $M_s(0)=256\\,\\,MeV$. Further, we extended this approach to the real vector gluon with careful consideration of zero-modes and go"},"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":"1706.06270","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-06-20T05:01:47Z","cross_cats_sorted":[],"title_canon_sha256":"cdc5cdcb86faf5b7724ef1979d038185051ed15ec4c90a9b409ea08a07323da6","abstract_canon_sha256":"61ba397b5d69d0498856fe25b9e67a5c6650affd3e0979f2af2af3cfc5212385"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:24:17.290414Z","signature_b64":"zG7r5KHmCOrBV5n/IMfblCFLklHGkbxrQmxGcCt8qz9Yu8WfRnO20hYfeHDr5+KFbNAhrMNITGdRNCLqj2ggCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8a1e616437504bb7af52b46b1d3a79db01560ae11e9ab849a24e6b8d3ce75d36","last_reissued_at":"2026-05-18T00:24:17.289784Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:24:17.289784Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dynamical gluon mass in the instanton vacuum model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"M. Musakhanov, O. Egamberdiev","submitted_at":"2017-06-20T05:01:47Z","abstract_excerpt":"We are considering the modifications of gluon properties in Instanton Liquid Model (ILM) for the QCD vacuum. Re-scattering of a gluons on an instantons leads to the dynamical momentum-dependent gluon mass $M_g(q).$ First, we considered scalar \"gluon\", since there are no zero-modes problem and found its dynamical mass $M_s(q)$. At the typical phenomenological values of the average instanton size $\\rho=1/3\\,\\,fm$ and average inter-instanton distance $R=1\\,\\, fm$ we got $M_s(0)=256\\,\\,MeV$. Further, we extended this approach to the real vector gluon with careful consideration of zero-modes and go"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.06270","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1706.06270","created_at":"2026-05-18T00:24:17.289884+00:00"},{"alias_kind":"arxiv_version","alias_value":"1706.06270v3","created_at":"2026-05-18T00:24:17.289884+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.06270","created_at":"2026-05-18T00:24:17.289884+00:00"},{"alias_kind":"pith_short_12","alias_value":"RIPGCZBXKBF3","created_at":"2026-05-18T12:31:39.905425+00:00"},{"alias_kind":"pith_short_16","alias_value":"RIPGCZBXKBF3PL2S","created_at":"2026-05-18T12:31:39.905425+00:00"},{"alias_kind":"pith_short_8","alias_value":"RIPGCZBX","created_at":"2026-05-18T12:31:39.905425+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.04803","citing_title":"Glueballs, Constituent Gluons and Instantons","ref_index":27,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/RIPGCZBXKBF3PL2SWRVR2OTZ3M","json":"https://pith.science/pith/RIPGCZBXKBF3PL2SWRVR2OTZ3M.json","graph_json":"https://pith.science/api/pith-number/RIPGCZBXKBF3PL2SWRVR2OTZ3M/graph.json","events_json":"https://pith.science/api/pith-number/RIPGCZBXKBF3PL2SWRVR2OTZ3M/events.json","paper":"https://pith.science/paper/RIPGCZBX"},"agent_actions":{"view_html":"https://pith.science/pith/RIPGCZBXKBF3PL2SWRVR2OTZ3M","download_json":"https://pith.science/pith/RIPGCZBXKBF3PL2SWRVR2OTZ3M.json","view_paper":"https://pith.science/paper/RIPGCZBX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1706.06270&json=true","fetch_graph":"https://pith.science/api/pith-number/RIPGCZBXKBF3PL2SWRVR2OTZ3M/graph.json","fetch_events":"https://pith.science/api/pith-number/RIPGCZBXKBF3PL2SWRVR2OTZ3M/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RIPGCZBXKBF3PL2SWRVR2OTZ3M/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RIPGCZBXKBF3PL2SWRVR2OTZ3M/action/storage_attestation","attest_author":"https://pith.science/pith/RIPGCZBXKBF3PL2SWRVR2OTZ3M/action/author_attestation","sign_citation":"https://pith.science/pith/RIPGCZBXKBF3PL2SWRVR2OTZ3M/action/citation_signature","submit_replication":"https://pith.science/pith/RIPGCZBXKBF3PL2SWRVR2OTZ3M/action/replication_record"}},"created_at":"2026-05-18T00:24:17.289884+00:00","updated_at":"2026-05-18T00:24:17.289884+00:00"}