{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:6LRKCYII4HVHNRM6NB73RBTL4T","short_pith_number":"pith:6LRKCYII","schema_version":"1.0","canonical_sha256":"f2e2a16108e1ea76c59e687fb8866be4f26f3323413f9feb66cdfba242d1ff55","source":{"kind":"arxiv","id":"1803.04123","version":1},"attestation_state":"computed","paper":{"title":"Characterization of quark gluon plasma as seen through the energy loss of heavy quarks","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Ashik Ikbal Sheikh, Zubayer Ahammed","submitted_at":"2018-03-12T06:01:13Z","abstract_excerpt":"The shear viscosity to entropy density ratio ({\\eta}/s) of quark gluon plasma produced in ultra- relativistic heavy-ion collisions has been studied from the energy loss of heavy quarks in QGP medium. We have also studied the bulk viscosity to entropy density ratio ({\\zeta}/s) and fluidity measure(F) of the medium using the obtained {\\eta}/s values. In addition to that, we have estimated the heavy quark bound state potential (V) inside this medium. Our finding of {\\eta}/s agrees well with the results obtained by Lattice QCD (LQCD) and functional renormalization group technique."},"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":"1803.04123","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-03-12T06:01:13Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"cbfee6928019a505f7206448c01a0b733b18c4079105244a21ff271f5321f070","abstract_canon_sha256":"781ad485ed8c38cfa4a6173e60d7dc0f31746d40d020fcf64e10ee3428985add"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:21:32.582448Z","signature_b64":"5jp9AwFYn7tKP+CV3l6Wx/S8Lwwu/2QkMYAuSYs3vL+1Dyr76pTwxGA0ABJy9zfD+vNsL1uvHzxbDqubMtxUAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f2e2a16108e1ea76c59e687fb8866be4f26f3323413f9feb66cdfba242d1ff55","last_reissued_at":"2026-05-18T00:21:32.581767Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:21:32.581767Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Characterization of quark gluon plasma as seen through the energy loss of heavy quarks","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Ashik Ikbal Sheikh, Zubayer Ahammed","submitted_at":"2018-03-12T06:01:13Z","abstract_excerpt":"The shear viscosity to entropy density ratio ({\\eta}/s) of quark gluon plasma produced in ultra- relativistic heavy-ion collisions has been studied from the energy loss of heavy quarks in QGP medium. We have also studied the bulk viscosity to entropy density ratio ({\\zeta}/s) and fluidity measure(F) of the medium using the obtained {\\eta}/s values. In addition to that, we have estimated the heavy quark bound state potential (V) inside this medium. Our finding of {\\eta}/s agrees well with the results obtained by Lattice QCD (LQCD) and functional renormalization group technique."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1803.04123","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":"1803.04123","created_at":"2026-05-18T00:21:32.581867+00:00"},{"alias_kind":"arxiv_version","alias_value":"1803.04123v1","created_at":"2026-05-18T00:21:32.581867+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1803.04123","created_at":"2026-05-18T00:21:32.581867+00:00"},{"alias_kind":"pith_short_12","alias_value":"6LRKCYII4HVH","created_at":"2026-05-18T12:32:11.075285+00:00"},{"alias_kind":"pith_short_16","alias_value":"6LRKCYII4HVHNRM6","created_at":"2026-05-18T12:32:11.075285+00:00"},{"alias_kind":"pith_short_8","alias_value":"6LRKCYII","created_at":"2026-05-18T12:32:11.075285+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/6LRKCYII4HVHNRM6NB73RBTL4T","json":"https://pith.science/pith/6LRKCYII4HVHNRM6NB73RBTL4T.json","graph_json":"https://pith.science/api/pith-number/6LRKCYII4HVHNRM6NB73RBTL4T/graph.json","events_json":"https://pith.science/api/pith-number/6LRKCYII4HVHNRM6NB73RBTL4T/events.json","paper":"https://pith.science/paper/6LRKCYII"},"agent_actions":{"view_html":"https://pith.science/pith/6LRKCYII4HVHNRM6NB73RBTL4T","download_json":"https://pith.science/pith/6LRKCYII4HVHNRM6NB73RBTL4T.json","view_paper":"https://pith.science/paper/6LRKCYII","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1803.04123&json=true","fetch_graph":"https://pith.science/api/pith-number/6LRKCYII4HVHNRM6NB73RBTL4T/graph.json","fetch_events":"https://pith.science/api/pith-number/6LRKCYII4HVHNRM6NB73RBTL4T/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6LRKCYII4HVHNRM6NB73RBTL4T/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6LRKCYII4HVHNRM6NB73RBTL4T/action/storage_attestation","attest_author":"https://pith.science/pith/6LRKCYII4HVHNRM6NB73RBTL4T/action/author_attestation","sign_citation":"https://pith.science/pith/6LRKCYII4HVHNRM6NB73RBTL4T/action/citation_signature","submit_replication":"https://pith.science/pith/6LRKCYII4HVHNRM6NB73RBTL4T/action/replication_record"}},"created_at":"2026-05-18T00:21:32.581867+00:00","updated_at":"2026-05-18T00:21:32.581867+00:00"}