{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:OKJPSAQF57BDTN7425XQ3CU6WK","short_pith_number":"pith:OKJPSAQF","schema_version":"1.0","canonical_sha256":"7292f90205efc239b7fcd76f0d8a9eb2a38e593ad15181767188ab012b71196e","source":{"kind":"arxiv","id":"1603.01952","version":2},"attestation_state":"computed","paper":{"title":"Estimating transport coefficients in hot and dense quark matter","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Guru Prakash Kadam, Hiranmaya Mishra, Paramita Deb","submitted_at":"2016-03-07T06:26:02Z","abstract_excerpt":"We compute the transport coefficients, namely, the coefficients of shear and bulk viscosity as well as thermal conductivity for hot and dense quark matter. The calculations are performed within the Nambu- Jona Lasinio (NJL) model. The estimation of the transport coefficients is made using a quasiparticle approach of solving the Boltzmann kinetic equation within the relaxation time approximation. The transition rates are calculated in a manifestly covariant manner to estimate the thermal-averaged cross sections for quark-quark and quark-antiquark scattering. The calculations are performed for f"},"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":"1603.01952","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-03-07T06:26:02Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"cfc35d54cb4b02860a03897ead4fcbce7a1d0c3097cc352f146d2c8de2843f43","abstract_canon_sha256":"ba4b2619e8aaceb891e9abbf80004857ead8bc5fa1f021a1b6812a134b60bdec"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:59:58.689827Z","signature_b64":"eqslYvQ8ppzj1619sGp2y5NOqNBX/I7O7sIubmn0Jr8rs1P2LPC/4Vmww1n/rcttFRho2UIm1pUEvXFsMLrGCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7292f90205efc239b7fcd76f0d8a9eb2a38e593ad15181767188ab012b71196e","last_reissued_at":"2026-05-18T00:59:58.689361Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:59:58.689361Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Estimating transport coefficients in hot and dense quark matter","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Guru Prakash Kadam, Hiranmaya Mishra, Paramita Deb","submitted_at":"2016-03-07T06:26:02Z","abstract_excerpt":"We compute the transport coefficients, namely, the coefficients of shear and bulk viscosity as well as thermal conductivity for hot and dense quark matter. The calculations are performed within the Nambu- Jona Lasinio (NJL) model. The estimation of the transport coefficients is made using a quasiparticle approach of solving the Boltzmann kinetic equation within the relaxation time approximation. The transition rates are calculated in a manifestly covariant manner to estimate the thermal-averaged cross sections for quark-quark and quark-antiquark scattering. The calculations are performed for f"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1603.01952","kind":"arxiv","version":2},"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":"1603.01952","created_at":"2026-05-18T00:59:58.689430+00:00"},{"alias_kind":"arxiv_version","alias_value":"1603.01952v2","created_at":"2026-05-18T00:59:58.689430+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1603.01952","created_at":"2026-05-18T00:59:58.689430+00:00"},{"alias_kind":"pith_short_12","alias_value":"OKJPSAQF57BD","created_at":"2026-05-18T12:30:36.002864+00:00"},{"alias_kind":"pith_short_16","alias_value":"OKJPSAQF57BDTN74","created_at":"2026-05-18T12:30:36.002864+00:00"},{"alias_kind":"pith_short_8","alias_value":"OKJPSAQF","created_at":"2026-05-18T12:30:36.002864+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2606.09633","citing_title":"Effective QCD model with consistent quasi-gluon treatment : formulation and application","ref_index":109,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/OKJPSAQF57BDTN7425XQ3CU6WK","json":"https://pith.science/pith/OKJPSAQF57BDTN7425XQ3CU6WK.json","graph_json":"https://pith.science/api/pith-number/OKJPSAQF57BDTN7425XQ3CU6WK/graph.json","events_json":"https://pith.science/api/pith-number/OKJPSAQF57BDTN7425XQ3CU6WK/events.json","paper":"https://pith.science/paper/OKJPSAQF"},"agent_actions":{"view_html":"https://pith.science/pith/OKJPSAQF57BDTN7425XQ3CU6WK","download_json":"https://pith.science/pith/OKJPSAQF57BDTN7425XQ3CU6WK.json","view_paper":"https://pith.science/paper/OKJPSAQF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1603.01952&json=true","fetch_graph":"https://pith.science/api/pith-number/OKJPSAQF57BDTN7425XQ3CU6WK/graph.json","fetch_events":"https://pith.science/api/pith-number/OKJPSAQF57BDTN7425XQ3CU6WK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OKJPSAQF57BDTN7425XQ3CU6WK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OKJPSAQF57BDTN7425XQ3CU6WK/action/storage_attestation","attest_author":"https://pith.science/pith/OKJPSAQF57BDTN7425XQ3CU6WK/action/author_attestation","sign_citation":"https://pith.science/pith/OKJPSAQF57BDTN7425XQ3CU6WK/action/citation_signature","submit_replication":"https://pith.science/pith/OKJPSAQF57BDTN7425XQ3CU6WK/action/replication_record"}},"created_at":"2026-05-18T00:59:58.689430+00:00","updated_at":"2026-05-18T00:59:58.689430+00:00"}