{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:73O4EQ7II64B274V4HGIKQ6EC2","short_pith_number":"pith:73O4EQ7I","schema_version":"1.0","canonical_sha256":"feddc243e847b81d7f95e1cc8543c416900dae981485f796ae7851e87c106a71","source":{"kind":"arxiv","id":"1602.04761","version":1},"attestation_state":"computed","paper":{"title":"Back reaction effects on the dynamics of heavy probes in heavy quark cloud","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Shankhadeep Chakrabortty, Tanay K. Dey","submitted_at":"2016-02-15T18:47:23Z","abstract_excerpt":"We holographically study the effect of back reaction on the hydrodynamical properties of $\\mathcal{N} = 4$ strongly coupled super Yang-Mills (SYM) thermal plasma. The back reaction we consider arises from the presence of static heavy quarks uniformly distributed over $\\mathcal{N} = 4$ SYM plasma. In order to study the hydrodynamical properties, we use heavy quark as well as heavy quark-antiquark bound state as probes and compute the jet quenching parameter, screening length and binding energy. We also consider the rotational dynamics of heavy probe quark in the back-reacted plasma and analyse "},"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":"1602.04761","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2016-02-15T18:47:23Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"6ff71ac0122f67b2eb2f6396cc4ec46f2083351e52cbae10b2b02c60dfd1e227","abstract_canon_sha256":"fd0f8c7f54285fc7be2d5ffa88829da513ad16fdc233abc2c359baa4eabc3e4e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:20:49.232386Z","signature_b64":"dJec5viwoVzBwNU/OLpDkbhj1Ep8oi0fA9c1ET8NvdCXlnd8sI50yefbRIl5TrqI+edWPUBNzV1WjVQN3ZEmDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"feddc243e847b81d7f95e1cc8543c416900dae981485f796ae7851e87c106a71","last_reissued_at":"2026-05-18T01:20:49.231949Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:20:49.231949Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Back reaction effects on the dynamics of heavy probes in heavy quark cloud","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Shankhadeep Chakrabortty, Tanay K. Dey","submitted_at":"2016-02-15T18:47:23Z","abstract_excerpt":"We holographically study the effect of back reaction on the hydrodynamical properties of $\\mathcal{N} = 4$ strongly coupled super Yang-Mills (SYM) thermal plasma. The back reaction we consider arises from the presence of static heavy quarks uniformly distributed over $\\mathcal{N} = 4$ SYM plasma. In order to study the hydrodynamical properties, we use heavy quark as well as heavy quark-antiquark bound state as probes and compute the jet quenching parameter, screening length and binding energy. We also consider the rotational dynamics of heavy probe quark in the back-reacted plasma and analyse "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1602.04761","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":"1602.04761","created_at":"2026-05-18T01:20:49.232012+00:00"},{"alias_kind":"arxiv_version","alias_value":"1602.04761v1","created_at":"2026-05-18T01:20:49.232012+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1602.04761","created_at":"2026-05-18T01:20:49.232012+00:00"},{"alias_kind":"pith_short_12","alias_value":"73O4EQ7II64B","created_at":"2026-05-18T12:30:04.600751+00:00"},{"alias_kind":"pith_short_16","alias_value":"73O4EQ7II64B274V","created_at":"2026-05-18T12:30:04.600751+00:00"},{"alias_kind":"pith_short_8","alias_value":"73O4EQ7I","created_at":"2026-05-18T12:30:04.600751+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/73O4EQ7II64B274V4HGIKQ6EC2","json":"https://pith.science/pith/73O4EQ7II64B274V4HGIKQ6EC2.json","graph_json":"https://pith.science/api/pith-number/73O4EQ7II64B274V4HGIKQ6EC2/graph.json","events_json":"https://pith.science/api/pith-number/73O4EQ7II64B274V4HGIKQ6EC2/events.json","paper":"https://pith.science/paper/73O4EQ7I"},"agent_actions":{"view_html":"https://pith.science/pith/73O4EQ7II64B274V4HGIKQ6EC2","download_json":"https://pith.science/pith/73O4EQ7II64B274V4HGIKQ6EC2.json","view_paper":"https://pith.science/paper/73O4EQ7I","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1602.04761&json=true","fetch_graph":"https://pith.science/api/pith-number/73O4EQ7II64B274V4HGIKQ6EC2/graph.json","fetch_events":"https://pith.science/api/pith-number/73O4EQ7II64B274V4HGIKQ6EC2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/73O4EQ7II64B274V4HGIKQ6EC2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/73O4EQ7II64B274V4HGIKQ6EC2/action/storage_attestation","attest_author":"https://pith.science/pith/73O4EQ7II64B274V4HGIKQ6EC2/action/author_attestation","sign_citation":"https://pith.science/pith/73O4EQ7II64B274V4HGIKQ6EC2/action/citation_signature","submit_replication":"https://pith.science/pith/73O4EQ7II64B274V4HGIKQ6EC2/action/replication_record"}},"created_at":"2026-05-18T01:20:49.232012+00:00","updated_at":"2026-05-18T01:20:49.232012+00:00"}