{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:BDQ72GRLDT4GX6R7FJIZLEIQ2R","short_pith_number":"pith:BDQ72GRL","schema_version":"1.0","canonical_sha256":"08e1fd1a2b1cf86bfa3f2a51959110d4412412fd7ca361f59fb7c09f567be630","source":{"kind":"arxiv","id":"1907.12301","version":1},"attestation_state":"computed","paper":{"title":"Jet suppression from small to intermediate to large radius","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Daniel Pablos","submitted_at":"2019-07-29T09:40:16Z","abstract_excerpt":"We present predictions for jet suppression from small to intermediate to very large radius, for low and very high energy jets created in heavy ion collisions at the LHC. We use the hybrid strong/weak coupling model for jet quenching that combines perturbative shower evolution with an effective strongly coupled description of the energy and momentum transfer from the jet into the hydrodynamic quark-gluon plasma. Because of momentum conservation, the wake created by the jet enhances or depletes the amount of particles generated at the freeze-out hypersurface depending on their orientation with r"},"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":"1907.12301","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-07-29T09:40:16Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"72a426ace3932eb1c16a983044640a9bbdb1693337efdcab1ddb7cec2106453b","abstract_canon_sha256":"bb0b62698f97aa913bcf409d38eb74f9bf74cfca86179428a608d8e0f31e32b5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:39:56.599061Z","signature_b64":"3Yb1KdjgHcRUPy7kSVnQUXsUvXibJngSYSST/ulkwV4moTuyh0xZtkjhw/b1lRuhxdFMKdM1uV/56n0+Sg1vAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"08e1fd1a2b1cf86bfa3f2a51959110d4412412fd7ca361f59fb7c09f567be630","last_reissued_at":"2026-07-05T00:39:56.598609Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:39:56.598609Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Jet suppression from small to intermediate to large radius","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Daniel Pablos","submitted_at":"2019-07-29T09:40:16Z","abstract_excerpt":"We present predictions for jet suppression from small to intermediate to very large radius, for low and very high energy jets created in heavy ion collisions at the LHC. We use the hybrid strong/weak coupling model for jet quenching that combines perturbative shower evolution with an effective strongly coupled description of the energy and momentum transfer from the jet into the hydrodynamic quark-gluon plasma. Because of momentum conservation, the wake created by the jet enhances or depletes the amount of particles generated at the freeze-out hypersurface depending on their orientation with r"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1907.12301","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1907.12301/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"1907.12301","created_at":"2026-07-05T00:39:56.598659+00:00"},{"alias_kind":"arxiv_version","alias_value":"1907.12301v1","created_at":"2026-07-05T00:39:56.598659+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1907.12301","created_at":"2026-07-05T00:39:56.598659+00:00"},{"alias_kind":"pith_short_12","alias_value":"BDQ72GRLDT4G","created_at":"2026-07-05T00:39:56.598659+00:00"},{"alias_kind":"pith_short_16","alias_value":"BDQ72GRLDT4GX6R7","created_at":"2026-07-05T00:39:56.598659+00:00"},{"alias_kind":"pith_short_8","alias_value":"BDQ72GRL","created_at":"2026-07-05T00:39:56.598659+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.28788","citing_title":"Energy-energy correlators inside single inclusive jets in heavy-ion collisions with CoLBT-hydro model","ref_index":109,"is_internal_anchor":false},{"citing_arxiv_id":"2605.17511","citing_title":"Study of jet-induced hydro response in high-energy heavy-ion collisions with a flow-matching generative model","ref_index":44,"is_internal_anchor":false},{"citing_arxiv_id":"2509.07842","citing_title":"Jet cone size dependence of single inclusive jet suppression due to jet quenching in Pb+Pb collisions at $\\sqrt{s_{\\rm NN}}=5.02$ TeV","ref_index":62,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/BDQ72GRLDT4GX6R7FJIZLEIQ2R","json":"https://pith.science/pith/BDQ72GRLDT4GX6R7FJIZLEIQ2R.json","graph_json":"https://pith.science/api/pith-number/BDQ72GRLDT4GX6R7FJIZLEIQ2R/graph.json","events_json":"https://pith.science/api/pith-number/BDQ72GRLDT4GX6R7FJIZLEIQ2R/events.json","paper":"https://pith.science/paper/BDQ72GRL"},"agent_actions":{"view_html":"https://pith.science/pith/BDQ72GRLDT4GX6R7FJIZLEIQ2R","download_json":"https://pith.science/pith/BDQ72GRLDT4GX6R7FJIZLEIQ2R.json","view_paper":"https://pith.science/paper/BDQ72GRL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1907.12301&json=true","fetch_graph":"https://pith.science/api/pith-number/BDQ72GRLDT4GX6R7FJIZLEIQ2R/graph.json","fetch_events":"https://pith.science/api/pith-number/BDQ72GRLDT4GX6R7FJIZLEIQ2R/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BDQ72GRLDT4GX6R7FJIZLEIQ2R/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BDQ72GRLDT4GX6R7FJIZLEIQ2R/action/storage_attestation","attest_author":"https://pith.science/pith/BDQ72GRLDT4GX6R7FJIZLEIQ2R/action/author_attestation","sign_citation":"https://pith.science/pith/BDQ72GRLDT4GX6R7FJIZLEIQ2R/action/citation_signature","submit_replication":"https://pith.science/pith/BDQ72GRLDT4GX6R7FJIZLEIQ2R/action/replication_record"}},"created_at":"2026-07-05T00:39:56.598659+00:00","updated_at":"2026-07-05T00:39:56.598659+00:00"}