{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:M7IRDIT7HH22D7SQ3RLPCSPJE2","short_pith_number":"pith:M7IRDIT7","canonical_record":{"source":{"id":"1508.00815","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-08-04T16:21:35Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"5f2b158d64243341d56cae829eb586fafcde3d845a2f1ffbddc76743d5f43a6e","abstract_canon_sha256":"02b65e20f5e104d7c204e41c7604667cbb65b045360522422818c7c6cdb2d57a"},"schema_version":"1.0"},"canonical_sha256":"67d111a27f39f5a1fe50dc56f149e926b7f938ea273e90b420307dd00d56bd21","source":{"kind":"arxiv","id":"1508.00815","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1508.00815","created_at":"2026-05-18T01:16:49Z"},{"alias_kind":"arxiv_version","alias_value":"1508.00815v2","created_at":"2026-05-18T01:16:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1508.00815","created_at":"2026-05-18T01:16:49Z"},{"alias_kind":"pith_short_12","alias_value":"M7IRDIT7HH22","created_at":"2026-05-18T12:29:32Z"},{"alias_kind":"pith_short_16","alias_value":"M7IRDIT7HH22D7SQ","created_at":"2026-05-18T12:29:32Z"},{"alias_kind":"pith_short_8","alias_value":"M7IRDIT7","created_at":"2026-05-18T12:29:32Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:M7IRDIT7HH22D7SQ3RLPCSPJE2","target":"record","payload":{"canonical_record":{"source":{"id":"1508.00815","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-08-04T16:21:35Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"5f2b158d64243341d56cae829eb586fafcde3d845a2f1ffbddc76743d5f43a6e","abstract_canon_sha256":"02b65e20f5e104d7c204e41c7604667cbb65b045360522422818c7c6cdb2d57a"},"schema_version":"1.0"},"canonical_sha256":"67d111a27f39f5a1fe50dc56f149e926b7f938ea273e90b420307dd00d56bd21","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:16:49.583240Z","signature_b64":"N0byf7cmef0DEMs1DTnw/7qnBtYfedn0JAD74fMRBxquaeLQyykcIPAQBjsPLR1CZUih1yhjKdMthGIHae1wDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"67d111a27f39f5a1fe50dc56f149e926b7f938ea273e90b420307dd00d56bd21","last_reissued_at":"2026-05-18T01:16:49.582466Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:16:49.582466Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1508.00815","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:16:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1W2QWqtkOdMEgyKj6AVfaI0qr3uI6M0J4YjQsi2WdFGpvgUKpuQDmooOWGaSqTf6VSmVqjFcO01OH/Ip8JwpDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T20:47:45.109353Z"},"content_sha256":"0982e59786809f2d763028668c34b48701de1ddadd9dd990116a7c5defc424ae","schema_version":"1.0","event_id":"sha256:0982e59786809f2d763028668c34b48701de1ddadd9dd990116a7c5defc424ae"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:M7IRDIT7HH22D7SQ3RLPCSPJE2","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Predictions for Boson-Jet Observables and Fragmentation Function Ratios from a Hybrid Strong/Weak Coupling Model for Jet Quenching","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Daniel Pablos, Doga Can Gulhan, Jorge Casalderrey-Solana, Jos\\'e Guilherme Milhano, Krishna Rajagopal","submitted_at":"2015-08-04T16:21:35Z","abstract_excerpt":"We have previously introduced a hybrid strong/weak coupling model for jet quenching in heavy ion collisions that describes the production and fragmentation of jets at weak coupling, using PYTHIA, and describes the rate at which each parton in the jet shower loses energy as it propagates through the strongly coupled plasma, dE/dx, using an expression computed holographically at strong coupling. The model has a single free parameter that we fit to a single experimental measurement. We then confront our model with experimental data on many other jet observables, focusing here on boson-jet observa"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1508.00815","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:16:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Vn7l8odpbduFqsKck/vjt6nl1xmCCxwNzyHnTk53vjizkXmMD4RaKlwkiQJzqGxcwmXaQJtchd5lgAZzfyd1BA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T20:47:45.109942Z"},"content_sha256":"80d0ce8aaf5517d0bb353b205b54b2e995a07c0de92a8f1415f22bfb240238a0","schema_version":"1.0","event_id":"sha256:80d0ce8aaf5517d0bb353b205b54b2e995a07c0de92a8f1415f22bfb240238a0"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/M7IRDIT7HH22D7SQ3RLPCSPJE2/bundle.json","state_url":"https://pith.science/pith/M7IRDIT7HH22D7SQ3RLPCSPJE2/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/M7IRDIT7HH22D7SQ3RLPCSPJE2/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-02T20:47:45Z","links":{"resolver":"https://pith.science/pith/M7IRDIT7HH22D7SQ3RLPCSPJE2","bundle":"https://pith.science/pith/M7IRDIT7HH22D7SQ3RLPCSPJE2/bundle.json","state":"https://pith.science/pith/M7IRDIT7HH22D7SQ3RLPCSPJE2/state.json","well_known_bundle":"https://pith.science/.well-known/pith/M7IRDIT7HH22D7SQ3RLPCSPJE2/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:M7IRDIT7HH22D7SQ3RLPCSPJE2","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"02b65e20f5e104d7c204e41c7604667cbb65b045360522422818c7c6cdb2d57a","cross_cats_sorted":["nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-08-04T16:21:35Z","title_canon_sha256":"5f2b158d64243341d56cae829eb586fafcde3d845a2f1ffbddc76743d5f43a6e"},"schema_version":"1.0","source":{"id":"1508.00815","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1508.00815","created_at":"2026-05-18T01:16:49Z"},{"alias_kind":"arxiv_version","alias_value":"1508.00815v2","created_at":"2026-05-18T01:16:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1508.00815","created_at":"2026-05-18T01:16:49Z"},{"alias_kind":"pith_short_12","alias_value":"M7IRDIT7HH22","created_at":"2026-05-18T12:29:32Z"},{"alias_kind":"pith_short_16","alias_value":"M7IRDIT7HH22D7SQ","created_at":"2026-05-18T12:29:32Z"},{"alias_kind":"pith_short_8","alias_value":"M7IRDIT7","created_at":"2026-05-18T12:29:32Z"}],"graph_snapshots":[{"event_id":"sha256:80d0ce8aaf5517d0bb353b205b54b2e995a07c0de92a8f1415f22bfb240238a0","target":"graph","created_at":"2026-05-18T01:16:49Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We have previously introduced a hybrid strong/weak coupling model for jet quenching in heavy ion collisions that describes the production and fragmentation of jets at weak coupling, using PYTHIA, and describes the rate at which each parton in the jet shower loses energy as it propagates through the strongly coupled plasma, dE/dx, using an expression computed holographically at strong coupling. The model has a single free parameter that we fit to a single experimental measurement. We then confront our model with experimental data on many other jet observables, focusing here on boson-jet observa","authors_text":"Daniel Pablos, Doga Can Gulhan, Jorge Casalderrey-Solana, Jos\\'e Guilherme Milhano, Krishna Rajagopal","cross_cats":["nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-08-04T16:21:35Z","title":"Predictions for Boson-Jet Observables and Fragmentation Function Ratios from a Hybrid Strong/Weak Coupling Model for Jet Quenching"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1508.00815","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:0982e59786809f2d763028668c34b48701de1ddadd9dd990116a7c5defc424ae","target":"record","created_at":"2026-05-18T01:16:49Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"02b65e20f5e104d7c204e41c7604667cbb65b045360522422818c7c6cdb2d57a","cross_cats_sorted":["nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-08-04T16:21:35Z","title_canon_sha256":"5f2b158d64243341d56cae829eb586fafcde3d845a2f1ffbddc76743d5f43a6e"},"schema_version":"1.0","source":{"id":"1508.00815","kind":"arxiv","version":2}},"canonical_sha256":"67d111a27f39f5a1fe50dc56f149e926b7f938ea273e90b420307dd00d56bd21","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"67d111a27f39f5a1fe50dc56f149e926b7f938ea273e90b420307dd00d56bd21","first_computed_at":"2026-05-18T01:16:49.582466Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:16:49.582466Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"N0byf7cmef0DEMs1DTnw/7qnBtYfedn0JAD74fMRBxquaeLQyykcIPAQBjsPLR1CZUih1yhjKdMthGIHae1wDw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:16:49.583240Z","signed_message":"canonical_sha256_bytes"},"source_id":"1508.00815","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0982e59786809f2d763028668c34b48701de1ddadd9dd990116a7c5defc424ae","sha256:80d0ce8aaf5517d0bb353b205b54b2e995a07c0de92a8f1415f22bfb240238a0"],"state_sha256":"e796e80e624d8cb07f4d84481dc0ffda699cff069827d3d7830d97d6c4f2f7c4"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0ZyONtDmhFwOpYU8mb178RGPsFeqOVALey9VrrUqrHZQLCR3kEL9+XY7MIfBMURA4eu6Mi0xPU8SZSjGPfN9Aw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T20:47:45.113562Z","bundle_sha256":"32cc0f24e73f938c380c20b96135654f75460f7a165d958b4c0f09a7719583c3"}}