{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1993:WSC576XN3IIVG42Y3UBCYEITKP","short_pith_number":"pith:WSC576XN","schema_version":"1.0","canonical_sha256":"b485dffaedda11537358dd022c111353ed7b222b16fa2d936bb5c9442ec66501","source":{"kind":"arxiv","id":"nucl-th/9306003","version":1},"attestation_state":"computed","paper":{"title":"Multiple Collisions and Induced Gluon Bremsstrahlung in QCD","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Mikols Gyulassy, Xin-Nian Wang","submitted_at":"1993-06-02T21:43:39Z","abstract_excerpt":"Induced soft gluon bremsstrahlung associated with multiple collisions is calculated via perturbative QCD. We derive the non-abelian analog of the Landau-Pomeranchuk effect that suppresses induced soft radiation with formation times exceeding the mean free path, $\\lambda$. The dependence of the suppression effect on the $SU(N)$ representation of the jet parton as well as the kinematic variables is expressed through a radiation formation factor. Unlike in QED, the finite contribution from the small $x$ regime in QCD leads to an approximately constant radiative energy loss per unit length, $dE/dz"},"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":"nucl-th/9306003","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"1993-06-02T21:43:39Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"f698167e4aae86a0f269052f45c7cbea2f091033730b883f9ae4d7be797ab25e","abstract_canon_sha256":"2632bb742e2cf7669108592ffd0dcf59a233e10ae4f0fe4d707753867a19052b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:54:14.459091Z","signature_b64":"+QIo6p3jxwXu5/QwSaYIonknzFSNdZyRryr72/+Laqp9o1QqGiCutKCxK5jwbLSLjfxm0+7m8UxtiSF0OLSOBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b485dffaedda11537358dd022c111353ed7b222b16fa2d936bb5c9442ec66501","last_reissued_at":"2026-07-04T15:54:14.458671Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:54:14.458671Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Multiple Collisions and Induced Gluon Bremsstrahlung in QCD","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Mikols Gyulassy, Xin-Nian Wang","submitted_at":"1993-06-02T21:43:39Z","abstract_excerpt":"Induced soft gluon bremsstrahlung associated with multiple collisions is calculated via perturbative QCD. We derive the non-abelian analog of the Landau-Pomeranchuk effect that suppresses induced soft radiation with formation times exceeding the mean free path, $\\lambda$. The dependence of the suppression effect on the $SU(N)$ representation of the jet parton as well as the kinematic variables is expressed through a radiation formation factor. Unlike in QED, the finite contribution from the small $x$ regime in QCD leads to an approximately constant radiative energy loss per unit length, $dE/dz"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/9306003","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/nucl-th/9306003/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"nucl-th/9306003","created_at":"2026-07-04T15:54:14.458732+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/9306003v1","created_at":"2026-07-04T15:54:14.458732+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/9306003","created_at":"2026-07-04T15:54:14.458732+00:00"},{"alias_kind":"pith_short_12","alias_value":"WSC576XN3IIV","created_at":"2026-07-04T15:54:14.458732+00:00"},{"alias_kind":"pith_short_16","alias_value":"WSC576XN3IIVG42Y","created_at":"2026-07-04T15:54:14.458732+00:00"},{"alias_kind":"pith_short_8","alias_value":"WSC576XN","created_at":"2026-07-04T15:54:14.458732+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":10,"internal_anchor_count":9,"sample":[{"citing_arxiv_id":"2606.26039","citing_title":"In-medium QCD splittings beyond the soft, large-$N_c$ and harmonic-oscillator approximations all at once","ref_index":16,"is_internal_anchor":true},{"citing_arxiv_id":"2606.20463","citing_title":"Observation of centrality-dependent dijet transverse momentum imbalance in O+O and Ne+Ne collisions at $\\sqrt{s_{NN}}$ = 5.36 TeV with the ATLAS detector","ref_index":4,"is_internal_anchor":true},{"citing_arxiv_id":"2607.00629","citing_title":"Gluon radiation from a QCD antenna with realistic parton-medium interactions","ref_index":41,"is_internal_anchor":true},{"citing_arxiv_id":"2605.28788","citing_title":"Energy-energy correlators inside single inclusive jets in heavy-ion collisions with CoLBT-hydro model","ref_index":4,"is_internal_anchor":true},{"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":18,"is_internal_anchor":true},{"citing_arxiv_id":"2510.17597","citing_title":"Photon radiation induced by rescattering in strong-interacting medium with a magnetic field","ref_index":50,"is_internal_anchor":true},{"citing_arxiv_id":"2512.05199","citing_title":"Jet Charge with Global Event Shapes: Probing Quark Flavor Dynamics","ref_index":57,"is_internal_anchor":true},{"citing_arxiv_id":"2512.12959","citing_title":"Energy Loss of a Heavy Quark in a Collisional Quark-Gluon Plasma","ref_index":17,"is_internal_anchor":true},{"citing_arxiv_id":"2605.04393","citing_title":"Medium Characterization with Hard Probes: From Cherenkov Light in QED to Jet Drift in QCD","ref_index":77,"is_internal_anchor":true},{"citing_arxiv_id":"2605.04393","citing_title":"Medium Characterization with Hard Probes: From Cherenkov Light in QED to Jet Drift in QCD","ref_index":77,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WSC576XN3IIVG42Y3UBCYEITKP","json":"https://pith.science/pith/WSC576XN3IIVG42Y3UBCYEITKP.json","graph_json":"https://pith.science/api/pith-number/WSC576XN3IIVG42Y3UBCYEITKP/graph.json","events_json":"https://pith.science/api/pith-number/WSC576XN3IIVG42Y3UBCYEITKP/events.json","paper":"https://pith.science/paper/WSC576XN"},"agent_actions":{"view_html":"https://pith.science/pith/WSC576XN3IIVG42Y3UBCYEITKP","download_json":"https://pith.science/pith/WSC576XN3IIVG42Y3UBCYEITKP.json","view_paper":"https://pith.science/paper/WSC576XN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-th/9306003&json=true","fetch_graph":"https://pith.science/api/pith-number/WSC576XN3IIVG42Y3UBCYEITKP/graph.json","fetch_events":"https://pith.science/api/pith-number/WSC576XN3IIVG42Y3UBCYEITKP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WSC576XN3IIVG42Y3UBCYEITKP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WSC576XN3IIVG42Y3UBCYEITKP/action/storage_attestation","attest_author":"https://pith.science/pith/WSC576XN3IIVG42Y3UBCYEITKP/action/author_attestation","sign_citation":"https://pith.science/pith/WSC576XN3IIVG42Y3UBCYEITKP/action/citation_signature","submit_replication":"https://pith.science/pith/WSC576XN3IIVG42Y3UBCYEITKP/action/replication_record"}},"created_at":"2026-07-04T15:54:14.458732+00:00","updated_at":"2026-07-04T15:54:14.458732+00:00"}