{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:2NSP5GXKAXN4VFRZQPFFT5IPV4","short_pith_number":"pith:2NSP5GXK","schema_version":"1.0","canonical_sha256":"d364fe9aea05dbca963983ca59f50faf3e18f49ffab364c96a94ea69b343c701","source":{"kind":"arxiv","id":"2602.13044","version":2},"attestation_state":"computed","paper":{"title":"Rotating synchrotron radiation: Photon emission from magnetized and rotating quark-gluon plasma","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"Jonathan D. Kroth, Kirill Tuchin, Matteo Buzzegoli, Nandagopal Vijayakumar, Sergiu Busuioc","submitted_at":"2026-02-13T15:59:16Z","abstract_excerpt":"This paper investigates the production of non-prompt photons originating from rotating synchrotron radiation (RoSyRa), specifically the emission of photons by a rigidly rotating quark-gluon plasma in thermal equilibrium, in the presence of an external magnetic field. We compute the non-prompt photon spectrum and its elliptic flow ($v_2$) at mid-rapidity. In particular, we investigate the finite volume effects. We find that at low transverse momentum, the magnetic field induces a significant $v_2$, while the plasma rotation boosts the synchrotron radiation of negatively charged quarks. These fi"},"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":"2602.13044","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2026-02-13T15:59:16Z","cross_cats_sorted":["hep-th","nucl-th"],"title_canon_sha256":"5e3a33acabe30222281422e8dac8b313c71ebc003408e6b1d7804a78dbe3b202","abstract_canon_sha256":"098348f2976d651db69dc19d72eb8c7c8eacd70a49f793ee1030fa0c7f227bfc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-09T02:08:39.098792Z","signature_b64":"F6gWtCewl1L58p9WeDl6S+A8Ge/yr8Z8z6wLflk4ZC3FOS+4Ni+L0tY9dm/5Sl5fdGG6XtqXu3T3vY6BYpiiAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d364fe9aea05dbca963983ca59f50faf3e18f49ffab364c96a94ea69b343c701","last_reissued_at":"2026-06-09T02:08:39.097874Z","signature_status":"signed_v1","first_computed_at":"2026-06-09T02:08:39.097874Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Rotating synchrotron radiation: Photon emission from magnetized and rotating quark-gluon plasma","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"Jonathan D. Kroth, Kirill Tuchin, Matteo Buzzegoli, Nandagopal Vijayakumar, Sergiu Busuioc","submitted_at":"2026-02-13T15:59:16Z","abstract_excerpt":"This paper investigates the production of non-prompt photons originating from rotating synchrotron radiation (RoSyRa), specifically the emission of photons by a rigidly rotating quark-gluon plasma in thermal equilibrium, in the presence of an external magnetic field. We compute the non-prompt photon spectrum and its elliptic flow ($v_2$) at mid-rapidity. In particular, we investigate the finite volume effects. We find that at low transverse momentum, the magnetic field induces a significant $v_2$, while the plasma rotation boosts the synchrotron radiation of negatively charged quarks. These fi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2602.13044","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2602.13044/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":"2602.13044","created_at":"2026-06-09T02:08:39.098031+00:00"},{"alias_kind":"arxiv_version","alias_value":"2602.13044v2","created_at":"2026-06-09T02:08:39.098031+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2602.13044","created_at":"2026-06-09T02:08:39.098031+00:00"},{"alias_kind":"pith_short_12","alias_value":"2NSP5GXKAXN4","created_at":"2026-06-09T02:08:39.098031+00:00"},{"alias_kind":"pith_short_16","alias_value":"2NSP5GXKAXN4VFRZ","created_at":"2026-06-09T02:08:39.098031+00:00"},{"alias_kind":"pith_short_8","alias_value":"2NSP5GXK","created_at":"2026-06-09T02:08:39.098031+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/2NSP5GXKAXN4VFRZQPFFT5IPV4","json":"https://pith.science/pith/2NSP5GXKAXN4VFRZQPFFT5IPV4.json","graph_json":"https://pith.science/api/pith-number/2NSP5GXKAXN4VFRZQPFFT5IPV4/graph.json","events_json":"https://pith.science/api/pith-number/2NSP5GXKAXN4VFRZQPFFT5IPV4/events.json","paper":"https://pith.science/paper/2NSP5GXK"},"agent_actions":{"view_html":"https://pith.science/pith/2NSP5GXKAXN4VFRZQPFFT5IPV4","download_json":"https://pith.science/pith/2NSP5GXKAXN4VFRZQPFFT5IPV4.json","view_paper":"https://pith.science/paper/2NSP5GXK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2602.13044&json=true","fetch_graph":"https://pith.science/api/pith-number/2NSP5GXKAXN4VFRZQPFFT5IPV4/graph.json","fetch_events":"https://pith.science/api/pith-number/2NSP5GXKAXN4VFRZQPFFT5IPV4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2NSP5GXKAXN4VFRZQPFFT5IPV4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2NSP5GXKAXN4VFRZQPFFT5IPV4/action/storage_attestation","attest_author":"https://pith.science/pith/2NSP5GXKAXN4VFRZQPFFT5IPV4/action/author_attestation","sign_citation":"https://pith.science/pith/2NSP5GXKAXN4VFRZQPFFT5IPV4/action/citation_signature","submit_replication":"https://pith.science/pith/2NSP5GXKAXN4VFRZQPFFT5IPV4/action/replication_record"}},"created_at":"2026-06-09T02:08:39.098031+00:00","updated_at":"2026-06-09T02:08:39.098031+00:00"}