{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2025:C7UKFJM3EDXQ5SGGDUOKNO6UTY","short_pith_number":"pith:C7UKFJM3","canonical_record":{"source":{"id":"2502.18354","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-02-25T16:44:22Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"603d050d39fc0ce4155454af08b0e28d68479a8948a60977162a213bc6f76c70","abstract_canon_sha256":"7a480534b0614b724570b9dcda68e3121ef82f7b323e84e47ee8dc6153358532"},"schema_version":"1.0"},"canonical_sha256":"17e8a2a59b20ef0ec8c61d1ca6bbd49e18e3803f0a3f34639bcee5bf45501467","source":{"kind":"arxiv","id":"2502.18354","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2502.18354","created_at":"2026-07-05T10:42:43Z"},{"alias_kind":"arxiv_version","alias_value":"2502.18354v2","created_at":"2026-07-05T10:42:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2502.18354","created_at":"2026-07-05T10:42:43Z"},{"alias_kind":"pith_short_12","alias_value":"C7UKFJM3EDXQ","created_at":"2026-07-05T10:42:43Z"},{"alias_kind":"pith_short_16","alias_value":"C7UKFJM3EDXQ5SGG","created_at":"2026-07-05T10:42:43Z"},{"alias_kind":"pith_short_8","alias_value":"C7UKFJM3","created_at":"2026-07-05T10:42:43Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2025:C7UKFJM3EDXQ5SGGDUOKNO6UTY","target":"record","payload":{"canonical_record":{"source":{"id":"2502.18354","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-02-25T16:44:22Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"603d050d39fc0ce4155454af08b0e28d68479a8948a60977162a213bc6f76c70","abstract_canon_sha256":"7a480534b0614b724570b9dcda68e3121ef82f7b323e84e47ee8dc6153358532"},"schema_version":"1.0"},"canonical_sha256":"17e8a2a59b20ef0ec8c61d1ca6bbd49e18e3803f0a3f34639bcee5bf45501467","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:42:43.931412Z","signature_b64":"YO0iZJmcmWyy0BCvwd1ifW4fZEWJDRTbF+CFPRWJqAx93x/e3+YP+UV0iOHqrYYYX7Z8Mwl4OcmmFDrsnWNtAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"17e8a2a59b20ef0ec8c61d1ca6bbd49e18e3803f0a3f34639bcee5bf45501467","last_reissued_at":"2026-07-05T10:42:43.930830Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:42:43.930830Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2502.18354","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":"2026-07-05T10:42:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4BvgPJ/tZkceiBSZXf3VMWjK5GNr4rhwj9GvOG8ziULUn9wj5w5PRjxtv55KMbCDvfq5ovOBWEKENZyLgZ66AA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-17T20:33:19.383010Z"},"content_sha256":"30cadf83f86d9f2325b877174febce41d927ad72d91a61902abea556909bf6f5","schema_version":"1.0","event_id":"sha256:30cadf83f86d9f2325b877174febce41d927ad72d91a61902abea556909bf6f5"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2025:C7UKFJM3EDXQ5SGGDUOKNO6UTY","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Rotational stability of magnetic field in rotating quark-gluon plasma","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Aritra Das, Kirill Tuchin","submitted_at":"2025-02-25T16:44:22Z","abstract_excerpt":"Relaxation of the magnetic field in rigidly rotating quark-gluon plasma is studied. It is shown that the infrared modes satisfying $k < |m|\\Omega$ and $k< |m\\pm 1|\\Omega$, where integer $m$ is the projection of the orbital angular momentum along the rotating axis and $\\Omega$ is the angular velocity, are unstable. The instability onset time and the magnetic field growth rate are computed for a standard initial profile of the magnetic field. Given the present phenomenological values of $\\Omega$ and electrical conductivity $\\sigma$ the instability is not expected to be a significant factor in th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2502.18354","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/2502.18354/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T10:42:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"aPZwCz2M2+7JL/zbV5EUyFJSNsaOiEKXJxHs3V/7OVzr/mCKUVJtpIYMizQbLFRHhYHyzZstISHs+TMecb85BQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-17T20:33:19.384758Z"},"content_sha256":"19737716948128d4e073b3050f8e7d0418e26f8decb051012f828d639512a5e9","schema_version":"1.0","event_id":"sha256:19737716948128d4e073b3050f8e7d0418e26f8decb051012f828d639512a5e9"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/C7UKFJM3EDXQ5SGGDUOKNO6UTY/bundle.json","state_url":"https://pith.science/pith/C7UKFJM3EDXQ5SGGDUOKNO6UTY/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/C7UKFJM3EDXQ5SGGDUOKNO6UTY/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":"2026-08-17T20:33:19Z","links":{"resolver":"https://pith.science/pith/C7UKFJM3EDXQ5SGGDUOKNO6UTY","bundle":"https://pith.science/pith/C7UKFJM3EDXQ5SGGDUOKNO6UTY/bundle.json","state":"https://pith.science/pith/C7UKFJM3EDXQ5SGGDUOKNO6UTY/state.json","well_known_bundle":"https://pith.science/.well-known/pith/C7UKFJM3EDXQ5SGGDUOKNO6UTY/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:C7UKFJM3EDXQ5SGGDUOKNO6UTY","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":"7a480534b0614b724570b9dcda68e3121ef82f7b323e84e47ee8dc6153358532","cross_cats_sorted":["nucl-th"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-02-25T16:44:22Z","title_canon_sha256":"603d050d39fc0ce4155454af08b0e28d68479a8948a60977162a213bc6f76c70"},"schema_version":"1.0","source":{"id":"2502.18354","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2502.18354","created_at":"2026-07-05T10:42:43Z"},{"alias_kind":"arxiv_version","alias_value":"2502.18354v2","created_at":"2026-07-05T10:42:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2502.18354","created_at":"2026-07-05T10:42:43Z"},{"alias_kind":"pith_short_12","alias_value":"C7UKFJM3EDXQ","created_at":"2026-07-05T10:42:43Z"},{"alias_kind":"pith_short_16","alias_value":"C7UKFJM3EDXQ5SGG","created_at":"2026-07-05T10:42:43Z"},{"alias_kind":"pith_short_8","alias_value":"C7UKFJM3","created_at":"2026-07-05T10:42:43Z"}],"graph_snapshots":[{"event_id":"sha256:19737716948128d4e073b3050f8e7d0418e26f8decb051012f828d639512a5e9","target":"graph","created_at":"2026-07-05T10:42:43Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2502.18354/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Relaxation of the magnetic field in rigidly rotating quark-gluon plasma is studied. It is shown that the infrared modes satisfying $k < |m|\\Omega$ and $k< |m\\pm 1|\\Omega$, where integer $m$ is the projection of the orbital angular momentum along the rotating axis and $\\Omega$ is the angular velocity, are unstable. The instability onset time and the magnetic field growth rate are computed for a standard initial profile of the magnetic field. Given the present phenomenological values of $\\Omega$ and electrical conductivity $\\sigma$ the instability is not expected to be a significant factor in th","authors_text":"Aritra Das, Kirill Tuchin","cross_cats":["nucl-th"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-02-25T16:44:22Z","title":"Rotational stability of magnetic field in rotating quark-gluon plasma"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2502.18354","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":"sha256:30cadf83f86d9f2325b877174febce41d927ad72d91a61902abea556909bf6f5","target":"record","created_at":"2026-07-05T10:42:43Z","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":"7a480534b0614b724570b9dcda68e3121ef82f7b323e84e47ee8dc6153358532","cross_cats_sorted":["nucl-th"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-02-25T16:44:22Z","title_canon_sha256":"603d050d39fc0ce4155454af08b0e28d68479a8948a60977162a213bc6f76c70"},"schema_version":"1.0","source":{"id":"2502.18354","kind":"arxiv","version":2}},"canonical_sha256":"17e8a2a59b20ef0ec8c61d1ca6bbd49e18e3803f0a3f34639bcee5bf45501467","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"17e8a2a59b20ef0ec8c61d1ca6bbd49e18e3803f0a3f34639bcee5bf45501467","first_computed_at":"2026-07-05T10:42:43.930830Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:42:43.930830Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"YO0iZJmcmWyy0BCvwd1ifW4fZEWJDRTbF+CFPRWJqAx93x/e3+YP+UV0iOHqrYYYX7Z8Mwl4OcmmFDrsnWNtAA==","signature_status":"signed_v1","signed_at":"2026-07-05T10:42:43.931412Z","signed_message":"canonical_sha256_bytes"},"source_id":"2502.18354","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:30cadf83f86d9f2325b877174febce41d927ad72d91a61902abea556909bf6f5","sha256:19737716948128d4e073b3050f8e7d0418e26f8decb051012f828d639512a5e9"],"state_sha256":"464f6e42b24fcb9b2dd49203a267219fb15084da685e72f5f2028e569f060fa3"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WrTU1iy8VbF7Z6jnnf9ygvoorWEn22zRqsIhxM3bwqUSbagIJq4heZOk6/z9hI1dtHQoIRp70gK6RU/3y2ZWBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-17T20:33:19.400202Z","bundle_sha256":"9abcf96af7e6eddda4a3d7b16616ae396f3e431a1807adf0682826510f3fb1ad"}}