{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2026:UWNGG3KRVI4DCQALC3KAUS3MPA","short_pith_number":"pith:UWNGG3KR","canonical_record":{"source":{"id":"2606.17554","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-06-16T05:58:25Z","cross_cats_sorted":["cond-mat.soft","physics.chem-ph"],"title_canon_sha256":"a155674e07f39aafac81f8e29fb5c3f0fe0ab43d71f88d47502067489ccdbe2e","abstract_canon_sha256":"cac75268273d944d634acf8d00d470cc1c2a39cca18d52f2d95c7398fb65d2e5"},"schema_version":"1.0"},"canonical_sha256":"a59a636d51aa3831400b16d40a4b6c781b37f88bd46798ceeb284e3b906291c1","source":{"kind":"arxiv","id":"2606.17554","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2606.17554","created_at":"2026-06-19T16:10:15Z"},{"alias_kind":"arxiv_version","alias_value":"2606.17554v1","created_at":"2026-06-19T16:10:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.17554","created_at":"2026-06-19T16:10:15Z"},{"alias_kind":"pith_short_12","alias_value":"UWNGG3KRVI4D","created_at":"2026-06-19T16:10:15Z"},{"alias_kind":"pith_short_16","alias_value":"UWNGG3KRVI4DCQAL","created_at":"2026-06-19T16:10:15Z"},{"alias_kind":"pith_short_8","alias_value":"UWNGG3KR","created_at":"2026-06-19T16:10:15Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2026:UWNGG3KRVI4DCQALC3KAUS3MPA","target":"record","payload":{"canonical_record":{"source":{"id":"2606.17554","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-06-16T05:58:25Z","cross_cats_sorted":["cond-mat.soft","physics.chem-ph"],"title_canon_sha256":"a155674e07f39aafac81f8e29fb5c3f0fe0ab43d71f88d47502067489ccdbe2e","abstract_canon_sha256":"cac75268273d944d634acf8d00d470cc1c2a39cca18d52f2d95c7398fb65d2e5"},"schema_version":"1.0"},"canonical_sha256":"a59a636d51aa3831400b16d40a4b6c781b37f88bd46798ceeb284e3b906291c1","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-19T16:10:15.847172Z","signature_b64":"OEVQ4OdoesYI5g1BcmibTVLQPFn07ka7T2NwTewH6VHOLq+BXL6IktKwqJzU9t+2d/C/fOSbs7N2jB1tydneAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a59a636d51aa3831400b16d40a4b6c781b37f88bd46798ceeb284e3b906291c1","last_reissued_at":"2026-06-19T16:10:15.846837Z","signature_status":"signed_v1","first_computed_at":"2026-06-19T16:10:15.846837Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2606.17554","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-06-19T16:10:15Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Dg3CGAXcppk1HZ/JxnrIfs40Aw/O2k/9tOuF7MdXxxpJGcsJ+C99t1B5uEqDzxlDWO2GjaawLrg1yyyMd6twBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-22T09:30:13.969431Z"},"content_sha256":"1300d58bfaaefd77e158fd0be7610be0ddeea49a134d4255a97c32380f15dd32","schema_version":"1.0","event_id":"sha256:1300d58bfaaefd77e158fd0be7610be0ddeea49a134d4255a97c32380f15dd32"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2026:UWNGG3KRVI4DCQALC3KAUS3MPA","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Brownian gyration of an inertial ellipsoid","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.soft","physics.chem-ph"],"primary_cat":"cond-mat.stat-mech","authors_text":"Arnab Saha, Soham Dutta","submitted_at":"2026-06-16T05:58:25Z","abstract_excerpt":"Recent studies on Brownian gyration (BG) have focused primarily on spherically symmetric particles under overdamped conditions. To explore BG in the underdamped regime with a spherically asymmetric particle, we investigate the inertial dynamics of a microscopic ellipsoid in a dissipative medium. The particle is confined in a spherically asymmetric trap and simultaneously coupled to two distinct thermal reservoirs. This configuration drives the system into a nonequilibrium steady state (NESS) characterised by BG, which is quantified by the mean and fluctuation of the particle's specific angular"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.17554","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/2606.17554/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":"2026-06-19T16:10:15Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"b7mJI/o38o3kWtug8aB9TRWAzNokwOO34eYmnrvjmDfrGAE4OymZz33S0MpIHpUsbPl7/eHJczcbBFMXc12LDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-22T09:30:13.969817Z"},"content_sha256":"cd973ce79aae9f04108e2e77758ec4ab9c824b16e10c7bbd604c6390abd03996","schema_version":"1.0","event_id":"sha256:cd973ce79aae9f04108e2e77758ec4ab9c824b16e10c7bbd604c6390abd03996"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/UWNGG3KRVI4DCQALC3KAUS3MPA/bundle.json","state_url":"https://pith.science/pith/UWNGG3KRVI4DCQALC3KAUS3MPA/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/UWNGG3KRVI4DCQALC3KAUS3MPA/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":"2026-06-22T09:30:13Z","links":{"resolver":"https://pith.science/pith/UWNGG3KRVI4DCQALC3KAUS3MPA","bundle":"https://pith.science/pith/UWNGG3KRVI4DCQALC3KAUS3MPA/bundle.json","state":"https://pith.science/pith/UWNGG3KRVI4DCQALC3KAUS3MPA/state.json","well_known_bundle":"https://pith.science/.well-known/pith/UWNGG3KRVI4DCQALC3KAUS3MPA/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:UWNGG3KRVI4DCQALC3KAUS3MPA","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":"cac75268273d944d634acf8d00d470cc1c2a39cca18d52f2d95c7398fb65d2e5","cross_cats_sorted":["cond-mat.soft","physics.chem-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-06-16T05:58:25Z","title_canon_sha256":"a155674e07f39aafac81f8e29fb5c3f0fe0ab43d71f88d47502067489ccdbe2e"},"schema_version":"1.0","source":{"id":"2606.17554","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2606.17554","created_at":"2026-06-19T16:10:15Z"},{"alias_kind":"arxiv_version","alias_value":"2606.17554v1","created_at":"2026-06-19T16:10:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.17554","created_at":"2026-06-19T16:10:15Z"},{"alias_kind":"pith_short_12","alias_value":"UWNGG3KRVI4D","created_at":"2026-06-19T16:10:15Z"},{"alias_kind":"pith_short_16","alias_value":"UWNGG3KRVI4DCQAL","created_at":"2026-06-19T16:10:15Z"},{"alias_kind":"pith_short_8","alias_value":"UWNGG3KR","created_at":"2026-06-19T16:10:15Z"}],"graph_snapshots":[{"event_id":"sha256:cd973ce79aae9f04108e2e77758ec4ab9c824b16e10c7bbd604c6390abd03996","target":"graph","created_at":"2026-06-19T16:10:15Z","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/2606.17554/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Recent studies on Brownian gyration (BG) have focused primarily on spherically symmetric particles under overdamped conditions. To explore BG in the underdamped regime with a spherically asymmetric particle, we investigate the inertial dynamics of a microscopic ellipsoid in a dissipative medium. The particle is confined in a spherically asymmetric trap and simultaneously coupled to two distinct thermal reservoirs. This configuration drives the system into a nonequilibrium steady state (NESS) characterised by BG, which is quantified by the mean and fluctuation of the particle's specific angular","authors_text":"Arnab Saha, Soham Dutta","cross_cats":["cond-mat.soft","physics.chem-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-06-16T05:58:25Z","title":"Brownian gyration of an inertial ellipsoid"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.17554","kind":"arxiv","version":1},"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":"sha256:1300d58bfaaefd77e158fd0be7610be0ddeea49a134d4255a97c32380f15dd32","target":"record","created_at":"2026-06-19T16:10:15Z","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":"cac75268273d944d634acf8d00d470cc1c2a39cca18d52f2d95c7398fb65d2e5","cross_cats_sorted":["cond-mat.soft","physics.chem-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-06-16T05:58:25Z","title_canon_sha256":"a155674e07f39aafac81f8e29fb5c3f0fe0ab43d71f88d47502067489ccdbe2e"},"schema_version":"1.0","source":{"id":"2606.17554","kind":"arxiv","version":1}},"canonical_sha256":"a59a636d51aa3831400b16d40a4b6c781b37f88bd46798ceeb284e3b906291c1","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a59a636d51aa3831400b16d40a4b6c781b37f88bd46798ceeb284e3b906291c1","first_computed_at":"2026-06-19T16:10:15.846837Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-06-19T16:10:15.846837Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"OEVQ4OdoesYI5g1BcmibTVLQPFn07ka7T2NwTewH6VHOLq+BXL6IktKwqJzU9t+2d/C/fOSbs7N2jB1tydneAg==","signature_status":"signed_v1","signed_at":"2026-06-19T16:10:15.847172Z","signed_message":"canonical_sha256_bytes"},"source_id":"2606.17554","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1300d58bfaaefd77e158fd0be7610be0ddeea49a134d4255a97c32380f15dd32","sha256:cd973ce79aae9f04108e2e77758ec4ab9c824b16e10c7bbd604c6390abd03996"],"state_sha256":"77d7d5d09d86515a44f4b5cef8091fd64872266954b14ac4678e60f8cbd75fdf"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4RPbNbGhA/Z6MAkWt+LojGJKfG7xBBFjqG/ZHLkyIluocm512HC2EmmaJTQBzXOBPJYjFi3b+t46i+3thrSuDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-22T09:30:13.971850Z","bundle_sha256":"87e8516ae330e13068dbd3079981ccbc88d53d4c0c6003bc04c3f27761ed3827"}}