{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:G75HEUNLPEKH224OMXOHCGZ5KA","short_pith_number":"pith:G75HEUNL","canonical_record":{"source":{"id":"1002.1861","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2010-02-09T14:06:32Z","cross_cats_sorted":[],"title_canon_sha256":"d114731498714b5c2ef37e08e7d9edac7180f611b4424d54f643cf91abef469e","abstract_canon_sha256":"c0d7b0b234d79c927572bb30cc690357bc78f1347519c9fc7d23dfb02944e6c3"},"schema_version":"1.0"},"canonical_sha256":"37fa7251ab79147d6b8e65dc711b3d501c8c8193d910a10c6261496387a70a30","source":{"kind":"arxiv","id":"1002.1861","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1002.1861","created_at":"2026-05-18T02:09:10Z"},{"alias_kind":"arxiv_version","alias_value":"1002.1861v1","created_at":"2026-05-18T02:09:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1002.1861","created_at":"2026-05-18T02:09:10Z"},{"alias_kind":"pith_short_12","alias_value":"G75HEUNLPEKH","created_at":"2026-05-18T12:26:07Z"},{"alias_kind":"pith_short_16","alias_value":"G75HEUNLPEKH224O","created_at":"2026-05-18T12:26:07Z"},{"alias_kind":"pith_short_8","alias_value":"G75HEUNL","created_at":"2026-05-18T12:26:07Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:G75HEUNLPEKH224OMXOHCGZ5KA","target":"record","payload":{"canonical_record":{"source":{"id":"1002.1861","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2010-02-09T14:06:32Z","cross_cats_sorted":[],"title_canon_sha256":"d114731498714b5c2ef37e08e7d9edac7180f611b4424d54f643cf91abef469e","abstract_canon_sha256":"c0d7b0b234d79c927572bb30cc690357bc78f1347519c9fc7d23dfb02944e6c3"},"schema_version":"1.0"},"canonical_sha256":"37fa7251ab79147d6b8e65dc711b3d501c8c8193d910a10c6261496387a70a30","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:09:10.853098Z","signature_b64":"ct9d7gAg6JR4wjLnN+nC8MHnuBexL21+ADyiUzUq3BMhrqmtqK60NlSgSkTA15mJ+lItl9c2SShzpQvUsG/1Bg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"37fa7251ab79147d6b8e65dc711b3d501c8c8193d910a10c6261496387a70a30","last_reissued_at":"2026-05-18T02:09:10.852294Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:09:10.852294Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1002.1861","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":"2026-05-18T02:09:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"D/e2nti+qYqWE7buTiJEUxa6bYKjRLJUj//aZ+vqdCgSg5RubxmhLehXB3fEBBDhxt8Dz1ZumXiBuOozetkgBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T02:13:21.871831Z"},"content_sha256":"5fe1f873394d66bd6fdb6dfef449702ed0ea556dad41194e8eef09e949ac9a62","schema_version":"1.0","event_id":"sha256:5fe1f873394d66bd6fdb6dfef449702ed0ea556dad41194e8eef09e949ac9a62"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:G75HEUNLPEKH224OMXOHCGZ5KA","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Asymptotical photon distributions in the dissipative Dynamical Casimir Effect","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"V. V. Dodonov","submitted_at":"2010-02-09T14:06:32Z","abstract_excerpt":"Asymptotical formulas for the photon distribution function of a quantum oscillator with time-dependent frequency and damping coefficients, interacting with a thermal reservoir, are derived in the case of a large mean number of quanta. Different regimes of excitation of an initial thermal state with an arbitrary temperature are considered. New formulas are used to predict the statistical properties of the electromagnetic field created in the experiments on the Dynamical Casimir Effect which are now under preparation."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1002.1861","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":""},"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":"2026-05-18T02:09:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cpu9wXAoaZ5iRFHvn6QeTeYxKwJ6eOlJHmEFyMDeABNVgxkDvJakxiS/0tDDfoOo/q6n3zOKGyzDj43EvDpXBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T02:13:21.872177Z"},"content_sha256":"6b1f168d627cb9d9f82f598794e28d4f36de1b12681fabda3f2694758f8e1ae9","schema_version":"1.0","event_id":"sha256:6b1f168d627cb9d9f82f598794e28d4f36de1b12681fabda3f2694758f8e1ae9"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/G75HEUNLPEKH224OMXOHCGZ5KA/bundle.json","state_url":"https://pith.science/pith/G75HEUNLPEKH224OMXOHCGZ5KA/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/G75HEUNLPEKH224OMXOHCGZ5KA/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":"2026-06-02T02:13:21Z","links":{"resolver":"https://pith.science/pith/G75HEUNLPEKH224OMXOHCGZ5KA","bundle":"https://pith.science/pith/G75HEUNLPEKH224OMXOHCGZ5KA/bundle.json","state":"https://pith.science/pith/G75HEUNLPEKH224OMXOHCGZ5KA/state.json","well_known_bundle":"https://pith.science/.well-known/pith/G75HEUNLPEKH224OMXOHCGZ5KA/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:G75HEUNLPEKH224OMXOHCGZ5KA","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":"c0d7b0b234d79c927572bb30cc690357bc78f1347519c9fc7d23dfb02944e6c3","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2010-02-09T14:06:32Z","title_canon_sha256":"d114731498714b5c2ef37e08e7d9edac7180f611b4424d54f643cf91abef469e"},"schema_version":"1.0","source":{"id":"1002.1861","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1002.1861","created_at":"2026-05-18T02:09:10Z"},{"alias_kind":"arxiv_version","alias_value":"1002.1861v1","created_at":"2026-05-18T02:09:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1002.1861","created_at":"2026-05-18T02:09:10Z"},{"alias_kind":"pith_short_12","alias_value":"G75HEUNLPEKH","created_at":"2026-05-18T12:26:07Z"},{"alias_kind":"pith_short_16","alias_value":"G75HEUNLPEKH224O","created_at":"2026-05-18T12:26:07Z"},{"alias_kind":"pith_short_8","alias_value":"G75HEUNL","created_at":"2026-05-18T12:26:07Z"}],"graph_snapshots":[{"event_id":"sha256:6b1f168d627cb9d9f82f598794e28d4f36de1b12681fabda3f2694758f8e1ae9","target":"graph","created_at":"2026-05-18T02:09:10Z","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":"Asymptotical formulas for the photon distribution function of a quantum oscillator with time-dependent frequency and damping coefficients, interacting with a thermal reservoir, are derived in the case of a large mean number of quanta. Different regimes of excitation of an initial thermal state with an arbitrary temperature are considered. New formulas are used to predict the statistical properties of the electromagnetic field created in the experiments on the Dynamical Casimir Effect which are now under preparation.","authors_text":"V. V. Dodonov","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2010-02-09T14:06:32Z","title":"Asymptotical photon distributions in the dissipative Dynamical Casimir Effect"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1002.1861","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":"sha256:5fe1f873394d66bd6fdb6dfef449702ed0ea556dad41194e8eef09e949ac9a62","target":"record","created_at":"2026-05-18T02:09:10Z","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":"c0d7b0b234d79c927572bb30cc690357bc78f1347519c9fc7d23dfb02944e6c3","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2010-02-09T14:06:32Z","title_canon_sha256":"d114731498714b5c2ef37e08e7d9edac7180f611b4424d54f643cf91abef469e"},"schema_version":"1.0","source":{"id":"1002.1861","kind":"arxiv","version":1}},"canonical_sha256":"37fa7251ab79147d6b8e65dc711b3d501c8c8193d910a10c6261496387a70a30","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"37fa7251ab79147d6b8e65dc711b3d501c8c8193d910a10c6261496387a70a30","first_computed_at":"2026-05-18T02:09:10.852294Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:09:10.852294Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ct9d7gAg6JR4wjLnN+nC8MHnuBexL21+ADyiUzUq3BMhrqmtqK60NlSgSkTA15mJ+lItl9c2SShzpQvUsG/1Bg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:09:10.853098Z","signed_message":"canonical_sha256_bytes"},"source_id":"1002.1861","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:5fe1f873394d66bd6fdb6dfef449702ed0ea556dad41194e8eef09e949ac9a62","sha256:6b1f168d627cb9d9f82f598794e28d4f36de1b12681fabda3f2694758f8e1ae9"],"state_sha256":"e227343dd82ccdff61db0a57b039f94932ed074fd97b7b4dad739312495d41ab"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"AAwRjF/rE0ngud7pWSnmQwzzbtQ4k0xdKPKZ6YEStOg46WZg5Z+Z4G7kIS0wBFbQeCwSzi03mpvzHKrgbMj2Aw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T02:13:21.874094Z","bundle_sha256":"67c94de29a658814a845f62ff6ab95399658507bf3668a6f58f58af4385de48b"}}