{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:32DURC54EODKMM4YCAVXU425JN","short_pith_number":"pith:32DURC54","canonical_record":{"source":{"id":"1403.6635","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2014-03-26T11:41:06Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"d7a4202a2455217e7890226ff366b2422871d3d40e172e4892ebfae16a93b890","abstract_canon_sha256":"5b0b28cf1989d4fcac2c6a93deb1052043b9330a1d1b7a7f8caa25c8dc853d0d"},"schema_version":"1.0"},"canonical_sha256":"de87488bbc2386a63398102b7a735d4b4a071fe4236b194348371710ef36ae49","source":{"kind":"arxiv","id":"1403.6635","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1403.6635","created_at":"2026-05-18T02:55:28Z"},{"alias_kind":"arxiv_version","alias_value":"1403.6635v1","created_at":"2026-05-18T02:55:28Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1403.6635","created_at":"2026-05-18T02:55:28Z"},{"alias_kind":"pith_short_12","alias_value":"32DURC54EODK","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_16","alias_value":"32DURC54EODKMM4Y","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_8","alias_value":"32DURC54","created_at":"2026-05-18T12:28:11Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:32DURC54EODKMM4YCAVXU425JN","target":"record","payload":{"canonical_record":{"source":{"id":"1403.6635","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2014-03-26T11:41:06Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"d7a4202a2455217e7890226ff366b2422871d3d40e172e4892ebfae16a93b890","abstract_canon_sha256":"5b0b28cf1989d4fcac2c6a93deb1052043b9330a1d1b7a7f8caa25c8dc853d0d"},"schema_version":"1.0"},"canonical_sha256":"de87488bbc2386a63398102b7a735d4b4a071fe4236b194348371710ef36ae49","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:55:28.442546Z","signature_b64":"aO/XgYGwAchwO9JtYARiPTfPn2FHZldkc83rRUS7PA4WuXbcZNHnMnajwXtgQmUSsYpb+nvAuirtncgBgI81Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"de87488bbc2386a63398102b7a735d4b4a071fe4236b194348371710ef36ae49","last_reissued_at":"2026-05-18T02:55:28.441850Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:55:28.441850Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1403.6635","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":"2026-05-18T02:55:28Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DD3KaDLZGaPB82+bHFa8JeCjEJOR4C+yfDyNmYxY9uCPFb0SMJXrliBxMqNg8GSiD9d0zmCJOvjTk4RZf2grDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-28T14:39:53.391322Z"},"content_sha256":"78e8de260295cfe450825ed4cdd5225bf3cb079362ad854b9bd0e40088b582f0","schema_version":"1.0","event_id":"sha256:78e8de260295cfe450825ed4cdd5225bf3cb079362ad854b9bd0e40088b582f0"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:32DURC54EODKMM4YCAVXU425JN","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Casimir friction at zero and finite temperatures","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"quant-ph","authors_text":"Iver Brevik, Johan S. H{\\o}ye","submitted_at":"2014-03-26T11:41:06Z","abstract_excerpt":"The Casimir friction problem for dielectric plates that move parallel to each other is treated by assuming one of the plates to be at rest. The other performs a closed loop motion in the longitudinal direction. Therewith by use of energy dissipation the formalism becomes more manageable and transparent than in the conventional setting where uniform sliding motion is assumed from $t=-\\infty$ to $t=+\\infty$. One avoids separating off a reversible interparticle force (independent of friction) from the total force. Moreover, the cases of temperatures $T=0$ and finite $T$ are treated on the same fo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1403.6635","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":"2026-05-18T02:55:28Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GWURjne1nXd3886RHksJYw1+5kcTMzeIyUAXFQM82Savjaaq3t7URioutj70mNwMj6uqAVomh73s29CsleUrBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-28T14:39:53.391665Z"},"content_sha256":"8f0cbac706164ee27968357e5b6fdb8d806ebff6912758668abb031691119b44","schema_version":"1.0","event_id":"sha256:8f0cbac706164ee27968357e5b6fdb8d806ebff6912758668abb031691119b44"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/32DURC54EODKMM4YCAVXU425JN/bundle.json","state_url":"https://pith.science/pith/32DURC54EODKMM4YCAVXU425JN/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/32DURC54EODKMM4YCAVXU425JN/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":"2026-06-28T14:39:53Z","links":{"resolver":"https://pith.science/pith/32DURC54EODKMM4YCAVXU425JN","bundle":"https://pith.science/pith/32DURC54EODKMM4YCAVXU425JN/bundle.json","state":"https://pith.science/pith/32DURC54EODKMM4YCAVXU425JN/state.json","well_known_bundle":"https://pith.science/.well-known/pith/32DURC54EODKMM4YCAVXU425JN/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:32DURC54EODKMM4YCAVXU425JN","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":"5b0b28cf1989d4fcac2c6a93deb1052043b9330a1d1b7a7f8caa25c8dc853d0d","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2014-03-26T11:41:06Z","title_canon_sha256":"d7a4202a2455217e7890226ff366b2422871d3d40e172e4892ebfae16a93b890"},"schema_version":"1.0","source":{"id":"1403.6635","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1403.6635","created_at":"2026-05-18T02:55:28Z"},{"alias_kind":"arxiv_version","alias_value":"1403.6635v1","created_at":"2026-05-18T02:55:28Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1403.6635","created_at":"2026-05-18T02:55:28Z"},{"alias_kind":"pith_short_12","alias_value":"32DURC54EODK","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_16","alias_value":"32DURC54EODKMM4Y","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_8","alias_value":"32DURC54","created_at":"2026-05-18T12:28:11Z"}],"graph_snapshots":[{"event_id":"sha256:8f0cbac706164ee27968357e5b6fdb8d806ebff6912758668abb031691119b44","target":"graph","created_at":"2026-05-18T02:55:28Z","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":"The Casimir friction problem for dielectric plates that move parallel to each other is treated by assuming one of the plates to be at rest. The other performs a closed loop motion in the longitudinal direction. Therewith by use of energy dissipation the formalism becomes more manageable and transparent than in the conventional setting where uniform sliding motion is assumed from $t=-\\infty$ to $t=+\\infty$. One avoids separating off a reversible interparticle force (independent of friction) from the total force. Moreover, the cases of temperatures $T=0$ and finite $T$ are treated on the same fo","authors_text":"Iver Brevik, Johan S. H{\\o}ye","cross_cats":["cond-mat.stat-mech"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2014-03-26T11:41:06Z","title":"Casimir friction at zero and finite temperatures"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1403.6635","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":"sha256:78e8de260295cfe450825ed4cdd5225bf3cb079362ad854b9bd0e40088b582f0","target":"record","created_at":"2026-05-18T02:55:28Z","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":"5b0b28cf1989d4fcac2c6a93deb1052043b9330a1d1b7a7f8caa25c8dc853d0d","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2014-03-26T11:41:06Z","title_canon_sha256":"d7a4202a2455217e7890226ff366b2422871d3d40e172e4892ebfae16a93b890"},"schema_version":"1.0","source":{"id":"1403.6635","kind":"arxiv","version":1}},"canonical_sha256":"de87488bbc2386a63398102b7a735d4b4a071fe4236b194348371710ef36ae49","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"de87488bbc2386a63398102b7a735d4b4a071fe4236b194348371710ef36ae49","first_computed_at":"2026-05-18T02:55:28.441850Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:55:28.441850Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"aO/XgYGwAchwO9JtYARiPTfPn2FHZldkc83rRUS7PA4WuXbcZNHnMnajwXtgQmUSsYpb+nvAuirtncgBgI81Aw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:55:28.442546Z","signed_message":"canonical_sha256_bytes"},"source_id":"1403.6635","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:78e8de260295cfe450825ed4cdd5225bf3cb079362ad854b9bd0e40088b582f0","sha256:8f0cbac706164ee27968357e5b6fdb8d806ebff6912758668abb031691119b44"],"state_sha256":"63b5ab7cc93f62a0066c20ef4aa75cff1203d325adb7bf61464c3575d117e324"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"C79JDGpfOM6qEFCeVA7CrB8yHMUEHXWS+kt/kU93dA9BeLyA9iaySS1bWme+QQe418QPI1RdWDZMMVN87EkMAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-28T14:39:53.393455Z","bundle_sha256":"3adeb16f100a92de53a22e212d475a388102282b4ee7f224233fc7d92b4ae5dc"}}