{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:BIURET4ETGLHEIGPB4LIAHDAQE","short_pith_number":"pith:BIURET4E","canonical_record":{"source":{"id":"1512.05914","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2015-12-18T11:57:04Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"7859d487ebafec0fcf3509b834dfa6b8ae671bc7f8e39b67fff14d898632caf2","abstract_canon_sha256":"30ccef006fd0d5d29d97f006a8c71fa97aff1c2e7eacd30c8537305beb806cbb"},"schema_version":"1.0"},"canonical_sha256":"0a29124f8499967220cf0f16801c608137028ec91c0e97ae8b16cf4b5cd015c0","source":{"kind":"arxiv","id":"1512.05914","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1512.05914","created_at":"2026-05-18T01:13:23Z"},{"alias_kind":"arxiv_version","alias_value":"1512.05914v2","created_at":"2026-05-18T01:13:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1512.05914","created_at":"2026-05-18T01:13:23Z"},{"alias_kind":"pith_short_12","alias_value":"BIURET4ETGLH","created_at":"2026-05-18T12:29:14Z"},{"alias_kind":"pith_short_16","alias_value":"BIURET4ETGLHEIGP","created_at":"2026-05-18T12:29:14Z"},{"alias_kind":"pith_short_8","alias_value":"BIURET4E","created_at":"2026-05-18T12:29:14Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:BIURET4ETGLHEIGPB4LIAHDAQE","target":"record","payload":{"canonical_record":{"source":{"id":"1512.05914","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2015-12-18T11:57:04Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"7859d487ebafec0fcf3509b834dfa6b8ae671bc7f8e39b67fff14d898632caf2","abstract_canon_sha256":"30ccef006fd0d5d29d97f006a8c71fa97aff1c2e7eacd30c8537305beb806cbb"},"schema_version":"1.0"},"canonical_sha256":"0a29124f8499967220cf0f16801c608137028ec91c0e97ae8b16cf4b5cd015c0","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:13:23.815616Z","signature_b64":"e90fxR/K6wrZR8C0t5UI5ukveO3OAV/Tv2qj2RtyNCJt1UfEFYOTCt38ph74w76mo7XbLuzaMTdgnXHpp51tBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0a29124f8499967220cf0f16801c608137028ec91c0e97ae8b16cf4b5cd015c0","last_reissued_at":"2026-05-18T01:13:23.815182Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:13:23.815182Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1512.05914","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":"2026-05-18T01:13:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vFNUD1fFkPQakD17kI7mSqmkFnA4nsMVhGTupZyMGCXODFvL2acHn2dH9WAbg+6Eqi5TUTyDbx0RKVIylst5Ag==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T20:48:18.974422Z"},"content_sha256":"f9fbe2d630c9fed80e8dfe33ac2e016181226f16bd3c639d805cd51523b46332","schema_version":"1.0","event_id":"sha256:f9fbe2d630c9fed80e8dfe33ac2e016181226f16bd3c639d805cd51523b46332"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:BIURET4ETGLHEIGPB4LIAHDAQE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Spectral mapping of heat transfer mechanisms at liquid-solid interfaces","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"physics.comp-ph","authors_text":"J. Oksanen, J. Tulkki, K. S\\\"a\\\"askilahti, S. Volz","submitted_at":"2015-12-18T11:57:04Z","abstract_excerpt":"Thermal transport through liquid-solid interfaces plays an important role in many chemical and biological processes, and better understanding of liquid-solid energy transfer is expected to enable improving the efficiency of thermally driven applications. We determine the spectral distribution of thermal current at liquid-solid interfaces from nonequilibrium molecular dynamics, delivering a detailed picture of the contributions of different vibrational modes to liquid-solid energy transfer. Our results show that surface modes located at the Brillouin zone edge and polarized along the liquid-sol"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1512.05914","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":""},"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":"2026-05-18T01:13:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"W1Bq+24JIVPEY5pKhYJTiXZFcr+uQXutyp0oAqsz0Dxsnxqo+IEPTUlEj185XbT5nPV0rv9+scV/tyONo/bSAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T20:48:18.975154Z"},"content_sha256":"4fa5e2df2ed0bb6353cb50bb10c2350e4f4da4aa259213771fcc35b86734dd57","schema_version":"1.0","event_id":"sha256:4fa5e2df2ed0bb6353cb50bb10c2350e4f4da4aa259213771fcc35b86734dd57"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/BIURET4ETGLHEIGPB4LIAHDAQE/bundle.json","state_url":"https://pith.science/pith/BIURET4ETGLHEIGPB4LIAHDAQE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/BIURET4ETGLHEIGPB4LIAHDAQE/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":"2026-05-31T20:48:18Z","links":{"resolver":"https://pith.science/pith/BIURET4ETGLHEIGPB4LIAHDAQE","bundle":"https://pith.science/pith/BIURET4ETGLHEIGPB4LIAHDAQE/bundle.json","state":"https://pith.science/pith/BIURET4ETGLHEIGPB4LIAHDAQE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/BIURET4ETGLHEIGPB4LIAHDAQE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:BIURET4ETGLHEIGPB4LIAHDAQE","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":"30ccef006fd0d5d29d97f006a8c71fa97aff1c2e7eacd30c8537305beb806cbb","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2015-12-18T11:57:04Z","title_canon_sha256":"7859d487ebafec0fcf3509b834dfa6b8ae671bc7f8e39b67fff14d898632caf2"},"schema_version":"1.0","source":{"id":"1512.05914","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1512.05914","created_at":"2026-05-18T01:13:23Z"},{"alias_kind":"arxiv_version","alias_value":"1512.05914v2","created_at":"2026-05-18T01:13:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1512.05914","created_at":"2026-05-18T01:13:23Z"},{"alias_kind":"pith_short_12","alias_value":"BIURET4ETGLH","created_at":"2026-05-18T12:29:14Z"},{"alias_kind":"pith_short_16","alias_value":"BIURET4ETGLHEIGP","created_at":"2026-05-18T12:29:14Z"},{"alias_kind":"pith_short_8","alias_value":"BIURET4E","created_at":"2026-05-18T12:29:14Z"}],"graph_snapshots":[{"event_id":"sha256:4fa5e2df2ed0bb6353cb50bb10c2350e4f4da4aa259213771fcc35b86734dd57","target":"graph","created_at":"2026-05-18T01:13:23Z","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":"Thermal transport through liquid-solid interfaces plays an important role in many chemical and biological processes, and better understanding of liquid-solid energy transfer is expected to enable improving the efficiency of thermally driven applications. We determine the spectral distribution of thermal current at liquid-solid interfaces from nonequilibrium molecular dynamics, delivering a detailed picture of the contributions of different vibrational modes to liquid-solid energy transfer. Our results show that surface modes located at the Brillouin zone edge and polarized along the liquid-sol","authors_text":"J. Oksanen, J. Tulkki, K. S\\\"a\\\"askilahti, S. Volz","cross_cats":["cond-mat.mes-hall"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2015-12-18T11:57:04Z","title":"Spectral mapping of heat transfer mechanisms at liquid-solid interfaces"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1512.05914","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:f9fbe2d630c9fed80e8dfe33ac2e016181226f16bd3c639d805cd51523b46332","target":"record","created_at":"2026-05-18T01:13:23Z","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":"30ccef006fd0d5d29d97f006a8c71fa97aff1c2e7eacd30c8537305beb806cbb","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2015-12-18T11:57:04Z","title_canon_sha256":"7859d487ebafec0fcf3509b834dfa6b8ae671bc7f8e39b67fff14d898632caf2"},"schema_version":"1.0","source":{"id":"1512.05914","kind":"arxiv","version":2}},"canonical_sha256":"0a29124f8499967220cf0f16801c608137028ec91c0e97ae8b16cf4b5cd015c0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0a29124f8499967220cf0f16801c608137028ec91c0e97ae8b16cf4b5cd015c0","first_computed_at":"2026-05-18T01:13:23.815182Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:13:23.815182Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"e90fxR/K6wrZR8C0t5UI5ukveO3OAV/Tv2qj2RtyNCJt1UfEFYOTCt38ph74w76mo7XbLuzaMTdgnXHpp51tBA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:13:23.815616Z","signed_message":"canonical_sha256_bytes"},"source_id":"1512.05914","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f9fbe2d630c9fed80e8dfe33ac2e016181226f16bd3c639d805cd51523b46332","sha256:4fa5e2df2ed0bb6353cb50bb10c2350e4f4da4aa259213771fcc35b86734dd57"],"state_sha256":"6b6afdfc4560b17ef6220a0dde53d1a116d422826102babbb417916375fc0584"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vcMIYxxswG1lseVqS2ZVdtv0fKS1dv+pQpl4h+h6al4u7P3hpvP5QA7aokAcrd3X+Q3yU9wKDw28Dbc7ni0VCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T20:48:18.979588Z","bundle_sha256":"829069a86ce26d262d4e3a18f5ba87b18874820f1db46840b859bb1e584ec84b"}}