{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:JJTUYRINA7H2FFAD4DP6HNGFSP","short_pith_number":"pith:JJTUYRIN","canonical_record":{"source":{"id":"1602.02734","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2016-02-08T20:37:14Z","cross_cats_sorted":["cond-mat.soft","physics.chem-ph"],"title_canon_sha256":"174e500fd236953a1b82cb17b401a306cfdaa2f3a0f8853aab10f91d21137a1c","abstract_canon_sha256":"9626a14877681b456a3a2c4a9b8ad88b27ada012e91a2609516edb6f981c45d6"},"schema_version":"1.0"},"canonical_sha256":"4a674c450d07cfa29403e0dfe3b4c593f3b364ff3f96514b86813563aa027723","source":{"kind":"arxiv","id":"1602.02734","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1602.02734","created_at":"2026-05-18T01:09:41Z"},{"alias_kind":"arxiv_version","alias_value":"1602.02734v4","created_at":"2026-05-18T01:09:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1602.02734","created_at":"2026-05-18T01:09:41Z"},{"alias_kind":"pith_short_12","alias_value":"JJTUYRINA7H2","created_at":"2026-05-18T12:30:25Z"},{"alias_kind":"pith_short_16","alias_value":"JJTUYRINA7H2FFAD","created_at":"2026-05-18T12:30:25Z"},{"alias_kind":"pith_short_8","alias_value":"JJTUYRIN","created_at":"2026-05-18T12:30:25Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:JJTUYRINA7H2FFAD4DP6HNGFSP","target":"record","payload":{"canonical_record":{"source":{"id":"1602.02734","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2016-02-08T20:37:14Z","cross_cats_sorted":["cond-mat.soft","physics.chem-ph"],"title_canon_sha256":"174e500fd236953a1b82cb17b401a306cfdaa2f3a0f8853aab10f91d21137a1c","abstract_canon_sha256":"9626a14877681b456a3a2c4a9b8ad88b27ada012e91a2609516edb6f981c45d6"},"schema_version":"1.0"},"canonical_sha256":"4a674c450d07cfa29403e0dfe3b4c593f3b364ff3f96514b86813563aa027723","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:09:41.770795Z","signature_b64":"XPo2i6wRsbHKC6SwVRmO6FZRhr8+MhUy1wiPYB2HcjrIge/QiaQ4xT5MqLYU8BD4ln7zIk/x/dnhKRZu7GknAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4a674c450d07cfa29403e0dfe3b4c593f3b364ff3f96514b86813563aa027723","last_reissued_at":"2026-05-18T01:09:41.770338Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:09:41.770338Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1602.02734","source_version":4,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:09:41Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4Mpi94LSLtALYCfbXFefEMgCu93Q1E2Z0ZsABgPQnSBSHZJFNaKsAit/ijLb3BDjKU45vVTWBCKm46KKUvnDDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T06:48:29.625124Z"},"content_sha256":"6ca52aa184a1729310228ee8cf0fe78433b24fffed4d3b5579a86c3f29e72e14","schema_version":"1.0","event_id":"sha256:6ca52aa184a1729310228ee8cf0fe78433b24fffed4d3b5579a86c3f29e72e14"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:JJTUYRINA7H2FFAD4DP6HNGFSP","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Non-equilibrium simulations of thermally induced electric fields in water","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.soft","physics.chem-ph"],"primary_cat":"physics.comp-ph","authors_text":"An{\\dj}ela \\v{S}ari\\'c, Christoph Dellago, Daan Frenkel, Domagoj Fijan, Martin Neumann, Peter Wirnsberger","submitted_at":"2016-02-08T20:37:14Z","abstract_excerpt":"Using non-equilibrium molecular dynamics simulations, it has been recently demonstrated that water molecules align in response to an imposed temperature gradient, resulting in an effective electric field. Here, we investigate how thermally induced fields depend on the underlying treatment of long-ranged interactions. For the short-ranged Wolf method and Ewald summation, we find the peak strength of the field to range between $2 \\times 10^7$ and $5 \\times 10^7~\\text{V/m}$ for a temperature gradient of $5.2~\\text{K/}\\unicode{x212B}$. Our value for the Wolf method is therefore an order of magnitu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1602.02734","kind":"arxiv","version":4},"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":"2026-05-18T01:09:41Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cwTkFVLpP/ZPN2cmvMk8jw4+GiViMuc1+XBBfx2CCbwfgE5F6Pdb2fpykV/HL9p5PaQe7rTjGVigRuCmOQqXAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T06:48:29.625750Z"},"content_sha256":"c8c604dfdba3f6a4fb685913487d07d0bb8d7b91cc13fc4a2ea027773538667c","schema_version":"1.0","event_id":"sha256:c8c604dfdba3f6a4fb685913487d07d0bb8d7b91cc13fc4a2ea027773538667c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/JJTUYRINA7H2FFAD4DP6HNGFSP/bundle.json","state_url":"https://pith.science/pith/JJTUYRINA7H2FFAD4DP6HNGFSP/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/JJTUYRINA7H2FFAD4DP6HNGFSP/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":"2026-05-27T06:48:29Z","links":{"resolver":"https://pith.science/pith/JJTUYRINA7H2FFAD4DP6HNGFSP","bundle":"https://pith.science/pith/JJTUYRINA7H2FFAD4DP6HNGFSP/bundle.json","state":"https://pith.science/pith/JJTUYRINA7H2FFAD4DP6HNGFSP/state.json","well_known_bundle":"https://pith.science/.well-known/pith/JJTUYRINA7H2FFAD4DP6HNGFSP/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:JJTUYRINA7H2FFAD4DP6HNGFSP","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":"9626a14877681b456a3a2c4a9b8ad88b27ada012e91a2609516edb6f981c45d6","cross_cats_sorted":["cond-mat.soft","physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2016-02-08T20:37:14Z","title_canon_sha256":"174e500fd236953a1b82cb17b401a306cfdaa2f3a0f8853aab10f91d21137a1c"},"schema_version":"1.0","source":{"id":"1602.02734","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1602.02734","created_at":"2026-05-18T01:09:41Z"},{"alias_kind":"arxiv_version","alias_value":"1602.02734v4","created_at":"2026-05-18T01:09:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1602.02734","created_at":"2026-05-18T01:09:41Z"},{"alias_kind":"pith_short_12","alias_value":"JJTUYRINA7H2","created_at":"2026-05-18T12:30:25Z"},{"alias_kind":"pith_short_16","alias_value":"JJTUYRINA7H2FFAD","created_at":"2026-05-18T12:30:25Z"},{"alias_kind":"pith_short_8","alias_value":"JJTUYRIN","created_at":"2026-05-18T12:30:25Z"}],"graph_snapshots":[{"event_id":"sha256:c8c604dfdba3f6a4fb685913487d07d0bb8d7b91cc13fc4a2ea027773538667c","target":"graph","created_at":"2026-05-18T01:09:41Z","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":"Using non-equilibrium molecular dynamics simulations, it has been recently demonstrated that water molecules align in response to an imposed temperature gradient, resulting in an effective electric field. Here, we investigate how thermally induced fields depend on the underlying treatment of long-ranged interactions. For the short-ranged Wolf method and Ewald summation, we find the peak strength of the field to range between $2 \\times 10^7$ and $5 \\times 10^7~\\text{V/m}$ for a temperature gradient of $5.2~\\text{K/}\\unicode{x212B}$. Our value for the Wolf method is therefore an order of magnitu","authors_text":"An{\\dj}ela \\v{S}ari\\'c, Christoph Dellago, Daan Frenkel, Domagoj Fijan, Martin Neumann, Peter Wirnsberger","cross_cats":["cond-mat.soft","physics.chem-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2016-02-08T20:37:14Z","title":"Non-equilibrium simulations of thermally induced electric fields in water"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1602.02734","kind":"arxiv","version":4},"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":"sha256:6ca52aa184a1729310228ee8cf0fe78433b24fffed4d3b5579a86c3f29e72e14","target":"record","created_at":"2026-05-18T01:09:41Z","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":"9626a14877681b456a3a2c4a9b8ad88b27ada012e91a2609516edb6f981c45d6","cross_cats_sorted":["cond-mat.soft","physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2016-02-08T20:37:14Z","title_canon_sha256":"174e500fd236953a1b82cb17b401a306cfdaa2f3a0f8853aab10f91d21137a1c"},"schema_version":"1.0","source":{"id":"1602.02734","kind":"arxiv","version":4}},"canonical_sha256":"4a674c450d07cfa29403e0dfe3b4c593f3b364ff3f96514b86813563aa027723","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4a674c450d07cfa29403e0dfe3b4c593f3b364ff3f96514b86813563aa027723","first_computed_at":"2026-05-18T01:09:41.770338Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:09:41.770338Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"XPo2i6wRsbHKC6SwVRmO6FZRhr8+MhUy1wiPYB2HcjrIge/QiaQ4xT5MqLYU8BD4ln7zIk/x/dnhKRZu7GknAw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:09:41.770795Z","signed_message":"canonical_sha256_bytes"},"source_id":"1602.02734","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6ca52aa184a1729310228ee8cf0fe78433b24fffed4d3b5579a86c3f29e72e14","sha256:c8c604dfdba3f6a4fb685913487d07d0bb8d7b91cc13fc4a2ea027773538667c"],"state_sha256":"228e790fba34fe56d0a4f7fa8085af0dba9485390756188f604dd5391e1ccc90"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"I23hjGPnGVgXyLnDLdiac7duC7EFY4I+jjYyDplopqAuWN58AsjsfPvQl/+1/QWauOYBcE2J3Xj4CM2Qo2YoAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T06:48:29.628669Z","bundle_sha256":"c3318b6dbcb88abfa79be8fab0ba9dc369ee0efaa8c13145aa5e630049e38303"}}