{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:KREKNJI7QRYPDYRDV6SZ5D63TM","short_pith_number":"pith:KREKNJI7","canonical_record":{"source":{"id":"1312.1508","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2013-12-05T11:36:06Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"4b1979f2017b7c13058d3170b25d9fc763c223488d11aefc39a657e809523855","abstract_canon_sha256":"3df1ff5718b501297a3d1ee5d6de07a6e25512ba4852881d93453ef492430638"},"schema_version":"1.0"},"canonical_sha256":"5448a6a51f8470f1e223afa59e8fdb9b1217cfafab8f52717e7b681466679608","source":{"kind":"arxiv","id":"1312.1508","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1312.1508","created_at":"2026-05-18T02:54:22Z"},{"alias_kind":"arxiv_version","alias_value":"1312.1508v1","created_at":"2026-05-18T02:54:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1312.1508","created_at":"2026-05-18T02:54:22Z"},{"alias_kind":"pith_short_12","alias_value":"KREKNJI7QRYP","created_at":"2026-05-18T12:27:51Z"},{"alias_kind":"pith_short_16","alias_value":"KREKNJI7QRYPDYRD","created_at":"2026-05-18T12:27:51Z"},{"alias_kind":"pith_short_8","alias_value":"KREKNJI7","created_at":"2026-05-18T12:27:51Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:KREKNJI7QRYPDYRDV6SZ5D63TM","target":"record","payload":{"canonical_record":{"source":{"id":"1312.1508","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2013-12-05T11:36:06Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"4b1979f2017b7c13058d3170b25d9fc763c223488d11aefc39a657e809523855","abstract_canon_sha256":"3df1ff5718b501297a3d1ee5d6de07a6e25512ba4852881d93453ef492430638"},"schema_version":"1.0"},"canonical_sha256":"5448a6a51f8470f1e223afa59e8fdb9b1217cfafab8f52717e7b681466679608","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:54:22.329949Z","signature_b64":"H95jQeAFw8uQoaVIFsBDnknN9Ul85q/usOxzbfE58k2PUYG7sWpVwuraxAJfu8i5cNpCSOQgm0qVSf8HSnpbDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5448a6a51f8470f1e223afa59e8fdb9b1217cfafab8f52717e7b681466679608","last_reissued_at":"2026-05-18T02:54:22.329477Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:54:22.329477Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1312.1508","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":"2026-05-18T02:54:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZiJtd6FzgLpt6BJbXSGkDtUTJX0sh/wTnodz3G7TWAgGug6yjwrilfdMuMuxbUU8njY4bmRxdZ8yGPolIO26Cg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-22T09:16:12.409604Z"},"content_sha256":"e70dbdf253e5bfb87fca67e2166dac97364b1c956444305ebb15c8490e643083","schema_version":"1.0","event_id":"sha256:e70dbdf253e5bfb87fca67e2166dac97364b1c956444305ebb15c8490e643083"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:KREKNJI7QRYPDYRDV6SZ5D63TM","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Photoelectron emission from plasmonic nanoparticles: Comparison between surface and volume photoelectric effects","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"physics.optics","authors_text":"Alexander V. Uskov, Andrey V. Lavrinenko, Eoin P. OReilly, Hongxing Xu, Igor E. Protsenko, Renat Sh. Ikhsanov, Sergei V. Zhukovsky, Viktoriia E. Babicheva","submitted_at":"2013-12-05T11:36:06Z","abstract_excerpt":"We study emission of photoelectrons from plasmonic nanoparticles into surrounding matrix. We consider two mechanisms of the photoelectric effect from nanoparticles - surface and volume ones, and use models of these two effects which allow us to obtain analytical results for the photoelectron emission rates from nanoparticle. Calculations have been done for the step potential at surface of spherical nanoparticle, and the simple model for the hot electron cooling have been used. We highlight the effect of the discontinuity of the dielectric permittivity at the nanoparticle boundary in the surfac"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1312.1508","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":"2026-05-18T02:54:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UJr6dvECtskWPGb5In6iWQYtQHt02Rzk5lIf7hDsMnoCvS4igbO/2GkmYxr3YSU90WI7R3Pet5jjDNdd/JIvDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-22T09:16:12.409960Z"},"content_sha256":"d8b4d3eea827de2ffa280b416ffe551304050342a9cbe7571fe5c255860a202e","schema_version":"1.0","event_id":"sha256:d8b4d3eea827de2ffa280b416ffe551304050342a9cbe7571fe5c255860a202e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/KREKNJI7QRYPDYRDV6SZ5D63TM/bundle.json","state_url":"https://pith.science/pith/KREKNJI7QRYPDYRDV6SZ5D63TM/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/KREKNJI7QRYPDYRDV6SZ5D63TM/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":"2026-06-22T09:16:12Z","links":{"resolver":"https://pith.science/pith/KREKNJI7QRYPDYRDV6SZ5D63TM","bundle":"https://pith.science/pith/KREKNJI7QRYPDYRDV6SZ5D63TM/bundle.json","state":"https://pith.science/pith/KREKNJI7QRYPDYRDV6SZ5D63TM/state.json","well_known_bundle":"https://pith.science/.well-known/pith/KREKNJI7QRYPDYRDV6SZ5D63TM/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:KREKNJI7QRYPDYRDV6SZ5D63TM","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":"3df1ff5718b501297a3d1ee5d6de07a6e25512ba4852881d93453ef492430638","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2013-12-05T11:36:06Z","title_canon_sha256":"4b1979f2017b7c13058d3170b25d9fc763c223488d11aefc39a657e809523855"},"schema_version":"1.0","source":{"id":"1312.1508","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1312.1508","created_at":"2026-05-18T02:54:22Z"},{"alias_kind":"arxiv_version","alias_value":"1312.1508v1","created_at":"2026-05-18T02:54:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1312.1508","created_at":"2026-05-18T02:54:22Z"},{"alias_kind":"pith_short_12","alias_value":"KREKNJI7QRYP","created_at":"2026-05-18T12:27:51Z"},{"alias_kind":"pith_short_16","alias_value":"KREKNJI7QRYPDYRD","created_at":"2026-05-18T12:27:51Z"},{"alias_kind":"pith_short_8","alias_value":"KREKNJI7","created_at":"2026-05-18T12:27:51Z"}],"graph_snapshots":[{"event_id":"sha256:d8b4d3eea827de2ffa280b416ffe551304050342a9cbe7571fe5c255860a202e","target":"graph","created_at":"2026-05-18T02:54:22Z","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":"We study emission of photoelectrons from plasmonic nanoparticles into surrounding matrix. We consider two mechanisms of the photoelectric effect from nanoparticles - surface and volume ones, and use models of these two effects which allow us to obtain analytical results for the photoelectron emission rates from nanoparticle. Calculations have been done for the step potential at surface of spherical nanoparticle, and the simple model for the hot electron cooling have been used. We highlight the effect of the discontinuity of the dielectric permittivity at the nanoparticle boundary in the surfac","authors_text":"Alexander V. Uskov, Andrey V. Lavrinenko, Eoin P. OReilly, Hongxing Xu, Igor E. Protsenko, Renat Sh. Ikhsanov, Sergei V. Zhukovsky, Viktoriia E. Babicheva","cross_cats":["cond-mat.mes-hall"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2013-12-05T11:36:06Z","title":"Photoelectron emission from plasmonic nanoparticles: Comparison between surface and volume photoelectric effects"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1312.1508","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:e70dbdf253e5bfb87fca67e2166dac97364b1c956444305ebb15c8490e643083","target":"record","created_at":"2026-05-18T02:54:22Z","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":"3df1ff5718b501297a3d1ee5d6de07a6e25512ba4852881d93453ef492430638","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2013-12-05T11:36:06Z","title_canon_sha256":"4b1979f2017b7c13058d3170b25d9fc763c223488d11aefc39a657e809523855"},"schema_version":"1.0","source":{"id":"1312.1508","kind":"arxiv","version":1}},"canonical_sha256":"5448a6a51f8470f1e223afa59e8fdb9b1217cfafab8f52717e7b681466679608","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5448a6a51f8470f1e223afa59e8fdb9b1217cfafab8f52717e7b681466679608","first_computed_at":"2026-05-18T02:54:22.329477Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:54:22.329477Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"H95jQeAFw8uQoaVIFsBDnknN9Ul85q/usOxzbfE58k2PUYG7sWpVwuraxAJfu8i5cNpCSOQgm0qVSf8HSnpbDA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:54:22.329949Z","signed_message":"canonical_sha256_bytes"},"source_id":"1312.1508","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e70dbdf253e5bfb87fca67e2166dac97364b1c956444305ebb15c8490e643083","sha256:d8b4d3eea827de2ffa280b416ffe551304050342a9cbe7571fe5c255860a202e"],"state_sha256":"86b9e931baa8049ffeeb6813bb030e5fb91b7d901fac144173f837e8796e71af"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cq9qyL70dYhXw6xXkcitqrXWuXErICrs30PzKHDR4SCgy5CU9VqvRAYlR4u2Fq4O4xSbbYJCvEwG2wuB/9PEBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-22T09:16:12.411944Z","bundle_sha256":"130f059b2319ae61a1e9b0184f90c7713c541df22bb5033c23d04a5f51ac536d"}}