{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:E23FMJEKWMMUQYQCJ3GSZ4AINS","short_pith_number":"pith:E23FMJEK","canonical_record":{"source":{"id":"1004.2969","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.other","submitted_at":"2010-04-17T16:41:12Z","cross_cats_sorted":["cond-mat.mtrl-sci"],"title_canon_sha256":"84e8857a599667944b6a3f3a63eba013253791fad09226d6b98731db9c88caa8","abstract_canon_sha256":"d8320a43cabfb3c24e458da5e7b1996a4acefab09d9cfa0b28e8b1aa9eb146e7"},"schema_version":"1.0"},"canonical_sha256":"26b656248ab3194862024ecd2cf0086c9baec9b69d952771e3fa5720f51e6ad1","source":{"kind":"arxiv","id":"1004.2969","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1004.2969","created_at":"2026-05-18T02:07:57Z"},{"alias_kind":"arxiv_version","alias_value":"1004.2969v1","created_at":"2026-05-18T02:07:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1004.2969","created_at":"2026-05-18T02:07:57Z"},{"alias_kind":"pith_short_12","alias_value":"E23FMJEKWMMU","created_at":"2026-05-18T12:26:06Z"},{"alias_kind":"pith_short_16","alias_value":"E23FMJEKWMMUQYQC","created_at":"2026-05-18T12:26:06Z"},{"alias_kind":"pith_short_8","alias_value":"E23FMJEK","created_at":"2026-05-18T12:26:06Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:E23FMJEKWMMUQYQCJ3GSZ4AINS","target":"record","payload":{"canonical_record":{"source":{"id":"1004.2969","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.other","submitted_at":"2010-04-17T16:41:12Z","cross_cats_sorted":["cond-mat.mtrl-sci"],"title_canon_sha256":"84e8857a599667944b6a3f3a63eba013253791fad09226d6b98731db9c88caa8","abstract_canon_sha256":"d8320a43cabfb3c24e458da5e7b1996a4acefab09d9cfa0b28e8b1aa9eb146e7"},"schema_version":"1.0"},"canonical_sha256":"26b656248ab3194862024ecd2cf0086c9baec9b69d952771e3fa5720f51e6ad1","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:07:57.223937Z","signature_b64":"vOsDo3sX0E9d7VveRHzbhsb2yJSGIQyyqrzV6RA1aA8PxEcMir48KwjpT5eFkndYQDiOu3Nw6pUB3/UK07/eDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"26b656248ab3194862024ecd2cf0086c9baec9b69d952771e3fa5720f51e6ad1","last_reissued_at":"2026-05-18T02:07:57.223249Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:07:57.223249Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1004.2969","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":"2026-05-18T02:07:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lcGJHskO8ojJYD1NtaE4JTpIorngE8R6gPnUKNzHanTxfxh8+QvfWCNM8R0ckzkGn0MF0sNat1Rzi1UoGnkqDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T11:56:33.560113Z"},"content_sha256":"8db026d4d3210b0a5bcab893dff0b8a31f604cc1cb0aa6a0e6bd6fc73ce077af","schema_version":"1.0","event_id":"sha256:8db026d4d3210b0a5bcab893dff0b8a31f604cc1cb0aa6a0e6bd6fc73ce077af"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:E23FMJEKWMMUQYQCJ3GSZ4AINS","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Thermal Fluctuations of the Electric Field in the Presence of Carrier Drift","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"cond-mat.other","authors_text":"Boris Shapiro","submitted_at":"2010-04-17T16:41:12Z","abstract_excerpt":"We consider a semiconductor in a non-equilibrium steady state, with a dc current. On top of the stationary carrier motion there are fluctuations. It is shown that the stationary motion of the carriers (i.e., their drift) can have a profound effect on the electromagnetic field fluctuations in the bulk of the sample as well as outside it, close to the surface (evanescent waves in the near field). The effect is particularly pronounced near the plasma frequency. This is because drift leads to a significant modification of the dispersion relation for the bulk and surface plasmons."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1004.2969","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":"2026-05-18T02:07:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+a+f0YApReVSA9j5lX7vk2Da092PwTGudG2J46sPN+4BpBzD/lVaBvLBcA5UVgUKRc4QEcvlDwFGKQHz0VmkCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T11:56:33.560734Z"},"content_sha256":"9015e9b151daa61d88e922c647f4c4c6482cfc07d791b6423425e3ed28f16754","schema_version":"1.0","event_id":"sha256:9015e9b151daa61d88e922c647f4c4c6482cfc07d791b6423425e3ed28f16754"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/E23FMJEKWMMUQYQCJ3GSZ4AINS/bundle.json","state_url":"https://pith.science/pith/E23FMJEKWMMUQYQCJ3GSZ4AINS/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/E23FMJEKWMMUQYQCJ3GSZ4AINS/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":"2026-05-26T11:56:33Z","links":{"resolver":"https://pith.science/pith/E23FMJEKWMMUQYQCJ3GSZ4AINS","bundle":"https://pith.science/pith/E23FMJEKWMMUQYQCJ3GSZ4AINS/bundle.json","state":"https://pith.science/pith/E23FMJEKWMMUQYQCJ3GSZ4AINS/state.json","well_known_bundle":"https://pith.science/.well-known/pith/E23FMJEKWMMUQYQCJ3GSZ4AINS/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:E23FMJEKWMMUQYQCJ3GSZ4AINS","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":"d8320a43cabfb3c24e458da5e7b1996a4acefab09d9cfa0b28e8b1aa9eb146e7","cross_cats_sorted":["cond-mat.mtrl-sci"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.other","submitted_at":"2010-04-17T16:41:12Z","title_canon_sha256":"84e8857a599667944b6a3f3a63eba013253791fad09226d6b98731db9c88caa8"},"schema_version":"1.0","source":{"id":"1004.2969","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1004.2969","created_at":"2026-05-18T02:07:57Z"},{"alias_kind":"arxiv_version","alias_value":"1004.2969v1","created_at":"2026-05-18T02:07:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1004.2969","created_at":"2026-05-18T02:07:57Z"},{"alias_kind":"pith_short_12","alias_value":"E23FMJEKWMMU","created_at":"2026-05-18T12:26:06Z"},{"alias_kind":"pith_short_16","alias_value":"E23FMJEKWMMUQYQC","created_at":"2026-05-18T12:26:06Z"},{"alias_kind":"pith_short_8","alias_value":"E23FMJEK","created_at":"2026-05-18T12:26:06Z"}],"graph_snapshots":[{"event_id":"sha256:9015e9b151daa61d88e922c647f4c4c6482cfc07d791b6423425e3ed28f16754","target":"graph","created_at":"2026-05-18T02:07:57Z","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 consider a semiconductor in a non-equilibrium steady state, with a dc current. On top of the stationary carrier motion there are fluctuations. It is shown that the stationary motion of the carriers (i.e., their drift) can have a profound effect on the electromagnetic field fluctuations in the bulk of the sample as well as outside it, close to the surface (evanescent waves in the near field). The effect is particularly pronounced near the plasma frequency. This is because drift leads to a significant modification of the dispersion relation for the bulk and surface plasmons.","authors_text":"Boris Shapiro","cross_cats":["cond-mat.mtrl-sci"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.other","submitted_at":"2010-04-17T16:41:12Z","title":"Thermal Fluctuations of the Electric Field in the Presence of Carrier Drift"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1004.2969","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":"sha256:8db026d4d3210b0a5bcab893dff0b8a31f604cc1cb0aa6a0e6bd6fc73ce077af","target":"record","created_at":"2026-05-18T02:07:57Z","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":"d8320a43cabfb3c24e458da5e7b1996a4acefab09d9cfa0b28e8b1aa9eb146e7","cross_cats_sorted":["cond-mat.mtrl-sci"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.other","submitted_at":"2010-04-17T16:41:12Z","title_canon_sha256":"84e8857a599667944b6a3f3a63eba013253791fad09226d6b98731db9c88caa8"},"schema_version":"1.0","source":{"id":"1004.2969","kind":"arxiv","version":1}},"canonical_sha256":"26b656248ab3194862024ecd2cf0086c9baec9b69d952771e3fa5720f51e6ad1","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"26b656248ab3194862024ecd2cf0086c9baec9b69d952771e3fa5720f51e6ad1","first_computed_at":"2026-05-18T02:07:57.223249Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:07:57.223249Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"vOsDo3sX0E9d7VveRHzbhsb2yJSGIQyyqrzV6RA1aA8PxEcMir48KwjpT5eFkndYQDiOu3Nw6pUB3/UK07/eDA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:07:57.223937Z","signed_message":"canonical_sha256_bytes"},"source_id":"1004.2969","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8db026d4d3210b0a5bcab893dff0b8a31f604cc1cb0aa6a0e6bd6fc73ce077af","sha256:9015e9b151daa61d88e922c647f4c4c6482cfc07d791b6423425e3ed28f16754"],"state_sha256":"42e3c27bf1019807b15bb3114ec8ce1d6efdaabc79ff8cf78c2ffa839f9a7909"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+fiUGM6D6fJUT8RgiexwhN4NNYFNw1EjIXdG6um3PfrR/sx7cUfYyb5hAQ+zjbJq6j0K33fM4OoUAer12vL9Bw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T11:56:33.564066Z","bundle_sha256":"dc23df6eb49f09dfac352261342156348f88bceaed253bd2fe5713ebc65a3daf"}}