{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:6XM5ZV3UN7DOXRVYNMTGKHXKXJ","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":"da4191d259b3eb5564e7c5d17e2a1bc90f18c8a9581b1a0d5c4b196e4b35ae95","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2017-07-13T04:58:16Z","title_canon_sha256":"0a02eb9310202057f4fb80e7d978a2fdb0b32e04addd582aa62f4a0356a89b2c"},"schema_version":"1.0","source":{"id":"1708.07108","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1708.07108","created_at":"2026-05-18T00:16:31Z"},{"alias_kind":"arxiv_version","alias_value":"1708.07108v1","created_at":"2026-05-18T00:16:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.07108","created_at":"2026-05-18T00:16:31Z"},{"alias_kind":"pith_short_12","alias_value":"6XM5ZV3UN7DO","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_16","alias_value":"6XM5ZV3UN7DOXRVY","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_8","alias_value":"6XM5ZV3U","created_at":"2026-05-18T12:31:03Z"}],"graph_snapshots":[{"event_id":"sha256:a2835f2116a98aa72a8bea449059a5fbe90ccf2057073c99bd3a8afcb544e228","target":"graph","created_at":"2026-05-18T00:16:31Z","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":"Spincaloritronic signal generation due to thermal spin injection and spin transport is demonstrated in a non-degenerate Si spin valve. The spin-dependent Seebeck effect is used for the spincaloritronic signal generation, and the thermal gradient of about 200 mK at an interface of Fe and Si enables generating a spin voltage of 8 {\\mu}V at room temperature. A simple expansion of a conventional spin drift-diffusion model with taking into account the spin-dependent Seebeck effect shows semiconductor materials are quite potential for the spincaloritronic signal generation comparing with metallic ma","authors_text":"Hayato Koike (2), Japan), Japan. (2) TDK Corporation, Japan. (3) Osaka Univ., Masashi Shiraishi (1) ((1) Kyoto Univ., Naoto Yamashita (1), Shinji Miwa (3), Yoshishige Suzuki (3), Yuichiro Ando (1)","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2017-07-13T04:58:16Z","title":"Spincaloritronic signal generation in non-degenerate Si"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.07108","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":"sha256:35d5206a7c0072445c69590d1b35af2da163e7b3946e7e9f3544efce293b4d94","target":"record","created_at":"2026-05-18T00:16:31Z","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":"da4191d259b3eb5564e7c5d17e2a1bc90f18c8a9581b1a0d5c4b196e4b35ae95","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2017-07-13T04:58:16Z","title_canon_sha256":"0a02eb9310202057f4fb80e7d978a2fdb0b32e04addd582aa62f4a0356a89b2c"},"schema_version":"1.0","source":{"id":"1708.07108","kind":"arxiv","version":1}},"canonical_sha256":"f5d9dcd7746fc6ebc6b86b26651eeaba7e31c5ed9b469da4ab88861dce73be80","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f5d9dcd7746fc6ebc6b86b26651eeaba7e31c5ed9b469da4ab88861dce73be80","first_computed_at":"2026-05-18T00:16:31.552275Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:16:31.552275Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"hYtj0WdONGhXJ5KsZB+ym0EnXlDYGdEWThURe8b7v+x93hUBbk3pDsFzrDYn5kS3IXFoysVhEeOVLqtgbMrlBA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:16:31.552870Z","signed_message":"canonical_sha256_bytes"},"source_id":"1708.07108","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:35d5206a7c0072445c69590d1b35af2da163e7b3946e7e9f3544efce293b4d94","sha256:a2835f2116a98aa72a8bea449059a5fbe90ccf2057073c99bd3a8afcb544e228"],"state_sha256":"576a97706bca2359981eb06aaa7cc70614c8f0fbb9faea4798e76107c7b8774a"}