{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2021:KKBZ3L2KBOKYFKIEYGAIUAQ2GC","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":"93f767032e383db79a8438760fb96d3905ad605adf3dcd799f443363093b8a83","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cs.ET","submitted_at":"2021-06-28T15:24:30Z","title_canon_sha256":"eb2eba30701d6fd29812e7e2f52a4d00405342742563628d0c0c71137175e641"},"schema_version":"1.0","source":{"id":"2106.14803","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2106.14803","created_at":"2026-07-05T02:52:54Z"},{"alias_kind":"arxiv_version","alias_value":"2106.14803v1","created_at":"2026-07-05T02:52:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2106.14803","created_at":"2026-07-05T02:52:54Z"},{"alias_kind":"pith_short_12","alias_value":"KKBZ3L2KBOKY","created_at":"2026-07-05T02:52:54Z"},{"alias_kind":"pith_short_16","alias_value":"KKBZ3L2KBOKYFKIE","created_at":"2026-07-05T02:52:54Z"},{"alias_kind":"pith_short_8","alias_value":"KKBZ3L2K","created_at":"2026-07-05T02:52:54Z"}],"graph_snapshots":[{"event_id":"sha256:484e8135b8f2e71da208132ba55397f4cb3a31bdd377eee3b185dab9915546e6","target":"graph","created_at":"2026-07-05T02:52:54Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2106.14803/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Any large-scale spiking neuromorphic system striving for complexity at the level of the human brain and beyond will need to be co-optimized for communication and computation. Such reasoning leads to the proposal for optoelectronic neuromorphic platforms that leverage the complementary properties of optics and electronics. Starting from the conjecture that future large-scale neuromorphic systems will utilize integrated photonics and fiber optics for communication in conjunction with analog electronics for computation, we consider two possible paths towards achieving this vision. The first is a ","authors_text":"Bryce A. Primavera, Jeffrey M. Shainline","cross_cats":["physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cs.ET","submitted_at":"2021-06-28T15:24:30Z","title":"Considerations for neuromorphic supercomputing in semiconducting and superconducting optoelectronic hardware"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2106.14803","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:b7caa280ee990055cf840481dcb2b8e8720952ce93647524854dea2dc7242daf","target":"record","created_at":"2026-07-05T02:52:54Z","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":"93f767032e383db79a8438760fb96d3905ad605adf3dcd799f443363093b8a83","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cs.ET","submitted_at":"2021-06-28T15:24:30Z","title_canon_sha256":"eb2eba30701d6fd29812e7e2f52a4d00405342742563628d0c0c71137175e641"},"schema_version":"1.0","source":{"id":"2106.14803","kind":"arxiv","version":1}},"canonical_sha256":"52839daf4a0b9582a904c1808a021a30a92cad6b331bd918b96a3815f0da4d22","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"52839daf4a0b9582a904c1808a021a30a92cad6b331bd918b96a3815f0da4d22","first_computed_at":"2026-07-05T02:52:54.019064Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T02:52:54.019064Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"DxJ3jhlrvotSBjQ2r23xwSwFQS10veB2/2qFyoSPHcwMXC11nDKPobf1DLlQRAMTGSerLH5iEJAbLDiXOxBBBw==","signature_status":"signed_v1","signed_at":"2026-07-05T02:52:54.019475Z","signed_message":"canonical_sha256_bytes"},"source_id":"2106.14803","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b7caa280ee990055cf840481dcb2b8e8720952ce93647524854dea2dc7242daf","sha256:484e8135b8f2e71da208132ba55397f4cb3a31bdd377eee3b185dab9915546e6"],"state_sha256":"d3c849e52e5d48b965f751b0d0fddc1d8ac2e8d0d8a5edaabc2cfd4f317f144d"}