{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:YBKTIKQOZ7YIHVJ64OUIUDBEIL","short_pith_number":"pith:YBKTIKQO","canonical_record":{"source":{"id":"1808.10404","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2018-08-30T17:15:47Z","cross_cats_sorted":["cond-mat.mtrl-sci","physics.comp-ph"],"title_canon_sha256":"03a58725603c4ee5be7011cbf1941f7839eeaea3b150e3019c51b27dc0255d27","abstract_canon_sha256":"50fbe10dd0c6ae4948e2c8ba80e6cbc5f0c6636753190c5ce3ffe8c051a5ab30"},"schema_version":"1.0"},"canonical_sha256":"c055342a0ecff083d53ee3a88a0c2442d356b3c72fdf4f01719c54c911991434","source":{"kind":"arxiv","id":"1808.10404","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1808.10404","created_at":"2026-05-17T23:57:40Z"},{"alias_kind":"arxiv_version","alias_value":"1808.10404v1","created_at":"2026-05-17T23:57:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1808.10404","created_at":"2026-05-17T23:57:40Z"},{"alias_kind":"pith_short_12","alias_value":"YBKTIKQOZ7YI","created_at":"2026-05-18T12:33:04Z"},{"alias_kind":"pith_short_16","alias_value":"YBKTIKQOZ7YIHVJ6","created_at":"2026-05-18T12:33:04Z"},{"alias_kind":"pith_short_8","alias_value":"YBKTIKQO","created_at":"2026-05-18T12:33:04Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:YBKTIKQOZ7YIHVJ64OUIUDBEIL","target":"record","payload":{"canonical_record":{"source":{"id":"1808.10404","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2018-08-30T17:15:47Z","cross_cats_sorted":["cond-mat.mtrl-sci","physics.comp-ph"],"title_canon_sha256":"03a58725603c4ee5be7011cbf1941f7839eeaea3b150e3019c51b27dc0255d27","abstract_canon_sha256":"50fbe10dd0c6ae4948e2c8ba80e6cbc5f0c6636753190c5ce3ffe8c051a5ab30"},"schema_version":"1.0"},"canonical_sha256":"c055342a0ecff083d53ee3a88a0c2442d356b3c72fdf4f01719c54c911991434","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:57:40.211502Z","signature_b64":"2krZGN7GHtPkfpTMJy4J6GWxDUW+aMc622J8l48MuCfz6bB/Tp+5q0GT/B62f5nV3/ABWHpDLuHsqM6XORe7CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c055342a0ecff083d53ee3a88a0c2442d356b3c72fdf4f01719c54c911991434","last_reissued_at":"2026-05-17T23:57:40.210969Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:57:40.210969Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1808.10404","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":"2026-05-17T23:57:40Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"h3KaBT77TMpOAf8t42ofHJkDwRx54bDNuRLJ0vilegv+aL88q2S2AdgXHoCGnv3dNd9Fn57Mg82z3lm933BGBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T15:54:22.321162Z"},"content_sha256":"6dea3d7eee51c08a4d7eb4617c786a4720b58f28ad1d78fb3223f358cf646e76","schema_version":"1.0","event_id":"sha256:6dea3d7eee51c08a4d7eb4617c786a4720b58f28ad1d78fb3223f358cf646e76"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:YBKTIKQOZ7YIHVJ64OUIUDBEIL","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Electron-hole correlations govern Auger recombination in nanostructures","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci","physics.comp-ph"],"primary_cat":"cond-mat.mes-hall","authors_text":"Eran Rabani, John P. Philbin","submitted_at":"2018-08-30T17:15:47Z","abstract_excerpt":"The fast nonradiative decay of multiexcitonic states via Auger recombination is a fundamental process affecting a variety of applications based on semiconductor nanostructures. From a theoretical perspective, the description of Auger recombination in confined semiconductor nanostructures is a challenging task due to the large number of valance electrons and exponentially growing number of excited excitonic and biexcitonic states that are coupled by the Coulomb interaction. These challenges have restricted the treatment of Auger recombination to simple, noninteracting electron-hole models. Here"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1808.10404","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":"2026-05-17T23:57:40Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+hMTjtq6pGuPsZfsry9aEcqLAsOLY0NwR//PIBH1XCPA0MNQe8s9NqbwKQd1TKw8w8b2iv5tDxutkj5uxQs/Aw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T15:54:22.321856Z"},"content_sha256":"488e412a5f985345d01e2def51e04b7340a225112db8b833cf9219c374299f70","schema_version":"1.0","event_id":"sha256:488e412a5f985345d01e2def51e04b7340a225112db8b833cf9219c374299f70"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/YBKTIKQOZ7YIHVJ64OUIUDBEIL/bundle.json","state_url":"https://pith.science/pith/YBKTIKQOZ7YIHVJ64OUIUDBEIL/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/YBKTIKQOZ7YIHVJ64OUIUDBEIL/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":"2026-06-11T15:54:22Z","links":{"resolver":"https://pith.science/pith/YBKTIKQOZ7YIHVJ64OUIUDBEIL","bundle":"https://pith.science/pith/YBKTIKQOZ7YIHVJ64OUIUDBEIL/bundle.json","state":"https://pith.science/pith/YBKTIKQOZ7YIHVJ64OUIUDBEIL/state.json","well_known_bundle":"https://pith.science/.well-known/pith/YBKTIKQOZ7YIHVJ64OUIUDBEIL/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:YBKTIKQOZ7YIHVJ64OUIUDBEIL","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":"50fbe10dd0c6ae4948e2c8ba80e6cbc5f0c6636753190c5ce3ffe8c051a5ab30","cross_cats_sorted":["cond-mat.mtrl-sci","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2018-08-30T17:15:47Z","title_canon_sha256":"03a58725603c4ee5be7011cbf1941f7839eeaea3b150e3019c51b27dc0255d27"},"schema_version":"1.0","source":{"id":"1808.10404","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1808.10404","created_at":"2026-05-17T23:57:40Z"},{"alias_kind":"arxiv_version","alias_value":"1808.10404v1","created_at":"2026-05-17T23:57:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1808.10404","created_at":"2026-05-17T23:57:40Z"},{"alias_kind":"pith_short_12","alias_value":"YBKTIKQOZ7YI","created_at":"2026-05-18T12:33:04Z"},{"alias_kind":"pith_short_16","alias_value":"YBKTIKQOZ7YIHVJ6","created_at":"2026-05-18T12:33:04Z"},{"alias_kind":"pith_short_8","alias_value":"YBKTIKQO","created_at":"2026-05-18T12:33:04Z"}],"graph_snapshots":[{"event_id":"sha256:488e412a5f985345d01e2def51e04b7340a225112db8b833cf9219c374299f70","target":"graph","created_at":"2026-05-17T23:57:40Z","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":"The fast nonradiative decay of multiexcitonic states via Auger recombination is a fundamental process affecting a variety of applications based on semiconductor nanostructures. From a theoretical perspective, the description of Auger recombination in confined semiconductor nanostructures is a challenging task due to the large number of valance electrons and exponentially growing number of excited excitonic and biexcitonic states that are coupled by the Coulomb interaction. These challenges have restricted the treatment of Auger recombination to simple, noninteracting electron-hole models. Here","authors_text":"Eran Rabani, John P. Philbin","cross_cats":["cond-mat.mtrl-sci","physics.comp-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2018-08-30T17:15:47Z","title":"Electron-hole correlations govern Auger recombination in nanostructures"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1808.10404","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":"sha256:6dea3d7eee51c08a4d7eb4617c786a4720b58f28ad1d78fb3223f358cf646e76","target":"record","created_at":"2026-05-17T23:57:40Z","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":"50fbe10dd0c6ae4948e2c8ba80e6cbc5f0c6636753190c5ce3ffe8c051a5ab30","cross_cats_sorted":["cond-mat.mtrl-sci","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2018-08-30T17:15:47Z","title_canon_sha256":"03a58725603c4ee5be7011cbf1941f7839eeaea3b150e3019c51b27dc0255d27"},"schema_version":"1.0","source":{"id":"1808.10404","kind":"arxiv","version":1}},"canonical_sha256":"c055342a0ecff083d53ee3a88a0c2442d356b3c72fdf4f01719c54c911991434","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c055342a0ecff083d53ee3a88a0c2442d356b3c72fdf4f01719c54c911991434","first_computed_at":"2026-05-17T23:57:40.210969Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:57:40.210969Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"2krZGN7GHtPkfpTMJy4J6GWxDUW+aMc622J8l48MuCfz6bB/Tp+5q0GT/B62f5nV3/ABWHpDLuHsqM6XORe7CQ==","signature_status":"signed_v1","signed_at":"2026-05-17T23:57:40.211502Z","signed_message":"canonical_sha256_bytes"},"source_id":"1808.10404","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6dea3d7eee51c08a4d7eb4617c786a4720b58f28ad1d78fb3223f358cf646e76","sha256:488e412a5f985345d01e2def51e04b7340a225112db8b833cf9219c374299f70"],"state_sha256":"6b47748855d41682bbf8eb18aaa5caaae1eea4ae3047e6e974a69ba79fb4c1ed"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"faOKpYSOvZV/Sy64Bkcu1HK305O9oDy27qGXJQfpu4zZhvW5GNhvS/6Dteu4uaBNeEuyNLKI7NCnLqBOrwe6Ag==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-11T15:54:22.325901Z","bundle_sha256":"527bdb397094890e8de2780a029abd8bdd6acc418a4755a59dfb5c71f052f5f9"}}