{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:4BYDPU7W32QJCUZ736FQJCUG5Z","short_pith_number":"pith:4BYDPU7W","canonical_record":{"source":{"id":"1709.07323","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-09-21T13:44:48Z","cross_cats_sorted":[],"title_canon_sha256":"c777941d78c2ffbfa9a9914feac86cbd08e3e623959c24d39bb40fb06112ef51","abstract_canon_sha256":"15ded2b2ff0ef2c476907a331a4e4dde9738f6777bc48c512d1bd6a724e55889"},"schema_version":"1.0"},"canonical_sha256":"e07037d3f6dea091533fdf8b048a86ee79381ece8659ee8e5f4ff6647bb156df","source":{"kind":"arxiv","id":"1709.07323","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1709.07323","created_at":"2026-05-18T00:26:36Z"},{"alias_kind":"arxiv_version","alias_value":"1709.07323v2","created_at":"2026-05-18T00:26:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1709.07323","created_at":"2026-05-18T00:26:36Z"},{"alias_kind":"pith_short_12","alias_value":"4BYDPU7W32QJ","created_at":"2026-05-18T12:30:58Z"},{"alias_kind":"pith_short_16","alias_value":"4BYDPU7W32QJCUZ7","created_at":"2026-05-18T12:30:58Z"},{"alias_kind":"pith_short_8","alias_value":"4BYDPU7W","created_at":"2026-05-18T12:30:58Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:4BYDPU7W32QJCUZ736FQJCUG5Z","target":"record","payload":{"canonical_record":{"source":{"id":"1709.07323","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-09-21T13:44:48Z","cross_cats_sorted":[],"title_canon_sha256":"c777941d78c2ffbfa9a9914feac86cbd08e3e623959c24d39bb40fb06112ef51","abstract_canon_sha256":"15ded2b2ff0ef2c476907a331a4e4dde9738f6777bc48c512d1bd6a724e55889"},"schema_version":"1.0"},"canonical_sha256":"e07037d3f6dea091533fdf8b048a86ee79381ece8659ee8e5f4ff6647bb156df","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:26:36.447667Z","signature_b64":"s70EAY9w8jwsfVGtc26f1r5zQ4hgsyZVz3F9kcrivmD8J5gwWE1/M7NkLQgfo4hqh19mkKIG235so/eeHcwPBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e07037d3f6dea091533fdf8b048a86ee79381ece8659ee8e5f4ff6647bb156df","last_reissued_at":"2026-05-18T00:26:36.446943Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:26:36.446943Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1709.07323","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:26:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nF3f08hetgypQh/Lg/YZaqNIzRlDCY6rz4dg9uRbxgWQMAUhpFf543DFeFZXTdB7xkr7mo7VrbwEniH1KmJ3CQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T13:23:22.450800Z"},"content_sha256":"b5e4e339e378ee2f001826557d90d1b56793dc0bd86cc967c15c03954c7893b8","schema_version":"1.0","event_id":"sha256:b5e4e339e378ee2f001826557d90d1b56793dc0bd86cc967c15c03954c7893b8"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:4BYDPU7W32QJCUZ736FQJCUG5Z","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Exciton lifetime and emission polarization dispersion in strongly in-plane asymmetric nanostructures","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"A. Mary\\'nski, A. Somers, G. S\\k{e}k, J. Misiewicz, J. P. Reithmaier, K. Gawarecki, {\\L}. Dusanowski, M. Gawe{\\l}czyk, M. Syperek, P. Mrowi\\'nski, S. H\\\"ofling","submitted_at":"2017-09-21T13:44:48Z","abstract_excerpt":"We present experimental and theoretical investigation of exciton recombination dynamics and the related polarization of emission in highly in-plane asymmetric nanostructures. Considering general asymmetry- and size-driven effects, we illustrate them with a detailed analysis of InAs/AlGaInAs/InP elongated quantum dots. These offer a widely varied confinement characteristics tuned by size and geometry that are tailored during the growth process, which leads to emission in the application-relevant spectral range of 1.25-1.65 {\\mu}m. By exploring the interplay of the very shallow hole confining po"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1709.07323","kind":"arxiv","version":2},"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":"2026-05-18T00:26:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Ul6S5JynR8y2VFzlwhcpJxSV7nW2fCVdIG08ph14eCbqPKdSUIa5vi3Fw+jhBdrFL+McNfum/EkYthHZDRiaAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T13:23:22.451467Z"},"content_sha256":"231f10c2eb9ef271e9165f5c0e51ad7faef1bc6834f18e4c3483f951f057e8e2","schema_version":"1.0","event_id":"sha256:231f10c2eb9ef271e9165f5c0e51ad7faef1bc6834f18e4c3483f951f057e8e2"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/4BYDPU7W32QJCUZ736FQJCUG5Z/bundle.json","state_url":"https://pith.science/pith/4BYDPU7W32QJCUZ736FQJCUG5Z/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/4BYDPU7W32QJCUZ736FQJCUG5Z/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":"2026-05-25T13:23:22Z","links":{"resolver":"https://pith.science/pith/4BYDPU7W32QJCUZ736FQJCUG5Z","bundle":"https://pith.science/pith/4BYDPU7W32QJCUZ736FQJCUG5Z/bundle.json","state":"https://pith.science/pith/4BYDPU7W32QJCUZ736FQJCUG5Z/state.json","well_known_bundle":"https://pith.science/.well-known/pith/4BYDPU7W32QJCUZ736FQJCUG5Z/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:4BYDPU7W32QJCUZ736FQJCUG5Z","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":"15ded2b2ff0ef2c476907a331a4e4dde9738f6777bc48c512d1bd6a724e55889","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-09-21T13:44:48Z","title_canon_sha256":"c777941d78c2ffbfa9a9914feac86cbd08e3e623959c24d39bb40fb06112ef51"},"schema_version":"1.0","source":{"id":"1709.07323","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1709.07323","created_at":"2026-05-18T00:26:36Z"},{"alias_kind":"arxiv_version","alias_value":"1709.07323v2","created_at":"2026-05-18T00:26:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1709.07323","created_at":"2026-05-18T00:26:36Z"},{"alias_kind":"pith_short_12","alias_value":"4BYDPU7W32QJ","created_at":"2026-05-18T12:30:58Z"},{"alias_kind":"pith_short_16","alias_value":"4BYDPU7W32QJCUZ7","created_at":"2026-05-18T12:30:58Z"},{"alias_kind":"pith_short_8","alias_value":"4BYDPU7W","created_at":"2026-05-18T12:30:58Z"}],"graph_snapshots":[{"event_id":"sha256:231f10c2eb9ef271e9165f5c0e51ad7faef1bc6834f18e4c3483f951f057e8e2","target":"graph","created_at":"2026-05-18T00:26:36Z","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 present experimental and theoretical investigation of exciton recombination dynamics and the related polarization of emission in highly in-plane asymmetric nanostructures. Considering general asymmetry- and size-driven effects, we illustrate them with a detailed analysis of InAs/AlGaInAs/InP elongated quantum dots. These offer a widely varied confinement characteristics tuned by size and geometry that are tailored during the growth process, which leads to emission in the application-relevant spectral range of 1.25-1.65 {\\mu}m. By exploring the interplay of the very shallow hole confining po","authors_text":"A. Mary\\'nski, A. Somers, G. S\\k{e}k, J. Misiewicz, J. P. Reithmaier, K. Gawarecki, {\\L}. Dusanowski, M. Gawe{\\l}czyk, M. Syperek, P. Mrowi\\'nski, S. H\\\"ofling","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-09-21T13:44:48Z","title":"Exciton lifetime and emission polarization dispersion in strongly in-plane asymmetric nanostructures"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1709.07323","kind":"arxiv","version":2},"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:b5e4e339e378ee2f001826557d90d1b56793dc0bd86cc967c15c03954c7893b8","target":"record","created_at":"2026-05-18T00:26:36Z","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":"15ded2b2ff0ef2c476907a331a4e4dde9738f6777bc48c512d1bd6a724e55889","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-09-21T13:44:48Z","title_canon_sha256":"c777941d78c2ffbfa9a9914feac86cbd08e3e623959c24d39bb40fb06112ef51"},"schema_version":"1.0","source":{"id":"1709.07323","kind":"arxiv","version":2}},"canonical_sha256":"e07037d3f6dea091533fdf8b048a86ee79381ece8659ee8e5f4ff6647bb156df","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e07037d3f6dea091533fdf8b048a86ee79381ece8659ee8e5f4ff6647bb156df","first_computed_at":"2026-05-18T00:26:36.446943Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:26:36.446943Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"s70EAY9w8jwsfVGtc26f1r5zQ4hgsyZVz3F9kcrivmD8J5gwWE1/M7NkLQgfo4hqh19mkKIG235so/eeHcwPBA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:26:36.447667Z","signed_message":"canonical_sha256_bytes"},"source_id":"1709.07323","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b5e4e339e378ee2f001826557d90d1b56793dc0bd86cc967c15c03954c7893b8","sha256:231f10c2eb9ef271e9165f5c0e51ad7faef1bc6834f18e4c3483f951f057e8e2"],"state_sha256":"122568702abaaaf62c413918ef222213990c7b66ccef617771e2fff2da358618"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"O9zvKkwrW9eaFeDaqo0qcadJUIGii8J0U5mHj+VwTrE9/mlIS4+yPRtszXlfCM81zYy03ZrLT0E/XoSB58ZGDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T13:23:22.454911Z","bundle_sha256":"0fbbf152b001860ea50832226a5f102a122700518f9a33d435f7c5502f3125b0"}}