{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:ITGRCXIWQ6GZFVLKXRV2DRIX5I","short_pith_number":"pith:ITGRCXIW","canonical_record":{"source":{"id":"1812.01616","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2018-12-04T19:00:03Z","cross_cats_sorted":["physics.app-ph","physics.optics","quant-ph"],"title_canon_sha256":"513054bc6b72ddbbd5347be79b7e48331a42db507347d49cb793bc86ce53ce5f","abstract_canon_sha256":"682ef919cc7c8802d88cc9a784feb7031e3b05fd574eda84cb23ebbafa74f81e"},"schema_version":"1.0"},"canonical_sha256":"44cd115d16878d92d56abc6ba1c517ea2d073f57a23f95ddf6b941b814a33d6a","source":{"kind":"arxiv","id":"1812.01616","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1812.01616","created_at":"2026-05-17T23:53:02Z"},{"alias_kind":"arxiv_version","alias_value":"1812.01616v1","created_at":"2026-05-17T23:53:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1812.01616","created_at":"2026-05-17T23:53:02Z"},{"alias_kind":"pith_short_12","alias_value":"ITGRCXIWQ6GZ","created_at":"2026-05-18T12:32:31Z"},{"alias_kind":"pith_short_16","alias_value":"ITGRCXIWQ6GZFVLK","created_at":"2026-05-18T12:32:31Z"},{"alias_kind":"pith_short_8","alias_value":"ITGRCXIW","created_at":"2026-05-18T12:32:31Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:ITGRCXIWQ6GZFVLKXRV2DRIX5I","target":"record","payload":{"canonical_record":{"source":{"id":"1812.01616","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2018-12-04T19:00:03Z","cross_cats_sorted":["physics.app-ph","physics.optics","quant-ph"],"title_canon_sha256":"513054bc6b72ddbbd5347be79b7e48331a42db507347d49cb793bc86ce53ce5f","abstract_canon_sha256":"682ef919cc7c8802d88cc9a784feb7031e3b05fd574eda84cb23ebbafa74f81e"},"schema_version":"1.0"},"canonical_sha256":"44cd115d16878d92d56abc6ba1c517ea2d073f57a23f95ddf6b941b814a33d6a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:53:02.581827Z","signature_b64":"KpnDEx7p8Pc61Uw0biF5Has/98DqfsscsX1hQba9tdE+RMVR3W79YLfHgBOMexTh3/+ClR2nPPv0l0mhUdubAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"44cd115d16878d92d56abc6ba1c517ea2d073f57a23f95ddf6b941b814a33d6a","last_reissued_at":"2026-05-17T23:53:02.581310Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:53:02.581310Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1812.01616","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":"2026-05-17T23:53:02Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XkvCvXjNahmqZNA4UFW1xUC+Gy+7v/HbOz/L1gXlL1QXWxmRxF235cShLXIz3fYbYe5OX/1E8ZlzVTSC4ICaCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-12T09:15:39.396388Z"},"content_sha256":"a0b28669832c9673912ef4d235521bd6770d60781994eddee2841157969349fa","schema_version":"1.0","event_id":"sha256:a0b28669832c9673912ef4d235521bd6770d60781994eddee2841157969349fa"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:ITGRCXIWQ6GZFVLKXRV2DRIX5I","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Large Stark Tuning of InAs/InP Quantum Dots","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.app-ph","physics.optics","quant-ph"],"primary_cat":"cond-mat.mes-hall","authors_text":"Chang-Min Lee, Christopher J. K. Richardson, Edo Waks, Mustafa Atabey Buyukkaya, Shahriar Aghaeimeibodi","submitted_at":"2018-12-04T19:00:03Z","abstract_excerpt":"InAs/InP quantum dots are excellent sources of telecom single-photon emission and are among the most promising candidates for scalable quantum photonic circuits. However, geometric differences in each quantum dot leads to slightly different emission wavelengths and hinders the possibility of generating multiple identical quantum emitters on the same chip. Stark tuning is an efficient technique to overcome this issue as it can control the emission energy of individual quantum dots through the quantum-confined Stark effect. Realizing this technique in InAs/InP quantum dots has previously been li"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1812.01616","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":"2026-05-17T23:53:02Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0W1EWTo8evcc2JfKIeK0Q3cC0BBYtAWtZT6FJEXVXKIVBPNwUCfY0CAm2Yy4aEMbBfrn778lkxtCZK7oVj6YBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-12T09:15:39.397010Z"},"content_sha256":"3cbd23fd17a0858a797162be58055c5ce836f97a7c52a0fa3f0d506471d716db","schema_version":"1.0","event_id":"sha256:3cbd23fd17a0858a797162be58055c5ce836f97a7c52a0fa3f0d506471d716db"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ITGRCXIWQ6GZFVLKXRV2DRIX5I/bundle.json","state_url":"https://pith.science/pith/ITGRCXIWQ6GZFVLKXRV2DRIX5I/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ITGRCXIWQ6GZFVLKXRV2DRIX5I/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":"2026-06-12T09:15:39Z","links":{"resolver":"https://pith.science/pith/ITGRCXIWQ6GZFVLKXRV2DRIX5I","bundle":"https://pith.science/pith/ITGRCXIWQ6GZFVLKXRV2DRIX5I/bundle.json","state":"https://pith.science/pith/ITGRCXIWQ6GZFVLKXRV2DRIX5I/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ITGRCXIWQ6GZFVLKXRV2DRIX5I/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:ITGRCXIWQ6GZFVLKXRV2DRIX5I","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":"682ef919cc7c8802d88cc9a784feb7031e3b05fd574eda84cb23ebbafa74f81e","cross_cats_sorted":["physics.app-ph","physics.optics","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2018-12-04T19:00:03Z","title_canon_sha256":"513054bc6b72ddbbd5347be79b7e48331a42db507347d49cb793bc86ce53ce5f"},"schema_version":"1.0","source":{"id":"1812.01616","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1812.01616","created_at":"2026-05-17T23:53:02Z"},{"alias_kind":"arxiv_version","alias_value":"1812.01616v1","created_at":"2026-05-17T23:53:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1812.01616","created_at":"2026-05-17T23:53:02Z"},{"alias_kind":"pith_short_12","alias_value":"ITGRCXIWQ6GZ","created_at":"2026-05-18T12:32:31Z"},{"alias_kind":"pith_short_16","alias_value":"ITGRCXIWQ6GZFVLK","created_at":"2026-05-18T12:32:31Z"},{"alias_kind":"pith_short_8","alias_value":"ITGRCXIW","created_at":"2026-05-18T12:32:31Z"}],"graph_snapshots":[{"event_id":"sha256:3cbd23fd17a0858a797162be58055c5ce836f97a7c52a0fa3f0d506471d716db","target":"graph","created_at":"2026-05-17T23:53:02Z","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":"InAs/InP quantum dots are excellent sources of telecom single-photon emission and are among the most promising candidates for scalable quantum photonic circuits. However, geometric differences in each quantum dot leads to slightly different emission wavelengths and hinders the possibility of generating multiple identical quantum emitters on the same chip. Stark tuning is an efficient technique to overcome this issue as it can control the emission energy of individual quantum dots through the quantum-confined Stark effect. Realizing this technique in InAs/InP quantum dots has previously been li","authors_text":"Chang-Min Lee, Christopher J. K. Richardson, Edo Waks, Mustafa Atabey Buyukkaya, Shahriar Aghaeimeibodi","cross_cats":["physics.app-ph","physics.optics","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2018-12-04T19:00:03Z","title":"Large Stark Tuning of InAs/InP Quantum Dots"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1812.01616","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:a0b28669832c9673912ef4d235521bd6770d60781994eddee2841157969349fa","target":"record","created_at":"2026-05-17T23:53:02Z","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":"682ef919cc7c8802d88cc9a784feb7031e3b05fd574eda84cb23ebbafa74f81e","cross_cats_sorted":["physics.app-ph","physics.optics","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2018-12-04T19:00:03Z","title_canon_sha256":"513054bc6b72ddbbd5347be79b7e48331a42db507347d49cb793bc86ce53ce5f"},"schema_version":"1.0","source":{"id":"1812.01616","kind":"arxiv","version":1}},"canonical_sha256":"44cd115d16878d92d56abc6ba1c517ea2d073f57a23f95ddf6b941b814a33d6a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"44cd115d16878d92d56abc6ba1c517ea2d073f57a23f95ddf6b941b814a33d6a","first_computed_at":"2026-05-17T23:53:02.581310Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:53:02.581310Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"KpnDEx7p8Pc61Uw0biF5Has/98DqfsscsX1hQba9tdE+RMVR3W79YLfHgBOMexTh3/+ClR2nPPv0l0mhUdubAQ==","signature_status":"signed_v1","signed_at":"2026-05-17T23:53:02.581827Z","signed_message":"canonical_sha256_bytes"},"source_id":"1812.01616","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a0b28669832c9673912ef4d235521bd6770d60781994eddee2841157969349fa","sha256:3cbd23fd17a0858a797162be58055c5ce836f97a7c52a0fa3f0d506471d716db"],"state_sha256":"5d7deb7fb1603ab3d348da9faf5878974c802399018e734ed0d0d34457f42974"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zTIQLf2x2Afw6HIVp0wp+V2BHwrDlp4l7jGTOrquWbUpFPlRv/b3W/dtZCQhqXhNRmKQDjmm6xGlNOpQ5kTcCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-12T09:15:39.400284Z","bundle_sha256":"b30ee322f3f6158c6595335286f9e51bc0196e98eb03fb8dd418288a90f82ebf"}}