{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:KXTA3FGRCMU7GFB6B5KSQWNBRN","short_pith_number":"pith:KXTA3FGR","canonical_record":{"source":{"id":"1802.07047","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2018-02-20T10:27:08Z","cross_cats_sorted":[],"title_canon_sha256":"5fd4cf223d2b00f1d18be86f253e824efe7a532bb994101aadd541a67bb1cc63","abstract_canon_sha256":"0e3995cc940fe1be1d106f3eff7a5995f353a6c89289ed2563c76ad01cb86d54"},"schema_version":"1.0"},"canonical_sha256":"55e60d94d11329f3143e0f552859a18b6b225aa752062b5dca869be47b752cfd","source":{"kind":"arxiv","id":"1802.07047","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1802.07047","created_at":"2026-05-18T00:22:22Z"},{"alias_kind":"arxiv_version","alias_value":"1802.07047v1","created_at":"2026-05-18T00:22:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1802.07047","created_at":"2026-05-18T00:22:22Z"},{"alias_kind":"pith_short_12","alias_value":"KXTA3FGRCMU7","created_at":"2026-05-18T12:32:33Z"},{"alias_kind":"pith_short_16","alias_value":"KXTA3FGRCMU7GFB6","created_at":"2026-05-18T12:32:33Z"},{"alias_kind":"pith_short_8","alias_value":"KXTA3FGR","created_at":"2026-05-18T12:32:33Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:KXTA3FGRCMU7GFB6B5KSQWNBRN","target":"record","payload":{"canonical_record":{"source":{"id":"1802.07047","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2018-02-20T10:27:08Z","cross_cats_sorted":[],"title_canon_sha256":"5fd4cf223d2b00f1d18be86f253e824efe7a532bb994101aadd541a67bb1cc63","abstract_canon_sha256":"0e3995cc940fe1be1d106f3eff7a5995f353a6c89289ed2563c76ad01cb86d54"},"schema_version":"1.0"},"canonical_sha256":"55e60d94d11329f3143e0f552859a18b6b225aa752062b5dca869be47b752cfd","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:22:22.396565Z","signature_b64":"f9yYJHyfp6sYHisF0Xk60AXRmvD/rK+2raNfGB4k6es1qxbLoK28KwmNzxUn4q/SXuYfYq9WGQlrIxGe87UcBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"55e60d94d11329f3143e0f552859a18b6b225aa752062b5dca869be47b752cfd","last_reissued_at":"2026-05-18T00:22:22.396011Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:22:22.396011Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1802.07047","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":"2026-05-18T00:22:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"hhvapDJ+TWP1R8MXZumSHtDCcN07bzpGwLxGWSX9UIlcdWYRDyCbtWDIwUm/gAe7z/ddB6DN8e1YOFiMUo/aBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-10T01:10:40.167962Z"},"content_sha256":"4fc426481f236ac485ac5b8f68c57f3fb58319223fe47424c2ffb46314d36357","schema_version":"1.0","event_id":"sha256:4fc426481f236ac485ac5b8f68c57f3fb58319223fe47424c2ffb46314d36357"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:KXTA3FGRCMU7GFB6B5KSQWNBRN","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Temporal complexity in emission from Anderson localized lasers","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"K Shadak Alee, M. Balasubrahmaniyam, Randhir Kumar, Sushil Mujumdar","submitted_at":"2018-02-20T10:27:08Z","abstract_excerpt":"Anderson localization lasers exploit resonant cavities formed due to structural disorder. The inherent randomness in the structure of these cavities realizes a probability distribution in all cavity parameters such as quality factors, mode volumes, mode structures etc, implying resultant statistical fluctuations in the temporal behavior. Here, we provide the first, direct experimental measurements of temporal width distributions of Anderson localization lasing pulses in intrinsically and extrinsically disordered coupled-microresonator arrays. We first illustrate signature exponential decays in"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1802.07047","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":"2026-05-18T00:22:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"RKAFzSH46Ees63TkyWPPyFOnUBwwvibf68kMHLgt5tjid/PCzZrxUQs36CF8nEcmRkCAp0Vn4lzDMcb0L5tkAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-10T01:10:40.168630Z"},"content_sha256":"1dca59813f43141d2d46c339b8f7cbfd85e1463bdacfc1a846415308954fcbdc","schema_version":"1.0","event_id":"sha256:1dca59813f43141d2d46c339b8f7cbfd85e1463bdacfc1a846415308954fcbdc"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/KXTA3FGRCMU7GFB6B5KSQWNBRN/bundle.json","state_url":"https://pith.science/pith/KXTA3FGRCMU7GFB6B5KSQWNBRN/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/KXTA3FGRCMU7GFB6B5KSQWNBRN/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":"2026-06-10T01:10:40Z","links":{"resolver":"https://pith.science/pith/KXTA3FGRCMU7GFB6B5KSQWNBRN","bundle":"https://pith.science/pith/KXTA3FGRCMU7GFB6B5KSQWNBRN/bundle.json","state":"https://pith.science/pith/KXTA3FGRCMU7GFB6B5KSQWNBRN/state.json","well_known_bundle":"https://pith.science/.well-known/pith/KXTA3FGRCMU7GFB6B5KSQWNBRN/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:KXTA3FGRCMU7GFB6B5KSQWNBRN","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":"0e3995cc940fe1be1d106f3eff7a5995f353a6c89289ed2563c76ad01cb86d54","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2018-02-20T10:27:08Z","title_canon_sha256":"5fd4cf223d2b00f1d18be86f253e824efe7a532bb994101aadd541a67bb1cc63"},"schema_version":"1.0","source":{"id":"1802.07047","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1802.07047","created_at":"2026-05-18T00:22:22Z"},{"alias_kind":"arxiv_version","alias_value":"1802.07047v1","created_at":"2026-05-18T00:22:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1802.07047","created_at":"2026-05-18T00:22:22Z"},{"alias_kind":"pith_short_12","alias_value":"KXTA3FGRCMU7","created_at":"2026-05-18T12:32:33Z"},{"alias_kind":"pith_short_16","alias_value":"KXTA3FGRCMU7GFB6","created_at":"2026-05-18T12:32:33Z"},{"alias_kind":"pith_short_8","alias_value":"KXTA3FGR","created_at":"2026-05-18T12:32:33Z"}],"graph_snapshots":[{"event_id":"sha256:1dca59813f43141d2d46c339b8f7cbfd85e1463bdacfc1a846415308954fcbdc","target":"graph","created_at":"2026-05-18T00:22:22Z","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":"Anderson localization lasers exploit resonant cavities formed due to structural disorder. The inherent randomness in the structure of these cavities realizes a probability distribution in all cavity parameters such as quality factors, mode volumes, mode structures etc, implying resultant statistical fluctuations in the temporal behavior. Here, we provide the first, direct experimental measurements of temporal width distributions of Anderson localization lasing pulses in intrinsically and extrinsically disordered coupled-microresonator arrays. We first illustrate signature exponential decays in","authors_text":"K Shadak Alee, M. Balasubrahmaniyam, Randhir Kumar, Sushil Mujumdar","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2018-02-20T10:27:08Z","title":"Temporal complexity in emission from Anderson localized lasers"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1802.07047","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":"sha256:4fc426481f236ac485ac5b8f68c57f3fb58319223fe47424c2ffb46314d36357","target":"record","created_at":"2026-05-18T00:22:22Z","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":"0e3995cc940fe1be1d106f3eff7a5995f353a6c89289ed2563c76ad01cb86d54","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2018-02-20T10:27:08Z","title_canon_sha256":"5fd4cf223d2b00f1d18be86f253e824efe7a532bb994101aadd541a67bb1cc63"},"schema_version":"1.0","source":{"id":"1802.07047","kind":"arxiv","version":1}},"canonical_sha256":"55e60d94d11329f3143e0f552859a18b6b225aa752062b5dca869be47b752cfd","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"55e60d94d11329f3143e0f552859a18b6b225aa752062b5dca869be47b752cfd","first_computed_at":"2026-05-18T00:22:22.396011Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:22:22.396011Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"f9yYJHyfp6sYHisF0Xk60AXRmvD/rK+2raNfGB4k6es1qxbLoK28KwmNzxUn4q/SXuYfYq9WGQlrIxGe87UcBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:22:22.396565Z","signed_message":"canonical_sha256_bytes"},"source_id":"1802.07047","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4fc426481f236ac485ac5b8f68c57f3fb58319223fe47424c2ffb46314d36357","sha256:1dca59813f43141d2d46c339b8f7cbfd85e1463bdacfc1a846415308954fcbdc"],"state_sha256":"7e8ac48525a749e58256b9d457e001836a554248b33efca72a4aecdd294a2a77"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XKKny7PA5IacOlxneGbgjdBXbuIm73gE1gMGNEI4WDUc83oGhfBLFZYUW658xVHvLTK49Ar8Em7x2KAXosZ0Bw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-10T01:10:40.172215Z","bundle_sha256":"75bba06629d292169ca8ee2cb7d5ff45073d0b47e44ed83f102eea750c4f7847"}}