{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:OY6WXNPYES6AFAUUPGE5HNI5VQ","short_pith_number":"pith:OY6WXNPY","canonical_record":{"source":{"id":"1407.6538","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2014-07-24T11:50:57Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"352720b3f4ae26a4088da9a689f4956e7c9a0b8aacb73f27c593d5c5add4aa2d","abstract_canon_sha256":"0b0ee98bcfba1e321df359d674c90154cf93a558ae324f61f727d7ed496788aa"},"schema_version":"1.0"},"canonical_sha256":"763d6bb5f824bc0282947989d3b51dac124b3aad02d0818a4148e1ea95ebd5fd","source":{"kind":"arxiv","id":"1407.6538","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1407.6538","created_at":"2026-05-18T02:46:38Z"},{"alias_kind":"arxiv_version","alias_value":"1407.6538v1","created_at":"2026-05-18T02:46:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.6538","created_at":"2026-05-18T02:46:38Z"},{"alias_kind":"pith_short_12","alias_value":"OY6WXNPYES6A","created_at":"2026-05-18T12:28:43Z"},{"alias_kind":"pith_short_16","alias_value":"OY6WXNPYES6AFAUU","created_at":"2026-05-18T12:28:43Z"},{"alias_kind":"pith_short_8","alias_value":"OY6WXNPY","created_at":"2026-05-18T12:28:43Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:OY6WXNPYES6AFAUUPGE5HNI5VQ","target":"record","payload":{"canonical_record":{"source":{"id":"1407.6538","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2014-07-24T11:50:57Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"352720b3f4ae26a4088da9a689f4956e7c9a0b8aacb73f27c593d5c5add4aa2d","abstract_canon_sha256":"0b0ee98bcfba1e321df359d674c90154cf93a558ae324f61f727d7ed496788aa"},"schema_version":"1.0"},"canonical_sha256":"763d6bb5f824bc0282947989d3b51dac124b3aad02d0818a4148e1ea95ebd5fd","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:46:38.521035Z","signature_b64":"hWZmOgwWRqUrvrsrBydfazvad3DCp5ZpRzsC/vqiEAfA0NO+E4/H6vlH+YGYnVCYyuW5FWVqLNYiGYyUElRFAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"763d6bb5f824bc0282947989d3b51dac124b3aad02d0818a4148e1ea95ebd5fd","last_reissued_at":"2026-05-18T02:46:38.520676Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:46:38.520676Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1407.6538","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":"2026-05-18T02:46:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fvTSG+6Z2f1IgDeKX9h8irZZOizCbHly10ig8hwvrAw+lxN2OoUVUq3VZYVhp3U28ylFy/GHgyid7eYoKwFjDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T00:35:05.743148Z"},"content_sha256":"1402e87d34a2a6790a2ebe5c342eef459989f41f87e24cd0febd1bcce6888cb1","schema_version":"1.0","event_id":"sha256:1402e87d34a2a6790a2ebe5c342eef459989f41f87e24cd0febd1bcce6888cb1"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:OY6WXNPYES6AFAUUPGE5HNI5VQ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Optimized multifrequency light collection by adaptive self-ordering of scatterers in optical resonators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.optics"],"primary_cat":"quant-ph","authors_text":"Helmut Ritsch, Valentin Torggler","submitted_at":"2014-07-24T11:50:57Z","abstract_excerpt":"Mobile light scatterers in a high-Q optical cavity transversely illuminated by laser light close to a cavity resonance form ordered patterns, which maximize light scattering into the cavity and induce optical self-trapping. We show that a generalized form of such crystallization dynamics appears in multicolored pump fields with several cavity modes. Here the particles arrange in spatial patterns maximizing total light collection into the resonator. For changing input frequencies and strengths the particles dynamically adapt to the current illumination. Interestingly the system keeps some memor"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.6538","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":"2026-05-18T02:46:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Mh6HAJMRMTc16bAzqSV64mPx3kU+vZTzhgzoMNj3bMMfRsmhFBHJ7RSET2MBvlWMbSXiAzO4oAwOt7JBSq5SBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T00:35:05.744154Z"},"content_sha256":"ad2d58dc936cac0b629615803b9ab3dc6bfc152cab1cc3d24af9792c60fff988","schema_version":"1.0","event_id":"sha256:ad2d58dc936cac0b629615803b9ab3dc6bfc152cab1cc3d24af9792c60fff988"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/OY6WXNPYES6AFAUUPGE5HNI5VQ/bundle.json","state_url":"https://pith.science/pith/OY6WXNPYES6AFAUUPGE5HNI5VQ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/OY6WXNPYES6AFAUUPGE5HNI5VQ/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":"2026-05-31T00:35:05Z","links":{"resolver":"https://pith.science/pith/OY6WXNPYES6AFAUUPGE5HNI5VQ","bundle":"https://pith.science/pith/OY6WXNPYES6AFAUUPGE5HNI5VQ/bundle.json","state":"https://pith.science/pith/OY6WXNPYES6AFAUUPGE5HNI5VQ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/OY6WXNPYES6AFAUUPGE5HNI5VQ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:OY6WXNPYES6AFAUUPGE5HNI5VQ","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":"0b0ee98bcfba1e321df359d674c90154cf93a558ae324f61f727d7ed496788aa","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2014-07-24T11:50:57Z","title_canon_sha256":"352720b3f4ae26a4088da9a689f4956e7c9a0b8aacb73f27c593d5c5add4aa2d"},"schema_version":"1.0","source":{"id":"1407.6538","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1407.6538","created_at":"2026-05-18T02:46:38Z"},{"alias_kind":"arxiv_version","alias_value":"1407.6538v1","created_at":"2026-05-18T02:46:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.6538","created_at":"2026-05-18T02:46:38Z"},{"alias_kind":"pith_short_12","alias_value":"OY6WXNPYES6A","created_at":"2026-05-18T12:28:43Z"},{"alias_kind":"pith_short_16","alias_value":"OY6WXNPYES6AFAUU","created_at":"2026-05-18T12:28:43Z"},{"alias_kind":"pith_short_8","alias_value":"OY6WXNPY","created_at":"2026-05-18T12:28:43Z"}],"graph_snapshots":[{"event_id":"sha256:ad2d58dc936cac0b629615803b9ab3dc6bfc152cab1cc3d24af9792c60fff988","target":"graph","created_at":"2026-05-18T02:46:38Z","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":"Mobile light scatterers in a high-Q optical cavity transversely illuminated by laser light close to a cavity resonance form ordered patterns, which maximize light scattering into the cavity and induce optical self-trapping. We show that a generalized form of such crystallization dynamics appears in multicolored pump fields with several cavity modes. Here the particles arrange in spatial patterns maximizing total light collection into the resonator. For changing input frequencies and strengths the particles dynamically adapt to the current illumination. Interestingly the system keeps some memor","authors_text":"Helmut Ritsch, Valentin Torggler","cross_cats":["physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2014-07-24T11:50:57Z","title":"Optimized multifrequency light collection by adaptive self-ordering of scatterers in optical resonators"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.6538","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":"sha256:1402e87d34a2a6790a2ebe5c342eef459989f41f87e24cd0febd1bcce6888cb1","target":"record","created_at":"2026-05-18T02:46:38Z","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":"0b0ee98bcfba1e321df359d674c90154cf93a558ae324f61f727d7ed496788aa","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2014-07-24T11:50:57Z","title_canon_sha256":"352720b3f4ae26a4088da9a689f4956e7c9a0b8aacb73f27c593d5c5add4aa2d"},"schema_version":"1.0","source":{"id":"1407.6538","kind":"arxiv","version":1}},"canonical_sha256":"763d6bb5f824bc0282947989d3b51dac124b3aad02d0818a4148e1ea95ebd5fd","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"763d6bb5f824bc0282947989d3b51dac124b3aad02d0818a4148e1ea95ebd5fd","first_computed_at":"2026-05-18T02:46:38.520676Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:46:38.520676Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"hWZmOgwWRqUrvrsrBydfazvad3DCp5ZpRzsC/vqiEAfA0NO+E4/H6vlH+YGYnVCYyuW5FWVqLNYiGYyUElRFAg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:46:38.521035Z","signed_message":"canonical_sha256_bytes"},"source_id":"1407.6538","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1402e87d34a2a6790a2ebe5c342eef459989f41f87e24cd0febd1bcce6888cb1","sha256:ad2d58dc936cac0b629615803b9ab3dc6bfc152cab1cc3d24af9792c60fff988"],"state_sha256":"1047a4d050e1757dea71ca5b7f4464376c9114c067e32abfcb6370972b5337a0"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"E2c3sGkJFWf83jLpkBmeSx11xmeuFtC29W9yV88hp5hf/ctjVILucloQDq9/IfePjx64zlcT+PoczFus0zLMCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T00:35:05.749021Z","bundle_sha256":"82d5d50c7f26a6e03c84ceb81656b65de897da5110934ccf81f1f4754ead5fce"}}