{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:74JXZPIQADJBRAXQYGNLQRSRDH","short_pith_number":"pith:74JXZPIQ","canonical_record":{"source":{"id":"1310.6246","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2013-10-23T15:00:47Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"6d9a9e7c35bca49d816b8eeab020f77c9f61a5c6d0547a5383e7d8bb9e8d0539","abstract_canon_sha256":"94d8f4978be79f092341c9af247d657f9c20f0368d257ece50d73e9c3881980b"},"schema_version":"1.0"},"canonical_sha256":"ff137cbd1000d21882f0c19ab8465119f29c9bb0cf6afad302f2964beddc6a70","source":{"kind":"arxiv","id":"1310.6246","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1310.6246","created_at":"2026-05-18T01:46:50Z"},{"alias_kind":"arxiv_version","alias_value":"1310.6246v3","created_at":"2026-05-18T01:46:50Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1310.6246","created_at":"2026-05-18T01:46:50Z"},{"alias_kind":"pith_short_12","alias_value":"74JXZPIQADJB","created_at":"2026-05-18T12:27:36Z"},{"alias_kind":"pith_short_16","alias_value":"74JXZPIQADJBRAXQ","created_at":"2026-05-18T12:27:36Z"},{"alias_kind":"pith_short_8","alias_value":"74JXZPIQ","created_at":"2026-05-18T12:27:36Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:74JXZPIQADJBRAXQYGNLQRSRDH","target":"record","payload":{"canonical_record":{"source":{"id":"1310.6246","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2013-10-23T15:00:47Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"6d9a9e7c35bca49d816b8eeab020f77c9f61a5c6d0547a5383e7d8bb9e8d0539","abstract_canon_sha256":"94d8f4978be79f092341c9af247d657f9c20f0368d257ece50d73e9c3881980b"},"schema_version":"1.0"},"canonical_sha256":"ff137cbd1000d21882f0c19ab8465119f29c9bb0cf6afad302f2964beddc6a70","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:46:50.701626Z","signature_b64":"Nopp0qRZaQTAe5ZST7zf/pO60dFcFQZTReaEW/N+BGeTSxIW7sE7gi7ZObdkVhE4y2WQIea/nGhk/B3cp8HzCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ff137cbd1000d21882f0c19ab8465119f29c9bb0cf6afad302f2964beddc6a70","last_reissued_at":"2026-05-18T01:46:50.701141Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:46:50.701141Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1310.6246","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:46:50Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"SMMApoowPdahgyAe1RZDENpYAoc6GL5TWtE8JPWQN5rBGLQE6pvAN/Nw0cS6BDIB1SW22IzWkioCHpfJ66uyCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T11:15:33.128890Z"},"content_sha256":"451e591f7ffe0579e0fd2b632e4db58a5552c99b41c2329af2db2b0148cc9379","schema_version":"1.0","event_id":"sha256:451e591f7ffe0579e0fd2b632e4db58a5552c99b41c2329af2db2b0148cc9379"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:74JXZPIQADJBRAXQYGNLQRSRDH","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Scattering approach to two-colour light forces and self-ordering of polarizable particles","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.optics"],"primary_cat":"quant-ph","authors_text":"Helmut Ritsch, Matthias Sonnleitner, Stefan Ostermann","submitted_at":"2013-10-23T15:00:47Z","abstract_excerpt":"Collective coherent scattering of laser light by an ensemble of polarizable point particles creates long range interactions, whose properties can be tailored by choice of injected laser powers, frequencies and polarizations. We use a transfer matrix approach to study the forces induced by non-interfering fields of orthogonal polarization or different frequencies in a 1D geometry and find long range self-ordering of particles without a prescribed order. Adjusting laser frequencies and powers allows to tune inter-particle distances and provides a wide range of possible dynamical couplings not ac"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.6246","kind":"arxiv","version":3},"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":"2026-05-18T01:46:50Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"uKenj8KVJlGUyhnVTjirnU7TESjPl9DwfhBdPKP4w8jWp1Ldtd3sbl2p+39Iied85w1htvV9i73Inz79rzYZBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T11:15:33.129644Z"},"content_sha256":"00e175d63e68a85e595f224bb9c70dd73cdb2f9bb106d0f9d4fcc18b74e3447d","schema_version":"1.0","event_id":"sha256:00e175d63e68a85e595f224bb9c70dd73cdb2f9bb106d0f9d4fcc18b74e3447d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/74JXZPIQADJBRAXQYGNLQRSRDH/bundle.json","state_url":"https://pith.science/pith/74JXZPIQADJBRAXQYGNLQRSRDH/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/74JXZPIQADJBRAXQYGNLQRSRDH/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":"2026-05-30T11:15:33Z","links":{"resolver":"https://pith.science/pith/74JXZPIQADJBRAXQYGNLQRSRDH","bundle":"https://pith.science/pith/74JXZPIQADJBRAXQYGNLQRSRDH/bundle.json","state":"https://pith.science/pith/74JXZPIQADJBRAXQYGNLQRSRDH/state.json","well_known_bundle":"https://pith.science/.well-known/pith/74JXZPIQADJBRAXQYGNLQRSRDH/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:74JXZPIQADJBRAXQYGNLQRSRDH","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":"94d8f4978be79f092341c9af247d657f9c20f0368d257ece50d73e9c3881980b","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2013-10-23T15:00:47Z","title_canon_sha256":"6d9a9e7c35bca49d816b8eeab020f77c9f61a5c6d0547a5383e7d8bb9e8d0539"},"schema_version":"1.0","source":{"id":"1310.6246","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1310.6246","created_at":"2026-05-18T01:46:50Z"},{"alias_kind":"arxiv_version","alias_value":"1310.6246v3","created_at":"2026-05-18T01:46:50Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1310.6246","created_at":"2026-05-18T01:46:50Z"},{"alias_kind":"pith_short_12","alias_value":"74JXZPIQADJB","created_at":"2026-05-18T12:27:36Z"},{"alias_kind":"pith_short_16","alias_value":"74JXZPIQADJBRAXQ","created_at":"2026-05-18T12:27:36Z"},{"alias_kind":"pith_short_8","alias_value":"74JXZPIQ","created_at":"2026-05-18T12:27:36Z"}],"graph_snapshots":[{"event_id":"sha256:00e175d63e68a85e595f224bb9c70dd73cdb2f9bb106d0f9d4fcc18b74e3447d","target":"graph","created_at":"2026-05-18T01:46:50Z","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":"Collective coherent scattering of laser light by an ensemble of polarizable point particles creates long range interactions, whose properties can be tailored by choice of injected laser powers, frequencies and polarizations. We use a transfer matrix approach to study the forces induced by non-interfering fields of orthogonal polarization or different frequencies in a 1D geometry and find long range self-ordering of particles without a prescribed order. Adjusting laser frequencies and powers allows to tune inter-particle distances and provides a wide range of possible dynamical couplings not ac","authors_text":"Helmut Ritsch, Matthias Sonnleitner, Stefan Ostermann","cross_cats":["physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2013-10-23T15:00:47Z","title":"Scattering approach to two-colour light forces and self-ordering of polarizable particles"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.6246","kind":"arxiv","version":3},"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":"sha256:451e591f7ffe0579e0fd2b632e4db58a5552c99b41c2329af2db2b0148cc9379","target":"record","created_at":"2026-05-18T01:46:50Z","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":"94d8f4978be79f092341c9af247d657f9c20f0368d257ece50d73e9c3881980b","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2013-10-23T15:00:47Z","title_canon_sha256":"6d9a9e7c35bca49d816b8eeab020f77c9f61a5c6d0547a5383e7d8bb9e8d0539"},"schema_version":"1.0","source":{"id":"1310.6246","kind":"arxiv","version":3}},"canonical_sha256":"ff137cbd1000d21882f0c19ab8465119f29c9bb0cf6afad302f2964beddc6a70","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ff137cbd1000d21882f0c19ab8465119f29c9bb0cf6afad302f2964beddc6a70","first_computed_at":"2026-05-18T01:46:50.701141Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:46:50.701141Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Nopp0qRZaQTAe5ZST7zf/pO60dFcFQZTReaEW/N+BGeTSxIW7sE7gi7ZObdkVhE4y2WQIea/nGhk/B3cp8HzCw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:46:50.701626Z","signed_message":"canonical_sha256_bytes"},"source_id":"1310.6246","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:451e591f7ffe0579e0fd2b632e4db58a5552c99b41c2329af2db2b0148cc9379","sha256:00e175d63e68a85e595f224bb9c70dd73cdb2f9bb106d0f9d4fcc18b74e3447d"],"state_sha256":"b65208657a52e073776bc6318b2d8788397c2947e468faed74b9f3dd93bc89f0"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qsgIhX97+vaVTuF5pRyT3Va1z5RXr5TIbT+f0LdkzHnjANVEL2imrgnv6vcZqMuflVwggmP/pY22ANBzbY5zCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T11:15:33.132919Z","bundle_sha256":"05b794d536b36bb9a89d5b67a4a929ad0a72548fdbede921446737655b9b476f"}}