{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:QBMZWCJPLHRVN6UMFIBN526ENW","short_pith_number":"pith:QBMZWCJP","canonical_record":{"source":{"id":"1509.04994","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2015-09-16T18:37:33Z","cross_cats_sorted":[],"title_canon_sha256":"f172d741f96e428a0865ebcfad11931e5d15274769f8e1daacacefffa9d1a254","abstract_canon_sha256":"f82bade2fd1abdfa5ab6cd5cdd07dfb8876bb25f479744192c5b34a5af25dd1a"},"schema_version":"1.0"},"canonical_sha256":"80599b092f59e356fa8c2a02deebc46d98eddc9928790a345ef4070a20466580","source":{"kind":"arxiv","id":"1509.04994","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1509.04994","created_at":"2026-05-18T01:14:25Z"},{"alias_kind":"arxiv_version","alias_value":"1509.04994v2","created_at":"2026-05-18T01:14:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1509.04994","created_at":"2026-05-18T01:14:25Z"},{"alias_kind":"pith_short_12","alias_value":"QBMZWCJPLHRV","created_at":"2026-05-18T12:29:37Z"},{"alias_kind":"pith_short_16","alias_value":"QBMZWCJPLHRVN6UM","created_at":"2026-05-18T12:29:37Z"},{"alias_kind":"pith_short_8","alias_value":"QBMZWCJP","created_at":"2026-05-18T12:29:37Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:QBMZWCJPLHRVN6UMFIBN526ENW","target":"record","payload":{"canonical_record":{"source":{"id":"1509.04994","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2015-09-16T18:37:33Z","cross_cats_sorted":[],"title_canon_sha256":"f172d741f96e428a0865ebcfad11931e5d15274769f8e1daacacefffa9d1a254","abstract_canon_sha256":"f82bade2fd1abdfa5ab6cd5cdd07dfb8876bb25f479744192c5b34a5af25dd1a"},"schema_version":"1.0"},"canonical_sha256":"80599b092f59e356fa8c2a02deebc46d98eddc9928790a345ef4070a20466580","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:14:25.884547Z","signature_b64":"PKzSMf3n+XMKyYiHfehORavE1AfUKlEFfiLcvzMxcl2ET3mkYeoWFGrXoD0Icdv5QwiqjpT75zChLOFO5X2ECA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"80599b092f59e356fa8c2a02deebc46d98eddc9928790a345ef4070a20466580","last_reissued_at":"2026-05-18T01:14:25.883660Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:14:25.883660Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1509.04994","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":"2026-05-18T01:14:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"NRORNPiQPwJAS4GPx+qyClv+DSKefy/ZZiPTzr0PeKdng2zSNn/MkD1n9BtcsAuu602M01r1T0ahYtAt8f6KBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-30T19:24:08.889550Z"},"content_sha256":"eeec18bc53bed7593163401ea333e1b8ea1f0f2869a91e016721abe773e79a79","schema_version":"1.0","event_id":"sha256:eeec18bc53bed7593163401ea333e1b8ea1f0f2869a91e016721abe773e79a79"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:QBMZWCJPLHRVN6UMFIBN526ENW","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Inverted Gabor holography principle for tailoring arbitrary shaped three-dimensional beams","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"Hans-Werner Fink, Tatiana Latychevskaia","submitted_at":"2015-09-16T18:37:33Z","abstract_excerpt":"It is well known that by modifying the wavefront in a certain manner, the light intensity can be turned into a certain shape. However, all known light modulation techniques allow for limited light modifications only: focusing within a restricted region in space, shaping into a certain class of parametric curves along the optical axis or bending described by a quadratic-dependent deflection as in the case of Airy beams. We show a general case of classical light wavefront shaping that allows for intensity and phase redistribution into an arbitrary profile including pre-determined switching-off o"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1509.04994","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":"2026-05-18T01:14:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"FF44hVSQNokn2jOksnF3TyYQj7+soyf5mvTOf6tXE1A36blWG5avtR7mZanvVq2b2t600nI9xYg6xHO+FhJ1CA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-30T19:24:08.889893Z"},"content_sha256":"36b225dbc25afc2292892514a82d62318bc8864aaf13cfe347dcb58504cf1f8e","schema_version":"1.0","event_id":"sha256:36b225dbc25afc2292892514a82d62318bc8864aaf13cfe347dcb58504cf1f8e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/QBMZWCJPLHRVN6UMFIBN526ENW/bundle.json","state_url":"https://pith.science/pith/QBMZWCJPLHRVN6UMFIBN526ENW/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/QBMZWCJPLHRVN6UMFIBN526ENW/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":"2026-06-30T19:24:08Z","links":{"resolver":"https://pith.science/pith/QBMZWCJPLHRVN6UMFIBN526ENW","bundle":"https://pith.science/pith/QBMZWCJPLHRVN6UMFIBN526ENW/bundle.json","state":"https://pith.science/pith/QBMZWCJPLHRVN6UMFIBN526ENW/state.json","well_known_bundle":"https://pith.science/.well-known/pith/QBMZWCJPLHRVN6UMFIBN526ENW/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:QBMZWCJPLHRVN6UMFIBN526ENW","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":"f82bade2fd1abdfa5ab6cd5cdd07dfb8876bb25f479744192c5b34a5af25dd1a","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2015-09-16T18:37:33Z","title_canon_sha256":"f172d741f96e428a0865ebcfad11931e5d15274769f8e1daacacefffa9d1a254"},"schema_version":"1.0","source":{"id":"1509.04994","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1509.04994","created_at":"2026-05-18T01:14:25Z"},{"alias_kind":"arxiv_version","alias_value":"1509.04994v2","created_at":"2026-05-18T01:14:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1509.04994","created_at":"2026-05-18T01:14:25Z"},{"alias_kind":"pith_short_12","alias_value":"QBMZWCJPLHRV","created_at":"2026-05-18T12:29:37Z"},{"alias_kind":"pith_short_16","alias_value":"QBMZWCJPLHRVN6UM","created_at":"2026-05-18T12:29:37Z"},{"alias_kind":"pith_short_8","alias_value":"QBMZWCJP","created_at":"2026-05-18T12:29:37Z"}],"graph_snapshots":[{"event_id":"sha256:36b225dbc25afc2292892514a82d62318bc8864aaf13cfe347dcb58504cf1f8e","target":"graph","created_at":"2026-05-18T01:14:25Z","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":"It is well known that by modifying the wavefront in a certain manner, the light intensity can be turned into a certain shape. However, all known light modulation techniques allow for limited light modifications only: focusing within a restricted region in space, shaping into a certain class of parametric curves along the optical axis or bending described by a quadratic-dependent deflection as in the case of Airy beams. We show a general case of classical light wavefront shaping that allows for intensity and phase redistribution into an arbitrary profile including pre-determined switching-off o","authors_text":"Hans-Werner Fink, Tatiana Latychevskaia","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2015-09-16T18:37:33Z","title":"Inverted Gabor holography principle for tailoring arbitrary shaped three-dimensional beams"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1509.04994","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:eeec18bc53bed7593163401ea333e1b8ea1f0f2869a91e016721abe773e79a79","target":"record","created_at":"2026-05-18T01:14:25Z","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":"f82bade2fd1abdfa5ab6cd5cdd07dfb8876bb25f479744192c5b34a5af25dd1a","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2015-09-16T18:37:33Z","title_canon_sha256":"f172d741f96e428a0865ebcfad11931e5d15274769f8e1daacacefffa9d1a254"},"schema_version":"1.0","source":{"id":"1509.04994","kind":"arxiv","version":2}},"canonical_sha256":"80599b092f59e356fa8c2a02deebc46d98eddc9928790a345ef4070a20466580","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"80599b092f59e356fa8c2a02deebc46d98eddc9928790a345ef4070a20466580","first_computed_at":"2026-05-18T01:14:25.883660Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:14:25.883660Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"PKzSMf3n+XMKyYiHfehORavE1AfUKlEFfiLcvzMxcl2ET3mkYeoWFGrXoD0Icdv5QwiqjpT75zChLOFO5X2ECA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:14:25.884547Z","signed_message":"canonical_sha256_bytes"},"source_id":"1509.04994","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:eeec18bc53bed7593163401ea333e1b8ea1f0f2869a91e016721abe773e79a79","sha256:36b225dbc25afc2292892514a82d62318bc8864aaf13cfe347dcb58504cf1f8e"],"state_sha256":"8d62911ac769a8d1692eb0cc808e6c32c7fadb85255b210b4990195d03db0083"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"myvIOL2tn1UMGtVOiCtMKGX3ZognQXoc2YWtBjE2bIJ3Zqa0tqiQs4Jw6J0lHAvcRWBCy1LHc3Q+IKPjfhZbDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-30T19:24:08.891795Z","bundle_sha256":"24ad17647acea58bff5b44ec71ddabfa394ab84b5dbe1dcf4d66bd6838c912cc"}}