{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:4QNS3VBDUR6ZFW5QLVIPW2O2YJ","short_pith_number":"pith:4QNS3VBD","canonical_record":{"source":{"id":"1201.0300","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2011-12-31T18:44:35Z","cross_cats_sorted":["cond-mat.mes-hall","math-ph","math.MP","physics.class-ph"],"title_canon_sha256":"fe42c5f8eb70c7ddbaf7fb336ad6c5e1c50b68f79c50c7352eb1a6b13cf3c69f","abstract_canon_sha256":"9d3cb6e5f928d8bcf33e7a252e4c6b069dd2ce08408701d4cd991ed34b8f33e1"},"schema_version":"1.0"},"canonical_sha256":"e41b2dd423a47d92dbb05d50fb69dac264328378cf379c559b76249e6bed9861","source":{"kind":"arxiv","id":"1201.0300","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1201.0300","created_at":"2026-05-18T03:57:00Z"},{"alias_kind":"arxiv_version","alias_value":"1201.0300v2","created_at":"2026-05-18T03:57:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.0300","created_at":"2026-05-18T03:57:00Z"},{"alias_kind":"pith_short_12","alias_value":"4QNS3VBDUR6Z","created_at":"2026-05-18T12:26:20Z"},{"alias_kind":"pith_short_16","alias_value":"4QNS3VBDUR6ZFW5Q","created_at":"2026-05-18T12:26:20Z"},{"alias_kind":"pith_short_8","alias_value":"4QNS3VBD","created_at":"2026-05-18T12:26:20Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:4QNS3VBDUR6ZFW5QLVIPW2O2YJ","target":"record","payload":{"canonical_record":{"source":{"id":"1201.0300","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2011-12-31T18:44:35Z","cross_cats_sorted":["cond-mat.mes-hall","math-ph","math.MP","physics.class-ph"],"title_canon_sha256":"fe42c5f8eb70c7ddbaf7fb336ad6c5e1c50b68f79c50c7352eb1a6b13cf3c69f","abstract_canon_sha256":"9d3cb6e5f928d8bcf33e7a252e4c6b069dd2ce08408701d4cd991ed34b8f33e1"},"schema_version":"1.0"},"canonical_sha256":"e41b2dd423a47d92dbb05d50fb69dac264328378cf379c559b76249e6bed9861","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:57:00.066886Z","signature_b64":"yk2NoPMtY6X2cU+bRNBO6J3JHDlPYioTtzM9m0viI5Zgx1v83elhFoMFrHG2afDRncTV467cc0bcy0YtAPBKCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e41b2dd423a47d92dbb05d50fb69dac264328378cf379c559b76249e6bed9861","last_reissued_at":"2026-05-18T03:57:00.065944Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:57:00.065944Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1201.0300","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":"2026-05-18T03:57:00Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qmJHcOtmZ0bk3XmCZRsy7HhXiK6XOY2Py3awSIDxoassBQ4xMjuio1Qx0U1hmmEMBkPyc1Mq9tMpzoSU5UVrAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T15:36:03.493417Z"},"content_sha256":"0c75fa77cfd8c043204ddfd78cbb7a072e2fd31a58b7395a055e098b7bfbd7d8","schema_version":"1.0","event_id":"sha256:0c75fa77cfd8c043204ddfd78cbb7a072e2fd31a58b7395a055e098b7bfbd7d8"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:4QNS3VBDUR6ZFW5QLVIPW2O2YJ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Non-Paraxial Accelerating Beams","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","math-ph","math.MP","physics.class-ph"],"primary_cat":"physics.optics","authors_text":"Ido Kaminer, Jonathan Nemirovsky, Mordechai Segev, Rivka Bekenstein","submitted_at":"2011-12-31T18:44:35Z","abstract_excerpt":"We present the spatially accelerating solutions of the Maxwell equations. Such non-paraxial beams accelerate in a circular trajectory, thus generalizing the concept of Airy beams. For both TE and TM polarizations, the beams exhibit shape-preserving bending with sub-wavelength features, and the Poynting vector of the main lobe displays a turn of more than 90 degrees. We show that these accelerating beams are self-healing, analyze their properties, and compare to the paraxial Airy beams. Finally, we present the new family of periodic accelerating beams which can be constructed from our solutions"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.0300","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":"2026-05-18T03:57:00Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9nAPbFWKbMg9ZUBcO69Pa+PyUYhIK2YwoWBK83G1DkXkFjidrYmttcv2ODOfZ8AN1fjKf+ZDC874KeIy5vwaDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T15:36:03.494457Z"},"content_sha256":"9d541d299ef0821de5a014785b38908a45b1f9fbeacca1d8b049a5b117f74b66","schema_version":"1.0","event_id":"sha256:9d541d299ef0821de5a014785b38908a45b1f9fbeacca1d8b049a5b117f74b66"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/4QNS3VBDUR6ZFW5QLVIPW2O2YJ/bundle.json","state_url":"https://pith.science/pith/4QNS3VBDUR6ZFW5QLVIPW2O2YJ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/4QNS3VBDUR6ZFW5QLVIPW2O2YJ/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":"2026-05-26T15:36:03Z","links":{"resolver":"https://pith.science/pith/4QNS3VBDUR6ZFW5QLVIPW2O2YJ","bundle":"https://pith.science/pith/4QNS3VBDUR6ZFW5QLVIPW2O2YJ/bundle.json","state":"https://pith.science/pith/4QNS3VBDUR6ZFW5QLVIPW2O2YJ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/4QNS3VBDUR6ZFW5QLVIPW2O2YJ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:4QNS3VBDUR6ZFW5QLVIPW2O2YJ","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":"9d3cb6e5f928d8bcf33e7a252e4c6b069dd2ce08408701d4cd991ed34b8f33e1","cross_cats_sorted":["cond-mat.mes-hall","math-ph","math.MP","physics.class-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2011-12-31T18:44:35Z","title_canon_sha256":"fe42c5f8eb70c7ddbaf7fb336ad6c5e1c50b68f79c50c7352eb1a6b13cf3c69f"},"schema_version":"1.0","source":{"id":"1201.0300","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1201.0300","created_at":"2026-05-18T03:57:00Z"},{"alias_kind":"arxiv_version","alias_value":"1201.0300v2","created_at":"2026-05-18T03:57:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.0300","created_at":"2026-05-18T03:57:00Z"},{"alias_kind":"pith_short_12","alias_value":"4QNS3VBDUR6Z","created_at":"2026-05-18T12:26:20Z"},{"alias_kind":"pith_short_16","alias_value":"4QNS3VBDUR6ZFW5Q","created_at":"2026-05-18T12:26:20Z"},{"alias_kind":"pith_short_8","alias_value":"4QNS3VBD","created_at":"2026-05-18T12:26:20Z"}],"graph_snapshots":[{"event_id":"sha256:9d541d299ef0821de5a014785b38908a45b1f9fbeacca1d8b049a5b117f74b66","target":"graph","created_at":"2026-05-18T03:57:00Z","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":"We present the spatially accelerating solutions of the Maxwell equations. Such non-paraxial beams accelerate in a circular trajectory, thus generalizing the concept of Airy beams. For both TE and TM polarizations, the beams exhibit shape-preserving bending with sub-wavelength features, and the Poynting vector of the main lobe displays a turn of more than 90 degrees. We show that these accelerating beams are self-healing, analyze their properties, and compare to the paraxial Airy beams. Finally, we present the new family of periodic accelerating beams which can be constructed from our solutions","authors_text":"Ido Kaminer, Jonathan Nemirovsky, Mordechai Segev, Rivka Bekenstein","cross_cats":["cond-mat.mes-hall","math-ph","math.MP","physics.class-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2011-12-31T18:44:35Z","title":"Non-Paraxial Accelerating Beams"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.0300","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":"sha256:0c75fa77cfd8c043204ddfd78cbb7a072e2fd31a58b7395a055e098b7bfbd7d8","target":"record","created_at":"2026-05-18T03:57:00Z","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":"9d3cb6e5f928d8bcf33e7a252e4c6b069dd2ce08408701d4cd991ed34b8f33e1","cross_cats_sorted":["cond-mat.mes-hall","math-ph","math.MP","physics.class-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2011-12-31T18:44:35Z","title_canon_sha256":"fe42c5f8eb70c7ddbaf7fb336ad6c5e1c50b68f79c50c7352eb1a6b13cf3c69f"},"schema_version":"1.0","source":{"id":"1201.0300","kind":"arxiv","version":2}},"canonical_sha256":"e41b2dd423a47d92dbb05d50fb69dac264328378cf379c559b76249e6bed9861","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e41b2dd423a47d92dbb05d50fb69dac264328378cf379c559b76249e6bed9861","first_computed_at":"2026-05-18T03:57:00.065944Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:57:00.065944Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"yk2NoPMtY6X2cU+bRNBO6J3JHDlPYioTtzM9m0viI5Zgx1v83elhFoMFrHG2afDRncTV467cc0bcy0YtAPBKCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T03:57:00.066886Z","signed_message":"canonical_sha256_bytes"},"source_id":"1201.0300","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0c75fa77cfd8c043204ddfd78cbb7a072e2fd31a58b7395a055e098b7bfbd7d8","sha256:9d541d299ef0821de5a014785b38908a45b1f9fbeacca1d8b049a5b117f74b66"],"state_sha256":"9193e725a34c4e24e2d9db1d5dbef868b4366bba68940a50b47a69d481299e7e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HWSO7XS40QczYPYoUdcyAK96bIV42LLqEXDz+SOJwehqwDMfPQq0UqoLhUrPqjxXwYjYfAxvfAvEkxeB8bEDAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T15:36:03.497405Z","bundle_sha256":"ad9c0a8ec02e86971319118046a053554b0eaa64817e3f5a1f123558a0fd544d"}}