{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:IATIXGMQTHD2XGB3DQ26BQRUNG","short_pith_number":"pith:IATIXGMQ","canonical_record":{"source":{"id":"1812.01376","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2018-12-04T12:38:30Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"843941433b1f79426be413a614705f6361e910245b81e1d53e9ef8af172ffa13","abstract_canon_sha256":"f31566d86ed24363378c26e2298d5ce0de2a72b62e5082b8c95c85a4eb890b0b"},"schema_version":"1.0"},"canonical_sha256":"40268b999099c7ab983b1c35e0c23469bd8aaf742e6d5eb7a34017637be20a09","source":{"kind":"arxiv","id":"1812.01376","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1812.01376","created_at":"2026-05-17T23:59:12Z"},{"alias_kind":"arxiv_version","alias_value":"1812.01376v1","created_at":"2026-05-17T23:59:12Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1812.01376","created_at":"2026-05-17T23:59:12Z"},{"alias_kind":"pith_short_12","alias_value":"IATIXGMQTHD2","created_at":"2026-05-18T12:32:28Z"},{"alias_kind":"pith_short_16","alias_value":"IATIXGMQTHD2XGB3","created_at":"2026-05-18T12:32:28Z"},{"alias_kind":"pith_short_8","alias_value":"IATIXGMQ","created_at":"2026-05-18T12:32:28Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:IATIXGMQTHD2XGB3DQ26BQRUNG","target":"record","payload":{"canonical_record":{"source":{"id":"1812.01376","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2018-12-04T12:38:30Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"843941433b1f79426be413a614705f6361e910245b81e1d53e9ef8af172ffa13","abstract_canon_sha256":"f31566d86ed24363378c26e2298d5ce0de2a72b62e5082b8c95c85a4eb890b0b"},"schema_version":"1.0"},"canonical_sha256":"40268b999099c7ab983b1c35e0c23469bd8aaf742e6d5eb7a34017637be20a09","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:59:12.636771Z","signature_b64":"DP8uM4locEp40VdlHnm0uZVfBSITxmPaKoqjewYm97m4cYSszoQJUb5FZxiDtXFBImaelc7AikDhGZ6t06ouDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"40268b999099c7ab983b1c35e0c23469bd8aaf742e6d5eb7a34017637be20a09","last_reissued_at":"2026-05-17T23:59:12.635636Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:59:12.635636Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1812.01376","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":"2026-05-17T23:59:12Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"n2vPIgDTJWXqNoee159lbwqvwxUYvE4QJgSalwz7R/jVdkP3GRUKy3x21oRSlYXdSwjWZWAXwPT/VvsvWd1tBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T17:42:24.858006Z"},"content_sha256":"8d6bdbcc33c4aa90dd33af17a2200fe633b9b4b5c60fcbe928986753dba34b6a","schema_version":"1.0","event_id":"sha256:8d6bdbcc33c4aa90dd33af17a2200fe633b9b4b5c60fcbe928986753dba34b6a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:IATIXGMQTHD2XGB3DQ26BQRUNG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Ultrafast tunable modulation of light polarization at terahertz frequencies","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.optics"],"primary_cat":"physics.app-ph","authors_text":"Gwena\\\"elle Vaudel, Janos Hebling, Thomas Pezeril, Vasily Temnov, Vincent Juv\\'e, Vitalyi Gusev, Zoltan Ollmann","submitted_at":"2018-12-04T12:38:30Z","abstract_excerpt":"Controlling light polarization is one of the most essential routines in modern optical technology. Since the demonstration of optical pulse shaping by spatial light modulators and its potential in controlling the quantum reaction pathways, it paved the way for many applications as a coherent control of the photoionization process or as polarization shaping of terahertz (THz) pulses. Here, we evidenced efficient nonresonant and noncollinear $\\chi^{(2)}$-type light-matter interaction in femtosecond polarization-sensitive time-resolved optical measurements. Such nonlinear optical interaction of v"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1812.01376","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":"2026-05-17T23:59:12Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dPasbVCk2BWDsBhcZjI5vCMCU1tDAIEMkqls7sSy3SOp1gCz8SbBHHnIF4kE3Z9Zkf9mxwFIAxBdc6/i66XuAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T17:42:24.858366Z"},"content_sha256":"a297c0c5a75d4859c4def5ca8e129ddc424cdd8b4101a14cd55ea9239b7a5092","schema_version":"1.0","event_id":"sha256:a297c0c5a75d4859c4def5ca8e129ddc424cdd8b4101a14cd55ea9239b7a5092"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/IATIXGMQTHD2XGB3DQ26BQRUNG/bundle.json","state_url":"https://pith.science/pith/IATIXGMQTHD2XGB3DQ26BQRUNG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/IATIXGMQTHD2XGB3DQ26BQRUNG/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":"2026-06-01T17:42:24Z","links":{"resolver":"https://pith.science/pith/IATIXGMQTHD2XGB3DQ26BQRUNG","bundle":"https://pith.science/pith/IATIXGMQTHD2XGB3DQ26BQRUNG/bundle.json","state":"https://pith.science/pith/IATIXGMQTHD2XGB3DQ26BQRUNG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/IATIXGMQTHD2XGB3DQ26BQRUNG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:IATIXGMQTHD2XGB3DQ26BQRUNG","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":"f31566d86ed24363378c26e2298d5ce0de2a72b62e5082b8c95c85a4eb890b0b","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2018-12-04T12:38:30Z","title_canon_sha256":"843941433b1f79426be413a614705f6361e910245b81e1d53e9ef8af172ffa13"},"schema_version":"1.0","source":{"id":"1812.01376","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1812.01376","created_at":"2026-05-17T23:59:12Z"},{"alias_kind":"arxiv_version","alias_value":"1812.01376v1","created_at":"2026-05-17T23:59:12Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1812.01376","created_at":"2026-05-17T23:59:12Z"},{"alias_kind":"pith_short_12","alias_value":"IATIXGMQTHD2","created_at":"2026-05-18T12:32:28Z"},{"alias_kind":"pith_short_16","alias_value":"IATIXGMQTHD2XGB3","created_at":"2026-05-18T12:32:28Z"},{"alias_kind":"pith_short_8","alias_value":"IATIXGMQ","created_at":"2026-05-18T12:32:28Z"}],"graph_snapshots":[{"event_id":"sha256:a297c0c5a75d4859c4def5ca8e129ddc424cdd8b4101a14cd55ea9239b7a5092","target":"graph","created_at":"2026-05-17T23:59:12Z","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":"Controlling light polarization is one of the most essential routines in modern optical technology. Since the demonstration of optical pulse shaping by spatial light modulators and its potential in controlling the quantum reaction pathways, it paved the way for many applications as a coherent control of the photoionization process or as polarization shaping of terahertz (THz) pulses. Here, we evidenced efficient nonresonant and noncollinear $\\chi^{(2)}$-type light-matter interaction in femtosecond polarization-sensitive time-resolved optical measurements. Such nonlinear optical interaction of v","authors_text":"Gwena\\\"elle Vaudel, Janos Hebling, Thomas Pezeril, Vasily Temnov, Vincent Juv\\'e, Vitalyi Gusev, Zoltan Ollmann","cross_cats":["physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2018-12-04T12:38:30Z","title":"Ultrafast tunable modulation of light polarization at terahertz frequencies"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1812.01376","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":"sha256:8d6bdbcc33c4aa90dd33af17a2200fe633b9b4b5c60fcbe928986753dba34b6a","target":"record","created_at":"2026-05-17T23:59:12Z","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":"f31566d86ed24363378c26e2298d5ce0de2a72b62e5082b8c95c85a4eb890b0b","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2018-12-04T12:38:30Z","title_canon_sha256":"843941433b1f79426be413a614705f6361e910245b81e1d53e9ef8af172ffa13"},"schema_version":"1.0","source":{"id":"1812.01376","kind":"arxiv","version":1}},"canonical_sha256":"40268b999099c7ab983b1c35e0c23469bd8aaf742e6d5eb7a34017637be20a09","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"40268b999099c7ab983b1c35e0c23469bd8aaf742e6d5eb7a34017637be20a09","first_computed_at":"2026-05-17T23:59:12.635636Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:59:12.635636Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"DP8uM4locEp40VdlHnm0uZVfBSITxmPaKoqjewYm97m4cYSszoQJUb5FZxiDtXFBImaelc7AikDhGZ6t06ouDw==","signature_status":"signed_v1","signed_at":"2026-05-17T23:59:12.636771Z","signed_message":"canonical_sha256_bytes"},"source_id":"1812.01376","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8d6bdbcc33c4aa90dd33af17a2200fe633b9b4b5c60fcbe928986753dba34b6a","sha256:a297c0c5a75d4859c4def5ca8e129ddc424cdd8b4101a14cd55ea9239b7a5092"],"state_sha256":"64f1639bdee710d0087cfd5f088cbe8f68702ee129e76f42d7af8af1133b6de6"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"OsS/rZeT0u8c+InDUy/r5Z9OjBH3c7gcEqNxaZ5TnGnyymUgPtBvhIPWjxQ4/c8zlOV9uZv5Cce/ljlIYXEoCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T17:42:24.860263Z","bundle_sha256":"c50f3d180373773f7608002de1e590d43bc800c3fc3d1316b64020e8dca7dc2a"}}