{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:FWTZK77G7EQSHKG5CPSS2CV6PQ","short_pith_number":"pith:FWTZK77G","canonical_record":{"source":{"id":"1609.07280","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-09-23T09:16:05Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"e8f7766b268c948ba79d11b41081c8e66a7f721eeb280397ce6e48168f9e1d6a","abstract_canon_sha256":"8b717d39c5a8a24791ed1e5d27ef59bdf25f8fac48bcae2716b531e6e1c63e54"},"schema_version":"1.0"},"canonical_sha256":"2da7957fe6f92123a8dd13e52d0abe7c22ae15b0bf45d9d48c48f7f4cf85de35","source":{"kind":"arxiv","id":"1609.07280","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1609.07280","created_at":"2026-05-18T00:57:10Z"},{"alias_kind":"arxiv_version","alias_value":"1609.07280v1","created_at":"2026-05-18T00:57:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1609.07280","created_at":"2026-05-18T00:57:10Z"},{"alias_kind":"pith_short_12","alias_value":"FWTZK77G7EQS","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_16","alias_value":"FWTZK77G7EQSHKG5","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_8","alias_value":"FWTZK77G","created_at":"2026-05-18T12:30:15Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:FWTZK77G7EQSHKG5CPSS2CV6PQ","target":"record","payload":{"canonical_record":{"source":{"id":"1609.07280","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-09-23T09:16:05Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"e8f7766b268c948ba79d11b41081c8e66a7f721eeb280397ce6e48168f9e1d6a","abstract_canon_sha256":"8b717d39c5a8a24791ed1e5d27ef59bdf25f8fac48bcae2716b531e6e1c63e54"},"schema_version":"1.0"},"canonical_sha256":"2da7957fe6f92123a8dd13e52d0abe7c22ae15b0bf45d9d48c48f7f4cf85de35","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:57:10.511376Z","signature_b64":"hCJkLZ1RPJyTjyIu2GqrpQuGtjV/B+nk8dvz+8GXEE0x1p/Ra6EAyGHyFU7bIJkQtjtkt32bwGW1xWIspz85AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2da7957fe6f92123a8dd13e52d0abe7c22ae15b0bf45d9d48c48f7f4cf85de35","last_reissued_at":"2026-05-18T00:57:10.510926Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:57:10.510926Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1609.07280","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":"2026-05-18T00:57:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yTsKdDH6Ev9mvA1LgBF51IJhqQgDcMVjvDs/ObRb0s/56oTl7LcM5wz8J8ycsVmXpNGlrkgNNoXOTwInJ7FCCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-27T06:53:04.588108Z"},"content_sha256":"9e46b9767ff31810b664c79790d860872dee093ecff73ab2b92b852fd5f8b548","schema_version":"1.0","event_id":"sha256:9e46b9767ff31810b664c79790d860872dee093ecff73ab2b92b852fd5f8b548"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:FWTZK77G7EQSHKG5CPSS2CV6PQ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Time-resolved dynamical Franz-Keldysh effect under elliptically polarized laser","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"physics.optics","authors_text":"T. Otobe","submitted_at":"2016-09-23T09:16:05Z","abstract_excerpt":"The analytical formula for the time-resolved dynamical Franz-Keldysh effect (Tr-DFKE) under an elliptically polarized laser in sub-femtosecond time-scale is reported. The Houston function is assumed as the time-dependent wave function of the parabolic two-band system. The resulting formula shows the sub-cycle change of the optical properties for elliptically polarization; the modulation of the dielectric function becomes smaller than that of linear polarization. On the other hand, the subcycle modulation of the dielectric function disappears for a circularly polarized laser, which is a signifi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1609.07280","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":"2026-05-18T00:57:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1XnfPNnHDC/vvHotcxBjiQq69UdfgD05N45SfL+SKF1jPYhpNqkgLUW1ebpbt/LSn4pAo67W/8FR6Cv1fuv2AA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-27T06:53:04.588457Z"},"content_sha256":"f0d6ea185bb2b57b008bf966ff0a2386cdfccf57a9f0a7f2ed95105dfe831adc","schema_version":"1.0","event_id":"sha256:f0d6ea185bb2b57b008bf966ff0a2386cdfccf57a9f0a7f2ed95105dfe831adc"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/FWTZK77G7EQSHKG5CPSS2CV6PQ/bundle.json","state_url":"https://pith.science/pith/FWTZK77G7EQSHKG5CPSS2CV6PQ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/FWTZK77G7EQSHKG5CPSS2CV6PQ/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":"2026-06-27T06:53:04Z","links":{"resolver":"https://pith.science/pith/FWTZK77G7EQSHKG5CPSS2CV6PQ","bundle":"https://pith.science/pith/FWTZK77G7EQSHKG5CPSS2CV6PQ/bundle.json","state":"https://pith.science/pith/FWTZK77G7EQSHKG5CPSS2CV6PQ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/FWTZK77G7EQSHKG5CPSS2CV6PQ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:FWTZK77G7EQSHKG5CPSS2CV6PQ","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":"8b717d39c5a8a24791ed1e5d27ef59bdf25f8fac48bcae2716b531e6e1c63e54","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-09-23T09:16:05Z","title_canon_sha256":"e8f7766b268c948ba79d11b41081c8e66a7f721eeb280397ce6e48168f9e1d6a"},"schema_version":"1.0","source":{"id":"1609.07280","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1609.07280","created_at":"2026-05-18T00:57:10Z"},{"alias_kind":"arxiv_version","alias_value":"1609.07280v1","created_at":"2026-05-18T00:57:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1609.07280","created_at":"2026-05-18T00:57:10Z"},{"alias_kind":"pith_short_12","alias_value":"FWTZK77G7EQS","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_16","alias_value":"FWTZK77G7EQSHKG5","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_8","alias_value":"FWTZK77G","created_at":"2026-05-18T12:30:15Z"}],"graph_snapshots":[{"event_id":"sha256:f0d6ea185bb2b57b008bf966ff0a2386cdfccf57a9f0a7f2ed95105dfe831adc","target":"graph","created_at":"2026-05-18T00:57:10Z","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":"The analytical formula for the time-resolved dynamical Franz-Keldysh effect (Tr-DFKE) under an elliptically polarized laser in sub-femtosecond time-scale is reported. The Houston function is assumed as the time-dependent wave function of the parabolic two-band system. The resulting formula shows the sub-cycle change of the optical properties for elliptically polarization; the modulation of the dielectric function becomes smaller than that of linear polarization. On the other hand, the subcycle modulation of the dielectric function disappears for a circularly polarized laser, which is a signifi","authors_text":"T. Otobe","cross_cats":["cond-mat.mes-hall"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-09-23T09:16:05Z","title":"Time-resolved dynamical Franz-Keldysh effect under elliptically polarized laser"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1609.07280","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":"sha256:9e46b9767ff31810b664c79790d860872dee093ecff73ab2b92b852fd5f8b548","target":"record","created_at":"2026-05-18T00:57:10Z","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":"8b717d39c5a8a24791ed1e5d27ef59bdf25f8fac48bcae2716b531e6e1c63e54","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-09-23T09:16:05Z","title_canon_sha256":"e8f7766b268c948ba79d11b41081c8e66a7f721eeb280397ce6e48168f9e1d6a"},"schema_version":"1.0","source":{"id":"1609.07280","kind":"arxiv","version":1}},"canonical_sha256":"2da7957fe6f92123a8dd13e52d0abe7c22ae15b0bf45d9d48c48f7f4cf85de35","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2da7957fe6f92123a8dd13e52d0abe7c22ae15b0bf45d9d48c48f7f4cf85de35","first_computed_at":"2026-05-18T00:57:10.510926Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:57:10.510926Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"hCJkLZ1RPJyTjyIu2GqrpQuGtjV/B+nk8dvz+8GXEE0x1p/Ra6EAyGHyFU7bIJkQtjtkt32bwGW1xWIspz85AA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:57:10.511376Z","signed_message":"canonical_sha256_bytes"},"source_id":"1609.07280","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:9e46b9767ff31810b664c79790d860872dee093ecff73ab2b92b852fd5f8b548","sha256:f0d6ea185bb2b57b008bf966ff0a2386cdfccf57a9f0a7f2ed95105dfe831adc"],"state_sha256":"9f6f5cb4b25ad1848c309233e9131d05bc7b7bee58de544824aefa23b15e6fbb"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HfwWltFIwuJ1YIixu6/wknf8iaxR0FdsX0fsJ9B+FzlagJsmcM311d6lmq37RZBh42IaDA+7p6qhsZEHbstDAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-27T06:53:04.590701Z","bundle_sha256":"5aa8bd7b0f685c65c1ec52d3ba0eb3063c56d03c6437ff570374cf8718603753"}}