{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:FCZZAWMB4IP4SCS6MHUMPOXQYL","short_pith_number":"pith:FCZZAWMB","canonical_record":{"source":{"id":"1605.09086","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-05-30T02:05:34Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"28e9bcb604a993cda910d0ffa89c8bdcb1277e08538d5b19207de4d55bd505c4","abstract_canon_sha256":"65648fe5a8e2c3e1a1bd1969505ea6ebc6c13921c976325b213d7f800522805b"},"schema_version":"1.0"},"canonical_sha256":"28b3905981e21fc90a5e61e8c7baf0c2efe9405618c3fbfd7d19982aeb7250e4","source":{"kind":"arxiv","id":"1605.09086","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1605.09086","created_at":"2026-05-18T01:13:22Z"},{"alias_kind":"arxiv_version","alias_value":"1605.09086v1","created_at":"2026-05-18T01:13:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1605.09086","created_at":"2026-05-18T01:13:22Z"},{"alias_kind":"pith_short_12","alias_value":"FCZZAWMB4IP4","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_16","alias_value":"FCZZAWMB4IP4SCS6","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_8","alias_value":"FCZZAWMB","created_at":"2026-05-18T12:30:15Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:FCZZAWMB4IP4SCS6MHUMPOXQYL","target":"record","payload":{"canonical_record":{"source":{"id":"1605.09086","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-05-30T02:05:34Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"28e9bcb604a993cda910d0ffa89c8bdcb1277e08538d5b19207de4d55bd505c4","abstract_canon_sha256":"65648fe5a8e2c3e1a1bd1969505ea6ebc6c13921c976325b213d7f800522805b"},"schema_version":"1.0"},"canonical_sha256":"28b3905981e21fc90a5e61e8c7baf0c2efe9405618c3fbfd7d19982aeb7250e4","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:13:22.142918Z","signature_b64":"Xrjv5TP1E4R69bWmVegqLKCuqQD2jK3GH0ArSev4VrJnm+8Bv8xaojvm9SPeCx5eSTBjfDoKoF2Kj1d/+hJGCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"28b3905981e21fc90a5e61e8c7baf0c2efe9405618c3fbfd7d19982aeb7250e4","last_reissued_at":"2026-05-18T01:13:22.142177Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:13:22.142177Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1605.09086","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":"2026-05-18T01:13:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6dJK8MnIwQszP0Q2TRy/x281RmaSBLb39yYPjIjFrUlMDOVfNC+uB1plajDcdnzhNuzmliRG44/Mtvhj1q/LBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-27T09:40:40.933482Z"},"content_sha256":"cca124c80153e6988b1ead1ced9ffb3ca4149ea2cb117efc0fd57cc2b5eb342c","schema_version":"1.0","event_id":"sha256:cca124c80153e6988b1ead1ced9ffb3ca4149ea2cb117efc0fd57cc2b5eb342c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:FCZZAWMB4IP4SCS6MHUMPOXQYL","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Analytical theory for the time-resolved dynamical Franz-Keldysh effect under circularly polarized light","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.optics"],"primary_cat":"cond-mat.mes-hall","authors_text":"T. Otobe","submitted_at":"2016-05-30T02:05:34Z","abstract_excerpt":"We report here the analytical formula for the time-resolved dynamical Franz-Keldysh effect (Tr-DFKE) under circularly polarized light. We assume the Houston function as the time-dependent wave function of the parabolic two-band system. Our formula shows that the sub-cycle change of the optical properties disappears, which is a significant feature of the Tr-DFKE under linear polarized light and is different from the static Franz-Keldysh effect."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1605.09086","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":"2026-05-18T01:13:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"skB48cq2+gXtxBOQ6PjCT+pW38o6GgPNHIDvudgP5Y8a/ps2ijy7Vsfyi9gYib8/wOCX6IUY/Q0aURhZGootBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-27T09:40:40.934004Z"},"content_sha256":"952df44b4937499cf543a0ab310c9c777fcd8fc6a070f88c75d12afc5ff67387","schema_version":"1.0","event_id":"sha256:952df44b4937499cf543a0ab310c9c777fcd8fc6a070f88c75d12afc5ff67387"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/FCZZAWMB4IP4SCS6MHUMPOXQYL/bundle.json","state_url":"https://pith.science/pith/FCZZAWMB4IP4SCS6MHUMPOXQYL/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/FCZZAWMB4IP4SCS6MHUMPOXQYL/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":"2026-06-27T09:40:40Z","links":{"resolver":"https://pith.science/pith/FCZZAWMB4IP4SCS6MHUMPOXQYL","bundle":"https://pith.science/pith/FCZZAWMB4IP4SCS6MHUMPOXQYL/bundle.json","state":"https://pith.science/pith/FCZZAWMB4IP4SCS6MHUMPOXQYL/state.json","well_known_bundle":"https://pith.science/.well-known/pith/FCZZAWMB4IP4SCS6MHUMPOXQYL/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:FCZZAWMB4IP4SCS6MHUMPOXQYL","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":"65648fe5a8e2c3e1a1bd1969505ea6ebc6c13921c976325b213d7f800522805b","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-05-30T02:05:34Z","title_canon_sha256":"28e9bcb604a993cda910d0ffa89c8bdcb1277e08538d5b19207de4d55bd505c4"},"schema_version":"1.0","source":{"id":"1605.09086","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1605.09086","created_at":"2026-05-18T01:13:22Z"},{"alias_kind":"arxiv_version","alias_value":"1605.09086v1","created_at":"2026-05-18T01:13:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1605.09086","created_at":"2026-05-18T01:13:22Z"},{"alias_kind":"pith_short_12","alias_value":"FCZZAWMB4IP4","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_16","alias_value":"FCZZAWMB4IP4SCS6","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_8","alias_value":"FCZZAWMB","created_at":"2026-05-18T12:30:15Z"}],"graph_snapshots":[{"event_id":"sha256:952df44b4937499cf543a0ab310c9c777fcd8fc6a070f88c75d12afc5ff67387","target":"graph","created_at":"2026-05-18T01:13:22Z","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 report here the analytical formula for the time-resolved dynamical Franz-Keldysh effect (Tr-DFKE) under circularly polarized light. We assume the Houston function as the time-dependent wave function of the parabolic two-band system. Our formula shows that the sub-cycle change of the optical properties disappears, which is a significant feature of the Tr-DFKE under linear polarized light and is different from the static Franz-Keldysh effect.","authors_text":"T. Otobe","cross_cats":["physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-05-30T02:05:34Z","title":"Analytical theory for the time-resolved dynamical Franz-Keldysh effect under circularly polarized light"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1605.09086","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:cca124c80153e6988b1ead1ced9ffb3ca4149ea2cb117efc0fd57cc2b5eb342c","target":"record","created_at":"2026-05-18T01:13:22Z","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":"65648fe5a8e2c3e1a1bd1969505ea6ebc6c13921c976325b213d7f800522805b","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-05-30T02:05:34Z","title_canon_sha256":"28e9bcb604a993cda910d0ffa89c8bdcb1277e08538d5b19207de4d55bd505c4"},"schema_version":"1.0","source":{"id":"1605.09086","kind":"arxiv","version":1}},"canonical_sha256":"28b3905981e21fc90a5e61e8c7baf0c2efe9405618c3fbfd7d19982aeb7250e4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"28b3905981e21fc90a5e61e8c7baf0c2efe9405618c3fbfd7d19982aeb7250e4","first_computed_at":"2026-05-18T01:13:22.142177Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:13:22.142177Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Xrjv5TP1E4R69bWmVegqLKCuqQD2jK3GH0ArSev4VrJnm+8Bv8xaojvm9SPeCx5eSTBjfDoKoF2Kj1d/+hJGCA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:13:22.142918Z","signed_message":"canonical_sha256_bytes"},"source_id":"1605.09086","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cca124c80153e6988b1ead1ced9ffb3ca4149ea2cb117efc0fd57cc2b5eb342c","sha256:952df44b4937499cf543a0ab310c9c777fcd8fc6a070f88c75d12afc5ff67387"],"state_sha256":"6fb786b5cb66f95c50afd921e8b1f7ed5bbcaa913f2d6bd80366ce164675a003"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zIKWw/xlrKUBt4NKEWIfZHDLrw6DsMWGw4qodv8dxearPGN0rwQHfm3Zt7llgrXH0wED5pIFJsCa2YP0eHqvCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-27T09:40:40.939343Z","bundle_sha256":"9ee3e43c2ce31ebb74e0dc34be11a85ab766e1cd58a873243086cc841b39fe74"}}