{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:IIL4CBGCPULNSTCF2XFIUL4FL2","short_pith_number":"pith:IIL4CBGC","canonical_record":{"source":{"id":"1609.02821","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-09-09T14:59:30Z","cross_cats_sorted":["physics.optics","quant-ph"],"title_canon_sha256":"0aaa2d3f21e74d130cb99257cd4e778160176e6f4660bd4c33ef7a175d3365ec","abstract_canon_sha256":"973a564d2d308293074ae2dfa5eb116d256d57fbbf57e4388c217e792237e975"},"schema_version":"1.0"},"canonical_sha256":"4217c104c27d16d94c45d5ca8a2f855ebf33a442232eee0cd2806f4f53d65110","source":{"kind":"arxiv","id":"1609.02821","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1609.02821","created_at":"2026-05-18T00:58:50Z"},{"alias_kind":"arxiv_version","alias_value":"1609.02821v2","created_at":"2026-05-18T00:58:50Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1609.02821","created_at":"2026-05-18T00:58:50Z"},{"alias_kind":"pith_short_12","alias_value":"IIL4CBGCPULN","created_at":"2026-05-18T12:30:22Z"},{"alias_kind":"pith_short_16","alias_value":"IIL4CBGCPULNSTCF","created_at":"2026-05-18T12:30:22Z"},{"alias_kind":"pith_short_8","alias_value":"IIL4CBGC","created_at":"2026-05-18T12:30:22Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:IIL4CBGCPULNSTCF2XFIUL4FL2","target":"record","payload":{"canonical_record":{"source":{"id":"1609.02821","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-09-09T14:59:30Z","cross_cats_sorted":["physics.optics","quant-ph"],"title_canon_sha256":"0aaa2d3f21e74d130cb99257cd4e778160176e6f4660bd4c33ef7a175d3365ec","abstract_canon_sha256":"973a564d2d308293074ae2dfa5eb116d256d57fbbf57e4388c217e792237e975"},"schema_version":"1.0"},"canonical_sha256":"4217c104c27d16d94c45d5ca8a2f855ebf33a442232eee0cd2806f4f53d65110","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:58:50.775659Z","signature_b64":"B3KmUccOeDmEPRJSDFFnD0e8FPTlQubRyr1DXV9vcmEaep71lW+LcD0pEpvU0XcuqX8ZfB32KgeLrGAyx106CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4217c104c27d16d94c45d5ca8a2f855ebf33a442232eee0cd2806f4f53d65110","last_reissued_at":"2026-05-18T00:58:50.775089Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:58:50.775089Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1609.02821","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":"2026-05-18T00:58:50Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"SPLfxw25G5pfdY5cX3u7dIDGhcl/5wYvqBHdDp81fkGhXGDhxcpKZh0ksU9SiPgy0vw3S5G04nc3DJlaw/UCAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T13:39:38.568360Z"},"content_sha256":"959b6036cd1eee909a265f1e5fef58b04e0be12910dabd5b4eb80e688bef0a2d","schema_version":"1.0","event_id":"sha256:959b6036cd1eee909a265f1e5fef58b04e0be12910dabd5b4eb80e688bef0a2d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:IIL4CBGCPULNSTCF2XFIUL4FL2","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Coherent destruction of tunneling in graphene irradiated by elliptically polarized lasers","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.optics","quant-ph"],"primary_cat":"cond-mat.mes-hall","authors_text":"Catherine Lefebvre, Denis Gagnon, Fran\\c{c}ois Fillion-Gourdeau, Joey Dumont, Steve MacLean","submitted_at":"2016-09-09T14:59:30Z","abstract_excerpt":"Photo-induced transition probabilities in graphene are studied theoretically from the viewpoint of Floquet theory. Conduction band populations are computed for a strongly, periodically driven graphene sheet under linear, circular, and elliptic polarization. Features of the momentum spectrum of excited quasi-particles can be directly related to the avoided crossing of the Floquet quasi-energy levels. In particular, the impact of the ellipticity and the strength of the laser excitation on the avoided crossing structure -- and on the resulting transition probabilities -- is studied. It is shown t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1609.02821","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":"2026-05-18T00:58:50Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nce6pHMuLUPZ8ZV2Fs++F2U6fYTQsWeeaDpKc7b9J6HyNSGBGawImxRESjOzox2GzaCF5p6QpabTOvWgCpyxDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T13:39:38.568719Z"},"content_sha256":"2cba174d76a8d8e6e4d63c1673471cb3346679af3ed79c9ff60eac92bc9093af","schema_version":"1.0","event_id":"sha256:2cba174d76a8d8e6e4d63c1673471cb3346679af3ed79c9ff60eac92bc9093af"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/IIL4CBGCPULNSTCF2XFIUL4FL2/bundle.json","state_url":"https://pith.science/pith/IIL4CBGCPULNSTCF2XFIUL4FL2/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/IIL4CBGCPULNSTCF2XFIUL4FL2/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":"2026-06-01T13:39:38Z","links":{"resolver":"https://pith.science/pith/IIL4CBGCPULNSTCF2XFIUL4FL2","bundle":"https://pith.science/pith/IIL4CBGCPULNSTCF2XFIUL4FL2/bundle.json","state":"https://pith.science/pith/IIL4CBGCPULNSTCF2XFIUL4FL2/state.json","well_known_bundle":"https://pith.science/.well-known/pith/IIL4CBGCPULNSTCF2XFIUL4FL2/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:IIL4CBGCPULNSTCF2XFIUL4FL2","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":"973a564d2d308293074ae2dfa5eb116d256d57fbbf57e4388c217e792237e975","cross_cats_sorted":["physics.optics","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-09-09T14:59:30Z","title_canon_sha256":"0aaa2d3f21e74d130cb99257cd4e778160176e6f4660bd4c33ef7a175d3365ec"},"schema_version":"1.0","source":{"id":"1609.02821","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1609.02821","created_at":"2026-05-18T00:58:50Z"},{"alias_kind":"arxiv_version","alias_value":"1609.02821v2","created_at":"2026-05-18T00:58:50Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1609.02821","created_at":"2026-05-18T00:58:50Z"},{"alias_kind":"pith_short_12","alias_value":"IIL4CBGCPULN","created_at":"2026-05-18T12:30:22Z"},{"alias_kind":"pith_short_16","alias_value":"IIL4CBGCPULNSTCF","created_at":"2026-05-18T12:30:22Z"},{"alias_kind":"pith_short_8","alias_value":"IIL4CBGC","created_at":"2026-05-18T12:30:22Z"}],"graph_snapshots":[{"event_id":"sha256:2cba174d76a8d8e6e4d63c1673471cb3346679af3ed79c9ff60eac92bc9093af","target":"graph","created_at":"2026-05-18T00:58:50Z","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":"Photo-induced transition probabilities in graphene are studied theoretically from the viewpoint of Floquet theory. Conduction band populations are computed for a strongly, periodically driven graphene sheet under linear, circular, and elliptic polarization. Features of the momentum spectrum of excited quasi-particles can be directly related to the avoided crossing of the Floquet quasi-energy levels. In particular, the impact of the ellipticity and the strength of the laser excitation on the avoided crossing structure -- and on the resulting transition probabilities -- is studied. It is shown t","authors_text":"Catherine Lefebvre, Denis Gagnon, Fran\\c{c}ois Fillion-Gourdeau, Joey Dumont, Steve MacLean","cross_cats":["physics.optics","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-09-09T14:59:30Z","title":"Coherent destruction of tunneling in graphene irradiated by elliptically polarized lasers"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1609.02821","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":"sha256:959b6036cd1eee909a265f1e5fef58b04e0be12910dabd5b4eb80e688bef0a2d","target":"record","created_at":"2026-05-18T00:58:50Z","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":"973a564d2d308293074ae2dfa5eb116d256d57fbbf57e4388c217e792237e975","cross_cats_sorted":["physics.optics","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-09-09T14:59:30Z","title_canon_sha256":"0aaa2d3f21e74d130cb99257cd4e778160176e6f4660bd4c33ef7a175d3365ec"},"schema_version":"1.0","source":{"id":"1609.02821","kind":"arxiv","version":2}},"canonical_sha256":"4217c104c27d16d94c45d5ca8a2f855ebf33a442232eee0cd2806f4f53d65110","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4217c104c27d16d94c45d5ca8a2f855ebf33a442232eee0cd2806f4f53d65110","first_computed_at":"2026-05-18T00:58:50.775089Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:58:50.775089Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"B3KmUccOeDmEPRJSDFFnD0e8FPTlQubRyr1DXV9vcmEaep71lW+LcD0pEpvU0XcuqX8ZfB32KgeLrGAyx106CA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:58:50.775659Z","signed_message":"canonical_sha256_bytes"},"source_id":"1609.02821","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:959b6036cd1eee909a265f1e5fef58b04e0be12910dabd5b4eb80e688bef0a2d","sha256:2cba174d76a8d8e6e4d63c1673471cb3346679af3ed79c9ff60eac92bc9093af"],"state_sha256":"9556a20ae38524d56cf62a71f1310d8f64544f182009a7812d3053faf511ba80"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Bf3O8AUWSbmBk1WcPqcLbXun8fzjILNFoGJhuqOo7nnCclVGu0pKhkihq3MYi1lHmFXZ2ephByUEaVdzu5IODw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T13:39:38.570754Z","bundle_sha256":"99649e05041dace13c2630f8531776d7e7d14698a8170a44cc82e45b1f604e68"}}