{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2019:6JAQKUF5YS7TXVEOUBMTY6WRQO","short_pith_number":"pith:6JAQKUF5","canonical_record":{"source":{"id":"1905.07743","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2019-05-19T13:44:55Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"cfaedc389cde4fa63aa5e54b479b202aa65982362e837c8e58460988074d02d9","abstract_canon_sha256":"c69ab1138d8ac350a441db2b7e44f0f4674931d05ccff557fce0bd1a91c34a0a"},"schema_version":"1.0"},"canonical_sha256":"f2410550bdc4bf3bd48ea0593c7ad1838946a1e932db705e8e6a476e92414e3f","source":{"kind":"arxiv","id":"1905.07743","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1905.07743","created_at":"2026-05-17T23:45:48Z"},{"alias_kind":"arxiv_version","alias_value":"1905.07743v1","created_at":"2026-05-17T23:45:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1905.07743","created_at":"2026-05-17T23:45:48Z"},{"alias_kind":"pith_short_12","alias_value":"6JAQKUF5YS7T","created_at":"2026-05-18T12:33:10Z"},{"alias_kind":"pith_short_16","alias_value":"6JAQKUF5YS7TXVEO","created_at":"2026-05-18T12:33:10Z"},{"alias_kind":"pith_short_8","alias_value":"6JAQKUF5","created_at":"2026-05-18T12:33:10Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2019:6JAQKUF5YS7TXVEOUBMTY6WRQO","target":"record","payload":{"canonical_record":{"source":{"id":"1905.07743","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2019-05-19T13:44:55Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"cfaedc389cde4fa63aa5e54b479b202aa65982362e837c8e58460988074d02d9","abstract_canon_sha256":"c69ab1138d8ac350a441db2b7e44f0f4674931d05ccff557fce0bd1a91c34a0a"},"schema_version":"1.0"},"canonical_sha256":"f2410550bdc4bf3bd48ea0593c7ad1838946a1e932db705e8e6a476e92414e3f","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:45:48.607978Z","signature_b64":"fQpFdkk1vj2Nw+4yWcU7tXgp6vNxK/1t4QjZ1YpRuvHt0K0dTMFQ6yNmKL6LinD04oCY1yvux13dxTX9IVeiCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f2410550bdc4bf3bd48ea0593c7ad1838946a1e932db705e8e6a476e92414e3f","last_reissued_at":"2026-05-17T23:45:48.607423Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:45:48.607423Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1905.07743","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":"2026-05-17T23:45:48Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"H7pPl7b+6ebae11Jdx3hxFYaWrb6N910HEiepbaK8OZy6VBGdF6qYnRUpjKxdU0TICynllA0S155kMTtqOreDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T08:49:34.069535Z"},"content_sha256":"7ba760d7c739b037ddfe5580583c932e8ec318a4e480efa1dcf18071c673d4a5","schema_version":"1.0","event_id":"sha256:7ba760d7c739b037ddfe5580583c932e8ec318a4e480efa1dcf18071c673d4a5"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2019:6JAQKUF5YS7TXVEOUBMTY6WRQO","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Two-dimensional Fano lineshapes: Excited-state absorption contributions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"physics.chem-ph","authors_text":"Daniel Finkelstein-Shapiro, Thorsten Hansen, T\\~onu Pullerits","submitted_at":"2019-05-19T13:44:55Z","abstract_excerpt":"Fano interferences in nanostructures are influenced by dissipation effects as well as many-body interactions. Two dimensional coherent spectroscopies have just begun to be applied to these systems where the spectroscopic signatures of a discrete-continuum structure are not known. In this article we calculate the excited-state absorption contribution for different models of higher-lying excited states. We find that the characteristic asymmetry of one-dimensional spectroscopies is recovered from the many-body contributions, and that the higher-lying excited manifolds have distorted lineshapes th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1905.07743","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":"2026-05-17T23:45:48Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dnCAulf2NF5xTiNvm9fQ7M+7xLRkmPNU2fFDMBrZQg0b4VFvkGStIlYcp/ikC0pmR6Fr+j2TA+seMH+R8GkTDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T08:49:34.070181Z"},"content_sha256":"142b5b4365f9977fba66f83aa4ef2ab0f08b8016e695cd78d165d4e6f911fabf","schema_version":"1.0","event_id":"sha256:142b5b4365f9977fba66f83aa4ef2ab0f08b8016e695cd78d165d4e6f911fabf"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6JAQKUF5YS7TXVEOUBMTY6WRQO/bundle.json","state_url":"https://pith.science/pith/6JAQKUF5YS7TXVEOUBMTY6WRQO/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6JAQKUF5YS7TXVEOUBMTY6WRQO/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":"2026-05-30T08:49:34Z","links":{"resolver":"https://pith.science/pith/6JAQKUF5YS7TXVEOUBMTY6WRQO","bundle":"https://pith.science/pith/6JAQKUF5YS7TXVEOUBMTY6WRQO/bundle.json","state":"https://pith.science/pith/6JAQKUF5YS7TXVEOUBMTY6WRQO/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6JAQKUF5YS7TXVEOUBMTY6WRQO/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:6JAQKUF5YS7TXVEOUBMTY6WRQO","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":"c69ab1138d8ac350a441db2b7e44f0f4674931d05ccff557fce0bd1a91c34a0a","cross_cats_sorted":["quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2019-05-19T13:44:55Z","title_canon_sha256":"cfaedc389cde4fa63aa5e54b479b202aa65982362e837c8e58460988074d02d9"},"schema_version":"1.0","source":{"id":"1905.07743","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1905.07743","created_at":"2026-05-17T23:45:48Z"},{"alias_kind":"arxiv_version","alias_value":"1905.07743v1","created_at":"2026-05-17T23:45:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1905.07743","created_at":"2026-05-17T23:45:48Z"},{"alias_kind":"pith_short_12","alias_value":"6JAQKUF5YS7T","created_at":"2026-05-18T12:33:10Z"},{"alias_kind":"pith_short_16","alias_value":"6JAQKUF5YS7TXVEO","created_at":"2026-05-18T12:33:10Z"},{"alias_kind":"pith_short_8","alias_value":"6JAQKUF5","created_at":"2026-05-18T12:33:10Z"}],"graph_snapshots":[{"event_id":"sha256:142b5b4365f9977fba66f83aa4ef2ab0f08b8016e695cd78d165d4e6f911fabf","target":"graph","created_at":"2026-05-17T23:45:48Z","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":"Fano interferences in nanostructures are influenced by dissipation effects as well as many-body interactions. Two dimensional coherent spectroscopies have just begun to be applied to these systems where the spectroscopic signatures of a discrete-continuum structure are not known. In this article we calculate the excited-state absorption contribution for different models of higher-lying excited states. We find that the characteristic asymmetry of one-dimensional spectroscopies is recovered from the many-body contributions, and that the higher-lying excited manifolds have distorted lineshapes th","authors_text":"Daniel Finkelstein-Shapiro, Thorsten Hansen, T\\~onu Pullerits","cross_cats":["quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2019-05-19T13:44:55Z","title":"Two-dimensional Fano lineshapes: Excited-state absorption contributions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1905.07743","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":"sha256:7ba760d7c739b037ddfe5580583c932e8ec318a4e480efa1dcf18071c673d4a5","target":"record","created_at":"2026-05-17T23:45:48Z","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":"c69ab1138d8ac350a441db2b7e44f0f4674931d05ccff557fce0bd1a91c34a0a","cross_cats_sorted":["quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2019-05-19T13:44:55Z","title_canon_sha256":"cfaedc389cde4fa63aa5e54b479b202aa65982362e837c8e58460988074d02d9"},"schema_version":"1.0","source":{"id":"1905.07743","kind":"arxiv","version":1}},"canonical_sha256":"f2410550bdc4bf3bd48ea0593c7ad1838946a1e932db705e8e6a476e92414e3f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f2410550bdc4bf3bd48ea0593c7ad1838946a1e932db705e8e6a476e92414e3f","first_computed_at":"2026-05-17T23:45:48.607423Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:45:48.607423Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"fQpFdkk1vj2Nw+4yWcU7tXgp6vNxK/1t4QjZ1YpRuvHt0K0dTMFQ6yNmKL6LinD04oCY1yvux13dxTX9IVeiCQ==","signature_status":"signed_v1","signed_at":"2026-05-17T23:45:48.607978Z","signed_message":"canonical_sha256_bytes"},"source_id":"1905.07743","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7ba760d7c739b037ddfe5580583c932e8ec318a4e480efa1dcf18071c673d4a5","sha256:142b5b4365f9977fba66f83aa4ef2ab0f08b8016e695cd78d165d4e6f911fabf"],"state_sha256":"127e7eedd66341955734835568bbdf731d2bfd813df60a180ca0ad600939319a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"kOG0WgsePNvEytmU6CXgGUSsqK5l9r7la/BPE9rDVJlc5wSft56Xf8SNX4L2+kW30ewzA/+MG324XMFMc19ODQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T08:49:34.073406Z","bundle_sha256":"eb1ffa11def88938b8879493a59b845174ebf1c3db15218baa1e19ee09e3c531"}}