{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:LGFQTIO66N362LNNTJ6STVHWTM","short_pith_number":"pith:LGFQTIO6","canonical_record":{"source":{"id":"1301.7585","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2013-01-31T12:08:30Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"d5e4f35046b72e76ca3f57a72606d7108540dada8aafdad9d7ad36839a70b5e1","abstract_canon_sha256":"1e13e2bab2829ee0aef5d9e67af585de7f78bd15c44a41f510594a98aba14f7d"},"schema_version":"1.0"},"canonical_sha256":"598b09a1def377ed2dad9a7d29d4f69b326ae093faefe5e49894a6e1ee4b278e","source":{"kind":"arxiv","id":"1301.7585","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1301.7585","created_at":"2026-05-18T03:13:46Z"},{"alias_kind":"arxiv_version","alias_value":"1301.7585v2","created_at":"2026-05-18T03:13:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1301.7585","created_at":"2026-05-18T03:13:46Z"},{"alias_kind":"pith_short_12","alias_value":"LGFQTIO66N36","created_at":"2026-05-18T12:27:51Z"},{"alias_kind":"pith_short_16","alias_value":"LGFQTIO66N362LNN","created_at":"2026-05-18T12:27:51Z"},{"alias_kind":"pith_short_8","alias_value":"LGFQTIO6","created_at":"2026-05-18T12:27:51Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:LGFQTIO66N362LNNTJ6STVHWTM","target":"record","payload":{"canonical_record":{"source":{"id":"1301.7585","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2013-01-31T12:08:30Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"d5e4f35046b72e76ca3f57a72606d7108540dada8aafdad9d7ad36839a70b5e1","abstract_canon_sha256":"1e13e2bab2829ee0aef5d9e67af585de7f78bd15c44a41f510594a98aba14f7d"},"schema_version":"1.0"},"canonical_sha256":"598b09a1def377ed2dad9a7d29d4f69b326ae093faefe5e49894a6e1ee4b278e","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:13:46.170180Z","signature_b64":"u31TNP6zzqkSVPMyfMMJhwW6F7ZbO8GPUW8PlxaY/SlmsJbBb2uV5nqHoPgJnzurjx6MJrC0G2IimxIUTBQ5AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"598b09a1def377ed2dad9a7d29d4f69b326ae093faefe5e49894a6e1ee4b278e","last_reissued_at":"2026-05-18T03:13:46.169454Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:13:46.169454Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1301.7585","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":"2026-05-18T03:13:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"BGIjNgIwNPDEdpDu3vm552xLxicoSfP9ialPBtUJFnCOiCtNevhJGDaQOAh0rcM+SfPMfK0NPYsT70Ym82EIAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T09:38:24.506137Z"},"content_sha256":"b7a60a3c4c4bc8b40973a81ed75d155c8e5e2e50acf18fd25dbaa660cb354f6c","schema_version":"1.0","event_id":"sha256:b7a60a3c4c4bc8b40973a81ed75d155c8e5e2e50acf18fd25dbaa660cb354f6c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:LGFQTIO66N362LNNTJ6STVHWTM","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Origin of electronic Raman scattering and the Fano resonance in metallic carbon nanotubes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Ahmad R. T. Nugraha, Eddwi H. Hasdeo, Kentaro Sato, Mildred S. Dresselhaus, Riichiro Saito","submitted_at":"2013-01-31T12:08:30Z","abstract_excerpt":"Fano resonance spectra for the G band in metallic carbon nanotubes are calculated as a function of laser excitation energy in which the origin of the resonance is given by an interference between the continuous electronic Raman spectra and the discrete phonon spectra. We found that the second-order scattering process of the non-zero q electron-electron interaction is more relevant to the continuous spectra rather than the q = 0 first-order process because the q = 0 direct Coulomb interaction vanishes due to the symmetry of the two sublattices of a nanotube. We also show that the RBM spectra of"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1301.7585","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":"2026-05-18T03:13:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ulQwr9yXBRHnkO/Exk5f3xI6GYewgtUutwEdmi90ABhfBP2sM/0po4HzXSMK1Itk1awHT8IpTpBDFwe4a242CQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T09:38:24.506509Z"},"content_sha256":"646ea8eb2358f3bcddbfaaab95430786de9c9136a8f3d8fde071e3c5a65d6ca7","schema_version":"1.0","event_id":"sha256:646ea8eb2358f3bcddbfaaab95430786de9c9136a8f3d8fde071e3c5a65d6ca7"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/LGFQTIO66N362LNNTJ6STVHWTM/bundle.json","state_url":"https://pith.science/pith/LGFQTIO66N362LNNTJ6STVHWTM/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/LGFQTIO66N362LNNTJ6STVHWTM/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":"2026-06-03T09:38:24Z","links":{"resolver":"https://pith.science/pith/LGFQTIO66N362LNNTJ6STVHWTM","bundle":"https://pith.science/pith/LGFQTIO66N362LNNTJ6STVHWTM/bundle.json","state":"https://pith.science/pith/LGFQTIO66N362LNNTJ6STVHWTM/state.json","well_known_bundle":"https://pith.science/.well-known/pith/LGFQTIO66N362LNNTJ6STVHWTM/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:LGFQTIO66N362LNNTJ6STVHWTM","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":"1e13e2bab2829ee0aef5d9e67af585de7f78bd15c44a41f510594a98aba14f7d","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2013-01-31T12:08:30Z","title_canon_sha256":"d5e4f35046b72e76ca3f57a72606d7108540dada8aafdad9d7ad36839a70b5e1"},"schema_version":"1.0","source":{"id":"1301.7585","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1301.7585","created_at":"2026-05-18T03:13:46Z"},{"alias_kind":"arxiv_version","alias_value":"1301.7585v2","created_at":"2026-05-18T03:13:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1301.7585","created_at":"2026-05-18T03:13:46Z"},{"alias_kind":"pith_short_12","alias_value":"LGFQTIO66N36","created_at":"2026-05-18T12:27:51Z"},{"alias_kind":"pith_short_16","alias_value":"LGFQTIO66N362LNN","created_at":"2026-05-18T12:27:51Z"},{"alias_kind":"pith_short_8","alias_value":"LGFQTIO6","created_at":"2026-05-18T12:27:51Z"}],"graph_snapshots":[{"event_id":"sha256:646ea8eb2358f3bcddbfaaab95430786de9c9136a8f3d8fde071e3c5a65d6ca7","target":"graph","created_at":"2026-05-18T03:13:46Z","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 resonance spectra for the G band in metallic carbon nanotubes are calculated as a function of laser excitation energy in which the origin of the resonance is given by an interference between the continuous electronic Raman spectra and the discrete phonon spectra. We found that the second-order scattering process of the non-zero q electron-electron interaction is more relevant to the continuous spectra rather than the q = 0 first-order process because the q = 0 direct Coulomb interaction vanishes due to the symmetry of the two sublattices of a nanotube. We also show that the RBM spectra of","authors_text":"Ahmad R. T. Nugraha, Eddwi H. Hasdeo, Kentaro Sato, Mildred S. Dresselhaus, Riichiro Saito","cross_cats":["cond-mat.mes-hall"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2013-01-31T12:08:30Z","title":"Origin of electronic Raman scattering and the Fano resonance in metallic carbon nanotubes"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1301.7585","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:b7a60a3c4c4bc8b40973a81ed75d155c8e5e2e50acf18fd25dbaa660cb354f6c","target":"record","created_at":"2026-05-18T03:13:46Z","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":"1e13e2bab2829ee0aef5d9e67af585de7f78bd15c44a41f510594a98aba14f7d","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2013-01-31T12:08:30Z","title_canon_sha256":"d5e4f35046b72e76ca3f57a72606d7108540dada8aafdad9d7ad36839a70b5e1"},"schema_version":"1.0","source":{"id":"1301.7585","kind":"arxiv","version":2}},"canonical_sha256":"598b09a1def377ed2dad9a7d29d4f69b326ae093faefe5e49894a6e1ee4b278e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"598b09a1def377ed2dad9a7d29d4f69b326ae093faefe5e49894a6e1ee4b278e","first_computed_at":"2026-05-18T03:13:46.169454Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:13:46.169454Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"u31TNP6zzqkSVPMyfMMJhwW6F7ZbO8GPUW8PlxaY/SlmsJbBb2uV5nqHoPgJnzurjx6MJrC0G2IimxIUTBQ5AA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:13:46.170180Z","signed_message":"canonical_sha256_bytes"},"source_id":"1301.7585","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b7a60a3c4c4bc8b40973a81ed75d155c8e5e2e50acf18fd25dbaa660cb354f6c","sha256:646ea8eb2358f3bcddbfaaab95430786de9c9136a8f3d8fde071e3c5a65d6ca7"],"state_sha256":"0bc6bd9ab28be227058f61576245d5485dda73a4e3cd95b54ee4afad30339287"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"s8O7IsgZQ4mMs61Q16zLXLsPkMY6h8KZP9aOV6bUuFMUdZVETlYU9mXTK0fQP/D8SLr9HNEqZfKAvd/jDkuRAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-03T09:38:24.508555Z","bundle_sha256":"f35cad21b9e270543d0b2c2b1140b8c7947f987f3ea5519ccba272d387f92e2f"}}