{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:MNWJQBUNQSEZWLQ3MN3DDQJDUU","short_pith_number":"pith:MNWJQBUN","schema_version":"1.0","canonical_sha256":"636c98068d84899b2e1b637631c123a53fdcbc5aca34afddfbb19b4ad63b3d7e","source":{"kind":"arxiv","id":"1603.08374","version":2},"attestation_state":"computed","paper":{"title":"Ultrafast response of plasma-like reflectivity edge in (TMTTF)2AsF6 driven by 7-fs, 1.5-cycle strong-light field","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"H. Itoh, K. Yamamoto, K. Yonemitsu, M. Dressel, S. Ishihara, S. Iwai, T. Ishikawa, T. Sasaki, Y. Kawakami, Y. Naitoh, Y. Sagae, Y. Tanaka","submitted_at":"2016-03-28T13:04:27Z","abstract_excerpt":"The strong light-field effect of (TMTTF)2AsF6 was investigated utilizing 1.5-cycle, 7-fs infrared pulses. The ultarfast (20 fs) and large (40%) response of the plasma-like reflectivity edge (0.7 eV) was analyzed by the changes in omega_p=sqrt(ne2/(epsilon_0*epsilon(infty)*m)} (n: number of charges in the 1/4 filled-band, m: mass of charge, epsilon(infty): dielectric constants for high-frequency and vacuum, e: elementary charge). The 3% reduction in omega_p is attributed to the 6% increase in m. Furthermore, 20 fs oscillation of omega_p in the time domain indicates that the plasma-like edge is "},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1603.08374","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2016-03-28T13:04:27Z","cross_cats_sorted":[],"title_canon_sha256":"c2fb71ed4043f3f3f0999fa2163825d43d707da48c0292013d631fed1cc5fcb8","abstract_canon_sha256":"704005adc8cffed54741fc2bdd6c1006601ff3b4074ccb96c443e253d8297546"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:16:37.422416Z","signature_b64":"f8wveDCEdAigmB72swwL9UFjp6j/g+qGGnrzlBkJGwtFVfDb0+47ojkfK6zNmMy9DOkOIt/PLYcLBfyJnq93Bw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"636c98068d84899b2e1b637631c123a53fdcbc5aca34afddfbb19b4ad63b3d7e","last_reissued_at":"2026-05-18T01:16:37.421848Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:16:37.421848Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Ultrafast response of plasma-like reflectivity edge in (TMTTF)2AsF6 driven by 7-fs, 1.5-cycle strong-light field","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"H. Itoh, K. Yamamoto, K. Yonemitsu, M. Dressel, S. Ishihara, S. Iwai, T. Ishikawa, T. Sasaki, Y. Kawakami, Y. Naitoh, Y. Sagae, Y. Tanaka","submitted_at":"2016-03-28T13:04:27Z","abstract_excerpt":"The strong light-field effect of (TMTTF)2AsF6 was investigated utilizing 1.5-cycle, 7-fs infrared pulses. The ultarfast (20 fs) and large (40%) response of the plasma-like reflectivity edge (0.7 eV) was analyzed by the changes in omega_p=sqrt(ne2/(epsilon_0*epsilon(infty)*m)} (n: number of charges in the 1/4 filled-band, m: mass of charge, epsilon(infty): dielectric constants for high-frequency and vacuum, e: elementary charge). The 3% reduction in omega_p is attributed to the 6% increase in m. Furthermore, 20 fs oscillation of omega_p in the time domain indicates that the plasma-like edge is "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1603.08374","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1603.08374","created_at":"2026-05-18T01:16:37.421944+00:00"},{"alias_kind":"arxiv_version","alias_value":"1603.08374v2","created_at":"2026-05-18T01:16:37.421944+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1603.08374","created_at":"2026-05-18T01:16:37.421944+00:00"},{"alias_kind":"pith_short_12","alias_value":"MNWJQBUNQSEZ","created_at":"2026-05-18T12:30:32.724797+00:00"},{"alias_kind":"pith_short_16","alias_value":"MNWJQBUNQSEZWLQ3","created_at":"2026-05-18T12:30:32.724797+00:00"},{"alias_kind":"pith_short_8","alias_value":"MNWJQBUN","created_at":"2026-05-18T12:30:32.724797+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MNWJQBUNQSEZWLQ3MN3DDQJDUU","json":"https://pith.science/pith/MNWJQBUNQSEZWLQ3MN3DDQJDUU.json","graph_json":"https://pith.science/api/pith-number/MNWJQBUNQSEZWLQ3MN3DDQJDUU/graph.json","events_json":"https://pith.science/api/pith-number/MNWJQBUNQSEZWLQ3MN3DDQJDUU/events.json","paper":"https://pith.science/paper/MNWJQBUN"},"agent_actions":{"view_html":"https://pith.science/pith/MNWJQBUNQSEZWLQ3MN3DDQJDUU","download_json":"https://pith.science/pith/MNWJQBUNQSEZWLQ3MN3DDQJDUU.json","view_paper":"https://pith.science/paper/MNWJQBUN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1603.08374&json=true","fetch_graph":"https://pith.science/api/pith-number/MNWJQBUNQSEZWLQ3MN3DDQJDUU/graph.json","fetch_events":"https://pith.science/api/pith-number/MNWJQBUNQSEZWLQ3MN3DDQJDUU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MNWJQBUNQSEZWLQ3MN3DDQJDUU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MNWJQBUNQSEZWLQ3MN3DDQJDUU/action/storage_attestation","attest_author":"https://pith.science/pith/MNWJQBUNQSEZWLQ3MN3DDQJDUU/action/author_attestation","sign_citation":"https://pith.science/pith/MNWJQBUNQSEZWLQ3MN3DDQJDUU/action/citation_signature","submit_replication":"https://pith.science/pith/MNWJQBUNQSEZWLQ3MN3DDQJDUU/action/replication_record"}},"created_at":"2026-05-18T01:16:37.421944+00:00","updated_at":"2026-05-18T01:16:37.421944+00:00"}