{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:VCNZCTFW7RXEH6VA7V6HDDMYGZ","short_pith_number":"pith:VCNZCTFW","schema_version":"1.0","canonical_sha256":"a89b914cb6fc6e43faa0fd7c718d983641c48d08abf04f95760a3420de9c9ea7","source":{"kind":"arxiv","id":"1702.05897","version":1},"attestation_state":"computed","paper":{"title":"A dynamical stability limit for the charge density wave in K0.3MoO3","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Andrea Cavalleri, Biaolong Liu, Daixiang Mou, Haiyun Liu, Michael F\\\"orst, Roberto Merlin, Roman Mankowsky, Srivats Rajasekaran, X. J. Zhou","submitted_at":"2017-02-20T08:48:16Z","abstract_excerpt":"We study the response of the one-dimensional charge density wave in K0.3MoO3 to different types of excitation with femtosecond optical pulses. We compare the response to direct excitation of the lattice at mid-infrared frequencies with that to the injection of quasi-particles across the low-energy charge density wave gap and to charge transfer excitations in the near infrared. For all three cases, we observe a fluence threshold above which the amplitude-mode oscillation frequency is softened and the mode becomes increasingly damped. We show that all the data can be collapsed onto a universal c"},"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":"1702.05897","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-02-20T08:48:16Z","cross_cats_sorted":[],"title_canon_sha256":"013cc74f13f9e5e2bd3c6d91e0430d7e8715bc0a99b4ed45e1f86869a8294307","abstract_canon_sha256":"9317d4f594faa2ac63204a3be25248cc5f497510aeda283f6124991c97c1d545"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:47:03.258637Z","signature_b64":"jCqzo5GpauSvS55XXFpbw4lYI1HvpDk6DYreLSu71pNfCDaYH0qHzfU79osaZoJllv6KOsMkZPBag+hFQp7TDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a89b914cb6fc6e43faa0fd7c718d983641c48d08abf04f95760a3420de9c9ea7","last_reissued_at":"2026-05-18T00:47:03.258197Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:47:03.258197Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A dynamical stability limit for the charge density wave in K0.3MoO3","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Andrea Cavalleri, Biaolong Liu, Daixiang Mou, Haiyun Liu, Michael F\\\"orst, Roberto Merlin, Roman Mankowsky, Srivats Rajasekaran, X. J. Zhou","submitted_at":"2017-02-20T08:48:16Z","abstract_excerpt":"We study the response of the one-dimensional charge density wave in K0.3MoO3 to different types of excitation with femtosecond optical pulses. We compare the response to direct excitation of the lattice at mid-infrared frequencies with that to the injection of quasi-particles across the low-energy charge density wave gap and to charge transfer excitations in the near infrared. For all three cases, we observe a fluence threshold above which the amplitude-mode oscillation frequency is softened and the mode becomes increasingly damped. We show that all the data can be collapsed onto a universal c"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1702.05897","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1702.05897","created_at":"2026-05-18T00:47:03.258262+00:00"},{"alias_kind":"arxiv_version","alias_value":"1702.05897v1","created_at":"2026-05-18T00:47:03.258262+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1702.05897","created_at":"2026-05-18T00:47:03.258262+00:00"},{"alias_kind":"pith_short_12","alias_value":"VCNZCTFW7RXE","created_at":"2026-05-18T12:31:49.984773+00:00"},{"alias_kind":"pith_short_16","alias_value":"VCNZCTFW7RXEH6VA","created_at":"2026-05-18T12:31:49.984773+00:00"},{"alias_kind":"pith_short_8","alias_value":"VCNZCTFW","created_at":"2026-05-18T12:31:49.984773+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/VCNZCTFW7RXEH6VA7V6HDDMYGZ","json":"https://pith.science/pith/VCNZCTFW7RXEH6VA7V6HDDMYGZ.json","graph_json":"https://pith.science/api/pith-number/VCNZCTFW7RXEH6VA7V6HDDMYGZ/graph.json","events_json":"https://pith.science/api/pith-number/VCNZCTFW7RXEH6VA7V6HDDMYGZ/events.json","paper":"https://pith.science/paper/VCNZCTFW"},"agent_actions":{"view_html":"https://pith.science/pith/VCNZCTFW7RXEH6VA7V6HDDMYGZ","download_json":"https://pith.science/pith/VCNZCTFW7RXEH6VA7V6HDDMYGZ.json","view_paper":"https://pith.science/paper/VCNZCTFW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1702.05897&json=true","fetch_graph":"https://pith.science/api/pith-number/VCNZCTFW7RXEH6VA7V6HDDMYGZ/graph.json","fetch_events":"https://pith.science/api/pith-number/VCNZCTFW7RXEH6VA7V6HDDMYGZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VCNZCTFW7RXEH6VA7V6HDDMYGZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VCNZCTFW7RXEH6VA7V6HDDMYGZ/action/storage_attestation","attest_author":"https://pith.science/pith/VCNZCTFW7RXEH6VA7V6HDDMYGZ/action/author_attestation","sign_citation":"https://pith.science/pith/VCNZCTFW7RXEH6VA7V6HDDMYGZ/action/citation_signature","submit_replication":"https://pith.science/pith/VCNZCTFW7RXEH6VA7V6HDDMYGZ/action/replication_record"}},"created_at":"2026-05-18T00:47:03.258262+00:00","updated_at":"2026-05-18T00:47:03.258262+00:00"}