{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:YVQGLKMV5SN4ID2CUU6ORV6VBN","short_pith_number":"pith:YVQGLKMV","schema_version":"1.0","canonical_sha256":"c56065a995ec9bc40f42a53ce8d7d50b40f8804c5f18a0cdf198941ff0a2ec7d","source":{"kind":"arxiv","id":"1805.10879","version":1},"attestation_state":"computed","paper":{"title":"Experimental demonstration of work fluctuations along a shortcut to adiabaticity with a superconducting Xmon qubit","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"GuoPing Guo, Jianlan Wu, Liang Xiang, Luyan Sun, Peng Duan, Tenghui Wang, Weizhou Cai, Yi Yin, Ze Zhan, Zhenxing Zhang, Zhilong Jia, Zhiwen Zong","submitted_at":"2018-05-28T11:59:22Z","abstract_excerpt":"In a `shortcut-to-adiabaticity' (STA) protocol, the counter-diabatic Hamiltonian, which suppresses the non-adiabatic transition of a reference `adiabatic' trajectory, induces a quantum uncertainty of the work cost in the framework of quantum thermodynamics. Following a theory derived recently [Funo et al 2017 Phys. Rev. Lett. 118 100602], we perform an experimental measurement of the STA work statistics in a high-quality superconducting Xmon qubit. Through the frozen-Hamiltonian and frozen-population techniques, we experimentally realize the two-point measurement of the work distribution for g"},"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":"1805.10879","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2018-05-28T11:59:22Z","cross_cats_sorted":[],"title_canon_sha256":"fd0c1f58f19bcaa333ae55e98e77089075cefc3877cb09fc92232f2c9380333a","abstract_canon_sha256":"ab07b6cd5d8767864205a33e79f9ec93b6c65cff1b0b55c32c1ff5df0e1a2125"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:06:59.580704Z","signature_b64":"sYapO96pjvu0vCpkk0SULuLfspJxhCihEySZ+Doq8k1riDNl2dajpDYTzB/0XXVEWG0bE1+dho7uOqDPEna4AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c56065a995ec9bc40f42a53ce8d7d50b40f8804c5f18a0cdf198941ff0a2ec7d","last_reissued_at":"2026-05-18T00:06:59.580097Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:06:59.580097Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Experimental demonstration of work fluctuations along a shortcut to adiabaticity with a superconducting Xmon qubit","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"GuoPing Guo, Jianlan Wu, Liang Xiang, Luyan Sun, Peng Duan, Tenghui Wang, Weizhou Cai, Yi Yin, Ze Zhan, Zhenxing Zhang, Zhilong Jia, Zhiwen Zong","submitted_at":"2018-05-28T11:59:22Z","abstract_excerpt":"In a `shortcut-to-adiabaticity' (STA) protocol, the counter-diabatic Hamiltonian, which suppresses the non-adiabatic transition of a reference `adiabatic' trajectory, induces a quantum uncertainty of the work cost in the framework of quantum thermodynamics. Following a theory derived recently [Funo et al 2017 Phys. Rev. Lett. 118 100602], we perform an experimental measurement of the STA work statistics in a high-quality superconducting Xmon qubit. Through the frozen-Hamiltonian and frozen-population techniques, we experimentally realize the two-point measurement of the work distribution for g"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1805.10879","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":"1805.10879","created_at":"2026-05-18T00:06:59.580183+00:00"},{"alias_kind":"arxiv_version","alias_value":"1805.10879v1","created_at":"2026-05-18T00:06:59.580183+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1805.10879","created_at":"2026-05-18T00:06:59.580183+00:00"},{"alias_kind":"pith_short_12","alias_value":"YVQGLKMV5SN4","created_at":"2026-05-18T12:33:04.347982+00:00"},{"alias_kind":"pith_short_16","alias_value":"YVQGLKMV5SN4ID2C","created_at":"2026-05-18T12:33:04.347982+00:00"},{"alias_kind":"pith_short_8","alias_value":"YVQGLKMV","created_at":"2026-05-18T12:33:04.347982+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/YVQGLKMV5SN4ID2CUU6ORV6VBN","json":"https://pith.science/pith/YVQGLKMV5SN4ID2CUU6ORV6VBN.json","graph_json":"https://pith.science/api/pith-number/YVQGLKMV5SN4ID2CUU6ORV6VBN/graph.json","events_json":"https://pith.science/api/pith-number/YVQGLKMV5SN4ID2CUU6ORV6VBN/events.json","paper":"https://pith.science/paper/YVQGLKMV"},"agent_actions":{"view_html":"https://pith.science/pith/YVQGLKMV5SN4ID2CUU6ORV6VBN","download_json":"https://pith.science/pith/YVQGLKMV5SN4ID2CUU6ORV6VBN.json","view_paper":"https://pith.science/paper/YVQGLKMV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1805.10879&json=true","fetch_graph":"https://pith.science/api/pith-number/YVQGLKMV5SN4ID2CUU6ORV6VBN/graph.json","fetch_events":"https://pith.science/api/pith-number/YVQGLKMV5SN4ID2CUU6ORV6VBN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YVQGLKMV5SN4ID2CUU6ORV6VBN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YVQGLKMV5SN4ID2CUU6ORV6VBN/action/storage_attestation","attest_author":"https://pith.science/pith/YVQGLKMV5SN4ID2CUU6ORV6VBN/action/author_attestation","sign_citation":"https://pith.science/pith/YVQGLKMV5SN4ID2CUU6ORV6VBN/action/citation_signature","submit_replication":"https://pith.science/pith/YVQGLKMV5SN4ID2CUU6ORV6VBN/action/replication_record"}},"created_at":"2026-05-18T00:06:59.580183+00:00","updated_at":"2026-05-18T00:06:59.580183+00:00"}