{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:66WSYNKWE6Y3ZREKLUKG7TSUET","short_pith_number":"pith:66WSYNKW","schema_version":"1.0","canonical_sha256":"f7ad2c355627b1bcc48a5d146fce5424e893e9f00228c899a107fd1210fbb2d9","source":{"kind":"arxiv","id":"1903.05336","version":2},"attestation_state":"computed","paper":{"title":"Topology by Dissipation: Transport properties","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","cond-mat.str-el"],"primary_cat":"cond-mat.quant-gas","authors_text":"Gal Shavit, Moshe Goldstein","submitted_at":"2019-03-13T07:02:23Z","abstract_excerpt":"Topological phases of matter are the center of much current interest, with promising potential applications in, e.g., topologically-protected transport and quantum computing. Traditionally such states are prepared by tuning the system Hamiltonian while coupling it to a generic bath at very low temperatures; This approach is often ineffective, especially in cold-atom systems. It was recently shown that topological phases can emerge much more efficiently even in the absence of a Hamiltonian, by properly engineering the interaction of the system with its environment, to directly drive the system "},"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":"1903.05336","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2019-03-13T07:02:23Z","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.str-el"],"title_canon_sha256":"ad4ff571efcab4249271c54a8e126e616e091038fcc562498e98c07a7b3aaa10","abstract_canon_sha256":"560549f2ae110c8f245ff8f8d4b484b4978707957cf91185b1cfbb55e14975fc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:47:56.344005Z","signature_b64":"RndpbYNIqTchy5S9H608YPZ000nOOT9NFZX+Fuzp6SvfO2ItOttXSfJikI2Ezv6QCwwZgi17d6p4MNFpRbxaBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f7ad2c355627b1bcc48a5d146fce5424e893e9f00228c899a107fd1210fbb2d9","last_reissued_at":"2026-07-05T00:47:56.343582Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:47:56.343582Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Topology by Dissipation: Transport properties","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","cond-mat.str-el"],"primary_cat":"cond-mat.quant-gas","authors_text":"Gal Shavit, Moshe Goldstein","submitted_at":"2019-03-13T07:02:23Z","abstract_excerpt":"Topological phases of matter are the center of much current interest, with promising potential applications in, e.g., topologically-protected transport and quantum computing. Traditionally such states are prepared by tuning the system Hamiltonian while coupling it to a generic bath at very low temperatures; This approach is often ineffective, especially in cold-atom systems. It was recently shown that topological phases can emerge much more efficiently even in the absence of a Hamiltonian, by properly engineering the interaction of the system with its environment, to directly drive the system "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1903.05336","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1903.05336/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"1903.05336","created_at":"2026-07-05T00:47:56.343651+00:00"},{"alias_kind":"arxiv_version","alias_value":"1903.05336v2","created_at":"2026-07-05T00:47:56.343651+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1903.05336","created_at":"2026-07-05T00:47:56.343651+00:00"},{"alias_kind":"pith_short_12","alias_value":"66WSYNKWE6Y3","created_at":"2026-07-05T00:47:56.343651+00:00"},{"alias_kind":"pith_short_16","alias_value":"66WSYNKWE6Y3ZREK","created_at":"2026-07-05T00:47:56.343651+00:00"},{"alias_kind":"pith_short_8","alias_value":"66WSYNKW","created_at":"2026-07-05T00:47:56.343651+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1908.08834","citing_title":"Tenfold Way for Quadratic Lindbladians","ref_index":23,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/66WSYNKWE6Y3ZREKLUKG7TSUET","json":"https://pith.science/pith/66WSYNKWE6Y3ZREKLUKG7TSUET.json","graph_json":"https://pith.science/api/pith-number/66WSYNKWE6Y3ZREKLUKG7TSUET/graph.json","events_json":"https://pith.science/api/pith-number/66WSYNKWE6Y3ZREKLUKG7TSUET/events.json","paper":"https://pith.science/paper/66WSYNKW"},"agent_actions":{"view_html":"https://pith.science/pith/66WSYNKWE6Y3ZREKLUKG7TSUET","download_json":"https://pith.science/pith/66WSYNKWE6Y3ZREKLUKG7TSUET.json","view_paper":"https://pith.science/paper/66WSYNKW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1903.05336&json=true","fetch_graph":"https://pith.science/api/pith-number/66WSYNKWE6Y3ZREKLUKG7TSUET/graph.json","fetch_events":"https://pith.science/api/pith-number/66WSYNKWE6Y3ZREKLUKG7TSUET/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/66WSYNKWE6Y3ZREKLUKG7TSUET/action/timestamp_anchor","attest_storage":"https://pith.science/pith/66WSYNKWE6Y3ZREKLUKG7TSUET/action/storage_attestation","attest_author":"https://pith.science/pith/66WSYNKWE6Y3ZREKLUKG7TSUET/action/author_attestation","sign_citation":"https://pith.science/pith/66WSYNKWE6Y3ZREKLUKG7TSUET/action/citation_signature","submit_replication":"https://pith.science/pith/66WSYNKWE6Y3ZREKLUKG7TSUET/action/replication_record"}},"created_at":"2026-07-05T00:47:56.343651+00:00","updated_at":"2026-07-05T00:47:56.343651+00:00"}