{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:EVE4QHHSCQ2SPBIPUCCPHQMUFJ","short_pith_number":"pith:EVE4QHHS","schema_version":"1.0","canonical_sha256":"2549c81cf2143527850fa084f3c1942a532aba205b543f28efdbf0632faca437","source":{"kind":"arxiv","id":"1802.04088","version":2},"attestation_state":"computed","paper":{"title":"On the number of Bose-selected modes in driven-dissipative ideal Bose gases","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","quant-ph"],"primary_cat":"cond-mat.quant-gas","authors_text":"Alexander Schnell, Andr\\'e Eckardt, Roland Ketzmerick","submitted_at":"2018-02-12T14:57:54Z","abstract_excerpt":"In an ideal Bose gas that is driven into a steady state far from thermal equilibrium, a generalized form of Bose condensation can occur. Namely, the single-particle states unambiguously separate into two groups: the group of Bose-selected states, whose occupations increase linearly with the total particle number, and the group of all other states whose occupations saturate [Phys. Rev. Lett. 111, 240405 (2013)]. However, so far very little is known about how the number of Bose-selected states depends on the properties of the system and its coupling to the environment. The answer to this questio"},"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":"1802.04088","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2018-02-12T14:57:54Z","cross_cats_sorted":["cond-mat.stat-mech","quant-ph"],"title_canon_sha256":"de75d712ac978fbc0173048e01f7dba5935b6039a0cd46450956272a03f44a9f","abstract_canon_sha256":"4975f2bb0e97666b87bf131f673cf59e21ab625e10d4581e6c181e6370dadaea"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:19:56.403407Z","signature_b64":"enibEiM0ekVXzNs6Ac3VcgQsQFn+aP498VZml/dEiCdnhLuYFVRYyj+0M04gj621wYlzORLNqA9lMZBDSfdzCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2549c81cf2143527850fa084f3c1942a532aba205b543f28efdbf0632faca437","last_reissued_at":"2026-05-18T00:19:56.402825Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:19:56.402825Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"On the number of Bose-selected modes in driven-dissipative ideal Bose gases","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","quant-ph"],"primary_cat":"cond-mat.quant-gas","authors_text":"Alexander Schnell, Andr\\'e Eckardt, Roland Ketzmerick","submitted_at":"2018-02-12T14:57:54Z","abstract_excerpt":"In an ideal Bose gas that is driven into a steady state far from thermal equilibrium, a generalized form of Bose condensation can occur. Namely, the single-particle states unambiguously separate into two groups: the group of Bose-selected states, whose occupations increase linearly with the total particle number, and the group of all other states whose occupations saturate [Phys. Rev. Lett. 111, 240405 (2013)]. However, so far very little is known about how the number of Bose-selected states depends on the properties of the system and its coupling to the environment. The answer to this questio"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1802.04088","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":"1802.04088","created_at":"2026-05-18T00:19:56.402923+00:00"},{"alias_kind":"arxiv_version","alias_value":"1802.04088v2","created_at":"2026-05-18T00:19:56.402923+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1802.04088","created_at":"2026-05-18T00:19:56.402923+00:00"},{"alias_kind":"pith_short_12","alias_value":"EVE4QHHSCQ2S","created_at":"2026-05-18T12:32:22.470017+00:00"},{"alias_kind":"pith_short_16","alias_value":"EVE4QHHSCQ2SPBIP","created_at":"2026-05-18T12:32:22.470017+00:00"},{"alias_kind":"pith_short_8","alias_value":"EVE4QHHS","created_at":"2026-05-18T12:32:22.470017+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/EVE4QHHSCQ2SPBIPUCCPHQMUFJ","json":"https://pith.science/pith/EVE4QHHSCQ2SPBIPUCCPHQMUFJ.json","graph_json":"https://pith.science/api/pith-number/EVE4QHHSCQ2SPBIPUCCPHQMUFJ/graph.json","events_json":"https://pith.science/api/pith-number/EVE4QHHSCQ2SPBIPUCCPHQMUFJ/events.json","paper":"https://pith.science/paper/EVE4QHHS"},"agent_actions":{"view_html":"https://pith.science/pith/EVE4QHHSCQ2SPBIPUCCPHQMUFJ","download_json":"https://pith.science/pith/EVE4QHHSCQ2SPBIPUCCPHQMUFJ.json","view_paper":"https://pith.science/paper/EVE4QHHS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1802.04088&json=true","fetch_graph":"https://pith.science/api/pith-number/EVE4QHHSCQ2SPBIPUCCPHQMUFJ/graph.json","fetch_events":"https://pith.science/api/pith-number/EVE4QHHSCQ2SPBIPUCCPHQMUFJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EVE4QHHSCQ2SPBIPUCCPHQMUFJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EVE4QHHSCQ2SPBIPUCCPHQMUFJ/action/storage_attestation","attest_author":"https://pith.science/pith/EVE4QHHSCQ2SPBIPUCCPHQMUFJ/action/author_attestation","sign_citation":"https://pith.science/pith/EVE4QHHSCQ2SPBIPUCCPHQMUFJ/action/citation_signature","submit_replication":"https://pith.science/pith/EVE4QHHSCQ2SPBIPUCCPHQMUFJ/action/replication_record"}},"created_at":"2026-05-18T00:19:56.402923+00:00","updated_at":"2026-05-18T00:19:56.402923+00:00"}