{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:EP46KGOZESPC3DWGL74TNH4GGK","short_pith_number":"pith:EP46KGOZ","schema_version":"1.0","canonical_sha256":"23f9e519d9249e2d8ec65ff9369f8632a3f0418f805938d1b92394a25118cbc9","source":{"kind":"arxiv","id":"1604.00865","version":2},"attestation_state":"computed","paper":{"title":"Phase Transitions in a Bose-Hubbard Model with Cavity-Mediated Global-Range Interactions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.quant-gas","authors_text":"F. Brennecke, N. Dogra, S.D. Huber, T. Donner","submitted_at":"2016-04-04T14:10:08Z","abstract_excerpt":"We study a system with competing short- and global-range interactions in the framework of the Bose-Hubbard model. Using a mean-field approximation we obtain the phase diagram of the system and observe four different phases: a superfluid, a supersolid, a Mott insulator and a charge density wave, where the transitions between the various phases can be either of first or second order. We qualitatively support these results using Monte-Carlo simulations. An analysis of the low-energy excitations shows that the second-order phase transition from the charge density wave to the supersolid is associat"},"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":"1604.00865","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2016-04-04T14:10:08Z","cross_cats_sorted":[],"title_canon_sha256":"a3523dc245432d119ccfe98c78717936cf8c78fa0ad0eb2b99498a45b09b120f","abstract_canon_sha256":"9a6a7b6f9212b75093a07fff224b500d1e5d7c94231afde0f86d0e57672e361b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:03:26.648224Z","signature_b64":"uGmnQ3wmV5035BJXLCHUGs73f+dC6NGCWftwas8AmUQBCj8AWXnyOdL3PR8v4VZQGxP1gNyHkuz2bfJ9VzFsCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"23f9e519d9249e2d8ec65ff9369f8632a3f0418f805938d1b92394a25118cbc9","last_reissued_at":"2026-05-18T01:03:26.647681Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:03:26.647681Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Phase Transitions in a Bose-Hubbard Model with Cavity-Mediated Global-Range Interactions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.quant-gas","authors_text":"F. Brennecke, N. Dogra, S.D. Huber, T. Donner","submitted_at":"2016-04-04T14:10:08Z","abstract_excerpt":"We study a system with competing short- and global-range interactions in the framework of the Bose-Hubbard model. Using a mean-field approximation we obtain the phase diagram of the system and observe four different phases: a superfluid, a supersolid, a Mott insulator and a charge density wave, where the transitions between the various phases can be either of first or second order. We qualitatively support these results using Monte-Carlo simulations. An analysis of the low-energy excitations shows that the second-order phase transition from the charge density wave to the supersolid is associat"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.00865","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":"1604.00865","created_at":"2026-05-18T01:03:26.647761+00:00"},{"alias_kind":"arxiv_version","alias_value":"1604.00865v2","created_at":"2026-05-18T01:03:26.647761+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.00865","created_at":"2026-05-18T01:03:26.647761+00:00"},{"alias_kind":"pith_short_12","alias_value":"EP46KGOZESPC","created_at":"2026-05-18T12:30:12.583610+00:00"},{"alias_kind":"pith_short_16","alias_value":"EP46KGOZESPC3DWG","created_at":"2026-05-18T12:30:12.583610+00:00"},{"alias_kind":"pith_short_8","alias_value":"EP46KGOZ","created_at":"2026-05-18T12:30:12.583610+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/EP46KGOZESPC3DWGL74TNH4GGK","json":"https://pith.science/pith/EP46KGOZESPC3DWGL74TNH4GGK.json","graph_json":"https://pith.science/api/pith-number/EP46KGOZESPC3DWGL74TNH4GGK/graph.json","events_json":"https://pith.science/api/pith-number/EP46KGOZESPC3DWGL74TNH4GGK/events.json","paper":"https://pith.science/paper/EP46KGOZ"},"agent_actions":{"view_html":"https://pith.science/pith/EP46KGOZESPC3DWGL74TNH4GGK","download_json":"https://pith.science/pith/EP46KGOZESPC3DWGL74TNH4GGK.json","view_paper":"https://pith.science/paper/EP46KGOZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1604.00865&json=true","fetch_graph":"https://pith.science/api/pith-number/EP46KGOZESPC3DWGL74TNH4GGK/graph.json","fetch_events":"https://pith.science/api/pith-number/EP46KGOZESPC3DWGL74TNH4GGK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EP46KGOZESPC3DWGL74TNH4GGK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EP46KGOZESPC3DWGL74TNH4GGK/action/storage_attestation","attest_author":"https://pith.science/pith/EP46KGOZESPC3DWGL74TNH4GGK/action/author_attestation","sign_citation":"https://pith.science/pith/EP46KGOZESPC3DWGL74TNH4GGK/action/citation_signature","submit_replication":"https://pith.science/pith/EP46KGOZESPC3DWGL74TNH4GGK/action/replication_record"}},"created_at":"2026-05-18T01:03:26.647761+00:00","updated_at":"2026-05-18T01:03:26.647761+00:00"}