{"record":{"author":{"account_ref":null,"orcid":null},"builds_on":[],"content_schema":"pubphys.content.revision/1","content_sha256":"f583ddb051454433ebe40f5337830f7ae185803b906d0b15698ea2367809fcdc","created":"2026-10-03T07:17:53Z","files":[],"origin":{"assisted_by":[],"kind":"seed"},"parents":["5475cf5dc5b1a72283d26dc95dc6e00d7ea4e00096a7c6492e409a1816eeb011"],"salt":"705f2c6f851ce282ed3031bbe6eaeda1066f4f5e51241bfa0cc2a3b7f5e640ba","schema":"pubphys.record/2","site":"pubphys.com","target":null,"type":"revision"},"content":{"answer_type":"value","assisted_by":[],"external_id":"amo.hubbard-simulation.doped-entropy-floor","kind":"well-posed","literature_status":"open","n":"1","parents":[],"plain":"Pairing in the Hubbard model needs very cold atoms, and the best experiments reached their coldest temperatures only at half filling, one atom per site. The question is how cold a doped sample with holes can be made, and what stops further cooling.","posed_since":"","precise":"Homogeneous (flat-bottom) 2D square-lattice Fermi-Hubbard sample with at least 100 sites, $U/t = 8$, hole doping $\\delta = 0.1\\ \\text{to}\\ 0.2$. Determine the minimum entropy per site $s_{\\mathrm{min}}$ (units of $k_{B}$) and temperature $T/t$ reachable by entropy redistribution into reservoirs and adiabatic loading, with independent thermometry, and identify the limiting heating processes (lattice-light scattering, technical noise, reservoir capacity). Answer: $s_{\\mathrm{min}}$ and $T/t$ in the doped region with an error budget, and whether $T/t < 0.05$ is reachable at $\\delta = 0.125$.","problem_ref":null,"references":"","settled_by":"A doped homogeneous sample with thermometry validated against finite-temperature numerics, plus a measured heating budget.","status_note":"A 2025 experiment reached $T/t = 0.05 (+0.06/-0.05)$ at half filling by entropy redistribution (Xu et al., Nature 642, 909, arXiv:2502.00095).","title":"Lowest entropy per site reachable in a doped homogeneous Hubbard sample","topic_ref":"3900d87db48f0080fb068d283e110f5923dafb6ad85daaf4e53a292a8a9304ef"},"attested":{"attestation":{"batch":null,"client_id":null,"id_token_sha256":null,"kind":"platform"},"record_hash":"f1754c92b010a70d32976ca358aff734bf0391f3b1de380b48340927eda5a08a","schema":"pubphys.attested/1"},"envelope":{"attested_hash":"c7ad7f805b4f7eccb51f1f310f81c87b7034eb13deba5ef792782323e01a7576","platform_signature":{"key_id":"c6afc19b31429869751f06879c75cd64ea92654423d15b44be775bf1310a60da","sig":"dQ-TOPb83CWy4zYAZrVoVyWkmZoFqESduvhUpZxpHkyZwOg7NqatDwLJSlbroUh3UbyyTWuOtDyn7nhJKQnMBA"},"schema":"pubphys.envelope/1"},"record_hash":"f1754c92b010a70d32976ca358aff734bf0391f3b1de380b48340927eda5a08a","leaf_index":414}