{"arxiv_id":"1305.6891","incoming":{"papers":6,"sentences":12,"groups":[{"kind":"extends","label":"Builds on it","papers":1,"sentences":1,"quotes":[{"arxiv_id":"2512.12866","title":"Local Quantum Cooling for Large Fermi Systems with Pairing","url":"/paper/2512.12866","section":"Introduction.","sentence":"This was the idea behind the LQF algorithm [ref] , which we extend here to the pairing channel.","intent_p":1.0,"contests_p":null}]},{"kind":"method_or_tool","label":"Uses its method or tool","papers":2,"sentences":3,"quotes":[{"arxiv_id":"1711.05803","title":"Suppressed solitonic cascade in spin-imbalanced superfluid Fermi gas","url":"/paper/1711.05803","section":"Initial state preparation","sentence":"Instead of solving ASLDA equations in 3D, which is prohibitively expensive, we followed a different strategy presented in [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"1302.2172","title":"Strength of the Vortex-Pinning Interaction from Real-Time Dynamics","url":"/paper/1302.2172","section":"Introduction","sentence":"The adiabatic state preparation can be significantly accelerated by introducing a “quantum friction” term to remove phonon noise [ref] .","intent_p":0.92,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites it as support","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1805.08908","title":"Unitary evolution with fluctuations and dissipation","url":"/paper/1805.08908","section":"Introduction","sentence":"The term $γ[n]ṅ∝- ∇·p(r,t)$, per continuity equation [ref] , plays the role of “quantum friction”, in which the “friction coefficient” $γ[n]$ can depend on the number density and/or its gradient, etc. and thus it can simulate volume and/or surface \"friction.\" In the presence of this “quantum friction” term alone $Ė_tot(t)≤0$ and $lim_t→∞ v(r,t)= 0$ [ref] , similarly to the classical Langevin equation.","intent_p":0.96,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1912.11069","title":"Dynamics of one-dimensional correlated nuclear systems within non-equilibrium Green's function theory","url":"/paper/1912.11069","section":"Preparing finite correlated nuclear systems","sentence":"The effects of a cooling friction during switching have been studied previously [ref] .","intent_p":0.91,"contests_p":null}]}],"unlabelled_sentences":6},"outgoing":{"papers":10,"sentences":17,"groups":[{"kind":"method_or_tool","label":"Uses the method or tool of","papers":4,"sentences":4,"quotes":[{"arxiv_id":"1008.3933","title":"The Unitary Fermi Gas: From Monte Carlo to Density Functionals","url":"/paper/1008.3933","section":"Introduction","sentence":"In the final example, we demonstrate local quantum friction applied to a large-scale TDDFT simulation modeling the unitary Fermi gas with the TDSLDA [ref] .","intent_p":0.83,"contests_p":null},{"arxiv_id":"1108.1779","title":"Quantum Shock Waves and Domain Walls in the Real-Time Dynamics of a Superfluid Unitary Fermi Gas","url":"/paper/1108.1779","section":"Introduction","sentence":"In the final example, we demonstrate local quantum friction applied to a large-scale TDDFT simulation modeling the unitary Fermi gas with the TDSLDA [ref] .","intent_p":0.83,"contests_p":null},{"arxiv_id":"1301.0357","title":"Time-Dependent Density Functional Theory and the Real-Time Dynamics of Fermi Superfluids","url":"/paper/1301.0357","section":"Introduction","sentence":"In the final example, we demonstrate local quantum friction applied to a large-scale TDDFT simulation modeling the unitary Fermi gas with the TDSLDA [ref] .","intent_p":0.83,"contests_p":null},{"arxiv_id":"1301.7354","title":"Use of the Discrete Variable Representation Basis in Nuclear Physics","url":"/paper/1301.7354","section":"Introduction","sentence":"We discretize the Schrödinger equation using the discrete variable representation (DVR) technique described in Ref. [ref] on a $32^3$ spatial lattice.","intent_p":0.99,"contests_p":null}]},{"kind":"background","label":"Cites as background","papers":1,"sentences":1,"quotes":[{"arxiv_id":"0904.2706","title":"Laser-driven nonlinear cluster dynamics","url":"/paper/0904.2706","section":"Introduction","sentence":"DFT and its time-dependent extension TDDFT, see e.g. [ref] , provide a unified approach to study both structure and reactions (dynamics).","intent_p":0.93,"contests_p":null}]}],"unlabelled_sentences":12},"claims":[],"thresholds":{"intent_p":0.8,"supports_p":0.95,"contests_p":0.7},"method":"Citing sentences come from each paper's LaTeX source; every \\cite marks the sentence and the works it cites. Pith's classifier typed each sentence. A label is shown at intent probability 0.8 or more (0.95 for support), a contest at 0.7 or more. Measured accuracy against two blind model families is at https://pith.science/accuracy. The quoted sentences are the citing authors' own.","held_up":null,"_links":{"html":"https://pith.science/paper/1305.6891"}}