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Time-Dependent Superfluid Local Density Approximation
Quantum Gases · Submitted 10 Jan 2013
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Unlike linear response theory, which is only valid for weak external fields, the (TDSLDA) approach allows one to study non-linear excitations in fermionic superfluids, including large amplitude collective modes, and the response to strong external probes.
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The abstract, sentence by sentence
The time-dependent superfluid local density approximation (TDSLDA) is an extension of the Hohenberg-Kohn density functional theory (DFT) to time-dependent phenomena in superfluid fermionic systems. Unlike linear response theory, which is only valid for weak external fields, the (TDSLDA) approach allows one to study non-linear excitations in fermionic superfluids, including large amplitude collective modes, and the response to strong external probes. Even in the case of weak external fields, the (TDSLDA) approach is technically easier to implement. We will illustrate the implementation of the (TDSLDA) for the unitary Fermi gas, where dimensional arguments and Galilean invariance simplify the form of the functional, and ab initio input from (QMC) simulations fix the coefficients to quite high precision.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The time-dependent superfluid local density approximation (TDSLDA) is an extension of the Hohenberg-Kohn density functional theory (DFT) to time-dependent phenomena in superfluid fermionic systems. | background 0.68 | 0.11 | 0.09 | asserted 1.00 |
| s1 | Unlike linear response theory, which is only valid for weak external fields, the (TDSLDA) approach allows one to study non-linear excitations in fermionic superfluids, including large amplitude collective modes, and the response to strong external probes. | contribution 0.38 | 0.15 | 0.20 | asserted 0.98 |
| s2 | Even in the case of weak external fields, the (TDSLDA) approach is technically easier to implement. | background 0.34 | 0.26 | 0.07 | asserted 1.00 |
| s3 | We will illustrate the implementation of the (TDSLDA) for the unitary Fermi gas, where dimensional arguments and Galilean invariance simplify the form of the functional, and ab initio input from (QMC) simulations fix the coefficients to quite high precision. | method 0.51 | 0.80 | 0.11 | asserted 0.97 |
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The paper
Original abstract
The time-dependent superfluid local density approximation (TDSLDA) is an extension of the Hohenberg-Kohn density functional theory (DFT) to time-dependent phenomena in superfluid fermionic systems. Unlike linear response theory, which is only valid for weak external fields, the (TDSLDA) approach allows one to study non-linear excitations in fermionic superfluids, including large amplitude collective modes, and the response to strong external probes. Even in the case of weak external fields, the (TDSLDA) approach is technically easier to implement. We will illustrate the implementation of the (TDSLDA) for the unitary Fermi gas, where dimensional arguments and Galilean invariance simplify the form of the functional, and ab initio input from (QMC) simulations fix the coefficients to quite high precision.
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How the literature uses it
1 arXiv paper cite this in 2 sentences
Papers citing it
Cites it as background 1 paper
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TDSLDA The time-dependent generalization of the SLDA (TDSLDA) provides a model for directly studying time-dependent phenomena in the UFG (see [ref] for a review).
Validating Simple Dynamical Simulations of the Unitary Fermi Gas · Introduction · 0.97
What it cites · 7 sentences without a confident label
Uses the method or tool of 3 papers
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The homogeneous equations can then be used to translate this into a position dependent $Λ(r)$ that may be used in the previous equations and which has very good convergence properties [ref] (see also [ref] ):
The Unitary Fermi Gas: From Monte Carlo to Density Functionals · The Functional · 0.84
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The homogeneous equations can then be used to translate this into a position dependent $Λ(r)$ that may be used in the previous equations and which has very good convergence properties [ref] (see also [ref] ):
Renormalization of the Hartree-Fock-Bogoliubov Equations in the Case of a Zero Range Pairing Interaction · The Functional · 0.84
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As a result, a memory limited implementation of Broyden's method [ref] works well to accelerate convergence, thereby determining equilibrium configurations to use as an initial state for a subsequent time-dependent simulation.
Broyden's Method in Nuclear Structure Calculations · Technical Notes · 0.95
Cites as background 2 papers
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Although exact in principle, there is no simple prescription for computing an exact density functional in a non-perturbative theory (see [ref] for recent discussions), and one must first formulate an approximate functional that captures the relevant physics.
Toward ab initio density functional theory for nuclei · Introduction · 0.87
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In nuclear physics Galilean invariance have been considered for quite some time [ref] , and the contribution of these currents is often essential for describing the properties of excited states.
TDDFT with Skyrme Forces: Effect of Time-Odd Densities on Electric Giant Resonances · The Functional · 0.87
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