Bose–Einstein condensation of atomic gases

By J. Anglin, W. Ketterle. Nature, 2002

614 citations recorded by the source corpus.

Subfields: Atomic and Molecular Physics, and Optics, Computational Mechanics

View Paper: https://www.semanticscholar.org/paper/0adfdce9adb3c21a39ab36a2c2fde4d9f0e950fa

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Citations in the corpus

Nobel lecture: When atoms behave as waves: Bose-Einstein condensation and the atom laser* (2002, background): “The history of the theory of BEC is very interesting, and is nicely described in the biographies of Einstein (Pais, 1982) and London (Gavroglu, 1995) and reviewed by Griffin (1999).”
Rotating trapped Bose-Einstein condensates (2008, background): “Typically, these systems have a macroscopic condensate wave function Ψ(r, t) that character- 2 izes the static and dynamic behavior of the BEC [for a general background, see, for example, Dalfovo et al. (1999); Inguscio et al. (1999); Pethick and Smith (2002); Pitaevskii and Stringari (2003)].”
Colloquium: Trapping and manipulating photon states in atomic ensembles (2003, background): “Spectacular manifestations ranging from experiments on ultracold atoms and matter waves [involving coherence of center-of-mass motion (Meystre, 2001; Anglin and Ketterle, 2002)] to generation of nonclassical light [involving quantum coherence of photon states (Walls and Milburn, 1994)] and coherent…”
A Multiscale Neural Network Based on Hierarchical Matrices (2018, methodology): “The nonlinear Schrödinger equation (NLSE) is widely used in quantum physics to describe the single particle properties of the Bose-Einstein condensation phenomenon [40, 2].”
Realization of Bose-Einstein condensates in lower dimensions. (2001, neutral): “…ξ = lt occurs if the number of condensate atoms becomes N1D = √ 32~ 225ma2 √ ω⊥ ω2z = √ ω⊥ ω2z × 7200 √ rad s (1) N2D = √ 32~ 225ma2 √ ω3z ω4 ⊥ = √ ω3z ω4 ⊥ × 7200 √ rad s , (2) where we have used the scattering length (a = 2.75 nm) and mass of 23Na atoms to derive the numerical factor.”
Ground-state solution of Bose--Einstein condensate by directly minimizing the energy functional (2003, neutral): “(23)Na used in MIT (group of Ketterle) with ωx = ωy >> ωz [8].”
Low-Disorder Microwave Cavity Lattices for Quantum Simulation with Photons (2012, methodology): “Two notable examples of the experiments with ultracold atomic gases are: observation of Bose-Einstein condensation [1, 4, 21] and observing a Mott insulator to superfluid phase transition [39].”
Thermally Induced Losses in Ultra-Cold Atoms Magnetically Trapped Near Room-Temperature Surfaces (2003, methodology): “This is done to minimize the heating effects of the Oort cloud.(19) Finally, the”