2019
DOI: 10.1002/zamm.201700370
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Sufficient conditions of collapse for dipolar Bose‐Einstein condensate

Abstract: This paper investigates dipolar Bose‐Einstein condensate modeled by the Gross‐Pitaevskii equation with harmonic confinement and dipolar interaction potential. With the help of a new estimate of the kinetic energy as well as a mechanical analogy, the known results of collapse[14] have been extended to a new ample condition for the existence of blowup solutions.

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Cited by 4 publications
(3 citation statements)
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References 23 publications
(38 reference statements)
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“…where ψ(x, t) is the complex wave envelope, |ψ(x, t)| 2 is the atomic density; g = 4π 2 N a m with the Planck constant , the total number of particles N ∈ N, the mass of single particle m > 0, the scattering length a ∈ R that can be adjusted to be positive or negative in the course of experiment; the external potential V ext represents the electromagnetic trap for the condensation [33].…”
Section: Option Pricing Model Of Quantum Originmentioning
confidence: 99%
“…where ψ(x, t) is the complex wave envelope, |ψ(x, t)| 2 is the atomic density; g = 4π 2 N a m with the Planck constant , the total number of particles N ∈ N, the mass of single particle m > 0, the scattering length a ∈ R that can be adjusted to be positive or negative in the course of experiment; the external potential V ext represents the electromagnetic trap for the condensation [33].…”
Section: Option Pricing Model Of Quantum Originmentioning
confidence: 99%
“…Next, we give the expression of the singular operator P, P x and Q, Q x under the new coordinate. It comes from (30) that…”
Section: An Associated Semilinear Systemmentioning
confidence: 99%
“…In addition, the researcher in [25] utilized Lagrangian coordinates to extend the previous results through lowering the common condition of the initial value for the D-G-H equation to the class of continuous differential periodic initial value, i.e., for any u 0 ∈ C 1 (R), there is some T(u 0 ) > 0 and a unique solution u ∈ C([0, T); C 1 (R)) ∩ C 1 ([0, T); C(R)). Such method is also succeeded in proving the periodic the C-H equation that lives up to the least action principle [26,27] and giving the threshold for global existence and blowup solutions [28][29][30]. Regarding the conservative solution of the C-H equation [1,31,32], Bressan and Constantin transferred the equation to the ODE system at first, in terms of a set of variables.…”
Section: Introductionmentioning
confidence: 99%