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In this paper, we present a minimisation method for computing the ground state of systems of coupled Gross Pitaevskii equations.
Both BESP and BFSP are spectral order accurate for computing the ground and first excited states in BEC.
In this section, we will propose an implicit numerical method for computing the ground states of a dipolar BEC.
There are various numerical methods proposed in literatures for computing the ground states of BEC [8, 9, 16 19].
A numerical method for computing the ground state solution of Bose Einstein condensates modeled by the Gross Pitaevskii equation is presented.
Extensive numerical examples in 3D are reported to demonstrate the efficiency and accuracy of our new numerical methods for computing the ground states and dynamics of dipolar BECs.
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We present a novel algorithm for computing the ground-state and excited-state solutions of M-coupled nonlinear Schrödinger equations (MCNLS).
FEM was used in [7] for computing the grounding grid resistance.
For example, grounded semantics can easily be specified in this formalism using a QBF, but computing the grounded extension can be done using an algorithm with polynomial running time.
To compute the ground state, an imaginary time method is adopted [14].
The backward Euler method in time and the sine spectral method in space are proposed to compute the ground states.
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