Spin-1 spin-orbit- and Rabi-coupled Bose-Einstein condensate solver
| Autor: | Dušan Vudragović, Sadhan K. Adhikari, Rajamanickam Ravisankar, Antun Balaž, Paulsamy Muruganandam |
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| Přispěvatelé: | Tiruchirappalli 620024, Pregrevica 118, Universidade Estadual Paulista (Unesp) |
| Rok vydání: | 2020 |
| Předmět: |
Fortran
General Physics and Astronomy FOS: Physical sciences Pattern Formation and Solitons (nlin.PS) 01 natural sciences Split-step Crank–Nicolson scheme 010305 fluids & plasmas law.invention law 0103 physical sciences 010306 general physics Wave function computer.programming_language Physics Condensed Matter::Quantum Gases Quantum Physics Partial differential equation Mathematical analysis Spinor Bose–Einstein condensate Function (mathematics) Solver Computational Physics (physics.comp-ph) Nonlinear Sciences - Pattern Formation and Solitons Gross–Pitaevskii equation Hardware and Architecture Quantum Gases (cond-mat.quant-gas) FORTRAN programs Spin–orbit coupling Condensed Matter - Quantum Gases Quantum Physics (quant-ph) computer Physics - Computational Physics Bose–Einstein condensate Stationary state |
| Zdroj: | Scopus Repositório Institucional da UNESP Universidade Estadual Paulista (UNESP) instacron:UNESP |
| DOI: | 10.48550/arxiv.2009.13507 |
| Popis: | We present OpenMP versions of FORTRAN programs for solving the Gross-Pitaevskii equation for a harmonically trapped three-component spin-1 spinor Bose-Einstein condensate (BEC) in one (1D) and two (2D) spatial dimensions with or without spin-orbit (SO) and Rabi couplings. Several different forms of SO coupling are included in the programs. We use the split-step Crank-Nicolson discretization for imaginary- and real-time propagation to calculate stationary states and BEC dynamics, respectively. The imaginary-time propagation programs calculate the lowest-energy stationary state. The real-time propagation programs can be used to study the dynamics. The simulation input parameters are provided at the beginning of each program. The programs propagate the condensate wave function and calculate several relevant physical quantities. Outputs of the programs include the wave function, energy, root-mean-square sizes, different density profiles (linear density for the 1D program, linear and surface densities for the 2D program). The imaginary- or real-time propagation can start with an analytic wave function or a pre-calculated numerical wave function. The imaginary-time propagation usually starts with an analytic wave function, while the real-time propagation is often initiated with the previously calculated converged imaginary-time wave function. Comment: 15 pages, 4 figures; programs can be downloaded at https://doi.org/10.17632/j3wr4wn946.1 |
| Databáze: | OpenAIRE |
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