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import matscipy | |
import numpy as np | |
import ase | |
from ase import Atoms | |
from ase.calculators.lj import LennardJones | |
# set up a heptamer | |
r0 = 1.0 | |
N = 6 | |
phi = np.linspace(0., (N-1)* 2*np.pi/N, N) |
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using JuLIP, JuLIP.ASE, JuLIP.Potentials | |
using ProgressMeter | |
# set up a heptamer | |
r0 = 1.0 | |
N = 6 | |
phi = linspace(0., (N-1)* 2*pi/N, N)|>collect | |
x0 = 2.5 # position of center | |
y0 = 2.5 | |
x = x0 + [0; r0 * cos.(phi)] |
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# benchmarking different ways to implement AnalyticPotential, | |
# in order to circumvent the World Age problem | |
using MacroTools | |
using BenchmarkTools | |
using Calculus: differentiate | |
using FunctionWrappers: FunctionWrapper | |
const F64fun = FunctionWrapper{Float64, Tuple{Float64}} |
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from numpy import * | |
import atomistica | |
from ase.atoms import * | |
X=array([1.42588,-3.44239,0.0,2.73662,-1.97199,1.3575,1.28782,-0.724414,2.715,2.59344,0.745918,4.0725,4.18105,-3.22103,2.715,5.49312,-1.74281,4.0725,4.04571,-0.49763,0.0,5.35298,0.981145,1.3575,1.1371,1.98901,0.0,2.43615,3.45883,1.3575,0.9722,4.69833,2.715,2.263,6.16731,4.0725,3.89681,2.22019,2.715,5.1976,3.69884,4.0725,3.73204,4.93248,0.0,5.02423,6.41037,1.3575,0.792067,7.40456,0.0,2.07289,8.87273,1.3575,0.596638,10.1094,2.715,1.86617,11.5773,4.0725,3.54938,7.64001,2.715,4.8305,9.11683,4.0725,3.34779,10.3446,0.0,4.61557,11.8207,1.3575,0.387448,12.8151,0.0,1.64536,14.2836,1.3575,0.168044,15.524,2.715,1.41555,16.9944,4.0725,3.12829,13.0491,2.715,4.38163,14.5256,4.0725,2.8949,15.7567,0.0,4.13502,17.2353,1.3575,0.0561522,25.2023,0.0,1.53117,26.4442,1.3575,0.278721,27.9135,2.715,1.75727,29.1525,4.0725,2.77516,24.9699,2.715,4.25935,26.2028,4.0725,3.01295,27.6802,0.0,4.50068,28.9098,1.3575,0.493591,30.6205,0.0,1.97151,31.8576,1.3575,0.696213,33.3255,2.71 |
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# | |
# Test performance of FunctionWrappers.jl | |
# | |
f1(r) = exp(3.0*r) | |
f2(r) = cos(7*r)^2 | |
# N evaluates of sin, cos; hard-coded | |
function test1(N) |