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13 Commits

Author SHA1 Message Date
ysyapa 8aa89fbf5f Added 1D system for testing 2023-04-08 20:01:23 -04:00
ysyapa ac540694d1 Minor bug fix 2023-04-08 18:56:53 -04:00
Nuwan Yapa a5cb029621 Adopt new interface 2023-04-07 22:41:53 -04:00
Nuwan Yapa a9098b3d65 Merge branch 'master' into debugging 2023-04-07 22:32:50 -04:00
ysyapa 3daddf7a9a Merge branch 'master' into debugging 2023-04-03 20:56:51 -04:00
ysyapa 94acb12d5f Store explicit H matrix in the memory and solve 2023-04-02 20:40:07 -04:00
ysyapa 677a09d680 Merge branch 'master' into debugging 2023-03-19 22:29:44 -04:00
ysyapa 0f53e4e719 Identified two discrepancies 2023-03-19 14:46:00 -04:00
ysyapa f7fc232d8b Check mean difference instead to sum 2023-03-18 17:29:05 -04:00
ysyapa f8e65bf498 Comparing with python calculation 2023-03-17 23:58:15 -04:00
ysyapa f281c6274c No images 2023-03-17 23:51:57 -04:00
ysyapa 17540a1a03 Write as byte file 2023-03-17 23:51:46 -04:00
ysyapa 0890f68d85 Write V diagonal values to a file 2023-03-17 22:43:33 -04:00
4 changed files with 302 additions and 0 deletions

51
V_dump.ipynb Normal file
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{
"cells": [
{
"cell_type": "code",
"execution_count": 2,
"metadata": {},
"outputs": [],
"source": [
"# ./En.run -d 3 -n 3 -e 5 -c eps=0 -c pot=v_gauss,v0=-4,r=2 -N 6 -L 5:14 -c n_imag=1\n",
"\n",
"include(\"common.jl\")\n",
"\n",
"T=Float32\n",
"\n",
"function V_test(r2::T)::T\n",
" return -4*exp(-r2/4)\n",
"end\n",
"\n",
"N=6\n",
"L::T=14.0\n",
"n_image=0\n",
"\n",
"V=calculate_Vs(V_test, 3, 3, N, L, n_image)\n",
"\n",
"outfile = \"temp/V_vals.dat\"\n",
"\n",
"open(outfile, \"w\") do f\n",
" for i in V\n",
" write(f, i)\n",
" end\n",
"end"
]
}
],
"metadata": {
"kernelspec": {
"display_name": "Julia 1.8.5",
"language": "julia",
"name": "julia-1.8"
},
"language_info": {
"file_extension": ".jl",
"mimetype": "application/julia",
"name": "julia",
"version": "1.8.5"
},
"orig_nbformat": 4
},
"nbformat": 4,
"nbformat_minor": 2
}

87
V_verify.ipynb Normal file
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{
"cells": [
{
"cell_type": "code",
"execution_count": null,
"metadata": {},
"outputs": [],
"source": [
"from itertools import chain\n",
"import numpy as np\n",
"import math\n",
"from scipy import sparse\n",
"from scipy.sparse.linalg import eigsh\n",
"\n",
"#sample potential\n",
"def V_gauss(dr_sqr):\n",
" return -4*math.exp(-dr_sqr/4)\n",
"\n",
"n=3 # no of particles\n",
"L=14\n",
"N=6 # no of lattice points\n",
"mu=1/2 # reduced mass\n",
"\n",
"DOF=(n-1)*3 # degrees of freedom after excluding CM\n",
"\n",
"s=np.arange(N**DOF) # matrix index\n",
"\n",
"# k index for each particle and each dimension\n",
"k=np.empty((n-1,3),dtype=np.dtype)\n",
"for dof in range(DOF):\n",
" k[dof//3,dof%3]=(s%N**(DOF-dof))//N**(DOF-1-dof)-N//2\n",
"\n",
"x=k*(L/N) # x coordinate from k index\n",
"\n",
"# adding up all non-local interactions\n",
"V_local=np.zeros(N**DOF)\n",
"\n",
"# 2-body interactions\n",
"V2=np.vectorize(V_gauss)\n",
"dxs=chain((x[i,:] for i in range(n-1)), (x[i,:]-x[j,:] for (i,j) in np.ndindex((n-1,n-1)) if i<j)) # with last particle + with each other\n",
"for dx in dxs:\n",
" dr_sqr=np.sum(dx*dx)\n",
" V_local+=V2(dr_sqr)"
]
},
{
"cell_type": "code",
"execution_count": null,
"metadata": {},
"outputs": [],
"source": [
"filename = \"temp/V_vals.dat\"\n",
"\n",
"with open(filename, 'br') as f:\n",
" buffer = f.read()\n",
"\n",
"V_julia = np.frombuffer(buffer, dtype=np.float32)\n",
"\n",
"abs_diff = np.abs(V_local-V_julia)\n",
"s = np.mean(abs_diff)\n",
"print(s)"
]
}
],
"metadata": {
"kernelspec": {
"display_name": "base",
"language": "python",
"name": "python3"
},
"language_info": {
"codemirror_mode": {
"name": "ipython",
"version": 3
},
"file_extension": ".py",
"mimetype": "text/x-python",
"name": "python",
"nbconvert_exporter": "python",
"pygments_lexer": "ipython3",
"version": "3.9.13"
},
"orig_nbformat": 4
},
"nbformat": 4,
"nbformat_minor": 2
}

42
mat_eig.jl Normal file
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include("Hamiltonian.jl")
T=Float32
function V_test(r2)
return -4 * exp(-r2 / 4)
end
d = 1
n = 3
N = 8
L::T = 16
n_imag = 0
μ::T = 0.5
H = HOperator{T}(V_test, d, n, N, L, μ, n_imag, cpu_tensor)
dim = N ^ (d * (n - 1))
H_mat = zeros(Complex{T}, dim, dim)
iter = CartesianIndices(vectorDims(H))
open("temp/mat_dump.csv", "w") do f
# this can be heavily optimized by getting rid of 'bi' vector
for i in 1 : dim
bi = zeros(Complex{T}, vectorDims(H)...)
bi[iter[i]] = 1
for j in 1 : dim
bj = zeros(Complex{T}, vectorDims(H)...)
bj[iter[j]] = 1
Hbj = similar(bj)
Hbj = mul!(Hbj, H, bj)
H_mat[i, j] = dot(bi, Hbj)
end
end
end
evals, _ = eigen(H_mat)
evals = real.(evals)
print(evals)

122
tester.ipynb Normal file
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{
"cells": [
{
"cell_type": "code",
"execution_count": null,
"metadata": {},
"outputs": [],
"source": [
"# ./En.run -d 3 -n 3 -e 5 -c pot=v_gauss,v0=-4,r=2 -N 8 -L 4 -c n_imag=0\n",
"# Calculating...\n",
"# -> N = 8\n",
"# -> L = 4\n",
"# -> Spectrum = {-6.07632,-3.81486,-3.71969,-3.71968,-3.38263}...\n",
"# Done.\n",
"# -> Time used = 12s\n",
"\n",
"include(\"Hamiltonian.jl\")\n",
"\n",
"T=Float32\n",
"\n",
"function V_test(r2)\n",
" return -4*exp(-r2/4)\n",
"end\n",
"\n",
"N=8\n",
"L::T=4\n",
"n_imag=0\n",
"\n",
"H=Hamiltonian{T}(V_test,3,3,N,L,convert(T,0),convert(T,0.5),n_imag,cpu_tensor)\n",
"@time evals,evecs,info=eig(H,5)\n",
"print(info.numops,\" operations : \")\n",
"println(evals)\n"
]
},
{
"cell_type": "code",
"execution_count": null,
"metadata": {},
"outputs": [],
"source": [
"# ./En.run -d 3 -n 3 -e 5 -c pot=v_gauss,v0=-4,r=2 -N 6 -L 14 -c n_imag=0\n",
"# Calculating...\n",
"# -> N = 6\n",
"# -> L = 14\n",
"# -> Spectrum = {-8.49538,-3.35492,-3.34356,-3.32830,-3.07909}...\n",
"# Done.\n",
"# -> Time used = 0.229049s\n",
"\n",
"include(\"Hamiltonian.jl\")\n",
"\n",
"T=Float32\n",
"\n",
"function V_test(r2)\n",
" return -4*exp(-r2/4)\n",
"end\n",
"\n",
"N=6\n",
"L::T=14\n",
"n_imag=0\n",
"\n",
"H=Hamiltonian{T}(V_test,3,3,N,L,convert(T,0),convert(T,0.5),n_imag,cpu_tensor)\n",
"@time evals,evecs,info=eig(H,5)\n",
"print(info.numops,\" operations : \")\n",
"println(evals)"
]
},
{
"cell_type": "code",
"execution_count": null,
"metadata": {},
"outputs": [],
"source": [
"# ./En.run -d 3 -n 3 -e 5 -c pot=v_gauss,v0=-4,r=2 -N 6 -L 14 -c n_imag=0\n",
"# Calculating...\n",
"# -> N = 6\n",
"# -> L = 14\n",
"# -> Spectrum = {-8.49538,-3.35492,-3.34356,-3.32830,-3.07909}...\n",
"# Done.\n",
"# -> Time used = 0.229049s\n",
"\n",
"include(\"Hamiltonian.jl\")\n",
"tolerance=1e-10\n",
"T=Float64\n",
"\n",
"function V_test(r2)\n",
" return -4*exp(-r2/4)\n",
"end\n",
"\n",
"N=4\n",
"L::T=16\n",
"n_imag=0\n",
"\n",
"H=Hamiltonian{T}(V_test,1,3,N,L,convert(T,0),convert(T,0.5),n_imag,cpu_tensor)\n",
"evals,evecs,info=eig(H,16)\n",
"display(evals)"
]
},
{
"cell_type": "code",
"execution_count": null,
"metadata": {},
"outputs": [],
"source": []
}
],
"metadata": {
"kernelspec": {
"display_name": "Julia 1.8.5",
"language": "julia",
"name": "julia-1.8"
},
"language_info": {
"file_extension": ".jl",
"mimetype": "application/julia",
"name": "julia",
"version": "1.8.5"
},
"orig_nbformat": 4
},
"nbformat": 4,
"nbformat_minor": 2
}