-
Notifications
You must be signed in to change notification settings - Fork 62
/
3dharmonic.cc
207 lines (168 loc) · 7.16 KB
/
3dharmonic.cc
1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
16
17
18
19
20
21
22
23
24
25
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
51
52
53
54
55
56
57
58
59
60
61
62
63
64
65
66
67
68
69
70
71
72
73
74
75
76
77
78
79
80
81
82
83
84
85
86
87
88
89
90
91
92
93
94
95
96
97
98
99
100
101
102
103
104
105
106
107
108
109
110
111
112
113
114
115
116
117
118
119
120
121
122
123
124
125
126
127
128
129
130
131
132
133
134
135
136
137
138
139
140
141
142
143
144
145
146
147
148
149
150
151
152
153
154
155
156
157
158
159
160
161
162
163
164
165
166
167
168
169
170
171
172
173
174
175
176
177
178
179
180
181
182
183
184
185
186
187
188
189
190
191
192
193
194
195
196
197
198
199
200
201
202
203
204
205
206
207
/*
This file is part of MADNESS.
Copyright (C) 2007,2010 Oak Ridge National Laboratory
This program is free software; you can redistribute it and/or modify
it under the terms of the GNU General Public License as published by
the Free Software Foundation; either version 2 of the License, or
(at your option) any later version.
This program is distributed in the hope that it will be useful,
but WITHOUT ANY WARRANTY; without even the implied warranty of
MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the
GNU General Public License for more details.
You should have received a copy of the GNU General Public License
along with this program; if not, write to the Free Software
Foundation, Inc., 59 Temple Place, Suite 330, Boston, MA 02111-1307 USA
For more information please contact:
Robert J. Harrison
Oak Ridge National Laboratory
One Bethel Valley Road
P.O. Box 2008, MS-6367
email: harrisonrj@ornl.gov
tel: 865-241-3937
fax: 865-572-0680
$Id$
*/
/*!
\file examples/3dharmonic.cc
\brief Solves for the ground state of the quantum 3d harmonic oscillator
\defgroup example3dharm Solves the 3D harmonic oscillator
\ingroup examples
The source is <a href=https://github.com/m-a-d-n-e-s-s/madness/blob/master/src/examples/3dharmonic.cc>here</a>.
\par Points of interest
- convolution with the Green's function
- need to adjust the zero of energy to use the bound-state Green's function
- failure of simple fixed-point iteration
- use of simple non-linear equation solver
- plotting 3D function along a line
\par Background
We seek the ground state of the 3D Schrodinger equation
\f[
\left( -\frac{1}{2} \nabla^2 + V(r) \right) \psi(r) = E \psi(r)
\f]
with
\f[
V(r) = \frac{1}{2} |r|^2
\f]
As usual, we rewrite the differential equation into integral form
\f[
\psi(r) = \left( -\frac{1}{2} \nabla^2 - E \right)^{-1} V(r) \psi(r)
\f]
but unfortunately we are left with two problems.
First, recall that application
of the inverse of the differential operator corresponds to convolution
with the Green's function to the Helmholtz equation that satisfies
\f[
\left(-\nabla^2 + \mu^2 \right) G(r,r'; \mu) = \delta(r-r')
\f]
In 3D, we have
\f[
G(r,r'; \mu) = \frac{e^{-\mu |r-r'|}}{4 \pi |r-r|}
\f]
that MADNESS can currently only apply efficiently for real \f$\mu\f$ and since
\f$\mu = \sqrt{-2 E}\f$ only for negative energies (hence bound
states). But for the harmonic oscillator there are no free particle
states and the zero of energy is not chosen to describe the lowest
energy of a free particle but simply as the zero of potential
energy. To solve this problem we can shift the zero of energy down
by subtracting a constant (\f$\Delta\f$) from both sides of the
equation, hence making the effective ground state energy negative.
\f[
\psi(r) = \left( -\frac{1}{2} \nabla^2 - E + \Delta \right)^{-1} \left( V(r) -\Delta\right) \psi(r)
\f]
How negative do we need to make the energy? To answer this we need
to discuss the second problem. The fixed-point iteration described
by the integral equation only reliably converges to the ground state
if the potential is negative everywhere the wave function is
significant. The exact solution is
\f$\psi(r)=\pi^{-1/4}\exp(-r^2 / 2)\f$ (with $E=$1.5) that
becomes 1e-6 (but how small is small enough?) at \f$r=5.3\f$ where
\f$V\f$ is 14.0. So let's take this as the value of \f$\Delta\f$ and
try the fixed point iteration. Bad news. It starts converging
(slowly) to the right answer but then diverges and even damping
(step restriction) does not solve the problem. We have to make the
shift large enough to make the potential negative in the entire
volume to avoid the divergence, but this makes the convergence
really slow.
The fix is to not rely upon the simple fixed point iteration but to
use an equation solver to force convergence. This also enables us
to choose the size of the shift to optimize the rate of convergence
(empirically \f$\Delta=7\f$ is best) rather than being forced to
pick a large value. We use the very easy to use solver in
mra/nonlinsol.h .
[Aside. It is possible to apply the operator for positive energies,
but efficient application requires separate treatment of the
singular and the long-range oscillatory terms, and the latter is
presently not a production capability of MADNESS. If you need this,
let us know.]
*/
#include <madness/mra/mra.h>
#include <madness/mra/funcplot.h>
#include <madness/mra/nonlinsol.h>
using namespace madness;
const double L = 7.0;
//const double DELTA = 3*L*L/2; // Use this to make fixed-point iteration converge
const double DELTA = 7.0;
// The initial guess wave function
double guess(const coord_3d& r) {
return exp(-(r[0]*r[0]+r[1]*r[1]+r[2]*r[2])/3.0);
}
// The shifted potential
double potential(const coord_3d& r) {
return 0.5*(r[0]*r[0]+r[1]*r[1]+r[2]*r[2]) - DELTA;
}
// Convenience routine for plotting
void plot(const char* filename, const real_function_3d& f) {
coord_3d lo(0.0), hi(0.0);
lo[2] = -L; hi[2] = L;
plot_line(filename,401,lo,hi,f);
}
double energy(World& world, const real_function_3d& phi, const real_function_3d& V) {
double potential_energy = inner(phi,V*phi); // <phi|Vphi> = <phi|V|phi>
double kinetic_energy = 0.0;
for (int axis=0; axis<3; axis++) {
real_derivative_3d D = free_space_derivative<double,3>(world, axis);
real_function_3d dphi = D(phi);
kinetic_energy += 0.5*inner(dphi,dphi); // (1/2) <dphi/dx | dphi/dx>
}
double energy = kinetic_energy + potential_energy;
//print("kinetic",kinetic_energy,"potential", potential_energy, "total", energy);
return energy;
}
int main(int argc, char** argv) {
initialize(argc, argv);
World world(SafeMPI::COMM_WORLD);
startup(world,argc,argv);
if (world.rank() == 0) printf("starting at time %.1f\n", wall_time());
const double thresh = 1e-5;
FunctionDefaults<3>::set_k(6);
FunctionDefaults<3>::set_thresh(thresh);
FunctionDefaults<3>::set_cubic_cell(-L,L);
real_function_3d phi = real_factory_3d(world).f(guess);
real_function_3d V = real_factory_3d(world).f(potential);
plot("potential.dat", V);
phi.scale(1.0/phi.norm2()); // phi *= 1.0/norm
double E = energy(world,phi,V);
NonlinearSolver solver;
for (int iter=0; iter<100; iter++) {
char filename[256];
snprintf(filename, 256, "phi-%3.3d.dat", iter);
plot(filename,phi);
real_function_3d Vphi = V*phi;
Vphi.truncate();
real_convolution_3d op = BSHOperator3D(world, sqrt(-2*E), 0.01, thresh);
real_function_3d r = phi + 2.0 * op(Vphi); // the residual
double err = r.norm2();
phi = solver.update(phi, r);
//phi = phi-r; // Replace the above line with this to use fixed-point iteration
double norm = phi.norm2();
phi.scale(1.0/norm); // phi *= 1.0/norm
E = energy(world,phi,V);
if (world.rank() == 0)
print("iteration", iter, "energy", E, "norm", norm, "error",err);
if (err < 5e-4) break;
}
print("Final energy without shift", E+DELTA);
if (world.rank() == 0) printf("finished at time %.1f\n", wall_time());
finalize();
return 0;
}