def printspins(fout, pot, coords2):
s = coords2ToCoords3(coords2)
h = pot.fields
c = coords2ToCoords3(coordsinit)
for node in pot.G.nodes():
i = pot.indices[node]
fout.write( "%g %g %g %g %g %g %g %g\n" % (node[0], node[1], \
s[i,0], s[i,1], s[i,2], h[i,0], h[i,1], h[i,2] ) )
def printspins(fout, pot, coords2):
s = coords2ToCoords3( coords2 )
h = pot.fields
c = coords2ToCoords3( coordsinit )
for node in pot.G.nodes():
i = pot.indices[node]
fout.write( "%g %g %g %g %g %g %g %g\n" % (node[0], node[1], \
s[i,0], s[i,1], s[i,2], h[i,0], h[i,1], h[i,2] ) )
def getEnergyGradient(self, coords):
"""
coords is a list of (theta, phi) spherical coordinates of the spins
where phi is the azimuthal angle (angle to the z axis)
"""
coords3 = coords2ToCoords3( coords )
coords2 = coords
E = 0.
grad3 = np.zeros( [self.nspins, 3] )
for edge in self.G.edges():
u = self.indices[edge[0]]
v = self.indices[edge[1]]
E -= np.dot( coords3[u,:], coords3[v,:] )
grad3[u,:] -= coords3[v,:]
grad3[v,:] -= coords3[u,:]
vdotf = np.sum( self.fields * coords3, axis=1 )
Efields = - np.sum( np.sum( self.fields * coords3, axis=1 )**2 )
grad3 -= 2.* self.fields * vdotf[:, np.newaxis]
#for i in range(self.nspins):
# grad3[i,:] /= np.linalg.norm( grad3[i,:] )
grad2 = grad3ToGrad2(coords2, grad3)
grad2 = np.reshape(grad2, self.nspins*2)
#print "EJ EH", E, Efields
return E + Efields, grad2
def getEnergyGradient(self, coords):
"""
coords is a list of (theta, phi) spherical coordinates of the spins
where phi is the azimuthal angle (angle to the z axis)
"""
coords3 = coords2ToCoords3(coords)
coords2 = coords
E = 0.
grad3 = np.zeros([self.nspins, 3])
for edge in self.G.edges():
u = self.indices[edge[0]]
v = self.indices[edge[1]]
E -= np.dot(coords3[u, :], coords3[v, :])
grad3[u, :] -= coords3[v, :]
grad3[v, :] -= coords3[u, :]
vdotf = np.sum(self.fields * coords3, axis=1)
Efields = -np.sum(np.sum(self.fields * coords3, axis=1)**2)
grad3 -= 2. * self.fields * vdotf[:, np.newaxis]
#for i in range(self.nspins):
# grad3[i,:] /= np.linalg.norm( grad3[i,:] )
grad2 = grad3ToGrad2(coords2, grad3)
grad2 = np.reshape(grad2, self.nspins * 2)
#print "EJ EH", E, Efields
return E + Efields, grad2
def getEnergy(self, coords):
"""
coords is a list of (theta, phi) spherical coordinates of the spins
where phi is the azimuthal angle (angle to the z axis)
"""
coords3 = coords2ToCoords3( coords )
E = 0.
for edge in self.G.edges():
u = self.indices[edge[0]]
v = self.indices[edge[1]]
E -= np.dot( coords3[u,:], coords3[v,:] )
Efields = - np.sum( np.sum( self.fields * coords3, axis=1 )**2 )
#print "EJ EH", E, Efields
return E + Efields
def getEnergy(self, coords):
"""
coords is a list of (theta, phi) spherical coordinates of the spins
where phi is the azimuthal angle (angle to the z axis)
"""
coords3 = coords2ToCoords3(coords)
E = 0.
for edge in self.G.edges():
u = self.indices[edge[0]]
v = self.indices[edge[1]]
E -= np.dot(coords3[u, :], coords3[v, :])
Efields = -np.sum(np.sum(self.fields * coords3, axis=1)**2)
#print "EJ EH", E, Efields
return E + Efields
def getm(coords2):
coords3 = coords2ToCoords3(coords2)
m = np.linalg.norm(coords3.sum(0)) / nspins
return m
def getm(coords2):
coords3 = coords2ToCoords3( coords2 )
m = np.linalg.norm( coords3.sum(0) ) / nspins
return m
def test():
pi = np.pi
L = 4
nspins = L**2
#phases = np.zeros(nspins)
pot = HeisenbergModelRA( dim = [L,L], field_disorder = 2. ) #, phases=phases)
coords = np.zeros([nspins, 2])
for i in range(nspins):
vec = rotations.vec_random()
coords[i,:] = make2dVector(vec)
coords = np.reshape(coords, [nspins*2])
if False:
normfields = np.copy(pot.fields)
for i in range(nspins): normfields[i,:] /= np.linalg.norm(normfields[i,:])
coords = coords3ToCoords2( np.reshape(normfields, [nspins*3] ) )
coords = np.reshape(coords, nspins*2)
#print np.shape(coords)
coordsinit = np.copy(coords)
#print "fields", pot.fields
print coords
if False:
coords3 = coords2ToCoords3(coords)
coords2 = coords3ToCoords2(coords3)
print np.reshape(coords, [nspins,2])
print coords2
coords3new = coords2ToCoords3(coords2)
print coords3
print coords3new
e = pot.getEnergy(coords)
print "energy ", e
if True:
print "numerical gradient"
ret = pot.getEnergyGradientNumerical(coords)
print ret[1]
if True:
print "analytical gradient"
ret2 = pot.getEnergyGradient(coords)
print ret2[1]
print ret[0]
print ret2[0]
#print "ratio"
#print ret2[1] / ret[1]
#print "inverse sin"
#print 1./sin(coords)
#print cos(coords)
print "try a quench"
from pygmin.optimize.quench import mylbfgs
ret = mylbfgs(coords, pot.getEnergyGradient)
print "quenched e = ", ret[1], "funcalls", ret[3]
print ret[0]
with open("out.spins", "w") as fout:
s = coords2ToCoords3( ret[0] )
h = pot.fields
c = coords2ToCoords3( coordsinit )
for node in pot.G.nodes():
i = pot.indices[node]
fout.write( "%g %g %g %g %g %g %g %g %g %g %g\n" % (node[0], node[1], \
s[i,0], s[i,1], s[i,2], h[i,0], h[i,1], h[i,2], c[i,0], c[i,1], c[i,2] ) )
coords3 = coords2ToCoords3( ret[0] )
m = np.linalg.norm( coords3.sum(0) ) / nspins
print "magnetization after quench", m
test_basin_hopping(pot, coords)
def test():
pi = np.pi
L = 4
nspins = L**2
#phases = np.zeros(nspins)
pot = HeisenbergModelRA(dim=[L, L], field_disorder=2.) #, phases=phases)
coords = np.zeros([nspins, 2])
for i in range(nspins):
vec = rotations.vec_random()
coords[i, :] = make2dVector(vec)
coords = np.reshape(coords, [nspins * 2])
if False:
normfields = np.copy(pot.fields)
for i in range(nspins):
normfields[i, :] /= np.linalg.norm(normfields[i, :])
coords = coords3ToCoords2(np.reshape(normfields, [nspins * 3]))
coords = np.reshape(coords, nspins * 2)
#print np.shape(coords)
coordsinit = np.copy(coords)
#print "fields", pot.fields
print coords
if False:
coords3 = coords2ToCoords3(coords)
coords2 = coords3ToCoords2(coords3)
print np.reshape(coords, [nspins, 2])
print coords2
coords3new = coords2ToCoords3(coords2)
print coords3
print coords3new
e = pot.getEnergy(coords)
print "energy ", e
if True:
print "numerical gradient"
ret = pot.getEnergyGradientNumerical(coords)
print ret[1]
if True:
print "analytical gradient"
ret2 = pot.getEnergyGradient(coords)
print ret2[1]
print ret[0]
print ret2[0]
#print "ratio"
#print ret2[1] / ret[1]
#print "inverse sin"
#print 1./sin(coords)
#print cos(coords)
print "try a quench"
from pygmin.optimize import mylbfgs
ret = mylbfgs(coords, pot)
print "quenched e = ", ret.energy, "funcalls", ret.nfev
print ret.coords
with open("out.spins", "w") as fout:
s = coords2ToCoords3(ret.coords)
h = pot.fields
c = coords2ToCoords3(coordsinit)
for node in pot.G.nodes():
i = pot.indices[node]
fout.write( "%g %g %g %g %g %g %g %g %g %g %g\n" % (node[0], node[1], \
s[i,0], s[i,1], s[i,2], h[i,0], h[i,1], h[i,2], c[i,0], c[i,1], c[i,2] ) )
coords3 = coords2ToCoords3(ret.coords)
m = np.linalg.norm(coords3.sum(0)) / nspins
print "magnetization after quench", m
test_basin_hopping(pot, coords)