def test_mcif(self):
m = Sample()
load_mcif(m, os.path.join(self._stdir,'Cd2Os2O7.mcif'))
m.add_muon([ float(x) for x in '0.125 0.125 0.125'.split() ])
# distance is l(Os1-H) = 2.20122(0) Å
r1 = locfield(m, 's',[1,1,1],2.3,4,2.3)
r1[0].ACont = 1.
# total field is 0
np.testing.assert_array_almost_equal(r1[0].T,np.zeros(3),decimal=7)
# distance to nnn is l(Os1-H) = 5.53962(0) Å
r1 = locfield(m, 's',[3,3,3],5.54,4,2.3)
r1[0].ACont = 1.
# total field is 0
np.testing.assert_array_almost_equal(r1[0].T,np.zeros(3),decimal=7)
# now use a funny cell
r1 = locfield(m, 's',[np.random.randint(3,10),np.random.randint(3,10),np.random.randint(3,10)],5.54,4,2.3)
r1[0].ACont = 1.
# total field is 0
np.testing.assert_array_almost_equal(r1[0].T,np.zeros(3),decimal=7)
def test_symbolic_fourier_components(self):
m = Sample()
load_xsf(m, os.path.join(self._stdir,'crys.xsf'))
rand_k = np.random.rand(3)
rand_real_fc = np.random.rand(3).reshape((1,3))+0.j # make array complex
mm = MM(1)
mm.k=np.array(rand_k)
mm.fc_set(rand_real_fc)
m.mm = mm
m.add_muon([0.1,0.1,0.1])
r = locfield(m, 's',[10,10,10],40)[0]
if have_sympy:
smm = SMM(1,"x,y,z")
smm.k=np.array(rand_k)
smm.set_symFC("[[x,y,z]]")
smm.set_params(rand_real_fc[0].real.tolist())
m.mm = smm
r2 = locfield(m, 's',[10,10,10],40)[0]
self.assertAlmostEqual( r.D[0], r2.D[0], places=10, msg=None, delta=None)
self.assertAlmostEqual( r.D[1], r2.D[1], places=10, msg=None, delta=None)
self.assertAlmostEqual( r.D[2], r2.D[2], places=7, msg=None, delta=None)
def test_mcif(self):
m = Sample()
load_mcif(m, os.path.join(self._stdir, 'Cd2Os2O7.mcif'))
m.add_muon([float(x) for x in '0.125 0.125 0.125'.split()])
# distance is l(Os1-H) = 2.20122(0) Å
r1 = locfield(m, 's', [1, 1, 1], 2.3, 4, 2.3)
r1[0].ACont = 1.
# total field is 0
np.testing.assert_array_almost_equal(r1[0].T, np.zeros(3), decimal=7)
# distance to nnn is l(Os1-H) = 5.53962(0) Å
r1 = locfield(m, 's', [3, 3, 3], 5.54, 4, 2.3)
r1[0].ACont = 1.
# total field is 0
np.testing.assert_array_almost_equal(r1[0].T, np.zeros(3), decimal=7)
# now use a funny cell
r1 = locfield(m, 's', [
np.random.randint(3, 10),
np.random.randint(3, 10),
np.random.randint(3, 10)
], 5.54, 4, 2.3)
r1[0].ACont = 1.
# total field is 0
np.testing.assert_array_almost_equal(r1[0].T, np.zeros(3), decimal=7)
def test_compare_ass_and_rass(self):
m = Sample()
load_xsf(m, os.path.join(self._stdir, 'crys2.xsf'))
mm = MM(9)
mm.k = np.array(np.random.rand(3))
mm.fc_set(
(np.random.rand(27) + 1.j * np.random.rand(27)).reshape(9, 3))
m.mm = mm
m.add_muon(np.random.rand(3))
m.add_muon(np.random.rand(3))
r1 = locfield(m, 's', [10, 10, 10], 20)
r2 = locfield(m, 'r', [10, 10, 10], 20, axis=[1, 1, 1], nangles=1)
r1[0].ACont = 1.0
r2[0].ACont = 1.0
r1[1].ACont = 1.0
r2[1].ACont = 1.0
min_oom = min(self.oom(r1[0].T), self.oom(r2[0].T[0]))
np.testing.assert_array_almost_equal(r1[0].T,
r2[0].T[0],
decimal=6 - min_oom)
min_oom = min(self.oom(r1[1].T), self.oom(r2[1].T[0]))
np.testing.assert_array_almost_equal(r1[1].T,
r2[1].T[0],
decimal=6 - min_oom)
def test_double_moment(self):
m = Sample()
load_xsf(m, os.path.join(self._stdir, 'crys.xsf'))
mm = MM(1)
mm.k = np.array([0., 0., 0.])
mm.fc_set(np.array([[0. + 0j, 0., 1. + 0.j]]))
m.mm = mm
m.add_muon([0.1, 0.1, 0.1])
r = locfield(m, 's', [1, 1, 1], 4)[0]
m.mm.fc_set(np.array([[0. + 0j, 0. + 0.j, 2. + 0.j]]))
r2 = locfield(m, 's', [1, 1, 1], 4)[0]
# r should be: [0 tesla, 11.4226 milliteslas, 11.4226 milliteslas]
#
# (magnetic_constant/4pi)⋅((1/(1angstrom⋅sqrt(2.5^2+2.5^2+2.5^2)))^3)⋅(3⋅(1 bohr_magneton)⋅cos(atan(sqrt(2)))⋅([1,1,1]/sqrt(3))−1bohr_magneton⋅[1,0,0])
#
#
self.assertAlmostEqual(r.D[0],
0.5 * r2.D[0],
places=10,
msg=None,
delta=None)
self.assertAlmostEqual(r.D[1],
0.5 * r2.D[1],
places=10,
msg=None,
delta=None)
self.assertAlmostEqual(r.D[2],
0.5 * r2.D[2],
places=7,
msg=None,
delta=None)
def test_compare_rass_and_incass(self):
m = Sample()
load_xsf(m, os.path.join(self._stdir,'crys.xsf'))
mm = MM(1)
# define three orthogonal vectors
rp1 = np.random.rand(3) # used for k
r2 = np.random.rand(3)
rp2 = np.cross(rp1,r2)
rp3 = np.cross(rp1,rp2)
# normalize a and b vectors
rp2 /= np.linalg.norm(rp2)
rp3 /= np.linalg.norm(rp3)
#chose a random value for stag moment
stm = np.random.ranf()*10.
rp2 *= stm
rp3 *= stm
mm.k=np.array(rp1)
mm.fc_set((rp2+1.j*rp3).reshape(1,3))
m.mm = mm
m.add_muon(np.random.rand(3))
m.add_muon(np.random.rand(3))
r1 = locfield(m, 's',[50,50,50],50)
r2 = locfield(m, 'r',[50,50,50],50,nangles=1200,axis=rp1)
r3 = locfield(m, 'i',[50,50,50],50,nangles=1200)
r1[0].ACont = 1.0
r2[0].ACont = 1.0
r3[0].ACont = 1.0
r1[1].ACont = 1.0
r2[1].ACont = 1.0
r3[1].ACont = 1.0
min_oom = min(self.oom(r1[0].T), self.oom(r2[0].T[0]))
np.testing.assert_array_almost_equal(r1[0].T,r2[0].T[0],decimal=7-min_oom)
min_oom = min(self.oom(r1[1].T), self.oom(r2[1].T[0]))
np.testing.assert_array_almost_equal(r1[1].T,r2[1].T[0],decimal=7-min_oom)
r2_norms = np.apply_along_axis(np.linalg.norm, 1, r2[0].D)
r3_norms = np.apply_along_axis(np.linalg.norm, 1, r3[0].D)
min_oom=min(self.oom(np.max(r2_norms)), self.oom(np.max(r3_norms)))
np.testing.assert_array_almost_equal(np.max(r2_norms),np.max(r3_norms),decimal=4-min_oom)
min_oom=min(self.oom(np.min(r2_norms)), self.oom(np.min(r3_norms)))
np.testing.assert_array_almost_equal(np.min(r2_norms),np.min(r3_norms),decimal=4-min_oom)
r2_norms = np.apply_along_axis(np.linalg.norm, 1, r2[1].T)
r3_norms = np.apply_along_axis(np.linalg.norm, 1, r3[1].T)
min_oom=min(self.oom(np.max(r2_norms)), self.oom(np.max(r3_norms)))
np.testing.assert_array_almost_equal(np.max(r2_norms),np.max(r2_norms),decimal=5-min_oom)
min_oom=min(self.oom(np.min(r2_norms)), self.oom(np.min(r3_norms)))
np.testing.assert_array_almost_equal(np.min(r3_norms),np.min(r3_norms),decimal=5-min_oom)
def test_mcif2(self):
m = Sample()
load_mcif(m, os.path.join(self._stdir,'ScMnO3.mcif'))
m.add_muon( [float(x) for x in '0.66666666 0.33333333 0.25'.split()])
# No contact
r1 = locfield(m, 's',[np.random.randint(10,14),np.random.randint(10,14),np.random.randint(10,14)],22,4,0.3)
r1[0].ACont = 1.
# total field is 0
np.testing.assert_array_almost_equal(r1[0].T,np.zeros(3),decimal=7)
def test_one_dipole_outside(self):
m = Sample()
load_xsf(m, os.path.join(self._stdir,'crys.xsf'))
mm = MM(1)
mm.k=np.array([0.,0.,0.])
mm.fc_set(np.array([[1.+0j,0.+1.j,0.+1.j]]))
m.mm = mm
m.add_muon([0.5,0.5,0.5])
# the diagonal is 8.6603
r = locfield(m, 's',[1,1,1],8.66/2.)[0]
self.assertEqual( np.sum(np.abs(r.D)), 0.)
def test_one_dipole_outside(self):
m = Sample()
load_xsf(m, os.path.join(self._stdir, 'crys.xsf'))
mm = MM(1)
mm.k = np.array([0., 0., 0.])
mm.fc_set(np.array([[1. + 0j, 0. + 1.j, 0. + 1.j]]))
m.mm = mm
m.add_muon([0.5, 0.5, 0.5])
# the diagonal is 8.6603
r = locfield(m, 's', [1, 1, 1], 8.66 / 2.)[0]
self.assertEqual(np.sum(np.abs(r.D)), 0.)
def test_rotation(self):
m = Sample()
load_xsf(m, os.path.join(self._stdir,'crys3.xsf'))
mm = MM(1)
mm.k=np.array([0.,0.,0.])
mm.fc_set(np.array([[0.+0j,1.+0.j,0.+0.j]]))
m.mm = mm
m.add_muon([0.0,0.001,0.0])
r = locfield(m, 'r',[1,1,1],1.2,nnn=0,nangles=300,axis=[1,0,0])[0]
# r for angle = 0 should be: [0 T, 1.8548 T, 0 T]
#
# (magnetic_constant/4pi)⋅((1/(1angstrom⋅sqrt(1^2)))^3)⋅(3⋅(1 bohr_magneton)⋅cos(0)⋅([0,1,0]/sqrt(1))−1bohr_magneton⋅[0,1,0])
#
#
# r for angle = 90 should be: [0 T, 0 T, −0.927401 T]
#
# (magnetic_constant/4pi)⋅((1/(1angstrom⋅sqrt(1^2)))^3)⋅(3⋅(1 bohr_magneton)⋅cos(pi/2)⋅([0,1,0]/sqrt(1))−1bohr_magneton⋅[0,0,1])
#
# Opposite moments produce opposite fields. 150 is half of 300
np.testing.assert_array_almost_equal(r.D[0],-r.D[150],decimal=7)
np.testing.assert_array_almost_equal(r.D[0],np.array([0., 1.8548018,0.]),decimal=7)
np.testing.assert_array_almost_equal(r.D[75],np.array([0., 0,-0.9274009]),decimal=6)
rnorms = np.apply_along_axis(np.linalg.norm,1,r.T-r.L)
self.assertAlmostEqual( np.min(rnorms), 0.9274009 ,places=6, msg=None, delta=None)
self.assertAlmostEqual( np.max(rnorms), 1.8548018 ,places=6, msg=None, delta=None)
r = locfield(m, 'r',[5,1,1],1.5,nnn=0,nangles=300,axis=[1,0,0])[0]
np.testing.assert_array_almost_equal(r.D[0],-r.D[150],decimal=7)
np.testing.assert_array_almost_equal(r.D[0],np.array([0., 2.18268753,0.]),decimal=7)
np.testing.assert_array_almost_equal(r.D[75],np.array([0., 0,-1.58317237]),decimal=6)
rnorms = np.apply_along_axis(np.linalg.norm,1,r.T-r.L)
self.assertAlmostEqual( np.min(rnorms), 1.58317237 ,places=6, msg=None, delta=None)
self.assertAlmostEqual( np.max(rnorms), 2.18268753 ,places=6, msg=None, delta=None)
# Now test incomm
mm = MM(1)
mm.k=np.array([0.,0.,0.])
mm.fc_set(np.array([[0.+0j,1.+0.j,0.+1.j]]))
m.mm = mm
i = locfield(m, 'i',[1,1,1],1.2,nnn=0,nangles=300)[0]
inorms = np.apply_along_axis(np.linalg.norm,1,i.T-i.L)
self.assertAlmostEqual( np.min(inorms), 0.9274009 ,places=6, msg=None, delta=None)
self.assertAlmostEqual( np.max(inorms), 1.8548018 ,places=6, msg=None, delta=None)
i = locfield(m, 'i',[5,1,1],1.5,nnn=0,nangles=300)[0]
rnorms = np.apply_along_axis(np.linalg.norm,1,i.T-i.L)
self.assertAlmostEqual( np.min(rnorms), 1.58317237 ,places=6, msg=None, delta=None)
self.assertAlmostEqual( np.max(rnorms), 2.18268753 ,places=6, msg=None, delta=None)
def test_mcif2(self):
m = Sample()
load_mcif(m, os.path.join(self._stdir, 'ScMnO3.mcif'))
m.add_muon([float(x) for x in '0.66666666 0.33333333 0.25'.split()])
# No contact
r1 = locfield(m, 's', [
np.random.randint(10, 14),
np.random.randint(10, 14),
np.random.randint(10, 14)
], 22, 4, 0.3)
r1[0].ACont = 1.
# total field is 0
np.testing.assert_array_almost_equal(r1[0].T, np.zeros(3), decimal=7)
def test_one_dipole_inside(self):
m = Sample()
load_xsf(m, os.path.join(self._stdir, 'crys.xsf'))
mm = MM(1)
mm.k = np.array([0., 0., 0.])
mm.fc_set(np.array([[1. + 0j, 0. + 0.j, 0. + 0.j]]))
m.mm = mm
m.add_muon([0.5, 0.5, 0.5])
r = locfield(m, 's', [1, 1, 1], 8.67 / 2.)[0]
# BDip should be: [0 tesla, 11.4226 milliteslas, 11.4226 milliteslas]
#
# (magnetic_constant/4pi)⋅((1/(1angstrom⋅sqrt(2.5^2+2.5^2+2.5^2)))^3)⋅(3⋅(1 bohr_magneton)⋅cos(atan(sqrt(2)))⋅([1,1,1]/sqrt(3))−1bohr_magneton⋅[1,0,0])
#
# BLor should be: [ 0.01138414 T, 0 , 0 ]
#
# 0.3333333333⋅magnetic_constant (1 bohr_magneton)/((4/3)pi(angstrom 8.67/2.)^3)
#
# BCont should be (Assuming ACont = 1 AA^-3 )
#
# (2/3)⋅magnetic_constant (1 bohr_magneton)⋅(1angstrom^−3) = 7.769376 T
#
self.assertAlmostEqual(r.D[0], 0., places=7, msg=None, delta=None)
self.assertAlmostEqual(r.D[1], r.D[2], places=10, msg=None, delta=None)
self.assertAlmostEqual(r.D[1],
11.4226e-3,
places=7,
msg=None,
delta=None)
self.assertAlmostEqual(r.L[0],
0.01138414,
places=7,
msg=None,
delta=None)
self.assertAlmostEqual(r.L[1], 0.0, places=7, msg=None, delta=None)
self.assertAlmostEqual(r.L[2], 0.0, places=7, msg=None, delta=None)
r.ACont = 1. # Ang^-3
self.assertAlmostEqual(r.C[0],
7.769376,
places=7,
msg=None,
delta=None)
self.assertAlmostEqual(r.C[1], 0.0, places=7, msg=None, delta=None)
self.assertAlmostEqual(r.C[2], 0.0, places=7, msg=None, delta=None)
def test_cubic_sym1(self):
m = Sample()
load_xsf(m, os.path.join(self._stdir,'crys.xsf'))
mm = MM(1)
mm.k=np.array([0.,0.,0.])
mm.fc_set(np.array([[1.+0j,0.+0.j,0.+0.j]]))
m.mm = mm
m.add_muon([0.5,0.5,0.5])
r = locfield(m, 's',[100,100,100],240)[0]
# Bdip should be: [0 tesla, 11.4226 milliteslas, 11.4226 milliteslas]
#
# (magnetic_constant/4pi)⋅((1/(1angstrom⋅sqrt(2.5^2+2.5^2+2.5^2)))^3)⋅(3⋅(1 bohr_magneton)⋅cos(atan(sqrt(2)))⋅([1,1,1]/sqrt(3))−1bohr_magneton⋅[1,0,0])
#
#
self.assertAlmostEqual( r.D[0], r.D[1],places=10, msg=None, delta=None)
self.assertAlmostEqual( r.D[0], r.D[2], places=10, msg=None, delta=None)
self.assertAlmostEqual( r.D[0], 0., places=7, msg=None, delta=None)
def test_mcif3(self):
m = Sample()
load_mcif(m, os.path.join(self._stdir,'LiFeSO4F.mcif'))
muon_set_frac(m, '0.25 0.25 0.25')
# symmetry null
r1 = locfield(m, 's',[np.random.randint(10,14),np.random.randint(10,14),np.random.randint(10,14)],22,4,10.)
r1[0].ACont = 1.
# total field is 0
np.testing.assert_array_almost_equal(r1[0].T,np.zeros(3),decimal=7)
muon_reset(m)
m.add_muon([float(x) for x in '0.15990 0.17820 0.14580'.split()]) # position of O3
# one atom, distance is 2.14251 AA
# dipolar field should be:
#
# def bfield(r,m):
# return 0.9274009*(3*r*np.dot(r,m)/(np.linalg.norm(r)**5)-m/(np.linalg.norm(r)**3))
# bfield(np.array([1.07574,1.59328,0.945826]),np.array([-1.70376,3.14961,-1.22045]))
#
r1 = locfield(m, 's',[np.random.randint(1,4),np.random.randint(1,4),np.random.randint(1,4)],2.2,1,2.14251+20.*np.random.ranf())
r1[0].ACont = 1.
np.testing.assert_array_almost_equal(r1[0].D,np.array([0.29531083, -0.09756855, 0.23347458]),decimal=6)
# contact field is (2/3)⋅magnetic_constant ([-1.70376 bohr_magneton ,3.14961bohr_magneton,-1.22045bohr_magneton])⋅(1angstrom^−3) =
# [-13.2372 T, 24.4705 T, -9.48213 T]
np.testing.assert_array_almost_equal(r1[0].C,np.array([-13.2372 , 24.4705 , -9.48213]),decimal=4)
r2 = locfield(m, 's',[np.random.randint(3,5),np.random.randint(3,5),np.random.randint(3,5)],4.2,3,5.+20.*np.random.ranf())
r2[0].ACont = 1.14299 # effective interaction increased since more nnn involved in acont
# still only 14% more
# three atoms, distances are 2.14251 AA, 4.191093 AA, 4.19413AA
#
# bfield(np.array([1.07574,1.59328,0.945826]),np.array([-1.70376,3.14961,-1.22045])) + \
# bfield(np.array([2.14396,2.77751,-2.29775]),np.array([1.70376,-3.14961,1.22045])) + \
# bfield(np.array([-2.28034,-2.66189,-2.29775]),np.array([1.70376,-3.14961,1.22045]))
np.testing.assert_array_almost_equal(r2[0].D,np.array([ 0.20781014, -0.07504131, 0.23329355]),decimal=6)
def test_symbolic_fourier_components(self):
m = Sample()
load_xsf(m, os.path.join(self._stdir, 'crys.xsf'))
rand_k = np.random.rand(3)
rand_real_fc = np.random.rand(3).reshape(
(1, 3)) + 0.j # make array complex
mm = MM(1)
mm.k = np.array(rand_k)
mm.fc_set(rand_real_fc)
m.mm = mm
m.add_muon([0.1, 0.1, 0.1])
r = locfield(m, 's', [10, 10, 10], 40)[0]
if have_sympy:
smm = SMM(1, "x,y,z")
smm.k = np.array(rand_k)
smm.set_symFC("[[x,y,z]]")
smm.set_params(rand_real_fc[0].real.tolist())
m.mm = smm
r2 = locfield(m, 's', [10, 10, 10], 40)[0]
self.assertAlmostEqual(r.D[0],
r2.D[0],
places=10,
msg=None,
delta=None)
self.assertAlmostEqual(r.D[1],
r2.D[1],
places=10,
msg=None,
delta=None)
self.assertAlmostEqual(r.D[2],
r2.D[2],
places=7,
msg=None,
delta=None)
def test_compare_ass_and_rass(self):
m = Sample()
load_xsf(m, os.path.join(self._stdir,'crys2.xsf'))
mm = MM(9)
mm.k=np.array(np.random.rand(3))
mm.fc_set((np.random.rand(27)+1.j*np.random.rand(27)).reshape(9,3))
m.mm = mm
m.add_muon(np.random.rand(3))
m.add_muon(np.random.rand(3))
r1 = locfield(m, 's',[10,10,10],20)
r2 = locfield(m, 'r',[10,10,10],20,axis=[1,1,1],nangles=1)
r1[0].ACont = 1.0
r2[0].ACont = 1.0
r1[1].ACont = 1.0
r2[1].ACont = 1.0
min_oom = min(self.oom(r1[0].T), self.oom(r2[0].T[0]))
np.testing.assert_array_almost_equal(r1[0].T,r2[0].T[0],decimal=6-min_oom)
min_oom = min(self.oom(r1[1].T), self.oom(r2[1].T[0]))
np.testing.assert_array_almost_equal(r1[1].T,r2[1].T[0],decimal=6-min_oom)
def test_one_dipole_inside(self):
m = Sample()
load_xsf(m, os.path.join(self._stdir,'crys.xsf'))
mm = MM(1)
mm.k=np.array([0.,0.,0.])
mm.fc_set(np.array([[1.+0j,0.+0.j,0.+0.j]]))
m.mm = mm
m.add_muon([0.5,0.5,0.5])
r = locfield(m,'s',[1,1,1],8.67/2.)[0]
# BDip should be: [0 tesla, 11.4226 milliteslas, 11.4226 milliteslas]
#
# (magnetic_constant/4pi)⋅((1/(1angstrom⋅sqrt(2.5^2+2.5^2+2.5^2)))^3)⋅(3⋅(1 bohr_magneton)⋅cos(atan(sqrt(2)))⋅([1,1,1]/sqrt(3))−1bohr_magneton⋅[1,0,0])
#
# BLor should be: [ 0.01138414 T, 0 , 0 ]
#
# 0.3333333333⋅magnetic_constant (1 bohr_magneton)/((4/3)pi(angstrom 8.67/2.)^3)
#
# BCont should be (Assuming ACont = 1 AA^-3 )
#
# (2/3)⋅magnetic_constant (1 bohr_magneton)⋅(1angstrom^−3) = 7.769376 T
#
self.assertAlmostEqual( r.D[0], 0.,places=7, msg=None, delta=None)
self.assertAlmostEqual( r.D[1], r.D[2], places=10, msg=None, delta=None)
self.assertAlmostEqual( r.D[1], 11.4226e-3, places=7, msg=None, delta=None)
self.assertAlmostEqual( r.L[0], 0.01138414 ,places=7, msg=None, delta=None)
self.assertAlmostEqual( r.L[1], 0.0 ,places=7, msg=None, delta=None)
self.assertAlmostEqual( r.L[2], 0.0 ,places=7, msg=None, delta=None)
r.ACont = 1. # Ang^-3
self.assertAlmostEqual( r.C[0], 7.769376 ,places=7, msg=None, delta=None)
self.assertAlmostEqual( r.C[1], 0.0 ,places=7, msg=None, delta=None)
self.assertAlmostEqual( r.C[2], 0.0 ,places=7, msg=None, delta=None)
from muesr.engines.clfc import locfield # Does the sum and returns the local field in its diff. contributions
from muesr.engines.clfc import find_largest_sphere # Aids in the calculation of the sphere's radius for the lattice sum.
from muesr.utilities.muon import muon_find_equiv # For finding and including the symmetry equivalent muon positions in the calculation
head,tail = os.path.split(os.path.realpath(__file__))
print("working from "+head)
#
np.set_printoptions(suppress=True,precision=5)
# Declare and load sample
fe= Sample()
load_cif(fe, os.path.join(head,'Cifs','1534895.cif'))
# To add the muon position
fe.add_muon([0.50,0.25,0.0])
# Finds and includes the symmetry equivalent positions of the above defined muon.
# For this example there are 12 sites "print (fe.muons)" will show their positions.
muon_find_equiv(fe)
# Description of the propagation vector k and fourier components fc
# with a new magnetic structure declared with fe.new_mm()
fe.new_mm()
fe.mm.k=np.array([0.0,0.0,0.0])
fe.mm.fc= np.array([[0.0+0.j, 0.0+0.j, 2.2+0.j],
[0.0+0.j, 0.0+0.j, 2.2+0.j],
[0.0+0.j, 0.0+0.j, 2.2+0.j],
[0.0+0.j, 0.0+0.j, 2.2+0.j]])
class TestSample(unittest.TestCase):
def setUp(self):
self._sample = Sample()
def _set_a_cell(self):
self._sample.cell = Atoms(symbols=['Co'],
scaled_positions=[[0,0,0]],
cell=[[3.,0,0],
[0,3.,0],
[0,0,3.]])
def test_set_attribute(self):
with self.assertRaises(TypeError):
self._sample.blabla = 1
def test_name_property(self):
self.assertEqual(self._sample.name,"No name")
self._sample.name = "test"
self.assertEqual(self._sample.name,"test")
#must be str or unicode
with self.assertRaises(TypeError):
self._sample.name = 1
self.assertEqual(self._sample.name,"test")
# test unicode
self._sample.name = u"àèé"
def test_muons_property(self):
self._sample._reset(cell=True,muon=True,sym=True,magdefs=True)
self._set_a_cell()
with self.assertRaises(MuonError):
self._sample.muons
def test_add_muon_property(self):
self._sample._reset(cell=True,muon=True,sym=True,magdefs=True)
with self.assertRaises(CellError):
self._sample.add_muon([0,0,0])
self._set_a_cell()
with self.assertRaises(TypeError):
self._sample.add_muon('0 0 0')
with self.assertRaises(ValueError):
self._sample.add_muon([0,0,0,0])
with self.assertRaises(ValueError):
self._sample.add_muon(np.array([0,0,0,0]))
self._sample.add_muon([0,0,0])
np.testing.assert_array_equal(self._sample.muons[0], np.zeros(3))
self._sample.add_muon([1,1,1])
np.testing.assert_array_equal(self._sample.muons[1], np.ones(3))
self._sample.add_muon([1,1,1], cartesian=True)
np.testing.assert_array_equal(self._sample.muons[2], np.ones(3)/3.)
a = 4.0 # some lattice constant
b = a / 2
self._sample.cell = Atoms(symbols=['Au'],
positions=[0,0,0],
cell=[(0, b, b), (b, 0, b), (b, b, 0)],
pbc=True)
self._sample.add_muon([1.,1.,1.], cartesian=True)
np.testing.assert_array_equal(self._sample.muons[3], np.ones(3)/4.)
self._sample.add_muon([.5,.5,.5], cartesian=False)
self._sample.add_muon([2.,2.,2.], cartesian=True)
np.testing.assert_array_equal(self._sample.muons[4], self._sample.muons[5])
def test_mm_property(self):
self._sample._reset(cell=True,magdefs=True,muon=True,sym=True)
with self.assertRaises(MagDefError):
self._sample.mm
with self.assertRaises(CellError):
self._sample.mm = MM(19) # randomly large number
self._sample._reset(magdefs=True)
self._set_a_cell()
with self.assertRaises(TypeError):
self._sample.mm = 1
self._sample._reset(magdefs=True, cell=True, muon=True, sym=True)
self._sample.cell = Atoms(symbols=['C'],
scaled_positions=[[0,0,0]],
cell=[[3.,0,0],
[0,3.,0],
[0,0,3.]])
with self.assertRaises(MagDefError):
self._sample.mm = MM(198) # randomly large number
self._sample.mm = MM(1)
def test_new_mm(self):
self._sample._reset(magdefs=True, cell=True, muon=True, sym=True)
with self.assertRaises(CellError):
self._sample.new_mm()
self._set_a_cell()
self._sample.new_mm()
self.assertTrue(isinstance(self._sample.mm, MM))
self.assertEqual(len(self._sample.mm.fc), 1)
def test_new_smm(self):
if have_sympy:
self._sample._reset(magdefs=True, cell=True, muon=True, sym=True)
with self.assertRaises(CellError):
self._sample.new_smm("x,y,z")
# TODO TESTING
else:
pass
def test_current_mm_idx_property(self):
self._sample._reset(magdefs=True, cell=True,muon=True, sym=True)
self._sample.cell = Atoms(symbols=['C'],
scaled_positions=[[0,0,0]],
cell=[[3.,0,0],
[0,3.,0],
[0,0,3.]])
self._sample.new_mm()
self._sample.mm.k=np.array([0,0,1.])
self.assertEqual(self._sample.current_mm_idx,0)
self._sample.new_mm()
self._sample.mm.k=np.array([0,0,2.])
self.assertEqual(self._sample.current_mm_idx,1)
self._sample.new_mm()
self._sample.mm.k=np.array([0,0,3.])
self.assertEqual(self._sample.current_mm_idx,2)
self._sample.current_mm_idx = 0
self.assertEqual(self._sample.current_mm_idx,0)
np.testing.assert_array_equal(self._sample.mm.k, np.array([0,0,1.]))
with self.assertRaises(IndexError):
self._sample.current_mm_idx = 3
with self.assertRaises(IndexError):
self._sample.current_mm_idx = -1
self.assertEqual(self._sample.current_mm_idx,0)
def test_sym_property(self):
self._sample._reset(cell=True,muon=True,sym=True,magdefs=True)
with self.assertRaises(SymmetryError):
self._sample.sym
with self.assertRaises(TypeError):
self._sample.sym = 1
self._sample.sym = Spacegroup(113)
self.assertEqual(self._sample.sym.no,113)
self.assertEqual(self._sample.sym.setting,1)
def test_cell_property(self):
#needs better testing
with self.assertRaises(CellError):
self._sample.cell
with self.assertRaises(TypeError):
self._sample.cell = 1
self._set_a_cell()
current_cell = self._sample.cell
self.assertEqual(current_cell.get_chemical_symbols(),['Co'])
current_cell.set_chemical_symbols(['Co'])
self.assertEqual(current_cell.get_chemical_symbols(),['Co'])
def test_reset(self):
# test cell reset
with warnings.catch_warnings(record=True) as w:
# Cause all warnings to always be triggered.
warnings.simplefilter("always")
self._sample._reset(cell=True)
assert len(w) == 3
for wi in w:
assert issubclass(wi.category, RuntimeWarning)
self.assertEqual(self._sample._cell, None)
with self.assertRaises(CellError):
self._sample.cell
# test magdef reset
self._sample._reset(magdefs=True)
self.assertEqual(self._sample._magdefs, [])
self.assertEqual(self._sample._selected_mm, -1)
with self.assertRaises(MagDefError):
self._sample.mm
# test muon reset
self._set_a_cell()
self._sample.add_muon([0,1.,2])
self._sample._reset(muon=True)
self.assertEqual(self._sample._muon, [])
with self.assertRaises(MuonError):
self._sample.muons
self._sample._reset(cell=True,muon=True,sym=True,magdefs=True)
#test symmetry reset
self._sample.sym = Spacegroup(113)
self._sample._reset(sym=True)
self.assertEqual(self._sample._sym, None)
with self.assertRaises(SymmetryError):
self._sample.sym
# TODO
def test_check_sym(self):
self._sample._reset(cell=True,muon=True,sym=True,magdefs=True)
with self.assertRaises(SymmetryError):
self._sample._check_sym()
# vary bad from user side
self._sample._sym = 1
with self.assertRaises(SymmetryError):
self._sample._check_sym()
self._sample.sym = Spacegroup(113)
self.assertTrue(self._sample._check_sym())
def test_check_lattice(self):
self._sample._reset(cell=True,muon=True,sym=True,magdefs=True)
with self.assertRaises(CellError):
self._sample._check_lattice()
self._set_a_cell()
self.assertTrue(self._sample._check_lattice())
self._sample._cell = 1
with self.assertRaises(CellError):
self._sample._check_lattice()
def test_check_magdefs(self):
self._sample._reset(cell=True,muon=True,sym=True,magdefs=True)
with self.assertRaises(MagDefError):
self._sample._check_magdefs()
self._set_a_cell()
self._sample.new_mm()
self.assertTrue(self._sample._check_magdefs())
self._sample._magdefs = 1
with self.assertRaises(MagDefError):
self._sample._check_magdefs()
def test_check_muon(self):
self._sample._reset(cell=True,muon=True,sym=True,magdefs=True)
with self.assertRaises(MuonError):
self._sample._check_muon()
self._set_a_cell()
self._sample.add_muon(np.zeros(3))
self.assertTrue(self._sample._check_muon())
self._sample.add_muon(np.zeros(3))
self._sample._muon[1] = 'a'
with self.assertRaises(MuonError):
self._sample._check_muon()
def load_sample(filename="", fileobj=None):
"""
This function load a sample from a file in YAML format.
:param str filename: the filename used to store data.
:param file fileobj: an optional file object. If specified, this
supersede the filename input.
:return: a sample object
:rtype: :py:class:`~Sample` object or None
:raises: ValueError, FileNotFoundError, IsADirectoryError
"""
# fail if YAML is not available
if not have_yaml:
warnings.warn("Warning, YAML python package not present!")
return
sample = Sample()
data = {}
if fileobj is None:
if filename == "":
raise ValueError("Specify filename or File object")
with open(filename,'r') as f:
data = load(f, Loader=Loader)
else:
data = load(fileobj, Loader=Loader)
if not(type(data) is dict):
raise ValueError('Invalid data file. (problems with YAML?)')
if data is None:
raise ValueError('Invalid/empty data file. (problems with YAML?)')
if 'Name' in data.keys():
sample.name = str(data['Name'])
if 'Lattice' in data.keys():
l = data['Lattice']
spos = None
cpos = None
if 'ScaledPositions' in l.keys():
spos = np.array(l['ScaledPositions'])
elif 'CartesianPositions' in l.keys():
cpos = np.array(l['CartesianPositions'])
cell = None
if 'Cell' in l.keys():
cell = np.array(l['Cell'])
symbols = None
if 'Symbols' in l.keys():
symbols = l['Symbols']
if (cell is None) or (symbols is None):
warnings.warn('Cell not loaded!', RuntimeWarning)
else:
if not spos is None:
sample.cell = Atoms(symbols = symbols, scaled_positions = spos, cell=cell, pbc=True)
elif not cpos is None:
sample.cell = Atoms(symbols = symbols, positions = cpos, cell=cell, pbc=True)
else:
warnings.warn('Cell not loaded!', RuntimeWarning)
else:
warnings.warn('Cell not loaded!', RuntimeWarning)
if 'Muon' in data.keys():
m = data['Muon']
if 'Positions' in m:
for p in m['Positions']:
sample.add_muon(p)
else:
warnings.warn('Muon positions not loaded!', RuntimeWarning)
else:
warnings.warn('Muon positions not loaded!', RuntimeWarning)
if 'Symmetry' in data.keys():
s = data['Symmetry']
if ('Number' in s.keys()) and \
('Symbol' in s.keys()) and \
('Rotations' in s.keys()) and \
('Translations' in s.keys()):
sample.sym = spacegroup_from_data(s['Number'],s['Symbol'],
rotations=np.array(s['Rotations']),
translations=np.array(s['Translations']))
else:
warnings.warn('Symmetry not loaded.', RuntimeWarning)
else:
warnings.warn('Symmetry not loaded!', RuntimeWarning)
if 'MagneticOrders' in data.keys():
m = data['MagneticOrders']
if len(m) > 0:
msize = int(m['Size'])
for mo in m['Orders']:
if 'lattice' in mo.keys():
n = MM(msize, \
np.array(mo['lattice']))
else:
n = MM(msize)
sample.mm = n
sample.mm.k = np.array(mo['k'])
sample.mm.phi = np.array(mo['phi'])
if 'desc' in mo.keys():
sample.mm.desc = str(mo['desc'])
rfcs, ifcs = np.hsplit(np.array(mo['fc']),2)
if mo['format'].lower() in ['bohr-cartesian', 'b-c']:
sample.mm.fcCart=(rfcs + 1.j*ifcs)
elif mo['format'].lower() in ['bohr/angstrom-lattic', 'b/a-l']:
sample.mm.fcLattBMA=(rfcs + 1.j*ifcs)
elif mo['format'].lower() in ['bohr-lattice','b-l']:
sample.mm.fcLattBM=(rfcs + 1.j*ifcs)
else:
raise ValueError('Invalid Fourier Components format specifier in YAML file.')
else:
warnings.warn('Magnetic definitions not loaded!', RuntimeWarning)
else:
warnings.warn('Magnetic definitions not loaded!', RuntimeWarning)
return sample
def test_compare_rass_and_incass(self):
m = Sample()
load_xsf(m, os.path.join(self._stdir, 'crys.xsf'))
mm = MM(1)
# define three orthogonal vectors
rp1 = np.random.rand(3) # used for k
r2 = np.random.rand(3)
rp2 = np.cross(rp1, r2)
rp3 = np.cross(rp1, rp2)
# normalize a and b vectors
rp2 /= np.linalg.norm(rp2)
rp3 /= np.linalg.norm(rp3)
#chose a random value for stag moment
stm = np.random.ranf() * 10.
rp2 *= stm
rp3 *= stm
mm.k = np.array(rp1)
mm.fc_set((rp2 + 1.j * rp3).reshape(1, 3))
m.mm = mm
m.add_muon(np.random.rand(3))
m.add_muon(np.random.rand(3))
r1 = locfield(m, 's', [50, 50, 50], 50)
r2 = locfield(m, 'r', [50, 50, 50], 50, nangles=1200, axis=rp1)
r3 = locfield(m, 'i', [50, 50, 50], 50, nangles=1200)
r1[0].ACont = 1.0
r2[0].ACont = 1.0
r3[0].ACont = 1.0
r1[1].ACont = 1.0
r2[1].ACont = 1.0
r3[1].ACont = 1.0
min_oom = min(self.oom(r1[0].T), self.oom(r2[0].T[0]))
np.testing.assert_array_almost_equal(r1[0].T,
r2[0].T[0],
decimal=7 - min_oom)
min_oom = min(self.oom(r1[1].T), self.oom(r2[1].T[0]))
np.testing.assert_array_almost_equal(r1[1].T,
r2[1].T[0],
decimal=7 - min_oom)
r2_norms = np.apply_along_axis(np.linalg.norm, 1, r2[0].D)
r3_norms = np.apply_along_axis(np.linalg.norm, 1, r3[0].D)
min_oom = min(self.oom(np.max(r2_norms)), self.oom(np.max(r3_norms)))
np.testing.assert_array_almost_equal(np.max(r2_norms),
np.max(r3_norms),
decimal=4 - min_oom)
min_oom = min(self.oom(np.min(r2_norms)), self.oom(np.min(r3_norms)))
np.testing.assert_array_almost_equal(np.min(r2_norms),
np.min(r3_norms),
decimal=4 - min_oom)
r2_norms = np.apply_along_axis(np.linalg.norm, 1, r2[1].T)
r3_norms = np.apply_along_axis(np.linalg.norm, 1, r3[1].T)
min_oom = min(self.oom(np.max(r2_norms)), self.oom(np.max(r3_norms)))
np.testing.assert_array_almost_equal(np.max(r2_norms),
np.max(r2_norms),
decimal=5 - min_oom)
min_oom = min(self.oom(np.min(r2_norms)), self.oom(np.min(r3_norms)))
np.testing.assert_array_almost_equal(np.min(r3_norms),
np.min(r3_norms),
decimal=5 - min_oom)
def test_mcif3(self):
m = Sample()
load_mcif(m, os.path.join(self._stdir, 'LiFeSO4F.mcif'))
muon_set_frac(m, '0.25 0.25 0.25')
# symmetry null
r1 = locfield(m, 's', [
np.random.randint(10, 14),
np.random.randint(10, 14),
np.random.randint(10, 14)
], 22, 4, 10.)
r1[0].ACont = 1.
# total field is 0
np.testing.assert_array_almost_equal(r1[0].T, np.zeros(3), decimal=7)
muon_reset(m)
m.add_muon([float(x) for x in '0.15990 0.17820 0.14580'.split()
]) # position of O3
# one atom, distance is 2.14251 AA
# dipolar field should be:
#
# def bfield(r,m):
# return 0.9274009*(3*r*np.dot(r,m)/(np.linalg.norm(r)**5)-m/(np.linalg.norm(r)**3))
# bfield(np.array([1.07574,1.59328,0.945826]),np.array([-1.70376,3.14961,-1.22045]))
#
r1 = locfield(m, 's', [
np.random.randint(1, 4),
np.random.randint(1, 4),
np.random.randint(1, 4)
], 2.2, 1, 2.14251 + 20. * np.random.ranf())
r1[0].ACont = 1.
np.testing.assert_array_almost_equal(
r1[0].D,
np.array([0.29531083, -0.09756855, 0.23347458]),
decimal=6)
# contact field is (2/3)⋅magnetic_constant ([-1.70376 bohr_magneton ,3.14961bohr_magneton,-1.22045bohr_magneton])⋅(1angstrom^−3) =
# [-13.2372 T, 24.4705 T, -9.48213 T]
np.testing.assert_array_almost_equal(
r1[0].C, np.array([-13.2372, 24.4705, -9.48213]), decimal=4)
r2 = locfield(m, 's', [
np.random.randint(3, 5),
np.random.randint(3, 5),
np.random.randint(3, 5)
], 4.2, 3, 5. + 20. * np.random.ranf())
r2[0].ACont = 1.14299 # effective interaction increased since more nnn involved in acont
# still only 14% more
# three atoms, distances are 2.14251 AA, 4.191093 AA, 4.19413AA
#
# bfield(np.array([1.07574,1.59328,0.945826]),np.array([-1.70376,3.14961,-1.22045])) + \
# bfield(np.array([2.14396,2.77751,-2.29775]),np.array([1.70376,-3.14961,1.22045])) + \
# bfield(np.array([-2.28034,-2.66189,-2.29775]),np.array([1.70376,-3.14961,1.22045]))
np.testing.assert_array_almost_equal(
r2[0].D,
np.array([0.20781014, -0.07504131, 0.23329355]),
decimal=6)
class TestCLFC(unittest.TestCase):
def setUp(self):
self.assertTrue(have_lfclib)
self.sample = Sample()
def _set_a_cell(self):
self.sample.cell = Atoms(symbols=['Co'],
scaled_positions=[[0, 0, 0]],
cell=[[3., 0, 0], [0, 3., 0], [0, 0, 3.]])
def test_find_largest_sphere(self):
self.sample._reset(cell=True, muon=True, sym=True, magdefs=True)
with self.assertRaises(CellError):
find_largest_sphere(self.sample, [3, 3, 3])
self._set_a_cell()
with self.assertRaises(MuonError):
find_largest_sphere(self.sample, [3, 3, 3])
self.sample.add_muon([0.5, 0.5, 0.5])
with self.assertRaises(TypeError):
find_largest_sphere(self.sample, 1)
with self.assertRaises(ValueError):
find_largest_sphere(self.sample, [0, 1, 2])
self.assertEqual(find_largest_sphere(self.sample, [1, 1, 1]), 1.5)
self.sample.add_muon([1., 1., 1.], cartesian=True)
self.assertEqual(find_largest_sphere(self.sample, [1, 1, 1]), 1.)
def test_locfield(self):
self.sample._reset(cell=True, muon=True, sym=True, magdefs=True)
# sample, ctype, supercellsize, radius, nnn = 2, rcont = 10.0, nangles = None, axis = None):
with self.assertRaises(TypeError):
locfield(None, None, None, None)
with self.assertRaises(TypeError):
locfield(self.sample, None, None, None)
with self.assertRaises(TypeError):
locfield(self.sample, 's', None, None)
with self.assertRaises(TypeError):
locfield(self.sample, 's', [2, 2, 2], None)
#with self.assertRaises(TypeError):
# locfield(self.sample, 's', [2,2,2], 3.)
with self.assertRaises(TypeError):
locfield(self.sample, 's', [2, 2, 2], 3., '2a')
with self.assertRaises(TypeError):
locfield(self.sample, 's', [2, 2, 2], 3., '2', '10b')
with self.assertRaises(ValueError):
locfield(self.sample, 'a', [2, 2, 2], 3.)
with self.assertRaises(ValueError):
locfield(self.sample, 'i', [2, 2, 2], 3.)
with self.assertRaises(ValueError):
locfield(self.sample, 's', [0, 2, 2], 3.)
print("Create sample...")
s = Sample()
print("done!")
print("Load CIF file...")
load_cif(s,os.path.join(head,'MnSi.cif'))
print("done!")
print("Calculate dipolar tensor for equivalent sites...\n")
# this is a general position along the 111,
# just to identify the form of the dipolar tensor for the sites
# along the 111
s.add_muon([0.45,0.45,0.45])
# we find the remainig eq muon sites
muon_find_equiv(s)
# apply an arbitrary small field to select magnetic atoms.
# the abslute value is not used, but it must be different from 0.
APP_FCs = 0.001*np.array([[0,0,1],
[0,0,1],
[0,0,1],
[0,0,1],
[0,0,0],
[0,0,0],
[0,0,0],
[0,0,0]], dtype=np.complex)
def load_sample(filename="", fileobj=None):
"""
This function load a sample from a file in YAML format.
:param str filename: the filename used to store data.
:param file fileobj: an optional file object. If specified, this
supersede the filename input.
:return: a sample object
:rtype: :py:class:`~Sample` object or None
:raises: ValueError, FileNotFoundError, IsADirectoryError
"""
# fail if YAML is not available
if not have_yaml:
warnings.warn("Warning, YAML python package not present!")
return
sample = Sample()
data = {}
if fileobj is None:
if filename == "":
raise ValueError("Specify filename or File object")
with open(filename, 'r') as f:
data = load(f, Loader=Loader)
else:
data = load(fileobj, Loader=Loader)
if not (type(data) is dict):
raise ValueError('Invalid data file. (problems with YAML?)')
if data is None:
raise ValueError('Invalid/empty data file. (problems with YAML?)')
if 'Name' in data.keys():
sample.name = str(data['Name'])
if 'Lattice' in data.keys():
l = data['Lattice']
spos = None
cpos = None
if 'ScaledPositions' in l.keys():
spos = np.array(l['ScaledPositions'])
elif 'CartesianPositions' in l.keys():
cpos = np.array(l['CartesianPositions'])
cell = None
if 'Cell' in l.keys():
cell = np.array(l['Cell'])
symbols = None
if 'Symbols' in l.keys():
symbols = l['Symbols']
if (cell is None) or (symbols is None):
warnings.warn('Cell not loaded!', RuntimeWarning)
else:
if not spos is None:
sample.cell = Atoms(symbols=symbols,
scaled_positions=spos,
cell=cell,
pbc=True)
elif not cpos is None:
sample.cell = Atoms(symbols=symbols,
positions=cpos,
cell=cell,
pbc=True)
else:
warnings.warn('Cell not loaded!', RuntimeWarning)
else:
warnings.warn('Cell not loaded!', RuntimeWarning)
if 'Muon' in data.keys():
m = data['Muon']
if 'Positions' in m:
for p in m['Positions']:
sample.add_muon(p)
else:
warnings.warn('Muon positions not loaded!', RuntimeWarning)
else:
warnings.warn('Muon positions not loaded!', RuntimeWarning)
if 'Symmetry' in data.keys():
s = data['Symmetry']
if ('Number' in s.keys()) and \
('Symbol' in s.keys()) and \
('Rotations' in s.keys()) and \
('Translations' in s.keys()):
sample.sym = spacegroup_from_data(
s['Number'],
s['Symbol'],
rotations=np.array(s['Rotations']),
translations=np.array(s['Translations']))
else:
warnings.warn('Symmetry not loaded.', RuntimeWarning)
else:
warnings.warn('Symmetry not loaded!', RuntimeWarning)
if 'MagneticOrders' in data.keys():
m = data['MagneticOrders']
if len(m) > 0:
msize = int(m['Size'])
for mo in m['Orders']:
if 'lattice' in mo.keys():
n = MM(msize, \
np.array(mo['lattice']))
else:
n = MM(msize)
sample.mm = n
sample.mm.k = np.array(mo['k'])
sample.mm.phi = np.array(mo['phi'])
if 'desc' in mo.keys():
sample.mm.desc = str(mo['desc'])
rfcs, ifcs = np.hsplit(np.array(mo['fc']), 2)
if mo['format'].lower() in ['bohr-cartesian', 'b-c']:
sample.mm.fcCart = (rfcs + 1.j * ifcs)
elif mo['format'].lower() in ['bohr/angstrom-lattic', 'b/a-l']:
sample.mm.fcLattBMA = (rfcs + 1.j * ifcs)
elif mo['format'].lower() in ['bohr-lattice', 'b-l']:
sample.mm.fcLattBM = (rfcs + 1.j * ifcs)
else:
raise ValueError(
'Invalid Fourier Components format specifier in YAML file.'
)
else:
warnings.warn('Magnetic definitions not loaded!', RuntimeWarning)
else:
warnings.warn('Magnetic definitions not loaded!', RuntimeWarning)
return sample
def test_rotation(self):
m = Sample()
load_xsf(m, os.path.join(self._stdir, 'crys3.xsf'))
mm = MM(1)
mm.k = np.array([0., 0., 0.])
mm.fc_set(np.array([[0. + 0j, 1. + 0.j, 0. + 0.j]]))
m.mm = mm
m.add_muon([0.0, 0.001, 0.0])
r = locfield(m,
'r', [1, 1, 1],
1.2,
nnn=0,
nangles=300,
axis=[1, 0, 0])[0]
# r for angle = 0 should be: [0 T, 1.8548 T, 0 T]
#
# (magnetic_constant/4pi)⋅((1/(1angstrom⋅sqrt(1^2)))^3)⋅(3⋅(1 bohr_magneton)⋅cos(0)⋅([0,1,0]/sqrt(1))−1bohr_magneton⋅[0,1,0])
#
#
# r for angle = 90 should be: [0 T, 0 T, −0.927401 T]
#
# (magnetic_constant/4pi)⋅((1/(1angstrom⋅sqrt(1^2)))^3)⋅(3⋅(1 bohr_magneton)⋅cos(pi/2)⋅([0,1,0]/sqrt(1))−1bohr_magneton⋅[0,0,1])
#
# Opposite moments produce opposite fields. 150 is half of 300
np.testing.assert_array_almost_equal(r.D[0], -r.D[150], decimal=7)
np.testing.assert_array_almost_equal(r.D[0],
np.array([0., 1.8548018, 0.]),
decimal=7)
np.testing.assert_array_almost_equal(r.D[75],
np.array([0., 0, -0.9274009]),
decimal=6)
rnorms = np.apply_along_axis(np.linalg.norm, 1, r.T - r.L)
self.assertAlmostEqual(np.min(rnorms),
0.9274009,
places=6,
msg=None,
delta=None)
self.assertAlmostEqual(np.max(rnorms),
1.8548018,
places=6,
msg=None,
delta=None)
r = locfield(m,
'r', [5, 1, 1],
1.5,
nnn=0,
nangles=300,
axis=[1, 0, 0])[0]
np.testing.assert_array_almost_equal(r.D[0], -r.D[150], decimal=7)
np.testing.assert_array_almost_equal(r.D[0],
np.array([0., 2.18268753, 0.]),
decimal=7)
np.testing.assert_array_almost_equal(r.D[75],
np.array([0., 0, -1.58317237]),
decimal=6)
rnorms = np.apply_along_axis(np.linalg.norm, 1, r.T - r.L)
self.assertAlmostEqual(np.min(rnorms),
1.58317237,
places=6,
msg=None,
delta=None)
self.assertAlmostEqual(np.max(rnorms),
2.18268753,
places=6,
msg=None,
delta=None)
# Now test incomm
mm = MM(1)
mm.k = np.array([0., 0., 0.])
mm.fc_set(np.array([[0. + 0j, 1. + 0.j, 0. + 1.j]]))
m.mm = mm
i = locfield(m, 'i', [1, 1, 1], 1.2, nnn=0, nangles=300)[0]
inorms = np.apply_along_axis(np.linalg.norm, 1, i.T - i.L)
self.assertAlmostEqual(np.min(inorms),
0.9274009,
places=6,
msg=None,
delta=None)
self.assertAlmostEqual(np.max(inorms),
1.8548018,
places=6,
msg=None,
delta=None)
i = locfield(m, 'i', [5, 1, 1], 1.5, nnn=0, nangles=300)[0]
rnorms = np.apply_along_axis(np.linalg.norm, 1, i.T - i.L)
self.assertAlmostEqual(np.min(rnorms),
1.58317237,
places=6,
msg=None,
delta=None)
self.assertAlmostEqual(np.max(rnorms),
2.18268753,
places=6,
msg=None,
delta=None)
class TestSample(unittest.TestCase):
def setUp(self):
self._sample = Sample()
def _set_a_cell(self):
self._sample.cell = Atoms(symbols=['Co'],
scaled_positions=[[0, 0, 0]],
cell=[[3., 0, 0], [0, 3., 0], [0, 0, 3.]])
def test_set_attribute(self):
with self.assertRaises(TypeError):
self._sample.blabla = 1
def test_name_property(self):
self.assertEqual(self._sample.name, "No name")
self._sample.name = "test"
self.assertEqual(self._sample.name, "test")
#must be str or unicode
with self.assertRaises(TypeError):
self._sample.name = 1
self.assertEqual(self._sample.name, "test")
# test unicode
self._sample.name = u"àèé"
def test_muons_property(self):
self._sample._reset(cell=True, muon=True, sym=True, magdefs=True)
self._set_a_cell()
with self.assertRaises(MuonError):
self._sample.muons
def test_add_muon_property(self):
self._sample._reset(cell=True, muon=True, sym=True, magdefs=True)
with self.assertRaises(CellError):
self._sample.add_muon([0, 0, 0])
self._set_a_cell()
with self.assertRaises(TypeError):
self._sample.add_muon('0 0 0')
with self.assertRaises(ValueError):
self._sample.add_muon([0, 0, 0, 0])
with self.assertRaises(ValueError):
self._sample.add_muon(np.array([0, 0, 0, 0]))
self._sample.add_muon([0, 0, 0])
np.testing.assert_array_equal(self._sample.muons[0], np.zeros(3))
self._sample.add_muon([1, 1, 1])
np.testing.assert_array_equal(self._sample.muons[1], np.ones(3))
self._sample.add_muon([1, 1, 1], cartesian=True)
np.testing.assert_array_equal(self._sample.muons[2], np.ones(3) / 3.)
a = 4.0 # some lattice constant
b = a / 2
self._sample.cell = Atoms(symbols=['Au'],
positions=[0, 0, 0],
cell=[(0, b, b), (b, 0, b), (b, b, 0)],
pbc=True)
self._sample.add_muon([1., 1., 1.], cartesian=True)
np.testing.assert_array_equal(self._sample.muons[3], np.ones(3) / 4.)
self._sample.add_muon([.5, .5, .5], cartesian=False)
self._sample.add_muon([2., 2., 2.], cartesian=True)
np.testing.assert_array_equal(self._sample.muons[4],
self._sample.muons[5])
def test_mm_property(self):
self._sample._reset(cell=True, magdefs=True, muon=True, sym=True)
with self.assertRaises(MagDefError):
self._sample.mm
with self.assertRaises(CellError):
self._sample.mm = MM(19) # randomly large number
self._sample._reset(magdefs=True)
self._set_a_cell()
with self.assertRaises(TypeError):
self._sample.mm = 1
self._sample._reset(magdefs=True, cell=True, muon=True, sym=True)
self._sample.cell = Atoms(symbols=['C'],
scaled_positions=[[0, 0, 0]],
cell=[[3., 0, 0], [0, 3., 0], [0, 0, 3.]])
with self.assertRaises(MagDefError):
self._sample.mm = MM(198) # randomly large number
self._sample.mm = MM(1)
def test_new_mm(self):
self._sample._reset(magdefs=True, cell=True, muon=True, sym=True)
with self.assertRaises(CellError):
self._sample.new_mm()
self._set_a_cell()
self._sample.new_mm()
self.assertTrue(isinstance(self._sample.mm, MM))
self.assertEqual(len(self._sample.mm.fc), 1)
def test_new_smm(self):
if have_sympy:
self._sample._reset(magdefs=True, cell=True, muon=True, sym=True)
with self.assertRaises(CellError):
self._sample.new_smm("x,y,z")
# TODO TESTING
else:
pass
def test_current_mm_idx_property(self):
self._sample._reset(magdefs=True, cell=True, muon=True, sym=True)
self._sample.cell = Atoms(symbols=['C'],
scaled_positions=[[0, 0, 0]],
cell=[[3., 0, 0], [0, 3., 0], [0, 0, 3.]])
self._sample.new_mm()
self._sample.mm.k = np.array([0, 0, 1.])
self.assertEqual(self._sample.current_mm_idx, 0)
self._sample.new_mm()
self._sample.mm.k = np.array([0, 0, 2.])
self.assertEqual(self._sample.current_mm_idx, 1)
self._sample.new_mm()
self._sample.mm.k = np.array([0, 0, 3.])
self.assertEqual(self._sample.current_mm_idx, 2)
self._sample.current_mm_idx = 0
self.assertEqual(self._sample.current_mm_idx, 0)
np.testing.assert_array_equal(self._sample.mm.k, np.array([0, 0, 1.]))
with self.assertRaises(IndexError):
self._sample.current_mm_idx = 3
with self.assertRaises(IndexError):
self._sample.current_mm_idx = -1
self.assertEqual(self._sample.current_mm_idx, 0)
def test_sym_property(self):
self._sample._reset(cell=True, muon=True, sym=True, magdefs=True)
with self.assertRaises(SymmetryError):
self._sample.sym
with self.assertRaises(TypeError):
self._sample.sym = 1
self._sample.sym = Spacegroup(113)
self.assertEqual(self._sample.sym.no, 113)
self.assertEqual(self._sample.sym.setting, 1)
def test_cell_property(self):
#needs better testing
with self.assertRaises(CellError):
self._sample.cell
with self.assertRaises(TypeError):
self._sample.cell = 1
self._set_a_cell()
current_cell = self._sample.cell
self.assertEqual(current_cell.get_chemical_symbols(), ['Co'])
current_cell.set_chemical_symbols(['Co'])
self.assertEqual(current_cell.get_chemical_symbols(), ['Co'])
def test_reset(self):
# test cell reset
with warnings.catch_warnings(record=True) as w:
# Cause all warnings to always be triggered.
warnings.simplefilter("always")
self._sample._reset(cell=True)
assert len(w) == 3
for wi in w:
assert issubclass(wi.category, RuntimeWarning)
self.assertEqual(self._sample._cell, None)
with self.assertRaises(CellError):
self._sample.cell
# test magdef reset
self._sample._reset(magdefs=True)
self.assertEqual(self._sample._magdefs, [])
self.assertEqual(self._sample._selected_mm, -1)
with self.assertRaises(MagDefError):
self._sample.mm
# test muon reset
self._set_a_cell()
self._sample.add_muon([0, 1., 2])
self._sample._reset(muon=True)
self.assertEqual(self._sample._muon, [])
with self.assertRaises(MuonError):
self._sample.muons
self._sample._reset(cell=True, muon=True, sym=True, magdefs=True)
#test symmetry reset
self._sample.sym = Spacegroup(113)
self._sample._reset(sym=True)
self.assertEqual(self._sample._sym, None)
with self.assertRaises(SymmetryError):
self._sample.sym
# TODO
def test_check_sym(self):
self._sample._reset(cell=True, muon=True, sym=True, magdefs=True)
with self.assertRaises(SymmetryError):
self._sample._check_sym()
# vary bad from user side
self._sample._sym = 1
with self.assertRaises(SymmetryError):
self._sample._check_sym()
self._sample.sym = Spacegroup(113)
self.assertTrue(self._sample._check_sym())
def test_check_lattice(self):
self._sample._reset(cell=True, muon=True, sym=True, magdefs=True)
with self.assertRaises(CellError):
self._sample._check_lattice()
self._set_a_cell()
self.assertTrue(self._sample._check_lattice())
self._sample._cell = 1
with self.assertRaises(CellError):
self._sample._check_lattice()
def test_check_magdefs(self):
self._sample._reset(cell=True, muon=True, sym=True, magdefs=True)
with self.assertRaises(MagDefError):
self._sample._check_magdefs()
self._set_a_cell()
self._sample.new_mm()
self.assertTrue(self._sample._check_magdefs())
self._sample._magdefs = 1
with self.assertRaises(MagDefError):
self._sample._check_magdefs()
def test_check_muon(self):
self._sample._reset(cell=True, muon=True, sym=True, magdefs=True)
with self.assertRaises(MuonError):
self._sample._check_muon()
self._set_a_cell()
self._sample.add_muon(np.zeros(3))
self.assertTrue(self._sample._check_muon())
self._sample.add_muon(np.zeros(3))
self._sample._muon[1] = 'a'
with self.assertRaises(MuonError):
self._sample._check_muon()
class TestCLFC(unittest.TestCase):
def setUp(self):
self.assertTrue(have_lfclib)
self.sample = Sample()
def _set_a_cell(self):
self.sample.cell = Atoms(symbols=['Co'],
scaled_positions=[[0,0,0]],
cell=[[3.,0,0],
[0,3.,0],
[0,0,3.]])
def test_find_largest_sphere(self):
self.sample._reset(cell=True,muon=True,sym=True,magdefs=True)
with self.assertRaises(CellError):
find_largest_sphere(self.sample,[3,3,3])
self._set_a_cell()
with self.assertRaises(MuonError):
find_largest_sphere(self.sample,[3,3,3])
self.sample.add_muon([0.5,0.5,0.5])
with self.assertRaises(TypeError):
find_largest_sphere(self.sample,1)
with self.assertRaises(ValueError):
find_largest_sphere(self.sample,[0,1,2])
self.assertEqual(find_largest_sphere(self.sample,[1,1,1]),1.5)
self.sample.add_muon([1.,1.,1.],cartesian=True)
self.assertEqual(find_largest_sphere(self.sample,[1,1,1]),1.)
def test_locfield(self):
self.sample._reset(cell=True,muon=True,sym=True,magdefs=True)
# sample, ctype, supercellsize, radius, nnn = 2, rcont = 10.0, nangles = None, axis = None):
with self.assertRaises(TypeError):
locfield(None, None, None, None)
with self.assertRaises(TypeError):
locfield(self.sample, None, None, None)
with self.assertRaises(TypeError):
locfield(self.sample, 's', None, None)
with self.assertRaises(TypeError):
locfield(self.sample, 's', [2,2,2], None)
#with self.assertRaises(TypeError):
# locfield(self.sample, 's', [2,2,2], 3.)
with self.assertRaises(TypeError):
locfield(self.sample, 's', [2,2,2], 3., '2a')
with self.assertRaises(TypeError):
locfield(self.sample, 's', [2,2,2], 3., '2', '10b')
with self.assertRaises(ValueError):
locfield(self.sample, 'a', [2,2,2], 3.)
with self.assertRaises(ValueError):
locfield(self.sample, 'i', [2,2,2], 3.)
with self.assertRaises(ValueError):
locfield(self.sample, 's', [0,2,2], 3.)