def plot_g2(G2, cplx=None, idx_labels=None, w=Idx(0), opt={}, title=None):
data = G2[w, :, :].data
if cplx == 're':
data = data.real
elif cplx == 'im':
data = data.imag
n = data.shape[-1]
N = n**2
subp = [N, N, 1]
colorbar_flag = True
import itertools
for idxs in itertools.product(xrange(n), repeat=4):
i1, i2, i3, i4 = idxs
d = data[:, :, i1, i2, i3, i4]
ax = plt.subplot(*subp)
subp[-1] += 1
if idx_labels is not None:
labels = [idx_labels[idx] for idx in idxs]
sub_title = r'$c^\dagger_{%s} c_{%s} c^\dagger_{%s} c_{%s}$' % tuple(
labels)
else:
sub_title = str(idxs)
plt.title(sub_title, fontsize=8)
#plt.pcolormesh(d, **opt)
if np.max(np.abs(d)) > 1e-10:
plt.imshow(d, **opt)
if colorbar_flag:
if title is not None:
plt.title(title)
plt.colorbar()
colorbar_flag = False
ax.set_xticks([])
ax.set_yticks([])
plt.axis('equal')
plt.tight_layout()
def plot_field(out):
plt.figure(figsize=(3.25 * 2, 8))
for p in out.data:
subp = [2, 1, 1]
ax = plt.subplot(*subp)
subp[-1] += 1
oplotr(p.G_tau['up'], 'b', alpha=0.25)
oplotr(p.G_tau['dn'], 'g', alpha=0.25)
ax.legend().set_visible(False)
plt.subplot(*subp)
subp[-1] += 1
plt.title(r'$\chi \approx %2.2f$' % out.chi)
plt.plot(out.h_vec, out.m_vec, '-og', alpha=0.5)
plt.plot(out.h_vec, out.m_ref_vec, 'xb', alpha=0.5)
plt.plot(out.h_vec, -out.chi * out.h_vec, '-r', alpha=0.5)
plt.tight_layout()
plt.savefig('figure_static_field.pdf')
#opt = dict(vmin=-10., vmax=10., cmap='PuOr')
#opt = dict(cmap='PuOr')
ax = plt.subplot(*subp)
subp[-1] += 1
oplot(ana.G_iw)
if True:
g2 = ana.gamma_m
label = 'gamma ana'
s = np.squeeze(g2.data[0, :, :])
ax = plt.subplot(*subp)
subp[-1] += 1
plt.title('Re ' + label + ' [i,:,:]')
plt.pcolormesh(s.real, **opt)
plt.colorbar()
if False:
g2 = ana.gamma_m
label = 'gamma ana'
s = np.squeeze(g2.data[idx, :, :])
ax = plt.subplot(*subp)
subp[-1] += 1
plt.title('Re ' + label + ' [i,:,:]')
plt.pcolormesh(s.real, **opt)
plt.colorbar()
# ----------------------------------------------------------------------
from pytriqs.operators import n
from pytriqs.operators.util.op_struct import set_operator_structure
from pytriqs.plot.mpl_interface import oplot, oplotr, oploti, plt
# ----------------------------------------------------------------------
from pyed.ParameterCollection import ParameterCollection
# ----------------------------------------------------------------------
if __name__ == '__main__':
plt.figure(figsize=(3.25, 2 * 3))
plt.title('Magnetic Susceptibility\n Hubbard atom + 2 bath sites.')
# ------------------------------------------------------------------
# -- external field pyed
filenames = glob.glob('pyed_beta*/data_pyed_extrap*.h5')
style = 'sk'
for filename in filenames:
print '--> Loading:', filename
with HDFArchive(filename, 'r') as s:
field = s['field']
plt.plot(1. / field.beta, field.chi, style, alpha=0.25)
plt.subplot(*subp); subp[-1] += 1
plt.plot(1./p.nwf, p.chi_G, 'o', color=color)
ps.append(p)
# -- Extrapolation to nwf -> oo
ps = ParameterCollections(objects=ps)
x, y = 1./ps.nwf, ps.chi_G
sidx = np.argsort(x)
x, y = x[sidx], y[sidx]
p = np.polyfit(x, y, 1)
y0 = np.polyval(p, 0)
X = np.linspace(0, x.max())
Y = np.polyval(p, X)
subp = [1, 2, 1]
plt.subplot(*subp); subp[-1] += 1
plt.plot(0, y0, 'rx')
plt.plot(0, 0.3479, 'r+')
plt.subplot(*subp); subp[-1] += 1
plt.plot(X, Y, '--k', lw=1.0, zorder=-100)
plt.plot(0, 0.3479, 'r+', label=r'Field')
plt.plot(0, y0, 'rx', label=r'BSE')
plt.grid(True); plt.legend(loc='best', fontsize=8)
plt.xlabel(r'$1/N_\nu$'); plt.ylabel(r'$\chi(\mathbf{0})$')
plt.title(
r'$\lim_{n_\nu \rightarrow \infty} \, \chi(\mathbf{0}) \approx $' + \
'${:3.4f}$'.format(y0))
plt.tight_layout()
plt.savefig('figure_bse.svg')
plt.show()
# TPRF. If not, see <http://www.gnu.org/licenses/>.
#
################################################################################
from common import *
from pytriqs.plot.mpl_interface import oplot, oplotr, plt
with HDFArchive('data_g2.h5', 'r') as a:
p = a['p']
plt.figure(figsize=(3.25 * 2.2, 2))
subp = [1, 3, 1]
opt = dict(cmap=plt.get_cmap('terrain_r'), vmin=0.0, vmax=0.01)
plt.subplot(*subp)
subp[-1] += 1
plt.title(r'$\chi^{(0)}_m$')
plt.imshow(np.squeeze(p.chi0_m.data).real, **opt)
plt.colorbar()
plt.subplot(*subp)
subp[-1] += 1
plt.title(r'$\chi_m$')
plt.imshow(np.squeeze(p.chi_m.data).real, **opt)
plt.colorbar()
plt.subplot(*subp)
subp[-1] += 1
plt.title(r'$\Gamma_m - U$')
plt.imshow((np.squeeze(p.gamma_m.data) - p.U).real,
cmap=plt.get_cmap('RdBu_r'),
vmin=-5,
vmax=5)
plt.colorbar()
from pytriqs.applications.susceptibility.fourier import chi4_iw_from_tau
chi4_iw = chi4_iw_from_tau(chi4_tau, nw)
from pytriqs.applications.susceptibility.fourier import chi4_tau_from_iw
chi4_tau_ref = chi4_tau_from_iw(chi4_iw, nt)
np.testing.assert_array_almost_equal(chi4_tau_ref.data, chi4_tau.data)
# ------------------------------------------------------------------
if False:
from pytriqs.plot.mpl_interface import oplot, plt
subp = [2, 2, 1]
plt.subplot(*subp)
subp[-1] += 1
plt.title('chi4_tau')
cut = chi4_tau[[0, all, all]]
plt.pcolormesh(cut.data[:, :, 0, 0, 0, 0].real)
plt.axis('square')
plt.subplot(*subp)
subp[-1] += 1
plt.title('chi4_tau_ref')
cut = chi4_tau_ref[[0, all, all]]
plt.pcolormesh(cut.data[:, :, 0, 0, 0, 0].real)
plt.axis('square')
cidx = 5 # cut idx
cut = chi4_iw[[cidx, all, all]]
plt.subplot(*subp)
from pytriqs.operators import n
from pytriqs.operators.util.op_struct import set_operator_structure
from pytriqs.plot.mpl_interface import oplot, oplotr, oploti, plt
# ----------------------------------------------------------------------
from brew_dmft.ParameterCollection import ParameterCollection
# ----------------------------------------------------------------------
if __name__ == '__main__':
U = 5.0
plt.figure(figsize=(3.25, 2 * 3))
plt.title('Static Magnetic Susceptibility' + '\n' +
r'half-filled Hubbard atom $U=%2.2f$' % U)
# ------------------------------------------------------------------
# -- Analytic result
T = np.logspace(-3, 2, num=400)
beta = 1. / T
# -- Analytic magnetization expecation value
# -- and static susceptibility
Z = 2. + 2 * np.exp(-beta * 0.5 * U)
m2 = 0.25 * (2 / Z)
chi_m = 2. * beta * m2
plt.plot(1. / beta, chi_m, '-k', lw=0.5)
chi0w0[qidx_lin] = chiw
# -- Plot static w=0 susceptibility in k-space
from pytriqs.plot.mpl_interface import oplot, oploti, oplotr, plt
# plot zeroth bosonic matsubara freq susceptibility
qx = np.array([q[0] for q in q_list])/np.pi
qy = np.array([q[1] for q in q_list])/np.pi
data = np.squeeze(chi0w0.data[iw_zero_idx])
data = -1.0 * data
vmax = np.max(data.real)
plt.title('Square-lattice ' + r'$\chi_0(q, \omega=0)$, $\beta=%2.2f$' % beta)
plt.pcolor(qx.reshape((n_k, n_k)), qy.reshape((n_k, n_k)), data.reshape((n_k, n_k)).real,
cmap='magma', vmin=0, vmax=vmax)
plt.colorbar()
plt.axis('equal')
plt.xlabel('$q_x/\pi$')
plt.ylabel('$q_y/\pi$')
plt.tight_layout()
plt.savefig('figure_chi0q_w0_square_latt.pdf')
# -- Plot Gamma and M point dynamic susceptibilities
opt = dict(vmin=-0.01, vmax=0.01, cmap='PuOr')
plt.figure(figsize=(12, 8))
ps = []
filenames = np.sort(glob.glob('data_B_*.h5'))
for filename in filenames:
with HDFArchive(filename, 'r') as a:
p = a['ps'].objects[-1]
ps.append(p)
ps = ParameterCollections(ps)
B, M = ps.B, ps.M
B = np.concatenate((-B[1:][::-1], B))
M = np.concatenate((-M[1:][::-1], M))
p = np.polyfit(M, B, 5)
m = np.linspace(-0.5, 0.5, num=1000)
b = np.polyval(p, m)
chi = 1. / np.polyval(np.polyder(p, 1), 0.).real
plt.figure(figsize=(3.25 * 1.5, 2.5 * 1.5))
plt.title(r'$\chi = \frac{dM}{dB}|_{B=0} \approx $' + '$ {:3.4f}$'.format(chi))
plt.plot(B, M, 'o', alpha=0.75, label='DMFT field')
plt.plot(b, m, '-', alpha=0.75, label='Poly fit')
plt.legend(loc='upper left')
plt.grid(True)
plt.xlabel(r'$B$')
plt.ylabel(r'$M$')
plt.xlim([B.min(), B.max()])
plt.ylim([-0.5, 0.5])
plt.tight_layout()
plt.savefig('figure_field.svg')
plt.show()
