def _count_bases(self, sequence):
"""PRIVATE: Return an array of base counts by column across all sequences
aggregated.
The array returned looks something like the following, when several
(n=2) sequences are aggregated:
array([[ 0., 1., 0., 1., 0.],
[ 0., 0., 0., 2., 0.],
[ 0., 0., 0., 2., 0.],
...
])
where each row represents a base position - thus row[0] is the count
for sequence position 0. The values within the vector give the counts
of each possible base where the index is given in self.nucleotide_positions
(in __init__):
self.nucleotide_positions = {'A':0, 'C':1, 'G':2, 'T':3, 'N':4}
Using numpy arrays lets us quickly sum across columns or rows, making
summary stats easier.
"""
for k, base in enumerate(sequence):
if numpy.ndim(self.bases) == 1 and k == 0:
self.bases[self.nucleotide_positions[base]] += 1
elif (numpy.ndim(self.bases) == 1) or (numpy.ndim(self.bases) > 1 and k == len(self.bases)):
self.bases = numpy.vstack((self.bases, numpy.zeros(5)))
self.bases[k][self.nucleotide_positions[base]] += 1
else:
self.bases[k][self.nucleotide_positions[base]] += 1
def sum_to_shape(X, s):
"""
Sum axes of the array such that the resulting shape is as given.
Thus, the shape of the result will be s or an error is raised.
"""
# First, sum and remove axes that are not in s
if np.ndim(X) > len(s):
axes = tuple(range(-np.ndim(X), -len(s)))
else:
axes = ()
Y = np.sum(X, axis=axes)
# Second, sum axes that are 1 in s but keep the axes
axes = ()
for i in range(-np.ndim(Y), 0):
if s[i] == 1:
if np.shape(Y)[i] > 1:
axes = axes + (i,)
else:
if np.shape(Y)[i] != s[i]:
raise ValueError("Shape %s can't be summed to shape %s" %
(np.shape(X), s))
Y = np.sum(Y, axis=axes, keepdims=True)
return Y
def __init__(self, x, y):
assert np.ndim(x)==2 and np.ndim(y)==2 and np.shape(x)==np.shape(y), \
'x and y must be 2D arrays of the same size.'
if np.any(np.isnan(x)) or np.any(np.isnan(y)):
x = np.ma.masked_where( (isnan(x)) | (isnan(y)) , x)
y = np.ma.masked_where( (isnan(x)) | (isnan(y)) , y)
self.x_vert = x
self.y_vert = y
mask_shape = tuple([n-1 for n in self.x_vert.shape])
self.mask_rho = np.ones(mask_shape, dtype='d')
# If maskedarray is given for verticies, modify the mask such that
# non-existant grid points are masked. A cell requires all four
# verticies to be defined as a water point.
if isinstance(self.x_vert, np.ma.MaskedArray):
mask = (self.x_vert.mask[:-1,:-1] | self.x_vert.mask[1:,:-1] | \
self.x_vert.mask[:-1,1:] | self.x_vert.mask[1:,1:])
self.mask_rho = np.asarray(~(~np.bool_(self.mask_rho) | mask), dtype='d')
if isinstance(self.y_vert, np.ma.MaskedArray):
mask = (self.y_vert.mask[:-1,:-1] | self.y_vert.mask[1:,:-1] | \
self.y_vert.mask[:-1,1:] | self.y_vert.mask[1:,1:])
self.mask_rho = np.asarray(~(~np.bool_(self.mask_rho) | mask), dtype='d')
self._calculate_subgrids()
self._calculate_metrics()
def prob_of_label(vol, labelvol):
"""
compute the probability of the labels in labelvol in each of the volumes in vols
Parameters:
vol (float numpy array of dim (nd + 1): volume with a prob dist at each voxel in a nd vols
labelvol (int numpy array of dim nd): nd volume of labels
Returns:
nd volume of probabilities
"""
# check dimensions
ndims = np.ndim(labelvol)
assert np.ndim(vol) == ndims + 1, "vol dimensions do not match [%d] vs [%d]" % (np.ndim(vol)-1, ndims)
shp = vol.shape
nb_voxels = np.prod(shp[0:ndims])
nb_labels = shp[-1]
# reshape volume to be [nb_voxels, nb_labels]
flat_vol = np.reshape(vol, (nb_voxels, nb_labels))
# normalize accross second dimension
rows_sums = flat_vol.sum(axis=1)
flat_vol_norm = flat_vol / rows_sums[:, np.newaxis]
# index into the flattened volume
idx = list(range(nb_voxels))
v = flat_vol_norm[idx, labelvol.flat]
return np.reshape(v, labelvol.shape)
def _test():
imdata = np.array([[1,2,3],[4,5,6]])
immask = imdata>2
print imdata
print immask
print imdata[immask]
print np.ndim(immask)
def reshape_skew(m, s=-1):
"""reshape n(n-1)/2 vector into nxn skew symm matrix or vice versa
indices in m are in row-major order (it's Python, babe)
when s == -1, returns skew-symmetric matrix
M = -M.T
when s == 1, returns symmetric matrix
M = M.T
"""
s = sign(s)
if ndim(m) == 1: # m is a vector, we need a matrix
n = 0.5*(1 + np.sqrt(1 + 8*len(m)))
if not (n==round(n)):
print "length of m doesn't lead to a square-sized matrix of size n(n-1)/2"
return
n = int(n)
out = zeros((n,n))
ind_start = 0
for i in xrange(n):
out[i,i+1:] = m[ind_start:ind_start+n-i-1]
ind_start += n-i-1
out += s*out.T
elif ndim(m) == 2: # m is a matrix, we need a vector
if not np.equal(*m.shape):
print "matrix m is not square"
return
if (norm(m - s*m.T)) > _small_number:
print "matrix m is not skew-symmetric or symmetric"
return
n = m.shape[0]
out = np.zeros(n*(n-1)/2)
ind_start = 0
for i in range(n):
out[ind_start:ind_start+n-i-1] = m[i,i+1:]
ind_start += n-i-1
return out
def py_vq(obs, code_book):
""" Python version of vq algorithm.
The algorithm computes the euclidian distance between each
observation and every frame in the code_book.
Parameters
----------
obs : ndarray
Expects a rank 2 array. Each row is one observation.
code_book : ndarray
Code book to use. Same format than obs. Should have same number of
features (eg columns) than obs.
Returns
-------
code : ndarray
code[i] gives the label of the ith obversation, that its code is
code_book[code[i]].
mind_dist : ndarray
min_dist[i] gives the distance between the ith observation and its
corresponding code.
Notes
-----
This function is slower than the C version but works for
all input types. If the inputs have the wrong types for the
C versions of the function, this one is called as a last resort.
It is about 20 times slower than the C version.
"""
# n = number of observations
# d = number of features
if np.ndim(obs) == 1:
if not np.ndim(obs) == np.ndim(code_book):
raise ValueError(
"Observation and code_book should have the same rank")
else:
return _py_vq_1d(obs, code_book)
else:
(n, d) = shape(obs)
# code books and observations should have same number of features and same
# shape
if not np.ndim(obs) == np.ndim(code_book):
raise ValueError("Observation and code_book should have the same rank")
elif not d == code_book.shape[1]:
raise ValueError("Code book(%d) and obs(%d) should have the same " \
"number of features (eg columns)""" %
(code_book.shape[1], d))
code = zeros(n, dtype=int)
min_dist = zeros(n)
for i in range(n):
dist = np.sum((obs[i] - code_book) ** 2, 1)
code[i] = argmin(dist)
min_dist[i] = dist[code[i]]
return code, sqrt(min_dist)
def SeparateStreets(lines):
# Separate Street Lines - Remove lines associated with horizon
# INPUT - CANNY IMAGE
# OUTPUT - LINES
if lines is None:
return None
# Handle 2 dimensions, or 3
new_lines = None
if np.ndim(lines) is 2:
new_lines = np.copy(lines)
elif np.ndim(lines) is 3:
new_lines = np.copy(lines[0])
else:
print 'Strange number of dimensions? in SeparateStreets()'
return new_lines
indices_for_removal = np.array([])
for i in range(np.shape(new_lines)[0]):
rho_theta = new_lines[i]
theta_degrees = rho_theta[1] * 180 / np.pi
# if isCloseToHorizontal(theta_degrees) or isCloseToVertical(theta_degrees):
if isMarkingsOfCurrentLane(theta_degrees): # and not isCloseToVertical(theta_degrees)
indices_for_removal = np.append(indices_for_removal, [i])
# print 'Removed:' + str(theta_degrees)
new_lines = np.delete(new_lines, indices_for_removal, axis=0)
return new_lines
def as2d(a):
if np.ndim(a) == 0:
return a[np.newaxis,np.newaxis]
elif np.ndim(a) == 1:
return a[:,np.newaxis]
else:
return a
def Zo(s):
if np.ndim(h) == 1:
s = s[:, np.newaxis]
if np.ndim(h) == 2:
s = s[:, np.newaxis, np.newaxis]
return (hc * s + C(s) * h) / (hc + h)
def GetLaneFromStdDeviation(cluster):
if cluster is None:
print "GetLaneFromMedian: cluster is empty"
return None
cluster_removed_outliers = RemoveOutliers(cluster)
if cluster_removed_outliers is None:
# IN THIS CASE NO VALUES ARE WITHIN ONE STD DEVIATION!
if np.ndim(cluster) is 1:
distances = cluster[0]
angles = cluster[1]
else:
distances = cluster[:, 0]
angles = cluster[:, 1]
# return None
# print 'Aww'
elif np.ndim(cluster_removed_outliers) is 1:
distances = cluster_removed_outliers[0]
angles = cluster_removed_outliers[1]
else:
distances = cluster_removed_outliers[:, 0]
angles = cluster_removed_outliers[:, 1]
avg_angle = np.mean(angles)
avg_distance = np.mean(distances)
return np.array([avg_distance, avg_angle])
def outer(A, B, ndim=1):
"""
Computes outer product over the last axes of A and B.
The other axes are broadcasted. Thus, if A has shape (..., N) and B has
shape (..., M), then the result has shape (..., N, M).
Using the argument `ndim` it is possible to change that how many axes
trailing axes are used for the outer product. For instance, if ndim=3, A and
B have shapes (...,N1,N2,N3) and (...,M1,M2,M3), the result has shape
(...,N1,M1,N2,M2,N3,M3).
"""
if not utils.is_integer(ndim) or ndim < 0:
raise ValueError('ndim must be non-negative integer')
if ndim > 0:
if ndim > np.ndim(A):
raise ValueError('Argument ndim larger than ndim of the first '
'parameter')
if ndim > np.ndim(B):
raise ValueError('Argument ndim larger than ndim of the second '
'parameter')
shape_A = np.shape(A) + (1,)*ndim
shape_B = np.shape(B)[:-ndim] + (1,)*ndim + np.shape(B)[-ndim:]
A = np.reshape(A, shape_A)
B = np.reshape(B, shape_B)
return A * B
def nan_detrend(x, y, deg=1):
"""Subtract a polynomial fit from the data, ignoring NaNs.
Parameters
----------
x : array_like
x data.
y : array_like
Data to detrend.
deg : int
Degree of polynomial to subtract. (Can be zero i.e. constant)
Returns
-------
y_out : numpy.array
Detrended data.
"""
y_out = np.nan*np.zeros_like(y)
if np.ndim(x) == 1:
nans = np.isnan(x) | np.isnan(y)
p = nan_polyfit(x, y, deg)
y_out[~nans] = y[~nans] - np.polyval(p, x[~nans])
elif np.ndim(x) == 2:
for i in xrange(x.shape[1]):
nans = np.isnan(x[:, i]) | np.isnan(y[:, i])
p = nan_polyfit(x[:, i], y[:, i], deg)
y_out[~nans, i] = y[~nans, i] - np.polyval(p, x[~nans, i])
else:
raise RuntimeError('Arguments must be 1 or 2 dimensional arrays.')
return y_out
def xcorr(x,y,**kwargs):
"""cross correlation by rfft"""
x = np.asarray(x)
y = np.asarray(y)
if np.ndim(x) == np.ndim(y):
shape=kwargs.get('shape',np.max((x.shape, y.shape), axis = 0))
return np.fft.irfftn(np.conjugate(np.fft.rfftn(x,s=shape))*np.fft.rfftn(y,s=shape))
elif np.ndim(y) == 1:
axis = kwargs.get('axis', 0)
shape=kwargs.get('shape', max(x.shape[axis], len(y)))
shape+=shape%2
outshape = np.array(x.shape[:])
outshape[axis] = shape
out = np.zeros(outshape)
y = np.fft.ifftshift(np.pad(y, pad_width = (int((shape-len(y)+1)/2), int((shape-len(y))/2)), mode = 'constant'))
y_fft = np.fft.rfft(y, n=shape)
x_fft = np.fft.rfft(x, n=shape, axis=axis)
if axis == 0:
for ii in range(len(x_fft[0])):
out[:,ii] = np.fft.irfft(x_fft[:,ii]*np.conjugate(y_fft))
else:
for ii in range(len(x_fft)):
out[ii] = np.fft.irfft(x_fft[ii]*np.conjugate(y_fft))
return out
else:
raise ValueError('Only inputs with dimensions of 1 or 2 can be processed.')
def _populate_vars(dz, zdr, kdp, rho, ldr, T, verbose):
"""
Check for presence of each var, and update dicts as needed.
Flattens multi-dimensional arrays to optimize processing.
The output array from csu_fhc_summer() will be re-dimensionalized later.
"""
varlist = [dz, zdr, kdp, rho, ldr, T]
keylist = ['DZ', 'DR', 'KD', 'RH', 'LD', 'T']
fhc_vars = {}
radar_data = {}
for i, key in enumerate(keylist):
var = varlist[i]
if var is not None:
if key == 'DZ':
shp = np.shape(var)
sz = np.size(var)
if np.ndim(var) > 1:
radar_data[key] = np.array(var).ravel().astype('float32')
elif np.ndim(var) == 1:
radar_data[key] = np.array(var).astype('float32')
else:
radar_data[key] = np.array([var]).astype('float32')
fhc_vars[key] = 1
else:
fhc_vars[key] = 0
if verbose:
print('USING VARIABLES: ', fhc_vars)
return radar_data, fhc_vars, shp, sz
def components(model,X):
"""
Given a Gaussian Mixture Model (GMM), returns the additive components of the model
Parameters
----------
model - GMM object fitted to the data; For e.g.,
from sklearn.mixture import GaussianMixture as GMM
model = GMM(n_components = 3).fit(X), where X is the input data
X - Array of size (n_samples,n_features) to which the GMM was fit.
Returns
-------
components - Array of size (n_samples,n_components); the Gaussian components weighted,
and added to fit the data
"""
import numpy as np
if np.ndim(X)==1:
X = X.reshape((-1,1))
#X = np.sort(X,axis = 0)
N = np.shape(X)[0]
X = np.array([np.linspace(np.min(feature),np.max(feature),N) for feature in X.T]).T
responsibilities = model.predict_proba(X)
pdf = np.exp(model.score_samples(X))
if np.ndim(pdf)==1:
pdf = pdf.reshape((-1,1))
comp = responsibilities*pdf
return comp
def nodes2elems(nodes, tri):
"""
Calculate a element centre value based on the average value for the
nodes from which it is formed. This necessarily involves an average,
so the conversion from nodes2elems and elems2nodes is not
necessarily reversible.
Parameters
----------
nodes : ndarray
Array of unstructured grid node values to move to the element
centres.
tri : ndarray
Array of shape (nelem, 3) comprising the list of connectivity
for each element.
Returns
-------
elems : ndarray
Array of values at the grid nodes.
"""
if np.ndim(nodes) == 1:
elems = nodes[tri].mean(axis=-1)
elif np.ndim(nodes) == 2:
elems = nodes[..., tri].mean(axis=-1)
else:
raise Exception('Too many dimensions (maximum of two)')
return elems
def _maskremove(self, img, mask, removeAction):
diff = mask.sum(axis=0)
diff = (diff > 0).sum().astype("int")
if (diff == 0):
return None
h, w = (0, 0)
if (np.ndim(img) == 3):
h, w, p = img.shape
elif np.ndim(img) == 2:
h, w = img.shape
else:
return None # Picture cannot be edit
efunc = self.getEnergyFunction(img)
efunc[mask > 0] = -abs(efunc.max()) * h * w # Be as little as possible so it cannot be reached otherwise.
res = img
for i in range(diff):
self.progress.emit(i * 100 / diff)
QtCore.QCoreApplication.processEvents()
seam = ML.findOptimalSeam(efunc,stopFunc=self._haveToQuit)
if (self._haveToQuit()):
return []
res = removeAction(res, seam)
efunc = ML.removeSeams(efunc, seam)
return res
def _applyImage(self, data):
img = data['img']
itera = self.itbox.value()
overl = self.olbox.value()
seams = []
if 'mask' in data:
mask = data['mask']
seams = self._findSeams(img, mask)
if self._haveToQuit():
return None
if (len(seams) == 0): # No Masking
diff = self.sbox.value()
h, w = (0, 0)
if (np.ndim(img) == 3):
h, w, p = img.shape
elif np.ndim(img) == 2:
h, w = img.shape
else:
return None # Picture cannot be edit
res = img
s = self.getEnergyFunction(img)
seams = ML.findTopDisjointSeams(s, diff, lambda i: self.progress.emit(i),stopFunc=self._haveToQuit)
if (self._haveToQuit()):
return None
res = ML.removeSeamsInGradient(res, seams, itera, overl,progressFunc=lambda i: self.progress.emit(i),stopFunc=self._haveToQuit)
return res
else:
return ML.removeSeamsInGradient(img, seams, itera, overl,progressFunc=lambda i: self.progress.emit(i),stopFunc=self._haveToQuit)
def convert_to_firing_rate(self, calciumtraces):
firingrate = []
denoisedcalicumtrace = []
for ii in xrange(0, np.size(calciumtraces, 1)):
fluor = calciumtraces[:, ii]
print 'Deconvolving..', ii
deconvolvedresult = constrained_foopsi(fluor)
print np.ndim(deconvolvedresult[5])
if np.ndim(deconvolvedresult[5]) > 1:
print 'Skipping..Cell ', ii
continue
firingrate.append(deconvolvedresult[5])
denoisedcalicumtrace.append(deconvolvedresult[0])
firingrate = np.asarray(np.vstack(firingrate)).T
denoisedcalicumtrace = np.asarray(np.vstack(denoisedcalicumtrace)).T
np.savetxt(os.path.join(self.WorkingDirectory, key + "_denoiseddata.csv"), denoisedcalicumtrace, delimiter=",")
np.savetxt(os.path.join(self.WorkingDirectory, key + "_firingrate.csv"), firingrate, delimiter=",")
plt.plot(np.clip(firingrate, 0, np.max(firingrate)), '.')
plt.savefig('/Users/seetha/Desktop/test1.png')
def _compute_moments(self, u_X):
"""
Tile the plates of the parent's moments.
"""
# Utilize broadcasting: If a tiled axis is unit length in u_X, there
# is no need to tile it.
u = list()
for ind in range(len(u_X)):
ui = u_X[ind]
shape_u = np.shape(ui)
if np.ndim(ui) > 0:
# Add variable dimensions
tiles_ind = tiles + (1,)*len(self.dims[ind])
# Utilize broadcasting: Do not tile leading empty axes
nd = min(len(tiles_ind), np.ndim(ui))
tiles_ind = tiles_ind[(-nd):]
# For simplicity, make tiles and shape equal length
(tiles_ind, shape_u) = misc.make_equal_length(tiles_ind,
shape_u)
# Utilize broadcasting: Use tiling only if the parent's
# moment has non-unit axis length.
tiles_ind = [tile if sh > 1 else 1
for (tile, sh) in zip(tiles_ind, shape_u)]
# Tile
ui = np.tile(ui, tiles_ind)
u.append(ui)
return u
def getMapping(self, mol):
(sel1, sel2) = self._getSelections(mol)
if np.ndim(sel1) == 2:
protatoms = np.ones(len(sel1)) * -1
for i in range(np.size(sel1, 1)):
protatoms[i] = np.where(sel1[i] == True)[0][0]
else:
protatoms = np.where(sel1)[0]
if np.ndim(sel2) == 2:
ligatoms = np.ones(len(sel1)) * -1
for i in range(np.size(sel2, 1)):
ligatoms[i] = np.where(sel2[i] == True)[0][0]
else:
ligatoms = np.where(sel2)[0]
numatoms1 = len(protatoms)
numatoms2 = len(ligatoms)
if np.array_equal(protatoms, ligatoms):
map = np.zeros((numatoms1 * (numatoms1-1) / 2, 2), dtype=int)
start = 0
for i in range(numatoms1):
finish = start + numatoms1 - i - 1
map[start:finish, 0] = protatoms[i]
map[start:finish, 1] = protatoms[i+1:]
start = finish
else:
map = np.zeros((numatoms1 * numatoms2, 2), dtype=int)
for i in range(numatoms2):
start = i * numatoms1
finish = (i+1) * numatoms1
map[start:finish, 0] = protatoms
map[start:finish, 1] = ligatoms[i]
return map
def read_h5_stack(fn, group='stack', crop=[None]*6, **kwargs):
"""Read a volume in HDF5 format into numpy.ndarray.
Parameters
----------
fn : string
The filename of the input HDF5 file.
group : string, optional (default 'stack')
The group within the HDF5 file containing the dataset.
crop : list of int, optional (default '[None]*6', no crop)
A crop to get of the volume of interest. Only available for 2D and 3D
volumes.
Returns
-------
stack : numpy ndarray
The stack contained in fn, possibly cropped.
"""
fn = os.path.expanduser(fn)
dset = h5py.File(fn, 'r')
if group not in dset:
raise ValueError("HDF5 file (%s) doesn't have group (%s)!" %
(fn, group))
a = dset[group]
if ndim(a) == 2:
xmin, xmax, ymin, ymax = crop[:4]
a = a[xmin:xmax, ymin:ymax]
elif ndim(a) == 3:
xmin, xmax, ymin, ymax, zmin, zmax = crop
a = a[xmin:xmax, ymin:ymax, zmin:zmax]
stack = array(a)
dset.close()
return stack
def sample_vMF(theta, kappa,size=1):
"""
Sampling from vMF
This is based on the implementation I found online here:
http://stats.stackexchange.com/questions/156729/sampling-from-von-mises-fisher-distribution-in-python
(**** NOTE THE FIX BY KEVIN *****)
which is based on :
Directional Statistics (Mardia and Jupp, 1999) and on the Ulrich-Wood's algorithm for sampling.
"""
warn('Not sure about sampling vMF, use with caution!!!! ')
#print "kappa : ", kappa
#print "norm direction :" , np.linalg.norm(theta)
np.testing.assert_array_almost_equal( np.linalg.norm(theta) , 1 )
#print "kappa : ", kappa
assert kappa > 0 , "kappa must be positive !"
if np.ndim(theta)==2:
theta = np.squeeze(theta)
assert np.ndim(theta)==1, "theta should be one one-dimensional!"
res_sampling = _rvMF(size, kappa * theta)
return np.vstack(res_sampling)
def helper():
flist = glob.iglob(os.path.join(directory, "*.img"))
flist = list(itertools.ifilter(lambda f: os.path.getmtime(f) > time0[0],
flist))
if not flist:
return
flist.sort(key=os.path.getmtime)
fpath = flist[-1]
time0[0] = os.path.getmtime(fpath)
data = open_img(fpath).data
data = np.rot90(data, -1)
if np.ndim(iw.image)==2 and iw.image.shape==data.shape:
newdata = np.concatenate([data[np.newaxis], iw.image[np.newaxis]],
axis=0)
elif np.ndim(iw.image)==3 and iw.image.shape[1:3]==data.shape:
newdata = np.concatenate([data[np.newaxis], iw.image], axis=0)
elif np.ndim(data)==2:
newdata = data
else:
return
print fpath
iw.setImage(newdata, autoLevels=False)
iw.labels.insert(0, fpath)
iw.win.setWindowTitle(fpath)
def sparse_jac_repeat(tape_tag, x, nnz, rind, cind, values):
"""
computes sparse Jacobian J for a function F:R^N -> R^M with
the sparsity pattern that has been computed previously (e.g. by calling sparse_jac_no_repeat)
I guess it also reuses the options that have been set previously. So it would be not necessary to set the options again.
[nnz, rind, cind, values] = sparse_jac_repeat(tape_tag, x, rind, cind, values)
INPUT:
The base point x at which the Jacobian should be computed, i.e. J = dF(x)/dx
OUTPUT:
nnz is the guessed number of nonzeros in the Jacobian. This can be larger than the true number of nonzeros.
sparse matrix representation in standard format:
rind is an nnz-array of row indices
cind is an nnz-array of column indices
values are the corresponding Jacobian entries
"""
assert type(tape_tag) == int
assert type(nnz) == int
assert numpy.ndim(x) == 1
assert numpy.ndim(rind) == 1
assert numpy.ndim(cind) == 1
assert numpy.ndim(values) == 1
x = numpy.asarray(x, dtype=float)
rind = numpy.asarray(rind, dtype=numpy.uint32)
cind = numpy.asarray(cind, dtype=numpy.uint32)
values = numpy.asarray(values, dtype=float)
return _colpack.sparse_jac_repeat(tape_tag, x, nnz, rind, cind, values)
def fastdtw(x, y, dist):
"""
Computes Dynamic Time Warping (DTW) of two sequences in a faster way.
Instead of iterating through each element and calculating each distance,
this uses the cdist function from scipy (https://docs.scipy.org/doc/scipy/reference/generated/scipy.spatial.distance.cdist.html)
:param array x: N1*M array
:param array y: N2*M array
:param string or func dist: distance parameter for cdist. When string is given, cdist uses optimized functions for the distance metrics.
If a string is passed, the distance function can be 'braycurtis', 'canberra', 'chebyshev', 'cityblock', 'correlation', 'cosine', 'dice', 'euclidean', 'hamming', 'jaccard', 'kulsinski', 'mahalanobis', 'matching', 'minkowski', 'rogerstanimoto', 'russellrao', 'seuclidean', 'sokalmichener', 'sokalsneath', 'sqeuclidean', 'wminkowski', 'yule'.
Returns the minimum distance, the cost matrix, the accumulated cost matrix, and the wrap path.
"""
assert len(x)
assert len(y)
if ndim(x)==1:
x = x.reshape(-1,1)
if ndim(y)==1:
y = y.reshape(-1,1)
r, c = len(x), len(y)
D0 = zeros((r + 1, c + 1))
D0[0, 1:] = inf
D0[1:, 0] = inf
D1 = D0[1:, 1:]
D0[1:,1:] = cdist(x,y,dist)
C = D1.copy()
for i in range(r):
for j in range(c):
D1[i, j] += min(D0[i, j], D0[i, j+1], D0[i+1, j])
if len(x)==1:
path = zeros(len(y)), range(len(y))
elif len(y) == 1:
path = range(len(x)), zeros(len(x))
else:
path = _traceback(D0)
return D1[-1, -1] / sum(D1.shape), C, D1, path
def project(self, *args, **kwargs):
""" Project molecule.
Parameters
----------
mol : :class:`Molecule <htmd.molecule.molecule.Molecule>`
A :class:`Molecule <htmd.molecule.molecule.Molecule>` object to project.
Returns
-------
data : np.ndarray
An array containing the projected data.
"""
# -------------- DEPRECATION PATCH --------------
if isinstance(self, np.ndarray) or isinstance(self, Molecule):
from warnings import warn
warn('Static use of the project method will be deprecated in the next version of HTMD. '
'Please change your projection code according to the tutorials on www.htmd.org')
data = _MetricDistanceOld.project(self, *args, **kwargs)
logger.warning('Static use of the project method will be deprecated in the next version of HTMD. '
'Please change your projection code according to the tutorials on www.htmd.org')
return data
# ------------------ CUT HERE -------------------
mol = args[0]
(sel1, sel2) = self._getSelections(mol)
if np.ndim(sel1) == 1 and np.ndim(sel2) == 1: # normal distances
metric = pp_calcDistances(mol, sel1, sel2, self.metric, self.threshold, self.pbc, truncate=self.truncate)
else: # minimum distances by groups
metric = pp_calcMinDistances(mol, sel1, sel2)
return metric
def interpolate_1x1(lon, lat, data, lon0=0.):
""" interpolate on a standard grid
"""
# already standard
if is_standard_grid(lon, lat, lon0=lon0):
return lon, lat, data
#
lon, data = rectify_longitude_data(lon, data, lon0)
res = 1
nx = int(360/res)
ny = int(180/res)
lon360 = np.linspace(lon0+0.5,lon0+359.5,nx)
lat180 = np.linspace(-89.5,89.5,ny)
print "Interpolate onto a standard 1deg grid...",
if np.ndim(data) == 2:
if isinstance(data, np.ma.MaskedArray):
data = data.filled(np.nan)
data = interp2(lon, lat, data, lon360,lat180, order=0)
lon, lat = lon360, lat180
elif np.ndim(data) == 3:
nt = np.size(data,0)
data180x360 = np.zeros((nt,ny,nx))
for i in range(nt):
data180x360[i,:,:] = interp2(lon, lat, np.squeeze(data[i,:,:]), lon360,lat180)
lon, lat, data = lon360, lat180, data180x360
print "Done"
return lon, lat, data
def transformImage(self, containerImage):
if type(containerImage) is not type(self.sourceImage):
raise TypeError
if np.ndim(containerImage) is not np.ndim(self.sourceImage):
raise ValueError
self.homography = Homography(sourcePoints=self.sourcePoints, targetPoints=self.targetPoints, effect=self.effect)
x = [f[0] for f in self.targetPoints]
y = [s[1] for s in self.targetPoints]
rowmin, rowmax = min(y), max(y) + 1
colmin, colmax = min(x), max(x) + 1
if self.effect != None:
self.sourcePoints = [(0,0), (self.sbound[1], 0), (0, self.sbound[0]), (self.sbound[1], self.sbound[0])]
self.homography = Homography(sourcePoints=self.sourcePoints, targetPoints=self.targetPoints, effect=self.effect)
else:
self.homography = Homography(sourcePoints=self.sourcePoints, targetPoints=self.targetPoints, effect=self.effect)
rbs = interpolate.RectBivariateSpline(np.arange(0.0, self.sbound[0]), np.arange(0.0, self.sbound[1]), self.sourceImage, kx=1, ky=1)
# Identify the target bounding box.
# For every point within the box, perform an inverse projection of the coordinates.
for i in np.arange(rowmin, rowmax):
for j in np.arange(colmin, colmax):
a = j, i
px, py = self.homography.inverseProject(a)
if 0 <= px and px <= self.sbound[1] - 1 and 0 <= py and py <= self.sbound[0] - 1:
# read value of source and use 2D interpolation
containerImage[i][j] = rbs(py, px)
return containerImage
def skyann(map,
xcent,
ycent,
rinn,
rout,
mask=None,
clip_low=None,
clip_high=3.0):
ny, nx = map.shape
nobj = xcent.size
skylev = numpy.empty_like(xcent)
skyrms = numpy.empty_like(xcent)
for iobj in range(nobj):
# Extract coords for this object and convert to zero-based.
if numpy.ndim(xcent) == 0:
thisxcent = xcent - 1
else:
thisxcent = xcent[iobj] - 1
if numpy.ndim(ycent) == 0:
thisycent = ycent - 1
else:
thisycent = ycent[iobj] - 1
# Bounds.
rb = rout + 0.5
xmin = int(math.floor(thisxcent - rb))
if xmin < 0:
xmin = 0
xmax = int(math.ceil(thisxcent + rb))
if xmax >= nx:
xmax = nx - 1
ymin = int(math.floor(thisycent - rb))
if ymin < 0:
ymin = 0
ymax = int(math.ceil(thisycent + rb))
if ymax >= ny:
ymax = ny - 1
# Extract what we need.
thismap = map[ymin:ymax + 1, xmin:xmax + 1]
if mask is not None:
thismask = mask[ymin:ymax + 1, xmin:xmax + 1]
else:
thismask = None
xtmp = numpy.arange(xmin, xmax + 1)
ytmp = numpy.arange(ymin, ymax + 1)
xx = numpy.tile(xtmp, (ymax - ymin + 1, 1))
yy = numpy.transpose(numpy.tile(ytmp, (xmax - xmin + 1, 1)))
# Make mask for desired annulus.
rr = numpy.hypot(xx - thisxcent, yy - thisycent)
ww = numpy.logical_and(rr >= rinn, rr <= rout)
annmap = thismap[ww]
if thismask is not None:
annmask = thismask[ww]
else:
annmask = None
# Compute sky level.
thisskylev, thisskyrms = skylevel(annmap,
mask=annmask,
clip_low=clip_low,
clip_high=clip_high)
if numpy.ndim(xcent) == 0:
skylev = thisskylev
skyrms = thisskyrms
else:
skylev[iobj] = thisskylev
skyrms[iobj] = thisskyrms
return skylev, skyrms
def gradient(f, *varargs, axis=None, edge_order=1):
f = np.asanyarray(f)
N = f.ndim # number of dimensions
axes = axis
del axis
if axes is None:
axes = tuple(range(N))
else:
axes = normalize_axis_tuple(axes, N)
len_axes = len(axes)
n = len(varargs)
if n == 0:
# no spacing argument - use 1 in all axes
dx = [1.0] * len_axes
elif n == 1 and np.ndim(varargs[0]) == 0:
# single scalar for all axes
dx = varargs * len_axes
elif n == len_axes:
# scalar or 1d array for each axis
dx = list(varargs)
for i, distances in enumerate(dx):
if np.ndim(distances) == 0:
continue
elif np.ndim(distances) != 1:
raise ValueError("distances must be either scalars or 1d")
if len(distances) != f.shape[axes[i]]:
raise ValueError(
"when 1d, distances must match the "
"length of the corresponding dimension"
)
diffx = np.diff(distances)
# if distances are constant reduce to the scalar case
# since it brings a consistent speedup
if (diffx == diffx[0]).all():
diffx = diffx[0]
dx[i] = diffx
else:
raise TypeError("invalid number of arguments")
if edge_order > 2:
raise ValueError("'edge_order' greater than 2 not supported")
# use central differences on interior and one-sided differences on the
# endpoints. This preserves second order-accuracy over the full domain.
outvals = []
# create slice objects --- initially all are [:, :, ..., :]
slice1 = [slice(None)] * N
slice2 = [slice(None)] * N
slice3 = [slice(None)] * N
slice4 = [slice(None)] * N
otype = f.dtype.char
if otype not in ["f", "d", "F", "D", "m", "M"]:
otype = "d"
# Difference of datetime64 elements results in timedelta64
if otype == "M":
# Need to use the full dtype name because it contains unit
# information
otype = f.dtype.name.replace("datetime", "timedelta")
elif otype == "m":
# Needs to keep the specific units, can't be a general unit
otype = f.dtype
# Convert datetime64 data into ints. Make dummy variable `y`
# that is a view of ints if the data is datetime64, otherwise
# just set y equal to the array `f`.
if f.dtype.char in ["M", "m"]:
y = f.view("int64")
else:
y = f
for i, axis in enumerate(axes):
if y.shape[axis] < edge_order + 1:
raise ValueError(
"Shape of array too small to calculate a numerical "
"gradient, at least (edge_order + 1) elements are "
"required."
)
# result allocation
out = np.empty_like(y, dtype=otype)
uniform_spacing = np.ndim(dx[i]) == 0
# Numerical differentiation: 2nd order interior
slice1[axis] = slice(1, -1)
slice2[axis] = slice(None, -2)
slice3[axis] = slice(1, -1)
slice4[axis] = slice(2, None)
if uniform_spacing:
out[slice1] = (f[slice4] - f[slice2]) / (2.0 * dx[i])
else:
dx1 = dx[i][0:-1]
dx2 = dx[i][1:]
a = -(dx2) / (dx1 * (dx1 + dx2))
b = (dx2 - dx1) / (dx1 * dx2)
c = dx1 / (dx2 * (dx1 + dx2))
# fix the shape for broadcasting
shape = np.ones(N, dtype=int)
shape[axis] = -1
a.shape = b.shape = c.shape = shape
# 1D equivalent --
# out[1:-1] = a * f[:-2] + b * f[1:-1] + c * f[2:]
out[slice1] = a * f[slice2] + b * f[slice3] + c * f[slice4]
# Numerical differentiation: 1st order edges
if edge_order == 1:
slice1[axis] = 0
slice2[axis] = 1
slice3[axis] = 0
dx_0 = dx[i] if uniform_spacing else dx[i][0]
# 1D equivalent -- out[0] = (y[1] - y[0]) / (x[1] - x[0])
out[slice1] = (y[slice2] - y[slice3]) / dx_0
slice1[axis] = -1
slice2[axis] = -1
slice3[axis] = -2
dx_n = dx[i] if uniform_spacing else dx[i][-1]
# 1D equivalent -- out[-1] = (y[-1] - y[-2]) / (x[-1] - x[-2])
out[slice1] = (y[slice2] - y[slice3]) / dx_n
# Numerical differentiation: 2nd order edges
else:
slice1[axis] = 0
slice2[axis] = 0
slice3[axis] = 1
slice4[axis] = 2
if uniform_spacing:
a = -1.5 / dx[i]
b = 2.0 / dx[i]
c = -0.5 / dx[i]
else:
dx1 = dx[i][0]
dx2 = dx[i][1]
a = -(2.0 * dx1 + dx2) / (dx1 * (dx1 + dx2))
b = (dx1 + dx2) / (dx1 * dx2)
c = -dx1 / (dx2 * (dx1 + dx2))
# 1D equivalent -- out[0] = a * y[0] + b * y[1] + c * y[2]
out[slice1] = a * y[slice2] + b * y[slice3] + c * y[slice4]
slice1[axis] = -1
slice2[axis] = -3
slice3[axis] = -2
slice4[axis] = -1
if uniform_spacing:
a = 0.5 / dx[i]
b = -2.0 / dx[i]
c = 1.5 / dx[i]
else:
dx1 = dx[i][-2]
dx2 = dx[i][-1]
a = (dx2) / (dx1 * (dx1 + dx2))
b = -(dx2 + dx1) / (dx1 * dx2)
c = (2.0 * dx2 + dx1) / (dx2 * (dx1 + dx2))
# 1D equivalent -- out[-1] = a * f[-3] + b * f[-2] + c * f[-1]
out[slice1] = a * y[slice2] + b * y[slice3] + c * y[slice4]
outvals.append(out)
# reset the slice object in this dimension to ":"
slice1[axis] = slice(None)
slice2[axis] = slice(None)
slice3[axis] = slice(None)
slice4[axis] = slice(None)
if len_axes == 1:
return outvals[0]
else:
return outvals
def apply_along_axis(obj, func, axis=None, skipna=False, args=(), **kwargs):
""" Apply along-axis numpy method to DimArray
apply_along_axis(obj, ...)
Where ... are the parameters below:
parameters:
----------
- func: numpy function name (`str`)
- {axis}
- {skipna}
- args : variable list of arguments before "axis"
- kwargs : variable dict of keyword arguments after "axis"
returns:
--------
- DimArray, or scalar
Examples:
>>> a = DimArray([[0,1],[2,3.]])
>>> b = a.copy()
>>> b[0,0] = np.nan
>>> c = DimArray.from_arrays([a,b],keys=['a','b'],axis='items')
>>> c
dimarray: 7 non-null elements (1 null)
dimensions: 'items', 'x0', 'x1'
0 / items (2): a to b
1 / x0 (2): 0 to 1
2 / x1 (2): 0 to 1
array([[[ 0., 1.],
[ 2., 3.]],
<BLANKLINE>
[[ nan, 1.],
[ 2., 3.]]])
>>> c.sum(axis=0)
dimarray: 3 non-null elements (1 null)
dimensions: 'x0', 'x1'
0 / x0 (2): 0 to 1
1 / x1 (2): 0 to 1
array([[ nan, 2.],
[ 4., 6.]])
>>> c.sum(0, skipna=True)
dimarray: 4 non-null elements (0 null)
dimensions: 'x0', 'x1'
0 / x0 (2): 0 to 1
1 / x1 (2): 0 to 1
array([[ 0., 2.],
[ 4., 6.]])
>>> c.median(0)
dimarray: 3 non-null elements (1 null)
dimensions: 'x0', 'x1'
0 / x0 (2): 0 to 1
1 / x1 (2): 0 to 1
array([[ nan, 1.],
[ 2., 3.]])
"""
# Deal with `axis` parameter, whether `int`, `str` or `tuple`
obj, idx, name = _deal_with_axis(obj, axis)
# Apply numpy function, dealing with NaNs
result = _apply_along_axis(obj.values,
func,
axis=idx,
skipna=skipna,
args=(),
**kwargs)
if type(func) is str:
funcname = func
func = getattr(np, func)
else:
funcname = func.__name__
# If `axis` was None (operations on the flattened array), just returns the numpy array
if axis is None or not isinstance(result, np.ndarray):
return result
#
# New axes
#
# standard case: collapsed axis
if np.ndim(result) == obj.ndim - 1:
newaxes = [ax for ax in obj.axes if ax.name != name]
# cumulative functions: axes remain unchanged
elif funcname in ('cumsum', 'cumprod', 'gradient'):
newaxes = obj.axes.copy()
# diff: reduce axis size by one
elif funcname == "diff":
oldaxis = obj.axes[idx]
newaxis = oldaxis[1:] # assume backward differencing
newaxes = obj.axes.copy()
newaxes[idx] = newaxis
# axes do not fit for some reason
else:
raise Exception("cannot find new axes for this transformation: " +
repr(funcname))
newobj = obj._constructor(result, newaxes, **obj._metadata)
# add stamp
#stamp = "{transform}({axis})".format(transform=funcname, axis=str(obj.axes[idx]))
#newobj._metadata_stamp(stamp)
return newobj
def __reverse_indexing(slices, m_child, plates, dims):
"""
A helpful function for performing reverse indexing/slicing
"""
j = -1 # plate index for parent
i = -1 # plate index for child
child_slices = ()
parent_slices = ()
msg_plates = ()
# Compute plate axes in the message from children
ndim = len(dims)
if ndim > 0:
m_plates = np.shape(m_child)[:-ndim]
else:
m_plates = np.shape(m_child)
for s in reversed(slices):
if misc.is_scalar_integer(s):
# Case: integer
parent_slices = (s, ) + parent_slices
msg_plates = (plates[j], ) + msg_plates
j -= 1
elif s is None:
# Case: newaxis
if -i <= len(m_plates):
child_slices = (0, ) + child_slices
i -= 1
elif isinstance(s, slice):
# Case: slice
if -i <= len(m_plates):
child_slices = (slice(None), ) + child_slices
parent_slices = (s, ) + parent_slices
if ((-i > len(m_plates) or m_plates[i] == 1)
and slicelen(s) == plates[j]):
# Broadcasting can be applied. The message does not need
# to be explicitly shaped to the full size
msg_plates = (1, ) + msg_plates
else:
# No broadcasting. Must explicitly form the full size
# axis
msg_plates = (plates[j], ) + msg_plates
j -= 1
i -= 1
else:
raise RuntimeError(
"BUG: Unknown index type. Should capture earlier.")
# Set the elements of the message
m_parent = np.zeros(msg_plates + dims)
if np.ndim(m_parent) == 0 and np.ndim(m_child) == 0:
m_parent = m_child
elif np.ndim(m_parent) == 0:
m_parent = m_child[child_slices]
elif np.ndim(m_child) == 0:
m_parent[parent_slices] = m_child
else:
m_parent[parent_slices] = m_child[child_slices]
return m_parent
def unpack_array(self, M):
""" OrderedDict.unpack_array(array)
unpacks an input 1d vector or 2d column array into the data dictionary
following the same order that it was unpacked
important that the structure of the data dictionary, and the shapes
of the contained values are the same as the data from which the
array was packed
Inputs:
array - either a 1D vector or 2D column array
Outputs:
a reference to self, updates self in place
"""
# dont require dict to have numpy
import numpy as np
from VyPy.tools.arrays import atleast_2d_col, array_type, matrix_type
# check input type
vector = np.ndim(M) == 1
# valid types for output
valid_types = (int, float, array_type, matrix_type)
# counter for unpacking
_index = [0]
# the unpacking function
def do_unpack(D):
for k, v in D.iteritems():
# type checking
if isinstance(v, OrderedDict):
do_unpack(v) # recursion!
continue
elif not isinstance(v, valid_types):
continue
# get this value's rank
rank = np.ndim(v)
# get unpack index
index = _index[0]
# skip if too big
if rank > 2:
continue
# scalars
elif rank == 0:
if vector:
D[k] = M[index]
index += 1
else: #array
continue
#raise RuntimeError , 'array size mismatch, all values in data must have same number of rows for array unpacking'
# 1d vectors
elif rank == 1:
n = len(v)
if vector:
D[k][:] = M[index:(index + n)]
index += n
else: #array
D[k][:] = M[:, index]
index += 1
# 2d arrays
elif rank == 2:
n, m = v.shape
if vector:
D[k][:, :] = np.reshape(M[index:(index + (n * m))],
[n, m],
order='F')
index += n * m
else: #array
D[k][:, :] = M[:, index:(index + m)]
index += m
#: switch rank
_index[0] = index
#: for each itme
#: def do_unpack()
# do the unpack
do_unpack(self)
# check
if not M.shape[-1] == _index[0]:
raise IndexError, 'did not unpack all values'
# done!
return self
def to_fluxd(self, wfb, aper, eph, unit=None, **kwargs):
"""Express as spectral flux density in an observation.
Assumes the small angle approximation.
Parameters
----------
wfb : `~astropy.units.Quantity`, `~synphot.SpectralElement`, list
Wavelengths, frequencies, bandpass, or list of
bandpasses of the observation. Bandpasses require
`~synphot`. Ignored if ``S`` is provided.
aper: `~astropy.units.Quantity`, `~sbpy.activity.Aperture`
Aperture of the observation as a circular radius (length
or angular units), or as an sbpy `~sbpy.activity.Aperture`.
eph: dictionary-like, `~sbpy.data.Ephem`
Ephemerides of the comet. Required fields: 'rh', 'delta'.
Optional: 'phase'.
unit : `~astropy.units.Unit`, string, optional
The flux density unit for the output.
"""
# This method handles the geometric quantities. Sub-classes
# will handle the photometric quantities in `_source_fluxd`.
# rho = effective circular aperture radius at the distance of
# the comet. Keep track of array dimensionality as Ephem
# objects can needlessly increase the number of dimensions.
if isinstance(aper, Aperture):
rho = aper.coma_equivalent_radius()
ndim = np.ndim(rho)
else:
rho = aper
ndim = np.ndim(rho)
rho = rho.to('km', sbu.projected_size(eph))
ndim = max(ndim, np.ndim(self))
# validate unit
if unit is not None:
unit = u.Unit(unit)
# get source spectral flux density
# * sunlight for Afrho,
# * blackbody emission for Efrho
# quantity = (delta**2 * F / rho) / source
# must have spectral flux density units
source = self._source_fluxd(wfb, eph, unit=unit, **kwargs)
if isinstance(source, u.Magnitude):
_source = source.physical
else:
_source = source
fluxd = self * rho / eph['delta']**2 * _source
# using Ephem can unnecessarily promote fluxd to an array
if np.ndim(fluxd) > ndim:
fluxd = np.squeeze(fluxd)
# and back to magnitudes, as needed
return fluxd.to(source.unit)
def __call__(self, sample):
#--- transf must follow this order:
#--- translate -> rotate -> shear -> scale
ch, H, W = sample['image'].shape
#--- centering mat
C, Cm = np.eye(3), np.eye(3)
C[0, 2] = W / 2
C[1, 2] = H / 2
Cm[0, 2] = -W / 2
Cm[1, 2] = -H / 2
T = np.eye(3, 3)
#--- Translate:
if np.random.rand() < self.prob:
#--- normal distribution is used to translate the data, an small
#--- stdv is recomended in order to keep the data inside the image
#--- [0.001 < stdv < 0.02 is recomended]
T[0:2, 2] = np.random.rand(2) * [W, H] * self.t_stdv
#--- rotate
if torch.rand(1)[0] < self.prob:
#--- r_kappa value controls von mises "concentration", so to kepp
#--- the rotation under controlled parameters r_kappa=30 keeps
#--- theta around +-pi/8 (if mu=0.0)
D = np.eye(3)
theta = np.random.vonmises(0.0, self.r_kappa)
D[0:2, 0:2] = [[math.cos(theta), math.sin(theta)],
[-math.sin(theta),
math.cos(theta)]]
T = np.dot(np.dot(np.dot(T, C), D), Cm)
#--- Shear (vert and Horz)
if np.random.rand() < self.prob:
#--- under -pi/8 < theta < pi/8 range tan(theta) ~ theta, then
#--- computation of tan(theta) is ignored. kappa will be
#--- selected to comply this restriction [kappa ~> 20 is a good value]
theta = np.random.vonmises(0.0, self.sh_kappa)
D = np.eye(3)
D[0, 1] = theta
T = np.dot(np.dot(np.dot(T, C), D), Cm)
if np.random.rand() < self.prob:
theta = np.random.vonmises(0.0, self.sh_kappa)
D = np.eye(3)
D[1, 0] = theta
T = np.dot(np.dot(np.dot(T, C), D), Cm)
#--- scale
if np.random.rand() < self.prob:
#--- Use log_normal distribution with mu=0.0 to perform scale,
#--- since scale factor must be > 0, stdv is used to control the
#--- deviation from 1 [0.1 < stdv < 0.5 is recomended]
D = np.eye(3)
D[0, 0], D[1, 1] = np.exp(np.random.rand(2) * self.sc_stdv)
T = np.dot(np.dot(np.dot(T, C), D), Cm)
if (T == np.eye(3)).all():
return sample
else:
if np.ndim(sample['image']) > 2:
for t in sample['image']:
t[:] = affine_transform(t, T)
else:
sample['image'] = affine_transform(sample['image'], T)
if np.ndim(sample['label']) > 2:
#--- affine transform over label must keep values in the matrix
#--- then, no interpolation or adding is performed
for t in sample['label']:
t[:] = affine_transform(t, T, mode='nearest', order=0)
else:
sample['label'] = affine_transform(sample['label'],
T,
mode='nearest',
order=0)
return sample
def handle_scalar_broadcasting(nd, x, bdim):
assert isinstance(get_aval(x), ShapedArray)
if bdim is None or nd == onp.ndim(x):
return x
else:
return x.reshape(x.shape + (1,) * (nd - x.ndim))
def __init__(self, cov):
if numpy.ndim(cov) == 1:
self.cov = numpy.diag(numpy.array(cov, dtype=numpy.float64))
else:
self.cov = numpy.array(cov, dtype=numpy.float64)
def convert_julian(JD, ASTYPE=None, FORMAT='dict'):
"""
Converts from Julian day to calendar date and time
Translated from caldat in "Numerical Recipes in C", by William H. Press,
Brian P. Flannery, Saul A. Teukolsky, and William T. Vetterling.
Cambridge University Press, 1988 (second printing).
Hatcher, D. A., "Simple Formulae for Julian Day Numbers and Calendar Dates",
Quarterly Journal of the Royal Astronomical Society, 25(1), 1984.
Arguments
---------
JD: Julian Day (days since 01-01-4713 BCE at 12:00:00)
Keyword arguments
-----------------
ASTYPE: convert output to variable type
FORMAT: format of output variables
'dict': dictionary with variable keys
'tuple': tuple with variable order YEAR,MONTH,DAY,HOUR,MINUTE,SECOND
'zip': aggregated variable sets
Returns
-------
year: calendar year
month: calendar month
day: day of the month
hour: hour of the day
minute: minute of the hour
second: second of the minute
"""
#-- convert to array if only a single value was imported
if (np.ndim(JD) == 0):
JD = np.atleast_1d(JD)
SINGLE_VALUE = True
else:
SINGLE_VALUE = False
JDO = np.floor(JD + 0.5)
C = np.zeros_like(JD)
#-- calculate C for dates before and after the switch to Gregorian
IGREG = 2299161.0
ind1, = np.nonzero(JDO < IGREG)
C[ind1] = JDO[ind1] + 1524.0
ind2, = np.nonzero(JDO >= IGREG)
B = np.floor((JDO[ind2] - 1867216.25) / 36524.25)
C[ind2] = JDO[ind2] + B - np.floor(B / 4.0) + 1525.0
#-- calculate coefficients for date conversion
D = np.floor((C - 122.1) / 365.25)
E = np.floor((365.0 * D) + np.floor(D / 4.0))
F = np.floor((C - E) / 30.6001)
#-- calculate day, month, year and hour
DAY = np.floor(C - E + 0.5) - np.floor(30.6001 * F)
MONTH = F - 1.0 - 12.0 * np.floor(F / 14.0)
YEAR = D - 4715.0 - np.floor((7.0 + MONTH) / 10.0)
HOUR = np.floor(24.0 * (JD + 0.5 - JDO))
#-- calculate minute and second
G = (JD + 0.5 - JDO) - HOUR / 24.0
MINUTE = np.floor(G * 1440.0)
SECOND = (G - MINUTE / 1440.0) * 86400.0
#-- convert all variables to output type (from float)
if ASTYPE is not None:
YEAR = YEAR.astype(ASTYPE)
MONTH = MONTH.astype(ASTYPE)
DAY = DAY.astype(ASTYPE)
HOUR = HOUR.astype(ASTYPE)
MINUTE = MINUTE.astype(ASTYPE)
SECOND = SECOND.astype(ASTYPE)
#-- if only a single value was imported initially: remove singleton dims
if SINGLE_VALUE:
YEAR = YEAR.item(0)
MONTH = MONTH.item(0)
DAY = DAY.item(0)
HOUR = HOUR.item(0)
MINUTE = MINUTE.item(0)
SECOND = SECOND.item(0)
#-- return date variables in output format (default python dictionary)
if (FORMAT == 'dict'):
return dict(year=YEAR,
month=MONTH,
day=DAY,
hour=HOUR,
minute=MINUTE,
second=SECOND)
elif (FORMAT == 'tuple'):
return (YEAR, MONTH, DAY, HOUR, MINUTE, SECOND)
elif (FORMAT == 'zip'):
return zip(YEAR, MONTH, DAY, HOUR, MINUTE, SECOND)
def tt_approximation(self, fun, shape):
'''
Approximation of a tensor of order d in tensor train format based on a
Principal Component Analysis.
For a prescribed precision, set TPCA.max_rank = np.inf and TPCA.tol to
the desired precision (possibly an array of length d-1).
For a prescribed rank, set TPCA.tol = np.inf and TPCA.max_rank to the
desired rank (possibly an array of length d-1).
See also the documentation of the class
TensorPrincipalComponentAnalysis.
Parameters
----------
fun : fun or tensap.Function
Function of d variables i_1, ..., i_d which returns the entries of
the tensor.
shape : list or numpy.ndarray
The shape of the tensor.
Raises
------
ValueError
If the provided tolerance and max ranks are not correct.
Returns
-------
tensap.TreeBasedTensor
A tensor in tree based format with a linear tree.
dict
Dictionnary containing the outputs of the method.
'''
solver = deepcopy(self)
d = len(shape)
tree = tensap.DimensionTree.linear(d)
is_active_node = np.full(tree.nb_nodes, True)
is_active_node[tree.dim2ind[1:] - 1] = False
rep_tt = np.nonzero(is_active_node)[0]
rep_tt = np.flip(rep_tt[1:])
if np.ndim(self.tol) == 1 and len(self.tol) == d - 1:
tol = solver.tol
solver.tol = np.zeros(tree.nb_nodes)
solver.tol[rep_tt] = tol
elif np.ndim(self.tol) == 1 and len(self.tol) > 1:
raise ValueError('tol should be a scalar or an array of length ' +
'd-1.')
if np.ndim(self.max_rank) == 1 and len(self.max_rank) == d - 1:
rank = solver.max_rank
solver.max_rank = np.zeros(tree.nb_nodes)
solver.max_rank[rep_tt] = rank
elif np.ndim(self.max_rank) == 1 and len(self.max_rank) > 1:
raise ValueError('max_rank should be a scalar or an array of ' +
'length d-1.')
return solver.tree_based_approximation(fun, shape, tree,
is_active_node)
def is_python_scalar(x):
try:
return x.aval.weak_type and np.ndim(x) == 0
except AttributeError:
return type(x) in python_scalar_dtypes
def gpu_strs(gpus):
if gpus is not None and np.ndim(gpus) == 0:
gpus = [gpus]
return ['/cpu:0'] if gpus is None else ['/gpu:%d' % x for x in gpus]
def tree_based_approximation(self, fun, shape, tree, is_active_node=None):
'''
Approximation of a tensor of order d in tree based tensor format based
on a Principal Component Analysis.
For a prescribed precision, set TPCA.max_rank = np.inf and TPCA.tol to
the desired precision (possibly an array of length d-1).
For a prescribed rank, set TPCA.tol = np.inf and TPCA.max_rank to the
desired rank (possibly an array of length d-1).
See also the documentation of the class
TensorPrincipalComponentAnalysis.
Parameters
----------
fun : fun or tensap.Function
Function of d variables i_1, ..., i_d which returns the entries of
the tensor.
shape : list or numpy.ndarray
The shape of the tensor.
tree : tensap.DimensionTree
The required dimension tree.
is_active_node : list or numpy.ndarray, optional
An array of booleans indicating which nodes of the tree are active.
The default is None, settings all the nodes active.
Raises
------
ValueError
If the provided tolerance and max ranks are not correct.
Returns
-------
tensap.TreeBasedTensor
A tensor in tree based format.
dict
Dictionnary containing the outputs of the method.
'''
solver = deepcopy(self)
d = len(shape)
if is_active_node is None:
is_active_node = np.full(tree.nb_nodes, True)
if (np.ndim(self.tol) == 0 or len(self.tol) == 1) and self.tol < 1:
solver.tol /= np.sqrt(np.count_nonzero(is_active_node) - 1)
if np.ndim(self.tol) == 0 or len(self.tol) == 1:
solver.tol = np.full(tree.nb_nodes, solver.tol)
elif len(self.tol) != tree.nb_nodes:
raise ValueError('tol should be a scalar or an array of length ' +
'tree.nb_nodes.')
if np.ndim(self.max_rank) == 0 or len(self.max_rank) == 1:
solver.max_rank = np.full(tree.nb_nodes, self.max_rank)
elif len(self.max_rank) != tree.nb_nodes:
raise ValueError('max_rank should be a scalar or an array of ' +
'length tree.nb_nodes.')
grids = [np.reshape(np.arange(x), (-1, 1)) for x in shape]
alpha_basis = np.empty(tree.nb_nodes, dtype=object)
alpha_grids = np.empty(tree.nb_nodes, dtype=object)
outputs = np.empty(tree.nb_nodes, dtype=object)
samples = np.empty(tree.nb_nodes, dtype=object)
tensors = [[]] * tree.nb_nodes
number_of_evaluations = 0
for nu in range(d):
alpha = tree.dim2ind[nu]
B_alpha = np.eye(shape[nu])
if is_active_node[alpha - 1]:
tol_alpha = np.min(
(solver.tol[alpha - 1], solver.max_rank[alpha - 1]))
pc_alpha, outputs[alpha-1] = \
solver.alpha_principal_components(fun, shape, nu,
tol_alpha, B_alpha,
grids[nu])
samples[alpha - 1] = outputs[alpha - 1]['samples']
shape_alpha = [shape[nu], pc_alpha.shape[1]]
tensors[alpha - 1] = tensap.FullTensor(pc_alpha, 2,
shape_alpha)
B_alpha = np.matmul(B_alpha, pc_alpha)
I_alpha = tensap.magic_indices(B_alpha)[0]
alpha_grids[alpha - 1] = grids[nu][I_alpha, :]
alpha_basis[alpha - 1] = B_alpha[I_alpha, :]
number_of_evaluations += outputs[alpha -
1]['number_of_evaluations']
if solver.display:
print('alpha = %i : rank = %i, nb_eval = %i' %
(alpha, shape_alpha[-1],
outputs[alpha - 1]['number_of_evaluations']))
else:
alpha_grids[alpha - 1] = grids[nu]
alpha_basis[alpha - 1] = B_alpha
for level in np.arange(np.max(tree.level), 0, -1):
for alpha in np.intersect1d(tree.nodes_with_level(level),
tree.internal_nodes):
S_alpha = tree.children(alpha)
B_alpha = TensorPrincipalComponentAnalysis.\
_tensor_product_b_alpha(alpha_basis[S_alpha-1])
alpha_grids[alpha-1] = \
tensap.FullTensorGrid(alpha_grids[S_alpha-1]).array()
tol_alpha = np.min(
(solver.tol[alpha - 1], solver.max_rank[alpha - 1]))
pc_alpha, outputs[alpha-1] = \
solver.alpha_principal_components(fun, shape,
tree.dims[alpha-1],
tol_alpha,
B_alpha,
alpha_grids[alpha-1])
samples[alpha - 1] = outputs[alpha - 1]['samples']
shape_alpha = np.concatenate(
([x.shape[1]
for x in alpha_basis[S_alpha - 1]], [pc_alpha.shape[1]]))
tensors[alpha - 1] = tensap.FullTensor(pc_alpha,
len(S_alpha) + 1,
shape_alpha)
B_alpha = np.matmul(B_alpha, pc_alpha)
I_alpha = tensap.magic_indices(B_alpha)[0]
alpha_grids[alpha - 1] = alpha_grids[alpha - 1][I_alpha, :]
alpha_basis[alpha - 1] = B_alpha[I_alpha, :]
number_of_evaluations += outputs[alpha -
1]['number_of_evaluations']
if solver.display:
print('alpha = %i : rank = %i, nb_eval = %i' %
(alpha, shape_alpha[-1],
outputs[alpha - 1]['number_of_evaluations']))
alpha = tree.root
S_alpha = tree.children(alpha)
B_alpha = TensorPrincipalComponentAnalysis.\
_tensor_product_b_alpha(alpha_basis[S_alpha-1])
I_alpha = tensap.FullTensorGrid(alpha_grids[S_alpha - 1]).array()
shape_alpha = [x.shape[1] for x in alpha_basis[S_alpha - 1]]
ind = [np.nonzero(tree.dims[alpha - 1] == x)[0][0] for x in range(d)]
tensors[alpha - 1] = tensap.FullTensor(
np.linalg.solve(B_alpha, fun(I_alpha[:, ind])), len(S_alpha),
shape_alpha)
alpha_grids[alpha - 1] = I_alpha
number_of_evaluations += I_alpha.shape[0]
samples[alpha - 1] = I_alpha
if solver.display:
print('Interpolation - nb_eval = %i' % I_alpha.shape[0])
f = tensap.TreeBasedTensor(tensors, tree)
output = {
'number_of_evaluations': number_of_evaluations,
'samples': samples,
'alpha_basis': alpha_basis,
'alpha_grids': alpha_grids,
'outputs': outputs
}
return f, output
def propagate(
fn: _tp.Callable,
x: _tp.Union[float, _Indexable[float]],
cov: _tp.Union[float, _Indexable[float], _Indexable[_Indexable[float]]],
**kwargs,
) -> _tp.Tuple[np.ndarray, np.ndarray]:
"""
Numerically propagates the covariance of function inputs to function outputs.
The function computes C' = J C J^T, where C is the covariance matrix of the input,
C' the matrix of the output, and J is the Jacobi matrix of first derivatives of the
mapping function fn. The Jacobi matrix is computed numerically.
Parameters
----------
fn: callable
Function that computes y = fn(x). x and y are each allowed to be scalars or
one-dimensional arrays.
x: float or array-like with shape (N,)
Input vector.
cov: float or array-like with shape (N,) or shape(N, N)
Covariance matrix of input vector. If the array is one-dimensional, it is
interpreted as the diagonal of a covariance matrix with zero off-diagonal
elements.
**kwargs:
Extra arguments are passed to :func:`jacobi`.
Returns
-------
y, ycov
y is the result of fn(x).
ycov is the propagated covariance matrix.
If ycov is a matrix, unless y is a number. In that case, ycov is also
reduced to a number.
"""
x = np.array(x)
y = fn(x)
jac = jacobi(fn, x, **kwargs)[0]
x_nd = np.ndim(x)
y_nd = np.ndim(y)
x_len = len(x) if x_nd == 1 else 1
y_len = len(y) if y_nd == 1 else 1
jac_nd = np.ndim(jac)
if jac_nd == 0:
jac = np.atleast_2d(jac)
elif jac_nd == 1:
jac = jac.reshape((y_len, x_len))
xcov = np.atleast_1d(cov)
xcov_nd = np.ndim(xcov)
if xcov.shape[0] != x_len:
raise ValueError("x and cov have incompatible shapes")
ycov = np.einsum("il,kl,l" if xcov_nd == 1 else "ij,kl,jl", jac, jac, xcov)
if np.ndim(y) == 0:
ycov = ycov[0, 0]
return y, ycov
def hopca(self, fun, shape):
'''
Return the set of alpha-principal components of an algebraic tensor,
for all alpha in {0,1,...,d-1}.
For prescribed precision, set TPCA.max_rank = np.inf and TPCA.tol to
the desired precision (possibly an array of length d).
For prescribed rank, set TPCA.tol = np.inf and TPCA.max_rank to the
desired rank (possibly an array of length d).
See also the documentation of the class
TensorPrincipalComponentAnalysis.
Parameters
----------
fun : fun or tensap.Function
Function of d variables i_1, ..., i_d which returns the entries of
the tensor.
shape : list or numpy.ndarray
The shape of the tensor.
Raises
------
ValueError
If the provided tolerance and max ranks are not correct.
Returns
-------
f_pc : list
List of the alpha-principal components of the tensor.
output : list
List containing the outputs of the method
alpha_principal_components.
'''
solver = deepcopy(self)
d = len(shape)
if np.ndim(self.tol) == 0 or len(self.tol) == 1:
solver.tol = np.full(d, self.tol)
elif len(self.tol) != d:
raise ValueError('tol should be a scalar or an array of length d.')
if np.ndim(self.max_rank) == 0 or len(self.max_rank) == 1:
solver.max_rank = np.full(d, self.max_rank)
elif len(self.max_rank) != d:
raise ValueError('max_rank should be a scalar or an array of ' +
'length d.')
f_pc = []
output = []
for alpha in range(d):
I_alpha = np.reshape(np.arange(shape[alpha]), (-1, 1))
B_alpha = np.eye(shape[alpha])
tol_alpha = np.min((solver.tol[alpha], solver.max_rank[alpha]))
f_pc_alpha, output_alpha = \
solver.alpha_principal_components(fun, shape, alpha, tol_alpha,
B_alpha, I_alpha)
f_pc.append(f_pc_alpha)
output.append(output_alpha)
return f_pc, output
def _batch_reducible_process(
self, element: types.Extracts) -> Sequence[types.Extracts]:
"""Invokes the tfjs model on the provided inputs and stores the result."""
result = copy.copy(element)
result[constants.PREDICTIONS_KEY] = []
batched_features = collections.defaultdict(list)
feature_rows = element[constants.FEATURES_KEY]
for r in feature_rows:
for key, value in r.items():
if value.dtype == np.int64:
value = value.astype(np.int32)
batched_features[key].append(value)
for spec in self._eval_config.model_specs:
model_name = spec.name if len(
self._eval_config.model_specs) > 1 else ''
if model_name not in self._loaded_models:
raise ValueError(
'model for "{}" not found: eval_config={}'.format(
spec.name, self._eval_config))
model_features = {}
for k in self._model_properties[model_name]['inputs']:
k_name = k.split(':')[0]
if k_name not in batched_features:
raise ValueError(
'model requires feature "{}" not available in '
'input.'.format(k_name))
dim = self._model_properties[model_name]['inputs'][k]
elems = []
for i in batched_features[k_name]:
if np.ndim(i) > len(dim):
raise ValueError(
'ranks for input "{}" are not compatible '
'with the model.'.format(k_name))
# TODO(dzats): See if we can support case where multiple dimensions
# are not defined.
elems.append(np.reshape(i, dim))
model_features[k] = elems
model_features = {
k: np.concatenate(v)
for k, v in model_features.items()
}
batched_entries = collections.defaultdict(list)
for feature, value in model_features.items():
batched_entries[_DATA_JSON].append(value.tolist())
batched_entries[_DTYPE_JSON].append(str(value.dtype))
batched_entries[_SHAPE_JSON].append(value.shape)
batched_entries[_TF_INPUT_NAME_JSON].append(feature)
cur_subdir = str(uuid.uuid4())
cur_input_path = os.path.join(
self._model_properties[model_name]['path'], _EXAMPLES_SUBDIR,
cur_subdir)
tf.io.gfile.makedirs(cur_input_path)
for entry, value in batched_entries.items():
with tf.io.gfile.GFile(os.path.join(cur_input_path, entry),
'w') as f:
f.write(json.dumps(value))
cur_output_path = os.path.join(
self._model_properties[model_name]['path'], _OUTPUTS_SUBDIR,
cur_subdir)
tf.io.gfile.makedirs(cur_output_path)
inference_command = [
self._binary_path, '--model_path=' + os.path.join(
self._model_properties[model_name]['path'], _MODEL_JSON),
'--inputs_dir=' + cur_input_path,
'--outputs_dir=' + cur_output_path
]
popen = subprocess.Popen(inference_command,
stdin=subprocess.PIPE,
stdout=subprocess.PIPE,
stderr=subprocess.PIPE)
stdout, stderr = popen.communicate()
if popen.returncode != 0:
raise ValueError(
'Inference failed with status {}\nstdout:\n{}\nstderr:\n{}'
.format(popen.returncode, stdout, stderr))
try:
with tf.io.gfile.GFile(
os.path.join(cur_output_path, _DATA_JSON)) as f:
data = json.load(f)
with tf.io.gfile.GFile(
os.path.join(cur_output_path, _DTYPE_JSON)) as f:
dtype = json.load(f)
with tf.io.gfile.GFile(
os.path.join(cur_output_path, _SHAPE_JSON)) as f:
shape = json.load(f)
except FileNotFoundError as e:
raise FileNotFoundError(
'Unable to find files containing inference result. This likely '
'means that inference did not succeed. Error {}'.format(e))
name = [
n.split(':')[0]
for n in self._model_properties[model_name]['outputs'].keys()
]
tf.io.gfile.rmtree(cur_input_path)
tf.io.gfile.rmtree(cur_output_path)
outputs = {}
for n, s, t, d in zip(name, shape, dtype, data):
d_val = [d[str(i)] for i in range(len(d))]
outputs[n] = np.reshape(np.array(d_val, t), s)
for v in outputs.values():
if len(v) != len(feature_rows):
raise ValueError(
'Did not get the expected number of results.')
for i in range(len(feature_rows)):
output = {k: v[i] for k, v in outputs.items()}
if len(output) == 1:
output = list(output.values())[0]
if len(self._eval_config.model_specs) == 1:
result[constants.PREDICTIONS_KEY].append(output)
else:
if i >= len(result[constants.PREDICTIONS_KEY]):
result[constants.PREDICTIONS_KEY].append({})
result[constants.PREDICTIONS_KEY][i].update(
{spec.name: output})
return [result]
def jacobi(
fn: _tp.Callable,
x: _tp.Union[int, float, _tp.Sequence],
*args,
method: _tp.Optional[int] = None,
mask: _tp.Optional[np.ndarray] = None,
rtol: float = 0,
maxiter: int = 10,
maxgrad: int = 3,
step: _tp.Optional[_tp.Tuple[float, float]] = None,
diagnostic: _tp.Optional[dict] = None,
):
"""
Return first derivative and its error estimate.
Parameters
----------
fn : Callable
Function with the signature `fn(x, *args)`, where `x` is a number or an
array of numbers and `*args` are optional auxiliary arguments.
x : Number or array of numbers
The derivative is computed with respect to `x`. If `x` is an array, the Jacobi
matrix is computed with respect to each element of `x`.
*args : tuple
Additional arguments passed to the function.
method : {-1, 0, 1} or None, optional
Whether to compute central (0), forward (1) or backward derivatives (-1).
The default (None) uses auto-detection.
mask : array or None, optional
If `x` is an array and `mask` is not None, compute the Jacobi matrix only for the
part of the array selected by the mask.
rtol : float, optional
Relative tolerance for the derivative. The algorithm stops when this relative
tolerance is reached. If 0 (the default), the algorithm iterates until the
error estimate of the derivative does not improve further.
maxiter : int, optional
Maximum number of iterations of the algorithm.
maxgrad : int, optional
Maximum grad of the extrapolation polynomial.
step : tuple of float or None, optional
Factors that reduce the step size in each iteration relative to the previous
step.
diagnostic : dict or None, optional
If an empty dict is passed to this keyword, it is filled with diagnostic
information produced by the algorithm. This reduces performance and is only
intended for debugging.
Returns
-------
array, array
Derivative and its error estimate.
"""
if maxiter <= 0:
raise ValueError("invalid value for keyword maxiter")
if maxgrad < 0:
raise ValueError("invalid value for keyword maxgrad")
if step is not None:
if not (0 < step[0] < 0.5):
raise ValueError("invalid value for step[0]")
if not (0 < step[1] < 1):
raise ValueError("invalid value for step[1]")
squeeze = np.ndim(x) == 0
x = np.atleast_1d(x).astype(float)
assert x.ndim == 1
x_indices = np.arange(len(x))
if mask is not None:
x_indices = x_indices[mask]
nx = len(x_indices)
if isinstance(diagnostic, dict):
diagnostic["method"] = np.zeros(nx, dtype=np.int8)
diagnostic["iteration"] = np.zeros(len(x_indices), dtype=np.uint8)
if method is not None and method not in (-1, 0, 1):
raise ValueError("invalid value for keyword method")
f0 = None
jac = None
err = None
for ik, k in enumerate(x_indices):
# if step is None, use optimal step sizes for central derivatives
h = _steps(x[k], step or (0.25, 0.5), maxiter)
# if method is None, auto-detect for each x[k]
md, f0, r = _first(method, f0, fn, x, k, h[0], args)
if diagnostic:
diagnostic["method"][ik] = md
if md != 0 and step is None:
# optimal step sizes for forward derivatives
h = _steps(x[k], (0.125, 0.125), maxiter)
r_shape = np.shape(r)
r = np.reshape(r, -1)
nr = len(r)
re = np.full(nr, np.inf)
todo = np.ones(nr, dtype=bool)
fd = [r]
if jac is None:
jac = np.empty(r_shape + (nx, ), dtype=r.dtype)
err = np.empty(r_shape + (nx, ), dtype=r.dtype)
if diagnostic:
diagnostic["call"] = np.zeros((nr, nx), dtype=np.uint8)
if diagnostic:
diagnostic["call"][:, ik] = 2 if md == 0 else 3
for i in range(1, len(h)):
fdi = _derive(md, f0, fn, x, k, h[i], args)
fdi = np.reshape(fdi, -1)
fd.append(fdi if i == 1 else fdi[todo])
if diagnostic:
diagnostic["call"][todo, ik] += 2
diagnostic["iteration"][ik] += 1
# polynomial fit with one extra degree of freedom
grad = min(i - 1, maxgrad)
start = i - (grad + 1)
stop = i + 1
q, c = np.polyfit(h[start:stop]**2,
fd[start:],
grad,
rcond=None,
cov=True)
ri = q[-1]
# pulls have roughly unit variance, however,
# the pull distribution is not gaussian and looks
# more like student's t
rei = c[-1, -1]**0.5
# update estimates that have significantly smaller error
sub_todo = rei < re[todo]
todo1 = todo.copy()
todo[todo1] = sub_todo
r[todo] = ri[sub_todo]
re[todo] = rei[sub_todo]
# do not improve estimates further which meet the tolerance
if rtol > 0:
sub_todo &= rei > rtol * np.abs(ri)
todo[todo1] = sub_todo
if np.sum(todo) == 0:
break
# shrink previous vectors of estimates
fd = [fdi[sub_todo] for fdi in fd]
jac[..., ik] = r.reshape(r_shape)
err[..., ik] = re.reshape(r_shape)
if diagnostic:
diagnostic["call"].shape = r_shape + (nx, )
if squeeze:
if diagnostic:
diagnostic["call"] = np.squeeze(diagnostic["call"])
jac = np.squeeze(jac)
err = np.squeeze(err)
return jac, err
def xcor(list_of_wls,
list_of_orders,
wlm,
fxm,
drv,
RVrange,
plot=False,
list_of_errors=None):
"""
This routine takes a combined dataset (in the form of lists of wl spaces,
spectral orders and possible a matching list of errors on those spectal orders),
as well as a template (wlm,fxm) to cross-correlate with, and the cross-correlation
parameters (drv,RVrange). The code takes on the order of ~10 minutes for an entire
HARPS dataset, which appears to be superior to my old IDL pipe.
The CCF used is the Geneva-style weighted average; not the Pearson CCF. Therefore
it measures true 'average' planet lines, with flux on the y-axis of the CCF.
The template must therefore be (something close to) a binary mask, with values
inside spectral lines (the CCF is scale-invariant so their overall scaling
doesn't matter),
It returns the RV axis and the resulting CCF in a tuple.
Thanks to Brett Morris (bmorris3), this code now implements a clever numpy broadcasting trick to
instantly apply and interpolate the wavelength shifts of the model template onto
the data grid in 2 dimensions. The matrix multiplication operator (originally
recommended to me by Matteo Brogi) allowed this 2D template matrix to be multiplied
with a 2D spectral order. np.hstack() is used to concatenate all orders end to end,
effectively making a giant single spectral order (with NaNs in between due to masking).
All these steps have eliminated ALL the forloops from the equation, and effectuated a
speed gain of a factor between 2,000 and 3,000. The time to do cross correlations is now
typically measured in 100s of milliseconds rather than minutes.
This way of calculation does impose some strict rules on NaNs, though. To keep things fast,
NaNs are now used to set the interpolated template matrix to zero wherever there are NaNs in the data.
These NaNs are found by looking at the first spectrum in the stack, with the assumption that
every NaN is in an all-NaN column. In the standard cross-correlation work-flow, isolated
NaNs are interpolated over (healed), after all.
The places where there are NaN columns in the data are therefore set to 0 in the template matrix.
The NaN values themselves are then set to to an arbitrary value, since they will never
weigh into the average by construction.
Parameters
----------
list_of_wls : list
List of wavelength axes of the data.
list_of_orders : list
List of corresponding 2D orders.
list_of_errors : list
Optional, list of corresponding 2D error matrices.
wlm : np.ndarray
Wavelength axis of the template.
fxm : np.ndarray
Weight-axis of the template.
drv : int,float
The velocity step onto which the CCF is computed. Typically ~1 km/s.
RVrange : int,float
The velocity range in the positive and negative direction over which to
evaluate the CCF. Typically >100 km/s.
plot : bool
Set to True for diagnostic plotting.
Returns
-------
RV : np.ndarray
The radial velocity grid over which the CCF is evaluated.
CCF : np.ndarray
The weighted average flux in the spectrum as a function of radial velocity.
CCF_E : np.ndarray
Optional. The error on each CCF point propagated from the error on the spectral values.
Tsums : np.ndarray
The sum of the template for each velocity step. Used for normalising the CCFs.
"""
import tayph.functions as fun
import astropy.constants as const
import tayph.util as ut
from tayph.vartests import typetest, dimtest, postest, nantest
import numpy as np
import scipy.interpolate
import astropy.io.fits as fits
import matplotlib.pyplot as plt
import sys
import pdb
#===FIRST ALL SORTS OF TESTS ON THE INPUT===
if len(list_of_wls) != len(list_of_orders):
raise ValueError(
f'In xcor(): List of wls and list of orders have different length ({len(list_of_wls)} & {len(list_of_orders)}).'
)
dimtest(wlm, [len(fxm)], 'wlm in ccf.xcor()')
typetest(wlm, np.ndarray, 'wlm in ccf.xcor')
typetest(fxm, np.ndarray, 'fxm in ccf.xcor')
typetest(drv, [int, float], 'drv in ccf.xcor')
typetest(
RVrange,
float,
'RVrange in ccf.xcor()',
)
postest(RVrange, 'RVrange in ccf.xcor()')
postest(drv, 'drv in ccf.xcor()')
nantest(wlm, 'fxm in ccf.xcor()')
nantest(fxm, 'fxm in ccf.xcor()')
nantest(drv, 'drv in ccf.xcor()')
nantest(RVrange, 'RVrange in ccf.xcor()')
drv = float(drv)
N = len(list_of_wls) #Number of orders.
if np.ndim(list_of_orders[0]) == 1.0:
n_exp = 1
else:
n_exp = len(list_of_orders[0][:, 0]) #Number of exposures.
#===Then check that all orders indeed have n_exp exposures===
for i in range(N):
if len(list_of_orders[i][:, 0]) != n_exp:
raise ValueError(
f'In xcor(): Not all orders have {n_exp} exposures.')
#===END OF TESTS. NOW DEFINE CONSTANTS===
c = const.c.to('km/s').value #In km/s
RV = fun.findgen(
2.0 * RVrange / drv +
1) * drv - RVrange #..... CONTINUE TO DEFINE THE VELOCITY GRID
beta = 1.0 - RV / c #The doppler factor with which each wavelength is to be shifted.
n_rv = len(RV)
#===STACK THE ORDERS IN MASSIVE CONCATENATIONS===
stack_of_orders = np.hstack(list_of_orders)
stack_of_wls = np.concatenate(list_of_wls)
if list_of_errors is not None:
stack_of_errors = np.hstack(list_of_errors) #Stack them horizontally
#Check that the number of NaNs is the same in the orders as in the errors on the orders;
#and that they are in the same place; meaning that if I add the errors to the orders, the number of
#NaNs does not increase (NaN+value=NaN).
if (np.sum(np.isnan(stack_of_orders)) != np.sum(
np.isnan(stack_of_errors + stack_of_orders))) and (np.sum(
np.isnan(stack_of_orders)) != np.sum(
np.isnan(stack_of_errors))):
raise ValueError(
f"in CCF: The number of NaNs in list_of_orders and list_of_errors is not equal ({np.sum(np.isnan(list_of_orders))},{np.sum(np.isnan(list_of_errors))})"
)
#===HERE IS THE JUICY BIT===
shifted_wavelengths = stack_of_wls * beta[:, np.
newaxis] #2D broadcast of wl_data, each row shifted by beta[i].
T = scipy.interpolate.interp1d(wlm, fxm, bounds_error=False, fill_value=0)(
shifted_wavelengths) #...making this a 2D thing.
T[:, np.isnan(
stack_of_orders[0]
)] = 0.0 #All NaNs are assumed to be in all-NaN columns. If that is not true, the below nantest will fail.
T_sums = np.sum(T, axis=1)
#We check whether there are isolated NaNs:
n_nans = np.sum(np.isnan(stack_of_orders),
axis=0) #This is the total number of NaNs in each column.
n_nans[n_nans == len(
stack_of_orders
)] = 0 #Whenever the number of NaNs equals the length of a column, set the flag to zero.
if np.max(
n_nans
) > 0: #If there are any columns which still have NaNs in them, we need to crash.
raise ValueError(
f"in CCF: Not all NaN values are purely in columns. There are still isolated NaNs. Remove those."
)
stack_of_orders[np.isnan(
stack_of_orders)] = 47e20 #Set NaNs to arbitrarily high values.
CCF = stack_of_orders @ T.T / T_sums #Here it the entire cross-correlation. Over all orders and velocity steps. No forloops.
CCF_E = CCF * 0.0
#If the errors were provided, we do the same to those:
if list_of_errors is not None:
stack_of_errors[np.isnan(
stack_of_errors
)] = 42e20 #we have already tested that these NaNs are in the same place.
CCF_E = stack_of_errors**2 @ (
T.T / T_sums)**2 #This has been mathematically proven.
#===THAT'S ALL. TEST INTEGRITY AND RETURN THE RESULT===
nantest(
CCF, 'CCF in ccf.xcor()'
) #If anything went wrong with NaNs in the data, these tests will fail because the matrix operation @ is non NaN-friendly.
nantest(CCF_E, 'CCF_E in ccf.xcor()')
if list_of_errors != None:
return (RV, CCF, np.sqrt(CCF_E), T_sums)
return (RV, CCF, T_sums)
def check_dims(array):
if np.ndim(array) == 1:
array = np.expand_dims(array, 1)
return array
def get_samples(self, sampleIndices, featVect_orig, numSamples=10):
'''
Input featVect the complete feature vector
sampleIndices the raveled(!) indices which we want to sample
numSamples how many samples to draw
'''
featVect = np.copy(featVect_orig)
# to avoid mistakes, remove the feature values of the part that we want to sample
featVect.ravel()[sampleIndices.ravel()] = 0
# reshape inputs if necessary
if np.ndim(sampleIndices) == 1:
sampleIndices = sampleIndices.reshape(3, self.win_size,
self.win_size)
if np.ndim(featVect) == 1:
featVect = featVect.reshape(
[3, self.image_dims[0], self.image_dims[1]])
# get a patch surrounding the sample indices and the indices relative to that
patch, patchIndices = self._get_surr_patch(featVect, sampleIndices)
# For each color channel, we will conditionally sample pixel
# values from a multivariate distribution
samples = np.zeros((numSamples, 3, self.win_size * self.win_size))
for c in [0, 1, 2]:
patch_c = patch[c].ravel()
patchIndices_c = patchIndices[c].ravel()
# get the conditional mean and covariance
if self.padding_size == 0:
cond_mean = self.meanVects[c]
cond_cov = self.covMat[c]
else:
cond_mean, cond_cov = self._get_cond_params(
patch_c, patchIndices_c, c)
# sample from the conditional distribution
# samples = np.random.multivariate_normal(cond_mean, cond_cov, numSamples)
# -- FASTER:
dimGauss = self.win_size * self.win_size
# --- (1) find real matrix A such that AA^T=Sigma ---
A = np.linalg.cholesky(cond_cov)
# --- (2) get (numSamples) samples from a standard normal ---
z = np.random.normal(size=numSamples * dimGauss).reshape(
dimGauss, numSamples)
# --- (3) x=mu+Az ---
samples[:, c] = cond_mean[np.newaxis, :] + np.dot(A, z).T
samples = samples.reshape((numSamples, -1))
# get the min/max values for this particular sample
# (since the data is preprocessed these can be different for each pixel!)\
#print self.minMaxVals[0].shape
minVals_sample = self.minMaxVals[0].ravel()[sampleIndices.ravel()]
maxVals_sample = self.minMaxVals[1].ravel()[sampleIndices.ravel()]
# clip the values
for i in xrange(samples.shape[0]):
samples[i][samples[i] < minVals_sample] = minVals_sample[
samples[i] < minVals_sample]
samples[i][samples[i] > maxVals_sample] = maxVals_sample[
samples[i] > maxVals_sample]
return samples
def _handle_scalar_broadcasting(nd, x, d):
if d is not_mapped or nd == np.ndim(x):
return x
else:
return x.reshape(x.shape + (1, ) * (nd - np.ndim(x)))
# sort image file names according to how they were stacked (when labeled in Fiji)
files = [
fn for fn in os.listdir(os.curdir)
if (".jpg" in fn and "_labelled" not in fn)
]
files.sort(key=lambda f: int(''.join(filter(str.isdigit, f))))
#print(files)
comparisonbodyparts = list(set(DataCombined.columns.get_level_values(1)))
for index, imagename in enumerate(files):
image = io.imread(imagename)
plt.axis('off')
if np.ndim(image)==2:
h, w = np.shape(image)
else:
h, w, nc = np.shape(image)
plt.figure(
figsize=(w * 1. / 100 * scale, h * 1. / 100 * scale))
plt.subplots_adjust(
left=0, bottom=0, right=1, top=1, wspace=0, hspace=0)
# This is important when using data combined / which runs consecutively!
imindex = np.where(
np.array(DataCombined.index.values) == folder + '/' + imagename)[0]
plt.imshow(image, 'bone')
for cc, scorer in enumerate(Scorers):
def initialize(self,
inputs,
input_lengths,
mel_targets=None,
linear_targets=None,
pml_targets=None,
gta=False,
locked_alignments=None,
logs_enabled=True):
'''Initializes the model for inference.
Sets "pml_outputs", and "alignments" fields.
Args:
inputs: int32 Tensor with shape [N, T_in] where N is batch size, T_in is number of
steps in the input time series, and values are character IDs
input_lengths: int32 Tensor with shape [N] where N is batch size and values are the lengths
of each sequence in inputs.
mel_targets: float32 Tensor with shape [N, T_out, M] where N is batch size, T_out is number
of steps in the output time series, M is num_mels, and values are entries in the mel
spectrogram. Only needed for training.
linear_targets: float32 Tensor with shape [N, T_out, F] where N is batch_size, T_out is number
of steps in the output time series, F is num_freq, and values are entries in the linear
spectrogram. Only needed for training.
pml_targets: float32 Tensor with shape [N, T_out, P] where N is batch_size, T_out is number of
steps in the PML vocoder features trajectories, P is pml_dimension, and values are PML vocoder
features. Only needed for training.
gta: boolean flag that is set to True when ground truth alignment is required
locked_alignments: when explicit attention alignment is required, the locked alignments are passed in this
parameter and the attention alignments are locked to these values
logs_enabled: boolean flag that defaults to True, if False no construction logs output
'''
# fix the alignments shape to (batch_size, encoder_steps, decoder_steps) if not already including
# batch dimension
locked_alignments_ = locked_alignments
if locked_alignments_ is not None:
if np.ndim(locked_alignments_) < 3:
locked_alignments_ = np.expand_dims(locked_alignments_, 0)
with tf.variable_scope('inference') as scope:
is_training = pml_targets is not None
batch_size = tf.shape(inputs)[0]
hp = self._hparams
# Embeddings
embedding_table = tf.get_variable(
'embedding', [len(symbols), hp.embed_depth],
dtype=tf.float32,
initializer=tf.truncated_normal_initializer(stddev=0.5))
embedded_inputs = tf.nn.embedding_lookup(
embedding_table, inputs) # [N, T_in, embed_depth=256]
# Encoder
prenet_outputs = prenet(
embedded_inputs, is_training,
hp.prenet_depths) # [N, T_in, prenet_depths[-1]=128]
encoder_outputs = encoder_cbhg(
prenet_outputs,
input_lengths,
is_training, # [N, T_in, encoder_depth=256]
hp.encoder_depth)
# Attention
attention_mechanism = BahdanauAttention(hp.attention_depth,
encoder_outputs)
attention_cell = LockableAttentionWrapper(
GRUCell(hp.attention_depth),
attention_mechanism,
alignment_history=True,
locked_alignments=locked_alignments_,
output_attention=False,
name='attention_wrapper') # [N, T_in, attention_depth=256]
# Apply prenet before concatenation in AttentionWrapper.
prenet_cell = DecoderPrenetWrapper(attention_cell, is_training,
hp.prenet_depths)
# Concatenate attention context vector and RNN cell output into a 2*attention_depth=512D vector.
concat_cell = ConcatOutputAndAttentionWrapper(
prenet_cell) # [N, T_in, 2*attention_depth=512]
# Decoder (layers specified bottom to top):
decoder_cell = MultiRNNCell(
[
OutputProjectionWrapper(concat_cell, hp.decoder_depth),
ResidualWrapper(GRUCell(hp.decoder_depth)),
ResidualWrapper(GRUCell(hp.decoder_depth))
],
state_is_tuple=True) # [N, T_in, decoder_depth=256]
# Project onto r PML feature vectors (predict r outputs at each RNN step):
output_cell = OutputProjectionWrapper(
decoder_cell, hp.pml_dimension * hp.outputs_per_step)
decoder_init_state = output_cell.zero_state(batch_size=batch_size,
dtype=tf.float32)
if is_training or gta:
helper = TacoTrainingHelper(inputs, pml_targets,
hp.pml_dimension,
hp.outputs_per_step)
else:
helper = TacoTestHelper(batch_size, hp.pml_dimension,
hp.outputs_per_step)
(decoder_outputs,
_), final_decoder_state, _ = tf.contrib.seq2seq.dynamic_decode(
BasicDecoder(output_cell, helper, decoder_init_state),
maximum_iterations=hp.max_iters) # [N, T_out/r, P*r]
# Reshape outputs to be one output per entry
pml_outputs = tf.reshape(
decoder_outputs,
[batch_size, -1, hp.pml_dimension]) # [N, T_out, P]
# Grab alignments from the final decoder state:
alignments = tf.transpose(
final_decoder_state[0].alignment_history.stack(), [1, 2, 0])
self.inputs = inputs
self.input_lengths = input_lengths
self.pml_outputs = pml_outputs
self.alignments = alignments
self.pml_targets = pml_targets
self.attention_cell = attention_cell
if logs_enabled:
log('Initialized Tacotron model. Dimensions: ')
log(' embedding: %d' %
embedded_inputs.shape[-1])
log(' prenet out: %d' % prenet_outputs.shape[-1])
log(' encoder out: %d' %
encoder_outputs.shape[-1])
log(' attention out: %d' %
attention_cell.output_size)
log(' concat attn & out: %d' % concat_cell.output_size)
log(' decoder cell out: %d' % decoder_cell.output_size)
log(' decoder out (%d frames): %d' %
(hp.outputs_per_step, decoder_outputs.shape[-1]))
log(' decoder out (1 frame): %d' % pml_outputs.shape[-1])
def mnorm(m, axis=None):
"""norm of a matrix of vectors stacked along the *axis* dimension.
"""
if axis is None:
axis = np.ndim(m) - 1
return np.sqrt((m**2).sum(axis))
def _get_cond_params(self, surrPatch, inPatchIdx, channel):
'''
Input:
surrpatch the variables over which we have a distribution
inPatchIdx the index/indices from what we want to sample
Output:
cond_mean the conditional mean of the inner patch,
conditioned on the surrounding pixels
cond_cov the conditional covariance
'''
# get the part of the surrPacth vector which we use to condition the values on
x2 = np.delete(surrPatch, inPatchIdx)
# split the mean vector into mu1 and mu2 (matching what we want to sample/condition on)
mu1 = np.take(self.meanVects[channel], inPatchIdx)
mu2 = np.delete(self.meanVects[channel], inPatchIdx)
path_dotProdForMean = self.path_folder + '{}_cov{}_win{}_dotProdForMean_{}_{}'.format(
self.netname, self.patchSize, self.win_size, inPatchIdx[0],
inPatchIdx[-1])
# get the dot product for the mean (check if precomputed, otherwise do this first)
if not os.path.exists(path_dotProdForMean + '.npy'):
cov11 = self.covMats[channel][inPatchIdx][:, inPatchIdx]
cov12 = np.delete(
self.covMats[channel][inPatchIdx, :], inPatchIdx,
axis=1) if np.ndim(inPatchIdx > 1) else np.delete(
self.covMats[channel][inPatchIdx, :], inPatchIdx)
cov21 = np.delete(self.covMats[channel][:, inPatchIdx],
inPatchIdx,
axis=0)
cov22 = np.delete(np.delete(self.covMats[channel],
inPatchIdx,
axis=0),
inPatchIdx,
axis=1)
# compute the conditional mean and covariance
dotProdForMean = np.dot(cov12, scipy.linalg.inv(cov22))
np.save(path_dotProdForMean, dotProdForMean)
else:
dotProdForMean = np.load(path_dotProdForMean + '.npy')
# with the dotproduct, we can now evaluate the conditional mean
cond_mean = mu1 + np.dot(dotProdForMean, x2 - mu2)
path_condCov = self.path_folder + '{}_cov{}_win{}_cond_cov_{}_{}_indep'.format(
self.netname, self.patchSize, self.win_size, inPatchIdx[0],
inPatchIdx[-1])
# get the conditional covariance
if not os.path.exists(path_condCov + '.npy'):
cov11 = self.covMats[channel][inPatchIdx][:, inPatchIdx]
cov12 = np.delete(
self.covMats[channel][inPatchIdx, :], inPatchIdx,
axis=1) if np.ndim(inPatchIdx > 1) else np.delete(
self.covMat[inPatchIdx, :], inPatchIdx)
cov21 = np.delete(self.covMats[channel][:, inPatchIdx],
inPatchIdx,
axis=0)
cov22 = np.delete(np.delete(self.covMats[channel],
inPatchIdx,
axis=0),
inPatchIdx,
axis=1)
cond_cov = cov11 - np.dot(np.dot(cov12, scipy.linalg.inv(cov22)),
cov21)
np.save(path_condCov, cond_cov)
else:
cond_cov = np.load(path_condCov + '.npy')
return cond_mean, cond_cov
def extract_svd(input_stack, L):
C = numpy.copy(input_stack) # temporary array
print('size of input_stack', numpy.shape(input_stack))
C = C / numpy.max(numpy.abs(C))
reps_acs = 16 #16
mysize = 4 #16
K = 3 # rank of 10 prevent singular? artifacts(certain disruption)
half_mysize = mysize / 2
dimension = numpy.ndim(C) - 1 # collapse coil dimension
if dimension == 1:
tmp_stack = numpy.empty((mysize, ), dtype=dtype)
svd_size = mysize
C_size = numpy.shape(C)[0]
data = numpy.empty((svd_size, L * reps_acs), dtype=dtype)
# for jj in xrange(0,L):
# C[:,jj]=tailor_fftn(C[:,jj])
# for kk in xrange(0,reps_acs):
# tmp_stack = numpy.reshape(tmp_stack,(svd_size,),order = 'F')
# data[:,jj] = numpy.reshape(tmp_stack,(svd_size,),order = 'F')
elif dimension == 2:
tmp_stack = numpy.empty((
mysize,
mysize,
), dtype=dtype)
svd_size = mysize**2
data = numpy.empty((svd_size, L * reps_acs), dtype=dtype)
C_size = numpy.shape(C)[0:2]
for jj in xrange(0, L):
# matplotlib.pyplot.imshow(C[...,jj].real)
# matplotlib.pyplot.show()
# tmp_pt=(C_size[0]-reps_acs)/2
C[:, :, jj] = tailor_fftn(C[:, :, jj])
for kk in xrange(0, reps_acs):
a = numpy.mod(kk, reps_acs**0.5)
b = kk / (reps_acs**0.5)
tmp_stack = C[C_size[0] / 2 - half_mysize -
(reps_acs**0.5) / 2 + a:C_size[0] / 2 +
half_mysize - (reps_acs**0.5) / 2 + a,
C_size[1] / 2 - half_mysize -
(reps_acs**0.5) / 2 + b:C_size[1] / 2 +
half_mysize - (reps_acs**0.5) / 2 + b, jj]
data[:, jj * reps_acs + kk] = numpy.reshape(tmp_stack,
(svd_size, ),
order='F')
elif dimension == 3:
tmp_stack = numpy.empty((mysize, mysize, mysize), dtype=dtype)
svd_size = mysize**3
data = numpy.empty((svd_size, L), dtype=dtype)
C_size = numpy.shape(C)[0:3]
for jj in xrange(0, L):
C[:, :, :, jj] = tailor_fftn(C[:, :, :, jj])
tmp_stack = C[C_size[0] / 2 - half_mysize:C_size[0] / 2 +
half_mysize, C_size[1] / 2 -
half_mysize:C_size[1] / 2 + half_mysize,
C_size[2] / 2 - half_mysize:C_size[2] / 2 +
half_mysize, jj]
data[:, jj] = numpy.reshape(tmp_stack, (svd_size, ), order='F')
# OK, data is the matrix of size (mysize*n, L) for SVD
# import scipy.linalg
# import scipy.sparse.linalg
(s_blah, vh_blah) = scipy.linalg.svd(data)[1:3]
for jj in xrange(0, numpy.size(s_blah)): #
if s_blah[jj] > 0.1 * s_blah[
0]: # 10% of maximum singular value to decide the rank
K = jj + 1
# pass
else:
break
v_blah = vh_blah.conj().T
C = C * 0.0 # now C will be used as the output stack
V_para = v_blah[:, 0:K]
print('shape of V_para', numpy.shape(V_para))
V_para = numpy.reshape(V_para, (reps_acs**0.5, reps_acs**0.5, L, K),
order='F')
C2 = numpy.zeros((C.shape[0], C.shape[1], L, K), dtype=dtype)
for jj in xrange(0, L): # coils
for kk in xrange(0, K): # rank
C2[C.shape[0] / 2 - reps_acs**0.5 / 2:C.shape[0] / 2 +
reps_acs**0.5 / 2, C.shape[1] / 2 -
reps_acs**0.5 / 2:C.shape[1] / 2 + reps_acs**0.5 / 2, jj,
kk] = V_para[:, :, jj, kk]
C2[:, :, jj, kk] = tailor_fftn(C2[:, :, jj, kk])
# C_value = numpy.empty_like(C)
for mm in xrange(0, C.shape[0]): # dim 0
for nn in xrange(0, C.shape[1]): # dim 1
tmp_g = C2[mm, nn, :, :]
# G = C2[mm,nn,:,:].T # Transpose (non-conjugated) of G
# # Gh = G.conj().T # hermitian
# Gh=C2[mm,nn,:,:].conj()
# G=
g = numpy.dot(tmp_g.conj(),
tmp_g.T) #construct g matrix for eigen-decomposition
# w,v = scipy.linalg.eig(g.astype(dtype), overwrite_a=True,
# check_finite=False) # eigen value:w, eigen vector: v
# print('L=',L,numpy.shape(g))
# w,v = scipy.sparse.linalg.eigs(g , 3)
w, v = myeig(g.astype(dtype))
ind = numpy.argmax(numpy.abs(w)) # find the maximum
# print('ind=',ind)
# the_eig = numpy.abs(w[ind]) # find the abs of maximal eigen value
tmp_v = v[:, ind] #*the_eig
# ref_angle=(numpy.sum(v[:,ind])/(numpy.abs(numpy.sum(v[:,ind]))))
# v[:,ind] = v[:,ind]/ref_angle # correct phase by summed value
ref_angle = numpy.sum(tmp_v)
ref_angle = ref_angle / numpy.abs(ref_angle)
C[mm, nn, :] = tmp_v / ref_angle # correct phase by summed value
C = C / numpy.max(numpy.abs(C))
# matplotlib.pyplot.figure(1)
# for jj in xrange(0,L):
# matplotlib.pyplot.subplot(2,4,jj+1)
# matplotlib.pyplot.imshow(abs(input_stack[...,jj]),
# norm=matplotlib.colors.Normalize(vmin=0.0, vmax=0.2),
# cmap=matplotlib.cm.gray)
# matplotlib.pyplot.subplot(2,4,jj+1+4)
# matplotlib.pyplot.imshow(abs(C[...,jj]),
# norm=matplotlib.colors.Normalize(vmin=0.0, vmax=1.0),
# cmap=matplotlib.cm.gray)
#
# # matplotlib.pyplot.subplot(2,8,jj+1+8)
# # matplotlib.pyplot.imshow(numpy.log(C[...,jj]).imag, cmap=matplotlib.cm.gray)
#
# matplotlib.pyplot.show()
# for jj in xrange(0,L):
# matplotlib.pyplot.subplot(2,2,jj+1)
# matplotlib.pyplot.imshow((input_stack[...,jj].real))
# matplotlib.pyplot.show()
return C # normalize the coil sensitivities
def float2frmt(self, y):
"""
Called a.o. by `itemDelegate.displayText()` for on-the-fly number
conversion. Returns fixpoint representation for `y` (scalar or array-like)
with numeric format `self.frmt` and `self.W` bits. The result has the
same shape as `y`.
The float is multiplied by `self.scale` and quantized / saturated
using fixp() for all formats before it is converted to different number
formats.
Parameters
----------
y: scalar or array-like
y has to be an integer or float decimal number either numeric or in
string format.
Returns
-------
A string, a float or an ndarray of float or string is returned in the
numeric format set in `self.frmt`. It has the same shape as `y`. For all
formats except `float` a fixpoint representation with `self.W` binary
digits is returned.
"""
"""
Define vectorized functions using numpys automatic type casting:
Vectorized functions for inserting binary point in string `bin_str`
after position `pos`.
Usage: insert_binary_point(bin_str, pos)
Parameters: bin_str : string
pos : integer
"""
insert_binary_point = np.vectorize(lambda bin_str, pos:(
bin_str[:pos+1] + "." + bin_str[pos+1:]))
binary_repr_vec = np.frompyfunc(np.binary_repr, 2, 1)
#======================================================================
if self.frmt == 'float': # return float input value unchanged (no string)
return y
elif self.frmt == 'float32':
return np.float32(y)
elif self.frmt == 'float16':
return np.float16(y)
elif self.frmt in {'hex', 'bin', 'dec', 'csd'}:
# return a quantized & saturated / wrapped fixpoint (type float) for y
y_fix = self.fixp(y, scaling='mult')
if self.frmt == 'dec':
if self.WF == 0:
y_str = np.int64(y_fix) # get rid of trailing zero
# y_str = np.char.mod('%d', y_fix)
# elementwise conversion from integer (%d) to string
# see https://docs.scipy.org/doc/numpy/reference/routines.char.html
else:
# y_str = np.char.mod('%f',y_fix)
y_str = y_fix
elif self.frmt == 'csd':
y_str = dec2csd_vec(y_fix, self.WF) # convert with WF fractional bits
else: # bin or hex
# represent fixpoint number as integer in the range -2**(W-1) ... 2**(W-1)
y_fix_int = np.int64(np.round(y_fix / self.LSB))
# convert to (array of) string with 2's complement binary
y_bin_str = binary_repr_vec(y_fix_int, self.W)
if self.frmt == 'hex':
y_str = bin2hex_vec(y_bin_str, self.WI)
else: # self.frmt == 'bin':
# insert radix point if required
if self.WF > 0:
y_str = insert_binary_point(y_bin_str, self.WI)
else:
y_str = y_bin_str
if isinstance(y_str, np.ndarray) and np.ndim(y_str) < 1:
y_str = y_str.item() # convert singleton array to scalar
return y_str
else:
raise Exception('Unknown output format "%s"!'%(self.frmt))
return None
def smooth_volume(data_img,
fwhm,
mask_img=None,
noise_img=None,
inplace=False):
"""Filter volume data with an isotropic gaussian kernel.
Smoothing can be constrained to occur within the voxels defined within
``mask_img`` and optionally can ignore/interpolate out the voxels
identified within ``noise_img``.
Parameters
----------
data_img : nibabel image
3D or 4D image data.
fwhm : positive float
Size of isotropic smoothing kernel in mm.
mask_img : nibabel image
3D binary image defining smoothing range.
noise_img : nibabel image
3D binary image defining voxels to be interpolated out.
inplace : bool
If True, overwrite data in data_img. Otherwise perform a copy.
Returns
-------
smooth_data : nibabel image
Image like ``data_img`` but after smoothing.
"""
data = data_img.get_data().astype(np.float, copy=not inplace)
if np.ndim(data) == 3:
need_squeeze = True
data = np.expand_dims(data, -1)
else:
need_squeeze = False
if mask_img is None:
mask = np.ones(data.shape[:3], np.bool)
else:
mask = mask_img.get_data().astype(np.bool)
smooth_from = mask.copy()
if noise_img is not None:
smooth_from &= ~noise_img.get_data().astype(np.bool)
sigma = voxel_sigmas(fwhm, data_img)
norm = gaussian_filter(smooth_from.astype(np.float), sigma)
valid_norm = norm > 0
for f in range(data.shape[-1]):
with np.errstate(all="ignore"):
data_f = gaussian_filter(data[..., f] * smooth_from, sigma) / norm
data_f[~valid_norm] = 0
data[..., f] = data_f
data[~mask] = 0
if need_squeeze:
data = data.squeeze()
return nib.Nifti1Image(data, data_img.affine, data_img.header)
def btens_to_params(btens, ztol=1e-10):
r"""Compute trace, anisotropy and assymetry parameters from b-tensors
Parameters
----------
btens : (3, 3) OR (N, 3, 3) numpy.ndarray
input b-tensor, or b-tensors, where N = number of b-tensors
ztol : float
Any parameters smaller than this value are considered to be 0
Returns
-------
bval: numpy.ndarray
b-value(s) (trace(s))
bdelta: numpy.ndarray
normalized tensor anisotropy(s)
b_eta: numpy.ndarray
tensor assymetry(s)
Notes
-----
This function can be used to get b-tensor parameters directly from the
GradientTable `btens` attribute.
Examples
--------
>>> lte = np.array([[1, 0, 0], [0, 0, 0], [0, 0, 0]])
>>> bval, bdelta, b_eta = btens_to_params(lte)
>>> print("bval={}; bdelta={}; b_eta={}".format(bdelta, bval, b_eta))
bval=[ 1.]; bdelta=[ 1.]; b_eta=[ 0.]
"""
# Bad input checks
value_error_msg = "`btens` must be a 2D or 3D numpy array, respectively" \
" with (3, 3) or (N, 3, 3) shape, where N corresponds" \
" to the number of b-tensors"
if not isinstance(btens, np.ndarray):
raise ValueError(value_error_msg)
nd = np.ndim(btens)
if nd == 2:
btens_shape = btens.shape
elif nd == 3:
btens_shape = btens.shape[1:]
else:
raise ValueError(value_error_msg)
if not btens_shape == (3, 3):
raise ValueError(value_error_msg)
# Reshape so that loop below works when only one input b-tensor is provided
if nd == 2:
btens = btens.reshape((1, 3, 3))
# Pre-allocate
n_btens = btens.shape[0]
bval = np.empty(n_btens)
bdelta = np.empty(n_btens)
b_eta = np.empty(n_btens)
# Loop over b-tensor(s)
for i in range(btens.shape[0]):
i_btens = btens[i, :, :]
i_bval, i_bdelta, i_b_eta = _btens_to_params_2d(i_btens, ztol)
bval[i] = i_bval
bdelta[i] = i_bdelta
b_eta[i] = i_b_eta
return bval, bdelta, b_eta
