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-rw-r--r--numpy/polynomial/hermite.py213
1 files changed, 141 insertions, 72 deletions
diff --git a/numpy/polynomial/hermite.py b/numpy/polynomial/hermite.py
index ace91d2e2..8781ff1e2 100644
--- a/numpy/polynomial/hermite.py
+++ b/numpy/polynomial/hermite.py
@@ -654,6 +654,8 @@ def hermder(c, m=1, scl=1, axis=0) :
axis : int, optional
Axis over which the derivative is taken. (Default: 0).
+ .. versionadded:: 1.7.0
+
Returns
-------
der : ndarray
@@ -752,6 +754,8 @@ def hermint(c, m=1, k=[], lbnd=0, scl=1, axis=0):
axis : int, optional
Axis over which the derivative is taken. (Default: 0).
+ .. versionadded:: 1.7.0
+
Returns
-------
S : ndarray
@@ -950,8 +954,6 @@ def hermval2d(x, y, c):
If `c` is a 1-D array a one is implicitly appended to its shape to make
it 2-D. The shape of the result will be c.shape[2:] + x.shape.
- .. versionadded::1.7.0
-
Parameters
----------
x, y : array_like, compatible objects
@@ -975,6 +977,11 @@ def hermval2d(x, y, c):
--------
hermval, hermgrid2d, hermval3d, hermgrid3d
+ Notes
+ -----
+
+ .. versionadded::1.7.0
+
"""
try:
x, y = np.array((x, y), copy=0)
@@ -1007,8 +1014,6 @@ def hermgrid2d(x, y, c):
its shape to make it 2-D. The shape of the result will be c.shape[2:] +
x.shape.
- .. versionadded:: 1.7.0
-
Parameters
----------
x, y : array_like, compatible objects
@@ -1032,6 +1037,11 @@ def hermgrid2d(x, y, c):
--------
hermval, hermval2d, hermval3d, hermgrid3d
+ Notes
+ -----
+
+ .. versionadded::1.7.0
+
"""
c = hermval(x, c)
c = hermval(y, c)
@@ -1056,8 +1066,6 @@ def hermval3d(x, y, z, c):
shape to make it 3-D. The shape of the result will be c.shape[3:] +
x.shape.
- .. versionadded::1.7.0
-
Parameters
----------
x, y, z : array_like, compatible object
@@ -1082,6 +1090,11 @@ def hermval3d(x, y, z, c):
--------
hermval, hermval2d, hermgrid2d, hermgrid3d
+ Notes
+ -----
+
+ .. versionadded::1.7.0
+
"""
try:
x, y, z = np.array((x, y, z), copy=0)
@@ -1117,8 +1130,6 @@ def hermgrid3d(x, y, z, c):
its shape to make it 3-D. The shape of the result will be c.shape[3:] +
x.shape + yshape + z.shape.
- .. versionadded:: 1.7.0
-
Parameters
----------
x, y, z : array_like, compatible objects
@@ -1143,6 +1154,11 @@ def hermgrid3d(x, y, z, c):
--------
hermval, hermval2d, hermgrid2d, hermval3d
+ Notes
+ -----
+
+ .. versionadded::1.7.0
+
"""
c = hermval(x, c)
c = hermval(y, c)
@@ -1151,28 +1167,38 @@ def hermgrid3d(x, y, z, c):
def hermvander(x, deg) :
- """Vandermonde matrix of given degree.
+ """Pseudo-Vandermonde matrix of given degree.
- Returns the Vandermonde matrix of degree `deg` and sample points `x`.
- This isn't a true Vandermonde matrix because `x` can be an arbitrary
- ndarray and the Hermite polynomials aren't powers. If ``V`` is the
- returned matrix and `x` is a 2d array, then the elements of ``V`` are
- ``V[i,j,k] = P_k(x[i,j])``, where ``P_k`` is the Hermite polynomial
- of degree ``k``.
+ Returns the pseudo-Vandermonde matrix of degree `deg` and sample points
+ `x`. The pseudo-Vandermonde matrix is defined by
+
+ .. math:: V[..., i] = H_i(x),
+
+ where `0 <= i <= deg`. The leading indices of `V` index the elements of
+ `x` and the last index is the degree of the Hermite polynomial.
+
+ If `c` is a 1-D array of coefficients of length `n + 1` and `V` is the
+ array ``V = hermvander(x, n)``, then ``np.dot(V, c)`` and
+ ``hermval(x, c)`` are the same up to roundoff. This equivalence is
+ useful both for least squares fitting and for the evaluation of a large
+ number of Hermite series of the same degree and sample points.
Parameters
----------
x : array_like
- Array of points. The values are converted to double or complex
- doubles. If x is scalar it is converted to a 1D array.
- deg : integer
+ Array of points. The dtype is converted to float64 or complex128
+ depending on whether any of the elements are complex. If `x` is
+ scalar it is converted to a 1-D array.
+ deg : int
Degree of the resulting matrix.
Returns
-------
- vander : Vandermonde matrix.
- The shape of the returned matrix is ``x.shape + (deg+1,)``. The last
- index is the degree.
+ vander: ndarray
+ The pseudo-Vandermonde matrix. The shape of the returned matrix is
+ ``x.shape + (deg + 1,)``, where The last index is the degree of the
+ corresponding Hermite polynomial. The dtype will be the same as
+ the converted `x`.
Examples
--------
@@ -1202,36 +1228,50 @@ def hermvander(x, deg) :
def hermvander2d(x, y, deg) :
- """Pseudo Vandermonde matrix of given degree.
-
- Returns the pseudo Vandermonde matrix for 2D Hermite series in `x` and
- `y`. The sample point coordinates must all have the same shape after
- conversion to arrays and the dtype will be converted to either float64
- or complex128 depending on whether any of `x` or 'y' are complex. The
- maximum degrees of the 2D Hermite series in each variable are specified
- in the list `deg` in the form ``[xdeg, ydeg]``. The return array has
- the shape ``x.shape + (order,)`` if `x`, and `y` are arrays or
- ``(1, order) if they are scalars. Here order is the number of elements
- in a flattened coefficient array of original shape ``(xdeg + 1, ydeg +
- 1)``. The flattening is done so that the resulting pseudo Vandermonde
- array can be easily used in least squares fits.
+ """Pseudo-Vandermonde matrix of given degrees.
+
+ Returns the pseudo-Vandermonde matrix of degrees `deg` and sample
+ points `(x, y)`. The pseudo-Vandermonde matrix is defined by
+
+ .. math:: V[..., deg[1]*i + j] = H_i(x) * H_j(y),
+
+ where `0 <= i <= deg[0]` and `0 <= j <= deg[1]`. The leading indices of
+ `V` index the points `(x, y)` and the last index encodes the degrees of
+ the Hermite polynomials.
+
+ If `c` is a 2-D array of coefficients of shape `(m + 1, n + 1)` and `V`
+ is the matrix ``V = hermvander2d(x, y, [m, n])``, then
+ ``np.dot(V, c.flat)`` and ``hermval2d(x, y, c)`` are the same up to
+ roundoff. This equivalence is useful both for least squares fitting and
+ for the evaluation of a large number of 2-D Hermite series of the same
+ degrees and sample points.
Parameters
----------
- x,y : array_like
- Arrays of point coordinates, each of the same shape.
- deg : list
+ x, y : array_like
+ Arrays of point coordinates, all of the same shape. The dtypes
+ will be converted to either float64 or complex128 depending on
+ whether any of the elements are complex. Scalars are converted to 1-D
+ arrays.
+ deg : list of ints
List of maximum degrees of the form [x_deg, y_deg].
Returns
-------
vander2d : ndarray
- The shape of the returned matrix is described above.
+ The shape of the returned matrix is ``x.shape + (order,)``, where
+ :math:`order = (deg[0]+1)*(deg([1]+1)`. The dtype will be the same
+ as the converted `x` and `y`.
See Also
--------
hermvander, hermvander3d. hermval2d, hermval3d
+ Notes
+ -----
+
+ .. versionadded::1.7.0
+
"""
ideg = [int(d) for d in deg]
is_valid = [id == d and id >= 0 for id, d in zip(ideg, deg)]
@@ -1247,37 +1287,51 @@ def hermvander2d(x, y, deg) :
def hermvander3d(x, y, z, deg) :
- """Pseudo Vandermonde matrix of given degree.
-
- Returns the pseudo Vandermonde matrix for 3D Hermite series in `x`,
- `y`, or `z`. The sample point coordinates must all have the same shape
- after conversion to arrays and the dtype will be converted to either
- float64 or complex128 depending on whether any of `x`, `y`, or 'z' are
- complex. The maximum degrees of the 3D Hermite series in each variable
- are specified in the list `deg` in the form ``[xdeg, ydeg, zdeg]``. The
- return array has the shape ``x.shape + (order,)`` if `x`, `y`, and `z`
- are arrays or ``(1, order) if they are scalars. Here order is the
- number of elements in a flattened coefficient array of original shape
- ``(xdeg + 1, ydeg + 1, zdeg + 1)``. The flattening is done so that the
- resulting pseudo Vandermonde array can be easily used in least squares
- fits.
+ """Pseudo-Vandermonde matrix of given degrees.
+
+ Returns the pseudo-Vandermonde matrix of degrees `deg` and sample
+ points `(x, y, z)`. If `l, m, n` are the given degrees in `x, y, z`,
+ then The pseudo-Vandermonde matrix is defined by
+
+ .. math:: V[..., (m+1)(n+1)i + (n+1)j + k] = H_i(x)*H_j(y)*H_k(z),
+
+ where `0 <= i <= l`, `0 <= j <= m`, and `0 <= j <= n`. The leading
+ indices of `V` index the points `(x, y, z)` and the last index encodes
+ the degrees of the Hermite polynomials.
+
+ If `c` is a 3-D array of coefficients of shape `(l + 1, m + 1, n + 1)`
+ and `V` is the matrix ``V = hermvander3d(x, y, z, [l, m, n])``, then
+ ``np.dot(V, c.flat)`` and ``hermval3d(x, y, z, c)`` are the same up to
+ roundoff. This equivalence is useful both for least squares fitting and
+ for the evaluation of a large number of 3-D Hermite series of the
+ same degrees and sample points.
Parameters
----------
- x,y,z : array_like
- Arrays of point coordinates, each of the same shape.
- deg : list
+ x, y, z : array_like
+ Arrays of point coordinates, all of the same shape. The dtypes will
+ be converted to either float64 or complex128 depending on whether
+ any of the elements are complex. Scalars are converted to 1-D
+ arrays.
+ deg : list of ints
List of maximum degrees of the form [x_deg, y_deg, z_deg].
Returns
-------
vander3d : ndarray
- The shape of the returned matrix is described above.
+ The shape of the returned matrix is ``x.shape + (order,)``, where
+ :math:`order = (deg[0]+1)*(deg([1]+1)*(deg[2]+1)`. The dtype will
+ be the same as the converted `x`, `y`, and `z`.
See Also
--------
hermvander, hermvander3d. hermval2d, hermval3d
+ Notes
+ -----
+
+ .. versionadded::1.7.0
+
"""
ideg = [int(d) for d in deg]
is_valid = [id == d and id >= 0 for id, d in zip(ideg, deg)]
@@ -1466,15 +1520,15 @@ def hermcompanion(c):
"""Return the scaled companion matrix of c.
The basis polynomials are scaled so that the companion matrix is
- symmetric when `c` represents a single Hermite polynomial. This
- provides better eigenvalue estimates than the unscaled case and in the
- single polynomial case the eigenvalues are guaranteed to be real if
+ symmetric when `c` is an Hermite basis polynomial. This provides
+ better eigenvalue estimates than the unscaled case and for basis
+ polynomials the eigenvalues are guaranteed to be real if
`numpy.linalg.eigvalsh` is used to obtain them.
Parameters
----------
c : array_like
- 1-d array of Legendre series coefficients ordered from low to high
+ 1-d array of Hermite series coefficients ordered from low to high
degree.
Returns
@@ -1482,6 +1536,11 @@ def hermcompanion(c):
mat : ndarray
Scaled companion matrix of dimensions (deg, deg).
+ Notes
+ -----
+
+ .. versionadded::1.7.0
+
"""
accprod = np.multiply.accumulate
# c is a trimmed copy
@@ -1563,12 +1622,13 @@ def hermroots(c):
def hermgauss(deg):
- """Gauss Hermite quadrature.
+ """
+ Gauss-Hermite quadrature.
Computes the sample points and weights for Gauss-Hermite quadrature.
These sample points and weights will correctly integrate polynomials of
- degree ``2*deg - 1`` or less over the interval ``[-inf, inf]`` with the
- weight function ``f(x) = exp(-x**2)``.
+ degree :math:`2*deg - 1` or less over the interval :math:`[-\inf, \inf]`
+ with the weight function :math:`f(x) = \exp(-x^2)`.
Parameters
----------
@@ -1584,14 +1644,17 @@ def hermgauss(deg):
Notes
-----
- The results have only been tested up to degree 100. Higher degrees may
+
+ .. versionadded::1.7.0
+
+ The results have only been tested up to degree 100, higher degrees may
be problematic. The weights are determined by using the fact that
- w = c / (H'_n(x_k) * H_{n-1}(x_k))
+ .. math:: w_k = c / (H'_n(x_k) * H_{n-1}(x_k))
- where ``c`` is a constant independent of ``k`` and ``x_k`` is the k'th
- root of ``H_n``, and then scaling the results to get the right value
- when integrating 1.
+ where :math:`c` is a constant independent of :math:`k` and :math:`x_k`
+ is the k'th root of :math:`H_n`, and then scaling the results to get
+ the right value when integrating 1.
"""
ideg = int(deg)
@@ -1628,11 +1691,12 @@ def hermgauss(deg):
def hermweight(x):
- """Weight function of the Hermite polynomials.
+ """
+ Weight function of the Hermite polynomials.
- The weight function for which the Hermite polynomials are orthogonal.
- In this case the weight function is ``exp(-x**2)``. Note that the
- Hermite polynomials are not normalized.
+ The weight function is :math:`\exp(-x^2)` and the interval of
+ integration is :math:`[-\inf, \inf]`. the Hermite polynomials are
+ orthogonal, but not normalized, with respect to this weight function.
Parameters
----------
@@ -1644,6 +1708,11 @@ def hermweight(x):
w : ndarray
The weight function at `x`.
+ Notes
+ -----
+
+ .. versionadded::1.7.0
+
"""
w = np.exp(-x**2)
return w