Source code for clifford.tools

"""
.. currentmodule:: clifford.tools

========================================
tools (:mod:`clifford.tools`)
========================================

Algorithms and tools of various kinds.


Tools for specific ga's
-----------------------

.. autosummary::
    :toctree: generated/

    g3
    g3c


Classifying conformal GAs
-------------------------

.. autosummary::
    :toctree: generated/

    classify


Determining Rotors From Frame Pairs or Orthogonal Matrices
-----------------------------------------------------------

Given two frames that are related by a orthogonal transform, we seek a rotor
which enacts the transform. Details of the mathematics and pseudo-code used to
create the algorithms below can be found at Allan Cortzen's website,
:cite:`ctz-frames`.

There are also some helper functions which can be used to translate matrices
into GA frames, so an orthogonal (or complex unitary) matrix can be directly
translated into a Versor.

.. autosummary::
    :toctree: generated/

    orthoFrames2Versor
    orthoMat2Versor
    mat2Frame
    frame2Mat
    func2Mat
    omoh
    rotor_decomp

"""

from functools import reduce

from typing import Union, Optional, List, Tuple
from math import sqrt
from numpy import eye, array, sign, zeros, sin, arccos,log
import numpy as np
from .. import Cl, gp, Frame, MultiVector
from .. import eps as global_eps

from warnings import warn


[docs]def omoh(A: Union[Frame, List[MultiVector]], B: Union[Frame, List[MultiVector]]) -> np.ndarray: r''' Determines homogenization scaling for two :class:`~clifford.Frame`\ s related by a Rotor This is used as part of the :func:`~clifford.tools.orthoFrames2Versor` algorithm, when the frames are given in CGA. It is required because the model assumes, ``B = R*A*~R``, but if data is given in the original space, only ``lambda*B' == homo(B)`` is observable. We need to determine lambda before the Cartan-based algorithm can be used. The name of this function is the reverse of :meth:`~clifford.ConformalLayout.homo`, which is the method used to homogenize. Parameters -------------- A : list of vectors, or clifford.Frame the set of vectors before the transform B : list of vectors, or clifford.Frame the set of vectors after the transform, and homogenzation. ie ``B=B/(B|einf)`` Returns --------- out : array of floats weights on `B`, which produce inhomogenous versions of `B`. If you multiply the input `B` by `lam`, it will fulfill `B = R*A*~R` Examples ---------- >>> lam = ohom(A, B) >>> B_ohom = Frame([B[k]*lam[k] for k in range(len(B)]) ''' if len(A) != len(B) or len(A) < 3: raise ValueError('input must be >=3 long and len(a)==len(b)') idx = range(len(A)) lam = zeros(len(A)) for i in idx: j, k = [p for p in idx if p != i][:2] lam[i] = \ float((A[i] * A[j])(0) * (A[i] * A[k])(0) * (B[j] * B[k])(0)) / \ float((B[i] * B[j])(0) * (B[i] * B[k])(0) * (A[j] * A[k])(0)) lam[i] = sqrt(float(lam[i])) return lam
[docs]def mat2Frame(A: np.ndarray, I: Optional[MultiVector] = None, is_complex: bool = None) -> Tuple[List[MultiVector], MultiVector]: ''' Translates a (possibly complex) matrix into a real vector frame The rows and columns of `A` are interpreted as follows * ``M, N = A.shape`` * ``M``: dimension of space * ``N``: number of vectors If A is complex M and N are doubled. Parameters ------------ A : ndarray MxN matrix representing vectors I : MultiVector if none we generate an algebra of Gn, if layout we take the vector basis from that, and if its a list we will assume its a vector basis. Returns ------- a : list of clifford.MultiVector The resulting vectors I : clifford.MultiVector The blade holding the vectors in ``a``. ''' # TODO: could simplify this by just implementing the real case and then # recursively calling this for A.real, and A.imag, then combine results # M = dimension of space # N = number of vectors M, N = A.shape if is_complex is None: if A.dtype == 'complex': is_complex = True else: is_complex = False if is_complex: N = N * 2 M = M * 2 if I is None: layout, blades = Cl(M) I = layout.pseudoScalar e_ = I.basis() a = [0 ^ e_[0]] * N if not is_complex: for n in range(N): for m in range(M): a[n] = (a[n]) + ((A[m, n]) ^ e_[m]) else: for n in range(N // 2): n_ = 2 * n for m in range(M // 2): m_ = 2 * m a[n_] = (a[n_]) \ + ((A[m, n].real) ^ e_[m_]) \ + ((A[m, n].imag) ^ e_[m_ + 1]) a[n_ + 1] = (a[n_ + 1]) \ + ((-A[m, n].imag) ^ e_[m_]) \ + ((A[m, n].real) ^ e_[m_ + 1]) return a, I
[docs]def frame2Mat(B, A=None, I=None, is_complex=None): ''' convert a list of vectors to a matrix Parameters ------------ B : list a list of vectors that have been transformed A : None, list of vectors a list of vectors in their initial state. if none we assume orthonormal basis given by B.pseudoScalar, or I I : MultiVector, None pseudoscalar of the space. if None, we use B.pseudoScalar is_complex: Bool do you want a complex matrix? ''' if is_complex is not None: raise NotImplementedError() if I is None: I = B[0].pseudoScalar if A is None: # assume we have orthonormal initial frame A = I.basis() # you need float() due to bug in clifford M = [float(b | a) for a in A for b in B] M = array(M).reshape(len(B), len(B)) return M, I
[docs]def func2Mat(f,I): ''' Convert a function to a matrix by acting on standard basis Parameters --------------- f : function function that maps vectors to vectors I : MultiVector psuedoscalar of basis See Also --------- frame2Mat ''' A = I.basis() B = [f(a) for a in A] return frame2Mat(B=B, A=A,I=I)
def orthoFrames2Versor_dist(A, B, eps=None): ''' Determines versor for two frames related by an orthogonal transform The frames themselves do not have to be orthogonal. Based on :cite:`ctz-frames,fontijne-reconstructing`. This works in Euclidean spaces and, under special circumstances in other signatures. See :cite:`ctz-frames` for limitations/details. ''' # TODO: should we test to see if A and B are related by rotation? # TODO: implement reflect/rotate based on distance (as in:cite:`ctz-frames`) # keep copy of original frames A = A[:] B = B[:] if len(A) != len(B): raise ValueError('len(A)!=len(B)') if eps is None: eps = global_eps() # store each reflector in a list r_list = [] # find the vector pair with the largest distance dist = [abs((a - b) ** 2) for a, b in zip(A, B)] k = dist.index(max(dist)) while dist[k] >= eps: r = (A[k] - B[k]) / abs(A[k] - B[k]) # determine reflector r_list.append(r) # append to our list A = A[1:] # remove current vector pair B = B[1:] if len(A) == 0: break # reflect remaining vectors for j in range(len(A)): A[j] = -r * A[j] * r # find the next pair based on current distance dist = [abs((a - b) ** 2) for a, b in zip(A, B)] k = dist.index(max(dist)) # print(str(len(r_list)) + ' reflections found') R = reduce(gp, r_list[::-1]) return R, r_list
[docs]def orthoFrames2Versor(B, A=None, delta: float = 1e-3, eps: Optional[float] = None, det=None, remove_scaling: bool = False): ''' Determines versor for two frames related by an orthogonal transform Based on :cite:`ctz-frames,fontijne-reconstructing`. This works in Euclidean spaces and, under special circumstances in other signatures. See :cite:`ctz-frames` for limitations/details. Parameters ----------- B : list of vectors, or clifford.Frame the set of vectors after the transform, and homogenzation. ie ``B = (B/B|einf)`` A : list of vectors, or clifford.Frame the set of vectors before the transform. If `None` we assume A is the basis given by ``B.layout.basis_vectors_lst``. delta : float Tolerance for reflection/rotation determination. If the normalized distance between A[i] and B[i] is larger than delta, we use reflection, otherwise use rotation. eps: float Tolerance on spinor determination. if pseudoscalar of A differs in magnitude from pseudoscalar of B by eps, then we have spinor. If `None`, use the `clifford.eps()` global eps. det : [+1,-1,None] The sign of the determinant of the versor, if known. If it is known a-priori that the versor is a rotation vs a reflection, this fact might be needed to correctly append an additional reflection which leaves transformed points invariant. See 4.6.3 of :cite:`fontijne-reconstructing`. remove_scaling : bool Remove the effects of homogenzation from frame B. This is needed if you are working in CGA, but the input data is given in the original space. See :func:`~clifford.tools.omoh` for more. See 4.6.2 of :cite:`fontijne-reconstructing`. Returns --------- R : clifford.MultiVector the Versor. rs : list of clifford.MultiVector ordered list of found reflectors/rotors. ''' # Checking and Setup if A is None: # assume we have orthonormal initial frame A = B[0].layout.basis_vectors_lst # make copy of original frames, so we can rotate A A = A[:] B = B[:] if len(A) != len(B): raise ValueError('len(A)!=len(B)') if eps is None: eps = global_eps() # Determine if we have a spinor spinor = False # store pseudoscalar of frame B, in case known det (see end) try: B = Frame(B) B_En = B.En except Exception: pass N = len(A) # Determine and remove scaling factors caused by homogenization if remove_scaling: lam = omoh(A, B) B = Frame([B[k] * lam[k] for k in range(N)]) try: # compute ratio of volumes for each frame. take Nth root A = Frame(A[:]) B = Frame(B[:]) alpha = abs(B.En / A.En) ** (1. / N) if abs(alpha - 1) > eps: spinor = True # we have a spinor, remove the scaling (add it back in at the end) B = [b / alpha for b in B] except Exception: # probably A and B are not pure vector correspondence # whatever, it might still work pass # Find the Versor # store each reflector/rotor in a list, make full versor at the # end of the loop r_list = [] for k in range(N): a, b = A[0], B[0] r = a - b # determine reflector if abs(b ** 2) > eps: d = abs(r ** 2) / abs(b ** 2) # conditional rotation tolerance else: # probably b is a null vector, make our best guess for tol! d = abs(r ** 2) if d >= delta: # reflection part r_list.append(r) A = A[1:] # remove current vector pair B = B[1:] for j in range(len(A)): A[j] = -r * A[j] * r.inv() else: # rotation part # if k==N: # see paper for explanation # break R = b * (a + b) if abs(R) > eps: # abs(R) can be <eps in null space r_list.append(R) # append to our list A = A[1:] # remove current vector pair B = B[1:] for j in range(len(A)): A[j] = R * A[j] * R.inv() R = reduce(gp, r_list[::-1]) # if det is known a priori check to see if it's correct, if not add # an extra reflection which leaves all points in B invariant if det is not None: I = R.pseudoScalar our_det = (R * I * ~R * I.inv())(0) if sign(float(our_det)) != det: R = B_En.dual() * R if abs(R) < eps: warn('abs(R)<eps. likely to be inaccurate') R = R / abs(R) if spinor: R = R * sqrt(alpha) return R, r_list
[docs]def orthoMat2Versor(A, eps=None, I=None, is_complex=None): ''' Translates an orthogonal (or unitary) matrix to a Versor `A` is interpreted as the frame produced by transforming a orthonormal frame by an orthogonal transform. Given this relation, this function will find the versor which enacts this transform. Parameters ------------ A : matrix matrix to be transformed eps : number tolerance I : MultiVector GA of A is_complex : boolean is A complex? ''' B, layout = mat2Frame(A, I=I, is_complex=is_complex) N = len(B) # if (A.dot(A.conj().T) -eye(N/2)).max()>eps: # warn('A doesnt appear to be a rotation. ') A, dum = mat2Frame(eye(N), I=I, is_complex=False) return orthoFrames2Versor(A=A, B=B, eps=eps)
[docs]def rotor_decomp(V: MultiVector, x: MultiVector) -> Tuple[MultiVector, MultiVector]: ''' Rotor decomposition of rotor V Given a rotor V, and a vector x, this will decompose V into a series of two rotations, U and H, where U leaves x invariant and H contains x. Limited to 4D for now. See :cite:`hestenes-space-time`, Appendix B, Theorem 4. Parameters --------------- V : clifford.MultiVector rotor x : clifford.MultiVector vector Returns ------- H : clifford.Multivector rotor which contains x U : clifford.Multivector rotor which leaves x invariant ''' H2 = V * x * ~V * x.inv() # inv needed to handle signatures H = (1 + H2) / sqrt(abs(float(2 * (1 + H2(0))))) U = H * x * V * x.inv() return H, U
def sinc(x): return sin(x)/x def log_rotor(V): ''' Logarithm of a simple rotor ''' if (V(2)**2).grades() != {0}: print(V) # raise ValueError('Bivector is not a Blade.') if abs(V(2)) < global_eps(): return log(float(V(0))) # numpy's trig correctly chooses hyperbolic or not with Complex args theta = arccos(complex(V(0))) return V(2)/sinc(theta).real