# Copyright (c) 2009-2017, Matthew Brett and Christoph Gohlke
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# Many methods borrow heavily or entirely from transforms3d:
# https://github.com/matthew-brett/transforms3d
# They have mostly been modified to support batched operations.

import numpy as np
import itertools

'''
Rotations
=========
Note: these have caused many subtle bugs in the past.
Be careful while updating these methods and while using them in clever ways.
See MuJoCo documentation here: http://mujoco.org/book/modeling.html#COrientation
Conventions
-----------
    - All functions accept batches as well as individual rotations
    - All rotation conventions match respective MuJoCo defaults
    - All angles are in radians
    - Matricies follow LR convention
    - Euler Angles are all relative with 'xyz' axes ordering
    - See specific representation for more information
Representations
---------------
Euler
    There are many euler angle frames -- here we will strive to use the default
        in MuJoCo, which is eulerseq='xyz'.
    This frame is a relative rotating frame, about x, y, and z axes in order.
        Relative rotating means that after we rotate about x, then we use the
        new (rotated) y, and the same for z.
Quaternions
    These are defined in terms of rotation (angle) about a unit vector (x, y, z)
    We use the following <q0, q1, q2, q3> convention:
            q0 = cos(angle / 2)
            q1 = sin(angle / 2) * x
            q2 = sin(angle / 2) * y
            q3 = sin(angle / 2) * z
        This is also sometimes called qw, qx, qy, qz.
    Note that quaternions are ambiguous, because we can represent a rotation by
        angle about vector <x, y, z> and -angle about vector <-x, -y, -z>.
        To choose between these, we pick "first nonzero positive", where we
        make the first nonzero element of the quaternion positive.
    This can result in mismatches if you're converting an quaternion that is not
        "first nonzero positive" to a different representation and back.
Axis Angle
    (Not currently implemented)
    These are very straightforward.  Rotation is angle about a unit vector.
XY Axes
    (Not currently implemented)
    We are given x axis and y axis, and z axis is cross product of x and y.
Z Axis
    This is NOT RECOMMENDED.  Defines a unit vector for the Z axis,
        but rotation about this axis is not well defined.
    Instead pick a fixed reference direction for another axis (e.g. X)
        and calculate the other (e.g. Y = Z cross-product X),
        then use XY Axes rotation instead.
SO3
    (Not currently implemented)
    While not supported by MuJoCo, this representation has a lot of nice features.
    We expect to add support for these in the future.
TODO / Missing
--------------
    - Rotation integration or derivatives (e.g. velocity conversions)
    - More representations (SO3, etc)
    - Random sampling (e.g. sample uniform random rotation)
    - Performance benchmarks/measurements
    - (Maybe) define everything as to/from matricies, for simplicity
'''

# For testing whether a number is close to zero
_FLOAT_EPS = np.finfo(np.float64).eps
_EPS4 = _FLOAT_EPS * 4.0


def euler2mat(euler):
    """ Convert Euler Angles to Rotation Matrix.  See rotation.py for notes """
    euler = np.asarray(euler, dtype=np.float64)
    assert euler.shape[-1] == 3, "Invalid shaped euler {}".format(euler)

    ai, aj, ak = -euler[..., 2], -euler[..., 1], -euler[..., 0]
    si, sj, sk = np.sin(ai), np.sin(aj), np.sin(ak)
    ci, cj, ck = np.cos(ai), np.cos(aj), np.cos(ak)
    cc, cs = ci * ck, ci * sk
    sc, ss = si * ck, si * sk

    mat = np.empty(euler.shape[:-1] + (3, 3), dtype=np.float64)
    mat[..., 2, 2] = cj * ck
    mat[..., 2, 1] = sj * sc - cs
    mat[..., 2, 0] = sj * cc + ss
    mat[..., 1, 2] = cj * sk
    mat[..., 1, 1] = sj * ss + cc
    mat[..., 1, 0] = sj * cs - sc
    mat[..., 0, 2] = -sj
    mat[..., 0, 1] = cj * si
    mat[..., 0, 0] = cj * ci
    return mat


def euler2quat(euler):
    """ Convert Euler Angles to Quaternions.  See rotation.py for notes """
    euler = np.asarray(euler, dtype=np.float64)
    assert euler.shape[-1] == 3, "Invalid shape euler {}".format(euler)

    ai, aj, ak = euler[..., 2] / 2, -euler[..., 1] / 2, euler[..., 0] / 2
    si, sj, sk = np.sin(ai), np.sin(aj), np.sin(ak)
    ci, cj, ck = np.cos(ai), np.cos(aj), np.cos(ak)
    cc, cs = ci * ck, ci * sk
    sc, ss = si * ck, si * sk

    quat = np.empty(euler.shape[:-1] + (4,), dtype=np.float64)
    quat[..., 0] = cj * cc + sj * ss
    quat[..., 3] = cj * sc - sj * cs
    quat[..., 2] = -(cj * ss + sj * cc)
    quat[..., 1] = cj * cs - sj * sc
    return quat


def mat2euler(mat):
    """ Convert Rotation Matrix to Euler Angles.  See rotation.py for notes """
    mat = np.asarray(mat, dtype=np.float64)
    assert mat.shape[-2:] == (3, 3), "Invalid shape matrix {}".format(mat)

    cy = np.sqrt(mat[..., 2, 2] * mat[..., 2, 2] + mat[..., 1, 2] * mat[..., 1, 2])
    condition = cy > _EPS4
    euler = np.empty(mat.shape[:-1], dtype=np.float64)
    euler[..., 2] = np.where(condition,
                             -np.arctan2(mat[..., 0, 1], mat[..., 0, 0]),
                             -np.arctan2(-mat[..., 1, 0], mat[..., 1, 1]))
    euler[..., 1] = np.where(condition,
                             -np.arctan2(-mat[..., 0, 2], cy),
                             -np.arctan2(-mat[..., 0, 2], cy))
    euler[..., 0] = np.where(condition,
                             -np.arctan2(mat[..., 1, 2], mat[..., 2, 2]),
                             0.0)
    return euler


def mat2quat(mat):
    """ Convert Rotation Matrix to Quaternion.  See rotation.py for notes """
    mat = np.asarray(mat, dtype=np.float64)
    assert mat.shape[-2:] == (3, 3), "Invalid shape matrix {}".format(mat)

    Qxx, Qyx, Qzx = mat[..., 0, 0], mat[..., 0, 1], mat[..., 0, 2]
    Qxy, Qyy, Qzy = mat[..., 1, 0], mat[..., 1, 1], mat[..., 1, 2]
    Qxz, Qyz, Qzz = mat[..., 2, 0], mat[..., 2, 1], mat[..., 2, 2]
    # Fill only lower half of symmetric matrix
    K = np.zeros(mat.shape[:-2] + (4, 4), dtype=np.float64)
    K[..., 0, 0] = Qxx - Qyy - Qzz
    K[..., 1, 0] = Qyx + Qxy
    K[..., 1, 1] = Qyy - Qxx - Qzz
    K[..., 2, 0] = Qzx + Qxz
    K[..., 2, 1] = Qzy + Qyz
    K[..., 2, 2] = Qzz - Qxx - Qyy
    K[..., 3, 0] = Qyz - Qzy
    K[..., 3, 1] = Qzx - Qxz
    K[..., 3, 2] = Qxy - Qyx
    K[..., 3, 3] = Qxx + Qyy + Qzz
    K /= 3.0
    # TODO: vectorize this -- probably could be made faster
    q = np.empty(K.shape[:-2] + (4,))
    it = np.nditer(q[..., 0], flags=['multi_index'])
    while not it.finished:
        # Use Hermitian eigenvectors, values for speed
        vals, vecs = np.linalg.eigh(K[it.multi_index])
        # Select largest eigenvector, reorder to w,x,y,z quaternion
        q[it.multi_index] = vecs[[3, 0, 1, 2], np.argmax(vals)]
        # Prefer quaternion with positive w
        # (q * -1 corresponds to same rotation as q)
        if q[it.multi_index][0] < 0:
            q[it.multi_index] *= -1
        it.iternext()
    return q


def quat2euler(quat):
    """ Convert Quaternion to Euler Angles.  See rotation.py for notes """
    return mat2euler(quat2mat(quat))


def subtract_euler(e1, e2):
    assert e1.shape == e2.shape
    assert e1.shape[-1] == 3
    q1 = euler2quat(e1)
    q2 = euler2quat(e2)
    q_diff = quat_mul(q1, quat_conjugate(q2))
    return quat2euler(q_diff)


def quat2mat(quat):
    """ Convert Quaternion to Euler Angles.  See rotation.py for notes """
    quat = np.asarray(quat, dtype=np.float64)
    assert quat.shape[-1] == 4, "Invalid shape quat {}".format(quat)

    w, x, y, z = quat[..., 0], quat[..., 1], quat[..., 2], quat[..., 3]
    Nq = np.sum(quat * quat, axis=-1)
    s = 2.0 / Nq
    X, Y, Z = x * s, y * s, z * s
    wX, wY, wZ = w * X, w * Y, w * Z
    xX, xY, xZ = x * X, x * Y, x * Z
    yY, yZ, zZ = y * Y, y * Z, z * Z

    mat = np.empty(quat.shape[:-1] + (3, 3), dtype=np.float64)
    mat[..., 0, 0] = 1.0 - (yY + zZ)
    mat[..., 0, 1] = xY - wZ
    mat[..., 0, 2] = xZ + wY
    mat[..., 1, 0] = xY + wZ
    mat[..., 1, 1] = 1.0 - (xX + zZ)
    mat[..., 1, 2] = yZ - wX
    mat[..., 2, 0] = xZ - wY
    mat[..., 2, 1] = yZ + wX
    mat[..., 2, 2] = 1.0 - (xX + yY)
    return np.where((Nq > _FLOAT_EPS)[..., np.newaxis, np.newaxis], mat, np.eye(3))

def quat_conjugate(q):
    inv_q = -q
    inv_q[..., 0] *= -1
    return inv_q

def quat_mul(q0, q1):
    assert q0.shape == q1.shape
    assert q0.shape[-1] == 4
    assert q1.shape[-1] == 4

    w0 = q0[..., 0]
    x0 = q0[..., 1]
    y0 = q0[..., 2]
    z0 = q0[..., 3]

    w1 = q1[..., 0]
    x1 = q1[..., 1]
    y1 = q1[..., 2]
    z1 = q1[..., 3]

    w = w0 * w1 - x0 * x1 - y0 * y1 - z0 * z1
    x = w0 * x1 + x0 * w1 + y0 * z1 - z0 * y1
    y = w0 * y1 + y0 * w1 + z0 * x1 - x0 * z1
    z = w0 * z1 + z0 * w1 + x0 * y1 - y0 * x1
    q = np.array([w, x, y, z])
    if q.ndim == 2:
        q = q.swapaxes(0, 1)
    assert q.shape == q0.shape
    return q

def quat_rot_vec(q, v0):
    q_v0 = np.array([0, v0[0], v0[1], v0[2]])
    q_v = quat_mul(q, quat_mul(q_v0, quat_conjugate(q)))
    v = q_v[1:]
    return v

def quat_identity():
    return np.array([1, 0, 0, 0])

def quat2axisangle(quat):
    theta = 0;
    axis = np.array([0, 0, 1]);
    sin_theta = np.linalg.norm(quat[1:])

    if (sin_theta > 0.0001):
        theta = 2 * np.arcsin(sin_theta)
        theta *= 1 if quat[0] >= 0 else -1
        axis = quat[1:] / sin_theta

    return axis, theta

def euler2point_euler(euler):
    _euler = euler.copy()
    if len(_euler.shape) < 2:
        _euler = np.expand_dims(_euler,0)
    assert(_euler.shape[1] == 3)
    _euler_sin = np.sin(_euler)
    _euler_cos = np.cos(_euler)
    return np.concatenate([_euler_sin, _euler_cos], axis=-1)

def point_euler2euler(euler):
    _euler = euler.copy()
    if len(_euler.shape) < 2:
        _euler = np.expand_dims(_euler,0)
    assert(_euler.shape[1] == 6)
    angle = np.arctan(_euler[..., :3] / _euler[..., 3:])
    angle[_euler[..., 3:] < 0] += np.pi
    return angle

def quat2point_quat(quat):
    # Should be in qw, qx, qy, qz
    _quat = quat.copy()
    if len(_quat.shape) < 2:
        _quat = np.expand_dims(_quat, 0)
    assert(_quat.shape[1] == 4)
    angle = np.arccos(_quat[:,[0]]) * 2
    xyz = _quat[:, 1:]
    xyz[np.squeeze(np.abs(np.sin(angle/2))) >= 1e-5] = (xyz / np.sin(angle / 2))[np.squeeze(np.abs(np.sin(angle/2))) >= 1e-5]
    return np.concatenate([np.sin(angle),np.cos(angle), xyz], axis=-1)

def point_quat2quat(quat):
    _quat = quat.copy()
    if len(_quat.shape) < 2:
        _quat = np.expand_dims(_quat, 0)
    assert(_quat.shape[1] == 5)
    angle = np.arctan(_quat[:,[0]] / _quat[:,[1]])
    qw = np.cos(angle / 2)

    qxyz = _quat[:, 2:]
    qxyz[np.squeeze(np.abs(np.sin(angle/2))) >= 1e-5] = (qxyz * np.sin(angle/2))[np.squeeze(np.abs(np.sin(angle/2))) >= 1e-5]
    return np.concatenate([qw, qxyz], axis=-1)

def normalize_angles(angles):
    '''Puts angles in [-pi, pi] range.'''
    angles = angles.copy()
    if angles.size > 0:
        angles = (angles + np.pi) % (2 * np.pi) - np.pi
        assert -np.pi-1e-6 <= angles.min() and angles.max() <= np.pi+1e-6
    return angles

def round_to_straight_angles(angles):
    '''Returns closest angle modulo 90 degrees '''
    angles = np.round(angles / (np.pi / 2)) * (np.pi / 2)
    return normalize_angles(angles)

def get_parallel_rotations():
    mult90 = [0, np.pi/2, -np.pi/2, np.pi]
    parallel_rotations = []
    for euler in itertools.product(mult90, repeat=3):
        canonical = mat2euler(euler2mat(euler))
        canonical = np.round(canonical / (np.pi / 2))
        if canonical[0] == -2:
            canonical[0] = 2
        if canonical[2] == -2:
            canonical[2] = 2
        canonical *= np.pi / 2
        if all([(canonical != rot).any() for rot in parallel_rotations]):
            parallel_rotations += [canonical]
    assert len(parallel_rotations) == 24
    return parallel_rotations