"""
Utility functions of matrix and vector transformations.

NOTE: convention for quaternions is (x, y, z, w)
"""

import math
import numpy as np
from scipy import linalg


PI = np.pi
EPS = np.finfo(float).eps * 4.

# axis sequences for Euler angles
_NEXT_AXIS = [1, 2, 0, 1]

# map axes strings to/from tuples of inner axis, parity, repetition, frame
_AXES2TUPLE = {
    "sxyz": (0, 0, 0, 0),
    "sxyx": (0, 0, 1, 0),
    "sxzy": (0, 1, 0, 0),
    "sxzx": (0, 1, 1, 0),
    "syzx": (1, 0, 0, 0),
    "syzy": (1, 0, 1, 0),
    "syxz": (1, 1, 0, 0),
    "syxy": (1, 1, 1, 0),
    "szxy": (2, 0, 0, 0),
    "szxz": (2, 0, 1, 0),
    "szyx": (2, 1, 0, 0),
    "szyz": (2, 1, 1, 0),
    "rzyx": (0, 0, 0, 1),
    "rxyx": (0, 0, 1, 1),
    "ryzx": (0, 1, 0, 1),
    "rxzx": (0, 1, 1, 1),
    "rxzy": (1, 0, 0, 1),
    "ryzy": (1, 0, 1, 1),
    "rzxy": (1, 1, 0, 1),
    "ryxy": (1, 1, 1, 1),
    "ryxz": (2, 0, 0, 1),
    "rzxz": (2, 0, 1, 1),
    "rxyz": (2, 1, 0, 1),
    "rzyz": (2, 1, 1, 1),
}

_TUPLE2AXES = dict((v, k) for k, v in _AXES2TUPLE.items())


def convert_quat(q, to="xyzw"):
    """
    Converts quaternion from one convention to another.
    The convention to convert TO is specified as an optional argument.
    If to == 'xyzw', then the input is in 'wxyz' format, and vice-versa.

    Args:
        q: a 4-dim numpy array corresponding to a quaternion
        to: a string, either 'xyzw' or 'wxyz', determining
            which convention to convert to.
    """
    if to == "xyzw":
        return q[[1, 2, 3, 0]]
    if to == "wxyz":
        return q[[3, 0, 1, 2]]
    raise Exception("convert_quat: choose a valid `to` argument (xyzw or wxyz)")


def quat_multiply(quaternion1, quaternion0):
    """Return multiplication of two quaternions.
    >>> q = quat_multiply([1, -2, 3, 4], [-5, 6, 7, 8])
    >>> np.allclose(q, [-44, -14, 48, 28])
    True
    """
    x0, y0, z0, w0 = quaternion0
    x1, y1, z1, w1 = quaternion1
    return np.array(
        (
            x1 * w0 + y1 * z0 - z1 * y0 + w1 * x0,
            -x1 * z0 + y1 * w0 + z1 * x0 + w1 * y0,
            x1 * y0 - y1 * x0 + z1 * w0 + w1 * z0,
            -x1 * x0 - y1 * y0 - z1 * z0 + w1 * w0,
        ),
        dtype=np.float32,
    )


def quat_conjugate(quaternion):
    """Return conjugate of quaternion.
    >>> q0 = random_quaternion()
    >>> q1 = quat_conjugate(q0)
    >>> q1[3] == q0[3] and all(q1[:3] == -q0[:3])
    True
    """
    return np.array(
        (-quaternion[0], -quaternion[1], -quaternion[2], quaternion[3]),
        dtype=np.float32,
    )


def quat_inverse(quaternion):
    """Return inverse of quaternion.
    >>> q0 = random_quaternion()
    >>> q1 = quat_inverse(q0)
    >>> np.allclose(quat_multiply(q0, q1), [0, 0, 0, 1])
    True
    """
    return quat_conjugate(quaternion) / np.dot(quaternion, quaternion)


def quat_distance(quaternion1, quaternion0):
    """
    Returns distance between two quaternions, such that distance * quaternion0 = quaternion1

    Note: Assumes quaternion in form: {x,y,z,w}
    """
    return quat_multiply(quaternion1, quat_inverse(quaternion0))


def quat_slerp(quat0, quat1, fraction, spin=0, shortestpath=True):
    """Return spherical linear interpolation between two quaternions.
    >>> q0 = random_quat()
    >>> q1 = random_quat()
    >>> q = quat_slerp(q0, q1, 0.0)
    >>> np.allclose(q, q0)
    True
    >>> q = quat_slerp(q0, q1, 1.0, 1)
    >>> np.allclose(q, q1)
    True
    >>> q = quat_slerp(q0, q1, 0.5)
    >>> angle = math.acos(np.dot(q0, q))
    >>> np.allclose(2.0, math.acos(np.dot(q0, q1)) / angle) or \
        np.allclose(2.0, math.acos(-np.dot(q0, q1)) / angle)
    True
    """
    q0 = unit_vector(quat0[:4])
    q1 = unit_vector(quat1[:4])
    if fraction == 0.0:
        return q0
    elif fraction == 1.0:
        return q1
    d = np.dot(q0, q1)
    if abs(abs(d) - 1.0) < EPS:
        return q0
    if shortestpath and d < 0.0:
        # invert rotation
        d = -d
        q1 *= -1.0
    angle = math.acos(np.clip(d, -1, 1)) + spin * math.pi
    if abs(angle) < EPS:
        return q0
    isin = 1.0 / math.sin(angle)
    q0 *= math.sin((1.0 - fraction) * angle) * isin
    q1 *= math.sin(fraction * angle) * isin
    q0 += q1
    return q0


def random_quat(rand=None):
    """Return uniform random unit quaternion.
    rand: array like or None
        Three independent random variables that are uniformly distributed
        between 0 and 1.
    >>> q = random_quat()
    >>> np.allclose(1.0, vector_norm(q))
    True
    >>> q = random_quat(np.random.random(3))
    >>> q.shape
    (4,)
    """
    if rand is None:
        rand = np.random.rand(3)
    else:
        assert len(rand) == 3
    r1 = np.sqrt(1.0 - rand[0])
    r2 = np.sqrt(rand[0])
    pi2 = math.pi * 2.0
    t1 = pi2 * rand[1]
    t2 = pi2 * rand[2]
    return np.array(
        (np.sin(t1) * r1, np.cos(t1) * r1, np.sin(t2) * r2, np.cos(t2) * r2),
        dtype=np.float32,
    )


def vec(values):
    """
    Converts value tuple into a numpy vector.

    Args:
        values: a tuple of numbers

    Returns:
        a numpy vector of given values
    """
    return np.array(values, dtype=np.float32)


def mat4(array):
    """
    Converts an array to 4x4 matrix.

    Args:
        array: the array in form of vec, list, or tuple

    Returns:
        a 4x4 numpy matrix
    """
    return np.array(array, dtype=np.float32).reshape((4, 4))


def mat2pose(hmat):
    """
    Converts a homogeneous 4x4 matrix into pose.

    Args:
        hmat: a 4x4 homogeneous matrix

    Returns:
        (pos, orn) tuple where pos is vec3 float in cartesian,
            orn is vec4 float quaternion
    """
    pos = hmat[:3, 3]
    orn = mat2quat(hmat[:3, :3])
    return pos, orn


def mat2quat(rmat, precise=False):
    """
    Converts given rotation matrix to quaternion.

    Args:
        rmat: 3x3 rotation matrix
        precise: If isprecise is True, the input matrix is assumed to be a precise
             rotation matrix and a faster algorithm is used.

    Returns:
        vec4 float quaternion angles
    """
    M = np.array(rmat, dtype=np.float32, copy=False)[:3, :3]
    if precise:
        q = np.empty((4,))
        t = np.trace(M)
        if t > M[3, 3]:
            q[0] = t
            q[3] = M[1, 0] - M[0, 1]
            q[2] = M[0, 2] - M[2, 0]
            q[1] = M[2, 1] - M[1, 2]
        else:
            i, j, k = 0, 1, 2
            if M[1, 1] > M[0, 0]:
                i, j, k = 1, 2, 0
            if M[2, 2] > M[i, i]:
                i, j, k = 2, 0, 1
            t = M[i, i] - (M[j, j] + M[k, k]) + M[3, 3]
            q[i] = t
            q[j] = M[i, j] + M[j, i]
            q[k] = M[k, i] + M[i, k]
            q[3] = M[k, j] - M[j, k]
            q = q[[3, 0, 1, 2]]
        q *= 0.5 / math.sqrt(t * M[3, 3])
    else:
        m00 = M[0, 0]
        m01 = M[0, 1]
        m02 = M[0, 2]
        m10 = M[1, 0]
        m11 = M[1, 1]
        m12 = M[1, 2]
        m20 = M[2, 0]
        m21 = M[2, 1]
        m22 = M[2, 2]
        # symmetric matrix K
        K = np.array(
            [
                [m00 - m11 - m22, 0.0, 0.0, 0.0],
                [m01 + m10, m11 - m00 - m22, 0.0, 0.0],
                [m02 + m20, m12 + m21, m22 - m00 - m11, 0.0],
                [m21 - m12, m02 - m20, m10 - m01, m00 + m11 + m22],
            ]
        )
        K /= 3.0
        # quaternion is Eigen vector of K that corresponds to largest eigenvalue
        w, V = linalg.eigh(K)
        q = V[[3, 0, 1, 2], np.argmax(w)]
    if q[0] < 0.0:
        np.negative(q, q)
    return q[[1, 2, 3, 0]]


def euler2mat(euler: object) -> object: #assume xyz

    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 mat2euler(rmat, axes="sxyz"):
    """
    Converts given rotation matrix to euler angles in radian.

    Args:
        rmat: 3x3 rotation matrix
        axes: One of 24 axis sequences as string or encoded tuple

    Returns:
        converted euler angles in radian vec3 float
    """
    try:
        firstaxis, parity, repetition, frame = _AXES2TUPLE[axes.lower()]
    except (AttributeError, KeyError):
        firstaxis, parity, repetition, frame = axes

    i = firstaxis
    j = _NEXT_AXIS[i + parity]
    k = _NEXT_AXIS[i - parity + 1]

    M = np.array(rmat, dtype=np.float32, copy=False)[:3, :3]
    if repetition:
        sy = math.sqrt(M[i, j] * M[i, j] + M[i, k] * M[i, k])
        if sy > EPS:
            ax = math.atan2(M[i, j], M[i, k])
            ay = math.atan2(sy, M[i, i])
            az = math.atan2(M[j, i], -M[k, i])
        else:
            ax = math.atan2(-M[j, k], M[j, j])
            ay = math.atan2(sy, M[i, i])
            az = 0.0
    else:
        cy = math.sqrt(M[i, i] * M[i, i] + M[j, i] * M[j, i])
        if cy > EPS:
            ax = math.atan2(M[k, j], M[k, k])
            ay = math.atan2(-M[k, i], cy)
            az = math.atan2(M[j, i], M[i, i])
        else:
            ax = math.atan2(-M[j, k], M[j, j])
            ay = math.atan2(-M[k, i], cy)
            az = 0.0

    if parity:
        ax, ay, az = -ax, -ay, -az
    if frame:
        ax, az = az, ax
    return vec((ax, ay, az))


def pose2mat(pose):
    """
    Converts pose to homogeneous matrix.

    Args:
        pose: a (pos, orn) tuple where pos is vec3 float cartesian, and
            orn is vec4 float quaternion.

    Returns:
        4x4 homogeneous matrix
    """
    homo_pose_mat = np.zeros((4, 4), dtype=np.float32)
    homo_pose_mat[:3, :3] = quat2mat(pose[1])
    homo_pose_mat[:3, 3] = np.array(pose[0], dtype=np.float32)
    homo_pose_mat[3, 3] = 1.
    return homo_pose_mat


def quat2mat(quaternion):
    """
    Converts given quaternion (x, y, z, w) to matrix.

    Args:
        quaternion: vec4 float angles

    Returns:
        3x3 rotation matrix
    """
    q = np.array(quaternion, dtype=np.float32, copy=True)[[3, 0, 1, 2]]
    n = np.dot(q, q)
    if n < EPS:
        return np.identity(3)
    q *= math.sqrt(2.0 / n)
    q = np.outer(q, q)
    return np.array(
        [
            [1.0 - q[2, 2] - q[3, 3], q[1, 2] - q[3, 0], q[1, 3] + q[2, 0]],
            [q[1, 2] + q[3, 0], 1.0 - q[1, 1] - q[3, 3], q[2, 3] - q[1, 0]],
            [q[1, 3] - q[2, 0], q[2, 3] + q[1, 0], 1.0 - q[1, 1] - q[2, 2]],
        ]
    )


def pose_in_A_to_pose_in_B(pose_A, pose_A_in_B):
    """
    Converts a homogenous matrix corresponding to a point C in frame A
    to a homogenous matrix corresponding to the same point C in frame B.

    Args:
        pose_A: numpy array of shape (4,4) corresponding to the pose of C in frame A
        pose_A_in_B: numpy array of shape (4,4) corresponding to the pose of A in frame B

    Returns:
        numpy array of shape (4,4) corresponding to the pose of C in frame B
    """

    # pose of A in B takes a point in A and transforms it to a point in C.

    # pose of C in B = pose of A in B * pose of C in A
    # take a point in C, transform it to A, then to B
    # T_B^C = T_A^C * T_B^A
    return pose_A_in_B.dot(pose_A)


def pose_inv(pose):
    """
    Computes the inverse of a homogenous matrix corresponding to the pose of some
    frame B in frame A. The inverse is the pose of frame A in frame B.

    Args:
        pose: numpy array of shape (4,4) for the pose to inverse

    Returns:
        numpy array of shape (4,4) for the inverse pose
    """

    # Note, the inverse of a pose matrix is the following
    # [R t; 0 1]^-1 = [R.T -R.T*t; 0 1]

    # Intuitively, this makes sense.
    # The original pose matrix translates by t, then rotates by R.
    # We just invert the rotation by applying R-1 = R.T, and also translate back.
    # Since we apply translation first before rotation, we need to translate by
    # -t in the original frame, which is -R-1*t in the new frame, and then rotate back by
    # R-1 to align the axis again.

    pose_inv = np.zeros((4, 4))
    pose_inv[:3, :3] = pose[:3, :3].T
    pose_inv[:3, 3] = -pose_inv[:3, :3].dot(pose[:3, 3])
    pose_inv[3, 3] = 1.0
    return pose_inv


def _skew_symmetric_translation(pos_A_in_B):
    """
    Helper function to get a skew symmetric translation matrix for converting quantities
    between frames.
    """
    return np.array(
        [
            0.,
            -pos_A_in_B[2],
            pos_A_in_B[1],
            pos_A_in_B[2],
            0.,
            -pos_A_in_B[0],
            -pos_A_in_B[1],
            pos_A_in_B[0],
            0.,
        ]
    ).reshape((3, 3))


def vel_in_A_to_vel_in_B(vel_A, ang_vel_A, pose_A_in_B):
    """
    Converts linear and angular velocity of a point in frame A to the equivalent in frame B.

    Args:
        vel_A: 3-dim iterable for linear velocity in A
        ang_vel_A: 3-dim iterable for angular velocity in A
        pose_A_in_B: numpy array of shape (4,4) corresponding to the pose of A in frame B

    Returns:
        vel_B, ang_vel_B: two numpy arrays of shape (3,) for the velocities in B
    """
    pos_A_in_B = pose_A_in_B[:3, 3]
    rot_A_in_B = pose_A_in_B[:3, :3]
    skew_symm = _skew_symmetric_translation(pos_A_in_B)
    vel_B = rot_A_in_B.dot(vel_A) + skew_symm.dot(rot_A_in_B.dot(ang_vel_A))
    ang_vel_B = rot_A_in_B.dot(ang_vel_A)
    return vel_B, ang_vel_B


def force_in_A_to_force_in_B(force_A, torque_A, pose_A_in_B):
    """
    Converts linear and rotational force at a point in frame A to the equivalent in frame B.

    Args:
        force_A: 3-dim iterable for linear force in A
        torque_A: 3-dim iterable for rotational force (moment) in A
        pose_A_in_B: numpy array of shape (4,4) corresponding to the pose of A in frame B

    Returns:
        force_B, torque_B: two numpy arrays of shape (3,) for the forces in B
    """
    pos_A_in_B = pose_A_in_B[:3, 3]
    rot_A_in_B = pose_A_in_B[:3, :3]
    skew_symm = _skew_symmetric_translation(pos_A_in_B)
    force_B = rot_A_in_B.T.dot(force_A)
    torque_B = -rot_A_in_B.T.dot(skew_symm.dot(force_A)) + rot_A_in_B.T.dot(torque_A)
    return force_B, torque_B


def rotation_matrix(angle, direction, point=None):
    """
    Returns matrix to rotate about axis defined by point and direction.

    Examples:

        >>> angle = (random.random() - 0.5) * (2*math.pi)
        >>> direc = numpy.random.random(3) - 0.5
        >>> point = numpy.random.random(3) - 0.5
        >>> R0 = rotation_matrix(angle, direc, point)
        >>> R1 = rotation_matrix(angle-2*math.pi, direc, point)
        >>> is_same_transform(R0, R1)
        True
        >>> R0 = rotation_matrix(angle, direc, point)
        >>> R1 = rotation_matrix(-angle, -direc, point)
        >>> is_same_transform(R0, R1)
        True
        >>> I = numpy.identity(4, numpy.float32)
        >>> numpy.allclose(I, rotation_matrix(math.pi*2, direc))
        True
        >>> numpy.allclose(2., numpy.trace(rotation_matrix(math.pi/2,
        ...                                                direc, point)))
        True

    """
    sina = math.sin(angle)
    cosa = math.cos(angle)
    direction = unit_vector(direction[:3])
    # rotation matrix around unit vector
    R = np.array(
        ((cosa, 0.0, 0.0), (0.0, cosa, 0.0), (0.0, 0.0, cosa)), dtype=np.float32
    )
    R += np.outer(direction, direction) * (1.0 - cosa)
    direction *= sina
    R += np.array(
        (
            (0.0, -direction[2], direction[1]),
            (direction[2], 0.0, -direction[0]),
            (-direction[1], direction[0], 0.0),
        ),
        dtype=np.float32,
    )
    M = np.identity(4)
    M[:3, :3] = R
    if point is not None:
        # rotation not around origin
        point = np.array(point[:3], dtype=np.float32, copy=False)
        M[:3, 3] = point - np.dot(R, point)
    return M


def clip_translation(dpos, limit):
    """
    Limits a translation (delta position) to a specified limit

    Scales down the norm of the dpos to 'limit' if norm(dpos) > limit, else returns immediately

    :param dpos: n-dim Translation being clipped (e,g.: (x, y, z)) -- numpy array
    :param limit: Value to limit translation by -- magnitude (scalar, in same units as input)
    :return: Clipped translation (same dimension as inputs) and whether the value was clipped or not
    """
    input_norm = linalg.norm(dpos)
    return (dpos * limit / input_norm, True) if input_norm > limit else (dpos, False)


def clip_rotation(quat, limit):
    """
    Limits a (delta) rotation to a specified limit

    Converts rotation to axis-angle, clips, then re-converts back into quaternion

    :param quat: Rotation being clipped (x, y, z, w) -- numpy array
    :param limit: Value to limit rotation by -- magnitude (scalar, in radians)
    :return: Clipped rotation quaternion (x, y, z, w) and whether the value was clipped or not
    """
    clipped = False

    # First, normalize the quaternion
    quat = quat / linalg.norm(quat)

    den = np.sqrt(max(1 - quat[3] * quat[3], 0))
    if den == 0:
        # This is a zero degree rotation, immediately return
        return quat, clipped
    else:
        # This is all other cases
        x = quat[0] / den
        y = quat[1] / den
        z = quat[2] / den
        a = 2 * math.acos(quat[3])

    # Clip rotation if necessary and return clipped quat
    if abs(a) > limit:
        a = limit * np.sign(a) / 2
        sa = math.sin(a)
        ca = math.cos(a)
        quat = np.array([
            x * sa,
            y * sa,
            z * sa,
            ca
        ])
        clipped = True

    return quat, clipped


def make_pose(translation, rotation):
    """
    Makes a homogenous pose matrix from a translation vector and a rotation matrix.

    Args:
        translation: a 3-dim iterable
        rotation: a 3x3 matrix

    Returns:
        pose: a 4x4 homogenous matrix
    """
    pose = np.zeros((4, 4))
    pose[:3, :3] = rotation
    pose[:3, 3] = translation
    pose[3, 3] = 1.0
    return pose


def unit_vector(data, axis=None, out=None):
    """
    Returns ndarray normalized by length, i.e. eucledian norm, along axis.

    Examples:

        >>> v0 = numpy.random.random(3)
        >>> v1 = unit_vector(v0)
        >>> numpy.allclose(v1, v0 / numpy.linalg.norm(v0))
        True
        >>> v0 = numpy.random.rand(5, 4, 3)
        >>> v1 = unit_vector(v0, axis=-1)
        >>> v2 = v0 / numpy.expand_dims(numpy.sqrt(numpy.sum(v0*v0, axis=2)), 2)
        >>> numpy.allclose(v1, v2)
        True
        >>> v1 = unit_vector(v0, axis=1)
        >>> v2 = v0 / numpy.expand_dims(numpy.sqrt(numpy.sum(v0*v0, axis=1)), 1)
        >>> numpy.allclose(v1, v2)
        True
        >>> v1 = numpy.empty((5, 4, 3), dtype=numpy.float32)
        >>> unit_vector(v0, axis=1, out=v1)
        >>> numpy.allclose(v1, v2)
        True
        >>> list(unit_vector([]))
        []
        >>> list(unit_vector([1.0]))
        [1.0]

    """
    if out is None:
        data = np.array(data, dtype=np.float32, copy=True)
        if data.ndim == 1:
            data /= math.sqrt(np.dot(data, data))
            return data
    else:
        if out is not data:
            out[:] = np.array(data, copy=False)
        data = out
    length = np.atleast_1d(np.sum(data * data, axis))
    np.sqrt(length, length)
    if axis is not None:
        length = np.expand_dims(length, axis)
    data /= length
    if out is None:
        return data


def get_orientation_error(target_orn, current_orn):
    """
    Returns the difference between two quaternion orientations as a 3 DOF numpy array.
    For use in an impedance controller / task-space PD controller.

    Args:
        target_orn: 4-dim iterable, desired orientation as a (x, y, z, w) quaternion
        current_orn: 4-dim iterable, current orientation as a (x, y, z, w) quaternion

    Returns:
        orn_error: 3-dim numpy array for current orientation error, corresponds to
            (target_orn - current_orn)
    """
    current_orn = np.array(
        [current_orn[3], current_orn[0], current_orn[1], current_orn[2]]
    )
    target_orn = np.array([target_orn[3], target_orn[0], target_orn[1], target_orn[2]])

    pinv = np.zeros((3, 4))
    pinv[0, :] = [-current_orn[1], current_orn[0], -current_orn[3], current_orn[2]]
    pinv[1, :] = [-current_orn[2], current_orn[3], current_orn[0], -current_orn[1]]
    pinv[2, :] = [-current_orn[3], -current_orn[2], current_orn[1], current_orn[0]]
    orn_error = 2.0 * pinv.dot(np.array(target_orn))
    return orn_error


def get_pose_error(target_pose, current_pose):
    """
    Computes the error corresponding to target pose - current pose as a 6-dim vector.
    The first 3 components correspond to translational error while the last 3 components
    correspond to the rotational error.

    Args:
        target_pose: a 4x4 homogenous matrix for the target pose
        current_pose: a 4x4 homogenous matrix for the current pose

    Returns:
        A 6-dim numpy array for the pose error.
    """
    error = np.zeros(6)

    # compute translational error
    target_pos = target_pose[:3, 3]
    current_pos = current_pose[:3, 3]
    pos_err = target_pos - current_pos

    # compute rotational error
    r1 = current_pose[:3, 0]
    r2 = current_pose[:3, 1]
    r3 = current_pose[:3, 2]
    r1d = target_pose[:3, 0]
    r2d = target_pose[:3, 1]
    r3d = target_pose[:3, 2]
    rot_err = 0.5 * (np.cross(r1, r1d) + np.cross(r2, r2d) + np.cross(r3, r3d))

    error[:3] = pos_err
    error[3:] = rot_err
    return error
