| from typing import Optional |
|
|
| import torch |
| import torch.nn.functional as F |
|
|
|
|
| def quaternion_to_axis_angle(quaternions: torch.Tensor) -> torch.Tensor: |
| """ |
| Convert rotations given as quaternions to axis/angle. |
| |
| Args: |
| quaternions: quaternions with real part first, |
| as tensor of shape (..., 4). |
| |
| Returns: |
| Rotations given as a vector in axis angle form, as a tensor |
| of shape (..., 3), where the magnitude is the angle |
| turned anticlockwise in radians around the vector's |
| direction. |
| """ |
| norms = torch.norm(quaternions[..., 1:], p=2, dim=-1, keepdim=True) |
| half_angles = torch.atan2(norms, quaternions[..., :1]) |
| angles = 2 * half_angles |
| eps = 1e-6 |
| small_angles = angles.abs() < eps |
| sin_half_angles_over_angles = torch.empty_like(angles) |
| sin_half_angles_over_angles[~small_angles] = ( |
| torch.sin(half_angles[~small_angles]) / angles[~small_angles] |
| ) |
| |
| |
| sin_half_angles_over_angles[small_angles] = ( |
| 0.5 - (angles[small_angles] * angles[small_angles]) / 48 |
| ) |
| return quaternions[..., 1:] / sin_half_angles_over_angles |
|
|
|
|
| def matrix_to_quaternion(matrix: torch.Tensor) -> torch.Tensor: |
| """ |
| Convert rotations given as rotation matrices to quaternions. |
| |
| Args: |
| matrix: Rotation matrices as tensor of shape (..., 3, 3). |
| |
| Returns: |
| quaternions with real part first, as tensor of shape (..., 4). |
| """ |
| if matrix.size(-1) != 3 or matrix.size(-2) != 3: |
| raise ValueError(f"Invalid rotation matrix shape {matrix.shape}.") |
|
|
| batch_dim = matrix.shape[:-2] |
| m00, m01, m02, m10, m11, m12, m20, m21, m22 = torch.unbind( |
| matrix.reshape(batch_dim + (9,)), dim=-1 |
| ) |
|
|
| q_abs = _sqrt_positive_part( |
| torch.stack( |
| [ |
| 1.0 + m00 + m11 + m22, |
| 1.0 + m00 - m11 - m22, |
| 1.0 - m00 + m11 - m22, |
| 1.0 - m00 - m11 + m22, |
| ], |
| dim=-1, |
| ) |
| ) |
|
|
| |
| quat_by_rijk = torch.stack( |
| [ |
| |
| |
| torch.stack([q_abs[..., 0] ** 2, m21 - m12, m02 - m20, m10 - m01], dim=-1), |
| |
| |
| torch.stack([m21 - m12, q_abs[..., 1] ** 2, m10 + m01, m02 + m20], dim=-1), |
| |
| |
| torch.stack([m02 - m20, m10 + m01, q_abs[..., 2] ** 2, m12 + m21], dim=-1), |
| |
| |
| torch.stack([m10 - m01, m20 + m02, m21 + m12, q_abs[..., 3] ** 2], dim=-1), |
| ], |
| dim=-2, |
| ) |
|
|
| |
| |
| flr = torch.tensor(0.1).to(dtype=q_abs.dtype, device=q_abs.device) |
| quat_candidates = quat_by_rijk / (2.0 * q_abs[..., None].max(flr)) |
|
|
| |
| |
|
|
| return quat_candidates[ |
| F.one_hot(q_abs.argmax(dim=-1), num_classes=4) > 0.5, : |
| ].reshape(batch_dim + (4,)) |
|
|
|
|
| def _sqrt_positive_part(x: torch.Tensor) -> torch.Tensor: |
| """ |
| Returns torch.sqrt(torch.max(0, x)) |
| but with a zero subgradient where x is 0. |
| """ |
| ret = torch.zeros_like(x) |
| positive_mask = x > 0 |
| ret[positive_mask] = torch.sqrt(x[positive_mask]) |
| return ret |
|
|
|
|
| def matrix_to_axis_angle(matrix: torch.Tensor) -> torch.Tensor: |
| """ |
| Convert rotations given as rotation matrices to axis/angle. |
| |
| Args: |
| matrix: Rotation matrices as tensor of shape (..., 3, 3). |
| |
| Returns: |
| Rotations given as a vector in axis angle form, as a tensor |
| of shape (..., 3), where the magnitude is the angle |
| turned anticlockwise in radians around the vector's |
| direction. |
| """ |
| return quaternion_to_axis_angle(matrix_to_quaternion(matrix)) |
|
|
|
|
| def euler_angles_to_axis_angle( |
| euler_angles: torch.Tensor, convention: str |
| ) -> torch.Tensor: |
| """ |
| Convert rotations given as Euler angles in radians to axis/angle. |
| |
| Args: |
| euler_angles: Euler angles in radians as tensor of shape (..., 3). |
| convention: Convention string of three uppercase letters from |
| {"X", "Y", and "Z"}. |
| |
| Returns: |
| Rotations given as a vector in axis angle form, as a tensor |
| of shape (..., 3), where the magnitude is the angle |
| turned anticlockwise in radians around the vector's |
| direction. |
| """ |
| return matrix_to_axis_angle(euler_angles_to_matrix(euler_angles, convention)) |
|
|
|
|
| def euler_angles_to_matrix(euler_angles: torch.Tensor, convention: str) -> torch.Tensor: |
| """ |
| Convert rotations given as Euler angles in radians to rotation matrices. |
| |
| Args: |
| euler_angles: Euler angles in radians as tensor of shape (..., 3). |
| convention: Convention string of three uppercase letters from |
| {"X", "Y", and "Z"}. |
| |
| Returns: |
| Rotation matrices as tensor of shape (..., 3, 3). |
| """ |
| if euler_angles.dim() == 0 or euler_angles.shape[-1] != 3: |
| raise ValueError("Invalid input euler angles.") |
| if len(convention) != 3: |
| raise ValueError("Convention must have 3 letters.") |
| if convention[1] in (convention[0], convention[2]): |
| raise ValueError(f"Invalid convention {convention}.") |
| for letter in convention: |
| if letter not in ("X", "Y", "Z"): |
| raise ValueError(f"Invalid letter {letter} in convention string.") |
| matrices = [ |
| _axis_angle_rotation(c, e) |
| for c, e in zip(convention, torch.unbind(euler_angles, -1)) |
| ] |
| |
| return torch.matmul(torch.matmul(matrices[0], matrices[1]), matrices[2]) |
|
|
|
|
| def _axis_angle_rotation(axis: str, angle: torch.Tensor) -> torch.Tensor: |
| """ |
| Return the rotation matrices for one of the rotations about an axis |
| of which Euler angles describe, for each value of the angle given. |
| |
| Args: |
| axis: Axis label "X" or "Y or "Z". |
| angle: any shape tensor of Euler angles in radians |
| |
| Returns: |
| Rotation matrices as tensor of shape (..., 3, 3). |
| """ |
|
|
| cos = torch.cos(angle) |
| sin = torch.sin(angle) |
| one = torch.ones_like(angle) |
| zero = torch.zeros_like(angle) |
|
|
| if axis == "X": |
| R_flat = (one, zero, zero, zero, cos, -sin, zero, sin, cos) |
| elif axis == "Y": |
| R_flat = (cos, zero, sin, zero, one, zero, -sin, zero, cos) |
| elif axis == "Z": |
| R_flat = (cos, -sin, zero, sin, cos, zero, zero, zero, one) |
| else: |
| raise ValueError("letter must be either X, Y or Z.") |
|
|
| return torch.stack(R_flat, -1).reshape(angle.shape + (3, 3)) |
|
|
|
|
| def axis_angle_to_quaternion(axis_angle: torch.Tensor) -> torch.Tensor: |
| """ |
| Convert rotations given as axis/angle to quaternions. |
| |
| Args: |
| axis_angle: Rotations given as a vector in axis angle form, |
| as a tensor of shape (..., 3), where the magnitude is |
| the angle turned anticlockwise in radians around the |
| vector's direction. |
| |
| Returns: |
| quaternions with real part first, as tensor of shape (..., 4). |
| """ |
| angles = torch.norm(axis_angle, p=2, dim=-1, keepdim=True) |
| half_angles = angles * 0.5 |
| eps = 1e-6 |
| small_angles = angles.abs() < eps |
| sin_half_angles_over_angles = torch.empty_like(angles) |
| sin_half_angles_over_angles[~small_angles] = ( |
| torch.sin(half_angles[~small_angles]) / angles[~small_angles] |
| ) |
| |
| |
| sin_half_angles_over_angles[small_angles] = ( |
| 0.5 - (angles[small_angles] * angles[small_angles]) / 48 |
| ) |
| quaternions = torch.cat( |
| [torch.cos(half_angles), axis_angle * sin_half_angles_over_angles], dim=-1 |
| ) |
| return quaternions |
|
|
|
|
| def axis_angle_to_matrix(axis_angle: torch.Tensor) -> torch.Tensor: |
| """ |
| Convert rotations given as axis/angle to rotation matrices. |
| |
| Args: |
| axis_angle: Rotations given as a vector in axis angle form, |
| as a tensor of shape (..., 3), where the magnitude is |
| the angle turned anticlockwise in radians around the |
| vector's direction. |
| |
| Returns: |
| Rotation matrices as tensor of shape (..., 3, 3). |
| """ |
| return quaternion_to_matrix(axis_angle_to_quaternion(axis_angle)) |
|
|
|
|
| def quaternion_to_matrix(quaternions: torch.Tensor) -> torch.Tensor: |
| """ |
| Convert rotations given as quaternions to rotation matrices. |
| |
| Args: |
| quaternions: quaternions with real part first, |
| as tensor of shape (..., 4). |
| |
| Returns: |
| Rotation matrices as tensor of shape (..., 3, 3). |
| """ |
| r, i, j, k = torch.unbind(quaternions, -1) |
| |
| two_s = 2.0 / (quaternions * quaternions).sum(-1) |
|
|
| o = torch.stack( |
| ( |
| 1 - two_s * (j * j + k * k), |
| two_s * (i * j - k * r), |
| two_s * (i * k + j * r), |
| two_s * (i * j + k * r), |
| 1 - two_s * (i * i + k * k), |
| two_s * (j * k - i * r), |
| two_s * (i * k - j * r), |
| two_s * (j * k + i * r), |
| 1 - two_s * (i * i + j * j), |
| ), |
| -1, |
| ) |
| return o.reshape(quaternions.shape[:-1] + (3, 3)) |
|
|
|
|
| def axis_angle_to_euler_angles(axis_angle: torch.Tensor) -> torch.Tensor: |
| """ |
| Convert rotations given as Euler angles in radians to axis/angle. |
| |
| Args: |
| axis_angle: Rotations given as a vector in axis angle form, |
| as a tensor of shape (..., 3), where the magnitude is |
| the angle turned anticlockwise in radians around the |
| vector's direction. |
| Returns: |
| Rotations given as a vector in axis angle form, as a tensor |
| of shape (..., 3), where the magnitude is the angle |
| turned anticlockwise in radians around the vector's |
| direction. |
| """ |
| return matrix_to_euler_angles(axis_angle_to_matrix(axis_angle), "XYZ") |
|
|
|
|
| def _angle_from_tan( |
| axis: str, other_axis: str, data, horizontal: bool, tait_bryan: bool |
| ) -> torch.Tensor: |
| """ |
| Extract the first or third Euler angle from the two members of |
| the matrix which are positive constant times its sine and cosine. |
| |
| Args: |
| axis: Axis label "X" or "Y or "Z" for the angle we are finding. |
| other_axis: Axis label "X" or "Y or "Z" for the middle axis in the |
| convention. |
| data: Rotation matrices as tensor of shape (..., 3, 3). |
| horizontal: Whether we are looking for the angle for the third axis, |
| which means the relevant entries are in the same row of the |
| rotation matrix. If not, they are in the same column. |
| tait_bryan: Whether the first and third axes in the convention differ. |
| |
| Returns: |
| Euler Angles in radians for each matrix in data as a tensor |
| of shape (...). |
| """ |
|
|
| i1, i2 = {"X": (2, 1), "Y": (0, 2), "Z": (1, 0)}[axis] |
| if horizontal: |
| i2, i1 = i1, i2 |
| even = (axis + other_axis) in ["XY", "YZ", "ZX"] |
| if horizontal == even: |
| return torch.atan2(data[..., i1], data[..., i2]) |
| if tait_bryan: |
| return torch.atan2(-data[..., i2], data[..., i1]) |
| return torch.atan2(data[..., i2], -data[..., i1]) |
|
|
|
|
| def _index_from_letter(letter: str) -> int: |
| if letter == "X": |
| return 0 |
| if letter == "Y": |
| return 1 |
| if letter == "Z": |
| return 2 |
| raise ValueError("letter must be either X, Y or Z.") |
|
|
|
|
| def matrix_to_euler_angles(matrix: torch.Tensor, convention: str) -> torch.Tensor: |
| """ |
| Convert rotations given as rotation matrices to Euler angles in radians. |
| |
| Args: |
| matrix: Rotation matrices as tensor of shape (..., 3, 3). |
| convention: Convention string of three uppercase letters. |
| |
| Returns: |
| Euler angles in radians as tensor of shape (..., 3). |
| """ |
| if len(convention) != 3: |
| raise ValueError("Convention must have 3 letters.") |
| if convention[1] in (convention[0], convention[2]): |
| raise ValueError(f"Invalid convention {convention}.") |
| for letter in convention: |
| if letter not in ("X", "Y", "Z"): |
| raise ValueError(f"Invalid letter {letter} in convention string.") |
| if matrix.size(-1) != 3 or matrix.size(-2) != 3: |
| raise ValueError(f"Invalid rotation matrix shape {matrix.shape}.") |
| i0 = _index_from_letter(convention[0]) |
| i2 = _index_from_letter(convention[2]) |
| tait_bryan = i0 != i2 |
| if tait_bryan: |
| central_angle = torch.asin( |
| matrix[..., i0, i2] * (-1.0 if i0 - i2 in [-1, 2] else 1.0) |
| ) |
| else: |
| central_angle = torch.acos(matrix[..., i0, i0]) |
|
|
| o = ( |
| _angle_from_tan( |
| convention[0], convention[1], matrix[..., i2], False, tait_bryan |
| ), |
| central_angle, |
| _angle_from_tan( |
| convention[2], convention[1], matrix[..., i0, :], True, tait_bryan |
| ), |
| ) |
| return torch.stack(o, -1) |
|
|
|
|
| def rotation_6d_to_matrix(d6: torch.Tensor) -> torch.Tensor: |
| """ |
| Converts 6D rotation representation by Zhou et al. [1] to rotation matrix |
| using Gram--Schmidt orthogonalisation per Section B of [1]. |
| Args: |
| d6: 6D rotation representation, of size (*, 6) |
| |
| Returns: |
| batch of rotation matrices of size (*, 3, 3) |
| |
| [1] Zhou, Y., Barnes, C., Lu, J., Yang, J., & Li, H. |
| On the Continuity of Rotation Representations in Neural Networks. |
| IEEE Conference on Computer Vision and Pattern Recognition, 2019. |
| Retrieved from http://arxiv.org/abs/1812.07035 |
| """ |
|
|
| a1, a2 = d6[..., :3], d6[..., 3:] |
| b1 = F.normalize(a1, dim=-1) |
| b2 = a2 - (b1 * a2).sum(-1, keepdim=True) * b1 |
| b2 = F.normalize(b2, dim=-1) |
| b3 = torch.cross(b1, b2, dim=-1) |
| return torch.stack((b1, b2, b3), dim=-2) |
|
|
|
|
| def matrix_to_rotation_6d(matrix: torch.Tensor) -> torch.Tensor: |
| """ |
| Converts rotation matrices to 6D rotation representation by Zhou et al. [1] |
| by dropping the last row. Note that 6D representation is not unique. |
| Args: |
| matrix: batch of rotation matrices of size (*, 3, 3) |
| |
| Returns: |
| 6D rotation representation, of size (*, 6) |
| |
| [1] Zhou, Y., Barnes, C., Lu, J., Yang, J., & Li, H. |
| On the Continuity of Rotation Representations in Neural Networks. |
| IEEE Conference on Computer Vision and Pattern Recognition, 2019. |
| Retrieved from http://arxiv.org/abs/1812.07035 |
| """ |
| return matrix[..., :2, :].clone().reshape(*matrix.size()[:-2], 6) |
|
|
|
|
| def axis_angle_to_rotation_6d(axis_angle: torch.Tensor) -> torch.Tensor: |
| return matrix_to_rotation_6d(axis_angle_to_matrix(axis_angle)) |
|
|
|
|
| def rotation_6d_to_axis_angle(d6: torch.Tensor) -> torch.Tensor: |
| return matrix_to_axis_angle(rotation_6d_to_matrix(d6)) |
|
|