本文整理汇总了Python中torch.asin方法的典型用法代码示例。如果您正苦于以下问题：Python torch.asin方法的具体用法？Python torch.asin怎么用？Python torch.asin使用的例子？那么恭喜您, 这里精选的方法代码示例或许可以为您提供帮助。您也可以进一步了解该方法所在类torch的用法示例。

在下文中一共展示了torch.asin方法的10个代码示例，这些例子默认根据受欢迎程度排序。您可以为喜欢或者感觉有用的代码点赞，您的评价将有助于我们的系统推荐出更棒的Python代码示例。

示例1: arcsin

# 需要导入模块: import torch [as 别名]
# 或者: from torch import asin [as 别名]
def arcsin(x, out=None):
    """
    Return the trigonometric arcsin, element-wise.

    Parameters
    ----------
    x : ht.DNDarray
        The value for which to compute the trigonometric cosine.
    out : ht.DNDarray or None, optional
        A location in which to store the results. If provided, it must have a broadcastable shape. If not provided
        or set to None, a fresh tensor is allocated.

    Returns
    -------
    arcsin : ht.DNDarray
        A tensor of the same shape as x, containing the trigonometric arcsin of each element in this tensor.
        Input elements outside [-1., 1.] are returned as nan. If out was provided, arcsin is a reference to it.

    Examples
    --------
    >>> ht.arcsin(ht.array([-1.,-0., 0.83]))
    tensor([-1.5708,  0.0000,  0.9791])
    """
    return local_op(torch.asin, x, out) 

示例2: test_with_terminate_on_inf

# 需要导入模块: import torch [as 别名]
# 或者: from torch import asin [as 别名]
def test_with_terminate_on_inf():

    torch.manual_seed(12)

    data = [
        1.0,
        0.8,
        torch.rand(4, 4),
        (1.0 / torch.randint(0, 2, size=(4,)).type(torch.float), torch.tensor(1.234)),
        torch.rand(5),
        torch.asin(torch.randn(4, 4)),
        0.0,
        1.0,
    ]

    def update_fn(engine, batch):
        return batch

    trainer = Engine(update_fn)
    h = TerminateOnNan()
    trainer.add_event_handler(Events.ITERATION_COMPLETED, h)

    trainer.run(data, max_epochs=2)
    assert trainer.state.iteration == 4 

示例3: __init__

# 需要导入模块: import torch [as 别名]
# 或者: from torch import asin [as 别名]
def __init__(self, size, complex=False, ABCD=None, ortho_init=False):
        """
        Parameters:
            size: size of butterfly matrix
            complex: real or complex matrix
            ABCD: block of [[A, B], [C, D]], of shape (2, 2, size//2) if real or (2, 2, size//2, 2) if complex
            ortho_init: whether the twiddle factors are initialized to be orthogonal (real) or unitary (complex)
        """
        super().__init__()
        assert size % 2 == 0, 'size must be even'
        self.size = size
        self.complex = complex
        self.mul_op = complex_mul if complex else operator.mul
        ABCD_shape = (2, 2, size // 2) if not complex else (2, 2, size // 2, 2)
        scaling = 1.0 / 2 if complex else 1.0 / math.sqrt(2)
        if ABCD is None:
            if not ortho_init:
                self.ABCD = nn.Parameter(torch.randn(ABCD_shape) * scaling)
            else:
                if not complex:
                    theta = torch.rand(size // 2) * math.pi * 2
                    c, s = torch.cos(theta), torch.sin(theta)
                    det = torch.randint(0, 2, (size // 2, ), dtype=c.dtype) * 2 - 1  # Rotation (+1) or reflection (-1)
                    self.ABCD = nn.Parameter(torch.stack((torch.stack((det * c, -det * s)),
                                                          torch.stack((s, c)))))
                else:
                    # Sampling from the Haar measure on U(2) is a bit subtle.
                    # Using the parameterization here: http://home.lu.lv/~sd20008/papers/essays/Random%20unitary%20[paper].pdf
                    phi = torch.asin(torch.sqrt(torch.rand(size // 2)))
                    c, s = torch.cos(phi), torch.sin(phi)
                    alpha, psi, chi = torch.randn(3, size // 2) * math.pi * 2
                    A = torch.stack((c * torch.cos(alpha + psi), c * torch.sin(alpha + psi)), dim=-1)
                    B = torch.stack((s * torch.cos(alpha + chi), s * torch.sin(alpha + chi)), dim=-1)
                    C = torch.stack((-s * torch.cos(alpha - chi), -s * torch.sin(alpha - chi)), dim=-1)
                    D = torch.stack((c * torch.cos(alpha - psi), c * torch.sin(alpha - psi)), dim=-1)
                    self.ABCD = nn.Parameter(torch.stack((torch.stack((A, B)),
                                                          torch.stack((C, D)))))
        else:
            assert ABCD.shape == ABCD_shape, f'ABCD must have shape {ABCD_shape}'
            self.ABCD = ABCD 

示例4: __init__

# 需要导入模块: import torch [as 别名]
# 或者: from torch import asin [as 别名]
def __init__(self, in_size, out_size, bias=True, complex=False, tied_weight=True, increasing_stride=True, ortho_init=False):
        super().__init__()
        self.in_size = in_size
        m = int(math.ceil(math.log2(in_size)))
        size = self.in_size_extended = 1 << m  # Will zero-pad input if in_size is not a power of 2
        self.out_size = out_size
        self.nstack = int(math.ceil(out_size / self.in_size_extended))
        self.complex = complex
        self.tied_weight = tied_weight
        self.increasing_stride = increasing_stride
        self.ortho_init = ortho_init
        twiddle_core_shape = (self.nstack, size - 1) if tied_weight else (self.nstack, m, size // 2)
        if not ortho_init:
            twiddle_shape = twiddle_core_shape + ((2, 2) if not complex else (2, 2, 2))
            scaling = 1.0 / 2 if complex else 1.0 / math.sqrt(2)
            self.twiddle = nn.Parameter(torch.randn(twiddle_shape) * scaling)
        else:
            if not complex:
                theta = torch.rand(twiddle_core_shape) * math.pi * 2
                c, s = torch.cos(theta), torch.sin(theta)
                det = torch.randint(0, 2, (twiddle_core_shape), dtype=c.dtype) * 2 - 1  # Rotation (+1) or reflection (-1)
                self.twiddle = nn.Parameter(torch.stack((torch.stack((det * c, -det * s), dim=-1),
                                                         torch.stack((s, c), dim=-1)), dim=-1))
            else:
                # Sampling from the Haar measure on U(2) is a bit subtle.
                # Using the parameterization here: http://home.lu.lv/~sd20008/papers/essays/Random%20unitary%20[paper].pdf
                phi = torch.asin(torch.sqrt(torch.rand(twiddle_core_shape)))
                c, s = torch.cos(phi), torch.sin(phi)
                alpha, psi, chi = torch.randn((3, ) + twiddle_core_shape) * math.pi * 2
                A = torch.stack((c * torch.cos(alpha + psi), c * torch.sin(alpha + psi)), dim=-1)
                B = torch.stack((s * torch.cos(alpha + chi), s * torch.sin(alpha + chi)), dim=-1)
                C = torch.stack((-s * torch.cos(alpha - chi), -s * torch.sin(alpha - chi)), dim=-1)
                D = torch.stack((c * torch.cos(alpha - psi), c * torch.sin(alpha - psi)), dim=-1)
                self.twiddle = nn.Parameter(torch.stack((torch.stack((A, B), dim=-2),
                                                         torch.stack((C, D), dim=-2)), dim=-2))
        if bias:
            bias_shape = (out_size, ) if not complex else (out_size, 2)
            self.bias = nn.Parameter(torch.Tensor(bias_shape))
        else:
            self.register_parameter('bias', None)
        self.reset_parameters() 

示例5: quan_to_angle

# 需要导入模块: import torch [as 别名]
# 或者: from torch import asin [as 别名]
def quan_to_angle(qw, qx, qy, qz):
    rx = torch.atan2(2.*(qw*qx + qy*qz), 1.-2.*(qx*qx + qy*qy))

    sinp = 2.*(qw*qy - qz*qx)
    sinp = sinp.clamp(-1., 1.)
    ry = torch.asin(sinp)

    rz = torch.atan2(2.*(qw*qz + qx*qy), 1.-2.*(qy*qy + qz*qz))

    return rx, ry, rz 

示例6: aten_asin

# 需要导入模块: import torch [as 别名]
# 或者: from torch import asin [as 别名]
def aten_asin(inputs, attributes, scope):
    inp = inputs[0]
    ctx = current_context()
    net = ctx.network
    if ctx.is_tensorrt and has_trt_tensor(inputs):
        layer = net.add_unary(inp, trt.UnaryOperation.ASIN)
        output = layer.get_output(0)
        output.name = scope
        layer.name = scope
        return [output]
    elif ctx.is_tvm and has_tvm_tensor(inputs):
        raise NotImplementedError

    return [torch.asin(inp)] 

示例7: test_with_terminate_on_nan

# 需要导入模块: import torch [as 别名]
# 或者: from torch import asin [as 别名]
def test_with_terminate_on_nan():

    torch.manual_seed(12)

    data = [1.0, 0.8, (torch.rand(4, 4), torch.rand(4, 4)), torch.rand(5), torch.asin(torch.randn(4, 4)), 0.0, 1.0]

    def update_fn(engine, batch):
        return batch

    trainer = Engine(update_fn)
    h = TerminateOnNan()
    trainer.add_event_handler(Events.ITERATION_COMPLETED, h)

    trainer.run(data, max_epochs=2)
    assert trainer.state.iteration == 5 

示例8: asin

# 需要导入模块: import torch [as 别名]
# 或者: from torch import asin [as 别名]
def asin(t):
    """
    Element-wise arcsine computed using cross-approximation; see PyTorch's `asin()`.

    :param t: input :class:`Tensor`

    :return: a :class:`Tensor`
    """

    return tn.cross(lambda x: torch.asin(x), tensors=t, verbose=False) 

示例9: qeuler

# 需要导入模块: import torch [as 别名]
# 或者: from torch import asin [as 别名]
def qeuler(q, order, epsilon=0):
    """
    Convert quaternion(s) q to Euler angles.
    Expects a tensor of shape (*, 4), where * denotes any number of dimensions.
    Returns a tensor of shape (*, 3).
    """
    assert q.shape[-1] == 4
    
    original_shape = list(q.shape)
    original_shape[-1] = 3
    q = q.view(-1, 4)
    
    q0 = q[:, 0]
    q1 = q[:, 1]
    q2 = q[:, 2]
    q3 = q[:, 3]
    
    if order == 'xyz':
        x = torch.atan2(2 * (q0 * q1 - q2 * q3), 1 - 2*(q1 * q1 + q2 * q2))
        y = torch.asin(torch.clamp(2 * (q1 * q3 + q0 * q2), -1+epsilon, 1-epsilon))
        z = torch.atan2(2 * (q0 * q3 - q1 * q2), 1 - 2*(q2 * q2 + q3 * q3))
    elif order == 'yzx':
        x = torch.atan2(2 * (q0 * q1 - q2 * q3), 1 - 2*(q1 * q1 + q3 * q3))
        y = torch.atan2(2 * (q0 * q2 - q1 * q3), 1 - 2*(q2 * q2 + q3 * q3))
        z = torch.asin(torch.clamp(2 * (q1 * q2 + q0 * q3), -1+epsilon, 1-epsilon))
    elif order == 'zxy':
        x = torch.asin(torch.clamp(2 * (q0 * q1 + q2 * q3), -1+epsilon, 1-epsilon))
        y = torch.atan2(2 * (q0 * q2 - q1 * q3), 1 - 2*(q1 * q1 + q2 * q2))
        z = torch.atan2(2 * (q0 * q3 - q1 * q2), 1 - 2*(q1 * q1 + q3 * q3))
    elif order == 'xzy':
        x = torch.atan2(2 * (q0 * q1 + q2 * q3), 1 - 2*(q1 * q1 + q3 * q3))
        y = torch.atan2(2 * (q0 * q2 + q1 * q3), 1 - 2*(q2 * q2 + q3 * q3))
        z = torch.asin(torch.clamp(2 * (q0 * q3 - q1 * q2), -1+epsilon, 1-epsilon))
    elif order == 'yxz':
        x = torch.asin(torch.clamp(2 * (q0 * q1 - q2 * q3), -1+epsilon, 1-epsilon))
        y = torch.atan2(2 * (q1 * q3 + q0 * q2), 1 - 2*(q1 * q1 + q2 * q2))
        z = torch.atan2(2 * (q1 * q2 + q0 * q3), 1 - 2*(q1 * q1 + q3 * q3))
    elif order == 'zyx':
        x = torch.atan2(2 * (q0 * q1 + q2 * q3), 1 - 2*(q1 * q1 + q2 * q2))
        y = torch.asin(torch.clamp(2 * (q0 * q2 - q1 * q3), -1+epsilon, 1-epsilon))
        z = torch.atan2(2 * (q0 * q3 + q1 * q2), 1 - 2*(q2 * q2 + q3 * q3))
    else:
        raise

    return torch.stack((x, y, z), dim=1).view(original_shape)

# Numpy-backed implementations 

示例10: rotmat2euler_torch

# 需要导入模块: import torch [as 别名]
# 或者: from torch import asin [as 别名]
def rotmat2euler_torch(R):
    """
    Converts a rotation matrix to euler angles
    batch pytorch version ported from the corresponding numpy method above

    :param R:N*3*3
    :return: N*3
    """
    n = R.data.shape[0]
    eul = Variable(torch.zeros(n, 3).float()).cuda()
    idx_spec1 = (R[:, 0, 2] == 1).nonzero().cpu().data.numpy().reshape(-1).tolist()
    idx_spec2 = (R[:, 0, 2] == -1).nonzero().cpu().data.numpy().reshape(-1).tolist()
    if len(idx_spec1) > 0:
        R_spec1 = R[idx_spec1, :, :]
        eul_spec1 = Variable(torch.zeros(len(idx_spec1), 3).float()).cuda()
        eul_spec1[:, 2] = 0
        eul_spec1[:, 1] = -np.pi / 2
        delta = torch.atan2(R_spec1[:, 0, 1], R_spec1[:, 0, 2])
        eul_spec1[:, 0] = delta
        eul[idx_spec1, :] = eul_spec1

    if len(idx_spec2) > 0:
        R_spec2 = R[idx_spec2, :, :]
        eul_spec2 = Variable(torch.zeros(len(idx_spec2), 3).float()).cuda()
        eul_spec2[:, 2] = 0
        eul_spec2[:, 1] = np.pi / 2
        delta = torch.atan2(R_spec2[:, 0, 1], R_spec2[:, 0, 2])
        eul_spec2[:, 0] = delta
        eul[idx_spec2] = eul_spec2

    idx_remain = np.arange(0, n)
    idx_remain = np.setdiff1d(np.setdiff1d(idx_remain, idx_spec1), idx_spec2).tolist()
    if len(idx_remain) > 0:
        R_remain = R[idx_remain, :, :]
        eul_remain = Variable(torch.zeros(len(idx_remain), 3).float()).cuda()
        eul_remain[:, 1] = -torch.asin(R_remain[:, 0, 2])
        eul_remain[:, 0] = torch.atan2(R_remain[:, 1, 2] / torch.cos(eul_remain[:, 1]),
                                       R_remain[:, 2, 2] / torch.cos(eul_remain[:, 1]))
        eul_remain[:, 2] = torch.atan2(R_remain[:, 0, 1] / torch.cos(eul_remain[:, 1]),
                                       R_remain[:, 0, 0] / torch.cos(eul_remain[:, 1]))
        eul[idx_remain, :] = eul_remain

    return eul 

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torch：torch五项是检查什么

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