def bev_box_encode(boxes, anchors, encode_angle_to_vector=False, smooth_dim=False):
"""box encode for VoxelNet
Args:
boxes ([N, 7] Tensor): normal boxes: x, y, z, l, w, h, r
anchors ([N, 7] Tensor): anchors
"""
xa, ya, wa, la, ra = paddle.split(anchors, 5, axis=-1)
xg, yg, wg, lg, rg = paddle.split(boxes, 5, axis=-1)
diagonal = paddle.sqrt(la**2 + wa**2)
xt = (xg - xa) / diagonal
yt = (yg - ya) / diagonal
if smooth_dim:
lt = lg / la - 1
wt = wg / wa - 1
else:
lt = paddle.log(lg / la)
wt = paddle.log(wg / wa)
if encode_angle_to_vector:
rgx = paddle.cos(rg)
rgy = paddle.sin(rg)
rax = paddle.cos(ra)
ray = paddle.sin(ra)
rtx = rgx - rax
rty = rgy - ray
return paddle.concat([xt, yt, wt, lt, rtx, rty], axis=-1)
else:
rt = rg - ra
return paddle.concat([xt, yt, wt, lt, rt], axis=-1)
def __measure_parameterized(self, state, which_qubits, result_desired,
theta):
r"""进行参数化的测量。
Args:
state (Tensor): 输入的量子态
which_qubits (list): 测量作用的量子比特编号
result_desired (str): 期望得到的测量结果
theta (Tensor): 测量运算的参数
Returns:
Tensor: 测量坍塌后的量子态
Tensor：测量坍塌得到的概率
str: 测量得到的结果
"""
n = self.get_qubit_number()
assert len(which_qubits) == len(result_desired), \
"the length of qubits wanted to be measured and the result desired should be same"
op_list = [paddle.to_tensor(np.eye(2, dtype=np.complex128))] * n
for idx in range(0, len(which_qubits)):
i = which_qubits[idx]
ele = result_desired[idx]
if int(ele) == 0:
basis0 = paddle.to_tensor(
np.array([[1, 0], [0, 0]], dtype=np.complex128))
basis1 = paddle.to_tensor(
np.array([[0, 0], [0, 1]], dtype=np.complex128))
rho0 = multiply(basis0, cos(theta[idx]))
rho1 = multiply(basis1, sin(theta[idx]))
rho = add(rho0, rho1)
op_list[i] = rho
elif int(ele) == 1:
# rho = diag(concat([cos(theta[idx]), sin(theta[idx])]))
# rho = paddle.to_tensor(rho, zeros((2, 2), dtype="float64"))
basis0 = paddle.to_tensor(
np.array([[1, 0], [0, 0]], dtype=np.complex128))
basis1 = paddle.to_tensor(
np.array([[0, 0], [0, 1]], dtype=np.complex128))
rho0 = multiply(basis0, sin(theta[idx]))
rho1 = multiply(basis1, cos(theta[idx]))
rho = add(rho0, rho1)
op_list[i] = rho
else:
print("cannot recognize the result_desired.")
# rho = paddle.to_tensor(ones((2, 2), dtype="float64"), zeros((2, 2), dtype="float64"))
measure_operator = paddle.to_tensor(op_list[0])
if n > 1:
for idx in range(1, len(op_list)):
measure_operator = kron(measure_operator, op_list[idx])
state_measured = matmul(matmul(measure_operator, state),
dagger(measure_operator))
prob = real(
trace(
matmul(matmul(dagger(measure_operator), measure_operator),
state)))
state_measured = divide(state_measured, prob)
return state_measured, prob, result_desired
def compute_rot_loss(output, target_bin, target_res, mask):
# output: (B, 128, 8) [bin1_cls[0], bin1_cls[1], bin1_sin, bin1_cos,
# bin2_cls[0], bin2_cls[1], bin2_sin, bin2_cos]
# target_bin: (B, 128, 2) [bin1_cls, bin2_cls]
# target_res: (B, 128, 2) [bin1_res, bin2_res]
# mask: (B, 128, 1)
# import pdb; pdb.set_trace()
# output = output.view(-1, 8)
# target_bin = target_bin.view(-1, 2)
# target_res = target_res.view(-1, 2)
# mask = mask.view(-1, 1)
output = output.reshape(-1, 8)
target_bin = target_bin.reshape(-1, 2)
target_res = target_res.reshape(-1, 2)
mask = mask.reshape(-1, 1)
loss_bin1 = compute_bin_loss(output[:, 0:2], target_bin[:, 0], mask)
loss_bin2 = compute_bin_loss(output[:, 4:6], target_bin[:, 1], mask)
# loss_res = torch.zeros_like(loss_bin1)
loss_res = paddle.zeros_like(loss_bin1, dtype='float32')
if target_bin[:, 0].nonzero().shape[0] > 0:
idx1 = target_bin[:, 0].nonzero()[:, 0]
# valid_output1 = torch.index_select(output, 0, idx1.long())
valid_output1 = paddle.index_select(output, idx1.cast('int32'), 0)
# valid_target_res1 = torch.index_select(target_res, 0, idx1.long())
valid_target_res1 = paddle.index_select(target_res, idx1.cast('int32'),
0)
# loss_sin1 = compute_res_loss(
# valid_output1[:, 2], torch.sin(valid_target_res1[:, 0]))
# loss_cos1 = compute_res_loss(
# valid_output1[:, 3], torch.cos(valid_target_res1[:, 0]))
loss_sin1 = compute_res_loss(valid_output1[:, 2],
paddle.sin(valid_target_res1[:, 0]))
loss_cos1 = compute_res_loss(valid_output1[:, 3],
paddle.cos(valid_target_res1[:, 0]))
loss_res += loss_sin1 + loss_cos1
if target_bin[:, 1].nonzero().shape[0] > 0:
idx2 = target_bin[:, 1].nonzero()[:, 0]
# valid_output2 = torch.index_select(output, 0, idx2.long())
# valid_target_res2 = torch.index_select(target_res, 0, idx2.long())
valid_output2 = paddle.index_select(output, idx2.cast('int32'), 0)
valid_target_res2 = paddle.index_select(target_res, idx2.cast('int32'),
0)
# loss_sin2 = compute_res_loss(
# valid_output2[:, 6], torch.sin(valid_target_res2[:, 1]))
# loss_cos2 = compute_res_loss(
# valid_output2[:, 7], torch.cos(valid_target_res2[:, 1]))
loss_sin2 = compute_res_loss(valid_output2[:, 6],
paddle.sin(valid_target_res2[:, 1]))
loss_cos2 = compute_res_loss(valid_output2[:, 7],
paddle.cos(valid_target_res2[:, 1]))
loss_res += loss_sin2 + loss_cos2
return loss_bin1 + loss_bin2 + loss_res
def delta2rbox(rrois,
deltas,
means=[0, 0, 0, 0, 0],
stds=[1, 1, 1, 1, 1],
wh_ratio_clip=1e-6):
"""
:param rrois: (cx, cy, w, h, theta)
:param deltas: (dx, dy, dw, dh, dtheta)
:param means:
:param stds:
:param wh_ratio_clip:
:return:
"""
means = paddle.to_tensor(means)
stds = paddle.to_tensor(stds)
deltas = paddle.reshape(deltas, [-1, deltas.shape[-1]])
denorm_deltas = deltas * stds + means
dx = denorm_deltas[:, 0]
dy = denorm_deltas[:, 1]
dw = denorm_deltas[:, 2]
dh = denorm_deltas[:, 3]
dangle = denorm_deltas[:, 4]
max_ratio = np.abs(np.log(wh_ratio_clip))
dw = paddle.clip(dw, min=-max_ratio, max=max_ratio)
dh = paddle.clip(dh, min=-max_ratio, max=max_ratio)
rroi_x = rrois[:, 0]
rroi_y = rrois[:, 1]
rroi_w = rrois[:, 2]
rroi_h = rrois[:, 3]
rroi_angle = rrois[:, 4]
gx = dx * rroi_w * paddle.cos(rroi_angle) - dy * rroi_h * paddle.sin(
rroi_angle) + rroi_x
gy = dx * rroi_w * paddle.sin(rroi_angle) + dy * rroi_h * paddle.cos(
rroi_angle) + rroi_y
gw = rroi_w * dw.exp()
gh = rroi_h * dh.exp()
ga = np.pi * dangle + rroi_angle
ga = (ga + np.pi / 4) % np.pi - np.pi / 4
ga = paddle.to_tensor(ga)
gw = paddle.to_tensor(gw, dtype='float32')
gh = paddle.to_tensor(gh, dtype='float32')
bboxes = paddle.stack([gx, gy, gw, gh, ga], axis=-1)
return bboxes
def rotation_3d_in_axis(points, angles, axis=0):
# points: [N, point_size, 3]
# angles: [N]
rot_sin = paddle.sin(angles)
rot_cos = paddle.cos(angles)
ones = paddle.ones_like(rot_cos)
zeros = paddle.zeros_like(rot_cos)
if axis == 1:
rot_mat_T = paddle.stack([
paddle.stack([rot_cos, zeros, -rot_sin]),
paddle.stack([zeros, ones, zeros]),
paddle.stack([rot_sin, zeros, rot_cos])
])
elif axis == 2 or axis == -1:
rot_mat_T = paddle.stack([
paddle.stack([rot_cos, -rot_sin, zeros]),
paddle.stack([rot_sin, rot_cos, zeros]),
paddle.stack([zeros, zeros, ones])
])
elif axis == 0:
rot_mat_T = paddle.stack([
paddle.stack([zeros, rot_cos, -rot_sin]),
paddle.stack([zeros, rot_sin, rot_cos]),
paddle.stack([ones, zeros, zeros])
])
else:
raise ValueError("axis should in range")
return paddle.einsum('aij,jka->aik', (points, rot_mat_T))
def bev_box_decode(box_encodings, anchors, encode_angle_to_vector=False, smooth_dim=False):
"""box decode for VoxelNet in lidar
Args:
boxes ([N, 7] Tensor): normal boxes: x, y, z, w, l, h, r
anchors ([N, 7] Tensor): anchors
"""
xa, ya, wa, la, ra = paddle.split(anchors, 5, axis=-1)
if encode_angle_to_vector:
xt, yt, wt, lt, rtx, rty = paddle.split(
box_encodings, 1, axis=-1)
else:
xt, yt, wt, lt, rt = paddle.split(box_encodings, 5, axis=-1)
# xt, yt, zt, wt, lt, ht, rt = paddle.split(box_encodings, 1, axis=-1)
diagonal = paddle.sqrt(la**2 + wa**2)
xg = xt * diagonal + xa
yg = yt * diagonal + ya
if smooth_dim:
lg = (lt + 1) * la
wg = (wt + 1) * wa
else:
lg = paddle.exp(lt) * la
wg = paddle.exp(wt) * wa
if encode_angle_to_vector:
rax = paddle.cos(ra)
ray = paddle.sin(ra)
rgx = rtx + rax
rgy = rty + ray
rg = atan2(rgy, rgx)
else:
rg = rt + ra
return paddle.concat([xg, yg, wg, lg, rg], axis=-1)
def get_neg_score(self,
heads,
relations,
tails,
batch_size,
mini_batch_size,
neg_sample_size,
neg_head=True):
mini_batch_num = int(batch_size / mini_batch_size)
if neg_head:
hidden_dim = heads.shape[-1]
re_tail, im_tail = paddle.chunk(tails, chunks=2, axis=-1)
phase_rel = relations / (self.emb_init / np.pi)
re_rel, im_rel = paddle.cos(phase_rel), paddle.sin(phase_rel)
real = re_tail * re_rel + im_tail * im_rel
imag = -re_tail * im_rel + im_tail * re_rel
emb_complex = paddle.concat([real, imag], axis=-1)
score = emb_complex.reshape([mini_batch_num, -1, 1, hidden_dim])
heads = heads.reshape([mini_batch_num, 1, -1, hidden_dim])
score = score - heads
re_score, im_score = paddle.chunk(score, chunks=2, axis=1)
score = paddle.stack(
[re_score, im_score], axis=-1).norm(
p=2, axis=-1)
return self.gamma - score.sum(-1)
else:
hidden_dim = heads.shape[-1]
re_head, im_head = paddle.chunk(heads, chunks=2, axis=-1)
phase_rel = relations / (self.emb_init / np.pi)
re_rel, im_rel = paddle.cos(phase_rel), paddle.sin(phase_rel)
real = re_head * re_rel - im_head * im_rel
imag = re_head * im_rel + im_head * re_rel
emb_complex = paddle.concat([real, imag], axis=-1)
score = emb_complex.reshape([mini_batch_num, -1, 1, hidden_dim])
tails = tails.reshape([mini_batch_num, 1, -1, hidden_dim])
score = score - tails
re_score, im_score = paddle.chunk(score, chunks=2, axis=1)
score = paddle.stack(
[re_score, im_score], axis=-1).norm(
p=2, axis=-1)
return self.gamma - score.sum(-1)
def create_matrix(self):
cs = paddle.cos(self.theta / 2)
sn = paddle.sin(self.theta / 2)
self.matrix = paddle.concat([
paddle.concat([cs, -sn], axis=1),
paddle.concat([sn, cs], axis=1),
],
axis=0)
def u_gate_matrix(params):
"""
U3
:param params:
:return:
"""
theta, phi, lam = params
if (type(theta) is paddle.Tensor and type(phi) is paddle.Tensor
and type(lam) is paddle.Tensor):
re_a = paddle.cos(theta / 2)
re_b = -paddle.cos(lam) * paddle.sin(theta / 2)
re_c = paddle.cos(phi) * paddle.sin(theta / 2)
re_d = paddle.cos(phi + lam) * paddle.cos(theta / 2)
im_a = paddle.zeros([1], 'float64')
im_b = -paddle.sin(lam) * paddle.sin(theta / 2)
im_c = paddle.sin(phi) * paddle.sin(theta / 2)
im_d = paddle.sin(phi + lam) * paddle.cos(theta / 2)
re = paddle.reshape(paddle.concat([re_a, re_b, re_c, re_d]), [2, 2])
im = paddle.reshape(paddle.concat([im_a, im_b, im_c, im_d]), [2, 2])
return re + im * paddle.to_tensor([1j], 'complex128')
elif (type(theta) is float and type(phi) is float and type(lam) is float):
return np.array(
[[np.cos(theta / 2), -np.exp(1j * lam) * np.sin(theta / 2)],
[
np.exp(1j * phi) * np.sin(theta / 2),
np.exp(1j * phi + 1j * lam) * np.cos(theta / 2)
]])
else:
assert False
def delta2rbox(self, rrois, deltas, wh_ratio_clip=1e-6):
"""
:param rrois: (cx, cy, w, h, theta)
:param deltas: (dx, dy, dw, dh, dtheta)
:param means: means of anchor
:param stds: stds of anchor
:param wh_ratio_clip: clip threshold of wh_ratio
:return:
"""
deltas = paddle.reshape(deltas, [-1, 5])
rrois = paddle.reshape(rrois, [-1, 5])
# fix dy2st bug denorm_deltas = deltas * self.stds + self.means
denorm_deltas = paddle.add(
paddle.multiply(deltas, self.stds), self.means)
dx = denorm_deltas[:, 0]
dy = denorm_deltas[:, 1]
dw = denorm_deltas[:, 2]
dh = denorm_deltas[:, 3]
dangle = denorm_deltas[:, 4]
max_ratio = np.abs(np.log(wh_ratio_clip))
dw = paddle.clip(dw, min=-max_ratio, max=max_ratio)
dh = paddle.clip(dh, min=-max_ratio, max=max_ratio)
rroi_x = rrois[:, 0]
rroi_y = rrois[:, 1]
rroi_w = rrois[:, 2]
rroi_h = rrois[:, 3]
rroi_angle = rrois[:, 4]
gx = dx * rroi_w * paddle.cos(rroi_angle) - dy * rroi_h * paddle.sin(
rroi_angle) + rroi_x
gy = dx * rroi_w * paddle.sin(rroi_angle) + dy * rroi_h * paddle.cos(
rroi_angle) + rroi_y
gw = rroi_w * dw.exp()
gh = rroi_h * dh.exp()
ga = np.pi * dangle + rroi_angle
ga = (ga + np.pi / 4) % np.pi - np.pi / 4
ga = paddle.to_tensor(ga)
gw = paddle.to_tensor(gw, dtype='float32')
gh = paddle.to_tensor(gh, dtype='float32')
bboxes = paddle.stack([gx, gy, gw, gh, ga], axis=-1)
return bboxes
def xywhr2xyrs(self, xywhr):
xywhr = paddle.reshape(xywhr, [-1, 5])
xy = xywhr[:, :2]
wh = paddle.clip(xywhr[:, 2:4], min=1e-7, max=1e7)
r = xywhr[:, 4]
cos_r = paddle.cos(r)
sin_r = paddle.sin(r)
R = paddle.stack(
(cos_r, -sin_r, sin_r, cos_r), axis=-1).reshape([-1, 2, 2])
S = 0.5 * paddle.nn.functional.diag_embed(wh)
return xy, R, S
def positional_embedding(self, inputs):
seq_len = inputs.shape[1]
pos_seq = paddle.arange(0, seq_len, dtype=dtype_float)
indices = paddle.arange(0, self.head_dim, 2, dtype=dtype_float)
indices = 1 / 10000**(indices / self.head_dim)
sinusoid_inp = paddle.einsum("i,d->id", pos_seq, indices)
pos_emb = paddle.concat(
[paddle.sin(sinusoid_inp),
paddle.cos(sinusoid_inp)], axis=-1)
pos_emb = paddle.reshape(pos_emb, (1, 1, seq_len, self.head_dim))
pos_emb.stop_gradient = True
return pos_emb
def delta2rbox(self, rrois, deltas, means, stds, wh_ratio_clip=1e-6):
"""
:param rrois: (cx, cy, w, h, theta)
:param deltas: (dx, dy, dw, dh, dtheta)
:param means: means of anchor
:param stds: stds of anchor
:param wh_ratio_clip: clip threshold of wh_ratio
:return:
"""
deltas = paddle.reshape(deltas, [-1, 5])
rrois = paddle.reshape(rrois, [-1, 5])
pd_means = paddle.ones(shape=[5]) * means
pd_stds = paddle.ones(shape=[5]) * stds
denorm_deltas = deltas * pd_stds + pd_means
dx = denorm_deltas[:, 0]
dy = denorm_deltas[:, 1]
dw = denorm_deltas[:, 2]
dh = denorm_deltas[:, 3]
dangle = denorm_deltas[:, 4]
max_ratio = np.abs(np.log(wh_ratio_clip))
dw = paddle.clip(dw, min=-max_ratio, max=max_ratio)
dh = paddle.clip(dh, min=-max_ratio, max=max_ratio)
rroi_x = rrois[:, 0]
rroi_y = rrois[:, 1]
rroi_w = rrois[:, 2]
rroi_h = rrois[:, 3]
rroi_angle = rrois[:, 4]
gx = dx * rroi_w * paddle.cos(rroi_angle) - dy * rroi_h * paddle.sin(
rroi_angle) + rroi_x
gy = dx * rroi_w * paddle.sin(rroi_angle) + dy * rroi_h * paddle.cos(
rroi_angle) + rroi_y
gw = rroi_w * dw.exp()
gh = rroi_h * dh.exp()
ga = np.pi * dangle + rroi_angle
ga = (ga + np.pi / 4) % np.pi - np.pi / 4
bboxes = paddle.stack([gx, gy, gw, gh, ga], axis=-1)
return bboxes
def get_sinusoid_encoding(n_position, feat_dim, wave_length=10000):
# [n_position]
positions = paddle.arange(0, n_position)
# [feat_dim]
dim_range = paddle.arange(0, feat_dim)
dim_range = paddle.pow(wave_length, 2 * (dim_range // 2) / feat_dim)
# [n_position, feat_dim]
angles = paddle.unsqueeze(positions, axis=1) / paddle.unsqueeze(dim_range,
axis=0)
angles = paddle.cast(angles, "float32")
angles[:, 0::2] = paddle.sin(angles[:, 0::2])
angles[:, 1::2] = paddle.cos(angles[:, 1::2])
return angles
def positional_embedding(pos_seq, inv_freq, bsz=None):
# Compute sinusoid_inp = einsum4x4("i,d->id", pos_seq, inv_freq)
sinusoid_inp = paddle.matmul(pos_seq.reshape([-1, 1]),
inv_freq.reshape([1, -1]))
pos_emb = paddle.concat(
[paddle.sin(sinusoid_inp),
paddle.cos(sinusoid_inp)], axis=-1)
pos_emb = paddle.unsqueeze(pos_emb, axis=1)
if bsz is not None:
pos_emb = pos_emb.expand([-1, bsz, -1])
pos_emb.stop_gradient = True
pos_emb.stop_gradient = True
return pos_emb
def _test_static(self, place, kwargs):
paddle.enable_static()
best = float("-10000") if kwargs['mode'] == "max" else float("10000")
current_lr = 1.0
cooldown_counter = 0
num_bad_epochs = 0
var_list = [best, current_lr, cooldown_counter, num_bad_epochs]
main_prog = paddle.static.Program()
start_prog = paddle.static.Program()
with paddle.static.program_guard(main_prog, start_prog):
x = fluid.layers.create_global_var([1],
1,
'float32',
persistable=True)
paddle.increment(x)
loss = paddle.sin(x)
scheduler = paddle.optimizer.lr.ReduceOnPlateau(**kwargs)
adam = paddle.optimizer.Adam(learning_rate=scheduler)
adam.minimize(loss)
lr_var = adam._global_learning_rate()
test_prog = main_prog.clone()
exe = paddle.static.Executor(place)
exe.run(start_prog)
for epoch in range(20):
for batch_id in range(1):
out, actual_lr = exe.run(main_prog,
fetch_list=[loss.name, lr_var.name])
expected_lr = reduce_lr_on_plateau(
kwargs['factor'], kwargs['threshold'], kwargs['cooldown'],
kwargs['patience'], kwargs['mode'],
kwargs['threshold_mode'], out[0], var_list)
scheduler.step(out[0])
actual_lr = scheduler()
self.assertEqual(actual_lr, np.array(expected_lr))
for epoch in range(10):
for batch_id in range(1):
out, actual_lr = exe.run(test_prog,
fetch_list=[loss.name, lr_var.name])
expected_lr = reduce_lr_on_plateau(
kwargs['factor'], kwargs['threshold'], kwargs['cooldown'],
kwargs['patience'], kwargs['mode'],
kwargs['threshold_mode'], out[0], var_list)
scheduler.step(out[0])
actual_lr = scheduler()
self.assertEqual(actual_lr, np.array(expected_lr))
def __init__(self, dropout, dim, max_len=5000):
super(PositionalEncoding, self).__init__()
self.dropout = nn.Dropout(p=dropout)
pe = paddle.zeros([max_len, dim])
position = paddle.arange(0, max_len, dtype=paddle.float32).unsqueeze(1)
div_term = paddle.exp(
paddle.arange(0, dim, 2).astype('float32') *
(-math.log(10000.0) / dim))
pe[:, 0::2] = paddle.sin(position * div_term)
pe[:, 1::2] = paddle.cos(position * div_term)
pe = pe.unsqueeze(0)
pe = pe.transpose([1, 0, 2])
self.register_buffer('pe', pe)
def forward(self, pos_seq, bsz=None):
sinusoid_inp = paddle.matmul(
pos_seq.unsqueeze([1]), self.inv_freq.unsqueeze([0]))
pos_emb = paddle.concat(
[paddle.sin(sinusoid_inp), paddle.cos(sinusoid_inp)], axis=-1)
if bsz is not None:
pos_emb = pos_emb.unsqueeze([0]).expand([bsz, -1, -1])
pos_emb.stop_gradient = True
return pos_emb
else:
pos_emb = pos_emb.unsqueeze([0])
pos_emb.stop_gradient = True
return pos_emb
def __init__(self, posistion: int = 60, d_model: int = 30):
super().__init__()
pos_enc = paddle.zeros(shape=[posistion, d_model], dtype='float32')
pos = paddle.arange(start=0, end=posistion,
dtype='float32').unsqueeze(1)
dim = paddle.arange(start=0, end=d_model, step=2, dtype='float32')
div_den = paddle.pow(
paddle.to_tensor(np.array([10000]), dtype='float32'),
-(dim / d_model))
pos_enc[:, 0::2] = paddle.sin(pos * div_den)
pos_enc[:, 1::2] = paddle.cos(pos * div_den)
pos_enc.stop_gradient = True
self.register_buffer('pos_enc', pos_enc)
def forward(self, x):
#TODO:
matrix = paddle.ones([1, 1], dtype=np.float32)
for t in self.thetas:
cs = paddle.cos(t / 2)
sn = paddle.sin(t / 2)
m = paddle.concat([
paddle.concat([cs, -sn], axis=1),
paddle.concat([sn, cs], axis=1),
],
axis=0)
matrix = paddle.kron(matrix, m)
x = paddle.matmul(matrix, x)
return x
def get_score(self, head, rel, tail):
re_head, im_head = paddle.chunk(head, chunks=2, axis=-1)
re_tail, im_tail = paddle.chunk(tail, chunks=2, axis=-1)
phase_rel = rel / (self.emb_init / np.pi)
re_rel, im_rel = paddle.cos(phase_rel), paddle.sin(phase_rel)
re_score = re_rel * re_tail + im_rel * im_tail
im_score = re_rel * im_tail - im_rel * re_tail
re_score = re_score - re_head
im_score = im_score - im_head
score = paddle.stack([re_score, im_score], axis=0)
score = self.gamma - paddle.sum(paddle.norm(score, p=2, axis=0),
axis=-1)
return score
def rotation_2d(points, angles):
"""rotation 2d points based on origin point clockwise when angle positive.
Args:
points (float array, shape=[N, point_size, 2]): points to be rotated.
angles (float array, shape=[N]): rotation angle.
Returns:
float array: same shape as points
"""
rot_sin = paddle.sin(angles)
rot_cos = paddle.cos(angles)
rot_mat_T = paddle.stack(
[paddle.stack([rot_cos, -rot_sin]),
paddle.stack([rot_sin, rot_cos])])
return paddle.einsum('aij,jka->aik', (points, rot_mat_T))
def dft_matrix(n: int,
return_complex: bool = False,
dtype: str = 'float64') -> Tensor:
"""Compute discrete Fourier transform matrix.
Parameters:
n(int): the size of dft matrix.
return_complex(bool): whether to return complex matrix. If True, the matrix will
be complex type. Otherwise, the real and image part will be stored in the last
axis of returned tensor.
dtype(str): the datatype of the returned dft matrix.
Shape:
output: [n, n] or [n,n,2]
Returns:
Complex tensor of shape (n,n) if return_complex=True, and of shape (n,n,2) otherwise.
Examples:
.. code-block:: python
import paddle
import paddleaudio.functional as F
m = F.dft_matrix(512)
print(m.shape)
>> [512, 512, 2]
m = F.dft_matrix(512, return_complex=True)
print(m.shape)
>> [512, 512]
"""
# This is due to a bug in paddle in lacking support for complex128, as of paddle 2.1.0
if return_complex and dtype == 'float64':
raise ValueError('not implemented')
x, y = paddle.meshgrid(paddle.arange(0, n), paddle.arange(0, n))
z = x.astype(dtype) * y.astype(dtype) * paddle.to_tensor(
(-2 * math.pi / n), dtype)
cos = paddle.cos(z)
sin = paddle.sin(z)
if return_complex:
return cos + paddle.to_tensor([1j]) * sin
cos = cos.unsqueeze(-1)
sin = sin.unsqueeze(-1)
return paddle.concat([cos, sin], -1)
def get_timestep_embedding(timesteps, embedding_dim):
"""
This matches the implementation in Denoising Diffusion Probabilistic Models:
From Fairseq.
Build sinusoidal embeddings.
This matches the implementation in tensor2tensor, but differs slightly
from the description in Section 3.5 of "Attention Is All You Need".
"""
assert len(timesteps.shape) == 1
half_dim = embedding_dim // 2
emb = math.log(10000) / (half_dim - 1)
emb = paddle.exp(paddle.arange(half_dim, dtype='float32') * -emb)
emb = timesteps.astype('float32').unsqueeze(1) * emb.unsqueeze(0)
emb = paddle.concat([paddle.sin(emb), paddle.cos(emb)], 1)
if embedding_dim % 2 == 1: # zero pad
emb = paddle.nn.functional.pad(emb, [0, 1, 0, 0])
return emb
def cosine(M: int, sym: bool = True, dtype: str = 'float64') -> Tensor:
"""Compute a window with a simple cosine shape.
Parameters:
M(int): window size.
sym(bool)：whether to return symmetric window.
The default value is True
dtype(str): the datatype of returned tensor.
Returns:
Tensor: the window tensor
Notes:
This function is consistent with scipy.signal.windows.cosine().
"""
if _len_guards(M):
return paddle.ones((M, ), dtype=dtype)
M, needs_trunc = _extend(M, sym)
w = paddle.sin(math.pi / M * (paddle.arange(0, M, dtype=dtype) + .5))
return _truncate(w, needs_trunc)
def _test_dygraph(self, place, kwargs):
paddle.disable_static(place)
best = float("-10000") if kwargs['mode'] == "max" else float("10000")
current_lr = 1.0
cooldown_counter = 0
num_bad_epochs = 0
var_list = [best, current_lr, cooldown_counter, num_bad_epochs]
linear = paddle.nn.Linear(10, 10)
scheduler = paddle.optimizer.lr.ReduceOnPlateau(**kwargs)
adam = paddle.optimizer.Adam(learning_rate=scheduler,
parameters=linear.parameters())
for epoch in range(20):
for batch_id in range(1):
x = paddle.to_tensor(epoch).astype('float32')
loss = paddle.sin(x)
loss.backward()
adam.step()
adam.clear_grad()
scheduler.step(loss)
# get lr from paddle
current_lr = adam.get_lr()
# get lr form python
expected_lr = reduce_lr_on_plateau(
kwargs['factor'], kwargs['threshold'], kwargs['cooldown'],
kwargs['patience'], kwargs['mode'], kwargs['threshold_mode'],
loss, var_list)
self.assertEqual(current_lr, expected_lr)
state_dict = adam.state_dict()
scheduler1 = paddle.optimizer.lr.ReduceOnPlateau(**kwargs)
adam1 = paddle.optimizer.Adam(learning_rate=scheduler1,
parameters=linear.parameters())
adam1.set_state_dict(state_dict)
self.assertEqual(scheduler.cooldown_counter,
scheduler1.cooldown_counter)
self.assertEqual(scheduler.best.numpy()[0], scheduler1.best)
self.assertEqual(scheduler.num_bad_epochs, scheduler1.num_bad_epochs)
self.assertEqual(scheduler.last_epoch, scheduler1.last_epoch)
self.assertEqual(scheduler.last_lr, scheduler1.last_lr)
def test_paddle_param():
U = paddle.to_tensor(
np.array([[1, -1], [1, 1]], dtype=np.float32) / np.sqrt(2))
U.stop_gradient = True
theta = paddle.static.create_parameter(shape=[1, 1], dtype='float32')
cs = paddle.cos(theta / 2)
sn = paddle.sin(theta / 2)
matrix = paddle.concat([
paddle.concat([cs, -sn], axis=1),
paddle.concat([sn, cs], axis=1),
],
axis=0)
loss = 1 - paddle.trace(paddle.matmul(U, paddle.transpose(matrix,
[1, 0]))) / 2
# I = paddle.to_tensor(np.eye(2, dtype=np.float32))
dt = paddle.grad(outputs=[loss],
inputs=[theta],
create_graph=False,
retain_graph=True)[0]
print(dt)
def __init__(self, dropout, dim, max_len=5000):
super(PositionalEncoding_2d, self).__init__()
self.dropout = nn.Dropout(p=dropout)
pe = paddle.zeros([max_len, dim])
position = paddle.arange(0, max_len, dtype=paddle.float32).unsqueeze(1)
div_term = paddle.exp(
paddle.arange(0, dim, 2).astype('float32') *
(-math.log(10000.0) / dim))
pe[:, 0::2] = paddle.sin(position * div_term)
pe[:, 1::2] = paddle.cos(position * div_term)
pe = pe.unsqueeze(0).transpose([1, 0, 2])
self.register_buffer('pe', pe)
self.avg_pool_1 = nn.AdaptiveAvgPool2D((1, 1))
self.linear1 = nn.Linear(dim, dim)
self.linear1.weight.data.fill_(1.)
self.avg_pool_2 = nn.AdaptiveAvgPool2D((1, 1))
self.linear2 = nn.Linear(dim, dim)
self.linear2.weight.data.fill_(1.)
def rzz_gate_matrix(params):
"""
RZZ gate
:return:
"""
theta = params
re_a = paddle.cos(theta / 2)
re_b = paddle.zeros([1], 'float64')
im_a = paddle.sin(theta / 2)
im_b = paddle.zeros([1], 'float64')
re = paddle.reshape(
paddle.concat([
re_a, re_b, re_b, re_b, re_b, re_a, re_b, re_b, re_b, re_b, re_a,
re_b, re_b, re_b, re_b, re_a
]), [4, 4])
im = paddle.reshape(
paddle.concat([
-im_a, im_b, im_b, im_b, im_b, im_a, im_b, im_b, im_b, im_b, im_a,
im_b, im_b, im_b, im_b, -im_a
]), [4, 4])
return re + im * paddle.to_tensor([1j], 'complex128')
def bohman(M: int, sym: bool = True, dtype: str = 'float64') -> Tensor:
"""Compute a Bohman window.
The Bohman window is the autocorrelation of a cosine window.
Parameters:
M(int): window size.
sym(bool)：whether to return symmetric window.
The default value is True
dtype(str): the datatype of returned tensor.
Returns:
Tensor: the window tensor
Notes:
This function is consistent with scipy.signal.windows.bohman().
"""
if _len_guards(M):
return paddle.ones((M, ), dtype=dtype)
M, needs_trunc = _extend(M, sym)
fac = paddle.abs(paddle.linspace(-1, 1, M, dtype=dtype)[1:-1])
w = (1 - fac) * paddle.cos(math.pi * fac) + 1.0 / math.pi * paddle.sin(
math.pi * fac)
w = _cat([0, w, 0], dtype)
return _truncate(w, needs_trunc)
