def phif(s):
pmagsq = np.sum(abarsq / np.square(lambar + s), axis=-1)
pmag = np.sqrt(pmagsq)
phipartial = np.reciprocal(pmag)
singular = np.any(np.equal(-s, lambar), axis=-1)
phipartial = np.where(singular, 0., phipartial)
phi = phipartial - np.reciprocal(trust_radius)
return phi
def minimum_volume_enclosing_ellipsoid(points,
tol,
init_u=None,
return_u=False):
"""
Performs the algorithm of
MINIMUM VOLUME ENCLOSING ELLIPSOIDS
NIMA MOSHTAGH
psuedo-code here:
https://stackoverflow.com/questions/1768197/bounding-ellipse
Args:
points: [N, D]
"""
N, D = points.shape
Q = jnp.concatenate([points, jnp.ones([N, 1])], axis=1) # N,D+1
def body(state):
(count, err, u) = state
V = Q.T @ jnp.diag(u) @ Q # D+1, D+1
# g[i] = Q[i,j].V^-1_jk.Q[i,k]
g = vmap(lambda q: q @ jnp.linalg.solve(V, q))(Q) # difference
# jnp.diag(Q @ jnp.linalg.solve(V, Q.T))
j = jnp.argmax(g)
g_max = g[j]
step_size = \
(g_max - D - 1) / ((D + 1) * (g_max - 1))
search_direction = jnp.where(jnp.arange(N) == j, 1. - u, -u)
new_u = u + step_size * search_direction
# new_u = (1. - step_size)*u
new_u = jnp.where(
jnp.arange(N) == j, u + step_size * (1. - u), u * (1. - step_size))
new_err = jnp.linalg.norm(u - new_u)
return (count + 1, new_err, new_u)
if init_u is None:
init_u = jnp.ones(N) / N
(count, err,
u) = while_loop(lambda state: state[1] > tol * jnp.linalg.norm(init_u),
body, (0, jnp.inf, init_u))
U = jnp.diag(u)
PU = (points.T @ u) # D, N
A = jnp.reciprocal(D) * jnp.linalg.pinv(points.T @ U @ points -
PU[:, None] @ PU[None, :])
c = PU
W, Q, Vh = jnp.linalg.svd(A)
radii = jnp.reciprocal(jnp.sqrt(Q))
rotation = Vh.conj().T
if return_u:
return c, radii, rotation, u
return c, radii, rotation
def init_fn(z, rng, step_size=1.0, inverse_mass_matrix=None, mass_matrix_size=None):
"""
:param z: Initial position of the integrator.
:param jax.random.PRNGKey rng: Random key to be used as the source of randomness.
:param float step_size: Initial step size.
:param inverse_mass_matrix: Inverse of the initial mass matrix. If ``None``,
inverse of mass matrix will be an identity matrix with size is decided
by the argument `mass_matrix_size`.
:param int mass_matrix_size: Size of the mass matrix.
:return: initial state of the adapt scheme.
"""
rng, rng_ss = random.split(rng)
if inverse_mass_matrix is None:
assert mass_matrix_size is not None
if dense_mass:
inverse_mass_matrix = np.identity(mass_matrix_size)
else:
inverse_mass_matrix = np.ones(mass_matrix_size)
mass_matrix_sqrt = inverse_mass_matrix
else:
if dense_mass:
mass_matrix_sqrt = cholesky_inverse(inverse_mass_matrix)
else:
mass_matrix_sqrt = np.sqrt(np.reciprocal(inverse_mass_matrix))
if adapt_step_size:
step_size = find_reasonable_step_size(inverse_mass_matrix, z, rng_ss, step_size)
ss_state = ss_init(np.log(10 * step_size))
mm_state = mm_init(inverse_mass_matrix.shape[-1])
window_idx = 0
return AdaptState(step_size, inverse_mass_matrix, mass_matrix_sqrt,
ss_state, mm_state, window_idx, rng)
def quantized_softmax(a):
# We compute softmax as exp(x-max(x))/sum_i(exp(x_i-max(x))), quantizing
# intermediate values. Note this differs from the log-domain
# implementation of softmax used above.
quant_hparams = softmax_hparams.quant_hparams
fp_quant_config = QuantOps.FloatQuant(is_scaled=False,
fp_spec=quant_hparams.prec)
quant_ops = QuantOps.create_symmetric_fp(fp_quant=fp_quant_config,
bounds=None)
a = quant_ops.to_quantized(a, dtype=dtype)
# Note that the max of a quantized vector is necessarily also quantized to
# the same precision since the max of a vector must be an existing element
# of the vector, so we don't need to explicitly insert a quantization
# operator to the output of the max reduction.
a_max = jnp.max(a, axis=norm_dims, keepdims=True)
a_minus_max = quant_ops.to_quantized(a - a_max, dtype=dtype)
a_exp = quant_ops.to_quantized(jnp.exp(a_minus_max), dtype=dtype)
sum_exp_quantized_reduction = quantization.quantized_sum(
a_exp,
axis=norm_dims,
keepdims=True,
prec=quant_hparams.reduction_prec)
sum_exp = quant_ops.to_quantized(sum_exp_quantized_reduction,
dtype=dtype)
inv_sum_exp = quant_ops.to_quantized(jnp.reciprocal(sum_exp),
dtype=dtype)
a_softmax = quant_ops.to_quantized(a_exp * inv_sum_exp, dtype=dtype)
return a_softmax.astype(dtype)
def test_welford_covariance(jitted, diagonal, regularize):
with optional(jitted,
disable_jit()), optional(jitted,
control_flow_prims_disabled()):
np.random.seed(0)
loc = np.random.randn(3)
a = np.random.randn(3, 3)
target_cov = np.matmul(a, a.T)
x = np.random.multivariate_normal(loc, target_cov, size=(2000, ))
x = device_put(x)
@jit
def get_cov(x):
wc_init, wc_update, wc_final = welford_covariance(
diagonal=diagonal)
wc_state = wc_init(3)
wc_state = fori_loop(0, 2000, lambda i, val: wc_update(x[i], val),
wc_state)
cov, cov_inv_sqrt = wc_final(wc_state, regularize=regularize)
return cov, cov_inv_sqrt
cov, cov_inv_sqrt = get_cov(x)
if diagonal:
diag_cov = jnp.diagonal(target_cov)
assert_allclose(cov, diag_cov, rtol=0.06)
assert_allclose(cov_inv_sqrt,
jnp.sqrt(jnp.reciprocal(diag_cov)),
rtol=0.06)
else:
assert_allclose(cov, target_cov, rtol=0.06)
assert_allclose(cov_inv_sqrt,
jnp.linalg.cholesky(jnp.linalg.inv(cov)),
rtol=0.06)
def final_fn(state, regularize=False):
"""
:param state: Current state of the scheme.
:param bool regularize: Whether to adjust diagonal for numerical stability.
:return: a triple of estimated covariance, the square root of precision, and
the inverse of that square root.
"""
mean, m2, n = state
# XXX it is not necessary to check for the case n=1
cov = m2 / (n - 1)
if regularize:
# Regularization from Stan
scaled_cov = (n / (n + 5)) * cov
shrinkage = 1e-3 * (5 / (n + 5))
if diagonal:
cov = scaled_cov + shrinkage
else:
cov = scaled_cov + shrinkage * jnp.identity(mean.shape[0])
if jnp.ndim(cov) == 2:
# copy the implementation of distributions.util.cholesky_of_inverse here
tril_inv = jnp.swapaxes(
jnp.linalg.cholesky(cov[..., ::-1, ::-1])[..., ::-1, ::-1], -2,
-1)
identity = jnp.identity(cov.shape[-1])
cov_inv_sqrt = solve_triangular(tril_inv, identity, lower=True)
else:
tril_inv = jnp.sqrt(cov)
cov_inv_sqrt = jnp.reciprocal(tril_inv)
return cov, cov_inv_sqrt, tril_inv
def pow_right(y, z, ildj_):
# x ** y = z
# x = f^-1(z) = z ** (1 / y)
# grad(f^-1)(z) = 1 / y * z ** (1 / y - 1)
# log(grad(f^-1)(z)) = (1 / y - 1)log(z) - log(y)
y_inv = np.reciprocal(y)
return lax.pow(z, y_inv), ildj_ + (y_inv - 1.) * np.log(z) - np.log(y)
def _sample_momentum(unpack_fn, inverse_mass_matrix, rng):
if inverse_mass_matrix.ndim == 1:
r = dist.norm(0., np.sqrt(
np.reciprocal(inverse_mass_matrix))).rvs(random_state=rng)
return unpack_fn(r)
elif inverse_mass_matrix.ndim == 2:
raise NotImplementedError
def restricted_mp2(geom, basis_name, xyz_path, nuclear_charges, charge, deriv_order=0):
nelectrons = int(jnp.sum(nuclear_charges)) - charge
ndocc = nelectrons // 2
E_scf, C, eps, G = restricted_hartree_fock(geom, basis_name, xyz_path, nuclear_charges, charge, deriv_order=deriv_order, return_aux_data=True)
nvirt = G.shape[0] - ndocc
nbf = G.shape[0]
G = partial_tei_transformation(G, C[:,:ndocc],C[:,ndocc:],C[:,:ndocc],C[:,ndocc:])
# Create tensor dim (occ,vir,occ,vir) of all possible orbital energy denominators
# Partial tei transformation is super efficient, it is this part that is bad.
eps_occ, eps_vir = eps[:ndocc], eps[ndocc:]
e_denom = jnp.reciprocal(eps_occ.reshape(-1, 1, 1, 1) - eps_vir.reshape(-1, 1, 1) + eps_occ.reshape(-1, 1) - eps_vir)
# Tensor contraction algo
#mp2_correlation = jnp.einsum('iajb,iajb,iajb->', G, G, e_denom) +\
# jnp.einsum('iajb,iajb,iajb->', G - jnp.transpose(G, (0,3,2,1)), G, e_denom)
#mp2_total_energy = mp2_correlation + E_scf
#return E_scf + mp2_correlation
# Loop algo (lower memory, but tei transform is the memory bottleneck)
# Create all combinations of four loop variables to make XLA compilation easier
indices = cartesian_product(jnp.arange(ndocc),jnp.arange(ndocc),jnp.arange(nvirt),jnp.arange(nvirt))
with loops.Scope() as s:
s.mp2_correlation = 0.
for idx in s.range(indices.shape[0]):
i,j,a,b = indices[idx]
s.mp2_correlation += G[i, a, j, b] * (2 * G[i, a, j, b] - G[i, b, j, a]) * e_denom[i,a,j,b]
return E_scf + s.mp2_correlation
def _sample_momentum(unpack_fn, inverse_mass_matrix, rng):
if inverse_mass_matrix.ndim == 1:
r = dist.Normal(0., np.sqrt(
np.reciprocal(inverse_mass_matrix))).sample(rng)
return unpack_fn(r)
elif inverse_mass_matrix.ndim == 2:
raise NotImplementedError
def body(state):
p_k = -(state.H_k @ state.g_k)
line_search_results = line_search(value_and_grad, state.x_k, p_k, old_fval=state.f_k, gfk=state.g_k,
maxiter=ls_maxiter)
state = state._replace(nfev=state.nfev + line_search_results.nfev,
ngev=state.ngev + line_search_results.ngev,
failed=line_search_results.failed,
ls_status=line_search_results.status)
s_k = line_search_results.a_k * p_k
x_kp1 = state.x_k + s_k
f_kp1 = line_search_results.f_k
g_kp1 = line_search_results.g_k
# print(g_kp1)
y_k = g_kp1 - state.g_k
rho_k = jnp.reciprocal(y_k @ s_k)
sy_k = s_k[:, None] * y_k[None, :]
w = jnp.eye(d) - rho_k * sy_k
H_kp1 = jnp.where(jnp.isfinite(rho_k),
jnp.linalg.multi_dot([w, state.H_k, w.T]) + rho_k * s_k[:, None] * s_k[None, :], state.H_k)
converged = jnp.linalg.norm(g_kp1, ord=norm) < gtol
state = state._replace(converged=converged,
k=state.k + 1,
x_k=x_kp1,
f_k=f_kp1,
g_k=g_kp1,
H_k=H_kp1
)
return state
def quantized_layernorm(x):
prec = hparams.quant_hparams.prec
fp_quant = QuantOps.FloatQuant(is_scaled=False, fp_spec=prec)
quant_ops = QuantOps.create_symmetric_fp(fp_quant=fp_quant,
bounds=None)
def to_quantized(x):
return quant_ops.to_quantized(x, dtype=dtype)
# If epsilon is too small to represent in the quantized format, we set it
# to the minimal representative non-zero value to avoid the possibility of
# dividing by zero.
fp_bounds = quantization.fp_cast.get_bounds(
prec.exp_min, prec.exp_max, prec.sig_bits)
epsilon = max(self.epsilon, fp_bounds.flush_to_zero_bound)
quantized_epsilon = to_quantized(jnp.array(epsilon, dtype=dtype))
# If the reciprocal of the quantized number of features is too small to
# represent in the quantized format, we set it to the minimal
# representative nonzero value so that the mean and variance are not
# trivially 0.
num_features_quantized = to_quantized(
jnp.array(num_features, dtype=dtype))
num_features_recip_quantized = to_quantized(
jnp.reciprocal(num_features_quantized))
num_features_recip_quantized = jax.lax.cond(
jax.lax.eq(num_features_recip_quantized,
0.0), lambda _: quantized_epsilon,
lambda _: num_features_recip_quantized, None)
x_quantized = to_quantized(x)
x_sum_quantized_reduction = quantization.quantized_sum(
x_quantized,
axis=-1,
keepdims=True,
prec=hparams.quant_hparams.reduction_prec)
x_sum = to_quantized(x_sum_quantized_reduction)
mean = to_quantized(x_sum * num_features_recip_quantized)
x_minus_mean = to_quantized(x - mean)
x_sq = to_quantized(lax.square(x_minus_mean))
x_sq_sum_quantized_reduction = quantization.quantized_sum(
x_sq,
axis=-1,
keepdims=True,
prec=hparams.quant_hparams.reduction_prec)
x_sq_sum = to_quantized(x_sq_sum_quantized_reduction)
var = to_quantized(x_sq_sum * num_features_recip_quantized)
# Prevent division by zero.
var_plus_epsilon = to_quantized(var + quantized_epsilon)
mul = to_quantized(lax.rsqrt(var_plus_epsilon))
if self.use_scale:
quantized_scale_param = to_quantized(scale_param)
mul = to_quantized(mul * quantized_scale_param)
y = to_quantized(x_minus_mean * mul)
if self.use_bias:
quantized_bias_param = to_quantized(bias_param)
y = to_quantized(y + quantized_bias_param)
return y.astype(self.dtype)
def body_fun(state: LBFGSResults):
# find search direction
p_k = _two_loop_recursion(state)
# line search
ls_results = line_search(
f=fun,
xk=state.x_k,
pk=p_k,
old_fval=state.f_k,
gfk=state.g_k,
maxiter=maxls,
)
# evaluate at next iterate
s_k = ls_results.a_k * p_k
x_kp1 = state.x_k + s_k
f_kp1 = ls_results.f_k
g_kp1 = ls_results.g_k
y_k = g_kp1 - state.g_k
rho_k_inv = jnp.real(_dot(y_k, s_k))
rho_k = jnp.reciprocal(rho_k_inv)
gamma = rho_k_inv / jnp.real(_dot(jnp.conj(y_k), y_k))
# replacements for next iteration
status = 0
status = jnp.where(state.f_k - f_kp1 < ftol, 4, status)
status = jnp.where(state.ngev >= maxgrad, 3, status) # type: ignore
status = jnp.where(state.nfev >= maxfun, 2, status) # type: ignore
status = jnp.where(state.k >= maxiter, 1, status) # type: ignore
status = jnp.where(ls_results.failed, 5, status)
converged = jnp.linalg.norm(g_kp1, ord=norm) < gtol
# TODO(jakevdp): use a fixed-point procedure rather than type-casting?
state = state._replace(
converged=converged,
failed=(status > 0) & (~converged),
k=state.k + 1,
nfev=state.nfev + ls_results.nfev,
ngev=state.ngev + ls_results.ngev,
x_k=x_kp1.astype(state.x_k.dtype),
f_k=f_kp1.astype(state.f_k.dtype),
g_k=g_kp1.astype(state.g_k.dtype),
s_history=_update_history_vectors(history=state.s_history,
new=s_k),
y_history=_update_history_vectors(history=state.y_history,
new=y_k),
rho_history=_update_history_scalars(history=state.rho_history,
new=rho_k),
gamma=gamma,
status=jnp.where(converged, 0, status),
ls_status=ls_results.status,
)
return state
def gaussian_euclidean_metric(
inverse_mass_matrix: np.DeviceArray,
) -> Tuple[Callable, Callable]:
"""Emulate dynamics on an Euclidean Manifold [1]_ for vanilla Hamiltonian
Monte Carlo with a standard gaussian as the conditional probability density
:math:`\\pi(momentum|position)`.
References
----------
.. [1]: Betancourt, Michael. "A general metric for Riemannian manifold
Hamiltonian Monte Carlo." International Conference on Geometric Science of
Information. Springer, Berlin, Heidelberg, 2013.
"""
ndim = np.ndim(inverse_mass_matrix)
shape = np.shape(inverse_mass_matrix)[:1]
if ndim == 1: # diagonal mass matrix
mass_matrix_sqrt = np.sqrt(np.reciprocal(inverse_mass_matrix))
@jax.jit
def momentum_generator(rng_key: jax.random.PRNGKey) -> np.DeviceArray:
std = jax.random.normal(rng_key, shape)
p = np.multiply(std, mass_matrix_sqrt)
return p
@jax.jit
def kinetic_energy(momentum: np.DeviceArray) -> float:
velocity = np.multiply(inverse_mass_matrix, momentum)
return 0.5 * np.dot(velocity, momentum)
return momentum_generator, kinetic_energy
elif ndim == 2:
mass_matrix_sqrt = cholesky_triangular(inverse_mass_matrix)
@jax.jit
def momentum_generator(rng_key: jax.random.PRNGKey) -> np.DeviceArray:
std = jax.random.normal(rng_key, shape)
p = np.dot(std, mass_matrix_sqrt)
return p
@jax.jit
def kinetic_energy(momentum: np.DeviceArray) -> float:
velocity = np.matmul(inverse_mass_matrix, momentum)
return 0.5 * np.dot(velocity, momentum)
return momentum_generator, kinetic_energy
else:
raise ValueError(
"The mass matrix has the wrong number of dimensions: "
+ "expected 1 or 2, got {}.".format(np.ndim(inverse_mass_matrix))
)
def integer_pow_inverse(z, *, y):
"""Inverse for `integer_pow_p` primitive."""
if y == 0:
raise ValueError('Cannot invert raising to a value to the 0-th power.')
elif y == 1:
return z
elif y == -1:
return np.reciprocal(z)
elif y == 2:
return np.sqrt(z)
return lax.pow(z, 1. / y)
def precision_matrix(self):
# We use "Woodbury matrix identity" to take advantage of low rank form::
# inv(W @ W.T + D) = inv(D) - inv(D) @ W @ inv(C) @ W.T @ inv(D)
# where :math:`C` is the capacitance matrix.
Wt_Dinv = (np.swapaxes(self.cov_factor, -1, -2)
/ np.expand_dims(self.cov_diag, axis=-2))
A = solve_triangular(Wt_Dinv, self._capacitance_tril, lower=True)
# TODO: find a better solution to create a diagonal matrix
inverse_cov_diag = np.reciprocal(self.cov_diag)
diag_embed = inverse_cov_diag[..., np.newaxis] * np.identity(self.loc.shape[-1])
return diag_embed - np.matmul(np.swapaxes(A, -1, -2), A)
def scaleSqFromModelParsSingleMu(A, e, M, W, etas, binCenters1, good_idx):
coeffe1 = binCenters1[..., 1]
coeffM1 = binCenters1[..., 0]
#term1 = A[good_idx[0]]-e[good_idx[0]]*coeffe1+M[good_idx[0]]*coeffM1 + W[good_idx[0]]*np.abs(coeffM1)
term1 = (A[good_idx[0]] - 1.) + np.reciprocal(
1 + e[good_idx[0]] *
coeffe1) + M[good_idx[0]] * coeffM1 + W[good_idx[0]] * np.abs(coeffM1)
scaleSq = np.square(1. - term1)
return scaleSq
def kl_divergence(p, q):
# From https://arxiv.org/abs/1605.06197 Formula (12)
a, b = p.concentration1, p.concentration0
alpha, beta = q.concentration1, q.concentration0
b_reciprocal = jnp.reciprocal(b)
a_b = a * b
t1 = (alpha / a - 1) * (jnp.euler_gamma + digamma(b) + b_reciprocal)
t2 = jnp.log(a_b) + betaln(alpha, beta) + (b_reciprocal - 1)
a_ = jnp.expand_dims(a, -1)
b_ = jnp.expand_dims(b, -1)
a_b_ = jnp.expand_dims(a_b, -1)
m = jnp.arange(1, p.KL_KUMARASWAMY_BETA_TAYLOR_ORDER + 1)
t3 = (beta - 1) * b * (jnp.exp(betaln(m / a_, b_)) / (m + a_b_)).sum(-1)
return t1 + t2 + t3
def MSAWeight_PB(msa):
gap_idx = msa.abc.charmap['-']
q = msa.abc.q
ax = msa.ax
(N, L) = ax.shape
## step 1: get counts:
c = np.sum(msa.ax_1hot, axis=0)
# set gap counts to 0
c = index_update(c, index[:, gap_idx], 0)
# get N x L array with count value for corresponding residue in alignment
# first, get N x L "column id" array (convenient for vmap)
# col_id[n,i] = i
col_id = np.int16(np.tensordot(np.ones(N), np.arange(L), axes=0))
# ax_c[n, i] = c[i, ax[n,i]]
ax_c = Get_Henikoff_Counts_Residue(col_id, ax, c)
## step 2: get number of unique characters in each column
r = np.float32(np.sum(np.array(c > 0), axis=1))
# transform r from Lx1 array to NxL array, where r2[n,i] = r[i])
# will allow for easy elementwise operations with ax_c
r2 = np.tensordot(np.ones(N), r, axes=0)
## step 3: get ungapped seq lengths
nongap = np.array(ax != gap_idx)
l = np.float32(np.sum(nongap, axis=1))
## step 4: calculate unnormalized weights
# get array of main terms in Henikoff sum
#wgt_un[n,i] = 1 / (r_[i] * c[i, ax[n,i] ])
wgt_un = np.reciprocal(np.multiply(ax_c, r2))
# set all terms involving gap to zero
wgt_un = np.nan_to_num(np.multiply(wgt_un, nongap))
# sum accoss all positions to get prelim unnormalized weight for each sequence
wgt_un = np.sum(wgt_un, axis=1)
# divide by gapless sequence length
wgt_un = np.divide(wgt_un, l)
# step 4: Normalize sequence wieghts
wgt = (wgt_un * np.float32(N)) / np.sum(wgt_un)
msa.wgt = wgt
return
def sigmaSqFromModelParsSingleMu(a, b, c, d, etas, binCenters1, good_idx):
#compute sigma from physics parameters
pt2 = binCenters1[..., 2]
L2 = binCenters1[..., 3]
#corr = binCenters1[...,4]
invpt2 = binCenters1[..., 4]
sigmaSq = a[good_idx[0]] * L2 + c[good_idx[0]] * pt2 * np.square(L2) + b[
good_idx[0]] * L2 * np.reciprocal(1 + d[good_idx[0]] * invpt2 / L2)
#sigmaSq = a[good_idx[0]]*L2 + c[good_idx[0]]*pt2*np.square(L2) + corr
return sigmaSq
def var_exp(self, freqs, Y_obs, sigma, amp, mu, gamma):
"""
Computes variational expectation
Args:
freqs: [Nf]
Y_obs: [Nf]
sigma: [Nf]
amp: [Nf]
mu: [M]
gamma: [M]
Returns: scalar
"""
f = self._phase_basis(self.freqs) # Nf,M
Nf = freqs.size
Sigma_real = jnp.square(sigma[:Nf])
Sigma_imag = jnp.square(sigma[Nf:])
Yreal = Y_obs[:Nf]
Yimag = Y_obs[Nf:]
a = jnp.reciprocal(Sigma_real)
b = jnp.reciprocal(Sigma_imag)
constant = -Nf * jnp.log(2. * jnp.pi)
logdet = -jnp.sum(jnp.log(sigma))
phi = jnp.dot(f, mu)
theta = jnp.dot(jnp.square(f), jnp.square(gamma))
exp_cos = jnp.exp(-0.5 * theta) * jnp.cos(phi)
exp_sin = jnp.exp(-0.5 * theta) * jnp.sin(phi)
exp_cos2 = 0.5 * (jnp.exp(-2. * theta) * jnp.cos(2. * phi) + 1.)
negtwo_maha = a * (jnp.square(Yreal) - 2. * amp * Yreal * exp_cos) \
+ b * (jnp.square(Yimag) - 2. * amp * Yimag * exp_sin) \
+ ((a - b) * exp_cos2 + b) * jnp.square(amp)
return constant + logdet - 0.5 * jnp.sum(negtwo_maha)
def init_fn(z_info,
rng_key,
step_size=1.0,
inverse_mass_matrix=None,
mass_matrix_size=None):
"""
:param IntegratorState z_info: The initial integrator state.
:param jax.random.PRNGKey rng_key: Random key to be used as the source of randomness.
:param float step_size: Initial step size.
:param inverse_mass_matrix: Inverse of the initial mass matrix. If ``None``,
inverse of mass matrix will be an identity matrix with size is decided
by the argument `mass_matrix_size`.
:param int mass_matrix_size: Size of the mass matrix.
:return: initial state of the adapt scheme.
"""
rng_key, rng_key_ss = random.split(rng_key)
if inverse_mass_matrix is None:
assert mass_matrix_size is not None
if dense_mass:
inverse_mass_matrix = jnp.identity(mass_matrix_size)
else:
inverse_mass_matrix = jnp.ones(mass_matrix_size)
mass_matrix_sqrt = mass_matrix_sqrt_inv = inverse_mass_matrix
else:
if dense_mass:
mass_matrix_sqrt_inv = jnp.swapaxes(
jnp.linalg.cholesky(
inverse_mass_matrix[..., ::-1, ::-1])[..., ::-1, ::-1],
-2, -1)
identity = jnp.identity(inverse_mass_matrix.shape[-1])
mass_matrix_sqrt = solve_triangular(mass_matrix_sqrt_inv,
identity,
lower=True)
else:
mass_matrix_sqrt_inv = jnp.sqrt(inverse_mass_matrix)
mass_matrix_sqrt = jnp.reciprocal(mass_matrix_sqrt_inv)
if adapt_step_size:
step_size = find_reasonable_step_size(step_size,
inverse_mass_matrix, z_info,
rng_key_ss)
ss_state = ss_init(jnp.log(10 * step_size))
mm_state = mm_init(inverse_mass_matrix.shape[-1])
window_idx = 0
return HMCAdaptState(step_size, inverse_mass_matrix, mass_matrix_sqrt,
mass_matrix_sqrt_inv, ss_state, mm_state,
window_idx, rng_key)
def unquantized_layernorm(x):
num_features_recip = jnp.reciprocal(num_features)
x_sum = jnp.sum(x, axis=-1, keepdims=True)
mean = x_sum * num_features_recip
x_minus_mean = x - mean
x_sq = lax.square(x_minus_mean)
x_sq_sum = jnp.sum(x_sq, axis=-1, keepdims=True)
var = x_sq_sum * num_features_recip
var_plus_epsilon = var + self.epsilon
mul = lax.rsqrt(var_plus_epsilon)
if self.use_scale:
mul = mul * scale_param
y = x_minus_mean * mul
if self.use_bias:
y = y + bias_param
return y.astype(self.dtype)
def body(state):
(i, _, key, done, _) = state
key, accept_key, sample_key, select_key = random.split(key, 4)
k = random.categorical(select_key, log_p)
mu_k = mu[k, :]
radii_k = radii[k, :]
rotation_k = rotation[k, :, :]
u_test = sample_ellipsoid(sample_key,
mu_k,
radii_k,
rotation_k,
unit_cube_constraint=unit_cube_constraint)
inside = vmap(lambda mu, radii, rotation: point_in_ellipsoid(
u_test, mu, radii, rotation))(mu, radii, rotation)
n_intersect = jnp.sum(inside)
done = (random.uniform(accept_key) < jnp.reciprocal(n_intersect))
return (i + 1, k, key, done, u_test)
def ellipsoid_params(C):
"""
If C satisfies the sectional inequality,
(x - mu)^T C (x - mu) <= 1
then this returns the radius and rotation matrix of the ellipsoid.
Args:
C: [D,D]
Returns: radii [D] rotation [D,D]
"""
W, Q, Vh = jnp.linalg.svd(C)
radii = jnp.reciprocal(jnp.sqrt(Q))
radii = jnp.where(jnp.isnan(radii), 0., radii)
rotation = Vh.conj().T
return radii, rotation
def debug_mvee():
import pylab as plt
n = random.normal(random.PRNGKey(0), (10000,2))
n = n /jnp.linalg.norm(n, axis=1, keepdims=True)
angle = jnp.arctan2(n[:,1], n[:,0])
plt.hist(angle, bins=100)
plt.show()
N = 120
D = 2
points = random.uniform(random.PRNGKey(0), (N, D))
from jax import disable_jit
with disable_jit():
center, radii, rotation = minimum_volume_enclosing_ellipsoid(points, 0.01)
plt.hist(jnp.linalg.norm((rotation.T @ (points.T - center[:, None])) / radii[:, None], axis=0))
plt.show()
print(center, radii, rotation)
plt.scatter(points[:, 0], points[:, 1])
theta = jnp.linspace(0., jnp.pi*2, 100)
ellipsis = center[:, None] + rotation @ jnp.stack([radii[0]*jnp.cos(theta), radii[1]*jnp.sin(theta)], axis=0)
plt.plot(ellipsis[0,:], ellipsis[1,:])
for i in range(1000):
y = sample_ellipsoid(random.PRNGKey(i), center, radii, rotation)
plt.scatter(y[0], y[1])
C = jnp.linalg.pinv(jnp.cov(points, rowvar=False, bias=True))
p = (N - D - 1)/N
def q(p):
return p + p**2/(4.*(D-1))
C = C / q(p)
c = jnp.mean(points, axis=0)
W, Q, Vh = jnp.linalg.svd(C)
radii = jnp.reciprocal(jnp.sqrt(Q))
rotation = Vh.conj().T
ellipsis = c[:, None] + rotation @ jnp.stack([radii[0] * jnp.cos(theta), radii[1] * jnp.sin(theta)], axis=0)
plt.plot(ellipsis[0, :], ellipsis[1, :])
plt.show()
def body_fun(state):
p_k = -_dot(state.H_k, state.g_k)
line_search_results = line_search(
fun,
state.x_k,
p_k,
old_fval=state.f_k,
old_old_fval=state.old_old_fval,
gfk=state.g_k,
maxiter=line_search_maxiter,
)
state = state._replace(
nfev=state.nfev + line_search_results.nfev,
ngev=state.ngev + line_search_results.ngev,
failed=line_search_results.failed,
line_search_status=line_search_results.status,
)
s_k = line_search_results.a_k * p_k
x_kp1 = state.x_k + s_k
f_kp1 = line_search_results.f_k
g_kp1 = line_search_results.g_k
y_k = g_kp1 - state.g_k
rho_k = jnp.reciprocal(_dot(y_k, s_k))
sy_k = s_k[:, jnp.newaxis] * y_k[jnp.newaxis, :]
w = jnp.eye(d, dtype=rho_k.dtype) - rho_k * sy_k
H_kp1 = (_einsum('ij,jk,lk', w, state.H_k, w)
+ rho_k * s_k[:, jnp.newaxis] * s_k[jnp.newaxis, :])
H_kp1 = jnp.where(jnp.isfinite(rho_k), H_kp1, state.H_k)
converged = jnp.linalg.norm(g_kp1, ord=norm) < gtol
state = state._replace(
converged=converged,
k=state.k + 1,
x_k=x_kp1,
f_k=f_kp1,
g_k=g_kp1,
H_k=H_kp1,
old_old_fval=state.f_k,
)
return state
def final_fn(state, regularize=False):
"""
:param state: Current state of the scheme.
:param bool regularize: Whether to adjust diagonal for numerical stability.
:return: a pair of estimated covariance and the square root of precision.
"""
mean, m2, n = state
# XXX it is not necessary to check for the case n=1
cov = m2 / (n - 1)
if regularize:
# Regularization from Stan
scaled_cov = (n / (n + 5)) * cov
shrinkage = 1e-3 * (5 / (n + 5))
if diagonal:
cov = scaled_cov + shrinkage
else:
cov = scaled_cov + shrinkage * np.identity(mean.shape[0])
if np.ndim(cov) == 2:
cov_inv_sqrt = cholesky_inverse(cov)
else:
cov_inv_sqrt = np.sqrt(np.reciprocal(cov))
return cov, cov_inv_sqrt
def sample_ellipsoid(key, center, radii, rotation, unit_cube_constraint=False):
"""
Sample uniformly inside an ellipsoid.
When unit_cube_constraint=True then during the sampling when a random radius is chosen, the radius is constrained.
u(t) = R @ (t * n) + c
u(t) == 1
1-c = t * R@n
t = (1 - c)/R@n take minimum t satisfying this
likewise for zero intersection
Args:
key:
center: [D]
radii: [D]
rotation: [D,D]
Returns: [D]
"""
direction_key, radii_key = random.split(key, 2)
direction = random.normal(direction_key, shape=radii.shape)
if unit_cube_constraint:
direction = direction / jnp.linalg.norm(direction)
R = rotation * radii
D = R @ direction
t0 = -center / D
t1 = jnp.reciprocal(D) + t0
t0 = jnp.where(t0 < 0., jnp.inf, t0)
t1 = jnp.where(t1 < 0., jnp.inf, t1)
t = jnp.minimum(jnp.min(t0), jnp.min(t1))
t = jnp.minimum(t, 1.)
return jnp.exp(
jnp.log(random.uniform(radii_key, minval=0., maxval=t)) /
radii.size) * D + center
log_norm = jnp.log(jnp.linalg.norm(direction))
log_radius = jnp.log(random.uniform(radii_key)) / radii.size
# x = direction * (radius/norm)
x = direction * jnp.exp(log_radius - log_norm)
return circle_to_ellipsoid(x, center, radii, rotation)
def body(state):
(key, i, u_test, x_test, log_L_test) = state
key, uniform_key, beta_key = random.split(key, 3)
# [M]
U_scale = random.uniform(uniform_key,
shape=spawn_point_U.shape,
minval=t_L,
maxval=t_R)
t_shrink = random.beta(beta_key, live_points_U.shape[0],
1)**jnp.reciprocal(spawn_point_U.size)
u_test_white = U_scale / t_shrink
# y_j =
# = dx + sum_i p_i * u_i
# = dx + R @ u
# x_i = x0_i + R_ij u_j
if whiten:
u_test = L @ (spawn_point_U + R @ u_test_white) + u_mean
else:
u_test = u_test_white
u_test = jnp.clip(u_test, 0., 1.)
x_test = prior_transform(u_test)
log_L_test = loglikelihood_from_constrained(**x_test)
return (key, i + 1, u_test, x_test, log_L_test)
