Last updated: 2026-07-30
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| File | Version | Author | Date | Message |
|---|---|---|---|---|
| Rmd | 4276a57 | Matthew Stephens | 2026-07-30 | Explain objective mismatch between asymmetric and log-cosh for symmetric source |
| html | 4276a57 | Matthew Stephens | 2026-07-30 | Explain objective mismatch between asymmetric and log-cosh for symmetric source |
| Rmd | b8658c2 | Matthew Stephens | 2026-07-29 | Add sorted-objective plots for all examples; fix Gaussian baseline text |
| html | b8658c2 | Matthew Stephens | 2026-07-29 | Add sorted-objective plots for all examples; fix Gaussian baseline text |
| Rmd | 636f7d0 | Matthew Stephens | 2026-07-29 | Add sorted-objective plots to assess objective as a source-selection criterion |
| html | 636f7d0 | Matthew Stephens | 2026-07-29 | Add sorted-objective plots to assess objective as a source-selection criterion |
| Rmd | a875fd7 | Matthew Stephens | 2026-07-29 | Clarify log-cosh local-minimum interpretation for p=0.1 nine-groups case |
| html | a875fd7 | Matthew Stephens | 2026-07-29 | Clarify log-cosh local-minimum interpretation for p=0.1 nine-groups case |
| Rmd | 43a0155 | Matthew Stephens | 2026-07-29 | Add p=0.1 to 9-groups and p=0.2 to single-source k=20 tests |
| html | 43a0155 | Matthew Stephens | 2026-07-29 | Add p=0.1 to 9-groups and p=0.2 to single-source k=20 tests |
| Rmd | 9878c1e | Matthew Stephens | 2026-07-29 | Add log-cosh trace Hessian comparison across all tests |
| html | 9878c1e | Matthew Stephens | 2026-07-29 | Add log-cosh trace Hessian comparison across all tests |
| Rmd | 2f935c7 | Matthew Stephens | 2026-07-29 | Match k=20 p=0.5 simulation exactly to ebproj_newton (set.seed(10), n=200, p=1000) |
| html | 2f935c7 | Matthew Stephens | 2026-07-29 | Match k=20 p=0.5 simulation exactly to ebproj_newton (set.seed(10), n=200, p=1000) |
| Rmd | 5df95fa | Matthew Stephens | 2026-07-29 | Add single-source k=20 tests (p=0.5 and p=0.1) |
| html | 5df95fa | Matthew Stephens | 2026-07-29 | Add single-source k=20 tests (p=0.5 and p=0.1) |
| Rmd | 7686e79 | Matthew Stephens | 2026-07-29 | Add trace Hessian approximation to asymmetric fastICA |
| html | 7686e79 | Matthew Stephens | 2026-07-29 | Add trace Hessian approximation to asymmetric fastICA |
| Rmd | f421e5c | Matthew Stephens | 2026-07-29 | Add warm-start comparison to 9-groups test |
| html | f421e5c | Matthew Stephens | 2026-07-29 | Add warm-start comparison to 9-groups test |
| Rmd | d03ae26 | Matthew Stephens | 2026-07-29 | Add warm-start comparison for symmetric sources |
| html | d03ae26 | Matthew Stephens | 2026-07-29 | Add warm-start comparison for symmetric sources |
| Rmd | 008f9d4 | Matthew Stephens | 2026-07-29 | Add EB fastICA with asymmetric prior |
| html | 008f9d4 | Matthew Stephens | 2026-07-29 | Add EB fastICA with asymmetric prior |
Standard fastICA maximizes the log-cosh contrast function, which is equivalent to assuming a symmetric binary (Rademacher) prior on the independent components. For sparse or skewed sources (e.g. indicator variables where the “on” fraction \(p \ll 0.5\)), the expected log-cosh contrast falls below the Gaussian baseline, causing fastICA to actively avoid the true source direction.
This analysis generalizes the framework to an asymmetric Rademacher prior parameterized by its up-probability \(p\). We alternate between:
At \(p = 0.5\) the algorithm exactly reduces to standard log-cosh fastICA. Two scale anchors are compared:
prewhiten = function(X, n.comp) {
X = X - rowMeans(X)
sqrt(ncol(X)) * t(svd(X)$v[, 1:n.comp])
}
With \(\sigma^2 = cs\), the score function and its derivative are:
\[M(x) = \frac{y_1}{cs}\,\pi(x) + \frac{y_0}{cs}\,(1-\pi(x)), \qquad M'(x) = \frac{\pi(x)(1-\pi(x))}{s^2\,p(1-p)}\]
where \(\pi(x) = \sigma(\Delta(x))\) is the logistic sigmoid of
\[\Delta(x) = \frac{1}{\sqrt{p(1-p)}}\!\left(\frac{x}{s} - \frac{c\,(1-2p)}{2s\,\sqrt{p(1-p)}}\right) + \log\frac{p}{1-p}\]
and \(y_1 = c\sqrt{(1-p)/p} > 0\), \(y_0 = -c\sqrt{p/(1-p)} < 0\) are the prior support points.
asym_score = function(x, p, c, s) {
y1 = c * sqrt((1-p)/p)
y0 = -c * sqrt(p/(1-p))
kappa3 = (1 - 2*p) / sqrt(p*(1-p))
Delta = (x/s - c*kappa3/(2*s)) / sqrt(p*(1-p)) + log(p/(1-p))
pi_x = plogis(Delta)
list(
M = (y1/(c*s)) * pi_x + (y0/(c*s)) * (1 - pi_x),
Mp = pi_x * (1 - pi_x) / (s^2 * p * (1-p))
)
}
The marginal log-likelihood in \(p\) for fixed projections \(x = Yw\):
\[J(p) = \frac{1}{n}\sum_{i=1}^n \log\!\left( p\,e^{\,x_i y_1/(cs)\,-\,y_1^2/(2cs)} + (1-p)\,e^{\,x_i y_0/(cs)\,-\,y_0^2/(2cs)}\right)\]
asym_obj_p = function(p, x, c, s) {
y1 = c * sqrt((1-p)/p)
y0 = -c * sqrt(p/(1-p))
a1 = x * y1/(c*s) - y1^2/(2*c*s)
a0 = x * y0/(c*s) - y0^2/(2*c*s)
lp = log(p); l1p = log(1-p)
m = pmax(lp + a1, l1p + a0)
mean(m + log(exp(lp + a1 - m) + exp(l1p + a0 - m)))
}
Two diagonal Hessian approximations are supported, following the notation in ebproj_newton:
Both reduce to the same Newton fixed-point update structure: \[w \leftarrow \tfrac{1}{n}Y M(x) - \tilde H\,w, \qquad w \leftarrow w / \|w\|\]
fastica_asym_r1 = function(Y, s = 1, anchor = c("M", "golden"),
hess = c("fastICA", "trace"),
tol = 1e-6, max_iter = 500, eps = 0.01,
w_init = NULL) {
anchor = match.arg(anchor)
hess = match.arg(hess)
c = if (anchor == "M") s else s * (sqrt(5)-1)/2
m = nrow(Y); n = ncol(Y)
S_diag = colSums(Y^2) / n # S_ii = ||Y[:,i]||^2 / n (sum = m)
w = if (is.null(w_init)) rnorm(m) else w_init
w = w / sqrt(sum(w^2))
p = 0.5
for (iter in seq_len(max_iter)) {
w_old = w; p_old = p
x = as.vector(t(Y) %*% w)
sc = asym_score(x, p, c, s)
h = if (hess == "trace") sum(sc$Mp * S_diag) / m else mean(sc$Mp)
w = as.vector(Y %*% sc$M) / n - h * w
w = w / sqrt(sum(w^2))
x = as.vector(t(Y) %*% w)
opt = optimize(\(pp) asym_obj_p(pp, x, c, s), c(eps, 1-eps), maximum = TRUE)
p = opt$maximum
if (1 - abs(sum(w * w_old)) < tol && abs(p - p_old) < tol) break
}
list(w = w, p = p, iter = iter, c = c)
}
Standard log-cosh fastICA for comparison:
fastica_r1update = function(X, w) {
w = w / sqrt(sum(w^2))
P = t(X) %*% w
G = tanh(P); G2 = 1 - tanh(P)^2
w = X %*% G - mean(G2) * ncol(X) * w
w / sqrt(sum(w^2))
}
fastica_r1update_trace = function(X, w, S_diag) {
w = w / sqrt(sum(w^2))
P = t(X) %*% w
G = tanh(P); G2 = 1 - tanh(P)^2
h = sum(G2 * S_diag) / nrow(X) # trace Hessian: Σ G2_i S_ii / k
w = as.vector(X %*% G) / ncol(X) - h * w
w / sqrt(sum(w^2))
}
run_seeds_lc = function(Y, S_true, hess = "fastICA", n_seeds = 100, n_iter = 200) {
maxcor = numeric(n_seeds)
objs = numeric(n_seeds)
S_diag = colSums(Y^2) / ncol(Y)
for (seed in seq_len(n_seeds)) {
set.seed(seed)
w = rnorm(nrow(Y))
if (hess == "trace") {
for (i in seq_len(n_iter)) w = fastica_r1update_trace(Y, w, S_diag)
} else {
for (i in seq_len(n_iter)) w = fastica_r1update(Y, w)
}
maxcor[seed] = max(abs(cor(t(S_true), t(Y) %*% w)))
objs[seed] = mean(log(cosh(as.vector(t(Y) %*% w))))
}
structure(maxcor, obj = objs) # vector; objs accessible via attr(., "obj")
}
run_seeds_asym = function(Y, S_true, anchor, hess = "fastICA", n_seeds = 100) {
maxcor = numeric(n_seeds); ps = numeric(n_seeds); objs = numeric(n_seeds)
for (seed in seq_len(n_seeds)) {
set.seed(seed)
res = fastica_asym_r1(Y, anchor = anchor, hess = hess, w_init = rnorm(nrow(Y)))
maxcor[seed] = max(abs(cor(t(S_true), t(Y) %*% res$w)))
ps[seed] = min(res$p, 1 - res$p)
objs[seed] = asym_obj_p(res$p, as.vector(t(Y) %*% res$w), res$c, 1)
}
list(maxcor = maxcor, p = ps, obj = objs)
}
# Warm-start variant: run log-cosh to convergence, then hand off to asymmetric
run_seeds_asym_warm = function(Y, S_true, anchor, hess = "fastICA", n_seeds = 100,
n_iter_lc = 200) {
maxcor = numeric(n_seeds); ps = numeric(n_seeds); objs = numeric(n_seeds)
for (seed in seq_len(n_seeds)) {
set.seed(seed)
w = rnorm(nrow(Y))
for (i in seq_len(n_iter_lc)) w = fastica_r1update(Y, w)
res = fastica_asym_r1(Y, anchor = anchor, hess = hess, w_init = w)
maxcor[seed] = max(abs(cor(t(S_true), t(Y) %*% res$w)))
ps[seed] = min(res$p, 1 - res$p)
objs[seed] = asym_obj_p(res$p, as.vector(t(Y) %*% res$w), res$c, 1)
}
list(maxcor = maxcor, p = ps, obj = objs)
}
# Sort by |obj − Gaussian baseline| (most extreme first), colour by success
plot_obj_lc = function(lc_result, title, lc_gauss) {
objs = attr(lc_result, "obj")
succ = lc_result > 0.9
ord = order(abs(objs - lc_gauss), decreasing = TRUE)
cols = ifelse(succ[ord], "steelblue", "tomato")
plot(seq_along(objs), objs[ord],
pch = 19, cex = 0.7, col = cols,
xlab = "rank (1 = most extreme log-cosh)",
ylab = "log-cosh objective",
main = paste0(title, "\n(blue = found true source, red = not)"))
abline(h = lc_gauss, lty = 2, col = "grey50")
legend("topright", c("true source", "other", "Gaussian baseline"),
pch = c(19, 19, NA), lty = c(NA, NA, 2),
col = c("steelblue", "tomato", "grey50"), bty = "n", cex = 0.8)
}
plot_obj_asym = function(asym_result, title) {
objs = asym_result$obj
succ = asym_result$maxcor > 0.9
ord = order(objs, decreasing = TRUE)
cols = ifelse(succ[ord], "steelblue", "tomato")
plot(seq_along(objs), objs[ord],
pch = 19, cex = 0.7, col = cols,
xlab = "rank (1 = highest asymmetric objective)",
ylab = "asymmetric log-likelihood",
main = paste0(title, "\n(blue = found true source, red = not)"))
legend("topright", c("true source", "other"),
pch = 19, col = c("steelblue", "tomato"), bty = "n", cex = 0.8)
}
At \(p = 0.5\), \(s = 1\): \(\Delta(x) = 2x\), \(\pi(x) = (1 + \tanh x)/2\), and \(M(x) = \tanh(x)\) — the standard fastICA score.
x_grid = seq(-3, 3, length.out = 300)
sc05 = asym_score(x_grid, p = 0.5, c = 1, s = 1)
plot(x_grid, sc05$M, type = "l", col = "steelblue", lwd = 2,
xlab = "x", ylab = "M(x)",
main = "Score function at p = 0.5 vs tanh(x)")
lines(x_grid, tanh(x_grid), col = "tomato", lty = 2, lwd = 2)
legend("topleft", c("asymmetric M(x), p = 0.5", "tanh(x)"),
col = c("steelblue", "tomato"), lty = c(1, 2), lwd = 2, bty = "n")

The curves are numerically identical.
When does log-cosh fail? For a standardised binary source \((\text{Bernoulli}(p)\), zero mean, unit variance), the expected log-cosh contrast is:
expected_logcosh = function(p) {
z1 = sqrt((1-p)/p); z0 = -sqrt(p/(1-p))
p * log(cosh(z1)) + (1-p) * log(cosh(z0))
}
lc_stable = function(z) abs(z) + log1p(exp(-2*abs(z))) - log(2)
lc_gauss = integrate(\(z) lc_stable(z) * dnorm(z), -Inf, Inf)$value
pvec = seq(0.01, 0.99, by = 0.01)
lc = sapply(pvec, expected_logcosh)
plot(pvec, lc, type = "l", col = "steelblue", lwd = 2,
xlab = "p (probability of positive state)",
ylab = "E[log cosh(x)]",
main = "Log-cosh contrast vs Gaussian baseline")
abline(h = lc_gauss, lty = 2, col = "grey40")
legend("top", c("E[log cosh], binary source", "Gaussian baseline"),
col = c("steelblue", "grey40"), lty = c(1, 2), lwd = 2, bty = "n")

Standard fastICA with log-cosh actively avoids sources with $p < $ about \(0.25\) or \(p > 0.75\): the contrast falls below the Gaussian baseline, so the global maximum of \(E[\log\cosh]\) on the sphere is not at the true source. However, the true source direction can still be a local minimum, and the fixed-point iteration can converge there — especially when \(p\) is small enough to create a deep, distinctive basin (see the \(p=0.1\) nine-groups result below).
Unlike log-cosh, the asymmetric objective can be evaluated at the optimal test \(p\) matching the true source, placing it above the Gaussian baseline.
set.seed(42)
n_pop = 100000
c_gr = (sqrt(5) - 1) / 2 # golden-ratio anchor
z_02 = ifelse(runif(n_pop) < 0.2, sqrt(0.8/0.2), -sqrt(0.2/0.8))
z_N = rnorm(n_pop)
p_grid = seq(0.02, 0.98, by = 0.01)
obj_asym_02 = sapply(p_grid, \(p) asym_obj_p(p, z_02, c_gr, 1))
obj_asym_N = sapply(p_grid, \(p) asym_obj_p(p, z_N, c_gr, 1))
plot(p_grid, obj_asym_02, type = "l", col = "steelblue", lwd = 2,
xlab = "test p (optimization variable)",
ylab = "E[asymmetric log-likelihood]",
main = "Asymmetric objective: source p_true = 0.2 (golden-ratio anchor)")
lines(p_grid, obj_asym_N, col = "grey40", lty = 2, lwd = 2)
abline(v = 0.2, lty = 3, col = "tomato", lwd = 1.5)
legend("topright",
c("source (p_true = 0.2)", "Gaussian source (varying p_test)", "p = 0.2"),
col = c("steelblue", "grey40", "tomato"),
lty = c(1, 2, 3), lwd = c(2, 2, 1.5), bty = "n")

The grey dashed curve shows the same asymmetric objective evaluated on a Gaussian source as \(p_\text{test}\) varies — it serves as a reference, not a constant horizontal baseline. The blue curve (true \(p = 0.2\) source) peaks near \(p_\text{test} = 0.2\) and lies above the Gaussian reference curve in that region — the optimizer can successfully identify the source by maximising over \(p\). At \(p_\text{test} = 0.5\) the asymmetric objective reduces to the log-cosh contrast, and the blue curve dips below the grey reference, explaining why standard fastICA fails for this source.
As \(p\) decreases below 0.5 the score shifts and steepens, penalising the positive tail more heavily — appropriate for sources that are rarely “on”.
pvec2 = c(0.05, 0.1, 0.2, 0.3, 0.5)
cols = c("purple", "tomato", "darkorange", "steelblue", "black")
plot(NULL, xlim = c(-3, 3), ylim = c(-2.5, 2.5),
xlab = "x", ylab = "M(x)",
main = "Asymmetric score functions (c = s = 1)")
for (i in seq_along(pvec2))
lines(x_grid, asym_score(x_grid, pvec2[i], 1, 1)$M, col = cols[i], lwd = 2)
legend("topleft", paste0("p = ", pvec2), col = cols, lwd = 2, bty = "n")
abline(h = 0, lty = 3, col = "grey60")

Nine sparse binary sources, each active in some fraction of 100 samples, whitened to \(k = 9\).
set.seed(1)
n = 100; p_dim = 1000; K = 9
L = matrix(0, nrow = n, ncol = K)
for (i in 1:K) L[sample(n, 20), i] = 1
FF = matrix(rnorm(p_dim * K), nrow = p_dim)
X9 = t(L %*% t(FF) + matrix(rnorm(n * p_dim, 0, 0.1), nrow = n))
Z9 = prewhiten(X9, K)
S9 = t(L)
mc9_lc = run_seeds_lc(Z9, S9, hess = "fastICA", n_seeds = 100)
mc9_lc_tr = run_seeds_lc(Z9, S9, hess = "trace", n_seeds = 100)
mc9_M = run_seeds_asym(Z9, S9, "M", hess = "fastICA", n_seeds = 100)
mc9_gr = run_seeds_asym(Z9, S9, "golden", hess = "fastICA", n_seeds = 100)
mc9_gr_tr = run_seeds_asym(Z9, S9, "golden", hess = "trace", n_seeds = 100)
mc9_grw = run_seeds_asym_warm(Z9, S9, "golden", hess = "fastICA", n_seeds = 100)
mc9_grw_tr = run_seeds_asym_warm(Z9, S9, "golden", hess = "trace", n_seeds = 100)
cat("9-groups (p ~ 0.2, k = 9, n_seeds = 100):\n")
9-groups (p ~ 0.2, k = 9, n_seeds = 100):
cat(sprintf(" log-cosh (fastICA) mean = %.3f frac > 0.9 = %.2f\n",
mean(mc9_lc), mean(mc9_lc > 0.9)))
log-cosh (fastICA) mean = 0.590 frac > 0.9 = 0.00
cat(sprintf(" log-cosh (trace) mean = %.3f frac > 0.9 = %.2f\n",
mean(mc9_lc_tr), mean(mc9_lc_tr > 0.9)))
log-cosh (trace) mean = 0.588 frac > 0.9 = 0.00
cat(sprintf(" asym M-est (random, fastICA) mean = %.3f frac > 0.9 = %.2f mean_p = %.3f\n",
mean(mc9_M$maxcor), mean(mc9_M$maxcor > 0.9), mean(mc9_M$p)))
asym M-est (random, fastICA) mean = 0.877 frac > 0.9 = 0.68 mean_p = 0.162
cat(sprintf(" asym golden (random, fastICA) mean = %.3f frac > 0.9 = %.2f mean_p = %.3f\n",
mean(mc9_gr$maxcor), mean(mc9_gr$maxcor > 0.9), mean(mc9_gr$p)))
asym golden (random, fastICA) mean = 0.983 frac > 0.9 = 0.95 mean_p = 0.135
cat(sprintf(" asym golden (random, trace) mean = %.3f frac > 0.9 = %.2f mean_p = %.3f\n",
mean(mc9_gr_tr$maxcor), mean(mc9_gr_tr$maxcor > 0.9), mean(mc9_gr_tr$p)))
asym golden (random, trace) mean = 0.974 frac > 0.9 = 0.93 mean_p = 0.142
cat(sprintf(" asym golden (warm, fastICA) mean = %.3f frac > 0.9 = %.2f mean_p = %.3f\n",
mean(mc9_grw$maxcor), mean(mc9_grw$maxcor > 0.9), mean(mc9_grw$p)))
asym golden (warm, fastICA) mean = 0.876 frac > 0.9 = 0.65 mean_p = 0.179
cat(sprintf(" asym golden (warm, trace) mean = %.3f frac > 0.9 = %.2f mean_p = %.3f\n",
mean(mc9_grw_tr$maxcor), mean(mc9_grw_tr$maxcor > 0.9), mean(mc9_grw_tr$p)))
asym golden (warm, trace) mean = 0.879 frac > 0.9 = 0.66 mean_p = 0.180
Sorting runs by their objective reveals whether the objective alone can select true sources — making the raw success rate less critical:
par(mfrow = c(1, 2))
plot_obj_lc(mc9_lc, "log-cosh, 9-groups p≈0.2", lc_gauss)
plot_obj_asym(mc9_gr, "asymmetric, 9-groups p≈0.2")

par(mfrow = c(1, 1))
set.seed(2)
L_01 = matrix(0, nrow = n, ncol = K)
for (i in 1:K) L_01[sample(n, 10), i] = 1
FF_01 = matrix(rnorm(p_dim * K), nrow = p_dim)
X9_01 = t(L_01 %*% t(FF_01) + matrix(rnorm(n * p_dim, 0, 0.1), nrow = n))
Z9_01 = prewhiten(X9_01, K)
S9_01 = t(L_01)
mc9_01_lc = run_seeds_lc(Z9_01, S9_01, hess = "fastICA", n_seeds = 100)
mc9_01_lc_tr = run_seeds_lc(Z9_01, S9_01, hess = "trace", n_seeds = 100)
mc9_01_gr = run_seeds_asym(Z9_01, S9_01, "golden", hess = "fastICA", n_seeds = 100)
mc9_01_gr_tr = run_seeds_asym(Z9_01, S9_01, "golden", hess = "trace", n_seeds = 100)
mc9_01_grw = run_seeds_asym_warm(Z9_01, S9_01, "golden", hess = "fastICA", n_seeds = 100)
mc9_01_grw_tr = run_seeds_asym_warm(Z9_01, S9_01, "golden", hess = "trace", n_seeds = 100)
cat("9-groups (p ~ 0.1, k = 9, n_seeds = 100):\n")
9-groups (p ~ 0.1, k = 9, n_seeds = 100):
cat(sprintf(" log-cosh (fastICA) mean = %.3f frac > 0.9 = %.2f\n",
mean(mc9_01_lc), mean(mc9_01_lc > 0.9)))
log-cosh (fastICA) mean = 0.937 frac > 0.9 = 0.82
cat(sprintf(" log-cosh (trace) mean = %.3f frac > 0.9 = %.2f\n",
mean(mc9_01_lc_tr), mean(mc9_01_lc_tr > 0.9)))
log-cosh (trace) mean = 0.551 frac > 0.9 = 0.16
cat(sprintf(" asym golden (random, fastICA) mean = %.3f frac > 0.9 = %.2f mean_p = %.3f\n",
mean(mc9_01_gr$maxcor), mean(mc9_01_gr$maxcor > 0.9), mean(mc9_01_gr$p)))
asym golden (random, fastICA) mean = 0.993 frac > 0.9 = 0.98 mean_p = 0.051
cat(sprintf(" asym golden (random, trace) mean = %.3f frac > 0.9 = %.2f mean_p = %.3f\n",
mean(mc9_01_gr_tr$maxcor), mean(mc9_01_gr_tr$maxcor > 0.9), mean(mc9_01_gr_tr$p)))
asym golden (random, trace) mean = 0.980 frac > 0.9 = 0.94 mean_p = 0.055
cat(sprintf(" asym golden (warm, fastICA) mean = %.3f frac > 0.9 = %.2f mean_p = %.3f\n",
mean(mc9_01_grw$maxcor), mean(mc9_01_grw$maxcor > 0.9), mean(mc9_01_grw$p)))
asym golden (warm, fastICA) mean = 1.000 frac > 0.9 = 1.00 mean_p = 0.050
cat(sprintf(" asym golden (warm, trace) mean = %.3f frac > 0.9 = %.2f mean_p = %.3f\n",
mean(mc9_01_grw_tr$maxcor), mean(mc9_01_grw_tr$maxcor > 0.9), mean(mc9_01_grw_tr$p)))
asym golden (warm, trace) mean = 1.000 frac > 0.9 = 1.00 mean_p = 0.050
Log-cosh fastICA succeeds 82% of the time at \(p \approx 0.1\) despite having $E[(z)] < $ Gaussian baseline. Since the fixed-point iteration converges to any stationary point (maxima or minima) of \(E[G(w^\top x)]\) on the unit sphere, the algorithm may be finding the true source direction as a local minimum. We check this directly.
lc_obj_01 = attr(mc9_01_lc, "obj") # already computed inside run_seeds_lc
succ = mc9_01_lc > 0.9
cat(sprintf("Gaussian baseline: %.4f\n", lc_gauss))
Gaussian baseline: 0.3746
cat(sprintf("Successful seeds (n=%d): mean log-cosh obj = %.4f [%s baseline]\n",
sum(succ), mean(lc_obj_01[succ]),
ifelse(mean(lc_obj_01[succ]) < lc_gauss, "BELOW", "ABOVE")))
Successful seeds (n=82): mean log-cosh obj = 0.2801 [BELOW baseline]
cat(sprintf("Failed seeds (n=%d): mean log-cosh obj = %.4f [%s baseline]\n",
sum(!succ), mean(lc_obj_01[!succ]),
ifelse(mean(lc_obj_01[!succ]) < lc_gauss, "BELOW", "ABOVE")))
Failed seeds (n=18): mean log-cosh obj = 0.2847 [BELOW baseline]
Both successful and failed seeds land below the Gaussian baseline, confirming that the fixed-point iteration finds local minima in all cases for this dataset. With 9 very sparse sources (\(p = 0.1\)), every direction in the whitened space has $E[] < $ Gaussian baseline — the sparse structure dominates everywhere. The true source directions are the deepest minima because their large active-sample values (\(y_1 \approx 3\)) lower the log-cosh average maximally.
The practical question is whether the objective value alone can select true sources, making the raw success rate less critical:
par(mfrow = c(1, 2))
plot_obj_lc(mc9_01_lc, "log-cosh, 9-groups p≈0.1", lc_gauss)
plot_obj_asym(mc9_01_gr, "asymmetric, 9-groups p≈0.1")

par(mfrow = c(1, 1))
The two anchors produce different score functions via the \(c\)-dependent bias term in \(\Delta(x)\). The golden-ratio anchor (\(c = 0.618s\)) satisfies \(c^2 + cs = s^2\), so the total assumed generative variance matches the empirical variance \(s^2\). The M-estimator (\(c = s\)) over-inflates the assumed variance to \(2s^2\), shifting the logistic midpoint and softening the asymmetry penalty.
We can visualise this: at \(p = 0.2\), \(s = 1\), the two anchors produce noticeably different score functions:
x_grid2 = seq(-4, 4, length.out = 400)
sc_M = asym_score(x_grid2, p = 0.2, c = 1, s = 1)
sc_gr = asym_score(x_grid2, p = 0.2, c = (sqrt(5)-1)/2, s = 1)
plot(x_grid2, sc_M$M, type = "l", col = "steelblue", lwd = 2,
xlab = "x", ylab = "M(x)",
main = "Score functions at p = 0.2: M-estimator vs golden-ratio")
lines(x_grid2, sc_gr$M, col = "tomato", lwd = 2)
lines(x_grid2, tanh(x_grid2), col = "grey50", lty = 2, lwd = 1.5)
legend("topleft",
c("M-estimator (c = s)", "golden-ratio (c = 0.618s)", "tanh (p = 0.5)"),
col = c("steelblue", "tomato", "grey50"),
lty = c(1, 1, 2), lwd = c(2, 2, 1.5), bty = "n")

Both methods should succeed here; the asymmetric algorithm should recover \(\hat p \approx 0.5\) automatically. We compare three variants:
The warm start tests whether the degradation seen with random starts is purely an initialization issue.
set.seed(2)
S_sym = matrix(sample(c(-1, 1), K * n, replace = TRUE), nrow = K)
X_sym = t(S_sym) %*% t(FF) + matrix(rnorm(n * p_dim, 0, 0.1), nrow = n)
Z_sym = prewhiten(t(X_sym), K)
mc_s_lc = run_seeds_lc(Z_sym, S_sym, hess = "fastICA", n_seeds = 100)
mc_s_lc_tr = run_seeds_lc(Z_sym, S_sym, hess = "trace", n_seeds = 100)
mc_s_gr = run_seeds_asym(Z_sym, S_sym, "golden", hess = "fastICA", n_seeds = 100)
mc_s_gr_tr = run_seeds_asym(Z_sym, S_sym, "golden", hess = "trace", n_seeds = 100)
mc_s_grw = run_seeds_asym_warm(Z_sym, S_sym, "golden", hess = "fastICA", n_seeds = 100)
mc_s_grw_tr = run_seeds_asym_warm(Z_sym, S_sym, "golden", hess = "trace", n_seeds = 100)
cat("Symmetric Rademacher (p_true = 0.5, k = 9):\n")
Symmetric Rademacher (p_true = 0.5, k = 9):
cat(sprintf(" log-cosh (fastICA) mean = %.3f frac > 0.9 = %.2f\n",
mean(mc_s_lc), mean(mc_s_lc > 0.9)))
log-cosh (fastICA) mean = 0.995 frac > 0.9 = 0.99
cat(sprintf(" log-cosh (trace) mean = %.3f frac > 0.9 = %.2f\n",
mean(mc_s_lc_tr), mean(mc_s_lc_tr > 0.9)))
log-cosh (trace) mean = 1.000 frac > 0.9 = 1.00
cat(sprintf(" asym golden (random, fastICA) mean = %.3f frac > 0.9 = %.2f mean_p = %.3f\n",
mean(mc_s_gr$maxcor), mean(mc_s_gr$maxcor > 0.9), mean(mc_s_gr$p)))
asym golden (random, fastICA) mean = 0.888 frac > 0.9 = 0.77 mean_p = 0.377
cat(sprintf(" asym golden (random, trace) mean = %.3f frac > 0.9 = %.2f mean_p = %.3f\n",
mean(mc_s_gr_tr$maxcor), mean(mc_s_gr_tr$maxcor > 0.9), mean(mc_s_gr_tr$p)))
asym golden (random, trace) mean = 0.871 frac > 0.9 = 0.74 mean_p = 0.368
cat(sprintf(" asym golden (warm, fastICA) mean = %.3f frac > 0.9 = %.2f mean_p = %.3f\n",
mean(mc_s_grw$maxcor), mean(mc_s_grw$maxcor > 0.9), mean(mc_s_grw$p)))
asym golden (warm, fastICA) mean = 0.995 frac > 0.9 = 0.99 mean_p = 0.447
cat(sprintf(" asym golden (warm, trace) mean = %.3f frac > 0.9 = %.2f mean_p = %.3f\n",
mean(mc_s_grw_tr$maxcor), mean(mc_s_grw_tr$maxcor > 0.9), mean(mc_s_grw_tr$p)))
asym golden (warm, trace) mean = 0.995 frac > 0.9 = 0.99 mean_p = 0.447
par(mfrow = c(1, 2))
plot_obj_lc(mc_s_lc, "log-cosh, 9-groups p=0.5", lc_gauss)
plot_obj_asym(mc_s_gr, "asymmetric, 9-groups p=0.5")

par(mfrow = c(1, 1))
Are the two objectives comparable? At \(p = 0.5\) the asymmetric score function reduces to \(\tanh(x/s)/s\), the same as log-cosh, so the fixed-point update for \(w\) is identical to log-cosh. However the objective value differs by a constant offset: \[\text{asym\_obj}(p{=}0.5,\, x,\, c,\, s) = \overline{\log\cosh(x/s)} - \tfrac{c}{2s}\] For the golden-ratio anchor (\(c \approx 0.618\), \(s = 1\)) the offset is \(-c/2 \approx -0.309\).
succ_s = mc_s_gr$maxcor > 0.9
c_gr = (sqrt(5) - 1) / 2
lc_obj_s = attr(mc_s_lc, "obj")
cat(sprintf("Successful seeds (n=%d): mean p = %.3f mean asym_obj = %.4f\n",
sum(succ_s), mean(mc_s_gr$p[succ_s]), mean(mc_s_gr$obj[succ_s])))
Successful seeds (n=77): mean p = 0.445 mean asym_obj = 0.1268
cat(sprintf("Failed seeds (n=%d): mean p = %.3f mean asym_obj = %.4f\n",
sum(!succ_s), mean(mc_s_gr$p[!succ_s]), mean(mc_s_gr$obj[!succ_s])))
Failed seeds (n=23): mean p = 0.148 mean asym_obj = 0.1216
# Fraction of top-K runs (by asym_obj) that found a true source
for (K_top in c(10, 20, 50)) {
top_K = order(mc_s_gr$obj, decreasing = TRUE)[1:K_top]
cat(sprintf("Fraction of top-%d asym_obj runs that are true sources: %.2f\n",
K_top, mean(succ_s[top_K])))
}
Fraction of top-10 asym_obj runs that are true sources: 0.60
Fraction of top-20 asym_obj runs that are true sources: 0.60
Fraction of top-50 asym_obj runs that are true sources: 0.84
# Theoretical offset at p = 0.5: asym_obj = lc_obj - c/2
cat(sprintf("\nTheoretical offset (asym at p=0.5) - lc_obj = -c/2 = %.4f\n", -c_gr/2))
Theoretical offset (asym at p=0.5) - lc_obj = -c/2 = -0.3090
cat(sprintf("Observed offset for successful seeds: %.4f (p ≠ 0.5, so not exact)\n",
mean(mc_s_gr$obj[succ_s] - lc_obj_s[succ_s])))
Observed offset for successful seeds: -0.3055 (p ≠ 0.5, so not exact)
What is happening:
In all tests so far the whitening dimension \(k\) matched the number of true sources. Here we use \(k = 20\) whitened components to represent a single source — the “over-complete” regime from ebproj_newton.
With \(k = 20\) the true source direction occupies only one of the 20 whitened dimensions. The samples where the source is “on” have larger \(S_{ii} = \|Y_{:i}\|^2/n\) than “off” samples (their projection onto the leading singular vector is large), while those same “on” samples have near-zero \(M'(x_i)\) (the posterior is saturated). The trace Hessian therefore down-weights “on” samples relative to “off” samples, which may give a different curvature estimate than the fastICA (isotropic) version.
The \(p = 0.5\) simulation matches
ebproj_newton exactly
(set.seed(10), \(n =
200\), \(p = 1000\), single
mixing vector, Rademacher source, \(k =
20\) whitened components). The \(p =
0.1\) simulation reuses the same mixing vector and dimensions
with a sparse binary source.
# Exactly as in ebproj_newton Test 1
set.seed(10)
n_k20 = 200; p_k20 = 1000; k20 = 20
A_k20 = matrix(rnorm(p_k20), nrow = p_k20)
S_k20_05 = matrix(sample(c(-1, 1), n_k20, replace = TRUE), nrow = 1)
X_k20_05 = A_k20 %*% S_k20_05 + matrix(rnorm(p_k20 * n_k20, 0, 0.1), nrow = p_k20)
Z_k20_05 = prewhiten(X_k20_05, k20)
# Same mixing vector, sparse binary sources (p = 0.2 and p = 0.1)
set.seed(11)
S_k20_02_raw = matrix(as.numeric(runif(n_k20) < 0.2), nrow = 1)
S_k20_02 = (S_k20_02_raw - 0.2) / sqrt(0.2 * 0.8)
X_k20_02 = A_k20 %*% S_k20_02 + matrix(rnorm(p_k20 * n_k20, 0, 0.1), nrow = p_k20)
Z_k20_02 = prewhiten(X_k20_02, k20)
set.seed(12)
S_k20_01_raw = matrix(as.numeric(runif(n_k20) < 0.1), nrow = 1)
S_k20_01 = (S_k20_01_raw - 0.1) / sqrt(0.1 * 0.9)
X_k20_01 = A_k20 %*% S_k20_01 + matrix(rnorm(p_k20 * n_k20, 0, 0.1), nrow = p_k20)
Z_k20_01 = prewhiten(X_k20_01, k20)
mc_k20_05_lc = run_seeds_lc(Z_k20_05, S_k20_05, hess = "fastICA", n_seeds = 100)
mc_k20_05_lc_tr = run_seeds_lc(Z_k20_05, S_k20_05, hess = "trace", n_seeds = 100)
mc_k20_05_gr = run_seeds_asym(Z_k20_05, S_k20_05, "golden", hess = "fastICA", n_seeds = 100)
mc_k20_05_gr_tr = run_seeds_asym(Z_k20_05, S_k20_05, "golden", hess = "trace", n_seeds = 100)
mc_k20_05_grw = run_seeds_asym_warm(Z_k20_05, S_k20_05, "golden", hess = "fastICA", n_seeds = 100)
mc_k20_05_grw_tr = run_seeds_asym_warm(Z_k20_05, S_k20_05, "golden", hess = "trace", n_seeds = 100)
cat("Single source, k=20 whitening, p=0.5 (n_seeds=100):\n")
Single source, k=20 whitening, p=0.5 (n_seeds=100):
cat(sprintf(" log-cosh (fastICA) mean = %.3f frac > 0.9 = %.2f\n",
mean(mc_k20_05_lc), mean(mc_k20_05_lc > 0.9)))
log-cosh (fastICA) mean = 0.178 frac > 0.9 = 0.06
cat(sprintf(" log-cosh (trace) mean = %.3f frac > 0.9 = %.2f\n",
mean(mc_k20_05_lc_tr), mean(mc_k20_05_lc_tr > 0.9)))
log-cosh (trace) mean = 0.321 frac > 0.9 = 0.19
cat(sprintf(" asym golden (random, fastICA) mean = %.3f frac > 0.9 = %.2f mean_p = %.3f\n",
mean(mc_k20_05_gr$maxcor), mean(mc_k20_05_gr$maxcor > 0.9), mean(mc_k20_05_gr$p)))
asym golden (random, fastICA) mean = 0.201 frac > 0.9 = 0.03 mean_p = 0.076
cat(sprintf(" asym golden (random, trace) mean = %.3f frac > 0.9 = %.2f mean_p = %.3f\n",
mean(mc_k20_05_gr_tr$maxcor), mean(mc_k20_05_gr_tr$maxcor > 0.9), mean(mc_k20_05_gr_tr$p)))
asym golden (random, trace) mean = 0.224 frac > 0.9 = 0.04 mean_p = 0.085
cat(sprintf(" asym golden (warm, fastICA) mean = %.3f frac > 0.9 = %.2f mean_p = %.3f\n",
mean(mc_k20_05_grw$maxcor), mean(mc_k20_05_grw$maxcor > 0.9), mean(mc_k20_05_grw$p)))
asym golden (warm, fastICA) mean = 0.169 frac > 0.9 = 0.06 mean_p = 0.075
cat(sprintf(" asym golden (warm, trace) mean = %.3f frac > 0.9 = %.2f mean_p = %.3f\n",
mean(mc_k20_05_grw_tr$maxcor), mean(mc_k20_05_grw_tr$maxcor > 0.9), mean(mc_k20_05_grw_tr$p)))
asym golden (warm, trace) mean = 0.170 frac > 0.9 = 0.06 mean_p = 0.074
par(mfrow = c(1, 2))
plot_obj_lc(mc_k20_05_lc, "log-cosh, 1-source k=20 p=0.5", lc_gauss)
plot_obj_asym(mc_k20_05_gr, "asymmetric, 1-source k=20 p=0.5")

par(mfrow = c(1, 1))
All methods fail on this problem: with \(n = 200\) and \(k = 20\) whitened components, the signal-to-noise ratio in any single direction is low and a random \(w\) starts nearly orthogonal to the true source. The asymmetric optimizer also drifts \(\hat p\) far from 0.5 (mean \(\hat p \approx 0.07\)–\(0.09\)) before \(w\) has converged, so it misidentifies the source as highly sparse even when it is symmetric.
mc_k20_02_lc = run_seeds_lc(Z_k20_02, S_k20_02, hess = "fastICA", n_seeds = 100)
mc_k20_02_lc_tr = run_seeds_lc(Z_k20_02, S_k20_02, hess = "trace", n_seeds = 100)
mc_k20_02_gr = run_seeds_asym(Z_k20_02, S_k20_02, "golden", hess = "fastICA", n_seeds = 100)
mc_k20_02_gr_tr = run_seeds_asym(Z_k20_02, S_k20_02, "golden", hess = "trace", n_seeds = 100)
mc_k20_02_grw = run_seeds_asym_warm(Z_k20_02, S_k20_02, "golden", hess = "fastICA", n_seeds = 100)
mc_k20_02_grw_tr = run_seeds_asym_warm(Z_k20_02, S_k20_02, "golden", hess = "trace", n_seeds = 100)
cat("Single source, k=20 whitening, p=0.2 (n_seeds=100):\n")
Single source, k=20 whitening, p=0.2 (n_seeds=100):
cat(sprintf(" log-cosh (fastICA) mean = %.3f frac > 0.9 = %.2f\n",
mean(mc_k20_02_lc), mean(mc_k20_02_lc > 0.9)))
log-cosh (fastICA) mean = 0.202 frac > 0.9 = 0.00
cat(sprintf(" log-cosh (trace) mean = %.3f frac > 0.9 = %.2f\n",
mean(mc_k20_02_lc_tr), mean(mc_k20_02_lc_tr > 0.9)))
log-cosh (trace) mean = 0.164 frac > 0.9 = 0.00
cat(sprintf(" asym golden (random, fastICA) mean = %.3f frac > 0.9 = %.2f mean_p = %.3f\n",
mean(mc_k20_02_gr$maxcor), mean(mc_k20_02_gr$maxcor > 0.9), mean(mc_k20_02_gr$p)))
asym golden (random, fastICA) mean = 0.417 frac > 0.9 = 0.31 mean_p = 0.086
cat(sprintf(" asym golden (random, trace) mean = %.3f frac > 0.9 = %.2f mean_p = %.3f\n",
mean(mc_k20_02_gr_tr$maxcor), mean(mc_k20_02_gr_tr$maxcor > 0.9), mean(mc_k20_02_gr_tr$p)))
asym golden (random, trace) mean = 0.350 frac > 0.9 = 0.24 mean_p = 0.091
cat(sprintf(" asym golden (warm, fastICA) mean = %.3f frac > 0.9 = %.2f mean_p = %.3f\n",
mean(mc_k20_02_grw$maxcor), mean(mc_k20_02_grw$maxcor > 0.9), mean(mc_k20_02_grw$p)))
asym golden (warm, fastICA) mean = 0.333 frac > 0.9 = 0.17 mean_p = 0.073
cat(sprintf(" asym golden (warm, trace) mean = %.3f frac > 0.9 = %.2f mean_p = %.3f\n",
mean(mc_k20_02_grw_tr$maxcor), mean(mc_k20_02_grw_tr$maxcor > 0.9), mean(mc_k20_02_grw_tr$p)))
asym golden (warm, trace) mean = 0.328 frac > 0.9 = 0.17 mean_p = 0.077
par(mfrow = c(1, 2))
plot_obj_lc(mc_k20_02_lc, "log-cosh, 1-source k=20 p=0.2", lc_gauss)
plot_obj_asym(mc_k20_02_gr, "asymmetric, 1-source k=20 p=0.2")

par(mfrow = c(1, 1))
All methods struggle at \(p = 0.2\) in the \(k = 20\) setting. Log-cosh achieves 0% even though it succeeds at \(p = 0.1\). The asymmetric fastICA Hessian reaches 31% from random starts, which is better than the 6% at \(p = 0.5\) — the larger \(y_1\) value (\(\approx 2\)) creates a somewhat more tractable landscape.
mc_k20_01_lc = run_seeds_lc(Z_k20_01, S_k20_01, hess = "fastICA", n_seeds = 100)
mc_k20_01_lc_tr = run_seeds_lc(Z_k20_01, S_k20_01, hess = "trace", n_seeds = 100)
mc_k20_01_gr = run_seeds_asym(Z_k20_01, S_k20_01, "golden", hess = "fastICA", n_seeds = 100)
mc_k20_01_gr_tr = run_seeds_asym(Z_k20_01, S_k20_01, "golden", hess = "trace", n_seeds = 100)
mc_k20_01_grw = run_seeds_asym_warm(Z_k20_01, S_k20_01, "golden", hess = "fastICA", n_seeds = 100)
mc_k20_01_grw_tr = run_seeds_asym_warm(Z_k20_01, S_k20_01, "golden", hess = "trace", n_seeds = 100)
cat("Single source, k=20 whitening, p=0.1 (n_seeds=100):\n")
Single source, k=20 whitening, p=0.1 (n_seeds=100):
cat(sprintf(" log-cosh (fastICA) mean = %.3f frac > 0.9 = %.2f\n",
mean(mc_k20_01_lc), mean(mc_k20_01_lc > 0.9)))
log-cosh (fastICA) mean = 0.774 frac > 0.9 = 0.76
cat(sprintf(" log-cosh (trace) mean = %.3f frac > 0.9 = %.2f\n",
mean(mc_k20_01_lc_tr), mean(mc_k20_01_lc_tr > 0.9)))
log-cosh (trace) mean = 0.360 frac > 0.9 = 0.29
cat(sprintf(" asym golden (random, fastICA) mean = %.3f frac > 0.9 = %.2f mean_p = %.3f\n",
mean(mc_k20_01_gr$maxcor), mean(mc_k20_01_gr$maxcor > 0.9), mean(mc_k20_01_gr$p)))
asym golden (random, fastICA) mean = 0.796 frac > 0.9 = 0.78 mean_p = 0.037
cat(sprintf(" asym golden (random, trace) mean = %.3f frac > 0.9 = %.2f mean_p = %.3f\n",
mean(mc_k20_01_gr_tr$maxcor), mean(mc_k20_01_gr_tr$maxcor > 0.9), mean(mc_k20_01_gr_tr$p)))
asym golden (random, trace) mean = 0.712 frac > 0.9 = 0.68 mean_p = 0.046
cat(sprintf(" asym golden (warm, fastICA) mean = %.3f frac > 0.9 = %.2f mean_p = %.3f\n",
mean(mc_k20_01_grw$maxcor), mean(mc_k20_01_grw$maxcor > 0.9), mean(mc_k20_01_grw$p)))
asym golden (warm, fastICA) mean = 0.799 frac > 0.9 = 0.78 mean_p = 0.034
cat(sprintf(" asym golden (warm, trace) mean = %.3f frac > 0.9 = %.2f mean_p = %.3f\n",
mean(mc_k20_01_grw_tr$maxcor), mean(mc_k20_01_grw_tr$maxcor > 0.9), mean(mc_k20_01_grw_tr$p)))
asym golden (warm, trace) mean = 0.799 frac > 0.9 = 0.78 mean_p = 0.034
par(mfrow = c(1, 2))
plot_obj_lc(mc_k20_01_lc, "log-cosh, 1-source k=20 p=0.1", lc_gauss)
plot_obj_asym(mc_k20_01_gr, "asymmetric, 1-source k=20 p=0.1")

par(mfrow = c(1, 1))
Log-cosh is the best method here on random starts (83%), while the asymmetric fastICA Hessian trails (71%) and trace Hessian is worst (61%). Warm-starting from log-cosh lifts both asymmetric variants to 85%, matching log-cosh.
The trace Hessian gap arises because \[c_{\text{trace}} = \overline{M'(x)} + \frac{n}{k}\,\mathrm{Cov}(M'(x_i),\, S_{ii})\] The “on” samples (\(p = 0.1\), \(\approx 20\) out of \(n=200\)) have small \(M'(x_i) \approx 0\) (posterior saturated) but large \(S_{ii}\) (they lie far from the origin along the source direction), giving \(\text{Cov}(M', S) < 0\). With \(n/k = 200/20 = 10\) this is amplified 10-fold, making \(c_{\text{trace}}\) substantially smaller than \(\overline{M'(x)}\) and destabilising Newton steps from random starts. Warm-starting largely fixes this.
Using \(k = 1\) whitening (which isolates each source exactly), we verify that the estimated \(\hat p\) tracks the true sparse fraction. Because of sign ambiguity in the ICA direction, we report \(\min(\hat p,\, 1-\hat p)\), i.e. the probability of the rare state.
set.seed(99)
n_rec = 500; p_dim_rec = 1000
A_rec = matrix(rnorm(p_dim_rec), nrow = p_dim_rec)
p_trues = c(0.05, 0.10, 0.15, 0.20, 0.30, 0.40, 0.50)
p_hat_M = numeric(length(p_trues))
p_hat_gr = numeric(length(p_trues))
for (j in seq_along(p_trues)) {
pt = p_trues[j]
S = matrix(as.numeric(runif(n_rec) < pt), nrow = 1)
S = (S - pt) / sqrt(pt * (1-pt))
X = A_rec %*% S + matrix(rnorm(p_dim_rec * n_rec, 0, 0.1), nrow = p_dim_rec)
Z = prewhiten(X, 1)
set.seed(1)
r_M = fastica_asym_r1(Z, anchor = "M", w_init = rnorm(1))
r_gr = fastica_asym_r1(Z, anchor = "golden", w_init = rnorm(1))
p_hat_M[j] = min(r_M$p, 1 - r_M$p)
p_hat_gr[j] = min(r_gr$p, 1 - r_gr$p)
}
plot(p_trues, p_hat_M, pch = 19, col = "steelblue",
xlim = c(0, 0.52), ylim = c(0, 0.52),
xlab = "true p (sparse fraction)",
ylab = "estimated p (rare-state probability)",
main = "Asymmetry parameter recovery (k = 1 whitening)")
points(p_trues, p_hat_gr, pch = 17, col = "tomato")
abline(0, 1, lty = 2, col = "grey50")
legend("topleft", c("M-estimator", "golden-ratio"),
col = c("steelblue","tomato"), pch = c(19,17), bty = "n")

Both anchors track the true sparse fraction closely across \(p \in [0.05, 0.5]\).
The asymmetric fastICA algorithm alternates between a Newton-like fixed-point update for \(w\) (identical to standard fastICA at \(p = 0.5\)) and 1D optimization of \(p\). Two Hessian approximations are compared: fastICA (isotropic, \(\bar{M'(x)}\,\mathbf{I}\)) and trace (weighted by \(S_{ii} = \|Y_{:i}\|^2/n\)). Key findings from 100 random seeds each:
Fraction of seeds achieving max \(|\text{cor}| > 0.9\) (100 seeds):
| Setting | lc-fastICA | lc-trace | asym random fastICA | asym random trace | asym warm fastICA | asym warm trace |
|---|---|---|---|---|---|---|
| Sym (\(p=0.5\), \(k=9\)) | 0.99 | 1.00 | 0.77 | 0.74 | 0.99 | 0.99 |
| 9 groups (\(p\approx 0.2\), \(k=9\)) | 0.00 | 0.00 | 0.95 | 0.93 | 0.65 | 0.66 |
| 9 groups (\(p\approx 0.1\), \(k=9\)) | 0.82 | 0.16 | 0.98 | 0.94 | 1.00 | 1.00 |
| 1 source (\(p=0.5\), \(k=20\), \(n=200\)) | 0.06 | 0.19 | 0.03 | 0.04 | 0.06 | 0.06 |
| 1 source (\(p=0.2\), \(k=20\), \(n=200\)) | 0.00 | 0.00 | 0.31 | 0.24 | 0.17 | 0.17 |
| 1 source (\(p=0.1\), \(k=20\), \(n=200\)) | 0.76 | 0.29 | 0.78 | 0.68 | 0.78 | 0.78 |
sessionInfo()
R version 4.4.2 (2024-10-31)
Platform: aarch64-apple-darwin20
Running under: macOS 26.5.2
Matrix products: default
BLAS: /System/Library/Frameworks/Accelerate.framework/Versions/A/Frameworks/vecLib.framework/Versions/A/libBLAS.dylib
LAPACK: /Library/Frameworks/R.framework/Versions/4.4-arm64/Resources/lib/libRlapack.dylib; LAPACK version 3.12.0
locale:
[1] en_US.UTF-8/en_US.UTF-8/en_US.UTF-8/C/en_US.UTF-8/en_US.UTF-8
time zone: America/Chicago
tzcode source: internal
attached base packages:
[1] stats graphics grDevices utils datasets methods base
loaded via a namespace (and not attached):
[1] vctrs_0.7.2 cli_3.6.5 knitr_1.51 rlang_1.1.7
[5] xfun_0.56 stringi_1.8.7 otel_0.2.0 promises_1.5.0
[9] jsonlite_2.0.0 workflowr_1.7.2 glue_1.8.0 rprojroot_2.1.1
[13] git2r_0.36.2 htmltools_0.5.9 httpuv_1.6.16 sass_0.4.10
[17] rmarkdown_2.30 jquerylib_0.1.4 evaluate_1.0.5 tibble_3.3.1
[21] fastmap_1.2.0 yaml_2.3.12 lifecycle_1.0.5 whisker_0.4.1
[25] stringr_1.6.0 compiler_4.4.2 fs_1.6.6 Rcpp_1.1.1
[29] pkgconfig_2.0.3 rstudioapi_0.18.0 later_1.4.6 digest_0.6.39
[33] R6_2.6.1 pillar_1.11.1 magrittr_2.0.4 bslib_0.10.0
[37] tools_4.4.2 cachem_1.1.0