yukawa-2d-diffusion / diffusion /plot_chi_hist.py
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2D Yukawa HMC data + diffusion model (g=0.1)
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"""
Histograms comparing HMC vs DM (log / linear schedule) for the magnetization
distribution P(M) and the bootstrap sampling distribution of
chi = V(<M^2> - <|M|>^2).
Usage:
python plot_chi_hist.py --ep 0019
"""
import argparse
import h5py
import numpy as np
import matplotlib.pyplot as plt
COL = {"HMC": "#2a78d6", "DM log": "#1baf7a", "DM linear": "#eda100"}
INK = "#333333"
def chi_conn(m, V):
return V * (np.mean(m ** 2) - np.mean(np.abs(m)) ** 2)
def bootstrap_chi(M, V, n_boot=2000, block=1, seed=1):
"""Bootstrap replicas of chi; block>1 resamples blocks (autocorrelated data)."""
rng = np.random.default_rng(seed)
n = len(M) // block * block
blocks = M[:n].reshape(-1, block)
n_blk = blocks.shape[0]
reps = np.empty(n_boot)
for b in range(n_boot):
idx = rng.integers(0, n_blk, size=n_blk)
reps[b] = chi_conn(blocks[idx].ravel(), V)
return reps
def main():
parser = argparse.ArgumentParser()
parser.add_argument("--g", type=float, default=0.1)
parser.add_argument("--L", type=int, default=16)
parser.add_argument("--ep", type=str, default="0019")
parser.add_argument("--steps", type=int, default=2000)
args = parser.parse_args()
V = args.L ** 2
run_dir = f"runs/yukawa_L{args.L}_g{args.g}_ncsnpp"
with h5py.File(f"../samples/yukawa_g{args.g}_L{args.L}_1000000.jld2", "r") as f:
M = {"HMC": np.array(f["configs"]).mean(axis=(1, 2))}
for sched in ["log", "linear"]:
s = np.load(f"{run_dir}/data/samples_em_{sched}_steps{args.steps}_{args.ep}.npy")
M[f"DM {sched}"] = s.mean(axis=(0, 1))
boot = {
"HMC": bootstrap_chi(M["HMC"], V, block=500),
"DM log": bootstrap_chi(M["DM log"], V),
"DM linear": bootstrap_chi(M["DM linear"], V),
}
fig, (ax1, ax2) = plt.subplots(1, 2, figsize=(10.5, 4.2))
for ax in (ax1, ax2):
ax.spines[["top", "right"]].set_visible(False)
ax.grid(alpha=0.25, linewidth=0.6)
ax.tick_params(colors=INK, labelsize=9)
# Panel A: P(M)
lim = max(np.abs(m).max() for m in M.values())
bins = np.linspace(-lim, lim, 61)
for name, m in M.items():
ax1.hist(m, bins=bins, density=True, histtype="step",
linewidth=1.8, color=COL[name], label=name)
ax1.set_xlabel("M = (1/V) Σ φ(x)", color=INK)
ax1.set_ylabel("P(M)", color=INK)
ax1.set_title("Magnetization distribution\n(χ = V·connected variance of this)",
fontsize=10, color=INK)
ax1.legend(frameon=False, fontsize=9, labelcolor=INK)
# Panel B: bootstrap distribution of chi
lo = min(r.min() for r in boot.values())
hi = max(r.max() for r in boot.values())
bins2 = np.linspace(lo, hi, 51)
for name, reps in boot.items():
c = chi_conn(M[name], V)
e = reps.std()
ax2.hist(reps, bins=bins2, density=True, histtype="step",
linewidth=1.8, color=COL[name],
label=f"{name}: χ = {c:.3f}({e * 1e3:02.0f})")
ax2.set_xlabel("χ = V(⟨M²⟩ − ⟨|M|⟩²)", color=INK)
ax2.set_ylabel("bootstrap density", color=INK)
ax2.set_title("Sampling distribution of χ̂ (bootstrap)", fontsize=10, color=INK)
ax2.legend(frameon=False, fontsize=9, labelcolor=INK)
fig.suptitle(f"Yukawa g={args.g}, L={args.L} — HMC (N={len(M['HMC'])}) vs "
f"DM epoch {args.ep} (N={len(M['DM log'])}, EM {args.steps} steps)",
fontsize=11, color=INK)
fig.tight_layout()
out = f"{run_dir}/data/chi_hist_ep{args.ep}.png"
fig.savefig(out, dpi=150)
print(f"Saved {out}")
if __name__ == "__main__":
main()