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0c3dd1d | 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 61 62 63 64 65 66 67 68 69 70 71 72 73 74 75 76 77 78 79 80 81 82 83 84 85 86 87 88 89 90 91 92 93 94 95 96 97 98 99 100 101 102 103 104 105 106 107 108 109 110 111 112 113 114 115 116 117 118 119 120 121 122 123 124 125 126 127 128 129 130 131 132 133 134 135 136 137 138 139 140 141 142 143 144 145 146 147 148 149 150 151 152 153 154 155 156 157 158 159 160 161 162 163 164 165 166 167 168 169 170 171 172 173 174 175 176 177 178 179 180 181 182 183 184 185 186 187 188 189 190 191 192 193 194 195 196 197 198 199 200 201 202 203 204 205 206 207 208 209 210 211 212 213 214 215 216 217 218 219 220 221 222 223 224 225 226 227 228 229 230 231 232 233 234 235 236 237 238 239 240 241 242 243 244 245 246 247 248 249 250 251 252 253 254 255 256 | """Case 1 (ART) analysis under the per-start rank rule: Tables I, IV and V, sensitivity, physical pair tests.
TR logs (Chrono digital twin): B01 (S2, 400 starts, logged 40 s), B06 (S0/S1/S3/S4, 200 starts each), B07 (S2 starts
with the channel conditions D1a-D5, 200 starts each); per-start metrics from the extract stage. Physical reference
(Sim2Real): physical_runs.csv, mean of the per-run MAEs (5 runs per path and controller). NN-HD column of the TR
order: ctrl_label nnhdx175 for Path 1-2 targets and nnhdx150 for Path 3 targets. Baseline orders (nominal
simulation, Monte Carlo RF-A/RF-B, nominal simulation of Tables II-III) from baseline_orders.json.
Usage: python case1_rank_analysis.py <per_start_dir> <physical_runs.csv> <baseline_orders.json> <out_dir>
"""
import csv, glob, gzip, itertools, json, math, sys
import numpy as np
PER_START, PHYS_CSV, BASE_JSON, OUT = sys.argv[1:5]
RNG = np.random.default_rng(20261105)
B = 2000
BASE = ('mpc', 'nnmpc', 'pid')
LBL = {'mpc': 'MPC', 'nnmpc': 'NN-MPC', 'pid': 'PID', 'nnhd': 'NN-HD'}
ITEMS = ('mpc', 'nnmpc', 'pid', 'nnhd')
TARGETS = ('P1_lateral', 'P1_heading', 'P2_lateral', 'P2_heading', 'P3_lateral', 'P3_heading')
GAIN = {'P1': 'nnhdx175', 'P2': 'nnhdx175', 'P3': 'nnhdx150'}
def load(batch, col_fn):
"""scenario key -> {ctrl_label: row}"""
d = {}
for f in glob.glob(f'{PER_START}/{batch}/recovery_part*.csv.gz'):
for r in csv.DictReader(gzip.open(f, 'rt')):
d.setdefault((r['tag_family'], r['tag_condition'], r['scenario_id']), {})[r['ctrl_label']] = r
return d
B01, B06, B07 = load('B01_main_tr', None), load('B06_severity_shape', None), load('B07_dist_recovery', None)
def times(d, fam, cond, L='L010', Hd='H010', H=25.0, gain='nnhdx175', ids=None):
"""N x 4 array of first tube-entry times (capped at H), columns ITEMS; NN-HD column uses `gain`."""
col = f'T{25 if H <= 25 else 40}_trk100_{L}{Hd}_first'
rows, keys = [], []
for (f, c, sid), v in sorted(d.items()):
if f != fam or c != cond or not all(k in v for k in BASE + (gain,)):
continue
if ids is not None and sid not in ids:
continue
rows.append([min(float(v[k][col]), H) for k in BASE + (gain,)]); keys.append(sid)
return np.array(rows), keys
def ranks(T):
"""per-start ranks with shared ties (1 = fastest)"""
less = (T[:, None, :] < T[:, :, None]).sum(2)
eq = (T[:, None, :] == T[:, :, None]).sum(2) - 1
return 1 + less + eq / 2.0
def order_of(score): # ITEMS sorted by ascending score
return [ITEMS[i] for i in np.argsort(score, kind='stable')]
def tau(a, b):
pa = {c: i for i, c in enumerate(a)}; pb = {c: i for i, c in enumerate(b)}
s = sum(np.sign((pa[x] - pa[y]) * (pb[x] - pb[y])) for x, y in itertools.combinations(ITEMS, 2))
return s / 6.0
def summary(T, H):
R = ranks(T); n = len(T)
fail = (T >= H)
ok = ~fail.any(1)
rank_pct = {}
for j, c in enumerate(ITEMS):
cnt = np.zeros(4)
for row_t in T:
lo = 1 + (row_t < row_t[j]).sum(); k = (row_t == row_t[j]).sum()
cnt[lo - 1:lo - 1 + k] += 1.0 / k
rank_pct[LBL[c]] = [round(100 * x / n, 1) for x in cnt]
win = {}
for i, j in itertools.combinations(range(4), 2):
w = (T[:, i] < T[:, j]) + 0.5 * (T[:, i] == T[:, j])
bs = [w[RNG.integers(0, n, n)].mean() for _ in range(B)]
win[f'{LBL[ITEMS[i]]} beats {LBL[ITEMS[j]]}'] = [round(w.mean(), 3), [round(float(np.percentile(bs, 2.5)), 3), round(float(np.percentile(bs, 97.5)), 3)]]
return {'n': n, 'order': [LBL[c] for c in order_of(R.mean(0))],
'mean_rank': {LBL[c]: round(float(R.mean(0)[j]), 2) for j, c in enumerate(ITEMS)},
'rank_pct': rank_pct,
'fail_pct': {LBL[c]: round(100 * float(fail[:, j].mean()), 1) for j, c in enumerate(ITEMS)},
'n_all_recover': int(ok.sum()),
'mean_st_all_recover': {LBL[c]: round(float(T[ok, j].mean()), 2) for j, c in enumerate(ITEMS)},
'pairwise_win_rate_ci95': win}
# ---------------- physical reference ----------------
phys = {}
for r in csv.DictReader(open(PHYS_CSV)):
c = {'MPC': 'mpc', 'NN-MPC': 'nnmpc', 'PID': 'pid', 'NN-HD': 'nnhd'}[r['controller']]
phys.setdefault(f"{r['path']}_lateral", {}).setdefault(c, []).append(float(r['run_mae_lateral_m']))
phys.setdefault(f"{r['path']}_heading", {}).setdefault(c, []).append(float(r['run_mae_heading_rad']))
phys = {t: {c: np.array(v) for c, v in phys[t].items()} for t in TARGETS}
phys_order = {t: order_of(np.array([phys[t][c].mean() for c in ITEMS])) for t in TARGETS}
def phys_boot():
return {t: order_of(np.array([RNG.choice(phys[t][c], len(phys[t][c])).mean() for c in ITEMS])) for t in TARGETS}
def perm_p(a, b): # exact two-sided permutation test on the difference of means
x = np.concatenate([a, b]); n = len(a); obs = abs(a.mean() - b.mean()); cnt = tot = 0
for idx in itertools.combinations(range(len(x)), n):
m = np.zeros(len(x), bool); m[list(idx)] = True
cnt += abs(x[m].mean() - x[~m].mean()) >= obs - 1e-12; tot += 1
return cnt / tot
phys_tests = {}
for t in TARGETS:
rows = []
for a, b in itertools.combinations(ITEMS, 2):
rows.append({'pair': f'{LBL[a]} vs {LBL[b]}', 'mean_a': round(float(phys[t][a].mean()), 4),
'mean_b': round(float(phys[t][b].mean()), 4), 'p_perm': round(perm_p(phys[t][a], phys[t][b]), 4)})
ps = sorted(range(len(rows)), key=lambda i: rows[i]['p_perm']); run = 0.0
for k, i in enumerate(ps): # Holm step-down adjustment across the 6 pairs of this target
run = max(run, min(1.0, (len(rows) - k) * rows[i]['p_perm'])); rows[i]['p_holm'] = round(run, 4)
phys_tests[t] = rows
# ---------------- methods: TR (rank rule) and baselines ----------------
TS2 = {g: times(B01, 'S2', 'none', H=25.0, gain=g)[0] for g in ('nnhdx175', 'nnhdx150')}
RS2 = {g: ranks(T) for g, T in TS2.items()}
tr_order = {t: order_of(RS2[GAIN[t[:2]]].mean(0)) for t in TARGETS}
base = json.load(open(BASE_JSON))
methods = {'TR (rank rule, S2)': tr_order}
for m, name in (('M-NOM', 'Nominal simulation'), ('NOM-archived-2024', 'Nominal simulation (2024 archive)'),
('RF-A', 'Monte Carlo, start jitter (RF-A)'), ('RF-B', 'Monte Carlo, jitter + disturbances (RF-B)')):
methods[name] = {t: base[m][t]['predicted_ordering'] for t in TARGETS}
boot_phys = [phys_boot() for _ in range(B)]
n = len(RS2['nnhdx175'])
boot_tr = []
for _ in range(B):
idx = RNG.integers(0, n, n)
boot_tr.append({t: order_of(RS2[GAIN[t[:2]]][idx].mean(0)) for t in TARGETS})
def ci(v):
return [round(float(np.percentile(v, 2.5)), 2), round(float(np.percentile(v, 97.5)), 2)]
compare = {}
for name, ords in methods.items():
taus = {t: tau(ords[t], phys_order[t]) for t in TARGETS}
bt = {t: [tau((boot_tr[b][t] if name.startswith('TR') else ords[t]), boot_phys[b][t]) for b in range(B)] for t in TARGETS}
bmean = [np.mean([bt[t][b] for t in TARGETS]) for b in range(B)]
sel = {t: ords[t][0] for t in TARGETS}
regret = {t: round(float(phys[t][sel[t]].mean() / min(phys[t][c].mean() for c in ITEMS)), 2) for t in TARGETS}
# concordance on physically resolved pairs (Holm-adjusted permutation p < 0.05)
conc = tot = 0
for t in TARGETS:
for r_ in phys_tests[t]:
if r_['p_holm'] < 0.05:
a, b = (next(k for k in ITEMS if LBL[k] == s) for s in r_['pair'].split(' vs '))
pa = ords[t].index(a) < ords[t].index(b); pp = phys_order[t].index(a) < phys_order[t].index(b)
conc += pa == pp; tot += 1
compare[name] = {'order': {t: [LBL[c] for c in ords[t]] for t in TARGETS},
'tau': {t: round(taus[t], 2) for t in TARGETS}, 'tau_ci95': {t: ci(bt[t]) for t in TARGETS},
'mean_tau': round(float(np.mean(list(taus.values()))), 2), 'mean_tau_ci95': ci(bmean),
'exact_order_matches': int(sum(v == 1 for v in taus.values())),
'best_selected': int(sum(sel[t] == phys_order[t][0] for t in TARGETS)),
'selected_error_ratio_to_best': regret,
'resolved_pairs_correct': [conc, tot]}
# paired difference TR - nominal in mean tau
bt_tr = [np.mean([tau(boot_tr[b][t], boot_phys[b][t]) for t in TARGETS]) for b in range(B)]
bt_nom = [np.mean([tau(methods['Nominal simulation'][t], boot_phys[b][t]) for t in TARGETS]) for b in range(B)]
d = np.array(bt_tr) - np.array(bt_nom)
compare_delta = {'TR minus nominal, mean tau': round(compare['TR (rank rule, S2)']['mean_tau'] - compare['Nominal simulation']['mean_tau'], 2),
'ci95': ci(d)}
# same for the nominal simulation of Tables II-III (the paper's nominal baseline; no new random draws)
NOM_T = 'Nominal simulation (2024 archive)'
bt_nom_t = [np.mean([tau(methods[NOM_T][t], boot_phys[b][t]) for t in TARGETS]) for b in range(B)]
d_t = np.array(bt_tr) - np.array(bt_nom_t)
pt_t = np.mean([tau(tr_order[t], phys_order[t]) for t in TARGETS]) - np.mean([tau(methods[NOM_T][t], phys_order[t]) for t in TARGETS])
compare_delta_tables = {'TR minus nominal (Tables II-III), mean tau': round(float(pt_t), 2), 'ci95': ci(d_t),
'min': round(float(d_t.min()), 2), 'share_of_replicates_gt_0': float(np.mean(d_t > 0))}
def mean_tau(R_by_gain):
return round(float(np.mean([tau(order_of(R_by_gain[GAIN[t[:2]]].mean(0)), phys_order[t]) for t in TARGETS])), 2)
# ---------------- Table I offset sweep ----------------
sweep = []
for fam, d_, H in (('S0', B06, 25.0), ('S1', B06, 25.0), ('S2', B01, 25.0), ('S3', B06, 25.0), ('S4', B06, 25.0)):
T = {g: times(d_, fam, 'none', H=H, gain=g)[0] for g in ('nnhdx175', 'nnhdx150')}
s = summary(T['nnhdx175'], H); s['range'] = fam
s['mean_tau_vs_physical'] = mean_tau({g: ranks(v) for g, v in T.items()})
sweep.append(s)
# ---------------- tube and horizon sensitivity (S2) ----------------
tube = []
for L in ('L005', 'L010', 'L020'):
for Hd in ('H005', 'H010', 'H020'):
for H in (15.0, 25.0, 40.0):
T = {g: times(B01, 'S2', 'none', L, Hd, H, g)[0] for g in ('nnhdx175', 'nnhdx150')}
R = ranks(T['nnhdx175'])
tube.append({'tube_lat_m': int(L[1:]) / 100, 'tube_head_rad': int(Hd[1:]) / 100, 'H_s': H,
'order': [LBL[c] for c in order_of(R.mean(0))],
'mpc_first_pct': round(100 * float((R[:, 0] == 1).mean()), 1),
'fail_pct': {LBL[c]: round(100 * float((T['nnhdx175'][:, j] >= H).mean()), 1) for j, c in enumerate(ITEMS)},
'mean_tau_vs_physical': mean_tau({g: ranks(v) for g, v in T.items()})})
# ---------------- number of trials ----------------
R = RS2['nnhdx175']; full = order_of(R.mean(0)); nsens = []
for N in (10, 25, 50, 100, 200, 400):
same = top = 0
for _ in range(B):
idx = RNG.choice(n, N, replace=False); o = order_of(R[idx].mean(0))
same += o == full; top += o[0] == 'mpc'
nsens.append({'N': N, 'p_same_order_as_400': round(same / B, 3), 'p_mpc_first': round(top / B, 3)})
mr = np.sort(R.mean(0)); gap = float(np.min(np.diff(mr)))
hoeff = {'loss': 'per-start rank, bounded in [1, 4] (B = 3)', 'K': 4, 'alpha': 0.05,
'smallest_adjacent_mean_rank_gap_at_N400': round(gap, 3),
'n_bound': int(math.ceil(2 * 9 / gap ** 2 * math.log(2 * 4 / 0.05)))}
# ---------------- ablation by channel (B07, CRN starts of B01) ----------------
CH = {'D1a': 'actuation: +0.10 s delay', 'D1b': 'actuation: +0.20 s delay', 'D2a': 'actuation: steering bias 0.013',
'D2b': 'actuation: steering bias 0.026', 'D3a': 'observation: pose noise 0.02 m / 0.01 rad',
'D3b': 'observation: pose noise 0.05 m / 0.03 rad', 'D4a': 'plant: friction 0.6', 'D4b': 'plant: friction 0.4',
'D5': 'combined D1a + D2a + D3a'}
abl = []
ids = None
for cond, desc in CH.items():
T = {g: times(B07, 'S2', cond, H=25.0, gain=g) for g in ('nnhdx175', 'nnhdx150')}
keys = {k.split('_', 1)[1] for k in T['nnhdx175'][1]}
T0 = {g: times(B01, 'S2', 'none', H=25.0, gain=g, ids=keys)[0] for g in ('nnhdx175', 'nnhdx150')}
s = summary(T['nnhdx175'][0], 25.0)
abl.append({'condition': cond, 'channel': desc, 'n': s['n'], 'order': s['order'], 'mean_rank': s['mean_rank'],
'fail_pct': s['fail_pct'], 'mpc_first_pct': s['rank_pct']['MPC'][0],
'mean_tau_vs_physical': mean_tau({g: ranks(v[0]) for g, v in T.items()}),
'same_starts_no_disturbance': {'order': [LBL[c] for c in order_of(ranks(T0['nnhdx175']).mean(0))],
'mean_tau_vs_physical': mean_tau({g: ranks(v) for g, v in T0.items()})}})
# MPC failures by start pose: see mpc_failures/d3_range.py (all 29 divergences start beyond the cost ridge).
res = {'label': 'Case 1 analysis. TR rows: Chrono digital-twin recovery tests; physical reference: archived physical runs (Sim2Real). Rule: per-start rank.',
'physical_order': {t: [LBL[c] for c in o] for t, o in phys_order.items()},
'physical_pairwise_tests': phys_tests, 'method_comparison': compare, 'tr_minus_nominal': compare_delta, 'tr_minus_nominal_tables_II_III': compare_delta_tables,
'offset_sweep': sweep, 'tube_horizon_sensitivity': tube, 'trial_number_sensitivity': nsens,
'hoeffding': hoeff, 'ablation_by_channel': abl, 'bootstrap_B': B}
json.dump(res, open(f'{OUT}/case1_rank_analysis.json', 'w'), indent=1)
print(json.dumps({k: res[k] for k in ('physical_order', 'tr_minus_nominal', 'tr_minus_nominal_tables_II_III', 'hoeffding')}, indent=1))
for name, v in compare.items():
print(name, v['mean_tau'], v['mean_tau_ci95'], 'exact', v['exact_order_matches'], 'best', v['best_selected'], 'pairs', v['resolved_pairs_correct'], v['selected_error_ratio_to_best'])
for s in sweep:
print(s['range'], s['n'], '>'.join(s['order']), 'fail', s['fail_pct'], 'tau', s['mean_tau_vs_physical'], 'MPC1st', s['rank_pct']['MPC'][0])
for s in tube:
print(s['tube_lat_m'], s['tube_head_rad'], s['H_s'], '>'.join(s['order']), s['mpc_first_pct'], s['mean_tau_vs_physical'])
print(nsens)
for a in abl:
print(a['condition'], a['channel'], '>'.join(a['order']), a['mpc_first_pct'], a['fail_pct'], a['mean_tau_vs_physical'], a['same_starts_no_disturbance'])
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