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v492_celestial_z4_orbifold.py
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"""v492 -- CELEST.WP1.01: the Z4-orbifold structure of the celestial chiral algebra
on C^2/Z4 (the A3 ALE space) vs the E8 mu4-glue grading -- WP1 of the research
contract CELEST.SEAM.01 (tfpt_research_contracts). Sympy exact.
Question: does the mu4 clock on the seam celestial sphere select the SAME Z4
structure as the E8 mu4-glue grading (v125/v128), when both are read through the
celestial-chiral-algebra (CCA) lens of Bittleston-Homans-Sharma (arXiv:2305.09451,
JHEP 09 (2023) 008; the Eguchi-Hanson Z2 case) with a flat connection at infinity
(Kronheimer-Nakajima / heterotic-on-ALE standard)? Here k = 4: the spatial deck is
(z1,z2) -> (i z1, i^-1 z2) (the unique Z4 in SU(2) up to conjugacy, quotient = A3),
and rho = the E8 mu4 glue (v128 grading, exact on all 240 roots).
[E] S1. INNER GRADING / FLAT MONODROMY. v128 replication (240 = 52+64+60+64,
additive on all 6720 root pairs, dims with Cartan (60,64,60,64), g0 =
D5+A3 carrier = 60) PLUS the new statement: the grading is INNER --
h = (2,2,2,2,2;0^4) gives <alpha,h> = class mod 4 for all 240 roots, so
the glue IS Ad(exp(2 pi i h/4)), an order-4 torus element = a flat Z4
monodromy in the Kronheimer-Nakajima sense; the A3-side detector
h' = (0^5;1,1,1,-3) reads the SAME class -- the glue charge is the
diagonal (1,1) of the discriminant group Z4 x Z4 (the v92/v125 Lagrangian
glue); Z2 halfway: g0+g2 = 120 = SO(16), g1+g3 = 128 = spinor (v125
sub-Q-system {0,2}).
[E] S2. C^2/Z4 IS THE A3 SINGULARITY. Molien table of C[z1,z2] under the deck
(grade j = (p-q) mod 4) reproduced exactly by the character average;
invariant ring C[X,Y,Z]/(XY - Z^4) (exact relation); Hilbert series
(1+t^4)/((1-t^2)(1-t^4)) = grade-0 column; conjugation symmetry
N[d][1] = N[d][3] (the spatial 64/64 pairing slot).
[E] S3. GLUE-EQUIVARIANT SDYM(E8) SECTOR CLOSES. The rho-equivariant modes
g_j (x) C[z1,z2]_m with j + m = 0 mod 4 form a Lie subalgebra (needs
EXACTLY the v128 additivity); graded dims D[d] = 60(d+1) even / 64(d+1)
odd -- uniform per parity BECAUSE dim g0 = dim g2 = 60, dim g1 = dim g3
= 64 (the v128 dims are the consistency condition); zero modes (d=0) =
g0 = carrier D5+A3+Cartan = 60; asymptotic density 62/248 = 1/4 =
1/|Z4| (orbifold index); halfway EH/Z2 sector = 120/128 towers (the BHS
Z2 case refined by mu4 exactly as 4 = 2 x 2, v125).
[E] S4. (E8)_1 CHARACTER = SUM OF THE 4 GLUE SECTORS. Theta_E8 splits into
the 4 glue-coset thetas; shell 1 = (52,64,60,64) re-derived from the
LATTICE (independent of the root construction); sector characters
Theta_Cj/eta^8 sum exactly to chi_(E8)_1 = 1 + 248q + 4124q^2 + 34752q^3
(the v377 series); level-1 currents per sector = (60,64,60,64); sector
weights h_D5 = (0,5/8,1/2,5/8), h_A3 = (0,3/8,1/2,3/8) = the v92/v125
discriminant form (5x^2+3y^2)/8 mod 1; glue-diagonal h = (0,1,1,1)
INTEGER <=> v125 isotropy <=> the extension to (E8)_1 is local.
[E] S5. THE CRITICAL CORRECTION (clock != deck; clock^2 = deck). The A3 deck
diag(i,i^-1) induces z -> -z on the celestial sphere (projective order
2, the sheet flip) -- NOT the order-4 clock z -> iz. Any SU(2) lift of
the clock has order 8 (spin group Z8, would quotient to A7); the exact
bridge is (spin clock)^2 = deck generator, |Z8| = 8 = 2|mu4| (the
c3 = 1/(8 pi) seam winding integer). The order-4 clock IS realised as
the U(2) phase diag(i,1): projective order 4, fixed points {0,inf},
free orbit {1,i,-1,-i} = mu4 (all v180 clock properties), normalising
the deck (preserves the glue flat connection), det = i rotating the
holomorphic symplectic form by the mu4 generator (a Kaehler, NOT
triholomorphic isometry). Clock-invariance selects from the versal A3
family XY = Z^4 + a2 Z^2 + a1 Z + a0 EXACTLY the 1-parameter family
XY = Z^4 + a0, whose 4 branch points are ONE mu4 orbit with cross-ratio
2 -- the seam marks (v179 clock orbit; v168/v214 cross-ratio 2 =>
j = 1728 pillowcase).
[E] S6. NEGATIVE CONTROLS. False spatial action diag(i,i): det = -1 not in
SL(2,C) (no CY/ALE resolution), Poisson bracket leaves the invariant
sector in 14/14 nonzero cases, monomial grades unsymmetric -- killed
three ways. False glue (60- and 64-blocks swapped): additivity breaks
on 3112/6720 root pairs. Rigidity: of all 24 relabelings exactly
{identity, j -> -j} = Aut(Z4) are additive.
[C] THE CLOCK-DECK IDENTIFICATION IS A NAMED EXTRA IDENTIFICATION (verdict B,
not A): the match holds under ONE precisely named identification --
clock^2 = deck on the sphere (sheet-Z2 spin bookkeeping via Z8) -- which
is consistent with v109/v233 sheet structure but is NOT itself forced by
the arithmetic here.
[O] FENCE: this module is STRUCTURAL ARITHMETIC on finite data (roots, cosets,
monomials, Moebius/spin matrices). It does NOT construct a celestial
holography / twistorial bulk for TFPT; the celestial path stays the
research contract CELEST.SEAM.01 (WP2-WP5); SEAM.EQUIV.01 (the continuum
(E8)_1 net on the seam) stays [O] and is untouched.
Status: [E] exact arithmetic (sympy, no floats); [C] the named clock^2 = deck
identification; [O] the celestial-dual construction (contract). Python (sympy);
Wolfram-mirrorable (exact), deferred to the next verified engine run."""
from fractions import Fraction as F
from itertools import combinations, permutations, product
import sympy as sp
from tfpt_constants import check, summary, reset, g_car, N_fam, rankE8
HALF = F(1, 2)
DMAX = 9 # polynomial degree cutoff for the mode tables
# ---------------------------------------------------------------------------
# E8 roots in D5 (+) A3 + glue coordinates (the v128 construction)
# ---------------------------------------------------------------------------
def build_roots():
d5_roots, d5_v = [], []
for i, j in combinations(range(5), 2):
for si in (1, -1):
for sj in (1, -1):
v = [F(0)] * 5
v[i], v[j] = F(si), F(sj)
d5_roots.append(tuple(v))
for i in range(5):
for s in (1, -1):
v = [F(0)] * 5
v[i] = F(s)
d5_v.append(tuple(v))
d5_s, d5_c = [], []
for signs in product((1, -1), repeat=5):
v = tuple(HALF * s for s in signs)
(d5_s if signs.count(-1) % 2 == 0 else d5_c).append(v)
a3_roots = []
for i in range(4):
for j in range(4):
if i != j:
v = [F(0)] * 4
v[i], v[j] = F(1), F(-1)
a3_roots.append(tuple(v))
def wclass(k):
out = []
for sub in combinations(range(4), k):
v = [F(-k, 4)] * 4
for i in sub:
v[i] += 1
out.append(tuple(v))
return out
z5, z4 = tuple([F(0)] * 5), tuple([F(0)] * 4)
roots = {}
for r in d5_roots:
roots[(r, z4)] = 0
for r in a3_roots:
roots[(z5, r)] = 0
for d in d5_s:
for w in wclass(1):
roots[(d, w)] = 1
for d in d5_v:
for w in wclass(2):
roots[(d, w)] = 2
for d in d5_c:
for w in wclass(3):
roots[(d, w)] = 3
return roots
def additivity(roots, classmap):
"""(# root pairs whose sum is a root, # violating grade additivity)."""
items = list(roots.keys())
pairs = viol = 0
for i in range(len(items)):
a1, b1 = items[i]
for j in range(i + 1, len(items)):
a2, b2 = items[j]
s = (tuple(x + y for x, y in zip(a1, a2)),
tuple(x + y for x, y in zip(b1, b2)))
if s in roots:
pairs += 1
if classmap[s] != (classmap[items[i]] + classmap[items[j]]) % 4:
viol += 1
return pairs, viol
def monomial_table(action, dmax=DMAX, modulus=4):
"""N[d][j] = # monomials z1^p z2^q of degree d with grade j (mod modulus)."""
N = []
for d in range(dmax + 1):
row = [0] * modulus
for p in range(d + 1):
row[action(p, d - p) % modulus] += 1
N.append(row)
return N
def section1():
print(" -- S1: E8 mu4-glue grading (v128 replication + inner-torus test)")
roots = build_roots()
counts = [sum(1 for c in roots.values() if c == k) for k in range(4)]
norm_ok = all(sum(x * x for x in a) + sum(x * x for x in b) == 2
for (a, b) in roots)
check("S1 [E]: 240 roots, all norm 2, glue split 240 = 52+64+60+64: %s" % counts,
len(roots) == 240 and norm_ok and counts == [52, 64, 60, 64])
dims = [counts[0] + rankE8] + counts[1:] # Cartan (rank 8) sits in grade 0
check("S1 [E]: graded dims with Cartan dim g_j = %s = (60,64,60,64); "
"g0 = D5+A3 carrier (45+15=60)" % dims,
dims == [60, 64, 60, 64] and 45 + 15 == 60)
pairs, viol = additivity(roots, roots)
check("S1 [E]: grading additive on ALL %d root pairs (violations: %d)"
% (pairs, viol), pairs == 6720 and viol == 0)
h_d5 = tuple(F(2) for _ in range(5))
ok_h = all((sum(x * y for x, y in zip(a, h_d5))) % 4 == c
and (sum(x * y for x, y in zip(a, h_d5))).denominator == 1
for (a, b), c in roots.items())
check("S1 [E]: INNER grading -- h = (2,2,2,2,2;0^4) gives <alpha,h> = class mod 4 "
"for all 240 roots => glue = Ad(exp(2 pi i h/4)), an order-4 torus element "
"(flat Z4 connection / Kronheimer-Nakajima monodromy)", ok_h)
h_a3 = (F(1), F(1), F(1), F(-3))
ok_h2 = all((sum(x * y for x, y in zip(b, h_a3))) % 4 == c
and (sum(x * y for x, y in zip(b, h_a3))).denominator == 1
for (a, b), c in roots.items())
check("S1 [E]: the SAME class read off the A3 side by h' = (0^5;1,1,1,-3) -- the "
"glue charge is the DIAGONAL (1,1) of the discriminant group Z4 x Z4 of "
"D5 (+) A3 (the v92/v125 Lagrangian glue <(1,1)>)", ok_h2)
even, odd = dims[0] + dims[2], dims[1] + dims[3]
check("S1 [E]: Z2 halfway refinement g0+g2 = %d = dim SO(16), g1+g3 = %d = spinor "
"128 (the v125 sub-Q-system {0,2} = SO(16)_1 step)" % (even, odd),
even == 120 and odd == 128)
return roots, dims
def section2():
print(" -- S2: Molien/Hilbert data of C[z1,z2] under the A3 deck Z4")
N = monomial_table(lambda p, q: p - q)
t = sp.symbols('t')
i4 = sp.I
molien = []
for j in range(4):
Fj = sp.Rational(1, 4) * sum(
i4 ** ((-j * k) % 4) / ((1 - i4 ** k * t) * (1 - i4 ** (-k) * t))
for k in range(4))
ser = sp.series(sp.simplify(Fj), t, 0, DMAX + 1).removeO()
molien.append([int(sp.expand(ser).coeff(t, d)) for d in range(DMAX + 1)])
ok_molien = all(molien[j][d] == N[d][j]
for j in range(4) for d in range(DMAX + 1))
check("S2 [E]: Molien series (character average) reproduces the monomial table "
"exactly for all grades j = 0..3, d <= %d" % DMAX, ok_molien)
z1, z2 = sp.symbols('z1 z2')
X, Y, Z = z1 ** 4, z2 ** 4, z1 * z2
check("S2 [E]: invariant ring generated by X=z1^4, Y=z2^4, Z=z1 z2 with the A3 "
"relation XY = Z^4 (exact): C^2/Z4 IS the A3 ALE singularity",
sp.simplify(X * Y - Z ** 4) == 0)
hilb = sp.series((1 + t ** 4) / ((1 - t ** 2) * (1 - t ** 4)),
t, 0, DMAX + 1).removeO()
ok_hilb = all(int(sp.expand(hilb).coeff(t, d)) == N[d][0]
for d in range(DMAX + 1))
check("S2 [E]: Hilbert series of C[X,Y,Z]/(XY - Z^4) = (1+t^4)/((1-t^2)(1-t^4)) "
"matches the grade-0 Molien column", ok_hilb)
ok_conj = all(N[d][1] == N[d][3] for d in range(DMAX + 1))
check("S2 [E]: conjugation symmetry N[d][1] = N[d][3] (z1 <-> z2 swap = Weyl of "
"SU(2)) -- the spatial side offers the 64/64 pairing slot", ok_conj)
return N
def equivariant_dims(dims, N, modulus=4):
"""D[d] = sum_j dim(g_j) * N[d][(-j) mod modulus] (j + m = 0 mod modulus)."""
return [sum(dims[j % len(dims)] * N[d][(-j) % modulus]
for j in range(len(dims))) for d in range(len(N))]
def section3(dims, N):
print(" -- S3: glue-equivariant CCA sector of SDYM(E8) on C^2/Z4")
D = equivariant_dims(dims, N)
ok_shape = all(D[d] == (60 if d % 2 == 0 else 64) * (d + 1)
for d in range(DMAX + 1))
check("S3 [E]: D[d] = 60(d+1) for even d, 64(d+1) for odd d -- uniform per parity "
"BECAUSE dim g0 = dim g2 = 60 and dim g1 = dim g3 = 64 (the v128 dims are "
"exactly what uniformity requires); D[0..%d] = %s" % (DMAX, D), ok_shape)
check("S3 [E]: zero modes (d=0) = g0 alone: dim %d = D5 (+) A3 carrier + Cartan "
"-- the unbroken algebra on the orbifold IS the carrier" % D[0],
D[0] == 60)
check("S3 [E]: asymptotic density D[d]/(248(d+1)) -> (60+64)/2/248 = 1/4 = 1/|Z4| "
"(orbifold index density)", sp.Rational(62, 248) == sp.Rational(1, 4))
# closure: root-grade additivity (S1, 0 violations) + monomial grade (p-q)
# additive under multiplication by construction => equivariant subalgebra
check("S3 [E]: closure -- [g_j (x) m, g_k (x) m'] in g_{j+k} (x) mm' with "
"(j+k) + (grade m + grade m') = 0 mod 4: the equivariant sector is a Lie "
"subalgebra (needs EXACTLY the v128 additivity, 0 violations)", True)
N2 = monomial_table(lambda p, q: p + q, modulus=2)
D2 = [sum((dims[0] + dims[2] if j == 0 else dims[1] + dims[3]) * N2[d][j]
for j in range(2)) for d in range(DMAX + 1)]
ok_eh = all(D2[d] == (120 if d % 2 == 0 else 128) * (d + 1)
for d in range(DMAX + 1))
check("S3 [E]: halfway EH/Z2 sector (deck^2 = -1, the BHS Z2 case): dims 120(d+1) "
"/ 128(d+1) = SO(16) adjoint / spinor -- the A3 tower refines the EH tower "
"exactly as mu4 refines the sheet Z2 (4 = 2 x 2, v125)", ok_eh)
return D
def d5_coset_norms(maxnorm):
"""norm -> count for the 4 cosets of D5*/D5: 0=D5, v, s, c."""
out = {k: {} for k in ('0', 'v', 's', 'c')}
rng_int = range(-2, 3)
for v in product(rng_int, repeat=5):
n = F(sum(x * x for x in v))
if n > maxnorm:
continue
key = '0' if sum(v) % 2 == 0 else 'v'
out[key][n] = out[key].get(n, 0) + 1
rng_half = [F(k, 2) for k in (-3, -1, 1, 3)]
for v in product(rng_half, repeat=5):
n = sum(x * x for x in v)
if n > maxnorm:
continue
key = 's' if (sum(v) - F(5, 2)) % 2 == 0 else 'c'
out[key][n] = out[key].get(n, 0) + 1
return out
def a3_coset_norms(maxnorm):
"""norm -> count for the 4 cosets of A3*/A3: w0=A3, w1, w2, w3."""
out = {k: {} for k in range(4)}
for k in range(4):
shift = F(-k, 4)
rng = [m + shift for m in range(-3, 4)]
for v in product(rng, repeat=4):
if sum(v) != 0:
continue
n = sum(x * x for x in v)
if n > maxnorm:
continue
out[k][n] = out[k].get(n, 0) + 1
return out
def series_mul(a, b, nmax):
out = [0] * (nmax + 1)
for i, ai in enumerate(a):
if i > nmax:
break
for j, bj in enumerate(b):
if i + j > nmax:
break
out[i + j] += ai * bj
return out
def section4():
print(" -- S4: (E8)_1 character = sum of the 4 mu4 glue sectors (exact)")
NMAX = 3 # character levels q^0..q^3
MAXNORM = 2 * NMAX
d5 = d5_coset_norms(MAXNORM)
a3 = a3_coset_norms(MAXNORM)
pairing = {0: ('0', 0), 1: ('s', 1), 2: ('v', 2), 3: ('c', 3)}
theta = {}
for j, (dk, ak) in pairing.items():
coeffs = [0] * (NMAX + 1)
for n5, c5 in d5[dk].items():
for n3, c3l in a3[ak].items():
n = n5 + n3
if n <= MAXNORM and n % 2 == 0 and F(n, 2).denominator == 1:
coeffs[int(n) // 2] += c5 * c3l
theta[j] = coeffs
shell1 = [theta[j][1] for j in range(4)]
check("S4 [E]: shell 1 (norm 2): %s = (52,64,60,64) -- the v128 split re-derived "
"from the LATTICE, independent of the root construction" % shell1,
shell1 == [52, 64, 60, 64])
shell2 = [theta[j][2] for j in range(4)]
check("S4 [E]: shell 2 (norm 4): %s sums to 2160 = |E8 shell 2| -- the Z4 glue "
"grading persists shell by shell (Theta_E8 = sum Theta_Cj)" % shell2,
sum(shell2) == 2160)
q = sp.symbols('q')
P8 = sp.Integer(1)
for n in range(1, NMAX + 1):
P8 *= sum(sp.binomial(7 + k, 7) * q ** (n * k)
for k in range(0, NMAX // n + 1))
P8 = sp.expand(P8)
p8 = [int(P8.coeff(q, k)) for k in range(NMAX + 1)]
sigma3 = lambda n: sum(d ** 3 for d in range(1, n + 1) if n % d == 0)
e4 = [1] + [240 * sigma3(n) for n in range(1, NMAX + 1)]
chi_e8 = series_mul(e4, p8, NMAX)
sector = {j: series_mul(theta[j], p8, NMAX) for j in range(4)}
total = [sum(sector[j][m] for j in range(4)) for m in range(NMAX + 1)]
check("S4 [E]: sum of the 4 sector characters Theta_Cj/eta^8 = chi_(E8)_1 = %s "
"(1, 248, 4124, 34752 -- the v377 series)" % total,
total == chi_e8 and chi_e8 == [1, 248, 4124, 34752])
lvl1 = [sector[j][1] for j in range(4)]
check("S4 [E]: level-1 currents per sector: %s = (60,64,60,64) -- the v128 dims "
"WITH Cartan appear as the 4 branching blocks of the 248" % lvl1,
lvl1 == [60, 64, 60, 64])
hmin = [min(n for n, c in
{0: d5['0'], 1: d5['s'], 2: d5['v'], 3: d5['c']}[j].items()
if c > 0 and n > 0) for j in range(4)]
hd5 = [F(0)] + [F(h, 2) for h in hmin[1:]]
ha3 = [F(0)] + [F(min(n for n in a3[k] if n > 0), 2) for k in (1, 2, 3)]
qform = lambda x, y: F(5 * x * x + 3 * y * y, 8)
ok_h = all(hd5[j] % 1 == F(5 * j * j, 8) % 1
and ha3[j] % 1 == F(3 * j * j, 8) % 1 for j in range(4))
check("S4 [E]: sector weights h(D5) = (0,5/8,1/2,5/8), h(A3) = (0,3/8,1/2,3/8): "
"equal mod 1 to 5x^2/8 and 3y^2/8 -- the v92/v125 DISCRIMINANT FORM "
"(5x^2+3y^2)/8 IS the pair of conformal weights of the lattice-CFT sectors",
ok_h)
ok_int = all(qform(j, j) % 1 == 0 and (hd5[j] + ha3[j]) % 1 == 0
for j in range(4))
check("S4 [E]: glue-diagonal weights h_j = h_D5 + h_A3 INTEGER for all j "
"(h = 0,1,1,1): v125 isotropy q(k(1,1)) = k^2 in Z <=> all four sectors "
"are CURRENTS <=> the extension to (E8)_1 is local", ok_int)
def moebius_of_diag(a, d):
"""induced factor on z = z1/z2 for (z1,z2) -> (a z1, d z2)."""
return sp.simplify(a / d)
def proj_order(factor, nmax=16):
f = sp.Integer(1)
for n in range(1, nmax + 1):
f = sp.simplify(f * factor)
if f == 1:
return n
return None
def section5():
print(" -- S5: which Z4 rotates the celestial sphere? (exact spin arithmetic)")
I = sp.I
zeta8 = sp.exp(sp.I * sp.pi / 4)
fac_deck = moebius_of_diag(I, 1 / I)
check("S5 [E]: deck diag(i,i^-1) induces z -> (%s) z on the celestial sphere: "
"PROJECTIVE ORDER %s -- the A3 deck acts as the sheet flip z -> -z, NOT as "
"the order-4 clock z -> iz" % (fac_deck, proj_order(fac_deck)),
fac_deck == -1 and proj_order(fac_deck) == 2)
zeta = sp.symbols('zeta')
sols = sp.solve(sp.Eq(zeta ** 2, I), zeta)
orders = [proj_order(sp.simplify(s ** 2)) for s in sols]
su2_orders = []
for s in sols:
g = sp.Matrix([[s, 0], [0, 1 / s]])
p, m = sp.eye(2), g
k = 1
while not m.equals(p):
m = sp.simplify(m * g)
k += 1
if k > 20:
break
su2_orders.append(k)
check("S5 [E]: SPIN OBSTRUCTION -- any SU(2) lift diag(zeta,1/zeta) of the clock "
"z -> iz needs zeta^2 = i (primitive 8th root): SU(2) orders %s = 8 -- the "
"clock's spin group is Z8 (would quotient to A7), NEVER the A3 deck Z4"
% su2_orders,
all(o == 8 for o in su2_orders) and all(o == 4 for o in orders))
g8 = sp.Matrix([[zeta8, 0], [0, 1 / zeta8]])
deck = sp.Matrix([[I, 0], [0, 1 / I]])
check("S5 [E]: SPIN BRIDGE -- (spin clock)^2 = diag(zeta8,zeta8^-1)^2 = "
"diag(i,i^-1) = the A3 deck generator EXACTLY; the deck Z4 is the unique "
"index-2 subgroup of the clock's Z8; |Z8| = 8 = 2|mu4| (the c3 = 1/(8 pi) "
"seam winding integer)",
sp.simplify(g8 ** 2 - deck) == sp.zeros(2, 2))
fac_clock = moebius_of_diag(I, 1)
z = sp.symbols('z')
fixed = sp.solve(sp.Eq(I * z, z), z)
orbit = {sp.simplify(I ** k) for k in range(4)}
check("S5 [E]: U(2) CLOCK -- diag(i,1) induces z -> iz with projective order %s, "
"fixed points {0,inf}, free orbit {1,i,-1,-i} = mu4: ALL v180 clock "
"properties hold for this (non-deck) isometry" % proj_order(fac_clock),
fac_clock == I and proj_order(fac_clock) == 4
and fixed == [0] and orbit == {1, I, -1, -I})
clock = sp.Matrix([[I, 0], [0, 1]])
comm = sp.simplify(clock * deck - deck * clock)
det_clock = sp.simplify(clock.det())
check("S5 [E]: the clock NORMALISES the deck (commutator = 0, preserves the glue "
"flat connection); det = i of order 4: it rotates the holomorphic "
"symplectic form omega = dz1^dz2 by exactly the mu4 generator (a Kaehler, "
"NOT triholomorphic isometry -> rotates the twistor sphere by pi/2)",
comm == sp.zeros(2, 2) and det_clock == I
and proj_order(det_clock) == 4)
check("S5 [E]: clock vs deck on the sphere -- clock^2 induces z -> (%s) z = the "
"deck's sphere image: projectively the deck is the SQUARE of the clock "
"(the sheet pair Z2 inside the clock Z4)" % sp.simplify(fac_clock ** 2),
sp.simplify(fac_clock ** 2 - fac_deck) == 0)
Z, a3c, a2c, a1c, a0c = sp.symbols('Z a3 a2 a1 a0')
P = Z ** 4 + a3c * Z ** 3 + a2c * Z ** 2 + a1c * Z + a0c
diff = sp.expand(P.subs(Z, sp.I * Z) - P)
sol = sp.solve([sp.Poly(diff, Z).coeff_monomial(Z ** k) for k in range(4)],
[a3c, a2c, a1c], dict=True)
ok_def = sol == [{a3c: 0, a2c: 0, a1c: 0}]
check("S5 [E]: CLOCK-INVARIANT DEFORMATION -- P(iZ) = P(Z) forces a3 = a2 = a1 = "
"0: of the 3-parameter versal A3 family XY = Z^4 + a2 Z^2 + a1 Z + a0 "
"(3 = rank A3 = N_fam resolution spheres), the clock fixes EXACTLY the "
"1-parameter family XY = Z^4 + a0", ok_def and N_fam == 3)
c = sp.symbols('c', positive=True)
roots4 = sp.solve(sp.Eq(Z ** 4, c ** 4), Z)
ratios = {sp.simplify(r / c) for r in roots4}
z1r, z2r, z3r, z4r = c, sp.I * c, -c, -sp.I * c
lam = sp.simplify((z1r - z3r) * (z2r - z4r) / ((z1r - z4r) * (z2r - z3r)))
check("S5 [E]: the 4 branch points of XY = Z^4 - c^4 are ONE mu4 orbit "
"{c, ic, -c, -ic} with CROSS-RATIO %s = 2: the seam marks (v179 clock "
"orbit; v168/v214 cross-ratio 2 => j = 1728 pillowcase) appear as the "
"celestial deformation branch points" % lam,
ratios == {1, sp.I, -1, -sp.I} and lam == 2)
def section6(roots):
print(" -- S6: negative controls (the test must kill the fakes)")
I = sp.I
det_false = sp.simplify(sp.Matrix([[I, 0], [0, I]]).det())
check("S6 [E]: NC1a -- diag(i,i) has det = %s != 1: NOT in SL(2,C) => quotient "
"not Gorenstein/CY, NO ALE hyperkaehler resolution, no SD-gravity "
"background" % det_false, det_false == -1)
z1, z2 = sp.symbols('z1 z2')
pb = lambda f, g: (sp.diff(f, z1) * sp.diff(g, z2)
- sp.diff(f, z2) * sp.diff(g, z1))
grade_false = lambda p_, q_: (p_ + q_) % 4
viol = tested = 0
invmons = [(p_, q_) for p_ in range(5) for q_ in range(5)
if grade_false(p_, q_) == 0 and p_ + q_ > 0]
for (pa, qa), (pb_, qb_) in combinations(invmons, 2):
b = sp.expand(pb(z1 ** pa * z2 ** qa, z1 ** pb_ * z2 ** qb_))
if b == 0:
continue
tested += 1
if grade_false(pa + pb_ - 1, qa + qb_ - 1) != 0:
viol += 1
check("S6 [E]: NC1b -- Poisson bracket of diag(i,i)-invariant monomials leaves "
"the invariant sector in %d/%d nonzero cases (bracket shifts the grade by "
"-2 mod 4): the false w-algebra sector does NOT close -- KILLED"
% (viol, tested), viol == tested and tested > 0)
Nf = monomial_table(lambda p_, q_: p_ + q_)
asym = [(d, Nf[d][1], Nf[d][3]) for d in range(DMAX + 1)
if Nf[d][1] != Nf[d][3]]
check("S6 [E]: NC1c -- under diag(i,i) the monomial grades have N[d][1] != "
"N[d][3] at %d of %d levels: the conjugate 64/64 pairing of g1/g3 has NO "
"spatial partner slots -- KILLED" % (len(asym), DMAX + 1),
len(asym) > 0)
swap = {0: 0, 1: 2, 2: 1, 3: 3}
fake = {r: swap[c] for r, c in roots.items()}
pairs, viol2 = additivity(roots, fake)
check("S6 [E]: NC2 -- swapping the glue classes of the 64-block and the 60-block "
"breaks grading additivity on %d of %d root pairs (>0) and the conjugate "
"pairing (dim fake-g1 = 60 != 64 = dim fake-g3): the false glue does NOT "
"define a graded Lie algebra -- KILLED" % (viol2, pairs), viol2 > 0)
good = []
for perm in permutations(range(4)):
relab = {r: perm[c] for r, c in roots.items()}
_, v = additivity(roots, relab)
if v == 0:
good.append(perm)
check("S6 [E]: NC3 RIGIDITY -- of all 24 relabelings of the glue classes exactly "
"%d are additive: %s = identity and negation j -> -j = Aut(Z4): the mu4 "
"glue grading is rigid up to the group automorphism" % (len(good), good),
sorted(good) == [(0, 1, 2, 3), (0, 3, 2, 1)])
def run():
reset()
print("v492 CELEST.WP1.01: Z4-orbifold structure of the celestial chiral algebra "
"on C^2/Z4 (A3 ALE) vs the E8 mu4-glue grading (WP1 of CELEST.SEAM.01)")
roots, dims = section1()
N = section2()
section3(dims, N)
section4()
section5()
section6(roots)
# fences (recorded, not computed): verdict B + the [O] contract scope
check("FENCE [C]: the clock-deck identification is a NAMED extra identification "
"(verdict B, not A): the match holds under clock^2 = deck on the sphere "
"(sheet-Z2 spin bookkeeping, Z8 with 8 = 2|mu4| = %d); consistent with the "
"v109/v233 sheet structure, not forced by the arithmetic here"
% (2 * 4), 2 * 4 == 8 == g_car + N_fam)
check("FENCE [O]: structural arithmetic ONLY -- no celestial duality is "
"constructed; the celestial path stays the research contract "
"CELEST.SEAM.01 (WP2-WP5); SEAM.EQUIV.01 stays [O], untouched", True)
return summary("v492 CELEST.WP1.01: E8 mu4-glue = inner order-4 torus automorphism = flat "
"Z4 monodromy on the A3 ALE C^2/Z4; glue-equivariant SDYM(E8) sector closes "
"with dims 60/64 alternating, zero modes = carrier; (E8)_1 character = sum of "
"the 4 glue sectors with h = discriminant form; the mu4 clock is the U(2) "
"phase diag(i,1) with clock^2 = deck (spin bridge Z8, 8 = 2|mu4|); "
"clock-invariant A3 deformation = 1-parameter, branch points = one mu4 orbit, "
"cross-ratio 2; negative controls kill false action/false glue; rigidity = "
"Aut(Z4). Verdict B; SEAM.EQUIV.01 untouched")
if __name__ == "__main__":
raise SystemExit(1 if run() else 0)
Recorded source fingerprint
7dc06180a0398a6b2d300b0c6d19150e4ad943eef3b058438d6a353b653ada44
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