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v1032_covariant_curvature.py
verification/v1032_covariant_curvature.py
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#!/usr/bin/env python3
"""Exact algebra for the free Lorentz-covariant curvature extension.
No TFPT-parent, interacting-gravity, T7-completion, TOE, or RH claim.
The distributional construction and its scope are proved in PROOF.tex.
Only SymPy is required. All checks below are exact, not floating scans.
Port provenance: native verification port of
`toe_round7_covariant_curvature/covariant_curvature_checker.py`
(source SHA-256 10eff5bab2ac8df6a532f5112503678e58233006d2fe93daa7e00271c6d9f210).
The port changes only harness integration and execution lifecycle.
"""
from __future__ import annotations
import json
import time
import sympy as s
from tfpt_constants import check as suite_check, reset, summary
ETA = s.diag(-1, 1, 1, 1)
PAIRS = ((0, 1), (0, 2), (0, 3), (1, 2), (1, 3), (2, 3))
CURV = tuple((a, b) for a in range(6) for b in range(a, 6))
SPATIAL = ((0, 0), (1, 1), (2, 2), (1, 2), (0, 2), (0, 1))
CHECKS: list[str] = []
FAILED = 0
def check(label, condition):
global FAILED
passed = suite_check(label, bool(condition))
CHECKS.append(label)
FAILED += int(not passed)
def zero(value):
values = list(value) if isinstance(value, s.MatrixBase) else [value]
return all(s.expand(v) == 0 for v in values)
def symbasis(n, pairs):
result = []
for i, j in pairs:
b = s.zeros(n)
b[i, j] = b[j, i] = 1 if i == j else 1/s.sqrt(2)
result.append(b)
return result
HPAIRS = tuple((i, j) for i in range(4) for j in range(i, 4))
HBASIS = symbasis(4, HPAIRS)
SBASIS = symbasis(3, SPATIAL)
def coordinates(h):
return s.Matrix([s.trace(b.T*h) for b in HBASIS])
def riemann(k, h, mu, nu, rho, sigma):
return (k[sigma]*k[nu]*h[mu, rho]
+ k[rho]*k[mu]*h[nu, sigma]
- k[rho]*k[nu]*h[mu, sigma]
- k[sigma]*k[mu]*h[nu, rho])/2
def curvature_map(k):
return s.Matrix([[riemann(k, h, *PAIRS[a], *PAIRS[b])
for h in HBASIS] for a, b in CURV])
def covariant_numerator():
# Pi_{mn,ab}=1/2(eta_ma eta_nb+eta_mb eta_na-eta_mn eta_ab).
return s.Matrix.hstack(*(
coordinates(ETA*h*ETA-ETA*s.trace(ETA*h)/2) for h in HBASIS))
def spatial_data(p):
r2 = (p.T*p)[0]
b = s.Matrix.hstack(*(h*p for h in SBASIS))
tr = s.Matrix([1, 1, 1, 0, 0, 0])
v = b.T*p
kp = s.eye(6)-tr*tr.T/2
kq = r2*(s.eye(6)-tr*tr.T)-2*b.T*b+tr*v.T+v*tr.T
c = s.expand(kq*kp*kq)
embedded = []
for h in SBASIS:
hh = s.zeros(4)
hh[1:4, 1:4] = h
embedded.append(coordinates(hh))
return r2, c, s.Matrix.hstack(*embedded)
def on_cone_zero(matrix, omega, r2):
modulus = s.Poly(omega**2-r2, omega)
return all(s.Poly(s.expand(v), omega).rem(modulus).is_zero for v in matrix)
def curvature_tensor_action(lorentz):
wedge = s.Matrix([
[lorentz[mu, a]*lorentz[nu, b]-lorentz[mu, b]*lorentz[nu, a]
for a, b in PAIRS] for mu, nu in PAIRS])
columns = []
for a, b in CURV:
tensor = s.zeros(6)
tensor[a, b] = tensor[b, a] = 1
transformed = wedge*tensor*wedge.T
columns.append(s.Matrix([transformed[i, j] for i, j in CURV]))
return s.Matrix.hstack(*columns)
def universal_checks():
omega, x, y, z = s.symbols('omega x y z', real=True)
p = s.Matrix([x, y, z])
k = s.Matrix([-omega, x, y, z])
a = curvature_map(k)
pi = covariant_numerator()
r2, c, embed = spatial_data(p)
kernel = s.expand(a*pi*a.T)
check('covariant metric numerator is symmetric but indefinite',
pi == pi.T and pi.det() != 0
and pi.eigenvals() == {-1: 4, 1: 6})
for j in range(4):
xi = s.eye(4)[:, j]
check(f'curvature annihilates arbitrary pure gauge column {j}',
zero(a*coordinates(k*xi.T+xi*k.T)))
check('kernel has homogeneous degree four and no momentum denominators',
all(v == 0 or s.Poly(v, omega, x, y, z).is_homogeneous
and s.Poly(v, omega, x, y, z).total_degree() == 4
for v in kernel))
defect = s.expand(a*(r2**2*pi-embed*c*embed.T)*a.T)
check('all 441 null-cone entries: A Pi A^T equals A P_TT A^T',
on_cone_zero(defect, omega, r2))
check('must-fail: same identity is false away from the null cone',
not zero(defect.subs({omega: 2, x: 0, y: 0, z: 1})))
trace = coordinates(ETA)
wrong = s.expand(a*(pi+trace*trace.T/2)*a.T-kernel)
check('must-fail: omitting trace reversal changes the null curvature kernel',
not zero(wrong.subs({omega: 1, x: 0, y: 0, z: 1})))
# Algebraic and differential identities checked on each of 10 metric bases.
check('Riemann antisymmetries and pair interchange for all metric columns',
all(zero(riemann(k,h,m,n,r,t)+riemann(k,h,n,m,r,t))
and zero(riemann(k,h,m,n,r,t)+riemann(k,h,m,n,t,r))
and zero(riemann(k,h,m,n,r,t)-riemann(k,h,r,t,m,n))
for h in HBASIS for m,n in PAIRS for r,t in PAIRS))
check('algebraic Bianchi identity for all metric columns and tensor indices',
all(zero(riemann(k,h,m,n,r,t)+riemann(k,h,m,r,t,n)
+riemann(k,h,m,t,n,r))
for h in HBASIS for m in range(4) for n in range(4)
for r in range(4) for t in range(4)))
check('differential Bianchi identity for all curvature columns',
all(zero(k[u]*riemann(k,h,m,n,r,t)
+k[r]*riemann(k,h,m,n,t,u)
+k[t]*riemann(k,h,m,n,u,r))
for h in HBASIS for m,n in PAIRS for u in range(4)
for r,t in PAIRS))
ricci = s.Matrix([
[sum(ETA[mu,mu]*riemann(k,h,mu,nu,mu,sigma)
for mu in range(4)) for h in HBASIS]
for nu in range(4) for sigma in range(4)])
check('on-cone Ricci tensor annihilates the whole TT range',
on_cone_zero(s.expand(ricci*embed*c), omega, r2))
electric = s.Matrix([[riemann(k,h,0,i+1,0,j+1)
for h in HBASIS] for i,j in SPATIAL])
normalization = s.diag(1,1,1,s.sqrt(2),s.sqrt(2),s.sqrt(2))
electric = normalization*electric
check('electric curvature R_0i0j is omega^2 q_ij/2 in radiation gauge',
zero(electric*embed-omega**2*s.eye(6)/2))
check('null electric covariance is exactly one quarter of Round 6 C',
on_cone_zero(s.expand(electric*pi*electric.T-c/4), omega, r2))
# W(x,y) has phase exp(-i omega (t_x-t_y)); differentiate y for <R dot R>.
delay = s.symbols('delay', real=True)
scalar_w = s.exp(-s.I*omega*delay)/(2*omega)
check('second-argument Wightman derivative fixes positive mixed sign',
s.simplify((-s.diff(scalar_w, delay)).subs(delay, 0)) == s.I/2)
check('two Wightman time derivatives fix positive derivative covariance',
s.simplify((-s.diff(scalar_w, delay, 2)).subs(delay, 0)) == omega/2)
check('mixed electric-time covariance equals i C/8 on the cone',
on_cone_zero(s.expand(s.I*electric*pi*electric.T/2-s.I*c/8), omega, r2))
return pi
def fibre_and_covariance_checks(pi):
for values in ((1,0,0,1),(3,1,2,2),(7,-2,3,6),(s.Rational(5,3),1,0,s.Rational(4,3))):
w,x,y,z = values
k = s.Matrix([-w,x,y,z])
a = curvature_map(k)
kernel = s.simplify(a*pi*a.T)
r2,c,embed = spatial_data(s.Matrix([x,y,z]))
ptt = c/r2**2
factor = s.simplify(a*embed*ptt)
check(f'exact positive factorization at null fibre {values}',
zero(kernel-factor*factor.T))
check(f'exact two physical curvature polarizations at fibre {values}',
kernel.rank() == 2 and factor.rank() == 2)
boost = s.eye(4)
boost[0,0] = boost[1,1] = s.Rational(5,3)
boost[0,1] = boost[1,0] = -s.Rational(4,3)
k = s.Matrix([-3,1,2,2])
action = curvature_tensor_action(boost)
a = curvature_map(k)
transformed_a = curvature_map(boost*k)
check('rational boost preserves eta and future null energy',
boost*ETA*boost.T == ETA and -(boost*k)[0] > 0
and ((boost*k).T*ETA*(boost*k))[0] == 0)
check('all 441 curvature kernel entries obey nontrivial boost covariance',
zero(transformed_a*pi*transformed_a.T-action*a*pi*a.T*action.T))
def little_group_checks():
k = s.Matrix([-1,0,0,1])
a = curvature_map(k)
plus = s.diag(0,1,-1,0)/s.sqrt(2)
cross = s.zeros(4)
cross[1,2] = cross[2,1] = 1/s.sqrt(2)
u,v = s.symbols('u v', real=True)
q = (u*u+v*v)/2
null_rotation = s.Matrix([[1+q,-u,-v,q],[-u,1,0,-u],
[-v,0,1,-v],[-q,u,v,1-q]])
check('all-parameter null rotations preserve eta and the reference momentum',
zero(null_rotation*ETA*null_rotation.T-ETA)
and zero(null_rotation*k-k))
for name,h in (('plus',plus),('cross',cross)):
check(f'null little-group translations act trivially on {name} curvature',
zero(a*coordinates(null_rotation*h*null_rotation.T-h)))
t = s.symbols('t', real=True)
cosine, sine = (1-t*t)/(1+t*t), 2*t/(1+t*t)
rotation = s.eye(4)
rotation[1:3,1:3] = s.Matrix([[cosine,-sine],[sine,cosine]])
pol = s.Matrix.hstack(coordinates(plus),coordinates(cross))
h_action = s.Matrix.hstack(coordinates(rotation*plus*rotation.T),
coordinates(rotation*cross*rotation.T))
double = s.Matrix([[cosine*cosine-sine*sine,-2*cosine*sine],
[2*cosine*sine,cosine*cosine-sine*sine]])
check('all-angle TT rotation has exactly spin-two double-angle action',
all(s.cancel(v) == 0 for v in h_action-pol*double))
for sign in (-1,1):
vector = s.Matrix([1,sign*s.I])
phase = (cosine-sign*s.I*sine)**2
check(f'circular curvature polarization has helicity {2*sign:+d}',
all(s.cancel(v) == 0 for v in double*vector-phase*vector))
def run() -> int:
global FAILED
reset()
CHECKS.clear()
FAILED = 0
started = time.perf_counter()
pi = universal_checks()
fibre_and_covariance_checks(pi)
little_group_checks()
print(json.dumps({'status':'PASS' if FAILED == 0 else 'FAIL',
'exact_checks':len(CHECKS),
'elapsed_seconds':time.perf_counter()-started,
'claim':'free covariant curvature extension only',
'checks':CHECKS}, indent=2))
return summary("v1032 covariant curvature")
if __name__ == '__main__':
raise SystemExit(run())
Recorded source fingerprint
2ba2ff1636eb1f712705d1b50b9e1be703597271d40209e6fb7ecf1ad099aefb
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