
sources the Ricci tensor via the Einstein equation. Because both quantities count the same
disrupted bonds, inertial and gravitational mass are identically equal at the microscopic level.
No WEP violation is predicted.
6.4. Gravitational Wave Speed and Lorentz Invariance
Treating spacetime as a discrete lattice fundamentally challenges established experimental
physics due to the threat of Lorentz Invariance Violation (LIV). In standard discrete spaces,
the propagation speed of waves theoretically depends on their energy, as shorter wavelengths
interact more directly with the lattice grain. These effects have been rigorously tested by
modern astrophysics. Time-of-flight measurements of high-energy photons from Gamma-Ray
Bursts, most notably the observations of GRB 090510 by the Fermi Large Area Telescope
[9], constrain linear Lorentz invariance violation to energy scales exceeding the Planck mass.
This effectively rules out any naive discrete spacetime lattice with a spacing larger than
∼ 0.8l
P
.
Furthermore, the joint detection of GW170817 (gravitational waves) and GRB 170817A
(gamma-ray burst) constrains the relative speed of gravitational waves to |v
GW
−c|/c < 10
−15
[10].
In a standard Newtonian or Minkowskian lattice framework, a grain size of L ≈ 1.84l
P
would produce massive, observable energy-dependent delays, severely violating these bounds.
However, the SSM survives these observational constraints because the 3D bulk is an isomet-
ric holographic projection of the 2D boundary [3]. Because the boundary state maintains
exact continuous rotational and translational symmetry, the projected 3D bulk inherits exact
macroscopic Lorentz invariance at all energy scales.
In the SSM, gravitational waves are transverse strain oscillations of the FCC tensor net-
work. The maximum propagation speed of any disturbance is set by the bond transmission
rate, which is identical to the maximum speed of electromagnetic disturbances. Both gravita-
tional and electromagnetic waves propagate on the same lattice at the same maximum bond
speed. The SSM therefore predicts exactly zero energy-dependent dispersion and strictly en-
forces v
GW
= c, perfectly satisfying the Fermi LAT and LIGO/Virgo observational bounds.
6.5. Bekenstein-Hawking Entropy
The Bekenstein-Hawking entropy S
BH
= A/(4l
2
P
) [11] is automatically satisfied by the
SSM construction. Equation 2 counts the entanglement entropy as the number of severed
bonds times ln 2. The RT relation (Eq. 5) maps this to S = Area/(4G
N
). Since G
N
= l
2
P
in natural units, this recovers S = A/(4l
2
P
) identically. The bond-counting origin of entropy
provides a microscopic derivation of the Bekenstein-Hawking formula: the entropy counts the
number of entanglement bonds severed by the horizon surface, with each bond contributing
exactly ln 2.
6.6. The Anomalous Spread in G
N
Measurements
Laboratory measurements of G
N
exhibit an anomalous spread of approximately ±500 ppm
across different experimental groups [12], far exceeding the quoted individual uncertainties.
The SSM does not currently explain this discrepancy, as it predicts a single, exact value of
G
N
for a given L. The anomalous spread likely originates in systematic errors in the torsion-
balance experiments (material properties, metrology, vibration isolation) rather than in new
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