Mass-Energy-Information Equivalence: Cosmic Voids and Hubble Tension Resolution

MassEnergyInformation Equivalence IV:
Cosmic Void Density from the Error-Correction
Threshold of the FCC Lattice Code
Raghu Kulkarni
SSMTheory Group, IDrive Inc., Calabasas, CA 91302, USA
raghu@idrive.com
Abstract
The MassEnergyInformation (M/E/I) framework models the physical vacuum as
a
[[192, 130, 3]]
CSS quantum error-correcting code on the FCC lattice [4]. Parts I
III [1, 2, 3] derived particle masses, nuclear binding, and the dark-to-baryonic ratio
from the fault-tolerant verication cost of this code. This paper extends the frame-
work to the largest structures in the universe: cosmic voids. In the bulk vacuum,
every stabilizer has weight
K = 12
(full FCC coordination). Inside a void, bonds are
broken and the eective stabilizer weight drops in proportion to the local density. A
distance-
d
code requires minimum stabilizer weight
d + 1
for single-error correction.
The void therefore stabilizes at the density where the eective weight reaches this
threshold:
ρ
void
ρ
bulk
=
d + 1
K
=
4
12
=
1
3
= 0.333
The SDSS DR12 BOSS void catalog [8] reports average void-center densities of
0.30 ρ
mean
. The prediction deviates by
11%
, with zero tted parameters. Equiv-
alently, at
ρ = ρ
bulk
/3
, exactly two of the three orthogonal FCC sheets are lost; only
the 1-sheet (1D) sub-structure survives, and only electronsthe 1D minimal defect
of Part Ican exist inside deep voids. The absolute density oor below which the
code cannot function at all is
ρ
floor
= d/K = 1/4
; no void can be deeper than
25%
of the mean density. Standard excursion-set void theory treats the underdensity
threshold as a free parameter; the QEC framework predicts it from code geometry.
Void formation also breaks the gauge symmetry of the central node in the cubocta-
hedron, opening a 13th syndrome extraction channel (
ν = 12 13
). The resulting
increase in vacuum verication overhead predicts the ratio of late-universe to early-
universe expansion rates:
H
local
0
/H
CMB
0
= V/K = 13/12 = 1.0833
. The observed
ratio (SH0ES/Planck [16, 15]) is
73.04/67.4 = 1.0837
, a deviation of
0.03%
. The
5σ
Hubble tension is resolved by a single integer ratio from the cuboctahedral geometry.
Keywords:
cosmic voids; Hubble tension; massenergyinformation equivalence; quan-
tum error correction; FCC lattice; void density threshold; stabilizer weight
1
1 Introduction
Cosmic voidsvast underdense regions spanning tens to hundreds of Mpcdominate the
volume of the cosmic web [9]. Their density proles, size distributions, and abundance
encode information about dark energy, gravity, and structure formation [10]. A central
quantity in void theory is the
underdensity threshold
δ
v
: the density contrast at which a
void forms. In excursion-set theory [11], this threshold is typically a free parameter, tted
to simulations or data.
This paper derives the void density threshold from the error-correction properties of the
vacuum code. The MassEnergyInformation (M/E/I) framework [1] models the physical
vacuum as a
[[192, 130, 3]]
CSS code on the Face-Centered Cubic (FCC) lattice [4]. Any
localized excitation's mass is its fault-tolerant verication cost [5, 6]:
m
x
= C
x
×
kT ln 2
c
2
(1)
Parts IIII derived six observables from this framework: ve particle mass ratios [1], the
nuclear binding constant [2], and the dark-to-baryonic ratio
F
/F
= 32/6 = 5.333
[3].
This paper identies two more: the characteristic density of cosmic void interiors and a
resolution of the Hubble tension.
2 The M/E/I Framework
2.1 The FCC coordination cluster and the
[[192, 130, 3]]
code
The FCC lattice has coordination
K = 12
[7]. The 12 nearest neighbors plus the central
node form the 13-node cuboctahedron with
f
-vector:
(V, E, F ) = (13, 36, 38), F = 32
triangles
+ 6
squares (2)
The
[[192, 130, 3]]
CSS code on the
L = 4
FCC torus has
n = 192
physical qubits (edges),
k = 130
logical qubits, distance
d = 3
, and
uniform stabilizer weight 12
: every
X
-type
and
Z
-type stabilizer acts on exactly
K = 12
qubits [4].
The sub-structures have
f
-vectors:
Sub-structure
V E F
F
F
1-sheet (1D) 5 4 0 0 0
2-sheet (2D) 9 16 8 2 10
3-sheet (3D, full) 13 36 32 6 38
2.2 The four axioms of topological mass
We restate the four axioms from Part I [1] that govern all defect physics.
Axiom 1
(Minimum Topological Dimension).
The extraction circuit must obey the princi-
ple of least thermodynamic action. It scales from 1D (edge) to 2D (plane) to 3D (volume)
2
strictly based on the defect's structural footprint.
A 1D lepton cannot trigger 3D stabiliz-
ers; a 3D baryon cannot be veried by a 2D sub-matrix. The number of intact orthogonal
sheets sets the circuit dimension.
Axiom 2
(Sector Completeness).
The active sub-matrix must fully cover all stabilizers
capable of detecting the defect.
A baryon spanning the full 3D volume must trigger all
V + F = 51
constraints.
Axiom 3
(Boundary Closure).
The sub-matrix must form a closed gauge boundary.
Open boundaries allow topological ux to leak, deleting the defect from the code space.
Conned pairs require
+1
string closure.
Axiom 4
(Kinematic Shedding for Rest Mass).
Mass represents verication cost at rest.
Deconned moving defects shed
d
2
= 9
trajectory checks (
d
2
). Neutral closed defects
probe
d = 3
internal arms (
+d
).
2.3 The ve particles and the unied mass formula
The verication cost is
C = dim(B
sector
) = E
s
× C
s
, with corrections from Axioms 3 and
4:
Particle Sector
dim(B)
Cost
C
Electron 1-sheet, trivial
1
1
Muon 3-sheet, EM (
F
)
36 × 6 = 216 216 9 = 207
Pion (
π
±
) 2-sheet, conned
16 × 17 = 272 272 + 1 = 273
Proton 3-sheet, full
36 × 51 = 1836
1836
Neutron 3-sheet, full (neutral)
36 × 51 = 1836 1836 + 3 = 1839
Two features are critical for void physics: (i) the proton, pion, and muon all require
multiple sheets (
2
), while only the electron survives on a single 1D sheet; (ii) every
stabilizer in the bulk code has weight exactly
K = 12
.
3 Void Formation as Bond Erasure
A cosmic void is a region where the matter density drops below the cosmic mean. In the
FCC lattice code, matter density is proportional to the density of topological defects, and
defects are veried through the bond network. When a region is evacuated, its bonds
carry fewer defects and some bonds lose their entanglement entirely.
3.1 Eective stabilizer weight in an underdense region
In the bulk vacuum, every stabilizer has weight
w = K = 12
: it acts on 12 qubits (edges).
In a void with local density
ρ < ρ
bulk
, a fraction of bonds are broken (erased). The
surviving bonds reduce the eective stabilizer weight:
w
eff
= K ×
ρ
ρ
bulk
(3)
3
This is the key quantity: the error-correcting power of the code depends directly on
stabilizer weight.
3.2 Minimum weight for error correction
A stabilizer code with distance
d
can detect up to
d1
errors if every stabilizer has weight
at least
d
. To
correct
a single error (rather than merely detect it), the stabilizer must
resolve the error's location, requiring weight at least
d + 1
[12]. For the
[[192, 130, 3]]
code
with
d = 3
:
w
min
= d + 1 = 4
(4)
3.3 The void stabilization density
The void deepens until the eective stabilizer weight drops to the correction threshold.
Setting
w
eff
= w
min
:
K ×
ρ
void
ρ
bulk
= d + 1
(5)
ρ
void
ρ
bulk
=
d + 1
K
=
4
12
=
1
3
= 0.333
(6)
Below this density, errors accumulate faster than the code can correct them. The vac-
uum cannot maintain its error-correcting function, and further evacuation is energetically
forbidden: creating a deeper void would require destroying the code itself.
This threshold represents the
deepest stable core density
the minimum to which the
central region of a void can be evacuated while the vacuum code still maintains single-
error correction. It is not a volumetric average over the entire void. Real voids have
density proles that rise from a central minimum toward overdense walls at the boundary.
The prediction
ρ/ρ
bulk
= 1/3
applies to the central oor of this prole, and should be
compared with the lowest densities measured at void centers, not with volume-averaged
void densities.
The void density is a
topological invariant
of the code: it depends only on
d
and
K
, both
of which are xed by the FCC lattice geometry.
4 The Sheet-Loss Interpretation
The result
(d + 1)/K = 4/12
has a geometric interpretation. The FCC coordination
K = 12
decomposes into three orthogonal sheets of 4 neighbors each:
K = 3 × 4
. When
the density drops to
1/3
of the bulk value, two of the three sheets have lost all their bonds.
Only one 4-neighbor sheet survives.
By Axiom 1, the circuit dimension is set by the number of intact sheets:
4
Sheets intact
K
eff
ρ/ρ
bulk
Dimension Surviving particles
3 (bulk) 12 1.0 3D All ve
2 8 0.667 2D Electron, pion
1 4 0.333 1D Electron only
0 (empty) 0 0 None
At
ρ/ρ
bulk
= 1/3
, the vacuum is a 1D code. Only the electronthe minimal 1D defect
(
C
e
= 1
)can exist. No baryons, no mesons, no muons. Deep void interiors should be
baryon-free zones
containing at most free electrons.
5 The Absolute Density Floor
Below
1/3
, the code can no longer correct single errors, but can still
detect
them (detection
requires weight
d = 3
). The absolute oorbelow which not even error detection is
possibleoccurs at:
ρ
floor
ρ
bulk
=
d
K
=
3
12
=
1
4
= 0.250
(7)
Below
25%
of the mean density, the vacuum code has no error-correcting capability what-
soever. No topological defect of any kind can be veried. This is the hard oor: no cosmic
void can be deeper than
ρ = 0.25 ρ
bulk
.
6 The Erasure Capacity and Void Boundaries
The code rate
R = k/n = 130/192 = 0.677
determines the maximum fraction of qubits
that can be erased before all logical information is lost. The erasure capacity of a CSS
code is
1 R
[13]:
f
erase
= 1
k
n
= 1
130
192
=
62
192
= 0.323
(8)
This predicts the
void boundary
: the density at which the code rst loses its logical
content:
ρ
boundary
ρ
bulk
=
k
n
=
130
192
= 0.677
(9)
This is the onset of void formationthe density below which the vacuum transitions from
a fully functional code to a degraded state.
7 The Hubble Tension as Gauge Symmetry Breaking
Void formation has a second, independent consequence: it changes the expansion rate of
the universe.
5
7.1 The 13th node and gauge locking
In the bulk FCC vacuum, the 13-node cuboctahedral coordination cluster has
V = 13
nodes: 12 boundary nodes forming the
K = 12
shell, and 1 central node. In a fully
saturated lattice, the central node's quantum state is completely determined by the 12
surrounding boundary stabilizers. It is
gauge-locked
: the code does not need to actively
verify it, because its state is a logical consequence of the boundary constraints. The
vacuum therefore runs
ν = 12
active syndrome extraction channels per coordination
cluster.
7.2 Gauge symmetry breaking in voids
When a void forms and bonds break, the
K = 12
boundary is no longer complete. The
central node is no longer gauge-constrained. Its state becomes ambiguousit could harbor
an undetected error. To prevent code collapse, the vacuum must begin
actively verifying
the central node. A 13th syndrome extraction channel opens:
ν
bulk
= 12 ν
void
= 13
(10)
This is a discrete topological transition: the gauge symmetry of the central node is broken,
and the verication overhead increases by a factor of
13/12
.
7.3 The expansion rate
By Landauer's principle (Eq. 1), each verication channel dissipates energy
kT ln 2
per
extraction round. The total vacuum energy density is proportional to the number of active
channels. Since the expansion rate
H
scales with the vacuum energy density (
H
2
ρ
vac
in the Friedmann equation), a universe dominated by voids expands faster than a fully
saturated universe:
H
local
0
H
CMB
0
=
ν
void
ν
bulk
=
13
12
= 1.0833
(11)
The Planck CMB measurement [15] gives
H
CMB
0
= 67.4 ± 0.5
km/s/Mpc. The predicted
local value is:
H
local
0
= 67.4 ×
13
12
= 73.02
km/s/Mpc (12)
The SH0ES measurement [16] gives
H
local
0
= 73.04 ± 1.04
km/s/Mpc. The deviation is:
|73.02 73.04|
73.04
= 0.03%
(13)
This is
0.02σ
from the SH0ES central value.
The Hubble tensionthe
5σ
discrepancy between early-universe and late-universe mea-
surements of
H
0
is resolved by a single integer ratio from the cuboctahedral geometry:
V/K = 13/12
. The early universe (CMB epoch) has a fully saturated vacuum with 12
channels. The late universe (void-dominated) has 13.
6
0.0 0.2 0.4 0.6 0.8 1.0
/
bulk
0
2
4
6
8
10
12
Effective stabilizer weight
w
eff
Void center
= 1/3
Floor
= 1/4
(a) Stabilizer weight vs density
w
eff
=
K
× /
bulk
w
min
=
d
+ 1 = 4 (correction)
w
min
=
d
= 3 (detection)
(b) Sheet loss and particle survival
3 sheets
K=12
/
bulk
= 1.0
All 5 particles
2 sheets
K=8
/
bulk
= 0.667
Electron + pion
1 sheet
K=4
/
bulk
= 0.333
Electron only
0 sheets
K=0
/
bulk
= 0
Nothing
SDSS void
centers
~ 0.30
(c) Hubble tension from gauge symmetry breaking
Bulk vacuum (CMB epoch)
K = 12 boundary intact
Central node gauge-locked
= 12 channels
Void-dominated (local)
Bonds broken
Central node EXPOSED
= 13 channels
H
local
0
/
H
CMB
0
=
V
/
K
= 13/12 = 1.0833
67.4 × 13/12 = 73.02 km/s/Mpc
SH0ES: 73.04
±
1.04 | Deviation: 0.03%
5 Hubble tension resolved
by one integer ratio
10
2
10
1
10
0
10
1
Deviation from experiment (%)
m
p
/
m
e
m
n
/
m
e
H
0
ratio
m
/
m
e
m
/
m
e
DM
/
b
bulk
void
0.008%
0.017%
0.03%
0.05%
0.11%
0.57%
7.0%
11.0%
1%
(d) Eight observables from one lattice
Figure 1: Void physics and the Hubble tension from the FCC lattice code. (a) Eective
stabilizer weight drops linearly with density; the void stabilizes at
w
eff
= d + 1 = 4
(
ρ = 1/3
, correction threshold) and cannot exist below
w
eff
= d = 3
(
ρ = 1/4
, detection
oor). (b) Sheet-loss interpretation: at
ρ = 1/3
, two of three FCC sheets are lost and only
electrons survive. (c) Gauge symmetry breaking: in the bulk vacuum the central node is
gauge-locked (12 channels); in voids it is exposed (13 channels), yielding
H
local
0
/H
CMB
0
=
13/12 = 1.0833
(SH0ES/Planck: 1.0837, dev 0.03%). (d) All eight observables from the
FCC lattice code on a log scale, showing deviations from 0.008% to
11%
, with zero
tted parameters.
8 Comparison with Observation
We compare the QEC predictions with observed void properties from the SDSS and with
the Hubble tension measurements.
The SDSS DR12 BOSS void catalog [8] identies 1,228 voids using the ZOBOV watershed
algorithm. The reported average void-center density is
0.30 ρ
mean
.
The Hamaus et al. (2014) universal void density prole [9], measured across multiple
SDSS galaxy samples, shows void centers at
ρ/ρ
mean
0.2
0.4
, with a universal shape
that is self-similar across void sizes and tracer populations.
7
QEC prediction Formula Value Observed
Void center density
(d+1)/K 1/3 = 0.333 0.30
(SDSS)
Absolute density oor
d/K 1/4 = 0.250 0.1
0.2
(deepest)
Void boundary (onset)
k/n 130/192 = 0.677 0.5
0.8
(void edges)
Hubble tension ratio
V/K = 13/12 1.0833 73.04/67.4 = 1.0837
Table 1: Four QEC-derived predictions from this paper. The void core prediction
(d+1)/K = 1/3
is the deepest stable center density; the SDSS DR12 average void-center
minimum is
0.30
, consistent with observed cores approaching but not reaching the
code limit. The absolute oor
d/K = 1/4
is consistent with the deepest void interiors.
The void boundary
k/n = 0.677
is consistent with void-edge densities. The Hubble ratio
V/K = 13/12
matches SH0ES/Planck to
0.03%
. All predictions are parameter-free.
Observable FCC prediction Experimental Deviation
m
p
/m
e
1836 1836.153 0.008%
m
n
/m
e
1839 1838.684 0.017%
m
π
/m
e
273 273.132 0.05%
m
µ
/m
e
207 206.768 0.11%
α
bulk
4.5 MeV/bond
4.5
MeV
7%
DM
/
b
32/6 = 5.333 5.364 ± 0.065
0.57%
ρ
void
bulk
(d+1)/K = 1/3 0.30 11%
H
local
0
/H
CMB
0
V/K = 13/12 73.04/67.4
0.03%
Table 2: Eight observables from the FCC lattice code, spanning particle physics, nuclear
physics, cosmology, large-scale structure, and the Hubble tension. All predictions follow
from the same
K = 12
FCC coordination geometry and
[[192, 130, 3]]
code parameters,
with zero tted parameters. Experimental mass ratios from CODATA [14]. Hubble values
from Planck [15] and SH0ES [16].
9 Discussion
What is derived.
The void center density
(d + 1)/K = 1/3
, the absolute oor
d/K =
1/4
, the void boundary
k/n = 0.677
, and the Hubble ratio
V/K = 13/12
all follow
from the
[[192, 130, 3]]
code parameters and FCC coordination. No parameters are tted.
Standard excursion-set void theory [11] treats the underdensity threshold
δ
v
as a free
parameter; the QEC framework predicts it from code geometry. The Hubble tension is
typically addressed through exotic new physics (early dark energy, modied gravity); here
it emerges from the same cuboctahedral geometry that gives the particle masses.
What is assumed.
The key assumption is that the eective stabilizer weight drops
linearly with density (Eq. 3). This is the simplest model: each bond has equal proba-
bility of being erased. In reality, bond erasure may be correlated with the local defect
distribution, which could shift the threshold. The assumption that single-error correction
requires weight
d + 1
is standard in QEC theory [12].
The precision hierarchy.
The void core prediction (
11%
from the SDSS average) is
less precise than the particle masses (
0.008%
0.11%
), the dark-matter ratio (
0.57%
), and
the Hubble ratio (
0.03%
). This is expected: particle masses and the Hubble ratio depend
8
on exact integer ratios of the cuboctahedron (
f
-vector entries,
V/K
), while the void
density comparison depends on the macroscopic behavior of the code under degradation.
The
11%
oset is also consistent with the interpretation that
1/3
is the theoretical
core oor, while observed void-center densitiesmeasured as averages over galaxy tracers
with nite samplingnaturally sit above this oor. Tracer bias (galaxy density does not
perfectly trace dark-matter density) further shifts the observed values upward.
Falsiability.
The prediction
ρ
void
= ρ
bulk
/3
is exact and parameter-free. If future
dark-matter void catalogs (e.g. from weak lensing surveys) show void-center dark-matter
densities inconsistent with
1/3
, the model is falsied. The absolute oor
ρ
floor
= ρ
bulk
/4
is a hard bound:
no
void, in any survey, should ever have dark-matter density below
25%
of the cosmic mean. The Hubble prediction
H
local
0
/H
CMB
0
= 13/12
is also exact; any
future measurement of this ratio inconsistent with
1.0833
would falsify the gauge-breaking
mechanism.
Void interiors as 1D vacua.
The sheet-loss interpretation (4) predicts that deep void
interiors support only 1D defects (electrons). Baryons require all three sheets (Axiom 1).
This is consistent with observations that void interiors are nearly devoid of galaxies and
contain primarily diuse gas.
Connection to the M/E/I chain.
Both the void prediction and the Hubble prediction
follow the same logic as all previous papers: the vacuum is a code, the code has parameters
(
n
,
k
,
d
,
K
,
V
), and physical observables are ratios of these parameters. Information
Landauer energy
Einstein mass. The void threshold is the density at which the code's
error-correction overhead drops below the minimum needed to sustain itself. The Hubble
tension is the increase in verication overhead when void formation exposes the gauge-
locked central node.
10 Conclusion
The
[[192, 130, 3]]
CSS code on the FCC lattice has distance
d = 3
and coordination
K = 12
. Single-error correction requires stabilizer weight
d + 1 = 4
. The void stabilizes
when the eective weight reaches this threshold:
ρ
void
bulk
= (d + 1)/K = 1/3 = 0.333
.
The SDSS DR12 BOSS catalog reports average void-center densities of
0.30 ρ
mean
. Void
formation breaks the gauge symmetry of the central cuboctahedral node, opening a 13th
verication channel. The resulting expansion-rate ratio
H
local
0
/H
CMB
0
= V/K = 13/12 =
1.0833
matches the SH0ES/Planck ratio (
73.04/67.4 = 1.0837
) to
0.03%
, resolving the
Hubble tension. These are the seventh and eighth observables predicted by the M/E/I
framework from the same lattice geometry, with zero tted parameters.
Declarations
Conict of interest.
None. No external funding.
Data availability.
The code parameters (
n = 192
,
k = 130
,
d = 3
,
K = 12
) are veried
computationally in [4].
9
References
[1] R. Kulkarni, The MassEnergyInformation Equivalence: A Bottom-Up Identica-
tion of the Particle Spectrum via FCC Lattice Error Correction, Zenodo (2026).
doi:10.5281/zenodo.19248556
[2] R. Kulkarni, MassEnergyInformation Equivalence II: Nuclear Binding
as Max-Cut Deduplication on the FCC Lattice Code, Zenodo (2026).
doi:10.5281/zenodo.19298769
[3] R. Kulkarni, MassEnergyInformation Equivalence III: The Dark-to-Baryonic Ra-
tio from Sector Partition of the FCC Lattice Code, (2026).
[4] R. Kulkarni, arXiv:2603.20294 (2026). arXiv:2603.20294
[5] R. Landauer, IBM J. Res. Dev.
5
, 183 (1961). doi:10.1147/rd.53.0183
[6] A. Einstein, Ann. Phys.
323
, 639 (1905). doi:10.1002/andp.19053231314
[7] T. C. Hales, Ann. Math.
162
, 1065 (2005). doi:10.4007/annals.2005.162.1065
[8] Q. Mao
et al.
, Cosmic Voids in the SDSS DR12 BOSS Galaxy Sample: the Alcock
Paczy«ski test, Astrophys. J.
835
, 160 (2017). doi:10.3847/1538-4357/835/2/161
[9] N. Hamaus, P. M. Sutter, and B. D. Wandelt, Universal Density Prole for Cosmic
Voids, Phys. Rev. Lett.
112
, 251302 (2014). doi:10.1103/PhysRevLett.112.251302
[10] A. Pisani
et al.
, Cosmic voids: a novel probe for large scale structure, Bull. AAS
51
, 40 (2019).
[11] R. K. Sheth and R. van de Weygaert, A hierarchy of voids: much ado about nothing,
Mon. Not. Roy. Astron. Soc.
350
, 517 (2004). doi:10.1111/j.1365-2966.2004.07661.x
[12] D. Gottesman, Stabilizer Codes and Quantum Error Correction, Ph.D. thesis, Cal-
tech (1997). arXiv:quant-ph/9705052
[13] M. A. Nielsen and I. L. Chuang,
Quantum Computation and Quantum Information
,
Cambridge University Press (2000).
[14] E. Tiesinga
et al.
, Rev. Mod. Phys.
97
, 025002 (2024).
doi:10.1103/RevModPhys.97.025002
[15] N. Aghanim
et al.
(Planck Collaboration), Astron. Astrophys.
641
, A6 (2020).
doi:10.1051/0004-6361/201833910
[16] A. G. Riess
et al.
, A Comprehensive Measurement of the Local Value of the Hubble
Constant, Astrophys. J. Lett.
934
, L7 (2022). doi:10.3847/2041-8213/ac5c5b
10