The vacuum-energy problem splits cleanly along Lorentz invariance. Lorentz-VIOLATING regulators (hard 3-momentum cutoff, spatial lattice) give w = +1/3 AND a quartic divergence; Lorentz-INVARIANT regulators (Pauli–Villars, dimensional regularisation) give w = −1 exactly AND no power divergence at all. The two columns are the same fact: a K⁴ term has no m⁴ to carry it, so it must be built from a regulator scale — and a Lorentz-invariant regulator has no preferred frame to build one from.
Sharpens the deflation found earlier: the famous huge number is an artifact of a Lorentz-breaking regulator. Two different 'hard cutoff' schemes even disagree on the K⁴ coefficient by a factor 1.94. What survives every scheme is the m⁴ log term — and its coefficient is scheme-independent to 8×10⁻¹⁶ across all three analytic regulators.
Falsify-box — how to kill this claim
Verification record — every quoted number, re-run 2026-07-26
| quantity | measured | verdict |
|---|---|---|
| hard 3-momentum cutoff | w = +1/3 exactly (T^μ_μ = 0 at m = 0 to 5.6e-17); quartic divergence PRESENT | MATCH |
| Pauli–Villars | w = −1 exactly (|w+1| = 1.3e-24 at 140 digits); no quartic divergence | MATCH |
| dimensional regularisation | w = −1 exactly at EVERY d, not just d → 4; only a log pole | MATCH |
| two hard cutoffs disagree | sphere cutoff vs lattice differ on the K⁴ coefficient by a factor 1.935 | MATCH |
| scheme-independent survivor | the m⁴ log coefficient agrees across all three analytic schemes to 7.9e-16 | MATCH |
| HONEST RESIDUAL from MEASURED masses | 10^54.7 × the observed density at μ = 1 GeV (top quark dominates at 10^54.8); adversarially tuning μ to cancel the top term buys only 2 of 55 decades | MATCH |
| the irreducible statement | dρ_Λ/dlnμ = 1.25e54 × ρ_obs per e-fold — no regulator choice touches this | MATCH |
Provenance
script status: PRESENT
datasets: information-seam-scripts (downloadable from /data — run it yourself)
re-run: 2026-07-26
Status, honestly
verified by adversarial re-run (workflow, 2026-07-26). Status here is computed from evidence — the author cannot set it, and neither can we. Independent reproduction would move it; nothing else will.
The founder's own run of this script, captured verbatim. A match proves the result is reproducible; it is still R0 on this registry's independence rings — same code, so it cannot move a status. Only an outside run does that.
125.25 1 -8.338342e+05 52.52
top quark 172.5 12 +2.523186e+07 54.00
------------------------------------------------------------------
SIGNED TOTAL +2.228655e+07 53.95
sum of |rho_i| +2.817716e+07 54.05
------------------------------------------------------------------
largest single term: top quark, |rho| = 2.5232e+07 GeV^4 = 10^54.00 rho_obs
*** THE SURVIVING DISCREPANCY ***
at mu = 1 GeV : |signed total| / rho_obs = 10^54.74
at mu = m_top : |signed total| / rho_obs = 10^53.95
change in the discrepancy across 2.24 decades of mu : 0.80 decades
THAT IS THE WHOLE mu-SENSITIVITY. Moving the renormalisation
scale by two and a bit decades moves the answer by LESS THAN
ONE decade, against a discrepancy of 55 decades. There is no
choice of mu -- none, not even an absurd one -- that brings the
measured-mass contributions anywhere near rho_obs.
ADVERSARIAL BEST CASE, COMPUTED RATHER THAN ASSERTED. Choose
mu by hand to make the LARGEST term vanish exactly: set
ln(m_top^2/mu^2) = 3/2, i.e. mu* = m_top exp(-3/4).
mu* = 81.4832 GeV
top-quark term at mu* = 3.735e-09 GeV^4 (zeroed)
signed total of everything else = -1.273623e+06 GeV^4
that residue / rho_obs = 10^52.70
sum of |terms| at mu* = 10^52.70 x rho_obs
Killing the single biggest contribution by fiat buys 2.0
decades out of 55. And it cannot be done for two particles
at once: one mu, seven masses.
Stated as running instead of as a value, which is the
scheme-independent way to say it (PART F):
d rho_Lambda / d ln mu = -sum_i (-1)^(2s) n_i m_i^4/(32 pi^2)
= +3.141356e+07 GeV^4 per e-fold
= 1.25e+54 x rho_obs per e-fold
The renormalised cosmological constant moves by 10^54 times
the entire observed dark-energy density when you shift the
renormalisation scale by ONE e-fold. No regulator choice
touches this: it is the log coefficient, and PART F showed all
three schemes agree on it.
HONESTY, EXPLICIT: this is a NATURALNESS statement, not an
inconsistency. The bare cosmological constant is a free
parameter and can absorb any finite number, so nothing above is a
failed PREDICTION of the Standard Model. What it is: the
observed value requires a cancellation to ~55 decimal places
between the bare parameter and terms computed from masses we have
measured in laboratories, and that cancellation has to be redone
by hand at every mass threshold. That is the problem, and PARTS
A-F establish that it is the ONLY part of the problem that
survives an honest regulator.
==============================================================================
VERDICT -- WHICH PART OF '10^120' IS A REGULATOR ARTEFACT
==============================================================================
*** NOTHING IN THIS FILE SOLVES THE COSMOLOGICAL CONSTANT
*** PROBLEM. NOTHING IN THIS FILE IS NEW. Every result is a
*** recomputation of Zel'dovich / Pauli-Villars / 't Hooft-
*** Veltman / Coleman-Weinberg / Akhmedov / Koksma-Prokopec.
ARTEFACT -- delete these and lose nothing:
1. THE QUARTIC DIVERGENCE. Present in both Lorentz-violating
regulators (hard cutoff: 0.006333 K^4; lattice: 1.193801/a^4)
and in NEITHER Lorentz-invariant one. The two Lorentz-
violating schemes do not even agree with each other on the
coefficient -- they differ by a factor of 1.94.
2. THE HEADLINE NUMBER ITSELF. '10^120' is (cutoff)^4 divided
by rho_obs. Both the cutoff and the quartic power are
supplied by the scheme. In dim reg there is no such term to
compute, so there is no 10^120 and, correspondingly, no
'120 digits of cancellation' to explain. The famous
fine-tuning COUNT is a property of a bad regulator.
3. THE OBJECT ITSELF. The hard-cutoff mode sum returns
w = +0.333333 -- a radiation bath. It is not a cosmological
constant at all. A calculation whose answer has the wrong
equation of state has not computed the quantity in dispute.
PHYSICAL -- no regulator choice removes these:
1. THE m^4 LOG TERM. Its coefficient, -1/(32 pi^2) per e-fold,
is identical in hard cutoff, Pauli-Villars and dimensional
regularisation (PART F, verified to ~1e-15 relative). It is
an RG running, and runnings are scheme independent.
2. THE MEASURED-MASS RESIDUAL. Evaluated in the clean scheme
for the electron, muon, tau, W, Z, Higgs and top, it
overshoots rho_obs by 10^54.7 (mu = 1 GeV) or 10^53.9
(mu = m_top). Two decades of mu move it by 0.8 decades.
Equivalently: the renormalised Lambda moves by 1e+54 times
rho_obs per e-fold of mu. Nothing here is assumed about
physics above the electroweak scale. There is no cutoff in
PART G at all.
SO THE SUMMARY SENTENCE IS: fixing the regulator deletes the
famous number and leaves the problem. The vacuum-energy problem
is not 'why is 10^120 not 1'; it is 'why does a sum of terms of
order m_top^4/(16 pi^2) -- computed from measured masses, in a
scheme with no arbitrary cutoff, with the right equation of state
-- come out 55 orders of magnitude smaller than each of its
own terms'. That question is smaller, sharper, and completely
unsolved.
WHAT THIS DOES NOT ESTABLISH (stated because the temptation is
real):
* It does NOT show the vacuum energy is small, or zero, or
calculable. It shows the standard estimate of its SIZE is
scheme-dependent, and then computes a scheme-INdependent
lower bound on the tuning that is still 55 decades.
* It does NOT show that zero-point energy gravitates. That is
the actual open question (wave 3, VERDICT) and no computation
decides it.
* The w = -1 results here are properties of a REGULATOR, not
measurements of nature. Whether the dark energy actually has
w = -1 is an empirical question handled in Test 15
(is_the_vacuum_constant.py), not here.
* No number in this file is a significance. Every small
residual quoted (1e-16, 1e-24, 1e-51) is either a truncation
of a physical limit or a floor of the arithmetic, and each
one is laddered in the output so the reader can see which.
None of them measures how well nature obeys anything.
* The four-regulator table is about SCHEMES, i.e. about our
bookkeeping. It is not a survey of candidate physics. The
only part of this file that touches nature is PART G, and
PART G is where the problem is.
STATUS: REPRODUCED, NOT DISCOVERED. SOLVES NOTHING.
==============================================================================
This script needs data files, a heavy dependency, or more time than a browser tab should take. Download it from /data and run it locally.