Q.C. Zhang Twistor Configuration Geometry
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Empirical Posture of the TCG Spin-1 Short-Range Force: Bound Overlay and Astrophysical Viability

Standalone short empirical-posture companion to the Predictions and No-Go consequences note. Anchors the cleanly surviving region λ ≲ 7–8 μm, m ≳ 25–28 meV to primary-source laboratory bounds (Geraci 2008 microcantilever |α| > 14,000 excluded at λ = 10 μm; Blakemore 2021 levitated microsphere |α| ≳ 10⁸ for λ > 10 μm; Venugopalan 2026 optomechanical vector sensing |α| ~ 10⁷ at λ ≃ 5 μm with ~100× improvement). Coupling translation g_X² = 4πGm_X²α_Y/(ℏc) yields TCG-required gauge couplings g_B ≈ 3.7×10⁻¹⁷ (baryon), g_e ≈ 2.0×10⁻²⁰ (electron), kinetic-mixing equivalent ε ≈ 6.7×10⁻²⁰. Documents structural protection from SN 1987A, red-giant cooling, BBN/CMB thermalization, and long-range EP exclusion by 7–10 orders of magnitude in representative vector and effective-mixing channels at the gravity-normalized coupling scale. Operator-coupling status: P_6 fixes spin s = 1 and strength α_Y = α⁻² but does NOT derive the operator coupling J^μ_Y. Spin-independent Yukawa searches (Channel A: mass, number, B−L currents) test the TCG prediction directly; spin-dependent searches (Channel B: spin or axial currents) are exploratory adjacent tests outside the TCG falsification chain unless a TCG-internal operator derivation is supplied. P_Y^op is named as a diagnostic empirical-posture bookkeeping label, NOT a new active-ledger residual, NOT an extension of the four-arc named-residual pattern. Only viable falsification path is direct short-range laboratory measurement in the cleanly surviving window. Six failure modes F1–F6 guard the common overreach drifts. Introduces NO new TCG postulate, NO new active-ledger residual, NO operator-coupling derivation, NO experimental protocol, NO claim of detection. Maturity register: predictions-and-no-go successor / empirical-posture consolidation, distinct from theorem-level construction/obstruction notes and from the synthesis review. Active TCG/τCG postulate ledger UNCHANGED.

Published
DOI 10.5281/zenodo.20738542

Abstract

The Predictions and No-Go consequences note identifies a spin-1 short-range mediator with effective Yukawa strength αYα21.88×104\alpha_Y \equiv \alpha^{-2} \approx 1.88 \times 10^4 relative to gravity — fixed by the integer-spin tower postulate P6P_6 of the TCG Construction (FPA Model) and normalized against the gravitational sector of Emergent Gravity — as the principal forward-falsifiable empirical prediction of the corpus. The cleanly surviving region narrows to λ78μm\lambda \lesssim 7\text{--}8\,\mu{\rm m}, m2528meVm \gtrsim 25\text{--}28\,{\rm meV}.

This short companion note anchors that surviving-region statement to primary-source laboratory bounds and documents the structural protection of the prediction from astrophysical, cosmological, and equivalence-principle exclusion.

Three primary-source laboratory bounds

λ\lambda rangeBoundSourceTCG status
λ=10μm\lambda = 10\,\mu{\rm m}α>14,000\|\alpha\| > 14{,}000 excludedGeraci et al. 2008 (microcantilever)TCG point above bound; excluded at 95% CL at λ=10μm\lambda = 10\,\mu{\rm m}
λ>10μm\lambda > 10\,\mu{\rm m}α108\|\alpha\| \gtrsim 10^8 excludedBlakemore et al. 2021 (levitated microsphere)outside cleanly surviving region
λ5μm\lambda \simeq 5\,\mu{\rm m}α107\|\alpha\| \sim 10^7 excludedVenugopalan et al. 2026 (optomechanical vector)TCG point 500×\sim 500\times below bound
λ10μm\lambda \gtrsim 10\,\mu{\rm m}α106\|\alpha\| \sim 10^6 excludedVenugopalan et al. 2026outside cleanly surviving region

The Geraci 2008 exclusion at λ=10μm\lambda = 10\,\mu{\rm m} falls below the TCG target αY1.88×104\alpha_Y \approx 1.88 \times 10^4. This is consistent with the cleanly surviving region λ78μm\lambda \lesssim 7\text{--}8\,\mu{\rm m} — the long end of the broader heuristic window has been understood to be in tension since the 2008 measurement; the narrower surviving-region statement of the Predictions and No-Go note already accommodates this. The verification accomplished is to anchor that surviving-region statement to specific primary citations.

The Venugopalan 2026 bound at λ5μm\lambda \simeq 5\,\mu{\rm m} leaves the TCG target untested by approximately a factor of 500500. This is a lower-window benchmark tied to the 2026 vector-sensing platform, not a global statement across the broader 510μm5\text{--}10\,\mu{\rm m} window.

Coupling translation

For a Yukawa potential matched to a gauge-form U(1)XU(1)_X potential with source charges QXQ_X, gX2=4πGmX2αYc.g_X^2 = \frac{4\pi G m_X^2 \alpha_Y}{\hbar c}. Using Gmp2/(c)=5.90×1039G m_p^2/(\hbar c) = 5.90 \times 10^{-39} and αY1.88×104\alpha_Y \approx 1.88 \times 10^4:

Coupling channelTCG-required value
gBg_B (baryon number)3.7×10173.7 \times 10^{-17}
geg_e (electron number)2.0×10202.0 \times 10^{-20}
ε\varepsilon (kinetic mixing equivalent)6.7×10206.7 \times 10^{-20}

Astrophysical and cosmological viability

ConstraintSensitivityTCG valueMargin
SN 1987A on gBg_B (Rrapaj–Reddy 2016)gB1.4×109g_B \lesssim 1.4 \times 10^{-9}3.7×10173.7 \times 10^{-17}8\sim 8 orders safe
SN 1987A on ε\varepsilon (Chang–Essig–McDermott 2017)ε109\varepsilon \lesssim 10^{-9}6.7×10206.7 \times 10^{-20}10\sim 10 orders safe
Red-giant / HB cooling (Hardy–Lasenby 2017)ε1012\varepsilon \lesssim 10^{-12}6.7×10206.7 \times 10^{-20}7\sim 7 orders safe
BBN/CMB thermalizationg107g \gtrsim 10^{-7} (rough)3.7×10173.7 \times 10^{-17}never thermalizes
Equivalence principle (long-range)composition fifth force at AU/cmer/λ0e^{-r/\lambda} \to 0 for rλr \gg \lambdanot applicable

The spin-1 entry is structurally protected from astrophysical, cosmological, and long-range EP exclusion in the representative vector and effective-mixing channels surveyed: production rates in stellar and supernova plasmas (scaling as g2g^2) are suppressed by factors of 1015\gtrsim 10^{15} to 102110^{21} below relevant bound thresholds; thermalization with the Standard Model bath is impossible at any cosmological epoch within standard production channels; the Yukawa range mismatch makes long-range EP tests inapplicable. Spin/axial channels require an operator-specific overlay once JYμJ^\mu_Y is derived; the gravity-normalized coupling scale makes a non-laboratory obstruction unlikely in those channels also.

Operator-coupling status

The TCG integer-spin tower postulate P6P_6 fixes the spin and the strength: P6s=1,αY=α2.P_6 \quad\Longrightarrow\quad s = 1, \quad \alpha_Y = \alpha^{-2}. It does not derive the operator coupling of the spin-1 mediator YY to Standard Model currents. The candidate channels are JYμ{Jmassμ,  Jnumberμ,  JBLμ,  Jspinμ,  J5μ}.J^\mu_Y \in \{J^\mu_{\rm mass},\; J^\mu_{\rm number},\; J^\mu_{B-L},\; J^\mu_{\rm spin},\; J^\mu_{5}\}.

For empirical-posture bookkeeping, the operator-coupling question is denoted by PYopP_Y^{\rm op}. This is a diagnostic label for a future operator-derivation problem (covering both the choice of JYμJ^\mu_Y and the corresponding sign of the Yukawa correction). It is not a new active-ledger residual, and it is not an extension of the four-arc named-residual pattern of the structural-state review.

Falsification chain implications.

The configurable-framing complement is preserved unchanged.

Verdict

Empirical-posture companion note — no new TCG postulate, no new active-ledger residual, no operator-coupling derivation, no experimental protocol, no claim of detection. The empirical posture of the Predictions and No-Go consequences note is internally consistent and is anchored here to primary-source laboratory bounds and a structural astrophysical-viability statement.

Active TCG/τCG postulate ledger UNCHANGED: P0P4,P5,P6,P7,PH,PSO(10).P_0\text{--}P_4, \quad P_{5'}, \quad P_6, \quad P_7, \quad P_{H'}, \quad P_{SO(10)}.

The 2026-05-01 framework closure verdict is preserved. The only viable falsification path for the TCG spin-1 entry remains direct short-range laboratory measurement in the cleanly surviving window.

Download paper (Zenodo) — 9 pages, 11 references. CC-BY-4.0.