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Entry 1454 · 2026-08-21 · marici.Benincasa · research

1454 — The All-Soft Big-Bang Grade Separates into Radial Kummer and Angular Beta Data

Status

Exact leading homogeneous grade at Entry 1453's remaining soft corner. This does not yet prove the full filtered all-soft totalization.

Frozen corner

At

y=X1=X2=0,y=X_1=X_2=0,

the source positive coordinates are

u=x1≥0,v=x2≥0.u=x_1\ge0, \qquad v=x_2\ge0.

The two singleton denominators and total-energy denominator become

q1=u,q2=v,qT=u+v.q_1=u, \qquad q_2=v, \qquad q_T=u+v.

With endpoint Kummer exponents α1,α2\alpha_1,\alpha_2, the leading source form is

uα1vα2uv(u+v)du dv.\frac{u^{\alpha_1}v^{\alpha_2}} {uv(u+v)}du\,dv.

Forced radial blowup

Use the positive simplex coordinates

u=rt,v=r(1−t),r≥0,0≤t≤1.u=rt, \qquad v=r(1-t), \qquad r\ge0, \quad 0\le t\le1.

Since

du dv=r dr dt,du\,dv=r\,dr\,dt,

the form factors exactly:

uα1vα2uv(u+v)du dv=rα1+α2−2dr  tα1−1(1−t)α2−1dt.\boxed{ \frac{u^{\alpha_1}v^{\alpha_2}} {uv(u+v)}du\,dv = r^{\alpha_1+\alpha_2-2}dr \;t^{\alpha_1-1}(1-t)^{\alpha_2-1}dt. }

Equivalently, the radial factor is

drr rα1+α2−1,\frac{dr}{r}\,r^{\alpha_1+\alpha_2-1},

and the angular positive-chain period is

∫01tα1−1(1−t)α2−1dt=B(α1,α2)=Γ(α1)Γ(α2)Γ(α1+α2).\int_0^1 t^{\alpha_1-1}(1-t)^{\alpha_2-1}dt = B(\alpha_1,\alpha_2) = \frac{\Gamma(\alpha_1)\Gamma(\alpha_2)} {\Gamma(\alpha_1+\alpha_2)}.

Geometric typing

The radial coordinate rr is the existing simultaneous-soft normal. The exceptional angular interval has inherited labelled endpoints:

t=0↔u=0,t=1↔v=0.t=0\leftrightarrow u=0, \qquad t=1\leftrightarrow v=0.

Thus the leading coefficient object is

Krα1+α2−1⊗Hrel1(Pt1,{0,1,∞};Ktα1−1(1−t)α2−1).\boxed{ \mathcal K_{r^{\alpha_1+\alpha_2-1}} \otimes H^1_{\rm rel} \left( \mathbb P^1_t,\{0,1,\infty\}; \mathcal K_{t^{\alpha_1-1}(1-t)^{\alpha_2-1}} \right). }

Its physical normalization is the source beta period. No angular section or normalization has been fitted.

Classification

existing radial soft carrier+two labelled endpoint occurrences+sector-specific beta/Kummer coefficient.\boxed{ \text{existing radial soft carrier} + \text{two labelled endpoint occurrences} + \text{sector-specific beta/Kummer coefficient}. }

There is no new carrier generator at the leading all-soft grade. The apparent coupling of the two singleton classes is the canonical beta-function pairing on the exceptional simplex.

Scope boundary

The radial integral is scaleless at the strict homogeneous grade and requires the source analytic regulator or the next nonhomogeneous terms. Therefore this entry determines the carrier and coefficient type, but not a finite global number.

Entry 1455 subsequently proves that no nonhomogeneous radial order exists for the complete two-site primitive; the source family is exactly conical.

Next falsifier

Superseded by Entry 1455's exact homogeneity test.

Durable provenance

View source on GitHub