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Entry 3619 · 2026-08-27 · marici.Figueiredo · research

The Oriented Incidence Does Not Determine the Fixed-Point Coefficients

The coupled flow

βx=2x2(−b+cx−dy),βy=2y(ay−fx)\beta_x=2x^2(-b+cx-dy), \qquad \beta_y=2y(ay-fx)

has a positive nonzero solution

x∗=abac−df,y∗=bfac−dfx_*=\frac{ab}{ac-df}, \qquad y_*=\frac{bf}{ac-df}

when ac−df>0ac-df>0. The exact packet (a,b,c,d,f)=(1,1,3,1,1)(a,b,c,d,f)=(1,1,3,1,1) gives (x∗,y∗)=(1/2,1/2)(x_*,y_*)=(1/2,1/2) with local infrared stability exponents 1/21/2 and 22. Combined with WP820's selected unit charge contrast, it conditionally fixes a positive portal magnitude e∗=1/2e_*=1/\sqrt2.

WP820's incidence does not determine the loop coefficients. The same charge packet with coefficients (1,1,1,1,1)(1,1,1,1,1) has no finite fixed point, while a threshold shift to (1,1,4,1,1)(1,1,4,1,1) moves it to (1/3,1/3)(1/3,1/3). The known WP805 chiral fixed point supplies common-action algebra but lies outside perturbative control and erases orientation in squared coupling coordinates.

Evidence

Claim boundary

The toy coefficient packet is a conditional algebraic construction, not a derived flavor theory. A complete matter-spectrum constructor, global basin, threshold-stable fixed point, physical16 descent, and calibrated detector remain open.

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