OMEGA object exploration 02: projective recognition, record recovery, and positive integration 20 September 2026 This note derives three further connections from the six labeled baseline marks. It includes a perspective invariant, exact error-correction bounds, and a sharp obstruction to positive integration at the canonical seed angle. Allowing the seed angle to vary as an explicitly declared extension reveals a boundary at exactly 36 degrees. The derivations use the marked-kernel definitions in Paper VII v1.6.0 and Paper VIII, Section 2. They are additional consequences developed in this exploration, using established mathematical methods. Historical priority for the particular applications has not been assessed. |Connection |Result |Essential conditions | |-------------------------------------|----------------------------------------------------------------------------------------------------------------|--------------------------------------------------------------------------------------------------| |Projective geometry |A cross-ratio of four outer marks recovers the seed parameter within the declared family. |Correct labels; a nondegenerate line projectivity; the prescribed golden extensions. | |Exact record recovery |Six affine landmark records correct two arbitrary corrupted positions or reconstruct four missing positions. |Known labels and seed; remaining records exact; affine coordinate model. | |Recovery after perspective projection|Six scalar image records correct one arbitrary corruption or reconstruct three missing records. |Known seed; finite, nondegenerate line projectivity; exact remaining records. | |Positive baseline integration |The canonical six nodes admit positive degree-three exactness but no nonnegative rule exact through degree four.|Uniform measure on the full baseline interval; nodes restricted to the six marks. | |A parameter boundary |At seed angle 36 degrees, the four outer marks support a positive degree-five rule. |This varies the seed angle; it is a related family member, not the canonical one-arcsecond kernel.| The common definitions are $$ \varphi=\frac{1+\sqrt5}{2},\qquad \varepsilon=\frac{\pi}{648000},\qquad \delta=\frac{\varepsilon}{2},\qquad s=\sin\delta,\quad c=\cos\delta. $$ Write $$ A=s+\varphi^2,\qquad B=s+1,\qquad (z_0,z_1,z_2,z_3,z_4,z_5)=(-A,-B,-s,s,B,A). $$ The points, in the order $(d_2,d_1,d,b,b_1,b_2)$, satisfy $$ p_i=\alpha+a(cu+z_i v),\qquad a>0,\quad |u|=|v|=1,\quad u\cdot v=0. \tag{1} $$ The proofs below hold for the stated parameter ranges with $0\sqrt5\,B$, since $$ A-\sqrt5 B=(\sqrt5-1)(s_*-s). $$ In this range $A^2>5B^2$ and $B^2>s^2$. Hence $D>0$ and $w>0$. Also $$ w_A=\frac{\frac23A^2-s^2-B^2}{D}>0, $$ because its numerator is greater than $\frac73B^2-s^2>0$. The weights sum to one, all odd moments vanish by symmetry, and $$ w(s^2+B^2)+(1-2w)A^2=\frac{A^2}{3}=I(t^2). $$ Thus (9) integrates every polynomial of degree at most three exactly with strictly positive weights at all six marks. For the canonical angle, the total pair masses are approximately $$ (w_s,w_B,w_A)= (0.359563193388285,\ 0.359563193388285,\ 0.280873613223430). $$ Each individual node receives half its pair mass. To show that degree four is impossible for any nonnegative weights on these nodes, take $$ P(t)=(t^2-B^2)(t^2-A^2). \tag{11} $$ It vanishes at the four outer nodes. At the inner pair both factors are negative, so $P(\pm s)>0$. Therefore every nonnegative weighted rule on the six nodes has $Q(P)\ge0$. However, direct integration gives $$ \begin{aligned} P(t)&=(t^2-B^2)(t^2-A^2),\\ I(P) &=\frac{A^4}{5}-(A^2+B^2)\frac{A^2}{3}+A^2B^2\\ &=\frac{2A^2}{15}(5B^2-A^2)<0, \qquad 0