Solution 1
Let , , and , so the condition becomes . Note that , so is the circumcenter of . Similarly, and are the circumcenters of and . Furthermore, . Thus, is cyclic. Similarly, and are cyclic. Let , , and be the circumcircles of , , and . As , we have that is not cyclic and , , and are distinct. By the radical axis theorem, , , and then concur at a point . Let denote the power of point to circle . We now compute . Let meet at and meet at . We have that and , so . Similarly, , , and . It follows by the law of sines on triangles and that . Thus, . By computing the analogous expressions for the other vertices, we conclude that . To conclude, recall the coaxial lemma: given two circles and and a constant , the locus of points for which is a circle coaxial to and . Hence, the circumcircle of is the locus of points with , and the analogous statements hold for the other vertices. The angle condition implies that segments , , and intersect, so the circumcircles of , , and pairwise intersect at two points. It follows that the circumcircles of and intersect at points and satisfying and for . But this then implies that for , so and both lie on the circumcircle of , as desired. Solution 2 Let be . Let be the power of an arbitrary point with respect to . Let . Define , and similarly. The angle condition becomes . An angle chase gives that so is the center of . We then further have . We now compute each of evaluated at each of . It's direct that . It suffices to compute as the remaining formulas follow from symmetry. Let meet at . We have By LOS on then , where is the side length of . Now we have all the powers!! The key claim that we've been building up to is the following: Lemma: If , and are defined similarly, then we have and . Proof: If we write any of the functions in coordinates, it's plus some linear equation. It's straightforward to check that (note ), so is a linear function. Our previous power of a point computation gives when is any of , , or . The only linear function that's zero at three noncollinear points is the zero function, so for all . Now, is the linear equation of the radical axis of and . We also have the analogous property for . But we also have , so these are the same line, as desired. Solution 3
Let ; the condition rewrites as . Firstly, we will make use of the angle condition: is circumcenter of We have that and lies on the perpendicular bisector of , so the conclusion follows. We have to find two points having equal powers with respect to the circles , and . We will first show that one of them is the concurrency point of . This claim is sufficient to prove the result: is cyclic. We have and similarly . Let and define similarly. We will prove that is cyclic, which will imply that concur at a point having equal powers to the three circles, which will finish the problem. Quadrilateral is cyclic. We have that and similarly , as wanted.
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