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Statement. If z1,z2,z3,z4∈R2z_1,z_2,z_3,z_4\in\mathbb R^2 and ∣z1−z2∣=∣z3−z4∣>0|z_1-z_2|=|z_3-z_4|>0, there is exactly one orientation-preserving Euclidean isometry gg with g(z1)=z3g(z_1)=z_3 and g(z2)=z4g(z_2)=z_4.

Source. Mathialagan, published 2021 PDF, p. 10, Proposition 20. The printed statement omits >0>0, although its proof uses it. The nonzero condition is part of the application to the paper's energy.

Proof. A proper Euclidean isometry has form g(x)=Rx+tg(x)=Rx+t, where RR is a planar rotation matrix. Indeed, after subtracting g(0)g(0), preservation of squared distances and the polarization identity preserve inner products; the images of the standard orthonormal basis then determine an orthogonal linear map. Preservation of orientation selects determinant 11.

The two endpoint requirements force R(z2−z1)=z4−z3R(z_2-z_1)=z_4-z_3. Two equal-length nonzero vectors determine a unique rotation: their normalized directions specify its sine and cosine. This fixes RR, and then t=z3−Rz1t=z_3-Rz_1 is forced. Conversely these choices meet both requirements. If R=IR=I, the motion is a translation, including the identity. Otherwise I−RI-R is invertible, since det⁡(I−R)=2−2cos⁡α>0\det(I-R)=2-2\cos\alpha>0 for its angle 0<α<2π0<\alpha<2\pi. Its unique fixed point is (I−R)−1t(I-R)^{-1}t, so it is a nonidentity rotation about that point.

If the common length were zero, arbitrary rotations followed by the forced translation would satisfy the requirements, explaining the qualification.

Application. Each positive-energy quadruple has one proper motion with g(p1)=q2g(p_1)=q_2 and g(q1)=p2g(q_1)=p_2, since the source segment (p1,q1)(p_1,q_1) and target segment (q2,p2)(q_2,p_2) have the same positive length. Partition these motions into translations and nonidentity rotations.

Verification scope. Verified within the independently reviewed Theorem 3 chain, retained in the final review; the corrected hypothesis and the motion classification are components of the living Theorem 3 record.

Bears on. Problem 661.